CA1304286C - System for recovery of petroleum from petroleum impregnated media - Google Patents

Abstract

Abstract of the Disclosure Process for in situ recovery of carbonaceous values from underground petroleum impregnated media such as oil shale, under controlled radiation from a microwave distributing source adjacent the media, e.g. in a borehole, effected in the absence of air, such that the radiation is distributed at least initially at incrementally increasing power and/or at least initially in intermittent interval cycles of on and off duration of the microwaves, for selective pyrolysis of the organic content of the media to liquid, vapor and gas form as the case may be under autogenous pressure in the pores of the media for driving the organic constituents therefrom for appropriate recovery, e.g. via the borehole, including breakup of larger molecules, e.g. hydrocarbons, for selective increase in the noncondensible gas quantities in proportion to the liquid and/or condensible oil vapor quantities, plus pyrolysis scavenging of residual carbon coke by gasification thereof to noncondensible gas constituents, optionally using a portion of the recovered noncondensible gases to produce electrical energy for energizing the microwave source, and conjoint probe apparatus having an adjustable extendable probe end for embedding in the porous media for in situ sensing of changes in the dielectric constant of the carbonaceous constituents undergoing microwave pyrolysis, and a mechanism for indicating the sensed changes, for adjusting the radiation in dependence upon such changes, the degree of extension of the probe end being adjustable in dependence upon the sensed frequency of the attendant radiation.

ABSTRACT PAGE

Description

SYST~ FOR R~COV~RY OF PRT~0LrUM
FRO~ PETR~L~M I~PRE~T~T~D ~DIA
~ACKGROUND OF TXE PRESE~T I~V~TIO~
The present invention relates to a microwave heating system for recovery of petroleum from petroleum i~pregnated media, and more particularly to the recove.ry of extractable organic or carbonaceous values from petroleum impregnated porous ~edi~ such as oil shale, oil and tar sands, heavy oil reservoir deposits and ~esidual heavy oil pools, e.g.
previously subjected to primary oil well drillin~ extraction, and the like, by the use of microwave or high frequency RF, i.e. radio frequency, radiation energy for in situ heating, preferentially of the liquifiable and gasifiable constituents such as hydrocarbons present in the pores of the media.
Hydrocarbons are found in varying compositions ~n various underground formation deposits, such as kerogen in oil shale and bitumen in oil sands and tar sands. Likewise, heavy oils with a high viscosity are found in reservoirs located within certain rock or sand formations~ These types of hydrocarbons found in such deposit~ require hèat to effect either thermal or chemical change for release and reco~ery of the desired carbonaceous constituents. Certain known processes require bot~ heating and chemical change to attain such recovery.
Howéver, attempts to recover, in situ, petroleum from oil bearing media have been limited to poorly controllable and inefficient bulk hea ing or yross heating recovery methods using primarily ~team or hot water to heat the media for causing the oil constituents to become suficiently flowable to be entrained in the steam or hot water and removed in admlxture therewith, whereupon the oil has to be separated from the mixture once rai~ed from the underground site to the ~3~

surf~ce.
These attempts typically require the steam or hot water to pass from the surface down a bore hole to the site of extraction at the underground level of the stratum in question, and to be pumped back to the surface a~ a mi~tur~
with the entrained oil constituents. Since the heating of the underground site is primarily by way of conduction heat transfer, both the desired oil constituents and the entire surrounding rock formation have to be heated in b~lk, and the system is beset with pronounced Btu (British thermal unit) heat loss through dissipation during travel of the steam or hot water along the pronounced distances of the bore hole between the surface steam generator or hot water heater and the underground deposit extraction site, in some cases amounting to many thousands o~ feet of separation.
As a consequence, the overall energy requirement for inefficiently proviaing such bulk heat at the underground extxaction site is so great that thes~ known methods are generally considered commercially impractical and economically unfeasible for industrial scale production purposes.
Even where open pit or strip mining and underground mining via open shaft and gallery arrangements, e.g. using the room and pillar method, are conducted, the attempts have not been successful since on the one hand, the landscape is inherently disturbed by open pit vr strip mining and the oper~tion must conform to go~ernmental environmental regulations and on the other hand, the mined oil bearing rock media must be brought in its entirety from the gallery through the shat to the surface. In both cases, the entire mass of the mi~ed oil bearing rock media mu~t be subjected to crushing and then retorting in a closed vessel.

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Such closed vessel retorting offers poor control and consumes large quantities of energy for heating the rock, as well as the oil, likewise by bulk heating, in most cases with the operation being carried out in the presence of air.
In the usual retorting operation, air is used to burn a portion of the desired oil content by ~irect combustion therewith in the retorting vessel so as to provide the necessary heat. This expedient not only consumes oil but also results in a gaseous fraction in which the valuable gasified oil constituents àre admixed and thus diluted with contaminating gaseous combustion products such as carbon dioxide.
Moreover, where incomplete combustion is carried out, iOe. with the use of smaller amounts of air in proportion to the carbon rich and/or hydrogen rich constituents in the oil, in addition to water formation the retorting leads to the production of carbon monoxide, rather than carbon dioxide, per the well known endothermic reaction by which any formed carbon dio~ide is reduced in the presence of e~cess carbon and/or hydrogen, relative to the attendant oxygen content, to carbon monoxide, depending on the attendant combustion conditions.
This renders the heating system nonuniorm and causes a loss in heat values to the extent that carbon monoxide, of comparatively low Btu value, is so formed in extra amounts than otherwi~e.
On the other hand, where the retorting is carried out in the absence of air, i.eO by indirect heat exchange, the bulk heating i~ even more inefficient, taking longer and thus consuming even more energy.
Pre~ent day consensus is that the United States must develop reali~tic alternative energy 80urce~ if the nation, ~3~

and indeed the industrialized world in gener~l, are to survive the portended future energy crisis.
One possible solution to the energy shortfall facing the United States in particular i5 the development of the vast oil shale deposits found especially in the States of Colorado, Utah and Wyoming. For instance~ oil shale of the Eocene Green River Formation in adjoining corners of these three states is estimated to contain 1.5 trillion barrels (bbls) of potential oil in place. This oil shale has low sulfur and high nitrogen content compared to petroleum as currently obtained.
Present oil ~hale activity in this regard is essentially experimental and its production insignificant due to the above noted drawbacks. Although many recovery methods are under ~tudy from time to time, costs have always been a deterrent, and environmental and/or technical barriers loom as insuperable.
It is estimated that present day oil shale recovery costs amount to from about ~35 to ~55 per barrel of produced oil, so that it is easy to see why present economics for developing otherwise readily available oil shale deposit~ are dubious O
As to surface retorting or fired methods, these not only involve the costs for mining the shale but also for crushing the rock to a retortable si~e, and then carrying out the actual r0torting. Underground mining al~o include~ the actual cost of physically bringing the mined rock to the surface through the open shaft.
Certain proposed underground mining me~hods contemplate the gallery or room and pillar method, but have been initially confined to shales of khe mahogany zone that are 1500 feet or le~ below the surface, and thak average 30 gallons per ton (g pt) or more in large beds 30 to 90 feet thick. These limitations are imposed by the costs currently encountered in underground mining.
Underground mining, and even surface mining by way of open pit or strip mining technique, involve measures that require at least five handlings Of the shale, e.g. for physically extracting or mining it, hauling lt, crushing it, retorting it, and disposing of the solid spent shale rock residue. These collectively const}tute a significant collateral cost to shale oil production.
Moreover, the environmentally acceptable disposal of the solid spent shale rock residue from the retorting, which represents about 80-85% of the weight of the shale, is itself costly, and is in addition to the cost~ of reh~bilitating the ground surface to meet governmental environmental regulations in the case of open pit~or st~rlp minlng, in particular.
In fact, not all underground oil Rhale deposits lend themselves to mining, and re~overy from the~e deposits is limited to in situ, or in place, methods. A typical example is an oil shale deposit of 625 square miles in the State of Wyoming that is estimated to ~ontain over 200 million barrels : ~ : : : : :
of oil per square mile. Unfortunately, where this rich oil shale occurs, the deposits are vertically discontinuous alternating thin horizontal beas of rich and lean oil shaleg rather than the more desirable vertically continuous or thick horizontal deposits. Hence, mining oil shale from this deposit is perforce economically unattractive, and recovery , would only be practical with in situ or in place methods.
Heat, of course, regardless of its source i8 essential in the processing of oil s~ale into shale oil whether by mlning and then surface retorting or by in situ retorting.

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The situation is the same where in situ retorting is used for treating tar sand deposits rather than oil shale.
Vast tar sand deposits exist in the United States and Canada which contain very heavy viscous crude oil or bitumen. This bitumen must be heated to facilitate its removal. Present heating methods use surface heated ~team to heat the bitumen, e.g. to 300 400~ (149-204C), to make it less viscous and thus more readily flowable. Such heating by steam is dependent upon the conduction of heat between fluid molecules, and is subject to heat loss and inefficiency problems.
In fact, the bitumen once recovered from the tar sands deposit must be converted into a light sweet crude before it can be refined or even transported. During such conversion, the bitumen is broken apart ~hermally into smaller fractions and the resulting material then hydrogenated. This helps to make the material sweeter and lighter. The process is not unlike hydrogenating margarine, and requires carbon removal and the addition of hydrogen, but represents and after-processing burden on the overall operation.
North American tar sands deposits are estimated to hold more oil potentially than the entire Middle ~ast, and exploitation of such tar sands deposits could help the industrialized West *o achieve energy independence. However, o these Yast "heavy oil" deposits, ik is considered that only about 100 billion barrel9 could be rec~overed within the limitations of current technology and economic conditions.
Improved technology would, of course, increase significantly that potential.

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A third source of potential fossil energy in significant amounts is found in the still remaining petroleum deposits or heavy crude oil reservoir deposits or residual heavy oil pools previously subjected to primary oil well drilling extraction. These latter deposits which are located in subsurface reservoirs or pools of depLeted or partially depleted oil wells, are what remain in exploiting our present main source of petroleum energy from "dome oil" wells. ~he primary recovery of this oil is effected by sinking wells into oil bearing formations and allowing the natural pressures within the oil impregnated strata to force the fluid into the well bore where it can be conveniently collected by pumping.
In some of these "dome oil" reservoirs and in partially depleted reservoirs there may not be enough natural pressure available to force the oil into the well bore at a sufficient rate to be economically profitable. In other reservoirs the oil flow may be retarded by the "heaYy oil" andparaffin content of the petroleum that closes the natural flow channels of these underground crude oil reservoirs. Standard secondary recovery methods such as the injection of wat~r, gas, air or a combination of these material~ i~to the formation are used, as well as the application of heat energy by either chemical or electrical means. Hence, these are often referred to as "huff and puff" pool oil wells.
Where direct firing or in situ retorting of the oil or gas bearing formations in these "dome oil" reservoirs or "huff and puff" pool oil wells is used in~tead, it is found to produce a contamination of tbe crude petroleum or gase~, and thus suffers from the same drawback a~ direct firing in the case of surface retorting of mined oil shale.
Chemical heating methods, like hot water and steam ~3~

heating methods, have generally been unable to provide sufficient heat economically or satisfactory results. For the same reason, electrical resistance heating methods have proven unsuitable in that the transfer of heat to the oil bearing strata is primarily bulk heating or gross heating, accomplished by conduction. In all of these cases, the rate of conduction is low and the heat is continually drawn away f~om the oil bearing strata by the pumping of the heated oil.
Chemically or electrically provided heat must also be expended to heat both the formation itself and the oil.
A particular problem with all conventional downhole heating methods which rely solely on heat conduction is that the heavier crudes, which require most of the heating, are the poorest type of thermal conductors among the crude oils. This aggravates the energy consumption in heating not only the oil but also the surrounding rock, since the rock is a poor thermal conductor as well and must be heated to the same e~tent as the oil, including the heavier crudes, before the temperature is sufficient consequent such bulk heating or gross heating to facilitate flow of the oil through the channels in the formation to the well bore.
The reason why oil shale requires the application of heat in order to produce oil is because the carbonaceous values contained in the oil shale rock are in the form of solid insoluble organic matter, and not oil. Howevex, this solid organic matter will decompose to yield oil, when heated, i.e. when it is retorted, such oil being recovered in the form of oil vapors along with gas, e.g. non-condensible gaceous constituent~ admixed with the oil vapor constituents.

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In this regard, oil shale has been described as a sedimentar~ rock with relatively high organic content, e.g.
30-60% volatile matter and fixed carbon, that yields an oil when heated. On the other hand, it does not yield oil when extracted with ordinary solvents. Typical oil shales may yield anywhere from 20-50 gallons of crude oil per ton (gpt), the oil constituents often being of a relatively unsaturated or olefinic character compared to the usual petroleum.
The organic oil yielding matter present in oil shales as solid insoluble matter is generally called kerogen.
Kerogen is not consider~d a definite compound but has been described as a complex mixture of various complex compounds that varies from one shale species to the next, and usually exists as a soft brown powdery material that is at best only slightly soluble in ordinary organic solvents, and that may contain small proportions of nitrogen and sulfur constituents as well as oxygen, e.g.as hetero atoms. The porous rock matrix in which the kerogen is ~ituated in oil shale usually contains associated free water and bound water of crystallization, e.g. where the rock consists of carbonates, silicates, aluminates, etc., often in conjunction with pyrites.
Kerogen in oil shale must be heated to high temperature before it pyrolyzes or decomposes. For this reason, in the case of surface retorting, the mined oil shale must first be crushed to reduce its size for more efficient exposure of the material to the heat. Despite significant world oil price increases, a primary reason why the known mining, crushing and retorting technique for recovering oil from oil shale has still not become commercially viable is because oil shale is relatively lean ore.

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Experience has shown that e~en a ton of relativ~ rich oil shale of 25 gpt (but actually a lean ore at 0.0125 yallon per pound, iOe. 25/2000) will only produce about 0.6 barrel of oil, after expending elaborate efforts in the five hanalings of mining, hauling, crushing and retorting the shale, and then disposing of the spent shale within environmentally acceptable guidelines, aside from the energy consumed in bulk heating of the shale to acc~mplish pyrolysis of the kerogen during the retorting.
The alternative of bulk heating of the oil shale in a surface retort is by burning or retorting it in place underground by direct combustion of a portion of the kerogen content with supplied extraneous air, but such is no less impracticable, aside from the contamination of the produced oil with combustion products and possible environmental hazards. This is because much of the oil shale encountered underground is nearly impermeable, despite its internal content of tiny pores containing the kerogen, and must first be mechanically broken up in order to permit the hot combustion gas to pass through it~
A satisfactory method to break up shale oil deposits in place has not been found. The present method in~olves blasting the rock and the removal o~ a portion of the rubble (about 25%) to allow for a fire-flow through the fractured deposit. Results are less than satisfactory because of tha inefficient burning of the shale due to the non uniform size of the rubble.
Ac ually, oil shale deposits exist as planes or discontinuous deposits or beds of varied thickness at random levels along the underground formation, and each may be a relatively rich or a relatively poor oil ~hale plane or bed alternating with intervening planes or beds of barren rock.
Because of the nature of the particular porous media and its impregnated petroleum content, whether in the form of oil shale, oil sands, tar sands, heavy oil reservoir deposits, residual heavy oil pools, e.g. previously subjected to primary oil well drilling extraction, and the like, the ~annex in which the particular deposit of the porous media occurs in the underground formation,e.g. in lean and rich discrete beds, often of narrow seam height randomly disposea along the vertical course of the formation, and/or in deposits or reservoirs or pools of pronounced depth from the ground surface, and furthermore, because of the inefficieneies and cost of gross heating or bulk heating, whether by in situ heating using hot water or steam, or chemical or electrical heating means, or by in situ retorting or direct firing with supplied e~traneous air, or by surface retorting using direct firing with supplied extraneous air or indirect heat exchange, normally preceded by crushing and followed by spent shale disposal, none of these known techniques has been commercially uccesæful or competitive with petroleum obtained by the usual primary oil drilling methods from dome oil reservoirs and the like.
U.S. Patent 4,193,448, issued March 18, 1980 to Calhoun G. Je mbey, discloses and claims an apparatus, e.g. in the form of an elongated shell attached to the lower end of a pipe arrangement, for recovery of petroleum from petroleum i~pregnated medla such as rock, shale and sands, and includes an ~lectrically energized microwave generator and a guide for directing mi~rowaves to a microwave dispersing chamber for heatin~ the media, plus a plurality of holes in the shell for the inflow of heated petroleum into a petroleum chamber from ~3~

the heated media. The apparatus i5 inserted into an opening, e.g. a borehole, in the media, then microwaves are dispersed into the ~edia to heat the same, and the heated petroleum is recovered therefrom in the petroleum chamber via the holes.
The system is safe, cost efficient and at least as fast as conventional methods for thP recovery of oil from shale, while using substantially less energy than that required for conv~ntional heating methods. In particular, there is no substantial alteration of the landscape nor appreciable environmental impact since the heating and recovery operations are conducted underground, i.e. at a downhole site in the borehole.
However, V.S. Patent 4,193,448 does not disclose extensive or particularized details as to the actual process of extracting or recovering in sit~ the petroleum or oil from the impregnated media, let alone the pyrolysis production of both oil and gas, including that traceable to residual solid ~orm carbon coke remaining after pyrolysis of kerogen, etc. to ~remove the initially generated liquid and gas constituents, while permitting molecular break down or "cracking" of the attendant hydrocarbon constituents to smaller molecules and particularly to increasing proportional amounts of noncondensible gase~.

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SUMMARY OF THE I~VENTION
~. _ It is amon~ the objects and advantages of the present invention to overcome the deficiencies and drawba~ks of the prior art, and to provide an economical and efficient process for in situ or in place recovery of e~tractable carbonaceous values, such as hydrocarbo~s from underground petroleum impregnated porous media, such as oil shale, oil and tar sands, heavy oil reservoirs and residual heavy oil pools previously sub~ected to primary oil well drilling extraction and the like type sources of synthetic fuel in which microwave radiation or radio frequency (~F) energy is applied to the media, such as from a microwave distributing or generating source substantially immediately adjacent the media, and distributed at least initially at incrementally increasing radiation power and/or in intermittent cycles of on a~nd off duration~, e.g., for preferentially heating the petroleum content in the medla selectively to a temperature sufficient for correspondingly liquifying and ga~ifying the ::
liquifiable and volatilizable constituents present, and incrementally progre~sively in a direction away from the ~source, to cau8e ~the tbereby liquified and gasified constituents to migrate under autogenous pressure through the porous~media in a direction toward the source, for recovery from the vicinity of the source~
It is among the add~itional objects and aavantages of :
the present invention to provide a process of the foregolng type, in which the microwave~heating temperature is ~elected to cau e the liquified constituents predominantly to gasify ~or forming a mixture of predominantly gasified constituents and a minor amount of residual liqui~ied constituents, and/or in which after recovery substantially of the liquified and ~L3~

gasified constituents from the media the microwave heating temperature is raised selectively for causin~ residual ur.liquified and ungasified carbon constituents present in the media to gasify and migrate under autogenous pressure for like recovery from the vicinity of the source, and/or especially in which a portion of the recovered, e.g. gasified, constituents is used to produce electrical energy for energizing the microwave distributing or generating source.
Yt is among the further objects and advantages of the present invention to provide a process of the stated type, in which the distribution and utilization of the microwave generated energy, such as from the in situ microwave distributor source locally adjacent the in situ media is selectively controlled in dispersement pattern, in intermittent interval cycle or continuous auration, as well as in varying or constant power as~the case may be, as it relates to the heating of the organic material present in the media, for maximizing the oil and ~as recovery capacity of the system by confining the energy distribution to a selective specific zone and by avoiding overheating of the media adjacent the microwave distributor source while preferentially heating the petroleum constituents progressively along the extent of the zone, from the portions thereof adjacent to those remote from su~h source.
It i~ among the still further objects and advantages of the present invention to provide a proce~s of the stated type;
which is able to use radio frequency or microwave energy for isl situ heating o~ the media for commercially producing oil and gas on an industrial scale that i9 both technically and economically feasible, enabling large deposits of readily accessible oil shale to be exploited, which for example, even 13~

at a modest 25~ recovery factor would yield in excess of an estimated 210 million barrels of oil from a given set of oil shale containing sections in the State of Wyoming alone, and in any case at an estimated cost below or competitive with current world market oil prices: which potentially produces all of its own field energy requirements from the recovered product itself, such product constituting a relatively clean oil product in comparison to that obtained by conventional retorting methods: and which requires almost no water and has virtually no negative environmental impact.
It is among the still further objects and advantages of the present invention to provide a sensing and indicating apparatus including a sensing probe for embedding in the underground porous media being worked for carrying out the pyrolysis under an ongoing indication of the changes in the dielectric constant of the constituents being pyrolyzed as a function of the microwave radiation being applied and optionally w1th associated means for oensing prevailing temperatures for controlling the operating conditions for optimum RF energy utilization.
It is among the still further objects and advantages of :
th~ present invention to provide an array of such probes in a given under~round porous media site being worked and for undertaking microwa~s pyrolysls ln conjunction therewith for ongoing measurement and control of the operating conditions, and to obtain operating condition information applicable for carrying out the pyrolysis at further underground porous media ~ite~ having comparable carbonaceous values and mineral content to that of the first mentioned site but without the need to use such array of probes at those further sit2s.

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It is among the still further objects and advantages of the present invention to provide a process of the stated type for carrying o~t the extraction of extractable carbonaceous values substantially simultaneously at a plurality of separate individual sites using at each site microwave radiation distributed at least initially in successive intermittent interval alternate cycles of on and off duration for heating the impregnated petroleum content, such that some vf the microwave sources at some of the sites are only energized during the alternate off duration cycles of the remainder of the microwave sources at the remainder of the sites respectively, and in turn the remainder of the microwave sources are only energized during the alternate of duration cycles of the first mentioned microwave sources, for substantially complete electric energy utili&ation~

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BRI~P DESCRIPTIO~ OP T~E DRAWI~GS
Other and further objects and advantages of the present invention will become apparent fro~ a study of the within specification and accompanying drawings, in which:
Fig. 1 is a schematic sectional view of a for~ation installation at a borehole or well bore with respect to whic~
the process for in situ recovery of extractable carbonaceous values may be carried out according to the present invention;
Figs. 2a and 2b are companion schematic views, not drawn to scale (i.e. non-scalarj, with Fig. 2a showing from above portions of successive annular rings of progressively increasiny selective, yet nonuniform, increments in feet of radius from a borehole or well bore extending through a stratum of oil shale, and the concordant increments in kilowatts of microwave raaiation (~F) associated with the pyrolysi production of oil and gas relative to the annular span of~each corresponaing ring~
and :with Fig. 2b showing a composite graph of such nonuniform increments in *eet of radius ~top abscissa) and in kilowatts of microwave radla~ion (bottom abscissa) as a function of~the on~and off Xeating cycle times in seconds:of the microwave radiation (l:eft ordinate)~and cumulatiYe oil and gas prodaction qu~antit~y at~an approxlmately constant production rate~(right o;rdinate and shaded area), plus the :
progressive:ly increasing pyrolysis temperature at pertinent levels ~along the non- calar slope of: the straight line intersecting curve~defining the boundary of the cumulatively increasing, and approximately: constant production rate, pyrolysis generated oil and gas quantity in the shaded area;
Fig. 3 is a schematio view of an in 5itu praba ~ystem which include8 a probe end which may be embedded in the ~3~428~

deposit of petroleum impregnated porous media for sensing and indicating the dielectric constant of the carbonaceous constituents undergoing pyrolysis as a function of the microwave radiation being applied to the porous media, and an associated embedded thermal analysis device for recording the temperature at the particular probe site; and Figs. 4 and 5 are schematic top and perspective views respectively of a spiral arrangement of sample probe bores containing probes or probe systems of the type shown in Fig.
3, for obtaining information during microwave pyrolysis operations carried out in a aeposit adjacent a borehole having an installation of the type shown in Fig. 1.

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DETAILED DESCRIPl'ION OF TIIE I1~1TIOl~

According to a first main aspect of the presen~
invention, a process for in situ recovery of extractable carbonaceous values from underground petroleum impregnated porous media is provided, comprising subjecting the underground petroleum impregnated porous media, in situ and in the substantial ahsence of air, to microwave radiation from a microwave distributing source substantially immediately adjacent the media and distributed at least initially at incrementally increasing radiation power, for heating the impregnated petroleum content preferentially relative to the corresponding porous media and progressively in a direction away from the microwave source.
- Such heatin~ is effected to a selective temperature of at least about 425C and sufficiently for liquifying substantially the liquifiable petroleum constituents present which liquify at the oorresponding heating temperature and for gasifying substantially the volatilizable petroleum constituents present which gasify at such heating temperature and in turn for causing the thereby formed mixture of liquified and gasified constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave ource. Hence, the migrating nstltuents can be readily recovered from the vicinity of the microwave source.
Thus, in accordance with a cycle feature of the present invention, the radiation may be distributed at least initially in intermittent interval cycles of on and off duration, for instance ~uch that at least initially the interval~ of on z~
duration progressively increase, and/or such that at least initially the intervals of off duration progressively decrease.
In particular, the radiation may be distributed initially in intermittent interval cycles of on and off duration in a first phase, and thereafter be distributed substantially continuously in a second phase, for instance with the intervals of on duration progress:ively increasin~ in the first phase and/or the intervals of off duration progressively decreasing in the first phase.
Also, in accordance with a power le~el feature of the present invention, the radiation may be distributed initially at incrementally increasing radiation power in the first phase, and thereafter be distributed at substantially constant correspondingly increased power in the second phase. In conjunction therewith, the radiation may be distributed in such intermittent interval cycles of on and off duration in the first phase, for instance with the intervals of on duration progressively increasing and/or the intervals of off duration progressively decreasing, and thereafter the radiation may be distributed substantially continuously in the second phase.
Moreover, in accordance with a distance range feature of the prPsent invention, the radiation may be distributed for heating the impregnated petroleum content to the linear extent of at least about 30 feet in at least one direction away from the microwave source.
In particular, the radiation may be distributed initially at incrementally increasing radiation power and until the heating of the impregnated petrole~m content has progressed to the linear extent of at least about 20 feet in at least one direction away from the microwave source in the first phase, and thereafter may be distributed at substantially constant correspondingly increased power in such direction in the second phase.
In conjunction therewith, as before, the radiation may be distributed initially in intermittent interval cycles of on and off auration in the first phase, and thereafter be distributed substantially continuously in the second pha~e, especially with the intervals of on duration pro~ressively increasing and/or the intervals of off duration progressively decreasing in the first phase.
Furthermore, in accordance with a temperature control feature of the present invention, the heating temperature may be maintained at between about 425-500C, for instance between about 425-475C for thereby forming a mixture of predominantly -liquified constituents and a corresponding remaining minor amount of gasified constituents, or between about 476-500C
for thereby forming a mi~ture of predominantly yasified constituents and a corresponding remaining minor amoant of liquified constituents.
In particular, in a first step the radiation may be distributed until substantially all of the liquifiable and volatilizable constituents present which concordantly liquify and gasify at the corresponding heatin~ temperature have been liquified and gasified and in turn recovered, and thereby leave a remainder content of re~idual unliquified and ungasifi~d carbon constituents in the corresponding porous medial and in a second step substantially without interruption the porous media may be thereafter subjected to continued ~l3~ 6 radiation from the microwave source correspondingly for heating such residual carbon constituents to a selective temperature of at least substantially about 525C and below about 600~C and sufficiently for gasifying substantially such residual carbon constituents a~d in turn for causing the thereby gasified residual carbon constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source. The migratin~ gasified residual carbon constituents may th~n likewise be recovered from the vicinity of the microwave source.
The microwave source may be favorably located in a well bore at a level adjacent the underground stratum of the porous media, and the migrating constituents thus may be recovered from the vicinity of the microwave source via the well bore.
In particular, where the porous media are oil shale media, the carbonaceous values will include kerogen which is correspondingly pyroly7ed by the microwave heating.
Advantageously, a portion of the recovered constituents is used to produce electrical energy for energi~ing the microwave distributing source.
According to a second main aspect of the present invention, a proce s fcr in situ recovery of extractable ~arbonaceous values from underground petroleum impregnated porous media i5 provided, comprisi~g two steps.
The ~irst step comprises subjecting an underground s~ratum of the petroleum impregnated porous media,~ in situ and in the substantial absence of air, to microwave radiation from a micro~ave distributing source located in a well bore at a level ~ubstantially immediately adjacent such underground stratum, for heating the impre~nated petroleum content to a 1304Z~6 selective temperature sufficiently for liquifying substantially the liquifiable petroleum constituents present which liquify at the corresponding heating temperature and for gasifying substantially the volatilizabIe petroleum constituents present which gasify at such heating temperature and in turn for causing the thereby formed mixture of liquified and gasified constituents to migrate under autoyenous pressure through the porous media in a direction toward the microwave source, and recovering the migrating constituents from the vicinity of the microwave source via the well bore.
The selective temperature of the first step is insufficient for liquifying and gasifying residual carbon constituents in the corresponding porous media, and thereby leaves a remainder content of residual unliquified and ungasified carbon constituents therein.
The second step comprises, substantially without interruption reIative to the first step, subjecting the porous media thereafter to continued radiation from the microwave source correspondingly~for heating such remainder content of residual unliquified and ungasified carbon constituents therein to a selective increased temperature sufficiently for gasifying substantially such residual carbon constituents and in turn for causing the thereby gasified residual carbon constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source, and recovering the migrating gasified residual carbon con~tituents from the vicinity of the microwave ~ource via the well bore.
In particular, the fir~t ~tep temperature may be between about 425-500C and the 9econd step temperature may be iL3~

at least substantially about 525C and below about 600C.
Preferably, a portion of the recovered gasified constituents includes noncondensible gas and a~ least a portion of such noneondensible gas is used to produce electrical energy for energizing the microwave distributing source. Hence, advantageously the first step temperature may be between about 476-500~C for thereby forming a mi~ture of predominantly gasified constituents and a corresponding remaining minor amount of liquified constituants.
Accordingly, where the porous media are oil shale media, the carbonaceous values will include kerogen which is correspondingly pyrolyzed by the microwave heating to provide such liquified and condensible and noncondensible gasified products.
According to a third main aspect of the present invention, a probe system or apparatus is provided for in situ sensing of changes in the dielectric constant of extractable carbonaceous values, e.g. hydrocarbons, in underground ~petroleum impregnated porous media during the subjecting thereof in situ to microwave radiation.

:: -The probe apparatus comprises an open ended coaxial transmission line having an in situ probe end and a remote end,: and :includes a conductive probe as core conductor insulated or ~eparated electrically from its counterpart coaxial conductive : jacket as peripheral conductor by an insulating material, e.gO high tempe~ature resistan~
thermosetting plastic, or alternatively, a void annular space or vacuum space from which air has been excluded and which may optionally be filled by captively contained inert gas and provided with insulating fixed radial spacer~ ke~p:Lng the ~3~ 8~i .

probe and jacket electrically apart along the course of the transmission line and with gas sealing insulating end radial spacers plugging the opposed ends of the transmission line or at least the in situ probe end.
The probe is arranged for axial movement relative to the jacket and rPlative to such plastic, or to such radial spacers where alternatively present, for extending the adjacent end portion of the probe a selective distance beyond the in situ probe end of the line to provide an adjustable length exposed probe end portion for embedding in such porous media.
Furthermore, indicating means are arranged at the remote end of the line for indicating the sensed changes in such dielectric constant.
Favourably, an associated conventional in situ thermal analysis device or means, or like type temperature sensing and recording means, is also provided in the probe apparatus, having a sensing portion adjacent the in situ probe end for embedding in the porous media whereby to sense and record the prevailing temperature at the particular in situ probe site.
In turn, such indicating means arranged at the remote end of the line are also arranged in this instance for indicating the temperature sensed by the censing portion at the in situ probe site.
In conjunction therewith, according to a fourth main aspect of the present invention, a method of using the above noted probe system or apparatus is in turn provided.
The method comprises embedding the probe end of the coaxial transmission line in an underground petroleum impregnated porous media and placing the remote end of the ~1' ~3~Z~6 transmission line and the indicating means at a remote location relative to the porous media, subjecting the porous media in situ to microwave radiation sufficiently for heating the impregnated petroleum content for extracting the extractable carbonaceous values therefrom, sensing changes in the dielectric constant of the extractable carbonaceous values, during the microwave radiation heating of such petroleum content, by the embedded probe end of the transmis~ion line,~ and indicating the sensea changes ~y the indicating means at the remote end of the transmission line, and ad justing the microwave radiation in dependence upon the sensed changes in such dielectric constant.
More particularly, the method of using the probe apparatus may be carried out such that the e~posed length of the end portion of the embedded probe end is adjusted in dependence upon the fre~uency of the attendant microwave radi~tion.
Desirably, such method further includes sensing in situ, e.g. via such sensing portion of the associated thsrmal analysis means, the prevailing temperature at the in situ probe site, and ad justing the microwave radiation in dependence upon the sensed changes in dielectric constant in conjunction with sensed changes in temperature, e.g. as recorded by such indicating means.
According to a related fifth main aspect of the present invention, an analogou~ process for in situ recovery of extractable carbonaceous values from underground petroleum impregnated porous media is provided utilizing an array o~
dielectric constant sen~ing probes.

~3~3~;8~

Desirably, such method further includes sensing in situ, e.g. via such sensing portion of the associated thermal analysis means, the prevailing temperature at the in situ probe site, and adjusting the microwave radiation in dependence upon the sensed changes in dielectric constant in conjunction with sensed changes in temperature, eOg. as recorded by such indicating means.
According to a related fifth main aspect of the present invention, an analogous process or in situ recovery of extractable carbonaceous values from underground petroleum impregnated porous media is provided utilizing an array of dielectric constant sensing probes.
This analogous process comprises positioning a microwave distributing sources in a bore hole t a vertical level adjacent the underground petroleum impregnated porous media, and also positioning such an array of dielectric constant sensing probes in a corresponding array of probe accommodating bores selectively positioned in spaced relation to each other and at conjointly incrementally increasing progressive radial distances from the bore hole as center such that the probes are at substantially the same vertical level as the microwave distributing source and are respectively embedded in situ in the adjacent underground petroleum impregnated porous media thereat.
In turn, the porous media is subjected in situ to microwave radiation from the microwave ~ource sufficiently for heating the impregnated petroleum content for extracting the extractable carbonaceouY values therefrom while sen~ing changes in the dielectric constant of the extractable carbonaceous values, durlng the microwave radiation heating of the petroleum content, by the corresponding probes along the progressive radial di9tances thereof from the bore ho:le, and the microwave radiation is correspondingly adjusted in dependence upon the sensed changes in such dielectric constant.
Preferably, the array of probe bores and probes is substantially in the f~rm of an outwardly increasing radius spiral arrangement at least partially around the bore hole as center.
Aavanta~eously, the sensed changes in dielectric content are recorded, and the process is repeated at a separate bore hole site having underground petroleum impregnated porous media of substantially the same content of carbonaceous values and mineral as the first mentioned porous media, but in this instance, without the array of probe bores and probes being used, instead carrying out the microwave radiation in dependence upon such already recorded sensed changes in dielectric constant.
Advantageously, the sensea changes in dielectric content are recorded, and the process is repeated at a separate bore hole site having underground petroleum impregnated porous media of substantially the same content of carbonaceous values and mineral as the first mentioned porous media, but in this instance without the array of probe bores and probes being used, instead carrying out the microwave radiation in dependence upon such already recorded sensed changes in dielectric constant.
Nere al~o, the probe6 desirably include such associated thermal analysis means for sensing the prevailing temperature, and ~he thermal analysis means are also respectively embedded in situ in the adjacent porous media thereat, such that the microwav~ radiation is adjusted in dependence upon the sensed changes in ~ielectric con~tant in conjunction with sensed changes ln such temperature.

In like manner, upon correspondingly recording the sensed changes in dielectric constant and prevailing temperature, the process may be repeated at such a separate bore.site, again without the array of probe bores and probes and associated thermal analysis ~eans, instead carrying out the microwa~e radiation in dependence upon such already recorded sensed changes in dielectric constant and prevailing temperature.
According to a sixth main aspect of the present invention, a multiple site process for in situ recovery of extractable carbonaceous values from underground petroleum impregnated porous media i8 provided, comprising substantially simultaneously subjecting each of a plurality of separate individual sites of underground petroleum impregnated porous media, in situ and in the substantial absence of air, to microwave radiation from ea~h of a corresponding plurality of microwave distributing sources substantially i~mediately adjacent the porous media at each such site respectively.
~ he micro~ave radiation is distributed at least initially in successive intermittent interval alternate cycles of on and of duration and sufficiently for heating the impregnated petroleum content for e~tracting extractable carbonaceous values therefrom, while ~orrespondingly at least initially selectively alternatively ~upplying electric~l energy concordantly in successive intermittent interval alternate cycles of no and off duration to the corre~ponding microwave sources.
In this way, electively some of the plurality of microwave sources are only energized during the alternate off duration cycles of the remainder of the plurality of microwave ~ources, and in turn the remainder of the miarowa~e sources are only energized during the alternate off duration cycles of 13~Z~36 the first mentioned microwave sources, for substantially complete utilization of the supplied electrical energy, and accordingly the thereby extracted carbonaceous values are in turn recovered.
Preferably, at least a portion of the recovered carbonaceous values is used to produce the electrical energy supplied to the plurality of microwave sources.
Desirably, the microwave radiation is distributed at least initially also at incrementally increasing radiation power and in intermittent cycles of on and off duration in a first phase, and thereafter is distributed at substantially constant correspondingly increased power to each of the microwave sources in a second phase under a concordantly increased supply of eleetric energy sufficiently to energize substantially simultaneously and continuously all of the microwave sources at such constant increased power at the same time.
In the latter instance, where at least a portion of the recovered carbonaceous values is used to produce the electric energy supplied to the plurality of microwave sources, correspondingly also at least a further portion of the recovered carbonaceous values is used to produce the increased ~upply of electrical energy u~ed in the second phase.
Broadly, in regard to a power distribution overall feature of the present invention, a process for in situ recovery of extractable carbonaceous values from underground petroleum impregnated porous media is provided, comprising subjecting ~uch media in situ to microwave radiation from a microwave distributing source and distributed at least ini$ially at incrementally increasing radiation power and sufficiently ~or heating the impregnated petroleum content for extracting extraatable carbonaceous valuas therefrom, and ~3~ 6 recovering the thereby extracted carbonaceous values.
Preferably, the radiation is distributed initially at incrementally increasing radiation power in a first phase, and thereafter is distributed at substantially constant corresp~ndingly increased power in a second phase.
Optionally, the radiation is distributed at least initially also in intermittent cycles of on and off duration, and preferably is distributed initially in intermittent interval cycles of on and off duration in a first phase, and thereafter is distributed substantially continuously in a second phase~
~ avorably, in this regard, the radiation is distributed initially both at incrementally increasing radiation power and in intermittent cycles of on and off duration in a first phase, and thereafter is distributed at substantially constant correspondingly increased power continuously in a second phase.
Broadly, in regard to a duration distribution overall feature of the present invention, a process for in situ recovery of extractable carbonaceous values from underground petrole~m impregnated porous media is provided, comprising subjecting such media in situ to microwave radiation from a microwave~diRtributlng source and ~distributed at least lnitially in interm:ittent cycles of on and off duration and suf~iciently for heating the impregnated petroleum content for extracting extractable carbonaceous values therefrom, and recovering the thereby extracted carbonaceous values.
Pre~erably, the radiation is distributed initially in intermittent interval cycle~ of on and off duration in a f irst phase, and thereafter is distributed ~ubstantially continuously in a second phase.

~30~

Microwaves constitute comparatively high frequency electromagnetic waves of short wave length. Microwave heating concerns the subjecting of materials to such high frequency electromagnetic waves whereby the microwave absorbent molecules in the materials are excited thereby and their agitation creates heat. On the other hand, certain materials are microwave transparent, having the ability to transmit microwaves without resistance or absorption and this without being heated thereby.
Microwave generating systems, such as that contemplated in the apparatus of said U.S. Patent 4,193,448, which are capable of providing microwave planar radiation, i.e.
generating a horizontal microwave radiated pattern confined to a selective predetermined vertical area, are particularly suitable for carrying out the in situ extraction or recovery of carbonaceous values from porous petroleum impregnated media such as oil shale, oil and tar sands and residual heavy oil pools, according to the process of the present invention, especially in the case of vertically discontinuous oil shale beds.
By distributing such microwave radia~ion or energy rom a bore hole into the media belng worked, the high frequency radio waves provide heat energy which causes in situ heating of the oil bearing media or ore, and such may be carried out under controlled conditions to cause the h~drocarbon molecules in any sol~d organic matter or kerogen in the deposit to become liquid and then vaporize, as in the case of oil shale, or to cause such molecules in any liquid organic matter or petroleum oil or bitumen in the deposit to vaporize directly, as in the case of oil and tar qands and/or re~idual heavy oil pools, all within a ~elective predetermined 3~Z~36 vertical are~ a~d a corresponding horizontal arc of selective angular extent from the bore hole as center or over the full 360 degree circumference of the radial area being worked.
In the case of oil shale, hydrogen and methane are the two major gases yiven off when the shale is heated. These noncondensible gases assist the flow of the oil constituents within the shale in the direction of the borehole. The created gases are advantageously captured and may be u~ed to power a surface electrical generator, e.g. a fuel cell such as a l-KW Raytheon fuel cell electrical generator or the like.
In fact, considering that t~e drilling ana microwave extraction operations normally occur in remote and sparsely populated locations, a ready source of extra electrical ener~y is inherently available for consumption by local communities, otherwise dependent on power supplied over long distance transmission line networks, by converting any surplus of the captured gaseous constituents provided by the oil shale via such a surface generator fuel cell or the like for that local consumption.
Advantageously, the removal of the organic material or kerogen from the oil shale deposits, according to the process of the present invention, does not appear to affect adversely the remaining crystalline rock or matrix inso~ar as its physical arrangement is concerned. Hence, regardless of the depth of the bed being worked, it is believed that the depleted or spent shale remaining after the microwave extraction op~ration will continue to support the overburden without significant concern for sinking or cave-in of the land thereat. Consequently, even in this respect, ~h~ operation does not appear to disturb the ecology o~ the region in any substantial way.

~3~42~6 Referring to the drawings, and initially to Fig.l, an arrangement 1 is shown on the ground surface 2 of an underground formation 3 of oil shale containing subterranean strata, including a series of levels of barren rock 4 containin~ intervening levels in generally horizontally extending planes of rich oil shale beds 5 and lean oil shale beds 6 of varying vertical thickness and random ordinal sequence downwardly along the depth of the ormation ~, e.g.
starting at an upper level depth of 500 or 600 feet below ground and going down to a iower level depth of llOQ or 12Q0 feet below ground. It will be understood that in certain deposits there may be little, if any barren rock strata whereupon the separate strata will comprise only rich oil shale deposits or lean oil shale deposits.
The rich oil shale beds 5 may, for instance, comprise about 20 or so vertically discontinuouK horizontal beds averaging about 3 feet in vertical thickness separated by low grade or lean oil shale beds 6, the various beds lying in substantially horizontal planes whose deviation from true horizontal is minimali e.g. 1eKS than 1%.
The formation 3 has a bore hole or well bore 7 which has been dri1led in conventional manner to the level of the lowermost oil shale bed from which the carbonaceous material s to be extracted according to the present invention.
Because of the manner of recovering the carbonaceous material from the beds, the bore hole 7 is normally not provided with a casing 8, or at least such casing 8 whera present does not extend downwardly far enough to se21 off the particular oil shale bed being worked from access to the bore hole 7.
Alternatively, the casing 8 may be provided with a plurality of in~low aperture9 therethrough ~not shown~ around its circumference and at least along the lowermo~t: vertical end or extent- thereo~ corresponding in vertical length ~3(~2l36 substantially to the vertical thickness or height of the oil shale beds to be worked to assure recovery of the exuding carbonaceous material from the bed ~ia the apertuxes and into the interior of the casing 8.
Where such a casing 8 is used without apertures, then the casing must be mounted via conventional means (not shown) at the surface 2 to permit it to be raised incrementally from the bore hole 7 so that its lower end or extent is above the particular bed being worked. Similarly, where the casing B
is provided with apertures only at its lowermost end or extent, then it must be mounted by such ~eans (not shown~ to permit it to be raised each time so that its lower end or extent is adjacent with the particular bed being worked for registering its inflow apertures with the adjacent surface portions of the bore hole 3 constituting the bed.
In any case, within the bore hole 7 and/or the casing 8, a delivery or outlet pipe 9 is lowered until its lower end, which is desirably provided wi~th a conventional inflatable sealing collar 10, is just above the bed to be worked.
Attached to the lower end of the pipe 9 is a microwave generator unit 11 such as that disclosed and claimed in said U.S. Patent 4,193,448 to Calhoun G. Jeambey.
This unit 11 contains a lower microwave generating or distributing source 12 (~hown in phantom), and an upper recovery chamber (not shown) which is in flow communication with the bore hole 7 via a plurality of holes throughout its exterior wall circumference and which leads interiorly to an outer concentric flow path at its upper end passing upwardly through the outlet pipe 9 to the surface 2. The recovery chamber i8 separated from the mi~rowave source 12 by a ~uitable internal wall and is arranged to receive oil and gas constituents via the hole~ for recovery via the outer ~3~ 6 concentric flow path in pipe 9.
A~ electrical conductor 13 extends from the surface 2 down through the pipe 9 and unit ll to the microwave source 12 to energize the source in the desired manner. This conductor 13 is separated ~rom the outer concentric flow path within the pipe 9 by an internal pipe or the like (not shown~ containing the conductor 13 and which also extends from the surface 2 to the unit ll, terminating at the ~icrowave source 12.
The pipe 9 is anchored at the surface 2 via a releasable holding mechanism 14 in conventional manner to per~it vertical movement thereof (and/or of the casing 8 where also present) for aligning its lower end such that the unit ll is locatable adjacent the particular bed to be worked and in flow communicating relation therewith whereupon the holding mechanism 14 is locked to maintain the pipe 9 in static suspended state within the bore hole 7.
Then the collar lO is inflated to seal off the area o the bore hole 7 above the collar lO from the area therebelow.
On the other hand, the lower end of the bore hole 7 is per se sealed by the underlying ~arren rock formation thereat.
In this condition of the installation, the microwave unit ll may be operated for heating the oil shale bed and recovering the exuding or emitted carbonaceous material in the form of oil and gas ccnstituents.
Since the borehole section containing the microwave unit 11 is sealed from a~ove by the collar lO and by the closed off end therebelow, not only will the area be sealed off from extraneous air, but the generated and emitted carbonaceous constituents will be readily recovered via the recovery chamber of the microwave unit ll.
The top end of the pipe 9 i8 enclosed by a sealing ~IL3~4Z86 recovery cap system 15 which communicates the outer concentric flow path of the pipe 9 with an oil and gas recovery line 16 leading to a gas separator 17, from which the oil constituents flow via oil line 18 to the oil holder 19, while the separated gas constituents flow via gas line 20 to a gas holder 21.
The electrical conductor 13 passes ~eparately from the cap system 15 to an electrical generator 22 used to generate the electricity for energizing the microwave generating or distributing source 12 in the unit 11.
The cap system 15, h~ldiny mechanism 14 and pipe 9 plus recovery line 16 and electrical conductor 13 are arranged in well known manner for positioning the lower end of the pipe 9 at any given point within the bore hole 7 and for raising the pipe 9 successively from the lowermost point to each next upper point at which a bed to be worked is located, while permitting delivery of power via electrical conductor 13 and product recovery via line 16 during the microwave oil and gas production worXing operation, as the artisan will appreciate.
After a given oil shale b~d has been worked, the portion of the bore hole 7 extending upwardly to the nest successive oil shale bed to be worked is sealed by a cement bore plug 23, thus preventing down10w of any of the carbonaceous constituents from such next above bed and reverse entry into the spent residual shale at the next below bed.
Thi~ operation is repeated successively upwardly along the formation 3 for effectively limiting movement of the e~uding or emitted oil and gas conætituents from a given bed between the ad jacent underlying cement bore plug 23 and ~he overlying collar 10, in the range of the bore hole 7 corre~ponding to the height o the oil shale bed and to the holes in the recovery chamber wall o~ the unit 11.

13~ 136 The ~nit 11, per said V.S. Patent 4,193,448, is able to produce controllable microwa~e planar radiation patterns, i.e.
vertically interposed between levels of barren rock, in an arrangement such as shown in Fig. 1.
Thus, once the bore hole 7 is drilled and the pipe 9 with the unit 11 attached at its lower end is inserted therein and positioned to align the unit 11 with the level of the oil shale bed being worked, the microwave source 12 may be energized to cause microwave radio frequency or RF energy to radiate into the oil shale surrounding the bore hole 7. After all the oil shale beds have been successively worXed, the entire arrangement 1 may be moved to the next hole and the operation repeated.
According to the process of the present invention, the frequency of the radiated microwave energy is selectively matched to the characteristics o~ the rock of the oil shale bed for preferential or selective heating of the carbonaceous material, i.e. organic matter generally in the form of kerogen and providing liquifiable constituents and volatilizable or gas1fiable or vaporizable constituent~. It has been determined that oil shale minerals in the rock or porous impregnated media constituting the oil shale bed absorb relatively little of~the RF energy, so that the organic matter in the pores of the media is preferentially heated.
Since the organic matter occupies more than about one third of the total volume of the rock, e.g. in the case of 30 gpt oil shale, the organic matter or kerogen wlll preferentially ab~orb the microwave or RF energy until the contemplated emitting temperature or pyrolysi~ temperature is reached, whereupon the organic matter decomposes or pyrolyzes, yielding constltuents such as ~lowable or llquid oil, oil ;~3~ 6 vapors, noncondensible gases, some water and a residual solid carbon or coke content in situ in the pores of the mineral or rock media.
As will be appreciated hereinafter, a higher order of magnitude emitting temperature must be subsequently maintained in a second step or stage in order to achieve gasification of such residual solid carbon or coke.
Nevertheless, at this intermediate point or first step or stage, the residual solid carbon or coke generally occupies only about 10 vol.~ of the pore space previously occupied by the organic ma~ter. The void space thus created provides a continuously developing pathway in a direction away from the microwave source and further into the oil shale media for escaplng vapors.
Under the intense pre~erential absorption of the ~F
energy by the organic matter, the liquid oil constituents vaporize and flow along ~ith the other gaseous constituents, including vaporized water, as escaping vapors through the ma~e of these created void spaces. These vapors are forced in a direction towards the bore hole 7 because of the huge volume increase accompanying volatilization of the preferentially heated constituent~ and the consequent attendant autogenous pressure.
It will be reali7ed that the generated vapors have little ability in that form for absorbi~g RF energy, and in~tead progressive production will heat the residual rock, mainly by inherent conduction heat transfer along the created flow paths to the bore hole 7 and this will ensure movement of the vapors to bore hole 7 for recovery via th2 recovery chamber in the unit 11 and the outer concentric flow path in pipe 9.

~3~4~6 Significantly, the RF radiation will be preferentially absorbed by the solid organic matter or kerogen, so as to create in the preferred 360 degree full arc of distributed microwaves, a c~ntinuously expanding ring of organic matter heating around the entire circumference of the bore hole 7 at the level of the oil shale bed being worked. The radial distance this energy is absorbed from the microwave source 12 as center in the bore hole 7 is relatively substantial as noted hereinafter.
However, when that maximum practical distance is reached, which is indicated by the fact that oil production, i.e. the vaporized and gasified organic constituents, e.g.
including gasified residual solid carbon or coke, from a particular bed drops significantly, radiation is discontinued and the production of the operation is terminated.
Such drop in production is a direct measure of the fact that the RF energy penetration has reached its practical maximum distance of heating effectiveness, and in turn that the production limit for that oil shale bed from that bore hole 7 has been reached.
; This maximum radial distance from the borehole, up to which microwaves will penetrate through the oil shale and by selective heatinq in turn cause t~e organic materials present to be released or emitted from the rock or mineral matrix in practical quantities, is normally ealled the recapture radius.
This recapture radius is a direct function of the microwave power input, and thus may ~e selectively increased by correspondingly increasing the level of microwaYe power applied to the formation.

13~ 2~36 After the final products have been removed from the bore hole via the pipe 9, the production equipment, including the unit 11, is pulled from the bore hole 7, the bore hole is plugged just beneath the next oil shale bed thereabove, as earlier described, and the production operation repeated until all oil shale beds in turn are developed or worked from the same bore hole 7.
When the oil production from the last or uppermost oil shale bed has been completed, the production equipment, including the unit 11, is withdrawn permanently and the bore hole 7 is surface sealed in conventional manner to minimi~e post development or post extraction environmental effects of the production operation. Then, the entire operation may be repeated at the next bore hole.
During production of a given oil shale bed, the oil vapors, water and noncondensible gas may be under sufficient autogenous intérnal pressure as created by the RF energy heating to cause these constituents to drive themselves via the pipe 9 to the surface 2, or surface pumping may be required in conventional manner, depending on the nature of the carbonaceous material and the type and condition of the oil shale bed, as well as upon the temperature to which the constituents are heated and the point in time and/or proximity to the outer limit o the recapture radius of the particular operation.
In any ca~e, as aforesaid, the radiation zone within the bore hole 7 and the pipe 9 at the level of the oil shale bed being worked i~ isolated by the inflatable collar 10 or other removable packer, in conventional manner, and this prevents air in the bore hole 7 thereabove from mixing with the exuding or emitting ga~e~ and oil entrained therewith ~1 ~3~2~36 which enter the bore hole 7 from the surro~nding oil shale bed. This insures that the in situ microwave radiation pyrolysis is carried out in the substantial absence of air according to the present invention.
On the other hand, at the surface 2, the product stream pzssing through the cap system 15 is condensed in conventio~al manner, as in the gas separator 17. In this way, the normally liquid oil constituents and attendant water are conden~ed from the non condensible gas constituents, enabling the latter to be separated via line 20 and passed to the gas holder 21 for further work up, e.g. stripping any attendant hydrogen sulfide from the gas in the usual way to remove this undesirable noxious constituent (by means not shown), prior to use of such recovered noncondensible gas.
Advantageously, according to the present invention, at least a portion of the remaining gases after 6uch work up is desirably used to generate power for operating the microwave generating or distributing source 12. For this purpose, such gases are fed via feed line 24 from the gas holder 21 to the electric generator 22, which may be a conventional gas operated generator or fuel cell (e.g. l-KW Raytheon).
Under the prevailing or selectively adjusted pyrolysis condition~, the noncondensible gas produced from the operation will normally provide sufficient available energy at least to support the power requirements of the microwave generating ~ource 12 and collateral surface e~uipment as well.
A~ to the normally liquid oil constituents and condensed attendant product water which accumulate in ~he gas separator 17, these may be passed via oil line 18 to the holder 19, where the oil may be readily ~eparated ~rom the product water in conventional manner, e.g. by phase ~2 ~3~4;286 separation, and re-covered as a commercially useful oil product, i.e. shale oil.
Alternatively, the gas separator 17 or other auxiliary means (not shown~ may be operated to cause the condensed product water to settle as a b~ttom liquid phase under and upper liquid phase of the condensed oil vapors, enabling the latter to be suitably tapped off by phase ~eparation technique via oil line 18, while the noncondensible gas is recovered via gas line 20 as before. In this case, the product water will be separately tapped off via a bottom line (not shown~ from the gas separator 17 or such other auxiliary means.
In any case, the separated product water may be disposed of in any convenient manner, such as by disposal in an evaporative tailing pond, whereas the produced oil will normally require some clean up before marketing, since it will generally contain ~itroyen plus other factors or constituents which should be removed, as the artisan will appreciate.
On the other hand, any potable water requirements may be met in the field by simply sinking a water well in the vicinity of the operation, since in the usual instance the formation will contain an artesian aquifer or water bearing ~tratum about 200 feet below the shale beds from which ~resh water is readily obtainable. These potable water requirements, of course, only concern those for personal use since, except for optional cooling of operating equipment, the proc S8 of the present invention requires no water, which i a ignificant environmental and economic advantage.
More important, the product water obtained i~ not extraneous to the region but repre ents a constituent indigenous to the very formation being worked and i9 extraoted from oil shale strata originally overlying the pre-existing ~3~ZI~

pure water in the artisian aquifer or water bearing stratum normally present about 200 feet therebelow.
Obviously, achievable oil and gas production varies in direct proportion to the raaius of RF energy penetration into the oil shale bed from the microwave source 12 in the bore hole 7. To maximize this radius, major RF power must be provided.
On the other hand, the use of such high power initially is not desired because full initial application of such high RF power might lead to detrimental effects upon the immediate area ~urroundin~ the bore hole 7, e.g. rapid expansion of the constituents as they pyrolyze, and in tur.n eventual expansion of the rock or mineral matrix or media itself as the pyrolysis progresses farther into the bed and the hot vaporized and gasified constituents continuously flow under autogenous pressure to that immediate area surrounding the bore hole 7 for recovery via the holes in the unit 11~
This could cause the adjacent areas of the bed to disintegrate, such that collapsing rock portions might trap and/or crush the unit 11, as where no casing 8 is used in the bore hole 7 or where its lower end terminates at some point above the level of the oil shale bed being worked.
It would, in any case, cause fluctuating conditions, detracting from the uniform production rate of oil and gas constituents under the applied microwave power levels, as fundamentally desired according to the present invention.
Hence, it is instead co~templated that the oil production or microwave heating extraction operation be carried out such that variabl.e RF power is selectively applied, e.g. beginning with a lower level o RF power and increasing that level an penetration progresses. In this way, ~3~3~2~

undesirable local overheating of the porous media, e.g. shale, ln the vicinity of the bore hole 7 will be avoided. Of course, this avoidance of local overheating will be reinforced by preferred use initially of intermittent i~ter~al cycles of on and off duration selective microwave power as noted below.
Commercial production by microwave heating via the borehole technique, requires the drilling of many boreholes, and installation and operation of the pertinent surface and underground equipment at each, in successive manner from the lowermost to the uppermost oil shale bed after preliminary plugging of the borehole portion at the underside of the particular bed next to be worked. Production equipment costs will, of course, decrease sharply as radius production increases, and this depends on the depth of radial penetration of the RF power, and ~n turn on the maximum efficient level of such power, relative to a given type of oil shale bed.
Por instance, generally at a 12 foot production radius, about 48 production boreholes per acre will be required, whereas at a 20 foot production radius, about 17 productio~
boreholes per acre will be required, at a conservative 50~
borehole density per acre to prevent overlap with the shale bed portions of the neighboring boreholes at the bed level being worked.
In this regard, since there are 640 acres per s~. mi.
or per 27,878,400 ft.2, and thus 43,560 ft.2 per acre (~7,878,400/640):
for a 12 f40t production radius the area per borehole amounts to 452.57 ft.2 (12 x 12 x 22/7~, which at a 50%
borehole density correspond~ to 48 boreholes per acra (50% x 43,560/452.57), and for a 20 ~oot production radiu~ the area per borehole ~3~ 36 amounts to 1257.14 ft.~ (20 x 20 x 22/7), which at a 50%
borehole density corresponds to 17 boreholes per acre ~50% x 43,560/1257.14).
Indeed, even at higher borehole densities, since the previously worked neighboring borehole areas of the beds will have been provided with cement plugs 23, any vaporized and gasified constituents at the outer portions of the bed radius then being worked, which may migrate into the radius o~ an already worked borehole area, will be prevented by such plugs from leaving the distant reaches of the bed and ~rom decreasing significantly in autogenous pressure, such that maximum recovery will still be achieved via the borehole being then used.
This may be aided by suction pumping of such constituents via the outer concentric flow path within pipe 9 in conventional manner ~by means not shown~.
Concomitantly, because of the plugging along and surface sealing of all neighboring boreholes, undesired access of extraneous air to the site being worked by seepage through the formation from such neighboring boreholes, especially under such suction pumping conditions, will be advantageously avoided.
More important, because of the general impermeability of the unheated perimetric boundaries o~ the given recapture radius outer limits at each borehole being worked, and the avoidance of overlap among tbe r capture radiu~ outer limits of neighboring boreholes, the generated gases will be prevented from migrating away from the borehole being worked, norwill any extraneous source of air be able to reach the pyrolysi~ range thereat from a point beyond such recapture radius.

~3~gZ8~

Regardless of the length of the prod~ction radi~s utilized, it will be appreciated that the oil production rates from each like type oil shale bed along the relatively shallow depth being worked tend to xemain fairly constant, e.g.
r~nging from about 10-15 barrels per day for rich oil shale, under a controlled application of the selected RF energy.
It will be seen that the borehole equipment and surface equipment are recoverable and reusable at the next borehole, except for the upper borehole casing 8 which where used is ordinarily left in place. The operation lends itself to the carrying out in the field of the various surface operations, including gas ætripping, hydrogen sulfide extraction, power generation, water removal from the recovered oil, water treatment for di~posal, or even reuse for instance in part as closed cycle cooling water for various operating equipment such as the field electrical generator 22, and oil treatment and temporary storage prior to transport for marketing.
Particular environmental advantages of the process according to the present invention, which immediately suggest th~mselves include:
1. The avoidance of apparent or obviou~ terrain changes since mining is not used and the boreholes are plugged after use.

2. The ability to ætrip and recover in the field by conventional means the hydrogen sulfiae present in the gaseous fraction of the recovered constituents.

3. The avoidance of disturbance to water aqui~ers present in the formation being worked since water i3 not required for carrying out the extraction operation, and at most minimal coolant water i~ needed which can be recycled in a closed system.

4. Labor requirements are not intensive, but instead are minim~l and thus minimize socio-economic impact in the area.

5. The avoidance of surface or air pollution since the pyrolysis decomposition occurs underground, in the absence of air, and the decomposition product~ are recovered ana processed on the surface in a closed piping system, and the commercial products and by products obtained are of no cJreater risk than those in general, consequent analogous industrial endeavors.
Figs. 2a and 2b show conditions under which the microwave radiation pyrolysis of oil shale may be carried out according to an embodiment of the present invention at a formation installation of the type indicated in Fig. 1.
One set of operating parameters, wherein the recapture radius is about 38 feet relative to ~he borehole 7 at a given oil shale bed or stratum ~Fig. 1), and in which the microwave distributing source 12 of the unit 11 is arranged for distributing the RF radiation throu~hout a full 360 degree arc, is set forth in the following Table ls TABL~ 1 Radiu~ ~otal Fram ~i~rowa~e ~eati~g CyclesC;rcular Ri~ Borehol~ P~r ~wer Interval~Area 11 ft.5~000 ~at~s 1 sec. on/3 ~ec. off 3.14ft2 23 ft.7,500 ~att~ 1 ~e~. on/2 ~ec. off 28.29ft2 35 ft.10,000 ~a~t~ 1 se~. on/l ~ec. off 7B~57ft2 47.5 ft.15,000 watt~ 2 ~e~. on/l se~. off 176.79ft2 59.6 ft.20,000 watt~ 3 ~c. onll ~ec. off 28~.65ft2 612.2 ft.30,000 watts 4 Be~- on/l sec. of 491-07ft2 715.0 ft.SO,OOO watt~ 5 ~. on/l sec. off 707.14ft2 819.S ft.7~/000 watt~ 6 sec. o~ e~. off 1,195.07ft2 g38.0 ft.100,000 watt~ constant o~4,538.2~ft~
*Power/time rates may vary depending upon characteristic~ of deposit.

4~

Considering the values given in Table 1 with those shown in Figs. 2a and 2b, it is seen that i~ the first annular ring of oil shale around the bore hole, the 1 foot radial distance of oil sha~e is subj~cted to 5,000 watts (5 KW~ of microwave power in input time heating cycles of 1 second on and 3 seconds off duration intervals for heating the annular ring area of 3.14ft2 (ignoring as relatively insignificant the area represented by the borehole itself), during which time the carbonaceous constituents or carbon content in the porous shale rock or mineral are preferentially heated, relative to the generally microwave transparent and thus not preferentially heated mineral content, such that the carbon content in the first ring progressively heats up to about 425C.
As the heating progresses in a direction away from the borehole, the next 2 feet of radial distance of the oil shale -in the second annular ring along with the 1 foot of the first ring, totaling 3 ~eet rad~al distance, is then subjected ~o ~, : 7,500 watts of microwave power in heating cycles of 1 second on and 2 seconds off duration i:ntervals for continued : progressive heating of the now 28.29ft2 cumulative first and ~econd annular ring area, such that the att~ndant carbon ~.
~:~ content increasingly heats up to about 450~C preferentially : ~ relative to the mine~al content.
In turn, the next 2 feet of radial distance in the ~ third annular ring, along with the previous 3 feet of the : ~ first and second annular rings, now totaling 5 eet radial : di tance, is eubjected to 10,000: watts of microwave power in heating cycles of 1 second on and 1 second o~ duration intervals for ~urther progressive heating of the now 78.59 ft2 cumulative first, second and third annular ring area, such ~9 ~31Q~2~i that the attenda~t carbon content increasingly heats up to about 475C preferentially relative to the mineral content.
This progressive and incremental heating of the successive annular rings of oil shale continues in accordance with the conditions given in Table 1 and as shown in Figs. 2a and 2b, until the ninth successive annular ring is reached at a recapture radius of 38 feet and embracing a c~lmulative total oil shale area of 4,538~29 ft2, during which time the mic~owave power is increased fxom 75,000 watts in heating cycles of 6 seconds on and 1 second off duration intexvals, per the eighth successive annular ring, to constant on power at 100,000 watts (100 KW), such that the attendant carbon content increasingly heats up to about 500C preferentially relative to the mineral content.
Of course, these radial distances are not critical, and similar results are obtained where the third ring has a 4.5 ft radius, the fourth ring has a 7.2 ft. radius, the sixth ring has a 12.5 ft radius, and the eighth ring has a 20 ft.
radius, all at corresponding concordant total circular areas for the 360 degree full arcs of distributed microwaves applied thereto.
Thus, the microwave power is incrementally, though nonuniformly, increased with incrementally, though non~niformly, increasing radial distance from the borehole and conjointly increasing total circular area subjected to the heating RF energy. At the ~ame time, until the microwave power is switched to constant on duration at the ninth æuccessive annular ring, the heating cycles progressively increase in the duration intervals of on time (power on) and correspondingly progressively decrease in the duration intervals of off time ~power off), the on time intervals actually being constant for ~3~4Z8G

the first three annular rings at 1 second and then uniformly increasing to 6 seconds for the eighth annular ring, while the off time intervals uniformly decrease from 3 seconds to 1 second for the first three annular rings and remain at the 1 second off time intervals through the eighth annular ring.
As may be appreciated from the shaded area of Fig. 2b, during the operation the cumulative oil and ga~ production quantity progressively in~reases and this, of oourse, is a function of the increasing total circular area around the borehole (cf. Fig. 2a) being subjected to the microwave heating energy, as listed in Table 1. Indeed, the actual quantity will depend on the width or vertical height of the oil shale bed or stratum being worked, such that for the sake of illustr~tion, the quantity of cumulative oil and gas produced from a 1 foot high bed section being worXed will be roughly one tenth that from a 10 foot high bed section being worked, i.e of the same total circular area or recapture radius As also indicated in Fig. 2b, the temperature of the carbon content in the bed area being worked progressively incrementally increases as well from a roughly minimum ~;~ production temperature of about~425~C at intermittent power eventually to about 500-C at con~tant power, the magnitude of such power o~ course progressively increa~ing as well, anderstandably, from a low level of 5 kilowatts to a high of 100 kilowatts.
Neverthele~s, under the controlled conditions of progressively increasing power, first at intermlttent on and off duration intervals and subsequently at constant on duxation or condltion, along the radially increasing distance rom the borehole, the production rate may be selectively ~3~
maintained constant, even though the total quantity of produced oil and ga~ cumulatively increases (cf. Fig. 2b).
A similar set of operating pa~ameters, wherein ~he recapture radius is about 30 feet relative to the borehole 7 at a given oil shale bed or stratum (Fig. 1), and in which the microwave distributing source 12 of the unit 11 is arranged for distributing the RF radiation throughoLIt a full 360 degree arc, analogous to the opera~ing parameters of Table 1 and the features shown in Figs. 2a and 2b, is set forth in the following Table 2:
TI~ 2 Radius ~ro~ Mi~rowa~e ~eating Cycleæ
Borehole Po~er Power InterYal3 1 1 ft.5,000 watts 1 ~ec. o~/3 sec. off 2 2 ft.7,500 ~atts 1 sec. o~/2 ~ec. off 3 3 ft.10,000 ~att~ 1 ~ec. on/l sec. off 4 5 ft.15~000 ~atts 2 sec. ~n/l sec. off 10 ft.20,000 ~tts 3:~e~. o~/3 sec. off 6 20 ft.50,000 ~atts 3 sec. o~2 sec. ~ff 7 30 ft.100,000 ~att~ 3 ~e~. on/l ~ec. off For increased production, the recapture radius may be extended, as in the case of Table 1, by continuing the microwave distribution at constant on power at lOG,000 watts, after the 30 foot radial distance of the seventh annular ring has been reached.
Of course, higher levels than 100,000 watts of RF power may be u~ed, as and if desired, as the radial di~tance approaches the outer limits of the recapture radiu~, depending on the actual shale conditions encountered, as the artisan will appreciate. Nevert~eless, a fundamental purpose of the process of the present invention is to maximize recovery of the oil and gas constituents in the particular petroleum impregnated porous media such as oil shale at correspondin~ly minimum expenditure of RF power.

~ 3~4~86 The RF power may be suitable applied at a frequency ranging, for instance, generally between about 10-2000 M Hz, or more, as desired. This high frequency electrical energy or microwave energy, which is generally in the radar range, is thus capable of being directed into the vil bearing strata considerable distances for accomplishing the pyrolysis extraction of the carbonaceous values present substantially completely throughout, due to the relatively low dielectric loss factor of the petroleum fluids which thereby act to conduct, or tr~nsmit, the microwaves rather than to attenuate them.
The advantage of this fact is striking in that the well may be pumped, i.e. the generated liquified and/or gasified constituents passing radially to the microwave unit 11 in the borehole 7 and in turn upwardly through the outlet pipe 9 may be withdrawn by pump means (not shown~ at cap system 15 (Fig. 1), as and if needed, at a higher rate with less adverse effect on the transfer of the high frequency electrical energy through the oiI and ga~ constituents in the bedding being worked than otherwi~e and such is not in any way impaired by gravity.
It will be realized that, due to the advantageous preferential or selective heating of the carbon content of the oil shale, and the apparently inherent general transparency of the mineral content thereof to mi~rowaves under the contemplated operating conditionst the total energy expended In providing for the microwave heating of the oil ~hale for the production of the carbon content thereof a5 recoverable oil and gas con~tituents, according to the pre~ent invention, is ~ignificantly le~s than that required in otherwise retorting the oil ~hale in ~itu by conventional means, whether 3~L2~6 in the presence of eontaminating combustion air which consumes a large proportional quantity of such carbon values as direct so~rce for providing the necessary heat, or in the absence of air using an indirect, and thus less efficient, source of heat.
This is because, according to the present invention, the relatively heavy mass of rock constituting the mineral content of the oil shale is not heated to any pertinent extent by the microwaves, whereas the carbon content is selectively inherently heated thereby. Of course, as the oil and gas constituents are generated under the applied microwave heating, a certain amount of indigenous sensible heat taken up by the liquified and gasified constituents of the in situ carbon content of the oil shale will be given ~p in turn to the surrounding mineral content by direct contact conduction transfer and perhaps also by normal heat transfer radiation~
However, the amount of such heat lost to the mineral content of the in situ rock of the oil shale formation will be substantially less than that imparted thereto per the conventional in ~itu retorting operation, whether carried out by direct combustion in air or by indirect heating using an extraneous and inefficient indirect heating xource, since in the conventional retorting operation the entir~ mass of the oil shale must be heated grossly, i.e. by bulk heating, with lit~le control, whereaæ by way of the process of the present invention primarily only the carbon content of such mass is preferentially or selectively heated and in controllable manner.
Thi~ differential heat 6aving is true even considering that energy must be expended in order to provide microwave power for the in situ pyrolysis o~ the oil shale or other ~3Q~86 petroleum impregnated porous media according to the present invention, hecause only a limited portion of the energy otherwise needed is involved in supplying thl microwave power.
More important, since inherently due to the make up of the carbon content in the oil shale or the like, a significant q~antity of the pyrolysis generated constituents will be in the form of gasified constituents, of which a pertinent portion will necessarily exist as noncondensible gas (which portion may be increased by controlli~g the pyrolysis conditions according to the process of the present invention), that portion alone may serve as by product energy source for generating the required microwave power without reducing the otherwise primarily sought oil product.
In this regard, the primary form in which the carbonaceous values represented by the carbon content of oil shale exists is kerogen. Oil shale, as aforesaid, may be regarded as a sedimentary rock having a relatively high organic content, i.e. kerogen, which may amount to roughly about 30-60% volatile matter and fixed carbon, such that when appropriately heated in the absence of air it gives up an oil.
Depending on its location, oil shale may yield from 20- S~ gpt of crude oil which general possesses a relatively olefinic type unsaturated nature compared to the typical petroleum obtainea by drilling methods.
As between microwave or RF heating of kerogen and conventional conductive heating t~ereof, it will be appreciated that in either case, kerogen must be h~ated to at least about 4~5C before pyrol~sis thereof will occur. Once this threshold temperature is reached, pyrolysis of the kerogen will oc~ur within time periods on the order of one second or le~s.

~3~ 8~i Electromagnetic e~ergy in the form of microwaves or radio frequency (RF) waves is quickly radiated into the oil shale, which is, as aforesaid, essentially transparent to RF
waves, and upon contact with the RF absorbe~t kerogen quickly reaches pyrolysis temperature, whereby to carry out the production process according to the present invention.
In contrast thereto, conventional bulk heating methods dspend upon the thermal conductivity of oil shale, which is low. Its thermal conductivity is about 000017 cal/cm3/sec./C
and drops to roughly half this value at 425C.
Thermal conductivity may be regarded as the capacity for conducting heat, e.g. expressed as the number of calories passing per second through a plate of 1 cm2 area and 1 cm thickness and having its opposing faces at a 1C dif erential t mperature, or alternatively expressed as Bt~/hr/ft2/F/ft of thic~ness of a given material.
From the foregoing, it is clear that RF heating of oil shale is significantly faster and thus consumes comparatively low orders of magnitude of energy. Conversely, conventional conductive heating time for bulk heating of oil shale is in the order of hours before pyrolysis can occur.
Typically, dolomi~e is the largest mineral component in oil shale and occupies only about 21 vol. ~ of the rock volume, the remainder being other mineral components plus the organic matter. Representative oil shales have the following appro~imate organic matter and mineral matter volume ratios:
23.5 gpt oil shale - 29 Yol. % organic matter: 71 vol. ~ mineral matter 25.0 gpt oil shale - 30 vol. ~ oryanic matter: 70 vol. % mineral matter ; 30.8 gpt oil shale - 36 vol. % organic matter: 64 vol. ~ mineral matter 46.2 gpt oil 8hale - 47 vol. ~ organic matter: 53 vol. % mineral matter.

~3~Z~36 As regards formation materials, other than the organic hydrocarbon consti~uents present, which might possibly absorb micro~ave ener~y, these generally include the silicates such as quart~, soda feldspar and potash feldspar, and the carbonates such as dolomite and calcite, which make up most of the mineral content in oil shale and which are rela~ively transparent to microwaves, plus water and prior to it5 gasification also the residual carbon or coke which remains in solid form after the volatilizable and gasifiable organic constituents have been pyrolyzed.
Water clearly absorbs microwave energy, and is usually present in the formation as compositional water since oil shale beds are generally impervious to ground water. This compositional water, Eor the most part, exists either as water of crystallization in the aæsociated mineral matter or as clay hydroxyl (0~) type water mostly in the form of analcime, which is the only hydrate normalIy found in any quantity in the contemplated oil shale deposits.
Analcime, or analcite, e.g. NaAlH2Si207, may be regarded as an isometric native sodium aluminum silicate zeolite, and its derived water will be volatilized from the analcime crystal under the microwave heating.
Illite clay, which also contains hydrosyl groups, is likewise often present in oil shale along with analcime, and its water content will be released under the microwave heating ~u~t as in the ca~e of analcime.
Moreover, iron constituents in the associated mineral content ~uch as pyrites (FeS2) will add to tho~e materials which, to the extent present, will absorb microwave radiation, in the case of pyrites probably leading under the pyrolysis conditions to the reaction thereof with the organic matter ~1.3~ 6 present to produce hydrogen sulfide (H2S). Generally, iron also occurs in the ubiquitous dolomite and widespread magnesium iron carbonate called "ferroan", which are usually present in oil shale deposits.
Thus, allowances must be made for absorption of some of the applied microwave energy in driving off water of crystallizatio~ and hydroxyl derived forms of water from the associated mineral content in the formation, as well as in the heating of iron constituents such as pyrites and ferroan which may also be present.
~ aturally, the amount of RF energy expended in these instances, as compared to that used for extracting the carbonaceous values sought, will vary as the amount of such RF energy absorbing noncarbonaceous constituents varies for a given type formation deposit, and thu the heat loss involved wilI concordantly vary, but its m~agnitude will be relatively-low compared to the magnitude of RF energy desirably pre~erentially absorbed by the carbonaceous constituents.
Theoretically, an additional RF energy heat loss may occur by heat transfer to the~tiny mineral crystalc which are often intimately intermixed with the organic matter in situ in the deposit. ~he size of this effect is impossible to estimate, and to the extent lt may exist will cimilarly vary with the~nature of the given deposit.
Because of tha relatively low thermal transmi~sivity of both the organic mattex and the mineral matter, the actual heat transfer effect of this possible source of heat loss in the intimate "oil" and "shale" or mineral component mi~ture, to the extent that it may exist, will nece88arily be correspondingly less than that equivalent to bulk heating or gross heating of the ma~ by way of conduction heat transfer, ~4~

and may be regarded as minimal or insignifica~t.
As to the actual mechanism by which the organic matter is extracted d~ring the microwave pyrolysis, it is belleved that as the organic matter, such as kerogen in oilshale, is heated by absorption of the microwave energy, its internal bonds begin to break, thereby generating additional e~citable -sites in the particular molecule, e.g. hydrocarbon, at which ~.ore energy is in turn absorbed s~ that the organic matter becomes fluid, with the process increasin~ with increasing temperature.
As the temperature rises to the point where the carbon-to-carbon bonds start to break indiscriminately, the absorption rate accelerates markedly until the organic matter is totally decomposed and oil vapor and noncondensible gas are produced.
Because of the way that the radiant energy is applied -and because of the slight delay inherently initially imposed by the internal back pressure generated in the pores of the porous media, the volatiliæation must proceed into the shale or other porous media progressively incrementally from the microwave distributing source.
Consequently, the generated oil vapor and noncondensibla gas, because of tha hage increase in volume as representad by such constituents in now gasified form within the surrounding pores and their corresponding huge decrease in density, e.g. as compared to solid form kerogen, these gasified constituents will drive themselves out of the rock or ~hale under autogenous pressure, i.e. in reverse direction to the microwave direction, and thus toward the microwave unit 11 ~Fig. 1) in the borehole or eventual recovery.
Hydrogen and methane are the two major ~uel ~ases given ~3~

off when oil shale is heated and, as earlier noted, these gases in particular assist the oil flow within the shale toward the bore hole due to their high relative volumes.
Once the various constituents are gasified and proceed under autogenous pressure out of the roc}c, they will stop absorbing further microwave energy, on the one hand because their pyrolysis breakdown has been sufficiently completed to the extent consistent with the microwave energy level applied and the corresponding temperature, and on the other hand because the pote~tial for further absorption of microwaves is reduced as the~e constituents become converted from solid and/or liquid form to pyrolyzed condensible and/or noncondensible gasified form.
In turn, under the continuous progression microwave heating, in effect the microwaves then excite the next layer of organic matter now exposed by gasification removal of the previous layer. Since ~hale oil is generally nonhomogeneous in nature, it is not believed that as the organic matter is heated at a given level or frequency, e.g. about 100,000 Hz (0.1 MHz), the liquid oil which forms absorbs the microwave energy at the given frequency, i.e. such that the nonhomgen~ou~ liquid oil would absorb energy at a specific frequency.
Instead, it is believed that any change in absorption rate reflects the change of the constituent makeup of the organic matter from nonhomogeneous to homogeneou~ nature, as represented by the incipient formation of carbon coke, i;e.
re~idual carbon in solid fixed form which constitutes a uniform material.
Hence, the microwave frequency may be selected for controlling the absorption rate for maximizing the energy ~31~4Z8~

absorption at minimum energy expenditure during the course of the pyrolysis operation.
In this regard, it has been demonstrated that the loss tangent (which is an index of the ability of a given material to absorb electromagnetic radiation energy) increase by a factor of 6 as shale richness increases from 10 gpt to 76 gpt.
If the oil yield is used to calculate the volume of the organic matter in the rock, the relationship between the loss tangent ana the volume of the organic matter is nearly linear, ana thi~ constitutes a strong indication of effectivP and thus preferential absorption of microwave energy by the organic matter.
As earlier noted, typically 23.5 gpt oil shale contains 29 vol.~ organic matter, 25 gpt oil shale contains 30 vol.%
organic matter, ~0.8 gpt oil shale contains 36 vol.~ organic matter, and 46.2 ypt oil shale contains 47 vol.% organic matter, and this is consistent with such nearly linear relationship between the loss tangent and the organic matter voIume.
It has aIso been demonstrated that the energy absorption by the organic matter in the oil shale is fairly con~tant over a wide range of micr~wave frequencies, since it has been indicated that the dielectric constant (to which the 108s tangent contributes) lS relatively stable over such wide range of fre~uencies.
On the other hand, that the mineral matter in the oil ~hale has only a limited ability apparently to absorb microwave energy, is indicated by the fact that the nearly linear relationship between the lc9~ tangent and the organic matter volume in the o~l shale could not exist if the mineral matter absorbed RF energy radiation to any signiican~ extent.

~3~4Z~36 As an obje~tive collateral vbservation, in this regard, it may be noted that the relative transparency of well crystallized silicates and ceramics to microwave radiation is confirmed each time one uses a kitchen rnicrowave oven.
Hence, the preferential or selective absorption of the microwave energy by the organic content to the relative exclusion of the mineral content in the rocX is demonstrated in terms of tl) the relative volume of the organic matter in concordance with the gpt yield on heating or retorting, ~2) the ability o~ the organic matter to absorb and be e~cited by microwave radiation as shown by the rise in the loss tangent with increase in the gpt yield richness of the oil shale, and (3) the conversely limited ability of the mineral matter to absorb microwaves consistent with the showing per point t2).
In fact, it has been shown that there i~ a marked increase in loss tangent at the contemplated pyrolysis temperatures, and an absorption peak has been detected at these temperatures at about 100,000 ~z, which could only occur from the generation of a new absorbing material. Because of the nonhomogeneous nature of the liquid oil generated by the pyrolysis, such absorption peak would not appear to be explainable by the liquid oil being able to absorb ~he RF
energy at a specific frequency, but instead is consistent with and e~plainable by the attendant formation of the residual carbont i.e. in the form of carbon coke, which is a uniform material seemingly capable of showing a frequency peak on absorption, as earlier discusaed.
Since the loss tangent dropæ off after such absorption peak, which increasing frequency, th~s provide~ a means for controlling the microwave energy 90 that optimum frequency of the RF radiation may be applied for optimum or maximized ~3~ 6 heating of the residual carbon at minimum expenditure of power per unit time, i.e. in the second step, according to the process of the present invention.
In general, therefore, according to the process of the present invention, volatilization or gasification of the organic matter as oil vapors, water vapors and noncondensible gas, under the contemplated pyrolysis conditions in the first step, will typically remove about 80% of the original ~eight and 90~ of the original volume of the in situ organic matter, e.g. kerogen in the oil shale, assumin~ that the residual carbon or solid ~i~ed carbon coke remaining after such gasification has a density of 2.
This i~ consistent with the fact that amorphous elemental carbon has a denslty around 2, while that of graphite is around 2.25 and that of diamond is around 3.5.
Of course, if the oil shale rock has a continuous phase in it, the contained organic matter will be in continuous phass .
As far as the first step is concerned, as volatilization or qasification of the organic matter proceeds into the rock fr~m the irradiated surface, i.e. in a direction away from the microwave source in the borehole, the incrementally vanishing organic volume will create the ~ontinuously growing network of tiny holes in the porous media for inherently providing egress routes for the gases created by organic decomposition and e~isting under autogenous preqsure at the contemplated pyrolysis heating temperature.
Since the~e ga~e~ must flow directly through the microwave radiation, there is little likelihood that the oil vapors can either condense or absorb further radiation energy, but even if ~uch were to occur during travel to the borehole, ~il3~

the resulting recondensed liquid oil constituents would again become centers for further microwave absorption and in turn be revolatilized.
Once the ensuing second step has been carried out to remove or scavenge essentially all of the remaining residual carbon by higher temperature gasification to noncondensible gas form (primarily carbon monoxide), the oil shale or other porous media will represent a spent rock containing empty internal spaces, which understandably will have lost some structural strength due to removal of its in si~u supporting organic matter, although there will be little if any change in its mineral content integrity in view of the fact that the mineral matter is generally transparent to microwave penetration and will have only experienced minimal heating by way of normal conduction, and possibly also normal radiation (as distinguished from microwave radiation), heat transf~r.
Naturally, the remai~ing strength or residual strength o~ the porous media will vary inversely with the volume of organic matter initially present in the rock and which has been excavated or remove2 by the pyrolysis. While this removed volume of organic matter will constitute the primary influence on the strength reduction of the spent porous media or rock, other factors may contribute thereto, and particularly the e~tent to which mineral reactions also occur during the heating, including loss of compositional water, formation of hydrogen sulfide from pyrites which may be present, modification of other iron constituents in the mineral, etc.
For instance, in shale yielding ~0 gpt, organio matter removal leaves a porous or hole ridden rock virtually as strong compressively as the initial rock. Its dolomite ~3~2~i framework for~s a competent structure. In shale yielding 38-42 gpt, the dolomite framework may be so dispersed by the large collective volume of organic matter that the residual rock after organic removal has virtually no compressive strength. Shale grades in between these two types retain some but not all of their compressive strength on removal of the in situ organic matter.
Ultimate compressive strength of 20 gpt shale perpendicular to the bedaing planes in the formation is about 18,000 psi, and for 42 gpt (i.e. 1 barrel per ton) it is about 13,000 psi. Although the residual compressive strength of 20 gpt shale is about 15,000 psi, the roughly 40% volume loss of 42 gpt shale makes precise determination of residual compressive ~trenqth thereof impractical. Of course, the intermediate 30 gpt shale will retain some residual compressive strength.
Since generally the apparent failure pressure seems substantially larger than the over burden pressure in the formation, based on extrapolation, the probability is that the residual strength of the average shale encountered, e.g. 30.8 gpt shale, will be adequate after the extraction to provide sufficient overburden support. Consequently, as in known methods for in situ recovery of the carbonacaous values in petroleum impr@gnated porous media, e.g. using steam or hot water, removal of the organic material, such as kerogen from oil shale, by in ~itu microwave heating in accordance with the process of the present invention will not affect adversely the remaining crystalline rock, and regardle~s of the depth of the petroleum containi~g bedding in the underground formation being worked the petroleum depleted rock ~hould adequately support the land or ground ~ur~ace without sinking or cave in ~31~Z86 .

occurring, and thus without disturbing the ecology in any way from this possible source of undesirable environmental imbalance.
Based on performed tests carried DUt with oil shale subjected to RF or microwave heating, the kerogen breakdown of constituents upon progressive heating is shown in the following Table 3:

T~BLE 3 ~em~perature _ Con~tituent~ Generated -- ~

Pyrolysis begins: 425C (797F) 85~ Oil - g% Gases - Total 94%
450C (842F) 82~ Oil - 11% Gases - Total 93 475C (887DF) 80% Oil - 15% Gases - Total 95%
500~C (9~2F) 75~ Oil Vapors-20% Gases-Total 95%

-:~ Residual carbon: 525C (977F) Carbon coke gasifies 600DC ~1112F) Water forms It is believed that the water which forms is not so much traceable to bound molecular water in the mineral content of the oil shale, but rather to oxygen present in bound mineral carbonate form in the mineral content which under the high localized heating temperature of 600DC releases carbon dio~ide which reacts with the comparatively rich hydrogen content of the Xerogen or its generated organic constituent products, e.g. ~ethane, ethane, etc., to form carbon monvxide and water by way of an undesirable heat consuming endothermic reactionD

~3(:! 4z1~36 To the extent that this may occur, it not only expends the microwave energy unnecessarily, but also consumes valuable hydrogen and carbon, otherwise available as markPtable hydrocarbon constituents. Instead, it ma:nufactures in situ, even in the absence of air, not only reactlon water of no commercial value and representing a contaminant ~y-product which must be disposed of, e.g. by way of an evaporative tailing pond, but also more importantly, oarbon mono~ide as a by-product of comparatively low heat value, along with attendant increased:amounts of gas diluting carbon dioxide released from the indigenous mineral carbonate present and not so reacted to form carbon monoxide at ~uch 600C temperature.
Hence, by maintaining the distribution of the microwave energy Ruch that the temperature remaine below about 600~C, not only is the amount of carbon dioxide released from the inaigenous mineral carbona~te present in the ~il shale suppressed or minimized, but also that reduced amount thereof which is relea~ed at temperatures below 600C will be less prone to endothermic reaction with the comparati~ely rich i hydrogen content present, e.g. in the hydrocarbon generated oil and gas constituents, such as methane, ethane, etc., to :~ form carbon monoxide and water.
Of co~rse, at such lower temperature, any : constitutional water present in the mineral content will be ::; less prone to release as product:water than at such 600C
`: temperature.
:
: The results of Table 3 particularly show that a~ the temperature incrementally increases during the prQgressive microwave heating, the proportion of oil decreases from 85~ to 80%, while the proportion o~ gase~ increases ~rom g~ to 15~
with the total of generated constituents re~aining in the Z~6 range of 93-95~, during the pyrolysis from its initiation at 425C to its 475~C heating stage.
When the temperature reaches 500C, it is seen that the oil constituents, which up to this point had only liquified, now become vaporized or volatilized, such that the oil is converted or gasified into oil vapors in a further reduced amount of 75%. At the same time, the proportion of generated gases also increases still further to 20~, yet the total of generated constituents re~ains at 95%.
The gases as shown in Table 3 are those constituents which constitute noncondensible gas (i.e. at ordinary temperature), whereas the oil vapors which are generated or gasified at the 5Q0C pyrolysis level are, of course, condensible. Under the autogenous pressure of the gases in tbe pores of the mineral content of the rock or shale, the attendant hot oil constituents are~entrained in the gasified, i.e. condensible and noncondensible gas, constituents at the ~corre~spondingly progressively increasing heating temperature, and pass in reverse direction to the microwaves and toward the borehole 7 for recovery via the recovery chamber of the unit 11 and in turn, the outlet pipe 9 (see Fig. 1).
ence, the set of cond~itions given in Table 1 and conjointly shown in Figs. 2a and 2b will contemplate an oil and gaæ mixture of con~tituents conforming to the propor ional percentages set forth in Ta~ble 3 at the corresponding temperatures. It wi~11 be appreciated that inherently by reason o~ the in situ pyrolysi3 of the oil shale, in the absence of air, the kerogen produce~ a significant quantity of noncondensible gas as compared to the quantity o~ oil primarily sought as marketable commercial product.
As will be again repeated for e~pha~i~, this quantity ~l3~4Z1~6 of noncondensible gas, which represents a necessary by-product of the process, may be advantageously used, according to the present invention, as energy source for operating the electric generator 22 (Fig. 1) for providin~ the microwave power basic to the overall recovery system. At the sarne time, this use of the necessarily produced noncondensible gas does not detract from the maximum recovery of the desired liquified oil and/or gasified but condensible gas sought as primary product of the system.
Moreover, since the present invention contemplates maximum extraction of the carbonaceous values in the oil shale, the operation will normally be continued beyond the 500C temperature level as contemplated in Table 1 and the conditions as shown in Pigs~ 2a and 2b, by raising the temperature in a second step, after complete conversion in the first step of the liquifiable and gasifiable carbonaceous constituents over the pyrolysis temperature range of 425-500 C .
For this purpose, without interruption, i.e. to preventneedless loss of heat through conduction to t~e surrounding mineral content ma6s, the microwave heating is continued at ma~imum power, e.g. 100,000 watts, under constant on condition, for gasifying the yet unconverted carbonaceous values stilI present in the oil hale.
As earlier noted, once the liquifiable oil or petroleum constituents present which liquify at pyrolysis temperatures up to 500C have been liquifie~ and the volatilizable or vapori~-able or gasifiable oil or petroleum constituents present which gasify at such pyrolysi~ temperatures have been gasified to condensible and noncondensible gases as the case may be, a valuable remainder content of residual unli~uified ~3~8~ii and ungasified carbon constituents will still exist in the pores of the shale. This remainder content in effect constitutes solid form or fixed carbon or carbon coke, w~ich may be termed residual carbon or residual cokeO
As indicated in Table 3, by continued microwave heating in the second step, the residual carbon pressnt in the shale begins to gasify at 525C. In order to avoid water formation for the reasons discussed above, this second ~tep heating is controlled such that the maximum heating temperature re~ains below about 600~C. The maximu~ heating temperature will therefore be that temperature below 600C at which water formation will be avoided, minimized or suppressed, according to the process of the present invention.
The recovered gasified carbon coke, by reason of the second step higher temperature pyrolysis thereof, i.e~ also in the absence of air as in the first step, will likewise necessarily produce noncondensible gas, in this case contributing primarily increased contents of carbon monoxide.
This second step noncondensible gas quantity may be advantageously added to that recovered from the first step, and uced in whole or in part for operating the electric generator 22 to produce the required microwave energy.
Of course, depending upon the field conditions, the recapture radiu and the makeup of the carbonaceous con~tituentæ of the particular oil shale involved, the quantity of pyrolysis generated gas from the second step alone may be sufficient to provide the energy for operating the microwave source 12, without the need to use the nonconden~ible and/or condensible gasified constituents from the ~ir~t ~tep, or more than a portion of the noncondensible gasified constituent~ from the fir~t step.

~3(;~

Although the noncondensible gas generated by gasification of the residual carbon coke in the second step will be comparatively enriched in carbo~ monoxide con~ent, such is still a significant fuel source for energizing the electric generator 22.
Naturally, if it is desired to maintain these different gasified portions separate fro~ each other, the gas line 20 from the gas separator 17 (Fig. 1) may contain ~ne or more branch lines leading to correspondingly separate gas holders analogous to gas holder 21, such that the gas recovered via pipe 9 from the first step may be tran~ferred to one such gas holder and that recovered via pipe 9 ~rom the second step may be transferred to a different such gas holder.

EXAMPL~ ~rgy Inputs and Produ~tiG~ Outp~ts ~30 gallons per ton oil shale) Based on an oil shale grade of about 30 gpt on Fischer assay, typical of the average shale grade in the State of Wyoming, the 30 gpt oil shale had the following characteristics:
- Denslty 2.145 gm/cc ~ - Organic Matter I7.4 wt.%; 34.8 vol.3 : - Mineral Rock 82.6 wt.%; 65.2 vol.%
Converting the density to 133.9 lb/ft3 ~i.e. 2.145 gm/cc x 62.4 lb/ft2 water density), the weight of the organic matter, i.e. kerogen, and mineral rock in 1 ft3 of such oil shale, comes to ~bout: .
- Organic Matter 23.3 lbs. (i.e., 133.9 x 17.4%) - Mineral Rock 110.6 lbs. (i.e~, 133.9 x 82.6~) On a 1 ft3 shAle basis, on heating in Fischer assay, the 23.3 lbs~ o~ organic matter converts to abou~ 15,32 lbs oil and about 1.8 lbs. residual coke, the remainder being ~3~4~8~

about 2.7 lbs. water and about 3.5 lbs. noncondensible gas ~i.e. noncondensible at ordinary ambient temperature).
The 3.5 lbs. noncondensible gas produced with the 15.32 lbs. oil weighs about 23% of the oil product (3.5/15.32) in the 2~.3 lbs. of organic matter and has the approximate composition as shown in the following Tab:Le 4:
TABL~ 4--~o~o~ae~si~le Ga~ Co~p~8iti~

GaseousMol.
ComponentWt. x Vol.~ -Mol. Fraction Methane 16 20.0 3.20 Ethane 30 7.0 2.10 Propane 44 3.3 1.45 Butanes 58 1.9 l.I0 Pentanes 72 1.1 0.79 Ethylene 28 2.8 0.78 Propylene42 3.0 1.26 Butenes 56 1.2 0.67 Pentenes 70 2.1 1.47 Hexenes 84 1.5 1.26 Butadienes 54 0.1 0.05 C2 44 12.9 So68 C0 28 5.5 ~.54 2 2 33.5 0.67 H2S 34 4.1 1.39 100.0% 23.41 Apparent Mol. Wt.
It will be noted th~at the predo=inant quantity of hydrocarbon constituents are of the hydrogen rich saturated type, mainly methane, and that in addition to hydrogen and hydrogen~sulfidei a sign~ficant content of carbon dioxide, , ~
along with some carbon monoxide, i also pre~ent.
: :
The apparent mol.wt. 23.41 of the 3.5 lb. product gas lndicate~ that 54~ft3 (STP, i.e. 0C or 273~A; 760 mm Hg) o noncondensible ga~ are produced from 1 ft3 of the 30 gpt oil :: :
shale. This converts as follows:

- At the underground formation conditions (30C or 303A; 580 mm Hg):
- about 78ft3 nonconden~ible gas ti.e. by the ga~ law:
(54 x 760/580 x 303/273);

- At the microwave heating or pyroly~is emission temperature 130~36 .

t500C or 773A):

- about 200ft3 noncondensible gas (i.e. by the gas law:
78 x 773/303)-On the other hand, the oil product, which has anavexage mol. wt. of 240, as volatile material at the 500C
emission temperature or pyrolysis temperature occupies about 8S ft3 as volatile oil.
The 2.7 lbs. water also produced from the lft3 of oil shale (about 2.0%, i.e. 2.7/133.9~ occupies about 53ft3 (STP), and at the underground formation pressure ~580 mmHg~ and emission temperature (500C), this volume converts to about 200ft3 of water vapor.
Based on the calculation that the organic matter i.n the shale requires 527 Btu/lb to heat up and volatilize (per E.W.
Cook, 1970, Colorado School of Mines Quarterly, Vol. 5, ~o. 4, pp. 133-140), the total heat required to heat the 23.3 lbs. of organic matter in lft3 of the shale amounts to 12,250 Btu ~i.e. 527 x 2303). Since 1 British Therma:L Unit equals 0~293û
watt hour, the no-Ioss ~F (microwave~ energy required to decompose and volatilize the organic matter in lft3 of the shale (i.e. neglecting any loss to the mineral rock) amounts to 3.6 KW-hr ti.e. 12,250 x 0.2930/1000 watts).
The 23.3 lbs of organic matter o 34.8 vol.% o the lft3 of the 30 gpt shale of 133.9 lb~/ft3 density will in turn yield about 2.0 gal. of Qil product (i.e. 133.9 x 30/2000 lbsO ) Of cour~e, if accompanying ~ineral heating including analcime dehydration is con~idered as occurring, this might require incxeasing the amount by roughly 2 times as much equivalent heat to the bulk heating (totaling 3-~old heating), whereupon the energy input required to drive out such 2.0 gals. of oil pxoduct from the lft3 of shale increase3 to about ~3~Z~3~

11 KW-hr (3.6 x 3 fold).
Analcime heat effect on this amount is considered to be less than 5% maximum, so that its presence does not require expending significantly more RF heat energy, especially since the organic matter is heated up by the microwaves preferentially relative to the mineral content of the shale.
Elence, at 11 KW-hr of expended RF energy per lft3 of the underground formation, allowing for bulk heating, the oil production rate (at a theoretical 100~ oil recovery) may achieve abo~t 2 gals. of oil product and about 1/3 gal. of water per hour.
However, considering that, as distinguished from bulk heating, the organic matter is heated preferentially relative to the miner~l content~ according to the process of the present invention, the actual production rate at such 11 KW-hr energy input will be correspondingly higher, reaching 6 gals.
of oil product plus 1 gal. of water per hour (at such 100%
theoretical oil recovery rate), i.e. based on the fact that the miner~l matter does not heat up until after the organic matter has volatilized.
In summary, based on a 30 gallon per ton yield on Fischer assay, the following weights and volumes of products are produced from 1 cubic foot of the oil shale:
ei~ht - Oil 15.3 pounds - Water 2.7 pounds - Gas 3.5 pounds - Residual Carbon ~
23.3 pound~ organic matter (and water) Volume (500C !_80_ mmHg ) *
- Oil 8S cubic feet ` ~3~8~

- Water 200 cubic feet - Gas 200 cubic feet 485ft3 organic matter (and water ~apor) *Pyrolysis conditions at underground formation pressure, such that the 1.8 lb. residual carbon is not gasified but only the 21.5 lbs. of oil, water and gas (iOe. 23.3 less 1.8).
Upon recovery and con~ensation of the volatilized oil and water ~ontent, the noncondensible gas volume in turn amounts to 78ft3 (580 mmHg~.
Understandably, these amounts must be adiusted for the particular gra~e and minerology of the shale encountered. For instance, attendant mineral derived water miqht add 25~ to the amount of water which must be accommodated, and should mineral carbonate decomposition occur, e.g. from attendant ferroan or doIomite, the gas volume might increase roughly 15% due to additional carbon dioxide generation.
It will be appreciated that the time rate of vapor or gas production is a function of the RF energy input as modified by any mineral absorption, such that the ma~imum amount of organic decomposition products will increase with increasing :power input. Ultimately, the balance between organic and mineral absorption of the RF energy under the partlcular field condition~ encountered will control the ra~e of or~anic matter recovered as compared to energy supplied at the pyrolysis site.
:
Generally, such mineral absorption of microwave energy ~limited only to pyrites (FeS2)~, analcime and illite clay, ;~ ~all of which will normally involved at mo~t relatively small quantities, and thu~ which will actually only add a minor amount to the RF energy neede~ to carry out the extraction operation according to the proces~ a~ the pre#ent invention.

~4~16 Thus, at a rate of 3.6 KW hr RF energy supplied to the rock site, it will take between one and three hours to evolve the above calculated 485ft3 of total gas (volatiles) available from lft3 of the stated type oil shale at the 500~C pyrolysis temperature and after cooling to 30C, the noncondensible gas will occupy 78ft3 as above noted. Of course, it is only upon the loss of heat into the surrounding mineral content at the pyrolysis site that this time range would stretch out to the maximum or upper limit of three hours.
The foregoing, of course, presumes that the 1.8 lbs. of residual carbon is not gasified, and that the 485ft3 of generated volatiles or gasified c~nstituents is based upon the 15.3 lb~. oil, 2.7 lbs. water and 3.5 lbs. gs, totaling 21.5 lbs., pyrolyzed at 500~C from the lft3 of the stated 30 gpt oil shale.
In recovering the emitted or generated volatilized organic matter, the gas flow which is receiYed in the recovery chamber of the microwave uni~ 11 in the borehole 7 must pass upwardly to the ground ~urface 2 through the outlet pipe 9 (Fig. 1). The velocity of this flow of gas volume into the pipe 9 is dependent on the rate of production of the vapors or gasified constituente from the oil shale formation, their temperature, and the flow cross sectional area of the pipe 9.
Using a 4 inch radius pipe for this purpose (pipe 9), thereby providing a flow cross sectional area of 0,35f~2, about 8ft3 per minute (i.e. 485/60) of hot gase~ weighing about 0.36 lb. (i.e. 21.S/60) will pass through the pipe per l~t3 per hour of the 80 pyrolyzed or heated ~hale. Thi~ ga~
velocity i8 equivalent to a "gale" wind speed of about 1/4 mile per hour through the 4 inch radiu~ pipe (i.e. 8 x 60/0.35 5280).

13~2~6 Alternatively, using a 3 inch radius pipe, thereby providing a comparatively reduced flow crvss sectional area of only 0.196ft2, such flow velocity lncreases by about 1.8 times (i.e. 0.35/0.196).
The gas separator 17 must therefore be sized to accommodate such flow vo~ume and flow rates of emitted product.
~ aturally, in the shale itself, decomposition of the organic matter will dev~lop pores resulting from the disappearance of the organic volume by volatilization, save for the residual carbon still in situ in the rock, and such pore volume will exist to the indicated extent of disappearance of about 90% of the organic volume originally present, which as earlier noted in 30 gpt oil shale originally occupies 34.8 vol.% of the rock. The void spaces so developed accordingly represent about 31% of the rock volume (i.e. 34.8 x O . 90 ) .
Considering the entirety of the void space as available for gas transmission from the rock, lft3 of 30 gpt shale provides about 0.3ft2 of continuous void area to enable the evolving gases to be discharged from the rock. The flow rate of these evolving gases will accordingly be equivalent to that between a 3 inch to a 4 inch radius outlet pipe 9.
However, because the pores or holes in the rock are very tiny and the resulting passages or routes therethrough a~re tortuous, only part of this flow area will normally be ffective as a practical matter. As a consequence, internal press~re buildup at the decomposing organic face will occur which will inherently serve advantageously to increase the flow rate through the effective flow area of the collective pores of the ~hale.

~3~428~

In su~, since the gas evolution rate is a direct function of the power input, the greater the effective power in, the more gas out. Generally, the energy input will be progressively increased as decomposition proceeds deeper into the formation from the borehole.
As compared to initially applyin~ the RF energy in increasing increments of power as a function of the total shale under treatment, the applying of RF energy by continuous input of steady or constant level power, with a view to attaining a production rate of evolving vapors which remains nearly the same throughout, is actually ~ubject to decrease in the production rate despite the steady level of power due to mineral, or even perhaps residual carbon, absorption concomitantly increasing as the length of the mineral or rock path increases in a direction away from the bore hole. Hence, the use initially of incrementally increasing power is desirable.
EXAMPLE 2 Gas ~nergy Bala~ce t25 gallo~s per ton oil s~ale a Organic matter in 25.16 gpt oil shale (which consists of 14.6 wt.% organic matter and 85.4~ mineral matter), upon normal bulk heating, produces 2.95 wt.% noncondensible gas, of which about 0.74 wt.% is CO2 unavoidably formed from mineral carbonate decomposition, and thus not traceable to the organic matter. With RF heating according to the process of the present invention, this mineral carbonate decomposition is laryely eliminated.
Therefore, upon normalized dictribution recalculation to eliminate such mineral carbonate decomposi~ion CO~
fraction, the organic matter is indicated to produce about 2.21 wt.% nonconden~ible ga~ (with appropriate CO2 reduction), and about 0.482 wt.~ CO2 as shown, based on a 100 gm sample of ~3~Z~6 25.16 gpt oil shale, in the following Table 5:

TABLE 5 ~ Gas Distribution ~lormalized To Re3nove Mine~al Carbonate Gaseou~; Frc~m lOOg~ wt.%
Component Shale SampleOr~anic Gas . .
Methane .324 14.7 Ethane .190 8.6 Propane .132 6 0 Butanes .102 4 6 Pentanes .077 3 5 Ethylene .066 3.0 Propylene .110 5.0 Butenes .072 3.3 Pentenes .129 5.8 Hexenes .109 4.9 Butadienes .006 0.3 C2 .4~2 21.8 CO .173 7.8 H2 .068 3 H S .124 5 6 N~3 .043 2 0 2.207 gms 100 096 Thus, as compared to 0.324 ~m methane which, as normalized, constitutes 14.7 wt.~6 (i.e. 0.324/2.207) of the total gas from the 100 gm sample, the normalized 0.482 gm CO2 constitu~es 21.8 wt.% (l.e. t).482/2.207~ of the total noncondensible gas.
This CO2 content, along with the CO content, may be explained in part by the fact that attendant water under the pyrolysis conditions undergoes a reaction with the carbonaceous constituents present, such~ as methane, so as to form these two carbon oxides.
Such 2.207 gms of noncondensibls gas in the 100 gm s2mple of 25.16 gpt oi~ shale is, of course, a part of the total 14.6 gms OI' organic matter present in the shale (14.Ç
wt.% organic matter and 85.4 wt.% mineral matter), and based on the normali~ed values of Table 5, the corresponding breakdown in wt.96 and mol. fraction o the nonconden~ible gas in 1 wt.% of the organic matter is shown in the following Table 6:

T~B~ 6 - Gas ~reak~own Per 1 ~t.% Orga~ic ~atter Gas Content In Wt.% Gas ~ol. Fraction 1~.6 g~ Organi~ Fro~ 1 ~t.% Fro~ 1 ~t.
Gaseous ~ol. In 100 gm of Organic Organic Comp~nent Wt. 25.16 ~pt _hale Matter Hatter Methane 16~04 .324 .0223 .001390 Ethane 30.1 .190 .0130 .000432 Propane 44.09 .132 .0090 .000204 Butanes 58.1 .102 .0070 .000120 Pentanes 22.15 .077 .0053 .000073 Ethylene 28.15 .066 .0045 .000160 Propylene 42.08 ~ .110 .0075 .000178 Butenes 56.1 .072 .0049 .000087 Pentenes 70.13 .129 .0088 .000126 Hexenes 86.2 .107 .0074 .000086 Butadienes 54.1 .006 .0004 ,000007 C2 44.01 .482 .0331 .000752 CO 28.01 .173 .0118 .000421 H2 2.02 .068 .0047 .002327 H S 34.08 .124 .0085 .000249 N~3 17.03 .043 .0029 .000170 2.207gm .1512% .006782 Thus, as compared to 0.0223 wt.~ methane in 1 wt.~
organic matter based on 0.324 gm methane in 14.6 gm organic matter (i.e. 0.324/14.6~, which constitutes a mol. fraction of-0.001390 methane (i.e. 0.0223/16.04), the CO2 content amounts to 0.0331 wt.% (i.e. 0.482/14.6), which constitutes a mol.
fraction of 0.000752 C02 (i.e. 0.0331/44.01)~ The total 2.207 r gm noncondensible gas amounts to 0.1512% (i.e. 2.207/14.6) for a ~cumulative mol. fraction of 0.006782 for all of the noncondensible gases taXen~collectively.
Since the organic~matter is preferentially heated by ~ ~ the RF radiation, about 125 cal/gm is indicated as required to :: :
~ heat the 25.16 gpt oil shale from the formation ~emperature : ` :
(30C) to at least 450-C. This~includes about 14 wt.% organic matter yet requires only about 28% of the total heat or about 35 cal/gm (i.e. 125 x 28%). Allowing liberally $or an equivalent heat 105B to the mineral matter using RF heating, as an extra one ~old amount to compensate for conduction heating and even direct mineral ab~orption, the total two fold ~0 ~3~4~
h~at required is still only 70 cal/gm (i.e. 35 x 2 fold).
It is indicated that the preferential absorption of the microwave energy by the organic matter remains fairly constant over a wide range of frequencies (RF), whereas the mineral matter, e.g. carbonates ~dolomite, caicite and the like), silica es (quartz, soda feldspar, potash feldspar and the like), aluminates, etc., is relatively transparent thereto throughout such range.
The heat from the above specified n~ncondensible gas evolved from 1 gm organic matter in the 25.16 gpt oil shale is shown in the following Table 7:
TABLE 7 - ~eat From Gas Fro~ 1 Gm Organic Hatter Gaseou~ 70 cal/g~
Component K Cnl Distribution Methane .293 Ethane .159 Propane .107 Butanes .083 Pentanes .006 Ethylene .053 Propylene .087 Butenes .057 Pentenes .102 Hexenes .083 Butadienes .004 1.034 Subtotal ~ydrocarbons 52.6 Hydrocarbons C2 None ~one CO .029 2.3 H2 .135 10.8 H S .036 2.9 N~3 .018 1~4 1.252 K Cal/Gm70.0 cal/gm Organic (in gas from 1 gm organic) The heat from the noncondensi~le gas evolved from 1 gm of organic matter in the ~hale as shown in Table 7, of course, does not include CO~ uince this is already in completely combusted condition.
It will be seen that the total heat of 1.252 K Cal ~or 1252 cal) available from the noncondensible gas from 1 gm of ~3~Z~6 organic ~atter corresponds to 2254 Btu/lb organic matter (i.e.
1.252 x 1800 where 1.8 Btu/lb. equals 1 cal/gm and 1800 Btu/lb. equals 1 K Cal/gm), and that the total heat available from combustion of the evolved gas is 14% of 1252 cal, or 175 calories.
Based on a 40% conversion efficiency of the combustion energy ~f such noncondensible gas to produce the RF power in the electrical generator 22 (Fig. 1), such as a gas operated fuel cell, the heat available as RF power from the gas evolved from the organic matter in 25,16 gpt shale is 70 cal/gm (i.e.
175 x 40%).
Converting the 70 cal/gm to 126 Btu (i.e. 70 x 1.8), and considering that at 25 gpt oil shale rates it takes 3360 lbs of oil shale to yield a barrel of oil (i.e. 42 x 2000/25 at 42 gal/bbl) at 100~ recovery, then assuming recovery is only 50%, the doubled energy requirement amounts to 846,720 Btu/bbl (i.e. 126 x 3360 x 2~.
Since 1 kilowatt hour equals 3413 Btu, it will take 248 KW-hrs. or 10 1/3 days (24 hour days) to produce 1 bbl of oil (i.e. ~46,720/3413). Nowever, if the RF radiation is increased to 10/000 watts (10 KW-hrs), it will take only 24.8 KW-hrs or 1 1/3 days to produce 1 bbl of oil, and if the radiated power is increased to 100,000 watts (100 KW), it will take only 2.5 XW-hrs to produce 1 bbl of oil or 9.6 bbls per 24 hour day (i.eO 24/~.S).
Of course, as will be appreclated, at increased radiation, the yield rate will increase by 2% per 1% increase ~at assumed sensitivity to recovery rate o~ 50~), whereas at decreased radiation, the yield rate will correspondingly decrease by 2% per 1% decrease.
Naturally, depending on the proportion of the created gas which is used to provide power in the electrical ~3~Z~6 .

generator 22, excess power so produced can be made available to local municipalities or otherwise marketed as a separate product.
As t~ the composition of the products volatilized or gasified by the microwave radiation pyrolysis of the oil shale or other porous media, and in turn the amounts of the condensible oil (vapors) and noncondensible gas generated, these will vary markedly with the heating rate. Very slow heating produces high conversion of the organic matter to oil, and the oil is primarily paraffinic. Conversely, very rapid heating produces low conversion of the organic matter and generates a primarily aromatic oil. Practical optimum time rates for heating by RF energy are selectively between these two e~tremes, yet such must be matched to a practical production rate at a total heat balance for the system which i8 best from a process economics standpoint.
Since organic matter absorbs RF radiation faster as it becomes hotter, continuous radial progression of organic decomposition to the outer limits of the recapture radius will be enhanced.
~ y providing an optimumly by steep thermal gradient across the heating front in the porous media, the organic matter at the reacting front will volatilize before ~ignificant thermal expansion will occur of the organic matter behind the reacting front~ i.e. in a direction more remote from the microwave source, and this effect may be controlled by controlling the local rate of heating of the organic matter.
In th~s way, the mechanical behavior of the rock will represent a minimum variable since it varies with the heating rate and the largest influence thereon stems ~rom the thermal ~3Q4Z136 expansion of the organic matter.
Hence, by controlling the local rate of heating of the organic matter, such thermal expansion of the organic matter will be confined to the reacting front and will minimize conduction heating of the rock itself and adverse modification of its mechanical behavior and 105s of compressive strength, thereby minimizing adverse environmental impact on the underground formation and any ramifications thereof on the integrity of the terrain at the ground surface.
It will be appreciated that correspondi~g results are analogously attainable in microwave heating of oil and tar sand deposits, heavy oil reservoir deposits, and residual heavy oil pools previously subjected to primary oil well drilling extraction, and the like, in accordance with the process of the present invention.
~ his is because the applied high frequency electric energy in the form of microwaves quickly transfers through a~d within the partlcular deposit of th~ petroleum impregnated porous media or pool and converts very rapidly t~ heat energy upon contact with the carbonaceous material present, e.g.
hydrocarbon molecules.
Unlike the disadvantageous use of hot water or steam heating in which there is inherently a major Btu loss due to heat dissipation along the downhole course between the ground surface steam generator or hot water heater and the deposit to be heated in ~itu in the underground formation, in some deposits representing many thousands of feet of vertical separation, there is no corresponding Btu loss between the ground surface and the deposit being worked according to the process of the present invention because the in situ heating i9 aarried out with RF energy heat generated immediately adjaaent the deposit at the underground level o the bedding.

8~

~3~ 6 Moreover, because of the nature of the microwave heating, just as the organic matter, i.e. kerogen, is thermally broken down into liquid and gaseous constituents, and especially into noncondensible gas by the pyrolysis, bitumen fracti~ns such as those present in oil and tar sands and in heavy oil reservoir deposits and residual heavy oil pools, and the like, will by analogy be similarly broken up to reduce the bitumen into smaller fractions, i.e. smaller molecules.
In this regard, while conventional downholP heating methods which rely solely on heat conduction by bulk heating or gross heating are beset with the complicating problem in dealing with the heavier crudes (which require most of the heating because they are the poorest type of thermal conductoxs among the crude oils), of expending even greater amounts of heat energy in order to extract them, such complication does not arise according to the process of the present invention because of the manner in which the pyrolysis heating is carried out using microwave energy for mol~cular breakdown of the carbonaceous constituents in situ.
A more important advantage of the process of the present~invention is that the microwave heating of the petroleum impregnated media, such as oil shale, oil and tar sands, heavy oil reservoir deposits, residual heavy oil pools, etc.! and specifically of the kerogen, tar, bitumen, heavy crude oil and the like sources of the desired synthetic fuel or "oil", provides for the inherent generation of large volumes of gas, especially noncondensible gas, under the pyrolysis conditions, which gas is primarily derived from de-polymerization or molecular breakup or in situ "cracking" of the oil constituents. Thi9 molecular breakup i9 inherently ~3~4~86 promoted as the autogenous pressure progressively increases with increasing generation of gaseous constituents.
Such is in addition to the role of the generated gas as an in situ drive factor under the at-tendant autogenous pressure to encourage the oil constituents, including any liquid oil constituents plus oil vapors admixed and entrained therewith, to migrate towards the borehole for efficient recovery via the microwave unit 11, where once recovered, it represents a convenient by-product usable to produce electrical energy in the electrical generator 22 without decreasing the amount of primarily sought oil as basic commercial product of the endeavor.
As to the migration of the generated oil constituents from the deposit to the borehole, it has also been found that the microwave energy during the pyrolysis specifically breaks down the paraffin content and similar accumulations present in the deposit which otherwise severely retard the normal migration of the oil constituents through the formation in carrying out conventional ln situ retorting or heating recovery techniques.
Added to this is the further fact that movement of the oil constituents in the desired migration flow is ~upplemented or further enhanced by the reduction of the surface tension within the oil constituents by the applied microwaves.
In connection with the foregoing, it should be noted that~ paraffin constituents are not highly reactive to RF
heating. However, the paraffin con}tituents are conveniently heated by way of molecular conduction by the otherwise R~
heated hydrocarbon constituents pre9ent in association therewith in the petroleum impregnated media involved during the production operation.

Advantageously, accordins to the present invention, a time domain technique may be used for the measurement of the dielectric properties or permittivity or inductivity of the petroleum impregnated porous media or deposit such as oil shale, over a broad frequency band of the RF energy within very short time intervals. The measured dielectric properties in turn will provide an indication of the ongoing chemical changes which occur during the pyrolysis decomposition of the carbonaceous values, e.g. hydrocarbons in kerogen in the oil shale, for monitoring and controlling the microwave radiation input as the pyrolysis operation progresses.
In general, the dielectric properties of oil shale, for instance, may be measured using the known point by point fre~uency domain method. Such a procedure has significantly limited the adequacy of the measurements to track fast or abrupt chemical changes occurring during the rapid heating of oil shale, e.g. using RF heating~ although a particular recent technique has been suggested which provides the permittivity behavior over a broad fxequency band from a single measurement (Proceedi~s of the IEEE, March, 1981, M.F. Iskander, AoL~
Tyler and D.F. Elkins, "A Time-Domain Technique For Measurement of the Dielectric Properties of Oil Shale During Processing.").
Basically, as appreciated in connectlon with such recent suggested technique, the process of recovering liquid and gas o~s fuels from oil shale ~or optimum results critically depends on ascertaining the manner in which kerogen decomposes under the particular pyrolysis conditions so as to ~orm bitumens, and in turn oil and gas constituentQ. In this regard, the thermal behavior of materials which under~o thermal decompositiOn or phase transformation, such as ~erogen ~3~4~8~
in oil shale, must be characterized in some way to achieve this purpose. It is conveniently done by thermo analytical techniq~e, e.g. differential thermal analysis or thermogravimetry. Indeed, measurement of the electrical properties of such materials is currently deemed more or less essential to any thermophysical characterization, considering the concordantly extreme sensitivity of such electrical properties to those physical and/or chemical changes which take place during the thermal decomposition or phase transformation of such materials under thé heating conditions.
In the general instance of the known point by point frequenc~ domain measurement technique, a large number of representative measurements over a wide frequency range has usually been considered necessary in order to obtain a complete characterization of a given dielectric material, thereby involving a time consuming procedure which may necessitate repeated and laborious measurement techniques.
This, in turn, severely limits the adequacy of the measurements for tracking such fast or abrupt chemical changes, e.g. those changes which take place as oil shale is heated rapidly, inasmuch ae an inherent minimum time limit for the heating rate which can be used lS governed by the minimum time it takes for the dielectric measuremen~s over the sweep of the frequency range at the given temperature.
According to the aforesaid recent particular technique which has been ugge~ted, the procedure requires considerably less time to perform the measurements, and employs a small shunt capicitor terminating a coaxial line section as the sample holder, whose geometrical dimensions were selected to provide a 50 (i.e. 50 omega or 50 ohm~ coaxial line terminated ~3~Z8g~
by a capicitance in the optimum range, because of the direct relation of the optimum capacitance value to the frequency band of interest and the dielectric constant of the material being tested. This particular recent technique provides broadband information on the frequency characteristics of the oil shale tested, from a single time-domain measurement, and is said to constitute a rapid and sensitive method of tracing reactions as they proceed under varying conditions.
The experimental (laboratory) set up of such measurements utilizes a time-domain reflectometer and oscilloscope connected to the csaxial transmission line section terminated by the small lumped capacitor, with the oil shale sample placed in the gap of the capacitor sample holder and the measurement procedure following closely that generally utili~-ed in the past. A reference signal from a short circuit placed at the sample holder location and the reflected signal at the sample interface are recorded, digitized, and their Fourier transform is calculated. This procedure determines the frequency dependence of the reflection coefficient, which can then be used to calculate the real and imaginary parts of the relative permittivity in the usual way.
The dielectric constant of the oil shale sample of estimated richnes6 of 120 liters/ton or 30 gpt (i.e. 120~4 at 4 liters/gal) was measured using the ~ample holder and the permittivity results obtained from such time-domain measurements were stated to agree clearly with the point by point frequency domain results obtained by former known methods, yet provided dielectric constant data for such oil shale in the frequency ranye which includ~d the band between 10-250 MHz, where no data were previously known. The results covered the dielectric con~tant of such 30 gpt oil shale as a ~3(~2~
function of the frequency over the broad band from 0.01 to 2.0 GHz (10 to 2,000 MHz), apparently all at a temperature of 25C, rather than at pyrolysis temperature.
In contrast to the foregoing known time domain technique and recent particular technique using a small shunt capacitor terminating a coaxial line section as sample holder, according to a further aspect of the present invention, as shown in E`ig. 3, an in situ probe system 30 is provided for on line measurements of the electrical properties of oil shale and other in situ sources of synthetic fuels such a s oil and tar sands, heavy oil reservoir deposits, residual heavy oil pools, and the like type petroleum impregnated porous media or petroleum deposits, using the time domain technique for provided an optimum ongoing RF control for maximizing the extraction of the carbonaceous values sought at minimum expenditure of microwave energy.
The probe system 30 is provided to track at high speed the chemical changes which occur during transformation of the kerogen in oil shale or of the analogeous organic matter in the other types of deposits which may be treated according to the present invention, for optimizing the selective RF
xadiation level of power and frequency for heating the organic constituents and focusing the energy in the oil shale volume or that of the other porous media involved.
The probe system 30, basically consists of an apparatus or assembly which includes an open ended coaxial transmi~sion line with an extended center conductor, such that the e~tended pvrtion of the center conductor may be ~mbedded in the deposit and its e~posed length adjusted for concordant optimum measurement result~ over the desired frequency band.
As shown in Fig. 3, the probe system or apparatus 30 inclu~es a center conductor or conductive probe 31 as core, insulated electrically, e.g. by the insulating material 32, from its counterpart coaxial peripheral conductor or conductive jacket 33, and having a protruding probe end portion 34 extending beyond the end face 35 of the probe system 30 a selective distance for providing a measuring arrangement for measuring di~ectly in situ the dielectric constant of the oil shale or other porous media in an ongoing manner.
The probe assembly 30 may be selectively positioned in the deposit with the probe end portion 34 embedded in the deposit and the opposite end of the coaxial transmission line may be led via the borehole 7 to the support surface 2 for connection to the usual indicating means such as the recording and information processing equipment 36 in conventional manner.
Alternatively, a separate borehole may be drilled into the formation outwardly of that containing the microwave unit 11 for positioning the probe system 30 more remote from the microwave source. In fact, a number of such separate boreholes may be provided each at a separate radius progressiyely farther away from the borehole 7 as center, each containing its own such probe system 30 optionally along with such a probe sy~tem 30 in the borehole 7.
In each case, the probe system 30 may be positioned in situ in the particular deposit at the desired location by conventional mining or oil drilling technique.
The probe 31 is, of course, slidably arran~ed within the insulating material 32 to permit relative axial movement thereof for adju~tment of the exposed length of the probe end portion 34 ~rom the opposite end af the coaxial transmi~sion ~3~4~6 line at the ground surface 2.
In this way, the probe system 30 will provide an on line measurement of the complex permittivity of the deposit and the condition of the oil and gas constituents being generated under the microwave pyrolysis, and a feed back system via the remainder of the arrangement leading to the recording and information processing equipment 36 at the ground surface 2, thereby enabling the permittivity probe system 30 to be used to sense and thus control and adjust the RF heating conaitions, i.e. by adjustment of the RF power and/or frequency, in accordance with the dielectric constant changes as sensed in situ by the probe end portion 34.
As will be appreciated, the RF frequency adjustment will be made as a function of the relaxation frequency as determined by the permittivity measurements of the probe system 30 and through the feedback system to the equipment 35 on the ground surface 2 as driven by the permittivity probe 31, whereby to control and adjust the RF power and/or frequency for m~intaining optimum heating oonditions throughout the oil shale volume or other porous media deposit and during the entire heating period.
~; Thus, using the time domain technique, the in situ probe system 30 is operatea according to the present invention to measure the dielectric properties of the particular porous media in the deposit being worked, over a broad frequency band, s.g. 0.01 to 2.0 GH~ or 10 to 2,000 M Hz, or more, under the pyrolysis conditions and throughout the volume of the deposit and durin~ the entire microwave heating period.
In particular, the length of the exposed pxobe end portion 34 beyond the open end face 35 of the coaxial transmission line as constituted by the probe ~ystem 30 will ~3~a2Z~36 be longer for measurements at lower attenuated feedback frequencies and shorter, or even possibly completely zero, i.e. with the probe end portion 34 flush with the end face 35, for measurements at higher attenuated feedback frequencies.
For instance, the outside diameter of the coaxial transmission line or probe system 30 may be 0.081 inch and the e~posed length of the probe end portion 34 may be from 0 (flush~ to 0.3 inch.
Thus, the in situ permittivity probe system 30 according to the present invention provides measurement advantages similar to those of the lumped capacitor sample holder earlier described, in that it also provides a link between low and high frequency measurement techniques.
Similar to the adjustment of the capacitance of the shunt capacitor of the transmission line of such sample holder, the in situ probe according to the present invention provides for maximum accuracy in the desired frequency range, but unlike the sample holder, provides for such accuracy not at 25C, but at the actual pyrolysis~temperature, and not at the ground surface, but remotely in situ in the deposit, and merely through selective change in the exposed length of the center conductor or probe end portion 34 extending beyond the ,.
end face 35 of the ground plane conductor as constituted by the coaxial transmis~ion line, i.e. as ad~usted remotely at the ground surface either manually or by automatic means (not shown) in conventional manner, e.g. in the manner of a Bowden cable. ~ -In essence, the coaxial transmission line or probe ~ystem 30 operates analogously to an adjustable receiving antenna or secondary coil of a trans~ormer in picking up as cQrresponding induced voltages the concordant signals z~

represented by the high frequency microwaves as modified by absorption by the organic matter of the deposit and thus providing an attenuated feedback frequency dependent indication of the ongoing level of the changing dielectric constant of the organic matter at any given point in the pyrolysis heating, and in tur~ of the degree of transformation and the nature of the transformed constituents present, such as to permit adjustment of the RF frequency in concordance with such changes.
Hence, by adjustment of the exposed length of the center conductor or probe 31 as constituted by the length of the probe end portion 34 extending beyond the end face 35, which by analogy performs the function of a receiving antenna, such antenna may be precisely tuned to the same frequency as that of the radiated microwaves as modified in frequency, i.e.
relative to the microwave ~ource originating frequency as reference frequency by the then degree of absorption by the organic matter, thereby providing an ongoing measure of the dielectric constant of such organic matter and changes therein and in turn, a corresponding indication of the ongoing changes in chemical reactions occorring during the pyrolysis.
In regard to an inherent modification of the probe apparatus 30, the lnsulating material 32, such as a high temperature resistant thermosetting plastic in which the probe 31 is axially slidably maintained, may be alternatively omitted, thereby leaving an electrically insulating void annular space or vacuum space from which air has been excluded 90 as to avoid a source of contaminating air for the microwave pyrolysis of the organic matter in the porous media.
In this case, as 5hown in phantom in Fig. 3, a series of lnsulating ~ixed rad.ial spacers 32a may be located along ~3~Z86 ~. , the course of the interior of the coaxial transmission line to keep the probe 31 and jacket 33 electrically apart, plus gas sealing insulating end radial spacers 32b plugging the opposed ends of the transmission line or at least the in situ probe end at the electrically open end face 35, in conventional manner.
Optionally, such void annular space may be filled by captively contained inert gas in place of a vacuum condition.
In any case, the probe end plugging spacers 32b, as the case may be, will be sized for sliding sealing fit with the probe 31 passing therethrough to prevent gas or liquid leakage thereat, so as to inhibit ~luid exchange between the porous media zone surrounding the embedded probe end 34 and the interior of the coaxial transmission line when not physically occupied by the insulating material 32.
Naturally, the remote end of the coaxial transmission line need not be positioned at the ground surface 2, but as the artisan will appreciate, may instead be positioned within o~ in the vicinity of the borehole 7 or the microwave unit ll, or in a separate borehole, as desired, and electrically connected by suitable wire leads to the equipment 36, and via a ~owden cable arrangement or the like, also mechanically connected to such equipment 36~for axially adjusting the probe 31 relative to the jacket 33.
Advantageously, as shownin phantom in Fig. 3, an as~ociated conventional in situ thermal analyæis device or meanq 37, or ~he like type temperature sensing and recording means, is optionally yet preferably also provided in the probe system 30.

~5 2~3~

The thermal analysis means 37 has an exposed sensing portion 38 adjacent the in situ probe end at which the probe end portion 34 of the axially shiftable centra7 conductive core 31 is located, for corresponding embedding in the porous media whereby to sense and record the prevailing temperature at the particular in situ probe site, by way of differential thermal analysis technique and attendant calculations as earlier described.
For this purpose, the indicating means of the conventional rPcording and information processing equipment 36 or the like is also arranged for indicating the temperature sensed by the sensing portion 38 at the in situ probe site in conventional manner, the thermal analysis means 37 being operatively connected with the equipment 36 or the like in the same way as the remainder to the probe system 30 is so connected as earlier described, w~ereby to achieve recordable form feeaback information as to both permittivity and temperature.
Hence, the overall probe system 30 may be operated not only for sensing in situ changes in the dielectric constant via the positioning of the probe end portion 34, but also for sensing in situ the prevailing temperature via the sensing portion 380 ; In this way, the microwave pyrolysis operation may be effectively carried out with ongoing adjustment of the microwave radiation in dependence upon the sensed changes in dielectric constant in conjunction with sensed changes in the prevailing pyrolysis temperature, i.e. as sensed, recorded and/or indicated via the indicating means such as the remotely located equipment 36~

g~ :

~3~4Z~i Of course, it will be appreciated that a separate temperature sensing alld recording means (not shown), may instead be used for sensing and indicating the prevailing pyrolysi 5 temperature at the pyrolysis site.
However, by incorporating such means in the probe system 30, as preferred in accordance ~ith the present invention, a more convenient and efficient overall combination, as a simplified composite unitary arrangement is provided, which assures that the temperature sensed is that at the very same localized point at which the probe end portion 34 is situated in the underground porous media, and which is positionable as a common embeddable assembly all at one and the same time.
In connection with the use and location of the instant in situ permittivity probe system 30, according to the present invention, it has been determined that petroleum impregnated medla, such as oil shale, etc., tend to be rather constant in their content for significant distances.
In the case of oil shale in particular, the consistency of its content or makeup, as between its composition of carbonaceous constituents and mineral constituents, within a specific bed or formation, can literally run for miles, or certainly at lea~t~thousands of feet horlzontallyt As earlier noted, the various beds of hydrocarbon impregnated media, sueh as oi} shale, ganerally are ~ituated in substantially horizontal planes whose deviation from true horizontal is minimal, e.g. less than 1%.
Therefore, it is normally not necessary to sample each bed in the vicinity o~ each borehole 7 being worked when recovering the carbonaceous values by the microwave pyrolysis proce~s according to the present invention, such as by the use ~3~9L286 of sample bores at progressive radial distances from each adjacent borehole in a given formation area to obtain preliminarily core samples at each vertically successive bed adjacent each such borehole for initially determining in conventional manner the concordant composition of the carbonaceous constituents and mineral constituents thereof, and especially potential gpt yield information, in conjunction with the subsequent use of the probe ~ystem 30 to indicate RF
values, times, etc. in terms of ongoing measurement of the dielectric constant and pyrolysi~ temperature at each corresponding underground site of the in situ pyrolysis process and at such progressive radial distances from the particular borehole 7 as the pyrolysis progresses, e.g. in the manner shown in Figs. 2a and 2b.
Instead, as to a give formation area, once the carbonaceous and mineral constituent content or makeup of each pertinent bed has been determined by core sample analysis in conjunction with the use of the probe system 30 in corresponding probe bores at representative progressively increasing radial distance from the borehole 7 being worked to obtain information as to RF values, times, etc. as noted above, consequent an initial microwave pyrolysis, it is reasonably safe to assume that the same dielectric constant and pyrolysis temperature information obtained by the indicating means such as the equipment 36 at that borehole 7 area bed site ~an be used to carry out the microwave pyrolysis operation at adjacent borehole areas being worked where substantiaIly the Bame gallons per ton carhonaceous values and minerology content exi~t, due to the consistency of the bed formation content ~or each appropriate bed or 9tratum over pronounced ~orizontal distanaes covering large areas as pointed out above.
1'hus, sample probe bores can be set at a predetermined radial distanee apart relative to a given borehole 7 being worked, and in conjunction with core sample analysis therefrom in turn can be pxovided with corresponding probe systems 30 embedded into the impreynated media adjacent each such probe bore at the le~el of the given bed beiny worked, for obtaining the desired infor~ation during the microwave pyrolysis operation carried out at that borehole 7, such that this sampling process need be used for instance only once per 100 adjacent boreholes 7 in a given vicinity.
In this regaxd, as shown in Fig. 1, where ~ore sample analysis of the rich oil shale beds S and lean oil shale beds 6 shows for instance that all of the beds 5 have substantially the same composition and gpt yield characteristics, and ~hat all of the beds 6 have the same composition and gpt yield characteristics, yet different from those of the beds 5, then the sampling process need be used only for a bed 5, i.e. the lowermost bed 5, and separately only once for a bed 6, i.e., the lowermost bed 6, at a given borehole 7.
This sampling process need only be modified for more frequent use i.e., for a lesser number of adjacent boreholes 7 in a given v1cinity or for a grea~ter numberof vertically disposed beds at a given borehole 7, when production differences are noted that indicate a change along or within the corresponding beds of a given formation as to gallons per ton carbonaceous ~alues or mineral content thereat.
A typical example of carrying out such sampling process using an array of in situ permittivity probe systems 30 according to the present invention is ~hown in ~igs. 4 and 5.

~ 3t~ 86 As seen fro~ above in ~ig. 4, r~lative to the main borehole 7 in the formation at the level of a given bed of the petroleum impregnated media, e.g. oil shale, being worked such as the lowermost bed (Fig. 1~, a series of sample probe bores, only probe bores b-1 to b-7 of which are shown, substantially vertically extending from the ground surface down to the level of the bed being worked and also substantially parallel to the associated main bore~ole 7, is provided.
Preferably, the probe bores are disposed in the form of a more or less generally outwardly increasing radius spiral arrangement at least partially around the main borehole 7 as center and spaced therefrom and from one another at intermittent distances to the full extent of the RF
penetration, i.e. along the entirety of the xecapture distance or recapture radius for that borehole 7.
Appropriate analysis of core samples from all of the beds is preliminarily undertaken (Fig. 1).
Each probe bore is provided with a corresponding probe system 30, here designated as probes, only concordant probes p-l to p-7 of which are shown, embedded in situ in the adjacent petroleum impregnated media at the particular probe bore at the corresponding level of the bed or stratum being wurked. Each such probe or probe system 30 is of course connected to an appropriate indica~ing means such as the equipment 36 as earlier described such as at the ground surface 2 (Fig. 1).
The actual spacing of the probes is determined by the carbonaceous values, e.g. gpt content, and associated minerology of the deposit involved at the given bed or stratum being worked, as determined by such preliminary core sample analysis .

~L3~ 86 For instance, in the case of 25 gpt oil shale the radial distance apart of the probe bores, and thus of the probes, is preferably one meter, although the actual distance apart or radial diqtance intervals at which the probe bores and associated probes are located may be varied, depending on the degree of detail or preciseness of the information desired to be provided via the indicating means such as the equipment 35, as well as upon the nature and consistency of the deposit along the extent of the recapture distance or recapture radius involved for the given bed level site.
It will be seen from Fig. 4 that the probe bores and thus the probes are at generally equal radial increments apart, i.e. at successive progressively increasing circumferential or annular zones or rings relative to the main borehole 7 as center, with each such annalar zone or ring having the same radial interval or internal radius span as the next. In this way, uniform and precise information can be obtained via the probes throughout the recapture distance or recapture radius of the borehole 7 being worked at the given bed level site.
On the other hand, it will be seen that the actual linear distance between adjacent probe bores and thus between adjacent probes progressively increases along the course of the spiral arrangement so that a representative arc portion about the ~orehole 7 at the given bed level site is provided with the probes.
Al~hough this arc is shown over an angular sweep of about 180 degrees from probe p-l to probe p-7, it will be appreciated that such arc may be conveniently selected to provide any desired sweep 80 long as it is able to provide representative permittivity information for the entirety of ~3~2~f~

the contemplated bed area within the pertinent recapture distance or r~capture radius involved.
Hence, where more than seven probe bores and associated probes are involved, e.g. at 1 meter intervals of progressively increasing radius apart, the linear distance between adjacent probe bores can be kept constant or of smaller increments of progressive increase apart to maintain the angular sweep of the spiral arrangement ~t about 180 degrees along the course of the recapture radi~s, or the angular sweep may extend therebeyond, e.g. over 270 degrees or even 360 degrees~, or may repeat itself in multiple spiral revolutions by continuing progressively to 540 or 720 degrees or more, as may be appropriate under the circumstances, especially in the case of more pronounced recapture radius deposits, e.g. having a recapture radius of 38 feet or more, all of course in dependence upon the conjoint equal or uniform or nonun1form progressively changing raaial increments apart of the probe bores (cf. the nonuniform radial increments at which the microwave power is incrementally increased according to the present invention as shown in Figs. 2a and 2b).
In any case, the spiral arrangement of the probes in ~he probe bores is such that the microwave radiation MR as schematically shown in Fig. 4 distributed from the microwave unit ll [Fig. 1), e.g. in a full 360 degree arc pattern, will be effectively sensed by the probes p-l to p~7, etc. as the ca~e may be for th~ desired purposes at the given bed lev~l site.
Because of the generally true ho~izontal orientation of the beds of petroleum impregnated media in the formation, it will be seen from Fig. 5 that the spiral array of probes p-l to p-7 etc. i~ located in a plane P generally parallel to the ~3!?~Z1~6 horizon or at right angles to the vertically disposed main borehole 7 in the formation, an~ disposed at the corresponding underground level of the microwave unit 11 suspended via the pipe 9 in the borehole 7, i.e. at the vertical depth at which the bed containing the deposit being worked is located.
Although such probes are generally arranged in a common horizontal plane at a 90 degree angle relative to the main borehole 7, as shown in Fig. 5, as where the bed being worked extends generally in true horizontal orientation as earlier described, naturally where the particular bed encountered lies at an inclined angle to the true horizontal, the probe bores will be adjusted in depth so that the probes may be lowered therein sufficiently to be positioned adjacent the corresponding bed level in each at which the deposit being worked is located, whereupon the common plane P containing the spiral array of probes will assume an inclined angle so as to register or conform intersectingly with the inclined angle bed deposit.
In this case, the microwave unit 11 will be angularly positioned as well for distributing its microwave radiation along and through the inclined angle bed deposit.
In all cases, the spiral array of probes is arranged æuch that readings are taken~at the same relative planar level or elsvation as the R source, i.e. the microwave unit 11, and thus at the average vertical center of the ~F energy radiated area.
For instance, for an oil shale hed of three feet in vertical height, the microwave unit 11 is desirable positioned in the borehole 7 such that the radiation is distributed in vertical alignment with the 1 1/2 foot midpoint height o the bed, and the probes p-1 to p-7 etc. are posit.ioned in their 10~

~3~Z&t~i respective probe bores b-1 to b-7 etc. in a common plane P
passing through the bed and in corresponding collective vertical alignment with such 1 1/2 foot midpoint height of the bed.
The sample probe bores, like the main borehole 7, are provided in co~ventional manner, and the probes are embedded into the adjacent deposit in conventional manner, e.g. via a pipe or line support arrangement similar to pipe 9 for borehole 7, preferable equipped with an inflatable sealing collar analogous to collar 10 and for the same purposes, or alternatively using ground surface sealing of the probe bores during the pyrolysis operation.
Thus, in the event the sampling process is used successively for each bed in the formation (Fig. 1), the probes are repositioned upwardly ln their corresponding bores at the level of the next above bed deposit to be worked, just as in:the case of the microwave unit 11 in the main borehole 7, and after the last or highest bed deposit in t~e formation has been worked, the probes will be pulled permanently from ~the bores for repea ed use at a different area where permitti~ity information is to be obtained, and the bores will be sealed permanently at the ground surface just as in the case of the main borehole 7.
Desirably, the e~tent of the probe bore below the level of the particular bed being worked at which the probe is located, will be plugged permanently by a cement plug analogous to cement plug 23 in the case of the main borehole 7 and for the ~ame reasons, and such cement plugs will be added along theupward course of the probe bores as the pyrolysis operation upwardly progres~e~ from one bed deposit to the next cf . Fig . 1 ) .

:~3~

On the other hand, where the core sample analysis shows that for a given bore hole 7 location the formation eontains for instance 2Q oil shale beds, e.g. including 4 very rich beds of 42 gpt, 9 average rich beds of 30 gpt and 7 lean beds of 20 gpt, the sampling process is used only at the corresponding lowermost bed of each of three different types of beds, and in the case of the intervening bed sites, the probe bores are plugged progressively upwardly as aforesaid so that the pyrolysis operation at th~ intervening bed sites is carried out with the microwave unit 11 alone being used in the main bore hole 7.
In this instance, the recorded information obtained pursuant to the sampling process, using the probes at each of three different type bed sites, is immediately employed for carrying out-the pyrolysis operation with the mi~rowave unit 11 alone in the main borehole 7 for each of the subsequent above beds of the same type.
In all instances, the second changes in dielectric ~consta~t, and favorably the associated sensed changes in pre~ailing temperature, at the in situ bed level site being worked and the timing of such sensed changes incrementally along the course of the progressing pyrolysis operation to the outer limit of the recapture radius involved, and consequent changes and their timing incrementally along such course of the applied RF energy; e.g. initially at incrementally increasing and thereafter substantially constant continuous correspondingly increased radiation power and/or initially in intermittent cycles of on ana off duration at substantially constant or preferably incrementally increasing radiation power, and especially initially both at incrementally 10~

~3~ 6 increasing radiation power and in intermittent cycles of on and off duration in a first phase, and thereafter at substantially constant correspondingly increased power continuously in a second phase (e.g. per Figs. 2a and 2b);
i.e. in dependence upon such sensed changes and their timing, will provide recorded parameter information for repeating the pyrolysis operation at a separate borehole site of such porous media of substantially the same type without the need for such probes thereat.
On the basi~ of test operations for carrying out micro~ave heating of petroleum impregnated media such as oil shale to achieve selective microwave pyrolysis of the carbonaceous values, it has been determined that there is really no optimum frequency that is best suited for hydrocarbon heating in situ in the impregnated media in accordance with the present invention.
As earlier noted in this regard, the energy absorption by the organic matter in the impregnated media is fairly constant over a wide range of microwave frequencies as indicated by the relative stability of the dielectric constant over such wide range of fequencies.
The important factor is generally only that the microwave frequency selected be within the radar range, i.e.
significantly higher than sound wave frequencies or audio frequencies which range from about 15 to 20,000 cycles per second [cps) or about Q.015 to 20 kilocycles per second (kps), and thus the radar range contemplated radio frequencies or microwave frequencies will be generally higher than 20 kps or 0.2 M ~z (million cycles or me~acycles per second), such a~ at least about 0.3 M ~z and up to over 30,0 M Hz or up to over 30 G Hz (billion cycles or giga cycles per second), e.g.

~3~ 8~

typically from about 10 to 5,000 M Hz, especially about 750 to 4000 M Hz.
It will be realized, of course, that as the microwave frequency selected increases, the power r~equired to generate such frequency decreases, and the analogous antenna length requirements for the exposed portion of the proba end portion 34 relative to the end face 35 of the particular probe system 30, for sensing in effect changes in attenuated feedback frequency, is concomitantly decreased or shortened. Hence, -other things being equal, the use of higher RF microwaves is preferred since this results in a conservation of the electric power which must be expended (cf. Figs. 2a and 2b).
For instance, microwave pyrolysis experiments of actual resource oil shale samples were conducted equally well using a comparatively low microwave frequency of 915 M Hz and separately using a comparatively ~igh microwave frequency of 2450 M Hzo The only significant difference was that the lower frequency microwaves seemed to carry or impart more heat, while the higher frequency microwaves seemed to possess or cause a greater degree of penetration, into the sample.
Perhaps more significant to the microwave pyrolysis process according to the present invention is the practical consideration of the available RF equipment, such as the microwave unit 11, and its particular physical characteristics.
yor example, where a microwave frequency of 915 M Hz was used in an a~sociated wave guide for distributing the RF
radiation into the ~ample for pyrolysis of the carbonaceous content of the impregnated media, the wave guide needec~ to be considerably larger than that in the case o~ such pyrolysis ~3~

using a hlgher micro~ave frequency such as 2450 M Hz.
Depending on the nature and disposition, therefore, of the particular formation deposit of petroleum impregnated media, the dimensions of the microwave distributing equipment may have to be matched or modified for accommodating the same.
Thus, should smaller eguipment dimensions for a given microwave unit 11 be required in order to best serve the particular characteristics of a give~ formation deposit, e.g.
involving a wave guide arrangement of smaller physical dimensions for distributing the microwave radiation, then higher microwave fre~uencies will in turn be used concordantly therewith, and vice versa.
It will be realized in this regard, that although generally any frequency within the radar range may be used for providing the microwave energy for in situ pyrolysis of the petroleum impregnated media according to the present invention, the particular frequency selected will normally not be changed but instead will remain static or constant throughout the usual pyrolysis production operation.
In this regard, the changes in attenuat~d feedback frequency sensed by the probe systems 30, where used, as the pyrolysi~ progresses, may thus be measured against the static or constant ~icrowave source originating frequen~y as an unchanging reference frequency.
On the other hand, at such static or constant frequency, the radiation power will incrPmentally increase during the in situ pyrolysis operation, and/or the energy ~upplied time intervals of on-off power will vary selectively, i.e. as individual or conjoint functions of the total in situ petroleum impregnated media under treatment for optimum result~ ~cf. Pig~. 2a and 2b).

~3~2~6 As earlier noted, the applying of RF energy by continuous input of steady or constant level power, e.g. at static or constant frequency, is to be avoided sinc~ this has been determined to result in a decrease in the production rate, rather than to provide a nearly constant rate of production throughout, due to mineral, or even perhaps residual carbon, absorption of microwave energy which concomitantly increases as the length of the mineral or rock path increases in a direction away from the borehole 7.
Accordingly, a desirable primary feature of the present invention is the carrying out of the in situ pyrolysis with the use initially of incrementally increasing power, e.g. at constant frequency, and/or at associated varying time intervals of on-off power as the pyrolysis progresses along the extent of the deposit towaras the outer ~one represented by the pertinent recapture radius.
Of course, depending ~pon the characteristics of the particular formation deposit to be worked, a modified form of the microwave aistributing equipment such as microwave unit 11, may have to be provided, such as one having a wave guide system of smaller dimensions, e.g. for supplying microwave radiation at a higher frequency range or level such as that of a 3500 M Hz frequency range or higher.
I n any case, for convenience, once a given microwave unit 11 is provided of given characteri~tics and dimension~, including its wave guide dimensions which will normally determine its microwave operating frequency, the equipment will be fa~hioned to operate generally only at the 8pecific frequency chosen.

In line with such considerations, Table 1 above provides a typical time schedule of applied incrementally increasing RF power, obtainable for exa~nple at a con~tant frequency of 915 M Hz and also alternatively at a constant frequency of 2450 M Hz. The temperatures reachedalong the successive ring portions of the deposit are illustrated in Fig. 2b, in this regard. In essence, the deposit is progressively subject2d to the pyrolysis temperatures indicated~ since inherently such temperatures must be reached for the conditions to be sufficient to induce organic decomposition, 8~. at an average of about 450C, as specified in Table 3 above.
~ hese various parameters are ascertained by a spiral arrangement of probe systems 30 as ~hown in Figs. 4 and 5.
It has been determined that the petroleum production curve rises sharply as the radius of penetration increases and as the wattage applied is increased accordingly as indicated iD Fig. 2b. The production rate (PR) may be desig~ated as the square of the radius (r) from the borehole 7 to that distant circumferential point that is effectively penetrated by the applied wattage at maximum power, e.g. 100 KW as shown in Fig.
2b. The makeup of the recovered products for a 30 gpt yield, from 1 cubic foot of oil shale, on a 23.3 pound organic matter (and water) ~eight basis, and on a 485 ft3 organic matter (and water vapor) basis, is as earlier listed~
Under~tandably, product production is subject to several factors such as the gpt yield potential of the depo~it, the height or vertical thickness of the bed being radiated by the microwave energy, etc. Even on the conservative as~u~ption that~ or a given microwave unit 11 of conventional deqign, a three foot vertical thicknes~ of a ~3~ 36 given bed deposit is the maximum range that can be successfully worked by the microwave unit 11, i.e. without having to reposition the unit 11 at a higher level .in alignment with the contiguous next higher level of vertical thickness of the same bed deposit, such as in the case of an ~il shale bed deposit of for instance 6 or 9 feet in overall verti~al thicknecs, then based on likewise conservative as~umption of a 50~ recovery rate of 30 gpt oil shale at a yield of only 0.049 bbl per cubic foot in the three ~oot bed thickness range involved, a production rate of 0.147 bbl per square foot of area of the three feet thick deposit being worked will be obtained (i.e. 0.049 x 3).
At a corresponding area of microwave penetration of 4,000 ft2, i.e. a total circular area corresponding to a recapture radius of just under 36 feet (cf. Table l above), about 588 bbl of oil or petroleum product will be obtained (i.e~ 0.147 x 4000).
For a typical Wyoming formation of 20 oil shale beds (cf~ Fig. 1), 11,760 bbl of oil or p0troleum product per borehole 7 will be accordingly obtained (i.e. 20 x 588).
Advantageously, once a microwave pyrolysis ~peration has been conducted with an arrangement of probes as shown in Figs. 4 and 5, to provide the desired information along with that for instance resulting of actual resource samples obtained from representative formation bed deposits, whereby to optimize the conditions of microwave radiation for each given type deposit to be worked, a determination can be conveniently made as regards the power requirements for each given type bed deposit, or cumulatively for all succe~sive bed deposits at a given borehole 7 (c~. Fig. 1).

~3~

This representative programming information can thus be used concordan*ly at different boreholes 7 in the same type formation.
In this way, the production operatioll can be undertaken such that a large number of separate boreholes 7 may be worked at the same ti~e. Clearly, it is practical and especially very economical to power several RF generators or microwave units 11 and ass~ciated borehole 7 operations from one DC
generator such as electric generator 22 (Fig. 1~.
This is especially so in the ca~e of the preferred predominant use at l~ast initially of intermittent microwave power intervals of on-off RF energy in a given borehole 7 as illustrated in Figs. 2a and 2b.
More specifically, due to the very nature of such on-off usage, there is excess incremental DC power available form a given DC gene~ator for the powering of additional RF
generators or mlcrowave units 11 during the intermittent off intervals. If this excess available DC power is not used, it is in effect wasted, as DC generators must run constantly as d:ynamic generators, and cannot be stopped and started synchronously with the on-off power demand of the RF generator or microwave unit 11, eOg. at less than 10 second intervals of on and/or off duration cycles as ~hown in Fig. 2b.
Advantageously, therefore, the dynamically generated DC
electrical anergy i8 selectively alternately supplied concordantly in ~ucceRsi~e intermittent interval alternate or out of phase cycles of on and off duration to the corresponding plurality of microwave units 11. This is done ~uch that, for instance of ten given microwave units 11 in ten corxesponding boreholes 7 being worked simultaneously, the even numbered (e.g. second, fourth, sixth, eighth, and tenth) ~3~2~

units 11 are only energized during the alternate off duration cycles of the remainder or odd numbered (e.g. first, third, fifth, seventh and ninth~ units 11, and in turn the remainder or odd numbered units 11 are only energized during the concordant alternate off duration cycle~ of the even numbered units 11.
The counterpart out of phase on-o~f intervals need not be of equal duration ~cf. Fig. 2b) so long as the overall available DC energy delivered is sufficient to complement or supplement that otherwise wasted intermittent off cycl2 energy of the even units 11 used as on cycle ener~y fcr the odd units 11, and vice versa, as the artisan will appreciate.
This factor makes possible the eficient more or less complete use of the generated DC power by distrlbuting the same operatively so as to energize several microwave units 11 at separate respective boreholes 7 bein~ worked at the same time and conserves the available energy for power generation, e.g. the noncondensible gas portion of the production product recovered via the pipe,9 at a given borehole 7 installation.
~ urther advantages are gained by connecting together in conventional manner several DC generators 22 at dif~erent borehole 7 installations being si~ultaneou ly worked, as by electrically connecting the generators within a common grid cystem that is arranged for compensatingly powering the microwave units 11 at many borehole 7 installations at once.
In turn, several such grid systems may be interconnected for large field production endeavors.
Selective use of the DC power available from such a grid syRtem may be effectively eontrolled ~y computer in conventional manner. Thi~ i5 effected, for instance, in ~3~ 6 conjuncti~n with information indicated by the eq~ipment 36 obtained from the in situ permittivity p~obe system 30 (Fig.
3), and/or fr~m a spiral array arrangement of such probe systems (Figs. 4 and 5) where used, and also with information obtained from core sample analysis and from surface monitoring of the collected resource, i.e. production product, such that the pertinent information is fed into the computer program in conventional manner and the computer in turn æhunts or distributes the DC power to demand points within the operating field in the contemplated way.
The economic advantages of such a grid system are self evid~nt. Not only is the energy resource, e.g. recovered noncondensible gas, that is applied for power generation effectively cons~rved and efficiently used, but also the capital investment for large scale field development is lowered, i.e. the number of DC generators such as fuel cells, turbines, etc. needed is reduced.
In all appropriate instances, the RF eneryy is applied at each borehole 7 being worked to distribute the microwave energy for the desired purposes, such as at least initially at incrementally increasing radiation power or at least initially ~in intermittent cycles of on and off duration at substantially : ~ ~ constant or preferably incrementally increasing radiation power; e.g. initially at incrementally increasing power in a fir~t pha~e and thereafter at substantially constant continuous corresponding increased radiation power in a ~econd phase, or initially in intermittent cycles of on and off duration at su~stantially constant or pre~erably incrementally increaæing radiation power in a first pha~e and thereafter at substantially conætant correspondingly increa~ed power continuously in a second phase, or especially initial}y both ~3(~4~

at incrementally increasing radiation power and in intermittent cycles of on and off duration in a first phase and thereafter at substantially constant correspondingly increased power continuously in a second phase~
Such intermittent cycles of on and off duration are generally of a duration of less than 10 seconds, as aforesaid, e.g. at least about 1 second and at most about 3 to 6 seconds in intermittent duration cycles.
On the other hand, where such a grid system is used for simultaneously energizing a plurality of microwave units 11 at separate borehole sites, and the second phase is effected at constant correspondingly increased power continuously, a further portion of the noncondensible gas recovered is desirably used to produce the increased supply of electrical energy needed to energize simultaneously and continuously all of the microwave units 11 at such constant increased power.
Thus, by way of the present invention, an advantageous method is provided which u~es the selective application of RF
energy for heating the carbonaceous values, e.g. hydrocarbons, in situ, in vario~s underground formation deposits, such as kerogen in oil shale, bitumen in oil sands and tar sands, and heavy oils of high viscosity found in reservoirs located within rock or sand formations, etc.
The application of RF energy or electromagnetic energy for such heating is equally purposeful regardless of the nature of the petroleum impregnated porous media, i.e. oil shale, oil sands, tar sands, heavy oil reservoirq, etc., because the organic matter preferentially absor~s and is molecularly e~cited by the controlled microwave radiation, regardless of the in ~itu ~ource o~ the organic matter, and Z~3~

will be efficiently expelled under the pyrolysis conditions in relatively pure form, i.e. uncontaminated by air or its resultant combustion products with the attendant organic matter.
Moreover, the microwave heating and pyrolysis may be controlled for desired varying of the applied microwave frequencies, intermittent on and off cycle duration and intensity of low or high power or wattage for producing predictable results when working deposits of oil shale, oil sands, tar sands, heavy oils, etc., and in particular, liquid oil, oil vapors, noncondensible gases, residual carbon coke and w~ter in dependence upon the controlled wattage, frequency and rate of application of the microwave energy to the deposit, and while avoiding adverse local overheating and detrimental structural modification of the mineral content which might otherwise rob the overburden of necessary support.
An especial advantage of the present invention is the provided ability to control the amount of each type produ~t yielded by the microwave pyrolysis under the autogenous pressure.
Thus, by continued radiation of the initially produced oil, e.g. from kerogen, tar, and the like, such liquid will be transformed into condensible oil vapors, and by increased xadiation of these transformed oil vapors and any liquid oil, :
the same will be chemically broken down or catalyzed to noncondensible gases, thus permitting selective increase in .

the content of gases produced.

~36E~Z1~36 In turn, the remaining deposit of carbonaceous val~es in the bedding which is left as A result of this first step of the process and which constitutes residual carbon coke or solid form fixed carbon, will be subsequently gasified as well upon additional and continued RF radiation i~ the following second stepO
~ hese additionally produced gases, primarily carbon monoxide, will enrich the total of noncondensible gases readily obtainable according to the microwave winning process of the present invention, for use in various purposes, and especially to provide the power needed to generate the microwave energy for the underlying pyrolysis extraction at one or simultaneously a plurality of borehole sites, in addition to supplying large amounts of gases for the gas market, as a complement to the amounts of oil ~eing made available for the oil market.
Hence, versatile control of the microwave application under ~he autogenous pres~sure conditions will enable the process to be carried out for selectively varying the proportion of the recovered oil and condensible oil vapors, on the one hand, and of the recovered noncondensible gases, on the other hand.
~ hese advantages distinguish the present invention from conventional methods of production sinc~ it avoids the fluid transfer method bulk heating and Btu heat loss through di~sipation of in situ heating by hot water or æteam from a surface generating source, or even che~ically provided heat/
as well as the fired method bulk heating and oxygen contamination and combustion products attendant such oxygen contamination of sur~ace retorting in the presence of air or oxygen, and the similar inefficiencies of indirect heating of ~3~4;z1~6 a retorting vessel closed off from air, after having to win the rock and raise it to the ground ~urface for such retorting.
Besides being mor~ efficient than such bulk heating methods, in applying the required heating energy by microwaves, the present invention accomplishes the heating in precisely controllable manner whereas inherently there can be little, if any, control ov~r the desired results whether using hot water, steam or chemically provided heat for in situ heating or direct or indirect combustion energy supplied fired heat in a surface retort.
Although, on the other hand, the device of said V.S.
Patent 4,193,448 contemplates the use of microwave energy for in situ heating of underground petroleum impregnated porou~
mediaj it does not apprise the skilled artisan of the carrying out of a controlled microwave energy pyrolysis of the organic matter in the porous media to achieve not only liquid oil flow, but also the generation of both condensible and : noncondensible gasified carbonaceous constituents in controllable proportions, and in turn, the scavenging of the remaining carbon coke by further more intensified microwave pyrolysis for gasifying such residual carbon values, all in the substantial a~sence of air, let alone the use of the noncondensible gas product recovered, in whole or in part, as fuel for generating the required power for operating the microwave distributing source, and thereby efficiently utilizing this plentiful and comparatively ine~pensive gas by-produc neces arily produced under the contemplated pyrolysis condition~, yet without diminishing the amount of liquid oil product basically sought as ~ynthetic fuel in offsett:Lng any currently exi~tin~ or potential future energy crisis.

3~ 6 In this regard, it has been heretofore considered that approximately 85~ of the shale oil potentially available from oil shale could be recovered in liquid form without vaporization and condensation, which would suggest that lower heat inputs would be required for this technique than for the vaporization of the generated oil. In the early stages of pyrolysis, it has been found that enough bonds are broken in the hydrocarbon constituents for the kerogen to become a viscous liquid with a small portion of about 9 wt.% being converted to gas products.
By way of the present invention, the pyrolysis under the applied microwave radiation is carried out at selectively higher generation of gases, including not only volatilization of the liquid oil to condensible vapor for~, but also creation of comparatively large proportional amounts of noncondensible gases under autogenous pressure promoted molecular breakup.
These gases serve to drive the oil constituents from the pores of the shale or other porous media, and under more intense heating increasing proportions of the liquid oil will vaporize and be gasified to noncondensible form, such that any remaining li~uid pha~e oil will be effectively admixed with and entrained in the flow of the gases under autogenous pressure expelling ~rom the pores of the deposit and traveling to the point of recov~ry? e.g. the mi~rowave unit 11 in the borehole 7.
In the particular case of oil shale, e.g. that containing more than about 30 gpt, when subjected to heating at 425C the porous media begins to yield oil under the autogenous ga~ pressure. After the ligulfiable and gasiiable con~tituents at the seleeted pyrolysis temperature, e.g. 425-500C, have been created or generated, increased ~nergy ~3~ 6 recovery can be undertaken simply by continuing the microwave radiation for gasification of the residual solid carbon left in the shale at that point in the pyrolysis process. This solid carbon residue significantly amounts in some cases to about 25 wt.~ of the carbon originally pres~ent in the kerogen, and is not included in the Fisoher assay of pyrolysis products obtained from oil shale at the usual temperature, e.g. 425-~OOC.
Thus, advantageously by way of the present invention,after the initial stage pyrolysis of the kerogen and its removal, gasification of the æolid residual carbon may be undertaken by continuing the RF radiation at higher pyrolysis temperature, e.g. from about 525C to sufficiently below about 600C to avoid formation of product water. This subsequent sta~e of the overall pyrolysis is aided by the fact that at this point the shale or other porous media iB quite porous and permeable to gas flow therethrough since the voids which had prev1ously contained kerogen will have been emptied, whereupon the so11d carbon or coke gasification will efficiently occur throughout the volume of the thus far processed shale and essentially completely scavenge all extractable carbonaceous constituents remaiDi~ng at that point.
It will be appreciated that the forego1ng specification and accompanying drawings are set forth by way of illustration ;and not Iimitation, and that vari~ous modifications and changes may be made therein without departing from the spirit and scope of the present invention which is to be limited solely by the scope of the appended c1aims.

Claims (31)

1. Process for in situ recovery of extractable car-bonaceous values from under ground petroleum impregnated porous media comprising:
subjecting the underground petroleum impregnated porous media, in situ and in the substantial absence of air, to microwave radiation from a microwave distributing source substantially immediately adjacent the media and distributed at least initially at incrementally increasing radiation power, for heating the impregnated petroleum content preferentially relative to the corresponding porous media and progressively in a direction away from the microwave source and to a selective temperature of at least about 425° C and sufficiently for liquefying substantially the liquefiable petroleum constituents present which liquify at the corresponding heating temperature and in turn for causing the thereby formed mixture of liquified and gasified constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source; and recovering the migrating constituents from the vicinity of the microwave source; and wherein the radiation is distributed initially in intermittent interval cycles of on and off duration in a first phase, and thereafter is distributed substantially continuously in a second phase.

2. Process of claim 1 wherein the intervals of on duration progressively increase in the first phase.

3. Process of claim 2 wherein the intervals of off duration progressively decrease in the first phase.

4. Process for in situ recovery of extractable car-bonaceous values form underground petroleum impregnated porous media comprising:
subjecting the underground petroleum impregnated porous media, in situ and in the substantial absence of air, to microwave radiation from a microwave distributing source substantially immediately adjacent the media and distributed at least initially at incrementally increasing radiation power, for heating the impregnated petroleum content preferentially relative to the corresponding porous media and progressively in a direction away from the microwave source and to a selective temperature of at least about 425° C and sufficiently for liquefying substantially the liquefiable petroleum constituents present which liquify at the corresponding heating temperature and in turn for causing the thereby formed mixture of liquified and gasified constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source; and recovering the migrating constituents from the vicinity of the microwave source; and wherein the radiation is distributed initially at incrementally increasing radiation power in a first phase, and thereafter is distributed at substantially constant correspond-ing increased power in a second phase.

5. Process of claim 4 wherein the radiation is dis-tributed in intermittent interval cycles of on and off duration in the first phase, and thereafter is distributed substantially continuously in the second phase.

6. Process of claim 5 wherein the intervals of on duration progressively increase in the first phase.

7. Process of claim 6 wherein the intervals of off duration progressively decrease in the first phase.

8. Process for in situ recovery of extractable car-bonaceous values from underground petroleum impregnated porous media comprising:
subjecting the underground petroleum impregnated porous media, in situ and in the substantial absence of air, to microwave radiation from a microwave distributing source substantially immediately adjacent the media and distributed at least initially at incrementally increasing radiation power, for heating the impregnated petroleum content preferentially relative to the corresponding porous media and progressively in a direction away from the microwave source and to a selective temperature of at least about 425°C and sufficiently for liquefying substantially the liquefiable petroleum constituents present which liquify at the corresponding heating temperature and in turn for causing the thereby formed mixture of liquified and gasified constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source; and recovering the migrating constituents from the vicinity of the microwave source; and wherein the radiation is distributed initially at incrementally increasing radiation power and until the heating of the impregnated petroleum content has progressed to the linear extent of at least about 20 feet in at least one direc-tion away from the microwave source in a first phase, and thereafter is distributed at substantially constant correspond-ingly increased power in such direction in a second phase.

9. Process of claim 8 wherein the radiation is dis-tributed initially in intermittent interval cycles of on and off duration in the first phase, and thereafter is distributed substantially continuously in the second phase.

10. Process of claim 9 wherein the intervals of on duration progressively increase in the first phase.

11. Process of claim 10 wherein the intervals of off duration progressively decrease in the first phase.

12. Process of claim 8 wherein the temperature is between about 425°-500°C.

13. Process of claim 12 wherein the temperature is between about 425°-475°C for thereby forming a mixture of predominantly liquified constituents and a corresponding remaining minor amount of gasified constituents.

14. Process of claim 12 wherein the temperature is between about 476°-500°C for thereby forming a mixture of predominantly gasified constituents and a corresponding remaining minor amount of liquified constituents.

15. Process for in situ recovery of extractable car-bonaceous values from and underground petroleum impregnated porous media comprising:
subjecting the underground petroleum impregnated porous media, in situ and in the substantial absence of air, to microwave radiation from a microwave distributing source substantially immediately adjacent the media and distributed at least initially at incrementally increasing radiation power, for heating the impregnated petroleum content preferentially relative to the corresponding porous media and progressively in a direction away from the microwave source and to a selective temperature is between about 425°-500°C and sufficiently for liquefying substantially the liquefiable petroleum constituents present which liquify at the corresponding heating temperature and in turn for causing the thereby formed mixture of liquified and gasified constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source; and recovering the migrating constituents from the vicinity of the microwave source; and wherein in a first step, the radiation is distributed until substantially all of the liquefiable and volatilizable constituents present which concordantly liquify and gasify at the corresponding heating temperature have been liquified and gasified and in turn recovered, and thereby leaves a remainder content of residual unliquified and ungasified carbon con-stituents in the corresponding porous media; and in a second step, substantially without interruption, the porous media is thereafter subjected to continued radiation from the microwave source correspondingly for heating such residual carbon constituents to a selective temperature of at least substantially about 525°C and below about 600°C and sufficiently for gasifying substantially such residual carbon constituents and in turn for causing the thereby gasified residual carbon constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source, and the migrating gasified residual carbon constituents are then recovered from the vicinity of the microwave source.

16. Process of claim 15 wherein the microwave source is located in a well bore at a level adjacent an underground stratum of the porous media, and the migrating constituents are recovered from the vicinity of the microwave source via the well bore.

17. Process of claim 15 wherein the porous media are oil shale media, and the carbonaceous values include kerogen which is correspondingly pyrolyzed by said heating.

18. Process of claim 15 wherein a portion of the recovered constituents is used to produce electrical energy for energizing the microwave distributing source.

19. Process for in situ recovery of extractable car-bonaceous values from underground petroleum impregnated porous media, comprising:
in a first step, subjecting an underground stratum of the petroleum impregnated porous media, in situ and in the substantial absence of air, to microwave radiation from 3 microwave distributing source located in a well bore at a level substantially immediately adjacent such underground stratum, for heating the impregnated petroleum content to a selective temperature sufficiently for liquefying substantially the liquefiable petroleum constituents present which liquify at the corresponding heating temperature and for gasifying substantial-ly the volatilizable petroleum constituents present which gasify at such heating temperature and in turn, for causing the thereby formed mixture of liquified and gasified constituents to migrate under autogenous pressure through the porous media in a direc-tion toward the microwave source; and recovering the migrating constituents from the vicinity of the microwave source via the well bore;
the selective temperature being insufficient for liquefying and gasifying residual carbon constituents in the corresponding porous media and thereby leaving a remainder content of residual unliquified and ungasified carbon con-stituents therein; and in a second step, substantially without interruption relative to the first step, subjecting the porous media there-after to a continued radiation from the microwave source cor-respondingly for heating such remainder content of residual unliquified and ungasified carbon constituents therein to a selective increased temperature sufficiently for gasifying substantially such residual carbon constituents and in turn, for causing the thereby gasified residual carbon constituents to migrate under autogenous pressure through the porous media in a direction toward the microwave source; and recovering the migrating gasified residual carbon constituents from the vicinity of the microwave source via the well bore; and wherein the first step temperature is between about 425-400°C. and the second step temperature is at least substan-tially about 525°C. and below about 600°C.

20. Process of claim 19 wherein a portion of the recovered gasified constituents includes noncondensible gas and at least a portion of such noncondensible gas is used to produce electrical energy for energizing the microwave distributing source.

21. Process of claim 20 wherein the first step temperature is between about 476°-500°C. for thereby forming a mixture of predominantly gasified constituents and a corresponding remain-ing minor amount of liquified constituents.

22. Process of claim 21 wherein the porous media are oil shale media, and the carbonaceous values include kerogen which is correspondingly pyrolyzed by said heating.

23. Process for in situ recovery of extractable car-bonaceous values from underground petroleum impregnated porous media, comprising:
substantially simultaneously subjecting each of a plurality of separate individual sites of underground petroleum impregnated porous media, in situ and in the substantial absence of air, to microwave radiation from each of a corresponding plurality of microwave distributing sources substantially immediately adjacent the porous media at each such site respec-tively and distributed at least initially in successive inter-mittent interval alternate cycles of on and off duration and sufficiently for heating the impregnated petroleum content for extracting extractable carbonaceous value therefrom, while correspondingly at least initially selectively alternately supplying electrical energy concordantly in successive intermit-tent interval alternate cycles of on and off duration to the corresponding microwave sources, such that selectively some of the plurality of microwave sources are only energized during the alternate off duration cycles of the remainder of the microwave sources are only energized during the alternate off duration cycles of the remainder of the microwave sources are only energized during the alternate off duration cycles of said some of the microwave sources, for substantially complete utilization of said electrical energy; and recovering the thereby extracted carbonaceous values;
and wherein the radiation is distributed initially at incremen-tally increasing radiation power and in intermittent cycles of on and off duration in a first phase, and thereafter is dis-tributed at substantially constant correspondingly increased power to each of the microwave sources in a second phase under a concordantly increased supply of electrical energy sufficiently to energize substantially simultaneously and continuously all of the microwave sources at such constant increased power.

24. Process of claim 23 wherein at least a further portion of the recovered carbonaceous values is used to produce the increased supply of electrical energy used in the second phase.

25. Process of claim 23 wherein at least a portion of the recovered carbonaceous values is used to produce the electrical energy supplied to the plurality of microwave sources.

26. Process for in situ recovery of extractable car-bonaceous values from underground petroleum impregnated porous media, comprising:
subjecting the underground petroleum impregnated porous media in situ to microwave radiation from a microwave distributing source and distributed at least initially at incrementally increasing radiation power and sufficiently for heating the impregnated petroleum content for extracting extractable carbonaceous values therefrom; and recovering the thereby extracted carbonaceous values;
and wherein the radiation is distributed initially at incrementally increasing radiation power in a first phase, and thereafter is distributed at substantially constant correspond-ingly increased power in a second phase.

27. Process for in situ recovery of extractable car-bonaceous values from underground petroleum impregnated porous media, comprising:

subjecting the underground petroleum impregnated porous media in situ to microwave radiation from a microwave distributing source and distributed at least initially at incrementally increasing radiation power and sufficiently for heating the impregnated petroleum content for extracting extractable carbonaceous values therefrom; and recovering the thereby extracted carbonaceous values;
and wherein the radiation is distributed initially at incremen-tally increasing radiation power and in intermittent cycles of on and off duration in a first phase, and thereafter is dis-tributed at substantially constant correspondingly increased power continuously in a second phase.

28. Process for in situ recovery of extractable car-bonaceous values from underground petroleum impregnated porous media, comprising:
subjecting the underground petroleum impregnated porous media in situ to microwave radiation from a microwave distributing source and distributed at least initially in intermittent cycles of on and off duration and sufficiently for heating the impregnated petroleum content for extracting extractable carbonaceous values therefrom; and recovering the thereby extracted carbonaceous values;
wherein the radiation is distributed initially in intermittent interval cycles of on and off duration in a first phase, and thereafter is distributed substantially continuously in a second phase.

29. Process for in situ recovery of extractable car-bonaceous values from underground petroleum impregnated porous media, comprising subjecting the underground petroleum impreg-nated porous media in situ to microwave radiation from a microwave distributing source and distributed at least initially at incrementally increasing. radiation power and sufficiently for heating the impregnated petroleum content for extracting extractable carbonaceous values therefrom, and recovering the thereby extracted carbonaceous values;
and wherein the radiation is distributed initially in intermittent interval cycles of on and off duration in a first phase; and thereafter is distributed substantially continuously in a second phase.

30. Probe apparatus for in situ sensing of changes in the dielectric constant of extractable carbonaceous values in underground petroleum impregnated porous media during the subjecting thereof in situ to microwave radiation, comprising an open ended coaxial transmission line having an in situ probe end and a remote end, and including a conductive probe as core conductor insulated electrically from its counterpart coaxial conductive jacket as peripheral conductor and arranged for remotely adjustable axial movement relative to the jacket for extending the adjacent end portion of the probe a selective distance beyond the in situ probe end of the line to provide an adjustable length exposed probe end portion for embedding in such porous media, and indicating means arranged at the remote end of the line for indicating the sensed changes in such dielectric constant.

31. Probe apparatus for in situ sensing of changes in the dielectric constant of extractable carbonaceous values in underground petroleum impregnated porous media during the subjecting thereof in situ to microwave radiation, comprising:
an open ended coaxial transmission line having an in situ probe end and a remote end, and including a conductive probe as core conductor insulated electrically from its counter-part coaxial conductive jacket as peripheral conductor and arranged for axial movement relative to the jacket for extending the adjacent end portion for the probe a selective distance beyond the in situ probe end of the line to provide an adjus-table length exposed probe end portion for embedding in such porous media, with indicating means arranged at the remote end of the line for indicating the sensed changes in such dielectric constant; and an associated thermal analysis means having a sensing portion adjacent the in situ probe end for embedding in the porous media whereby to sense the prevailing temperature at the in situ probe site, said indicating means arranged for indicat-ing the temperature sensed by the sensing portion at the in situ probe site.