CA2254969C

CA2254969C - Liquid atomization process

Info

Publication number: CA2254969C
Application number: CA002254969A
Authority: CA
Inventors: Alfonso Ganan Calvo; Antonio Barrero Ripoll
Original assignee: Universidad de Sevilla
Current assignee: Universidad de Sevilla
Priority date: 1996-05-13
Filing date: 1997-02-18
Publication date: 2005-08-23
Anticipated expiration: 2017-02-18
Also published as: US6119953A; DE69714583D1; JP3664404B2; US6174469B1; US6241159B1; JP2000503591A; WO1997043048A1; EP0899017A1; DE69714583T2; CA2254969A1; EP0899017B1; JP2004268037A; JP2004000904A; ES2140998B1; ES2180931T3; ES2140998A1

Abstract

The object of the present invention is a liquid atomization procedure that uses appropriate geometric parameters and physical properties to ensure that the liquid to be atomized is discharged as a continuous, steady capillary microjet through a suitable orifice. The procedure relies on the microwithdrawal effect undergone by a liquid-gas interface when the gas is withdrawn from a point (orifice) near the liquid surface. The invented procedure is applicable to any mechanism involving homogeneous atomization of liquids (particularly electronic fuel injection).

Description

A LIQUID ATOMIZATION PROCEDURE
FIELD OF THE INVENTION
The present invention relates generally to the field of liquid atomization and more particularly to a procedure that uses appropriate geometric parameters and physical properties to ensure that the liquid to be atomized is discharged as a continuous, steady capillary microjet through a suitable orifice.
BACKGROUND OF THE TECHNIQUE
Combined withdrawal of an interface between two immiscible fluids (two liquids or a liquid and a gas) has recently been studied by authors such as E.O. Tuck and J.M. van den Broek ("A cusp-like free surface flow due to a submerged source or sink", J.
Austral. Math. Soc. Ser.
B., 25, 433-450, 1984); L.K. Forbes and G.C. Hocking ("Flow caused by a point sink in a fluid having a free surface", J. Austral. Math. Soc. Ser. B., 32, 231-249, 1990);
and T.J. Singler and J.F. Geer Singler ("A hybrid perturbation-Galerkin solution to a problem in selective withdrawal", Phys. Fluids A, 5, 1156-1166, 1993). It is acknowledged to be a particular case of a more general interfacial instability phenomenon known as selective withdrawallcombined withdrawal. Studies in this field have focused largely on the determination of parameters (e.g.
the distance from the sink to the free surface, the fluid density ratio, the surface tension between the fluids) at the onset of combined withdrawal (i.e. of sweeping of the fluid behind the free surface when the fluid in front of it is withdrawn at a given distance from the surface).
However, the fluid dynamics of the microjet produced by combined withdrawal seemingly remains unexplored. The observation and study of the microjet, its peculiar properties and its potential uses, led to the present atomization procedure.
Existing atomization methods convert the type of energy supplied to the system (e.g.
kinetic energy of the gas in pneumatic atomizers, electrical energy in sonic and ultrasonic piezoelectric atomizers, mechanical energy in rotary atomizers, electrostatic energy in electrohydrodynamic atomizers, etc.) into surface tension free energy since the liquid-gas surface is dramatically expanded by the effect of these processes. As a function of the resulting degree of disorder, part of the energy is also degraded in the statistical dispersion of the resulting drop sizes. Depending on how disorderly and rapidly (or gradually and efficiently) the processes by which the above-mentioned energies are converted into free surface energy take place, the resulting sprays are suitable for different specific uses.
As a rule, the spray should consist of small drops of uniform size. A small drop size is always in conflict with a high flow-rate in the fluid to be atomized, which results in high energy use per time unit. Also, uniformity in drop size relies on gradual, non-turbulent, scarcely random processes that are incompatible with the rapid conversion of volumetric energy into surface energy required by the typically high liquid flow-rates involved in many cases and with technological simplicity in the atomizer. Mechanical simplicity and expeditiousness in the atomizer, and irreversibility and randomness in the atomization process, are all highly correlated.
Existing pneumatic atomizers involve the cascading breaking of the interface from a high Weber number to a unity Weber number, the latter being accomplished when drop diameters are such that surface tension forces offset the inertia of the gas relative to the liquid. Such atomizers include the straightforward coaxial model of S. Nukiyama and Y. Tanasawa ("Experiments on the atomization of liquids in the airstream", Trans. Soc. Mech. Eng. Jpn., 5, 68-75, 1939) or the airblast models developed by LD. Wigg ("Drop-size predictions for twin fluid atomizers," J.
Inst. Fuel, 27, 500-505, 1964), G.E. Lorenzetto and A.H. Lefebvre ("Measurements of drop size on a plain jet airblast atomizer", AIAA J., 15, 1006-1010, 1977), A.K. Jasuja ("Plain jet airblast atomization of alternative liquid petroleum fuels under high ambient air pressure conditions", ASME Paper 82-GT-32. 1982), and N.K. Risk and A.H. Lefebvre ("Spray characteristics of plain jet-airblast atomizers", Trans. ASME J. Eng. Gas Turbines Power, 106, 639-644, 1983), among many others, or that reported by A. Unal ("Flow separation and liquid rundown in gas-atomization process", Metall. Trans. B., 20B, 613-622, 1989), based on the coaxial atomization of a liquid metal using a supersonic gas flow.
Cascading processes in existing pneumatic atomizers involved highly turbulent flows and randomness, which result in highly disperse drop size and atomizates.
One other major disadvantage of this type of atomizer is the limited sizes it provides (above 20 microns on average at best).
Whistling atomizers also have their pitfalls, prominent among which are noise, a relative complexity - they use wave generators and piezoelectric devices to excite the capillary jet produced -, and a limited drop size (usually larger than 50 p,m).
One novel atomization system that also provides extremely small, monodisperse drop sizes is electrostatic or electrospray atomization. The system has been disclosed (e.g. by M.L. Colelough and T.J. Noakes, "Apparatus and process for producing powders and other granular materials", European Patent EP0250164 B 1 ). The chief disadvantage of this method in many cases is that it requires using a high-voltage do source - which poses serious problems - and hence a discharge system (e.g.
electrical crowns), both of which add up to the inherent complexity, large weight and low manipulability of this system.
SUMMARY OF THE INVENTION
The present invention is a liquid atomization procedure based of the withdrawal of the liquid to be atomized by a gas flow. The liquid flows through a feeding point housed in a pressure chamber. The feeding point faces an orifice that communicates the pressure chamber with the outside. The withdrawing gas flows across the chamber and surrounds the liquid to be atomized, delivered by the feeding point, to form the atomizate.
The object of this patent application provides drops of extremely small (1 micron or less) and highly monodisperse size (depending on the operating conditions, the relative standard deviation is 10-30%) The proposed system also possesses the simplicity and economy of a pneumatic system. In addition, the drop size can be adjusted at will via the flow-rate of the injected liquid and the pressure drop across the pressure chamber, from which the liquid jet is concentrically and axially withdrawn.
The capillary microjet formed by liquid flowing from the feeding point to the exit of the pressure changer is accelerated and stabilized by tangential viscous stress exerted by the gas on the liquid surface. The microjet leaves the pressure chamber through the exit orifice and then splits into microdrops with the following properties:

(1) an extremely small size (1 micron or less) resulting from breakage of the capillary microjet, and (2) very low size dispersion provided the jet diameter is stable, which is the case as long as the liquid flow-rate of the jet is stable.
This invention provides a device for atomizing a liquid, comprising:
a feeding source comprising an opening at a first end for adding liquid to an internal channel of the 'feeding source, which channel leads to an exit opening from which liquid is expelled in a flow path of liquid; and a pressure chamber having a first opening into which gas is added and a second opening at which the gas is accelerated and expelled from the pressure chamber, wherein the exit opening of the feeding source is positioned in the pressure chamber relative to and in front of the second opening so that in use, a stable liquid-gas interface is maintained in the flow path of liquid before entering the second opening and liquid in the flow path forms a stable capillary jet.
This invention also provides a method of creating an aerosol, comprising:
forcing a liquid through a channel of a feeding source in a manner which causes the liquid to be expelled from an exit opening;
forcing a gas through a pressure chamber in a manner which causes the gas to exit the pressure chamber and be accelerated at an opening positioned in front of a flow path of liquid expelled from the exit opening of the feeding source;
wherein a stable liquid-gas interface is maintained and the liquid forms a stable capillary jet between the feeding source exit opening and the opening of tree pressure chamber.
This invention also provides a method of creating an aerosol, comprising:
feeding liquid through a feeding source to an outlet;
accelerating a flow of gas through an orifice positioned in front of'the feeding source outlet in a direction parallel to a direction of flow out of the feeding source outlet; , wherein the feeding of liquid and the flow of gas are each at a rate relative to each other so as to maintain a stable capillary microjet of liquid which enters thc~ orifice and thereafter forms aerosolized particles.

BRIEF DESCRIPTION OF THE FIGURE
Figure 1 is a schematic depiction of an atomizer of the invention.
DETAILED DESCRIPTION OF THE INVENTION
Formation of the microjet and its acceleration are based on the abrupt pressure drop associated with the steep acceleration experienced by the gas on passing through the orifice. This results in a large pressure difference between the liquid and gas, which in turn produces a highly curved zone on the liquid surface near the orifice and in the formation of a cuspidal point from which a steady microjet flows provided the amount of liquid withdrawn through the orifice is replenished.
The parameter window used ( i . a . the set of special values 2o for the liquid properties, flow-rate used, feeding needle diameter, pressure ratio, etc.) should be large enough to be compatible with virtually any liquid (dynamic viscosities in the range from 10'4 to 1 kg m'1 s-1) : in this way, the capillary microjet that emerges from the end of the feeding needle is absolutely stable and perturbations produced by breakage of the jet cannot travel upstream. Downstream, the microjet splits evenly shaped drops simply by effect of capillary instability (see, for example, Raileigh, "On the instability of jets", Proc. London Math. Soc., 4-13, 1878), similarly to a laminar capillary jet falling from a half-open tap.
When the stationary, steady regime is reached, the capillary jet that emerges from the end of the drop at the outlet of the feeding point is concentrically withdrawn into the nozzle. After the jet emerges from the drop, the liquid is accelerated by tangential sweeping forces exerted by the gas stream flowing on its surface, which gradually decreases the jet cross-section.
The forces exerted by the gas flow on the liquid surface should be steady enough to prevent surface oscillations. Therefore, any turbulence in the gas motion should be avoided:
even if the gas velocity is high, the characteristic size of the orifice should ensure that the gas motion is laminar (similarly to the boundary layers formed on the jet and on the inner surface of the nozzle or hole):
In summary, the gas flow, which effects the liquid withdrawal and its subsequent acceleration after the jet is formed, should be very rapid, but also uniform, in order to avoid perturbing the fragile capillary interface (the surface of the drop that emerges from the jet) and hence its breaking. Therefore, the dynamic forces exerted by the gas should never exceed the surface tension (drop and microjet) at any time during the process. In terms of non-dimensional fluid dynamics numbers, the Weber number (i.e. the dynamic to surface tension force ratio) should not exceed unity during the process. The Weber number for the microjet will inevitably be unity because the pressure drop in the gas is similar in magnitude to the effect of the surface tension:
2Y 1 va d ~ 2P g where Y and p are the surface tension and liquid density, respectively; and d~
and vg are the characteristic diameter of the jet and characteristic velocity of the gas.
Also, the velocity of the gas around the drop that produces the jet must be related to that across the orifice via the areas, i. e. I~gDo' ~ vgdol, where Vg is the velocity of the gas around the drop, and Do and d" are the diameters of the feeding point and orifice, respectively. Since the maximum possible gas velocity at the orifice is similar to the speed of sound, one has d 2 V ~ ° X 320 m/s D

and, for the jet diameter, 4y 4 < 2 ~ 10 S gym (y - 2 . lOz Nlm 2 for n -heptane) p v ? 1.2 < 3202 rr This suggests that micrometric drop sizes can be obtained.
At the smallest diameters possible with this system (similar to the thickness of the boundary layer), the kinetic energies per unit volume of the liquid and gas should be of the same order. The resulting liquid velocity will be ys Yi~ P8 v ~ 10 mls pl s where pl is the liquid density. From the previous equation, the liquid flow-rate turns out to be ~l -". dj2vl "' 1 ~-11 m3/S
at the smallest drop sizes.
The gas flow should be laminar in order to avoid a turbulent regime -turbulent fluctuations in the gas flow, which has a high frequency, would perturb the liquid-gas interface.
The Reynolds numbers reached at the orifice are vd Re = g ° ~ 4000 v s where vg is the kinematic viscosity of the gas. Even though this number is quite high, there are large pressure gradients downstream (a highly convergent geometry), so a turbulent regime is very unlikely to develop.
The essential difference from existing pneumatic atomizers (which possess large Weber numbers) is that the aim is not to rupture the liquid-gas interface but the opposite, i.e. to increase the stability of the interface until a capillary jet is obtained. The jet, which will be very thin provided the pressure drop resulting from withdrawal is high enough, splits into drops the sizes of which are much more uniform than those resulting from disorderly breakage of the liquid-gas interface in existing pneumatic atomizers.

The proposed procedure for atomizing liquids can be used for electronic fuel injection as well as in inhalers for delivery of drugs or anaesthesia and in nebulizers for chemical analyses, among others. Also, it affords mass production of ceramic powders and sintering semiconductors used to manufacture ceramic materials, semiconductors, plastics, etc.
In order to complement the above description and facilitate understanding the invention, this report includes an illustrative rather than limitative plan for a prototype model.
Figure 1: Schematic depiction of an atomizer prototype.
1. Feeding needle.
2. End of the feeding needle used to insert the liquid to be atomized.
3. Pressure chamber.
4. Orifice used as gas inlet.
S. End of the feeding needle used to evacuate the liquid to be atomized.
6. Orifice through which withdrawal takes place.
7. Atomizate (spray).
Do = diameter of the feeding needle; do = diameter of the orifice through which the microjet is passed; a = axial length of the orifice through which withdrawal takes place; H = distance from the feeding needle to the microjet outlet; Po = pressure inside the chamber; P~ = atmospheric pressure.
EXEMPLARY USES OF THE INVENTION
The proposed atomization system obviously requires delivery of the liquid to be atomized and the gas to be used in the resulting spray. Both should be fed at a rate ensuring that the system lies within the stable parameter window. Multiplexing is effective when the flow-rates needed exceed those on an individual cell. The flow-rates used should also ensure the mass ratio between the flows is compatible with the specifications of each application.
Obviously, the gas can be externally supplied at a higher flow-rate in specific applications (e.g. burning, drug inhalation) since this need not interfere with the atomizer operation.

The gas and liquid can be dispensed by any type of continuous delivery system (e.g. a compressor or a pressurized tank the former and a volumetric pump or a pressurized bottle the latter). If multiplexing is needed, the liquid flow-rate should be as uniform as possible among cells; this may entail propulsion through several capillary needles, porous media or any other medium capable of distributing a uniform flow among different feeding points.
Each individual atomization device should consist of a feeding point (a capillary needle, a point with an open microchannel, a microprotuberance on a continuous edge, etc.) 0.05-2 mm (but, preferentially 0.1-0.4 mm) in diameter, where the drop emerging from the microjet can be anchored, and a small orifice 0.05-2 mm (preferentially 0.1-0.25 mm) in diameter facing the drop and separated 0.1-2 mm (preferentially 0.2-0.5 mm) from the feeding point. The orifice communicates the withdrawal gas around the drop, at an increased pressure, with the zone where the atomizate is produced, at a decreased pressure.
The atomizer can be made from a variety of materials (metal, plastic, ceramics, glass);
the choice is dictated by the projected application.
Figure 1 depicts a tested prototype where the liquid to be atomized is inserted through one end of the system (2) and the propelling gas in introduced via the special inlet (4) in the pressure chamber (3). The prototype was tested at gas feeding rates from 100 to 2000 mBar above the atmospheric pressure Pa at which the atomized liquid was discharged.
The whole enclosure around the feeding needle (1) was at a pressure Po > Pa. The liquid feeding pressure, P,, should always be slightly higher than the gas propelling pressure, Po.
Depending on the pressure drop in the needle and the liquid feeding system, the pressure difference (P, - Po > 0) and the flow-rate of the liquid to be atomized, Q, are linearly related provided the flow is laminar - which is indeed the case with this prototype. The critical dimensions are the distance from the needle to the plate (H), the needle diameter (D"), the diameter of the orifice through which the microjet (6) is discharged (do) and the axial length, e, of the orifice (i.e. the thickness of the plate where the orifice is made). In this prototype, H was varied from 0.3 to 0.7 mm on constancy of the distances (D" = 0.45 mm, d" - 0.2 mm) and a - 0.5 mm. The quality of the resulting spray (7) did not vary appreciably with changes in H provided the operating regime (i.e. stationary drop and microjet) was maintained. However, the system stability suffered at the longer H distances (about 0.7 mm). The other atomizer dimensions had no effect on the spray or the prototype functioning provided the zone around the needle (its diameter) was large enough relative to the feeding needle.

Claims

WHAT IS CLAIMED IS:

1. A device for atomizing a liquid, comprising:
a feeding source comprising an opening at a first end for adding liquid to an internal channel of the feeding source, which channel leads to an exit opening from which liquid is expelled in a flow path of liquid; and a pressure chamber having a first opening into which gas is added and a second opening at which the gas is accelerated and expelled from the pressure chamber, wherein the exit opening of the feeding source is positioned in the pressure chamber relative to and in front of the second opening so that in use, a stable liquid-gas interface is maintained in the flow path of liquid before entering the second opening and liquid in the flow path forms a stable capillary jet.

2. The device of claim 1, wherein the exit opening of the feeding source has diameter (D0) and its position in the pressure chamber relative to the second opening is such that, in use, liquid flowing out of the exit opening of the feeding source is surrounded by gas of the pressure chamber to form a liquid jet having a diameter d j, which diameter is defined by the formula:
wherein .gamma. is surface tension of the liquid, .RHO. is density of the liquid and V g is velocity of the gas.

3. The device of claim 1 or 2, wherein the exit opening of the feeding source has a diameter in the range of from 0.05 mm to 2 mm, and the second opening of the pressure chamber has a diameter in the range of 0.05 mm to 2 mm.

4. The device of claim 1 or 2, wherein the exit opening of the feeding source has a diameter in the range of from 0.1 mm to 0.4 mm and the second opening of the pressure chamber has a diameter in the range of 0.1 mm to 0.25 mm.

5. The device of any one of claims 1 to 4, wherein the feeding source is a feeding needle.

6. The device of any one of claims 1 to 5, wherein the exit opening of the feeding source is positioned at a point in the range of 0.2 mm to 0.5 mm from the second opening of the pressure chamber.

7. A method of creating an aerosol, comprising:
forcing a liquid through a channel of a feeding source and expelling the liquid from an exit opening;
forcing a gas through a pressure chamber in a manner which causes the gas to exit the pressure chamber and be accelerated at an opening positioned in front of a flow path of liquid expelled from the exit opening of the feeding source;
wherein a stable liquid-gas interface is maintained and the liquid forms a stable capillary jet between the feeding source exit opening and the opening of the pressure chamber.

8. The method of claim 7, wherein the exit opening of the feeding source has a diameter (D0) and its position in the pressure chamber relative to the opening is such that liquid flowing out of the exit opening of the feeding source is surrounded by gas of the pressure chamber to form a liquid jet having a diameter d j, which diameter is defined by the formula:
wherein .gamma. is surface tension of the liquid, .RHO. is density of the liquid and V g is velocity of the gas.

9. The method of claim 7 or 8, wherein the liquid has a viscosity in a range of from 10 -4 to 1 kg/m/sec.

10. The method of claim 7 or 8, wherein the liquid has a viscosity in a range of from 0.3 × 10 -3 to 5 × 10 -2 kg/m/sec.

11. The method of any one of claims 7 to 10, wherein the liquid is forced through the channel at a rate in a range of 0.01 nl/sec to 100 µl/sec.

12. The method of any one of claims 7 to 10, wherein the liquid is forced through the channel at a rate in a range of 1 nl/sec to 10 µl/sec.

13. The method of any one of claims 7 to 12, wherein the gas is forced through the opening of the pressure chamber at a rate in the range of from 50 m/sec to 2000 m/sec.

14. The method of any one of claims 7 to 12, wherein the gas is forced through the opening of the pressure chamber at a rate in the range of from 100 to 500 m/sec.

15. The method of any one of claims 7 to 14, wherein the exit opening of the feeding source is circular having a diameter in the range of from 0.1 mm to 0.4 mm and wherein the opening in the pressure chamber is circular and positioned directly in front of the exit opening of the feeding source and has a diameter in the range of 0.1 mm to 0.25 mm.

16. A method of creating an aerosol, comprising:
feeding liquid through a feeding source to an outlet;

accelerating a flow of gas through an orifice positioned in front of the feeding source outlet in a direction parallel to a direction of flow out of the feeding source outlet;
wherein the feeding of liquid and the flow of gas are each at a rate relative to each other so as to maintain a stable capillary microjet of liquid which enters the orifice and thereafter forms aerosolized particles.

17. The method of claim 16, wherein the outlet of the feeding source has a diameter (D0) and is positioned relative to the orifice such that liquid flowing out of the outlet of the feeding source is surrounded by gas to form a liquid jet having a diameter d j, which is defined by the formula:
wherein .gamma. is surface tension of the liquid, .RHO. is density of the liquid and V g is velocity of the gas.

18. The method of claim 16 or 17, wherein the gas is forced into an area around the feeding source outlet at a pressure in the range of 100 to 2000 mBar above atmospheric pressure.

19. The method of claim 16, 17, or 18, wherein the liquid has a viscosity in the range of from 10 -4 to 1 kg/m/sec.

20. The method of any one of claims 16 to 19, wherein the gas surrounds the liquid exiting the feeding source outlet, which liquid and gas are drawn into the orifice concentrically and the liquid forms a microjet which disassociates and forms aerosolized particles which are uniform in size to the extent of having a relative size standard deviation of 10 to 30%.