CA1231565A

CA1231565A - Photoradiator

Info

Publication number: CA1231565A
Application number: CA000434203A
Authority: CA
Inventors: Kei Mori
Original assignee: Individual
Current assignee: Individual
Priority date: 1982-08-26
Filing date: 1983-08-09
Publication date: 1988-01-19
Also published as: ES525139A0; IL69563A0; ES8500416A1; FI73061B; FI73061C; GR78682B; NZ205144A; US4585298A; AU544107B2; AU1761783A; AU2406984A; DK386583A; DK386583D0; IL69563A; FI832972A0; EP0103729A1; AU555460B2; NO833060L; FI832972A

Abstract

ABSTRACT
A photo radiator has an elongate light conducting member which is supplied with converged light at one end thereof. Light radiating portions are arranged on the light conductor so that the light propagating through the light conductor may stream out in any desired light amount distribution along the axis of the light conductor.
The radiating portions comprise spaced annular strips or spiral strips each being made of a material whose refract live index is larger than that of the light conductor.
A mirror is positioned at the other end of the light conductor to reflect components of the incoming light which are substantially parallel to the axis of the light conductor, thereby promoting efficient radiation of the incoming light through the radiating portions.

Description

I

P~IOTO~ADIATOR

BACKGROUND Ox THE INVENTION
The present invention relates to a photo radiator for effectively radiating light such as the sunlight to the ambience which is routed through a fiber optic cable or like light conducting member.
Effective use of solar energy is the key to energy saving today and has been studied in various fields active-lye or the most effective use of solar energy, solar energy has to be availed as it is without being trays-formed into thermal energy, electrical energy or like different kind of energy. In light of this, I have made various proposals for an illumination system which utilizes solar energy. The illumination system employs a fiber optic cable through which the sunlight converged by a lens or the like is conducted to a desired location to stream out thereat to illuminate the ambience.
In the illumination system of the type described, the light advancing through the fiber optic cable has direct tivity. Therefore, if the light is output at a simple cut end of the cable, it becomes radiated over an angle which is usually as small as about 46 degrees. The light streaming through the simple cut end of the cable would fail to evenly illuminate a desired space such as a room.
I have proposed in various forms a photo radiator which is designed to effectively diffuse light conducted by a fiber optic cable to provide even illumination over a wide range.
The present invention constitutes a farther I

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improvement over such predecessors.

SUMMARY Of' THE INVENTION
It is an object of the present invention to provide a photo radiator which allows light to be radiated in any desired quantity distribution in a desired direction along the periphery of a light conducting member.
It is another object of the present invention to provide a photo radiator which is capable of effectively radiating to the outside of a light conducting member even the light components which propagate through the light conducting member substantially parallel to the axis of the latter.
It is another object of the present invention to provide a generally improved photo radiator.
cording to the present invention, there is provided a photo radiator, comprising-- an elongate light conducting member for conducting converged light from one end to the other end thereof - radiating means for radiating the light there through to the ambience radially outwardly of the light conducting member, said radiating means comprising a plurality of radiating means positioned at spaced locations along the axis of the light conducting member; and - reflecting means for reflecting light incident thereon, said reflecting means being positioned at said other end of the light conducting member with a reflecting surface thereof faced inwardly of the light conducting member;
- said radiating means being constructed to set up a selective quantity distribution of the radiated light at least along an axis of the light conducting member;
- said radiating means being constructed such that US

the total quantity of light so radiated through each of the radiating means after being introduced into the light conducting member and light ski radiated through said radiating means after being reflected by the reflecting means, so + ski, has a specific value relative to the other radiating means, in which a selected amount of light So to be radiated from the radiating means satisfies the equation:

So = ( 1 Bit - 1 n where S = n (So ski), n is the number of the radiating means, By is a preselected value, and (1 i) ill the above and other objects, features and advantages of the present invention will become apparent from the following detailed description taken with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a side elevation of a photo radiator embodying the present invention;
Figures 2 and 3 are plots representing operational principles of the present invention US Figure 4 is a view similar to Figure 1 but showing another embodiment of the present invention Figure pa is a side elevation of another embodiment of the present invention;
Figure 5b is a section along line b-b of Figure pa;
Figures and 7 are side elevations of alternative light radiating means applicable to the present invention;
and Figures 8-12 are sections showing various mirror B

.

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configurations applicable to the present invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS
While the photo radiator of the present invention is susceptible of numerous physical embodiments, depending upon the environment and requirements of use, substantial numbers of the herein shown and described embodiments have been made, tested and used, and all have performed in an eminently satisfactory manner.

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~2;~6~i Refrying Jo Figure 1 of the drawings, a photora~iator embodying the present invention includes an elongate transparent light conducting member 10 made of silica glass or acrylic resin. One end of the light conducting member 10 connects to one end of a light conducting cable 12 the other end of which connects to a lens system (not shown). Light, such as the sunlight, is converged by the lens system into the cable 12 and routed there-through to the light conducting member 10.
A plurality of light radiating members in the form of annular strips 141-14n are carried on the light conduct ion 10 at spaced locations along the axis of the latter.
In this particular embodiment, four light radiators 141-14n are shown for convenience. Each light radiator 14 has a retractive index which is larger than that of the light conductor 10. A mirror 16 is rigidly mounted on the other end of the light conductor 10 such that its reflecting surface opposes the light input end. In this construction, the light propagates through the light conductor 10 as indicated by an arrow I while being reflected by the periphery of the light conductor 10 to stream radially outward at the individual light radiators 141-14n. The rest of the light, reached the mirror 16, is reflected thereby Jo follow the propagation path backward as indicated by an arrow R, while being radiated to the outside through the light radiators 141-14n.
For the description which will follow, the light conductor 10 is assumed to have a length L and carry the light radiators l41_14n at spacings Al' Q2' Q3~ Q4 and Q5. The radiation coefficients of the light radiators 141-14n are supposed to be I I and , respectively.
In accordance with a characteristic feature of the present invention, an arrangement is made such that light issues through the light radiators 141 14 in a desired quantity distribution along the axis of the light conductor US

10, thereby realizing any desired light distribution curve in illuminating the ambience.
Referring to Figures 2 and 3, the operational principles of the present invention will be described using the construction shown in Figure 1. Constants employed for the description are a total quantity of light introduced into the light conductor 10 from the cable 12, a quantity of light Row incident on the mirror 16, quantities of light sly so, so and so individually issuing from the light radiators 141, 142, 143 and 14 without the intermediary of the mirror 16, quantities of light so so so and 5'1 individually streaming through the light radiators 14n, 143, 142 and 141 after being reflected by the mirror 16, quantities of light If, It, It and It individually reaching the light radiators 141, 142, 143 and 144 upon entry into the light conductor 10 from the cable 12, quantities of light I'm, I'3,.I'2 and Ill individually reflected by the mirror 16 to become incident on the light radiators 14n, 143, 142 and 141, and a quantity of light I'm reflected by the mirror 16 to return to the light input end of the light conductor 10 where the cable 12 is located.
Supposing that the radiation coefficients at, I
an no in this embodiment) of -the light radiators 141, 142 14n are the same (represented by hereinafter), the quantity of light In reaching any one of the first to "n" light radiators counted from the cable side is expressed as:

If Ire En. (1) so Ire 1 En. (2) It (If Sloe 2 = (1 - Ire ( 1 2) En.

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So = It = Ire 1 2 En. (4) where is the absorption of the light conductor 10.
In the same manner, the quantity In at the "n" light radiator 14n is produced by:

n ( n-l Nile = (1 _ no 1 Ire Qj) En. (5) Thus, the quantity Sun radiated from the "n" light radiator is:

sun = awn = I - a) 1 Ire (j-l Jo En. (6) The quantity of light Row allowed to reach the mirror 16 in the above situation is expressed as:
0 ( n n) nil ) Ire (j-l j) En. I
nil where i L-The light reflected by the mirror 16 propagates backward through the light conductor 10 toward the light input end. Again, this part of the light is absorbed by the light conductor 10 or radiated through the light radiators 144, 143, 142 and 141. The quantity of light Ion reaching the "n (= 4)" light radiator is obtained as:

'n = (1 - Roy nil = (1 - I _ Noah Lo nil) En. (8) ~3~5i65i where is the reflection coefficient of the mirror 16.
Therefore, the quantity of light sin issuing from the "n" light radiator is:

Sun = inn (1 - (1 a) It nil En. (9) In the same manner, the quantity of light Ill reaching the first light radiator 14l is produced by:
I
lo I' = (It - s' ye 2 = (1 - I _ on l I AL Al) En. (lo) The light quantity sit emanating from the first light radiator 14l is:

2n-l -Allah - Q ) En. (11) 1 a 1 = (l - l - a) It The light amount I'm returned to the light input end of the light conductor lo is obtained as:

I' = (I' - sly clue Ire En. (12) In the above equations, light attenuation inside the light conductor lo may generally be represented by the following expression:

i (I i-l s isle ill nil = (l - lo _ on i It Lo jowl j) En. (13) In the equations shown above, because all the factors I, Ion I, L, n and the like are known, it is possible to ~23~,~6~

obtain the individual values sly so ... sun, Row sol, so ... Sun and Ill by determinirlg relations between 1 1' So s 2 sun + sun inasmuch as the number of unknowns and that of equations are the same. They in turn will provide the distances Al' Q2 ... On between the adjacent light radiators. Suppose, for example, that light input from the cable 12 into the conductor 10 is radiated by each light radiator by an amount six light reflected by the mirror 16 is radiated by the light -radiator by an amount sol, and an average amount of light actually radiated from the light radiators is So Then the light will stream through the individual light radiators in any desired quantity distribution under the following conditions:
s = 1 ill (So + S 1) where n is the number of the radiators;

So = (1 + i) where So is a desired (set) quantity of light to issue from a desired light radiator, and n (1 + Bit = 1, So = So lQi);

lsi + Soil - So <<
S i ' E

where E Jo 1 and on the order of 10 I for example.
It will thus be seen that if the spacings between the adjacent light radiators 141-14n are selected to satisfy the conditions stated above, light can be radiated in any desired quantity from each of the light radiators thereby setting up a desired light distribution curve ~L23~6~

along the axis of the light conductor lo If desired, the factor By may be made zero in order to emit a same quantity of light from all the light radiators 14l 14n.
This would illuminate the ambience evenly with a same intensity throughout the length of the light conductor lo In the above description, a desired light disturb-lion has been implemented by designing the spacings between adjacent light radiators as desired, while selecting a common radiation coefficient for all the lo radiators. Instead, the radiation coefficient may be varied from one radiator to another while forming the radiators at equally spaced positions on the light conductor lo in which case the various factors will be expressed as:
If = Ire En. (l') So = Ox En. (2') l (I s err (l I e 2~Q En. I

So ~2I2 = ~2(1 - Lowe Q En. (4') n hi - Snowily = Ire no Eke') n nun on Ire nay En. (6') Row = (In Snow = (l - e Eke') I' = (1 - Roy = (l - I) (l - joy LO En. (8') ~23~S~

S' = I
n n n = (1 no Jo Ire Alec) En. (9 Ill = (It - Sue a 10 = (1 Ire Allah Q) Eke') Sol = oilily

2 (1 Ire AL Q) En. (11') = (I 1 s 1) Ire Al En. (12') In conjunction with the above equations, the attenuation of light inside the light conductor 10 may be expressed as:

(1 isle (1 - Ire a(~n+l-i)Q) En.. (13') To summarize the embodiment described above, the elongate light conductor 10 carries thereon a plurality of annular light radiators 14 at spaced locations along the axis thereof. The distance between adjacent light radiators or the radiation coefficient of each light radiator may be selected so that any desired light ~L23~Lr.i6~

distribution curve is established along the axis of the light conductor 10. It will be seen that the radiation coefficient is determined by, for example, the width of the radiator, i.e. length thereof in the axial direction 5 of the conductor 10.
Referring to Figure 4, a second embodiment of the present invention is shown which is distinguished from the first by a spiral configuration of light radiators.
As shown, a plurality of spiral strips made of a light radiating material extend throughout the length of the light conductor 10l two spiral strips 201 and 202 being shown in the drawing. Again, any desired light radiation coefficient is achievable for each light radiator 201 or 22 by selecting a width or a pitch P of each light radiator accordingly, along the axis of the light conduct ion 10. The rest of the construction, including the mirror 16, is the same as in the first embodiment.
If desired, the radiators, whether annular or spiral may be formed each in a discontinuous configuration so that the resulting light distribution becomes uneven in the radial direction of the light conductor 10 as well.
A third embodiment of the present invention is shown in Figures Spa and 5b. A plurality of light radian ions, 221-224 extend individually along the axis of the light conductor 10. As jest shown in Figure 5b, the light radiators 221-224 are spaced from adjacent ones along the circumference of the light conductor 10. The widths of the light radiators, represented by the width W of the radiator 222, may be so determined along the axis of the light conductor 10 as to satisfy the equations previously shown, thereby setting up desired light distributions in the axial direction of the conductor 10.
While the light radiators described so far have comprised annular or spiral members each having a refractive index larger than that of the light conductor lo their role may be played by annular or spiral grooves formed in a light conductor. Such implementations will be outlined with reference to Figures 6 and 7.

In Figure 6, the elongate light conducting member lo is formed with a number of annular grooves 14'1-14'n at spaced positions along the axis thereof. In Figure 7, on the other hand, the light conducting member lo is formed with spiral grooves 20'l and 20l2 from one end to the other end thereof. It will be understood that the radiation coefficient may be distributed as desired by selecting, for example, a specific depth in the case of the annular grooves or a specific depth or a pitch in the case of the spiral grooves.
In the foregoing embodiments, the mirror 16 ~16') employed for efficient light radiation has been oriented perpendicular to the axis of the light conductor 10.
Generally, the light routed by the cable 12 into the light Z0 conductor lo includes components which are substantially parallel to the axis of the light conductor lo and this part of the light is allowed to directly reach the mirror 16 without being reflected by the periphery of the light conductor 10 or, if reflected, a small number of times.
Such light components tends to fail to stream through the light radiators as represented by the En. l12) or (12'). Reference will now be made to Figures 8-10 which individually illustrate other embodiments of the present invention designed to effectively steer even the sub Stan-tidally purl components to the ambience of the light conductor 10. In Figures Lowe, no light radiators are shown for the simplicity of illustration.
The light conductor 10 shown in each of Figures 8 and 9 is furnished with a mirror 16' which is formed convex to the light input end of the light conductor 10 go I

The conductor 10 in Figure 10 has a mirror 16' which is suitably inclined relative to the axis of the light conductor I In any of such constructions, substantially parallel components of light incident on the mirror 16' will become unparallel to the axis of the light conductor 10 when reflected by the mirror 16' and, therefore, will be reflected a larger number of times by the periphery of the light conductor 10 while propagating toward the light input end. This part of the light is more apt to break through the light radiators and thereby increase the light radiation efficiency of the photo radiator, compared to the case with the perpendicular mirror 16.
Modifications to the mirror configurations described above with reference to Figures 8 and 9 are shown in Figures 11 and 12, respectively. The mirror 16" in Figure 11 is concave to the light input end of the light conductor 10 and so is the mirror 16" of Figure 12~ It will be apparent that the mirrors 16" shown in Figures 11 and 12, like the mirrors 16' of Figures 8 and 9, effective-lye reflect substantially parallel components in different directions so that this part of the light may also stream through the light radiators before routed back to the light input end.
In summary, it will be seen that the present invention provides a photo radiator which, despite its simple con-struction, realizes any desired light quality distribution at least along the axis of a light conducting member and causes even substantially parallel light components entered the light conductor to be steered efficiently to the ambience.
Various modifications will become possible for those skilled in the art after receiving the teachings of the present disclosure without departing from the scope thereof. For example, the mirror 16 or 16' for reflecting substantially parallel light components may be replaced

3~S6' by the end of the light conductor itself where it is located, if that end is suitably treated to reflect the light components concerned in the same manner. Again, the reflecting end of the light conductor may be perpendicular or angled to the axis of the light conductor, or convex or concave to the other or light input end of the light conductor.

Claims

The embodiments of the invention in which an exclusive property of privilege is claimed are defined as follows:

1. Photoradiator, comprising:
- an elongate light conducting member for conducting converged light from one end to the other end thereof;
- radiating means for radiating the light therethrough to the ambience radially outwardly of the light conducting member, said radiating means comprising a plurality of radiating means positioned at spaced locations along the axis of the light conducting member; and - reflecting means for reflecting light incident thereon, said reflecting means being positioned at said other end of the light conducting member with a reflecting surface thereof faced inwardly of the light conducting member;
- said radiating means being constructed to set up a selective quantity distribution of the radiated light at least along an axis of the light conducting member;
- said radiating means being constructed such that the total quantity of light si radiated through each of the radiating means after being introducted into the light conducting member and light s'i radiated through said radiating means after being reflected by the reflecting means, si + s'i, has a specific value relative to the other radiating means, in which a selected amount of light Si to be radiated from the radiating means satisfies the equation:
Si = (1 + Bi) ?
where , n is the number of the radiating means, Bi is a preselected value, and (1 + Bi) = 1.

2. Photoradiator as claimed in claim 1, in which the reflecting means comprises a mirror.

3. Photoradiator as claimed in claim 2, in which the mirror is positioned perpendicular to the axis of the light conducting member.

4. Photoradiator as claimed in claim 2, in which the mirror is convex to said one end of the light conducting member.

5. Photoradiator as claimed in claim 2, in which the mirror is concave to said one end of the light conducting member.

6. Photoradiator as claimed in claim 2, in which the mirror is inclined relative to the axis of the light conducting member.

7. Photoradiator as claimed in claim 1, in which the reflecting means comprises said other end of the light conducting member which is treated for reflection.

8. Photoradiator as claimed in claim 7, in which said other end of the light conducting member is perpendicular to the axis of the light conducting member.

9. Photoradiator as claimed in claim 7, in which said other end of the light conducting member is convex to said one end.

10. Photoradiator as claimed in claim 7, in which said other end of the light conducting member is concave to said one end.

11. Photoradiator as claimed in claim 7, in which said other end of the light conducting member is inclined relative to the axis of the light conducting member.

12. Photoradiator as claimed in claim 1, in which the radiating means are positioned at equal distances along the axis of the light conducting member.

13. Photoradiator as claimed in claim 1, in which the radiating means are provided with a same radiation coefficient as each other.

14. Photoradiator as claimed in claim 1, in which the radiating means comprise annular spaced sprips of a light transmitting material formed on the outer periphery of the light conducting member, said material being higher in refractive index than the light conducting member.

15. Photoradiator as claimed in claim 1, in which the radiating means comprise annular spaced grooves formed in the outer periphery of the light conducting member.

16. Photoradiator as claimed in claim 1, in which the radiating means comprises a plurality of continuous radiating means extending along the axis of the light conducting member.

17. Photoradiator as claimed in claim 1, in which a total quantity of light si radiated through each of the radiating means after being introduced into the light conducting member and light s'i radiated through said radiating means after being reflected by the reflecting means, si + s'i, is determined as a function of a length of the light conducting member measured from said one end.

18. Photoradiator as claimed in claim 1, in which the radiating means comprise elongate strips formed on the light conducting member and made of a material having a larger refractive index thant the light conducting member.

19. Photoradiator as claimed in claim 18, in which each of the strips extends spirally along the axis of the light conducting member.

20. Photoradiator as claimed in claim 18, in which each of the strips extends linearly along the axis of the light conducting member.

21. Photoradiator as claimed in claim 1, in which the radiating means comprise grooves formed in the outer periphery of the light conducting member.

22. Photoradiator as claimed in claim 21, in which each of the grooves extends spirally along the axis of the light conducting member.