CA1127896A

CA1127896A - Radiant energy reflector device

Info

Publication number: CA1127896A
Application number: CA283,052A
Authority: CA
Inventors: Michael D. Boyd
Original assignee: Individual
Current assignee: Individual
Priority date: 1976-07-19
Filing date: 1977-07-19
Publication date: 1982-07-20
Also published as: IT1079347B; DE2732592A1; JPS5328442A; SE7708345L; FR2393331A1; GB1589163A

Abstract

TITLE

RADIANT ENERGY REFLECTING STRUCTURES

ABSTRACT

Radiant energy reflecting structures are described which are elongate and which have a plurality of reflecting elements on or in their surface. Each reflecting element has a "major axis" of reflection (the term "major axis" is defined in this specification) and a feature of the reflecting structures is that the direction of the "major axis" varies progressively with the transverse position of a reflecting element on the structure. The reflecting surfaces of the reflecting elements may be formed as corrugated, elongate, planar reflectors. Alternatively they may be formed as a known form of retro-reflective surface construction. Preferably, the reflecting surfaces are overlaid with a transparent medium. The structures may be used to construct louvred radiant energy screens.

Description

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This invention relates to radiant energy reflecting devices, and in particular concerns a radiant energy reflecting member which can be used to form a solar energy barrier or screen having a plurality-of reflecting members which are disposed in such a manner as to prevent the penetration of un~wanted energy by reflection into a shaded space. The invention has particular, but not exclusive, application to solar - energy screens which are constructed as louvred screens, latticed screens or folded or gathered screens. The term "louvred screens" will generally be understood to include venetian blinds, louvred storm windows, and louvred doors and shutters.
Other areas of application of the present invention include gr.illes to allow the passage o fluid media, but not radiant energy, for example, ventilation grilles for equipment and for buildings.
The reflecting member of the present invention utilises certain aspects of one form of "retro-reflection"
of energy. Retro-reflectors are reflecting bodies which reflect incident radiation back in the direction from which it is incident. They generally take one of three basic forms, namely (a) two or three planar reflectors at right angles to each other, (b) a lens with a mirror in its focal plane, and (c) a concave mirror with a - ~

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smaller mirror at or near its focus. Each of these basic forms may be eith r a first-surface reflector ~in which reflection occurs on the front face of the reflector) or a second-surface reflector tin which the incident radiation penetrates a transparent material~ the front surface of which constitutes the first face, and reflection occurs at the second or rear face of the transparent material).
The present invention has a number of similarities to these types of retroreflector surfaces, but the distinction between such surfaces and the present invention will become apparent as the description proceeds.
In more detail, the property of retro-reflection is exhibited where two reflectors are placed at right angles to each other. An incident energy ray in any plane which is reflected from one reflector to the other will be reflected in a parallel (but displaced) plane. Furthermore, if three reflectors are placed at right angles to each other (so as to form the internal corner of a cube), an incident energy ray which is reflected sequentially from each of the three reflectors, will be reflected in a parallel (but displaced) path. Such reflectors are known variously as retro-reflectors, retro-directive mirrors~
and cube-corner reflectors. This principle is further described, for example, in the l'Encyclopedia of Science and Technology" published by the McGraw-Hill Book Company, . ~ :

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Inc., in 1960 under the headiny "Mirror Optics'l.
The closest prior art ~o the present invention is believed to be the venetian blind assembly illustrated in U.S. pa~ent specification No. 2l103,788 (to Mohrfeld)~ That specification discloses a slat for venetian blinds and the like in which one surface of the slat has a plurality of longitudinally extending, adjoining, narrow, highly reflecting surfaces disposed at an angle of approximately 45~ to the plane of the slat and at angles of approximately 90 to each other. Such a surface comprises a two-plane, first-surface retro-reflector as discusse`d above, and such a surface does operate to reduce the amount of solar energy penetrating into a space shaded b~ the venetian blind. However, blinds constructed in accordance with Mr. Mohrfeld's design suffer from a disad-vantage; they permit inward re-reflection of incident energy (as will be shown later).
Re-reflection of incident energy into the shaded space is also a problem with the highly reflective sur-faces disclosed in Australian patent speci~ication No. 203,859.
It is a prime ob~ective of the present invention to provide a radiant energy reflecting member which can be used in venetian blinds and the like and which are effective to reduce the transferrence of radiant energy _~_ ~7~6 into the shaded space by re-reflection.
According to the present invention, there is provided a radiant energy reflecting member comprising ~a) an elongate body; and (b) a p-lurality of reflecting elements formed in or attached to said body, said elements being located adjacent to each other, each element providing retro-reflection of all incident energy from one particular direction, said elements being arranged so that said particular direction varies progressively with the transverse position of the elements on said body.
Preferably the elements each comprise a pair of elongate reflecting surfaces inclined relative to each other.
Also, the elongate body is preferably a lamellar body.
In another aspect of the present invention, there is provided a radiant energy screen assembly comprising a plurality of radiant energy reflecting members of the present invention, having lamellar bodies, arranged in a louvre configuration. This aspect of the present invention is especially useful for the construction of light- and heat-screen assemblies such as blind assemblies, particularly venetian blind assemblies, for the exterior windows of buildings.

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The present invention, as will be seen, also encompasses radiant energy reflecting members of the ~ype defined above, in which a layer of transparent material is located on top of the reflecting surfaces of the reflecting elements.
The radiant energy reflecting members of the present invention may be formed in any suitable manner, including rolling, casting or stamping the desired reflective surface configuration into a body, such as venetian blind strip material, and subsequently (if necessary) applying a coating of a reflective material. Other methods o-f forming the radiant energy reflecting members will be described later.
-To further understand the present invention, this description will now contlnue with reference to the accompanying drawings, in which : -Figure 1 illustrates a portion of a known form of .radiant energy reflector device, namely the venetian blind slat construction chosen by Mohrfeld for the screen illustrated.and-described in his U.S. patent specification No. 2,103,788;
Figure 2 illustrates the retro-reflective property of the surface of the embodiment of Figure 1, and its failure to be retro-reflective :in general;
Figures 3 and 4 illustrate possihle re-reflection paths for incident radiant energy in louvred screen devices which incorporate slats having the structure of ~igure l;
Figures 5 and 6 are cross-sectional representations of alternative embodiments of radiant energy reflecting members constructed in accordance with the present invention;
Figures 7 and 8 illustrat~ a radiant energy reflec-ting member, constructed in accordance with the present invention, in the form of a second surface reflector;
Figures 9 and 10 illustrate a retro-reflective ~7--.~
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surface utilising a cube-corner reflector; and Fi~ures 11 to 14 illustrate further slat constructions, utilising lensjfocal plane mirror retro-reflectors and concave mirror/secondary mirror retro-reflectors, which the present inventor has designed.
Referring firstly to Figure 1, there is shown a two-plane first-surface retro-reflective device which consists o~ a longitudinally corrugated aluminium reflector having reflective surfaces A and B disposed substantially at righ~ angles to each other. Referring to Figure 2, which is a cross-section through two reflective surfaces of the device of Figure 1, it will be seen that, in general, when a beam of energy is incident upon.the reflective surface, a portion of the beam, typified by the illustrated beam 15 path 6-8, it will be reflected from the surface A to the surface B along the path 8-9 and, on re-reflection from the surface B, will emerge from the reflactor alon~ path 9-10 in a parallel plane. It will al.so be apparent from Figure

2 that another portion of the beam of energy incident upon the reflective surface, typified by beam paths 4-1 and 5-7, will be reflected once only to be scattered in direction 1-11 and 7-12. Thus it can be seen from this Figure that in general, only a portion of an incident beam of ener~y is `' ' ' ~ ' ~7~3~6 truly retro-reflected~ unless the incident beam strikes at one particular angle, which is illustrated by rays P-1-3-S and Q-7-9-R. Because the rays P-1-3-S and Q-7-9-R
are totally retro-reflected rays 7 and incident beams from all o~her direction are only partially retro-reflected, I
have termed the direction from which beams P, Q, R and S
are incident the "major axis" of the reflector ~those familiar with reflecting surfaces will recognise that, in the case of the slat of Figure 1, the "major axis" is a pencil beam, having cross-sectional dimensions which correspond to the peripheral shape of the slat, and whose direction is at right angles to the slat).
Thus, the "major axis" of a reElecting element is, at any point on that element, the direction from which every beam of electro-magnetic energy having a wavelength in the visible, near infra-red and near ultra-violet regions of the s~ectrum, will be -fully retro-reflected.
Figures 3 and ~ illustrate a venetian blind constructed of slats having the shape illustrated in Figure 1, positioned between imaging inner and outer surfaces, 17 and 18, res~ectively. From these Figures it can be seen how undesirable re-reflection o~ incident energy can occur.
Figure 3 illustrates a case in which slats C and D are oriented so that a ray entering along path 15 is deflected ~rom one slat to the next and into the shaded space along path 16. Similarly, referring to Figure 4, it can be seen that such undesirable re-reflection into the shaded space may take place when a high elevation beam 15 strikes the outer end of the reflector surface.D. It can be seen rrom these diagrams that, in practice, inward re-reflections from a low sun angle ~Figure 3) occur as a result of a beam such as beam 4-l-ll in Figure 2.
I have found that such single reflections from louvred screens having this type of slat construction can -be reduced if the reflecting facets on the edge of the screen slats on the shaded side of the screen are reduced from the profile 1-2-3 of Yigure 2 to, for example, profile 7-2-3 of Figure 2, and the reflec:ting facets on the other edge of the screen slats are simultaneously reduced from profile 1-2-3 of Figure 2 to, Eor example, profile 1-2 9 of Figure 2. That is, reflection of energy into the shaded space will be reduced if the slats which constitute the reflecting members of a louvred screen are shaped so that the "major axes" of the reflecting members vary pxogressively across the width of the screen. Clearly a similar result is obtained if a reflecting structure which is not a corrugated lamellar body, but nevertheless has a varying : "major axis", is used for the slats.
Figures.5 and 6 illustrate alternative embodiments '~ f~78~

incorporating such new reflecting members. Figure 5 illustrates a corrugated retro-reflective construction in which the included angles between reflecting elements remain unaltered at approximately 90, but the element widths are varied so that the energy reflecting member has a curved profile. The reflective sturcture shown in Figure 6 is also corrugated but the reflective surfaces are constructed so that the upper included angle between the reflective elements is 90 only at the mid-width point 10 of the lamellar structure. In this embodiment, alternate reflective facets no longer lie in parallel planes.
Figures 7 and 8 illustrate a further embodiment of the present invention r in which each reflecting element is a two-plane second-surface reflector. This structure may 15 conveniently be formed by extruding a transparent venetian blind slat with the corrugations on the underside, configured in accordance with the principles illustrated in Figures 5 and 6, then coating the underside of the slat with a reflec-tive film. Figure 8 is a cross-section thorugh such a 20 reflecting element and illustrates that a ray incident along path 6-1, strikes the surface of the transparent material at point 1, and is refracted along path 1-2. It is then reflected along path 2-8 to point 8 on the surface, where it is totally internally reflected. It then strikes the reflecting 25 surface at 4 and leaves the structure along path 5-7 at a different angle to the ray emerging along path 1-11 of Figure 2, but , ~ - : ' 7~

nevertheless at an angle which would be effective to prevent energy penetrating a louvred screen having .
slats made ln this fashion by re-reflection, as shown in Figures 3 and 4. Thus, by utilising this form of reflecting member, the undesirable reflections illustrated in Figures 3 and ~ may be further reduced or eliminated.
Turning now to Figures 9 and 10, there is shown a known form of three-plane, first-surface (Figure 9) and second-surface (Figure 10) reflector structure, namely an array of "cube-corner" reflectors, which may.be embodied in a curved venetian blind slat to form a radiant.energy reflecting member of the present invention.
When compared with similar two-plane reflectors, the reflec-ting structures of these Figures exhibit the further advantage that reflected incident energy is reflected in a parallel line, and not a parallel plane. Once again, this form of reflecting surface may be overlaid with a transparent medium, thus utilising the principles discussed above in relation to the embodiment of Figures 7 and 8.
It is also possible for energy reflecting members of the present invention to ~e constituted by a curved lens/focal plane mirror construction. As with two-plane and three-plane reflecting structures, these can provide retro-reflectivity in two dimensions (for example, in the form of an extruded transparent curved sheet with lens---1~--., .

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profile surfaces, mounted over a mirror-surfaced base member) or in three dimensions (for example, in the form of an array of glass spherical beads, suspended over a curved reflective surface). Figure 11 illustrates one such configuration in which elements 21 are transparent rods or spheres set in a matrix 22 of lesser refractive index, above a reflective base member 23. They may be - -first-surface reflective, (therefore with the reflector separate from the lens) or more commonly second-surface reflective, with the reflector attached to the rear of the lens system (for example, as shown in Figure 11). The advantage of such a reflecting structure is that non retro-reflection of the type illustrated in Figures 2 and 8 does not occur.
Figure 12 illustrates a modified form of the venetian blind slat of Figure 11. The slat of Figure 12 has an outer surface 51 comprising a matrix of glass bead lens element located in the surface of a transparent medium, above a reflecting surface 52.
The last form of energy reflecting member illustrated in the drawings is a curved lamellar body constructed as a concave mirror/secondary mirror retro~reflector (~or example, a "cats-eye" retro-reflector). In Figure 13, a concave mirror 31-32, which may be circular or parabolic in cross-section, has a small mirror 33 near its focus~ A typical ` ~

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~7~6 ray path 34-32 is retro-reflected through 180~ to emergy along ray path 31-35. As with other retro-reflec-tor types, these embodiments may be two-directional with longitudinally extending mirrors of constant cross-section, or they may be three dimensional, with primary mirrors formed of sphere segments, thus providing total retro-reflectivity rather than planar retro-reflectivity. In addition, reflection may be either first or second surface reflection, although the preferred form for the present application would be as second surface reflectors. Figure 14 is a cross-secticn through a venetian blind slat, in which 41 is the transparent body of the slat, elements 42 are a series of concave reflectors formed on the rear of the slat, and elements 43 are small secondary reflectors formed on the transparent face of the slat.
Finally, it should be noted that since the energy reflecting members of the present invention are effective to reduce the transmission of energy by re-reflection when incorporated into louvred screens, it is possible to make the inward facing surfaces o~ such screens highly reflec-tive, hence lowering their emissivity.
While the present invention has been described herein with reference to preferred embodiments, it wi.ll be generally understood by persons skilled in the art `i`: . i `

~l~278.~6 that various changes may be made and equivalents substituted for ~lements thereof without departing from the true spirit and scope of the present invention. -'' ,.

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Claims

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

1. A radiant energy reflecting member comprising (a) an elongate body; and (b) a plurality of reflecting elements formed in or attached to said body, said elements being located adjacent to each other, each element providing retro-reflection of all incident energy from one particular direction, said elements being arranged so that said particular direction varies progressively with the transverse position of the elements on said body.

2. A radiant energy reflecting member as defined in claim 1, in which each element comprises a group of planar reflecting surfaces inclined relative to each other.

3. A radiant energy reflecting member as defined in claim 1, in which said reflecting elements are elongate reflecting elements, located adjacent to each other with their longitudinal directions parallel to the longitudinal direction of said body, each of said elements comprising a pair of elongate reflecting surfaces inclined relative to each other.

4. A reflecting member as defined in claim 3, in which the surface of the body is formed into a corrugated surface of reflecting elements with the distance between the peaks of adjacent corrugations varying progressively transverse the body.

5. A reflecting member as defined in claim 4, wherein the peaks of said corrugations lie in a first plane, and the troughs of the corrugations lie in a second plane, which is parallel to said first plane.

6. A reflecting member as defined in claim 5, in which the included angle between the reflecting elements varies from 90° transversely across said body.

7. A reflecting member as defined in claim 4, in which the peaks of said corrugations lie in an arcuate surface which is arcuate in a direction transverse said body and both the included peak angles of the corrugations and the included trough angles of the corrugations are substantially 90°.

8. A reflecting member as defined in claim 4, in which said corrugations are filled with a transparent medium, to thereby form a smooth outer surface of said body.

9. A reflecting member as defined in claim 8, in which the outer surface of said transparent medium extends beyond the plane or curved cylindrical surface in which the peaks of the corrugations lie.

10. A reflecting member as defined in claim 1, claim 4, or claim 9, in which said body is a lamellar body.

11. A reflecting member as defined in claim 9, in which said body portion is a sheet of said transparent medium and said elements are established by forming the inverse of said corrugations in one surface of said sheet and establishing a reflecting surface in contact with said inversely-formed corrugations.

12. A reflecting member as defined in claim 11, in which the establishment of said reflecting surfaces is effected by depositing a reflecting material on said inversely formed corrugations.

13. A reflecting member as defined in claim 1, in which said elongate body is an elongate, transversely curved lamellar body and each said element comprises a three-plane reflector structure in the form of a "cube-corner"
reflector.

14. A reflecting member as defined in claim 13, including a transparent medium over-lying the reflecting elements.

15. A reflecting member as defined in claim l, in which said body is lamellar and each reflecting element comprises a lens adapted to focus energy on to a mirror.

16. A reflecting member as defined in claim 15, in which said lens is a cylindrical lens and said mirror is an elongate plane mirror, the axis of curvature of the cylindrical lens and the longitudinal direction of the plane mirror being parallel to the longitudinal direction of said body.

17. A reflecting member as defined in claim 15, in which said lens is a spherical lens and said mirror is a plane mirror.

18. A reflecting member as defined in claim l, in which said body is a lamellar body and said reflecting elements are formed as an array of glass beads extending over substantially the entire surface of said body, said surface of said body being constituted by a smooth, highly-reflecting material.

19. A reflecting member as defined in claim 1, in which each reflecting element comprises a concave mirror, at the focus of which is located a small planar mirror.

20. A radiant energy reflecting member as defined in claim 19, in which said concave mirror is an elongate mirror, the cross-sectional shape of the reflecting surface of which is parabolic, and said small planar mirror is an elongate planar mirror mounted at the elongate focus of the parabolic reflecting surface.