FIELD OF THE INVENTION
[0001] The present invention relates to a light apparatus useful for illuminating transparent
displays.
BACKGROUND OF THE INVENTION
[0002] Illuminated displays which display images carried on a transparent substrate are
well known, and are often used as advertising or other displays. Such displays typically
have a housing which is enclosed except for a front light opening, across which the
transparency carrying the image is to be positioned. A light source is positioned
within the housing and behind the transparency. A plurality of elongated light sources,
such as fluorescent tubes, are usually used as the light source. In order that the
light source itself is not observed through the image carrying transparency, a diffuser
in the form of a diffusing sheet, may be positioned between the light source and the
transparency. Displays of the foregoing type may be used for transparencies carrying
a regular two-dimensional image, such as formed from a photograph. More recently it
has been known to use a transparency carrying an integral image.
[0003] Integral image elements which use a lenticular lens sheet, fly's eye lens sheet,
or barrier strip sheet and a three-dimensional integral image aligned with the sheet,
so that a user can view the three-dimensional image without any special glasses or
other equipment, are known. Such imaging elements and their construction, are described
in "Three-Dimensional Imaging Techniques" by Takanori Okoshi, Academic Press, Inc.,
New York, 1976. Integral image elements having a lenticular lens sheet (that is, a
sheet with a plurality of adjacent, parallel, elongated, and partially cylindrical
lenses) are also described in the following Unites States patents: US 5,391,254; US
5,424,533; US 5,241,608; US 5,455,689; US 5,276,478; US 5,391,254; US 5,424,533 and
others; as well as allowed US patent application Serial Number 07/931,744. Integral
image elements with lenticular lens sheets use interlaced vertical image slices which,
in the case of a three-dimensional integral image, are aligned with the lenticules
so that a three-dimensional image is viewable when the lenticules are vertically oriented
with respect to a viewer's eyes. The image may be conveniently laminated (that is,
adhered) to an integral or lenticular lens sheet. Similar integral image elements,
such as described in US 3,268,238 and US 3,538,632, can be used to convey a number
of individual two-dimensional scenes (such as unrelated scenes or a sequence of scenes
depicting motion) rather than one or more three-dimensional images, the scenes being
viewable at different respective angles with respect to the element.
[0004] It has previously been appreciated, at least with respect to regular two-dimensional
images, that it is desirable to have the image, carrying transparency evenly illuminated
from behind. This is particularly true in larger displays which have several laterally
spaced elongated light sources. The regions on the transparency between the light
sources will have less illumination. Thus, the use of the diffuser sheet previously
mentioned. However, diffuser sheets are not entirely satisfactory in that the transparency
is still not evenly illuminated by such linear or other light sources. Thus, US 5,195,818
and US 5,224,770 describe reflector arrangements in which the reflectors have parallel
V-shaped grooves extending transverse to an elongated light source. However, for reasons
recognized by the present invention and discussed below, such designs inherently will
provide uneven illumination of a transparency.
[0005] It would be desirable then, to provide a light apparatus for illuminating a transparency
from behind, which apparatus can provide good uniformity of illumination to the transparency.
SUMMARY OF THE INVENTION
[0006] The present invention realizes that even with simple reflectors or diffusers, illumination
intensity at a location where the transparency is to be positioned, must necessarily
decrease at positions which are between light sources. This is so since luminance
must decrease with distance from any light source. Thus, because of this physical
law, previous attempts to design various reflectors or diffusers which try to spread
light more evenly between light sources can only have limited success. The present
invention takes a different approach in recognizing that the source of the problem
is simply the space that exists where there is no light source (such as between a
plurality of light sources). While this could be overcome by providing more light
sources, such an approach may not be practical given construction and operations costs.
However, the present invention attempts to obtain an equivalent effect.
[0007] The present invention then provides a light apparatus which in a first aspect comprises:
a) a housing having a back side and a front light opening through which light can
pass;
b) at least one light source within the housing emitting light in a forward and a
rearward direction;
c) a lenticular lens sheet positioned behind the light source in the housing, the
sheet having a plurality of parallel elongated, laterally convex, lens surfaces extending
in a path to form a pattern geometrically following the contour of the light source,
and facing the linear light source; and
d) a reflecting surface behind the lens surfaces to redirect light emitted from the
light source in the rearward direction to the forward direction.
[0008] In a second aspect of the invention, the light apparatus comprises:
a) a transparency carrying an image for display;
b) at least one light source positioned behind the transparency to illuminate the
transparency, the light source emitting light in a forward and a rearward direction;
c) a lenticular lens sheet positioned behind the light source, the sheet having a
plurality of parallel elongated, laterally convex, lens surfaces extending in a path
to form a pattern geometrically following the contour of the light source, and facing
the linear light source; and
d) a reflecting surface behind the lens surfaces to redirect light emitted in a rearward
direction from the light source, to the forward direction.
[0009] Another aspect of the present invention provides a light source, lenticular lens
sheet behind the light source with lens surfaces facing the light source, and reflector
behind the lens surfaces to redirect rearwardly emitted light, to the forward direction.
[0010] A light apparatus of the present invention can provide illumination of good uniformity
to an image bearing transparency positioned forward of the light source, even though
there may be considerable area behind the transparency at which there is no actual
light source. For a light apparatus with a fixed number of light sources, illumination
uniformity can be improved. Alternatively, the same illumination uniformity can be
retained and the number of light sources reduced.
BRIEF DESCRIPTION OF THE DRAWINGS
[0011] Embodiments of the invention will now be described with reference to the drawings,
in which:
FIG. 1 is a lateral cross-section view of a light apparatus illustrating the operation
of a conventional reflecting surface;
FIG. 2 is a perspective view of a light apparatus of the present invention;
FIG. 3 is a lateral cross-section along the line 3-3 of FIG. 2;
FIGS. 4-8 illustrate a geometrical determination of the positioning of light sources
and a lenticular lens sheet as used in the apparatus of FIG. 2;
FIG. 8A is a plot of calculated light distribution in an appratus of the present invention;
FIG. 9 is a lateral cross-section of an alternate light apparatus of the present invention;
FIG. 10 is a front view illustrating the shape of a lenticular lens sheet positioned
behind a non-linear light source, in a further alternate light apparatus of the present
invention; and
FIG. 11 is a lateral cross-section of the further alternate light source of FIG. 10
with the additional use of a collimating lens.
[0012] To facilitate understanding, identical reference numerals have been used, where possible,
to designate identical elements that are common to the figures.
EMBODIMENTS OF THE INVENTION
[0013] Referring first to FIG. 1, there is shown a lateral cross-section of a light apparatus
similar to that of FIG. 2, but not using a lenticular lens sheet as used in the present
invention. The apparatus shown comprises a plurality of linear, parallel, identical
light sources 36a, 36b, such as linear fluorescent bulbs (extending in a direction
perpendicular to the plane of the drawing). A diffuser sheet is positioned forward
of light sources 36a, 36b, and forward and adjacent diffuser sheet 18 is a transparency
carrying an image for viewing from a further forward position.
[0014] Reflector 8 is a flat specular reflector (although the same type of result is obtained
with a diffuse reflector). Note that rays 9 from a back side of light source 36a necessarily
spread outward as they travel toward reflector 8, and further spread after their reflection
from reflector 8. Thus, while these reflected rays 9 will increase the total light
received at diffuser 18 than would be received simply from rays 14, the intensity
of illumination on diffuser 18 will necessarily decrease moving in a lateral direction
away from light source 36a toward light source 36b. A similar result will be obtained
from light source 36b, the net result being that even with reflector 9 present, illumination
on diffuser 18 still necessarily decreases moving in a direction away from light sources
36a, 36b toward a mid-point 18a between those sources.
[0015] Turning now to FIG. 2 there is shown a light apparatus 10 of the present invention.
Apparatus 10 includes an opaque housing 12 except for a front light opening 16 through
which light can pass. Light opening 16 is defined by a light transmitting diffuser
18 (such as a translucent white plastic sheet) positioned to extend across the area
defined by a front periphery 14. and a transparency 20 positioned adjacent and forward
of diffuser 18. Transparency 20 is co-extensive with diffuser 18 and carries a visible
image for display. Diffuser 18 and transparency 20 are shown mostly cut away in FIG.
2 so that the inside of light apparatus 10 can be more clearly seen. Transparency
20 can carry any type of image including a typical ordinary two-dimensional image
(such as obtained from enlarging a conventional photograph) or may carry an integral
image as described further below.
[0016] A plurality of identical linear light sources 36, such as linear fluorescent lamps,
are positioned within housing 12 and emit light in a forward direction toward diffuser
18, and in a rearward direction. A lenticular lens sheet 30, of well known construction,
is positioned adjacent an opaque back wall 35 of housing 12. Lens sheet 30 has a flat
back surface 34 and a plurality of parallel, elongated and linear cylindrical lens
surfaces 32 on a front side. Back surface 34 is preferably itself reflecting. To accomplish
this it is preferably a somewhat diffuse reflecting surface which is integral with
the remainder of lens sheet 30, such as may be obtained by a finely abrasive treatment
of back surface 34 (for example, by fine sandblasting). Alternatively, back surface
34 can simply result from back surface 34 being flat and polished, and then solely
relying upon internal reflection at back surface 34 (although this is less preferred).
However, a separate reflecting layer (such as a reflecting metal or metal oxide coating)
could be provided to make back surface 34 reflecting. For example back wall 35 could
be forward reflecting. Such a separate reflecting layer is preferably positioned immediately
adjacent back surface 34. It will be appreciated that back wall 35 could be omitted,
particularly for example, if back surface 34 has an adjacent reflecting metal layer.
[0017] Note that lens surfaces 32 are in the form of a pattern which follows the contour
of the light sources 36. By "contour" of the light sources is referenced the outline
of the two-dimensional direct projection of the light sources 36 toward front light
opening 16 (by direct projection is meant that rays are traced from the back toward
the front in a direction 90 degrees to the front light opening 16). That is, the light
sources 36 have a linear contour, therefore the lens surfaces 32 follow this contour
and are therefore arranged in a linear pattern parallel to light sources 36. Thus,
transparency 20 can be viewed from a forward direction when light sources 36 are energized.
However, it will be appreciated in this application that such "following" does not
have to be precise (that is, it does not have to be parallel to the contour). Some
benefit will be obtained even as the lens surfaces deviate from the contour, although
the uniformity of the light distribution at the diffuser plane will decrease. This
feature in iteself could be used for aesthetic appeal where light uniformity is to
be varied in some desired manner.
[0018] The use of the lenticular lens sheet to effectively fill in light on diffuser 18
at positions between light sources 36 will now be described. This first requires an
understanding of lenticular geometry and optics followed by the application of such
optics to the light apparatus geometry, such as apparatus 10. These aspects are discussed
below in relation to FIGS. 4-8 in particular. Light incident on diffuser 18 arrives
by three paths. First, light emitted by source 36 in a rearward direction imaged by
the lenticules onto the back surface 34 of the lenticular sheet and re-directed in
the forward direction by the next adjacent lenticule such as lenticule 42. This can
be referenced as the first satellite image. Second, light imaged on the rear surface
of the lenticular sheet and re-directed forward by the second adjacent lenticule,
such as lenticule 43. This can be referenced as the second satellite image. Higher
order satellite images exist in theory but are of insignificant intensity. Third,
direct emission in a forward direction from the light source 36 to diffuser 18, illustrated
in FIG. 8 (which occurs without any reflecting surface in the light apparatus).
Lenticular Geometry
[0019] The applicable optical paths for the first and second satellite images for the lenticular
lens sheet 30, are shown in FIGS. 4 and 5, respectively. In Figure 4, a ray 40 enters
a lenticule 41 and strikes the planar back surface 34 causing an illumination of the
intercept point 44. Point 44 becomes an object for the next adjacent lenticule 42
and light is refracted from lenticule 42 along the refracted path 45. The initial
angle of incidence "
a" to a centerline 41c and the refractive index "
n" of the lens sheet 30 relative to the external refractive index number "
no" determines by Snell's law the angle "
b". For the sake of this discussion, the thickness "
t" of lens sheet 30 will be substantially equal to the focal length of the lens surface
32. Such thickness is measured from the top of the convex lens surface (that is, it
will be the maximum thickness). However,
t need not be equal to the focal length, and could be modified to alter the distribution
of intercept points resulting from the first and second satellite images if desired.
Ray 40 is thereby refracted to ray 40r. Point 44 is the object of lenticule 42 at
an angle "
c" from its centerline 42c.
[0020] A ray 60 is the reflected path of photons emitted from point 44 toward the lens surface
32 of lenticule 42. Again by Snell's law, ray 60 is refracted to a new angle "
d" as ray 60r. The spacing of lenticules 41 and 42 and other similar lenticules in the
lens sheet 30 is "
p". The values of
a,
b,
c and
d can then be determined to be given in equations (2), (5) and (7) below from the following
geometric relationships:

therefore:

Also:

and:

therefore:

Also:

therefore:

[0021] Figure 5 is similar to Figure 4 except that the second satellite image is analyzed.
The equations given earlier are then expanded to include by the same reasoning, this
second satellite case:
[0022] s is calculated as before.

[0023] Similar analyses can be applied to higher order satellites, although the amount of
light emitted from point 504 at increasing angles
e will lessen by the rules associated with Lambertian surface emissions.
[0024] The surface treatment of the back surface 34 of lens sheet 30 will affect the efficiency
of light transmitted along refracted ray 60r. A diffuse white surface is preferred
over a plane unfinished surface. A diffuse "sandblasted" back surface 34 may be better
than a plane surface polished surface. In any case, the addition of a metal or metal
oxide layer behind back surface 34 can be used to improve reflectivity.
Apparatus Geometry
[0025] FIG. 6 is a portion of the view shown in FIG. 3 illustrating the first satellite
image. As shown in FIG. 6, for any given photon path 40 exiting normal to the surface
of light source 36 in a direction which intercepts the lenticular lens sheet 30, the
incident angle is
a. Therefore, the intercept distance from
xO (the central axis of the center of light source 36) is:

where
g is the distance from the tube center to the lenticular plane 002.
[0026] By the mathematics discussed in preceding "Lenticular Geometry" section, the photon
refracts away from lenticular lens sheet 30 at angle
d on a new ray 60r. This photon "hits" diffuser 18 at point 70 located at a distance
"
k1" from
xo. The additional lateral translation (sometimes referenced as the x translation) of
ray 60r is represented by
xr and can be calculated as:

where
h is the distance from diffuser 18 to axis
x0 and g is the distance from axis
x0 to lenticular lens sheet 30. Note that

for any value of
a.
[0027] For the second satellite image, the same series of calculations can be made except
replacing
c with
e and
d with
f.
[0028] A computer spreadsheet is a convenient way to calculate the series of intercepts
similar to that at point 70 which result from other incident photon paths similar
to the specific path 40, as shown in FIG. 7. FIG. 7 is a view the same as in FIG.
6 but illustrating the paths of additional light rays.
[0029] In FIG. 7 a series of photon paths at incrementally increasing angles 102, 103, 104,
105 result in refracted photon paths 102r, 103r, 104r, 105r respectively, and intercept
diffuser 18 at "hit" points 112, 113, 114, 115, respectively. The distances
k1 in FIG. 6 corresponding to each of points 112, 113, 114, 115, can be calculated and
plotted for display. An arrangement of equally distant points would be seen as a uniformly
illuminated section of the diffuse plane.
[0030] It is particularly instructive from FIG. 7 to note that light from light source 36
emitted in a backward direction, is being refocussed by lenticular lens sheet 30 at
a position between adjacent light sources 36. Light directed backward is not simply
being reflected as would be the case with a simple planar reflector or reflected and
scattered as would occur with a diffuse planar reflecting surface only. Thus, illumination
at a position on diffuser 18 midway between adjacent light sources 36 can actually
be increased such that illumination on diffuser 18 does not necessarily decrease toward
a position midway between adjacent light sources 36.
[0031] Referring to FIG. 8, this is a view the same as FIG. 7 but showing the a similar
set of photon paths emitted from a front side of light source 36 and directly intercept
diffuser 18. Again, paths 201, 202, 203, 204 are normal to the surface of light source
369, but directed forward toward diffuser 18. The respective intercepts with diffuser
18 are at points 211, 212, 213, 214. These intercepts, k
0, can be calculated as follows:

[0032] For a distribution analysis, the values of
a can be the same as the earlier, analysis of refracted photon paths, but are measured
clockwise from the Y axis 291 of the coordinate system centered at
x0.
[0033] The previously mentioned spreadsheet can calculate and plot the intercepts "hit"
points 211, 212, 213, and 214 and the like by the addition of the appropriate equations.
[0034] Using the foregoing analysis a spreadsheet program by Microsoft Excel was used to
analyze light ray intercepts (referenced as "Photon Path Intercepts" in FIG. 8A) on
a diffuser 18 in a light assembly constructed according to FIG. 3 and having the parameters
of TABLE 1. Note that in Table 1 all linear dimensions, including k
0, k
1, k
2, and have been normalized to the bulb spacing S
b. This simplifies the design of light boxes which might vary greatly in dimensions,
by allowing the same set of calculations to be used for varying S
b.
[0035] The light ray intercepts between adjacent light sources 36 is plotted in FIG. 8A.
The vertical axis is the ratio of box thickness
g +
h (which passes through the center of the lamp), normalized to the lamp spacing S
b. The horizontal axis is position as a ratio of lamp spacing (thus, another lamp would
be present at position 1). Note that unlike the use of a flat reflector, such as shown
and described above in connection with Figure 1, that the density of intercepts does
not fall to a minimum at a position midway between adjacent light sources 36, but
increases because of the effect of light being redirected by the lenticular lens sheet
30. The intercept density may not have a one-to-one correspondence with light intensity
though, because of imperfections in the lenticular lens sheet 30 and efficiency of
reflectance from the back surface 34. Of course, these are characteristics that can
be controlled to some degree during production to optimize performance or cost.
[0036] It will be appreciated then that the above type of analysis can be used as a technque
to construct

a light apparatus such as apparatus 10, so as to have the most uniform illumination
on diffuser 18 given constraints such as the number of light sources 36 and size of
front opening 16. It will also be understood that in the foregoing analysis the emitted
photon paths were assumed to be normal to the light source. A more complete analysis
could be performed by including consideration for the diffuse nature of the light
source surface and the falloff of light intensity with distance. However, the analysis
presented above is a convenient practical first order approximation which is sufficient
for most purposes. Alternatively, for an apparatus having the foregoing constraints
pre-determined, a second technique is simply to determine the spacing of lenticular
lens sheet 30 and diffuser from light sources 36 experimentally. This can be done
by simply varying the foregoing spacings manually until the best or a satisfactory
uniformity of illumination on diffuser 18 is observed. Additionally, lenticular lens
sheets having varying lenticule sizes, which are available commercially from Imaging
Technology Internationl, Duluth, Georgia, USA and elsewhere, could be tried. Either
technique can, if desired, be used to minimize non-uniformity of illumination at the
area to be illuminated (for example, diffuser 18) given preselected constraints on
the number and type of light sources and the area to be illuminated by them. Such
non-uniformity can be determined by measuring light intensity across the area to be
illuminated and calculating standard deviation or variance using statistical techniques.
[0037] Referring now to FIG. 9 there is shown a lateral cross-section of another light apparatus
10a of the present invention. Apparatus 10a is similar in construction to apparatus
10 of FIGS. 2 and 3. However, apparatus 10a has a curved image carrying transparency
20a positioned in front of a curved diffuser 18a, both of which extend to a back wall
35a (note that both transparency 20a and diffuser 18a are curved concavely about the
direction of linear light sources 36). Two linear light sources 36, the same as those
of apparatus 10, are positioned behind diffuser 18a and forward of two lenticular
lens sheets 30a. Each lenticular lens sheet 30a is the same as sheet 30 in apparatus
10, but each only extends laterally outward from behind its corresponding light source
36 (that is, there is no lenticular lens sheet behind and between the two light sources
36. It will be appreciated that by proper adjustment of the curvature of diffuser
18a and transparency 20a, and the positioning of light sources 36, fairly uniform
illumination on diffuser 18 can be obtained.
[0038] FIG. 10 illustrates a different pattern of lenticular lens elements. In particular,
in FIG. 10 a light source 300 is provided which has a circular contour, such as a
spherical light source. Lenticular lens sheet 30b in this case has parallel, elongated,
convex lens surfaces 32b, which follow the circular contour of light source 300 and
thus form a pattern of concentric circles. It should be noted here that "elongated"
in the context of the lens surface shapes, does not require that they be linear, unless
the contrary is indicated. Lenticular lens sheet 30b otherwise may be constructed
in any of the manners described in connection with lens sheet 30 described above.
A diffuser and transparency carrying an image, could be placed in sequence in front
of such a light source. Alternatively, such a light source 300 and lens sheet 30b
could be used with our without a diffuser as a light source to project light forwardly.
[0039] FIG. 11 shows a lateral cross-section across an apparatus incorporating the arrangement
shown in FIG. 10. In the light apparatus 10b of FIG. 11, a housing 12b is opaque but
has a front light opening defined by a convex lens in the form of a light transmitting
Fresnel lens 302. Housing 12b includes a back wall 35b against which lens sheet 30b
is positioned. Back wall 35b may have a forwardly reflecting surface adjacent lens
sheet 30b, similar to back wall 35 described above. The light assembly 10b of FIG.
11 may have a diffuser positioned adjacent and in front of Fresnel lens 302. A transparency
carrying an image may be positioned adjacent and in front of Fresnel lens 302 if it
is desired to use light assembly 10b to display an image carried by such a transparency.
Alternatively, the transparency can be omitted and the light assembly 10b, with or
without diffuser, used as a forward projecting light source for other purposes. Note
that Fresnel lens 302 tends to collimate light passing forwardly through it.
[0040] In the present invention the lenticular lens sheets have been described as having
a "convex" lens surfaces. It will be understood that such lens surfaces may be physical
convex surfaces (which is preferred), in the sense that they have a physical convexity.
Alternatively, the convex lens surfaces can be functional ones, in the sens that the
optical effect provided is the same as that provided by physical convex lens surfaces
of leticules. In this latter regard is included lens sheets which may be physically
flat on either side but use regions of varying indices of refraction through its volume
configured in such a way as to provide (in conjunction with the surfaces of the sheet,
such as a curved external surface, flat external surface or some other shape) the
same optical deflection of light rays as would be provided by a lenticular lens sheet
with physical convex lens surfaces. It will also be appreciated in the present invention
that the back surface of the lenticular lens sheet may also be curved so as to either
strengthen the lens effect or compensate for the curved focal plain which may be inherent
in the lens construction. Consequently, the curvature on the back side may be of such
a shape as to match the curvature of the focal plain of the lens.
[0041] Additionally, for particular applications, where a different distribution of light
is desired, the entire lens sheet such as lens sheet 30, may be curved or otherwise
shaped, such as curved concavely or convexly about an axis parallel to that of a linear
light source. With reference to a "linear" light source in this application, it will
be appreciated that such a source includes a line of individual sources (such as a
line of spherical incandescent bulbs).
[0042] It will be appreciated that the light distribution to be received on the diffuser
18 could also be altered by altering the characteristics of the reflecting back surface
34. For example, bands of diffuse reflecting areas 400 could be provided, as shown
in FIGS. 12 and 13, if it was desired to provide more diffuse satellite images. FIG.
12 shows the effect on the first satellite images while FIG. 13 shows the effect on
the second satellite image. Alternatively, areas 400 could be colored if color effects
were desired, or they could be angled zones if other effects were desired.
[0043] As to the type of image carried by a transparency described above, as already mentioned
such an image can be a conventional two-dimensional image obtained from enlarging
a conventional photograph or the like. However, such an image may particularly be
an integral image for use with a lenticular lens sheet (thus, it will have interlaced
strips from multiple two-dimensional images, as described above; integral images specifically
constructed for lenticular lens sheets are sometimes referenced as "lenticular images").
The strips are to be aligned with individual lenses of an integral lens sheet so that
each of the images is viewable when a user's eyes are at the correct angle relative
to the imaging element. The integral image can be one or more three-dimensional images,
one or more two dimensional images, or any combination of the foregoing. By a "three-dimensional
image", is meant an integral image which, when viewed through the lens, has a visible
depth element. A depth element means the ability to at least partially look around
an object in the scene. This can be obtained by interlacing lines from different perspective
views of the same scene (that is, views from different angular positions with respect
to the scene). Thus, a three-dimensional image necessarily includes at least two views
of a scene. By a two-dimensional image is referenced an image which, when viewed in
the final product, does not have any viewable depth element.
[0044] The invention has been described with reference to a preferred embodiment. However,
it will be appreciated that variations and modifications can be effected by a person
of ordinary skill in the art without departing from the scope of the invention.
PARTS LIST
[0045]
- 002
- Lenticular Plane
- 8
- Reflector
- 9
- Rays
- 10, 10a
- Apparatus
- 10b
- Assembly
- 12, 12b
- Housing
- 13
- Front Periphery
- 14
- Rays
- 16
- Opening
- 18
- Diffuser
- 18a
- Mid-Point
- 20, 20a
- Transparency
- 30, 30a, 30b,
- Lens Sheets
- 32, 32b
- Lens Surfaces
- 34
- Back Surface
- 35, 35a, 35b
- Back Wall
- 36, 36a, 36b
- Light Sources
- 40, 40r
- Ray
- 40
- Path
- 41
- Lenticules
- 41c, 42c
- Centerline
- 43
- Lenticule
- 44
- Point
- 45
- Refracted Path
- 60, 60r
- Rays
- 70
- Point
- 102, 103, 104, 105
- Angles
- 102r, 103r, 104r, 105r
- Paths
- 112, 113, 114, 115
- "Hit" Points
- 201, 202, 203, 204
- Paths
- 211, 212, 213, and 214
- "Hit" Points
- 291
- Y Axis
- 300
- Light Source
- 302
- Fresnel Lens
- 400
- Areas
- 504
- Point
1. A light apparatus comprising:
a) a housing having a back side and a front light opening through which light can
pass;
b) at least one light source within the housing emitting light in a forward and a
rearward direction;
c) a lenticular lens sheet positioned behind the light source in the housing, the
sheet having a plurality of parallel elongated, laterally convex, lens surfaces extending
in a path to form a pattern geometrically following the contour of the light source,
and facing the linear light source; and
d) a reflecting surface behind the lens surfaces to redirect light emitted from the
light source in the rearward direction to the forward direction.
2. A light apparatus according to claim 1 wherein the light source contour and lens pattern
are circular.
3. A light apparatus according to claim 1 wherein the light source is linear and the
lens pattern is linear.
4. An apparatus according to claim 1 wherein the reflecting back surface comprises a
diffuse reflecting surface.
5. An apparatus according to claim 1 wherein the lenticular lens sheet is positioned
behind the light source at a distance which minimizes non-uniformity of illumination
within the extent of the front light opening.
6. A light apparatus comprising:
a) a transparency carrying an image for display;
b) at least one light source positioned behind the transparency to illuminate the
transparency, the light source emitting light in a forward and a rearward direction;
c) a lenticular lens sheet positioned behind the light source, the sheet having a
plurality of parallel elongated, laterally convex, lens surfaces extending in a path
to form a pattern geometrically following the contour of the light source, and facing
the linear light source; and
d) a reflecting surface behind the lens surfaces to redirect light emitted in a rearward
direction from the light source, to the forward direction.
7. A light apparatus according to claim 6 wherein the light source is linear and the
lens pattern is linear.
8. A light apparatus comprising:
a) at least one linear light source emitting light in a forward and rearward direction;
b) a lenticular lens sheet positioned behind the light source, the sheet having a
plurality of elongated, parallel cylindrical lens surfaces oriented in the same direction
as, and facing, the linear light source; and
c) a reflecting surface behind the lens surfaces to redirect light emitted from the
light source in the rearward direction to the forward direction.
9. A light apparatus comprising:
a) a housing having a back side and a front light opening through which light can
pass;
b) at least one linear light source within the housing emitting light in a forward
and a rearward direction;
c) a lenticular lens sheet positioned behind the light source in the housing, the
sheet having a plurality of elongated, parallel cylindrical lens surfaces oriented
in the same direction as, and facing, the linear light source; and
d) a reflecting surface behind the lens surfaces to redirect light emitted from the
light source in the rearward direction to the forward direction.
10. An apparatus according to claim 9 additionally comprising an image carrying transparency
positioned forward of the light source.
11. An apparatus according to claim 10 wherein the transparency comprises a lenticular
element having a lenticular image and a lenticular lens sheet positioned forward of
the image.