U.S. patent number 3,735,124 [Application Number 05/169,303] was granted by the patent office on 1973-05-22 for prismatic lenses for lighting fixtures.
This patent grant is currently assigned to Emerson Electric Co.. Invention is credited to Leo G. Stahlhut.
United States Patent |
3,735,124 |
Stahlhut |
May 22, 1973 |
PRISMATIC LENSES FOR LIGHTING FIXTURES
Abstract
A prismatic lens for an overhead lighting fixture is formed from
a transparent material and has a lower face composed of a plurality
of arcuate surfaces arranged side-by-side. These surfaces form
convex magnifying segments or lenticules in the lens. The opposite
or upper face is composed of a plurality of V-shaped depressions
extending downwardly from a generally flat intervening surface. The
depressions are located behind and centered relative to the arcuate
surfaces, whereas the intervening surfaces are positioned directly
behind the junctures of adjacent arcuate surfaces. The prismatic
lens diverts light rays emanating from a light source behind it
primarily into zones disposed oblique to the lens so that the
intensity of illumination is minimal in the reflected glare zone
located directly beneath the lens and in the direct glare zone
located generally to the side of the lens, but is maximum in the
oblique zones located between the reflected and direct glare zones.
This distribution provides the most pleasant and comfortable
illumination for most visual observations performed beneath the
fixture.
Inventors: |
Stahlhut; Leo G. (Kirkwood,
MO) |
Assignee: |
Emerson Electric Co. (St.
Louis, MO)
|
Family
ID: |
22615098 |
Appl.
No.: |
05/169,303 |
Filed: |
August 5, 1971 |
Current U.S.
Class: |
362/333;
362/330 |
Current CPC
Class: |
F21V
5/00 (20130101); F21Y 2113/00 (20130101); F21Y
2103/00 (20130101) |
Current International
Class: |
F21V
5/00 (20060101); F21v 005/04 () |
Field of
Search: |
;240/93,78LD,16R,106.1,146,147 ;350/168,188 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
|
|
|
|
|
|
|
8,324 |
|
Sep 1909 |
|
GB |
|
620,639 |
|
Mar 1949 |
|
GB |
|
Primary Examiner: Matthews; Samuel S.
Assistant Examiner: Adams, Jr.; Russell E.
Claims
What is claimed is:
1. A lens for distributing light emitted by a light source to
better illuminate an area in front of the light source, said lens
comprising: a relatively thin light-transmitting material
positioned between the light source and the area to be illuminated
and having a front face presented toward the area to be illuminated
and a rear face presented toward the light source, one of said
faces being comprised of a plurality of adjacent convex surfaces,
the other of said faces being comprised of a plurality of surfaces
inclined with respect to the general direction assumed by the thin
light transmitting material and arranged to form depressions in the
material, each depression being located directly behind a convex
surface on said one face, the other of said faces being further
comprised of an intervening surface area located between the
depressions and oriented generally in the direction assumed by the
relatively thin light-transmitting material, the convex surfaces,
the inclined surfaces, and the intervening surface area being
positioned relative to one another such that light from the light
source, after passing through the lens, is concentrated in zones
oblique to the general direction assumed by the light-transmitting
material.
2. A lens according to claim 1 wherein the adjacent convex surfaces
intersect, and the intervening surface area intersects the inclined
surfaces.
3. A lens according to claim 2 wherein each depression is centered
relative to a convex surface and the intervening surfaces are
located directly opposite the junctures of adjacent convex
surfaces.
4. A lens according to claim 3 wherein the depressions are V-shaped
in cross-section with the apex of each V-shaped configuration being
located directly opposite and centered relative to a convex
surface.
5. A lens according to claim 4 wherein the spacing between the
centers of adjacent depressions equals the width of the arcuate
surfaces.
6. A lens according to claim 1 wherein each convex surface is
formed about a center whereby it forms the segment of a circle.
7. A lens according to claim 6 wherein the width of each convex
surface is between 1.00 and 1.87 times the radius of the convex
surface.
8. A lens according to claim 6 wherein the thickness of the lens
measured between the intervening surface area and the outermost
portion of the convex surface is between 0.75 and 1.5 times the
radius of the convex surface.
9. A lens according to claim 4 wherein the greatest angle between
the opposed inclined surfaces which form the depression is between
40.degree. and 78.degree..
10. A lens according to claim 4 wherein each depression is a groove
and each convex surface forms a segment of a cylinder.
11. A lens according to claim 4 wherein each convex surface forms a
segment of a sphere.
12. A lens according to claim 11 wherein each depression possesses
the shape of a four-sided pyramid.
13. A lens according to claim 1 wherein the light-transmitting
material is nonlaminate, and the front and rear surfaces thereof
are completely exposed.
14. A lens according to claim 1 wherein the face comprised of the
inclined surfaces and intervening surface area is presented toward
the light source and the face comprised of the convex surfaces is
presented toward the area to be illuminated.
15. A lens according to claim 1 wherein the intervening surface
area is disposed at no more than 15.degree. with respect to the
general direction assumed by the light transmitting material.
16. A lens according to claim 1 wherein the intervening surface
area is planar.
17. A light fixture lens having the capability of concentrating
light emitted from a light source in a light fixture in zones
generaly oblique to the nadir of the lens to provide more pleasant
illumination of the area beyond the lens and fixture, said lens
comprising a nonlaminate light transmitting material which is
relatively thin and has a rear face presented toward the light
source and a front face presented toward the area to be
illuminated, the rear face being comprised of a generally flat
surface area presented substantially perpendicular to the nadir of
the lens and a plurality of intersecting inclined surfaces
presented at oblique angles with respect to the generally flat
surface area to form generally V-shaped depressions in the light
transmitting material, the front face being comprised of adjacent
convex surfaces with each convex surface being presented in front
of a different V-shaped depression and being centered with respect
to that depression so that the junctures of adjacent convex
surfaces will be in front of the generally flat surface area, the
relative positioning of the convex surfaces, the inclined surfaces,
and the generally flat surface area being such that the light from
the light source, after passing through the lens, is concentrated
in zones oblique to the nadir for the lens.
18. A lens for distributing light emitted by a light source to
better illuminate an area in front of the light source; said lens
comprising: a relatively thin one-piece light-transmitting material
positioned between the light source and the lens and having a rear
face presented toward the light source and a front face presented
toward the area to be illuminated, the front face being comprised
of a plurality of adjacent convex surfaces, the back face being
comprised of a surface area extended generally in the direction
assumed by the thin light-transmitting material and surfaces
inclined with respect to that surface area to form depressions
which open toward the light source and interrupt the surface area,
the relative positioning of the depressions, the surface area and
the convex surfaces, and the configuration of the depressions all
being such that light from the light source, after passing through
the lens, is concentrated in zones oblique to the general direction
in which the light-transmitting material extends so that the
concentration of light is minimized along the nadir to the
lens.
19. A lens according to claim 18 wherein the front and rear faces
of the light-transmitting material are completely exposed.
Description
BACKGROUND OF THE INVENTION
This invention relates to lighting devices and more particularly to
lenses for lighting fixtures.
Extensive research in the field of overhead lighting has developed
that light rays emitted obliquely with respect to the horizontal or
vertical produce the most pleasant and comfortable lighting
conditions for offices and most other applications where overhead
lighting is employed. Indeed, lighting engineers consider it
desirable to concentrate most, if not practically all, of the liqht
emitted from overhead fixtures in oblique zones extending between
about 25.degree. to 60.degree. with respect to the nadir, that is
with respect to a line extending vertically from the fixture. Light
which leaves the fixture at greater angles, that is at angles
approaching the horizontal, produces a condition known as direct
glare. This simply means that one looking across the room observes
glare from the overhead light fixtures, and when the intensity of
illumination in this zone is high, the direct glare becomes
annoying and extremely uncomfortable. On the other hand, light rays
which leave the fixture at lesser angles, that is at angles
approaching the vertical or nadir, produce a condition known as
reflected glare. This condition results in a large amount of
reflection from horizontal working surfaces such as desk tops and
any printed matter on those surfaces, and when that reflection is
of a high intensity visual work performed at such surfaces becomes
uncomfortable, although the source of the discomfort may not be
readily apparent to the worker. For purposes of comparison
reflected glare may be equated to the glare observed when reading a
newspaper in direct sunlight, whereas the more comfortable lighting
effect derived from oblique light rays in the oblique zone may be
equated to reading the same newspaper in the shade. Lighting
engineers describe the desired oblique concentration of
illumination as a "batwing" pattern or distribution.
Heretofore, lighting engineers have eliminated direct glare to a
large measure by installing baffles on lighting fixtures. These
baffles, however, are large and unsightly and not compatible with
present architectural practices. Moreover, they make lighting
fixtures unnecessarily complicated. Aside from baffling, so-called
prismatic lenses have been developed for lighting fixtures and
these lenses substantially reduce the intensity of direct glare
from overhead lighting fixtures.
Insofar as the reflected glare is concerned, diffusing panels have
been developed which reduce such glare considerably, but not enough
to eliminate all discomfort from high intensity fixtures.
Furthermore, diffusing panels do not eliminate or for that matter
even significantly reduce direct glare.
Currently, prismatic lenses are being produced which significantly
reduced both direct and reflected glare. These lenses, however,
require opaque coatings at critical areas on their surfaces and as
a result they block some of the light which might otherwise be
emitted from the light fixtures. In other words, they reduce the
efficiency of the lighting fixture. Furthermore, the opaque
coatings necessitate an additional production step, adding
appreciably to the cost of the lenses.
SUMMARY OF THE INVENTION
One of the principal object of the present invention is to produce
a prismatic lens which concentrates the light emitted from overhead
lighting fixtures in oblique zones. Another object is to produce a
lens of the type stated which substantially eliminates both direct
glare and reflected glare, and accordingly distributes light from
an overhead fixture in a manner which is comfortable and pleasant
to one working beneath it. A further object is to produce a fixture
lens of the type stated which is highly efficient. An additional
object is to produce a lens of the type stated which is easy and
economical to manufacture. Still another object is to produce a
lens of the type stated which is attractive in appearance and does
not conflict with contemporary architecture. Yet another object is
to provide a lenticule for providing a fixture lens with the
foregoing advantages. These and other objects and advantages will
become apparent hereinafter.
The present invention is embodied in a transparent lens having a
plurality of arcuate surfaces arranged side-by-side on one face and
inclined surfaces forming depressions in the opposite face. An
intervening surface extends between each depression. Each arcuate
surface forms a separate lenticule and the invention further
resides in the individual lenticules. The lens concentrates rays in
zones oblique to it. The invention also consists in the parts and
in the arrangements and combinations of parts hereinafter described
and claimed.
DESCRIPTION OF THE DRAWINGS
In the accompanying drawings which form part of the specification
and wherein like numerals and letters refer to like parts wherever
they occur:
FIG. 1 is a sectional view in elevation showing a ceiling
containing a light fixture provided with a lens constructed in
accordance with and embodying the present invention, details of
contour being omitted from the lens inasmuch as they are
illustrated in enlarged form in FIG. 2;
FIG. 2 is a transverse sectional view of the lens;
FIG. 3 is a plan view taken along line 3--3 of FIG. 2 and showing
the underside of the lens;
FIG. 4 is a plan view taken along line 4--4 of FIG. 2 and showing
the top surface of the lens;
FIG. 5 is a sectional view of the lighting fixture showing its
light distribution with and without the lens, the light
distribution being graphed in polar coordinates;
FIG. 6 is a sectional view of the lens showing various light rays
in the lens;
FIG. 7 is a plan view showing the underside of a modified lens;
FIGS. 8 and 9 are sectional views taken along lines 8--8 and 9--9,
respectively, of FIG. 7;
FIG. 10 is a plan view showing the top surface of the modified lens
illustrated in FIG. 7;
FIG. 11 is a plan view showing the underside of another modified
lens;
FIG. 12 is a fragmentary plan view showing the underside of still
another modified lens; and
FIG. 13 is a sectional view taken along line 13--13 of FIG. 12.
DETAILED DESCRIPTION
Referring now to the drawings (FIG. 1) 2 designates a room having a
ceiling 4 from which a false ceiling 6 is suspended by means of
wires 8 and a grid formed by crossed T-bars 10. Aside from the
T-bars 10, the false ceiling 6 includes ceiling panels 12 which
occupy some of the grid spaces and lighting fixtures 20 which
occupy the remaining grid spaces. Actually, the sides and ends of
the panels 12 and fixtures 20 rest upon the horizontal flanges of
the T-bars 10 and are easily removed for access to the true ceiling
4 or pipes and other conduits extending between the true ceiling 4
and the false ceiling 6.
Each lighting fixture 14 includes (FIG. 1) a reflector 22 which is
configured to reflect light downwardly into the room 2, a plurality
of sockets 24 positioned in front of the reflector 16, and a series
of fluorescent lamps 26, the ends of which fit into and are engaged
with the sockets 24. In addition, each lighting fixture 20 is
provided with a prismatic lens 30 which extends completely across
the reflector 22 in front of the fluorescent lamps 26 and lies
generally flush with the ceiling panels 12. The prismatic lens 30
completely masks the lamps 26 and reflector 22 and concentrates the
light emitted from the lamps 26 in oblique zones extending on each
side of the nadir.
The prismatic lens 30 is formed as an integral unit from any
suitable transparent material such as clear acrylic or
polycarbonate plastic or glass. The lens 30 possesses a lenticular
pattern, meaning that its light refracting and light reflecting
surfaces are substantially greater in length than breadth and
normally extend longitudinally of the lens 30 and fixture 20.
Consequently, the prismatic lens 30 may be formed in an extruding
operation, provided, of course, that the transparent material of
the lens 30 is capable of being extruded.
The downwardly presented face of the lens 30, that is the face
presented away from the lamps 26 and toward the interior of the
room 2, is composed of (FIGS. 2 and 3) a plurality of
longitudinally extending arcuate surfaces 32 which are positioned
side-by-side and intersect at lines x. Each surface 32 forms a
segment of an arc having a radius R which emanates from a center p
located to the rear of the surface 32. In effect, the surfaces 32
form convex lenticules or lens segments 34, which are cylindrical
magnifiers in the lens 30. The focal point of each lens segment 34
is located at a point f, or more accurately at a line f, which is
disposed behind the lens 30 and is centered relative to the arcuate
surface 32 forming the lens segment 34. The distance from the
center of the arcuate surface 32 to the focal point f represents
the focal length F of the lens segment 34, and as is the case with
cylindrical lenses in general, this distance F is approximately
21/2 to 23/4 times greater than the radius R of the arcuate surface
32. The distance between the lines x--x at each side of every lens
segment 34 is termed the width A of the lens segment 34.
The opposite or rear face of the lens 30, that is the face
presented toward the lamps 26, is composed of (FIGS. 2 and 4) a
plurality of V-shaped grooves 36 which are disposed directly behind
the arcuate surfaces 32 and are separated by intervening surfaces
38 which are located directly behind the lines x forming the
intersections of the arcuate surfaces 32. The intervening surfaces
38 are normally planar and coplanar with respect to each other, and
they lie in a plane which is parallel to and located above the
horizontal center plane of the lens 30. Each surface 38, however,
may be curved slightly or composed of a pair of intersecting flat
surfaces disposed at an angle no greater than 15.degree. with
respect to the horizontal center plane of the lens 30. The greatest
vertical distance between the intervening surface 38 and the lowest
point along the arcuate surfaces 32 is called the thickness B of
the lens 30. Lines interconnecting the focal point f and the lines
x--x at the sides of the lens segment 34 intersect the plane
defined by the intervening surfaces 38 at points, or more
accurately lines, w--w which are spaced a distance W apart.
Each groove 36 (FIGS. 2 and 4) is defined by a pair of planar side
surfaces 40 and 42 which are disposed at an angle K with respect to
each other and intersect each other at a line t which is centered
relative to the corresponding arcuate surface 32. The distance
between the lines t of adjacent grooves 36 represents the spacing C
between adjacent grooves 36. The side surfaces 40 and 42 also
intersect the intervening surfaces 38 and the spacing between the
lines of intersection so formed is termed the width D of the groove
36.
Since the convex lens segments 34, the grooves 36, and the
intervening surfaces 38 are substantially greater in length than in
width and furthermore possess the same transverse cross-sectional
shape anywhere along the lens 30, the lens 30 is classified as a
lenticular lens arrangement as opposied to a spherical lens
arrangement.
In the prismatic lens 30 the following relationships between the
foregoing dimensions should exist:
A. The width A of the lens segment 34 should equal the spacing C
between the grooves 36.
B. The thickness B of the lens 30 should be between approximately
0.75 and 1.50 the radius R of the arcuate surfaces 32.
C. The width D of the groove 36 should be between 0.50 and 1.25 the
distance W between the lines w--w.
D. The groove angle K should be between 40.degree. and 78.degree.
and preferably 60.degree..
In operation, the fluorescent lamps 26 emit light rays which pass
outwardly through the prismatic lens 30 and illuminate the room 2.
Behind the lens 30 the combined effect of the rays emitted directly
from the lamps 26 as well as the rays reflected from the reflector
22 results in a large concentration of rays directly below the
lamps and this concentration diminishes as the angle from the
normal or nadir increases (see FIG. 5, left side). In other words,
the illumination provided by the fixture 20 alone has its greatest
intensity directly below the fixture 20, that is along the nadir,
and the intensity becomes progressively less as the angle from the
vertical increases. Thus, without the lens 30 the fixture 20 would
produce high intensity illumination in the reflected zone directly
beneath it, and this in turn would produce uncomfortable and
annoying reflection from horizontal working surfaces in the room 2
as well as from objects on those surfaces. The fixture 2 absent its
lens 30 would also furnish a substantial illumination in the
oblique zones on each side of the reflected zone, and would further
cause significant illumination in the direct glare zone. The
latter, of course, would be annoying to one looking directly across
the room 2. The prismatic lens 30 through refraction of the light
rays redistributes the rays in a more pleasing pattern and in
particular distributes the rays such that the intensity of
illumination is greatest in the oblique zones (see FIG. 5, right
side). The light rays emitted into the reflected glare and direct
glare zones are indeed minimal and are clearly not offensive.
The light distribution produced by the fixture 20 both with and
without its lens is best illustrated in the polar graph of FIG. 5.
Note that without the lens (left side of graph) the intensity of
the illumination is greatest directly beneath the fixture in the
reflected glare zone and as the angle from the nadir increases the
intensity of the illumination progressively diminishes. The left
side of the graph represents the lighting distribution behind the
lens 30 or in other words, the orientation and relative
concentration of rays entering the lens 30. Note further that with
the lens 30 the illumination has its greatest intensity in the
oblique zones and in the reflected glare and direct glare zones the
intensity is diminished considerably.
While the light rays emanating from the lamps 26 pass downwardly
through the prismatic lens 30 and enter the room 2, for purposes of
analysis it is more desirable to consider the rays as emanating
from the room, or more particularly from the eye of an individual
working within the room, and then tracing them backwardly into the
lighting fixture 20, if in fact they do enter the interior of the
fixture 20. This is a standard and accepted practice in the field
of optics and derives from the fact that light rays are perfectly
reversible. By tracing the rays backwardly one can determine with a
fair degree of accuracy the relative intensity of illumination at
various angles below the lens 30.
Referring now to FIG. 6 and still tracing rays backwardly,
practically all of the normal or 0.degree. rays which can be traced
into the lens 30 through one of the arcuate surfaces 32 thereof are
reflected outwardly through adjacent arcuate surfaces 32. For
example, any ray G enters the lens 30 through the arcuate surface
32 in offset relation to the line t which represents the center of
the corresponding groove 36. Upon entering the lens 30 the ray G is
refracted slightly toward the overlying groove 36 and approaches
side surface 42 of that groove 36 at an angle greater than the
critical angle for the transparent material, which in this
graphical analysis is acrylic plastic marketed by Rohm and Haas
under the trademark PLEXIGLASS. In this connection, it should be
noted that the critical angles as well as other angles of
refraction are measured from the normal to the air-acrylic
interface at the point where the rays meet that interface. Inasmuch
as the ray G approaches the surface 42 at an angle greater than the
critical angle, the surface 42 reflects the ray G toward the
intervening surface 38, and the ray G approaches that surface also
an angle greater than the critical angle. The intervening surface
38 therefore reflects the ray G toward the side surface 40 of the
adjacent groove 36 and since the ray G also approaches that surface
at an angle greater than the critical angle it is again reflected.
The final reflection directs the ray G toward arcuate surface 32 of
the adjacent convex lens segment 34, and the ray G leaves the lens
30 through that surface, being refracted as it does. Consequently,
one who sights along the foregoing path, which is the nadir to the
lens, would not observe the lamps 26 or any light derived from the
lamp 26, but instead would merely observe a reflection of some
object located in the room 2 below the false ceiling 6.
However, a ray H which can be traced into the lens 30 close to the
center of one arcuate surface 32, will pass with little refraction
toward the portion of its side surface 40 located near the line t
of the overlying groove 36. The ray H will furthermore approach the
side surface 40 at an angle greater than the critical angle, and as
a result that ray will be reflected toward the side surface 42 of
the adjacent groove 36. The ray H is presented almost perpendicular
to the surfaces 42 of the adjacent groove 36 and clearly at an
angle less than the critical angel. As a result it leaves the lens
30 through that side surface 42, and when again in air it is
disposed at a relatively large angle with respect to the vertical
or nadir. The ray H demonstrates that light rays emanating from the
lamps 26 and oriented at a steep angle behind the lens 30 will
enter the lens 30 through the surfaces 40 and 42 near the juncture
of those surfaces and the intervening surfaces 38 and will further
pass through the lens 30, leaving it in a downwardly or vertical
path which lies within the reflected glare zone. From the foregoing
analysis it is quite apparent that relatively few rays will, after
passing through the lens 30, be directed vertically, and those rays
which do come through are oriented at a steep angle behind the lens
30. Bearing in mind that the fixture 2 absent the lens 30 produces
its highest concentration of illumination directly downwardly and
that at steep angles the illumination is extremely low in
intensity, the illumination which does leave the lens 30 along the
vertical is also low in intensity. Clearly, the intensity is not
enough to produce an offensive glare in the reflected glare
zone.
Still continuing to trace rays backwardly (FIG. 6), at 15.degree.
most of the rays which can be traced into the lens 30 from below
are reflected back into the room 2, although some do pass through.
Those rays which do pass through are furthermore oriented at very
small angles with respect to the vertical, and when actual
situation is considered, these represent paths along which light
passes through the lens 30 and leaves it at 15.degree.. Since the
unreflected rays are disposed at relatively small angles behind the
lens 30 they are in effect high intensity rays emitted by the lamps
26. Accordingly, at 15.degree. more illumination exists on the
underside of the fixture than at 0.degree., but the concentration
is not great enough to cause annoyance or discomfort,
notwithstanding the fact the 15.degree. rays are also within the
reflected glare zone.
At 25.degree., 35.degree. and 45.degree. (FIG. 6) all of which are
within the oblique zone, it is apparent that for all intents and
purposes the lens 30 is fully transparent since all of the rays
pass completely through the lens 30. Moreover, on the back side of
the lens 30 the rays so traced are presented at relatively small
angles with respect to the vertical or nadir and consequently
correspond with high intensity rays emitted directly from the lamps
26 or reflected by the reflector 22.
At 60.degree. (FIG. 6) few rays can be traced thorough the lens 30,
indicating that little light is emitted at that angle.
At 70.degree. and 80.degree. (FIG. 6) rays can be traced backwardly
only into one-half of each arcuate surface 32, whereas at lesser
angles the rays can be traced into more than one-half and in most
instances into the entire surface 32. By reason of this fact, the
light passing through the lens 30 at 70.degree. and 80.degree. is
greatly diminished. Nevertheless, the 70.degree. and 80.degree.
rays do pass through the lens 30 and are disposed at moderate
angles behind it. Thus, they correspond to rays of moderate
intensity emitted by the lamps 26, but by reason of the limited
area of emergence at the arcuate surface 32 they are not
concentrated significantly to produce significant glare in the
direct glare zone.
The direct glare produced by the 70.degree. and 80.degree. rays may
be reduced still further, however, by positioning an overlay sheet
similar to the one described in U.S. Pat. No. 3,288,990 over the
upwardly presented face of the lens 30.
From the foregoing analysis it is apparent that the prismatic lens
30 distributes the light from the lamps 26 and reflector 22 with
greatest intensity is in the oblique zones and with considerably
reduced intensity in the reflected glare and direct glare zones.
Since the light from the lamps 26 is for the most part distributed
obliquely into the oblique zones, it provides maximum comfort to
those making visual observations in the room 2. The lens 30
contains no opaque surfaces and by reason of this fact absorbs only
a minimal amount of the light emanating from the lamp 26.
Accordingly, the lens 30 is highly efficient.
It is also possible to incorporate the foregoing principles into a
prismatic lens 50 (FIGS. 7-10) which is similar to the lens 30, but
has its reflecting and refracting surfaces arranged in a spherical
pattern instead of a lenticular pattern. Thus, in lieu of
longitudinally extending arcuate surfaces 32 which create the
cylindrical lens segments 34, the lens 50 on its bottom face is
provided with adjoining surfaces 52, each of which forms a segment
of a sphere. The surfaces 52 create button-like protrusions or more
accurately spherical lenticules or convex lens segments 54 (FIGS.
8-9) on the lens 50, and these segments correspond to the
cylindrical lens segments 34 of the lens 30. Instead of grooves 36,
the lens 50 behind each spherical lens segment 54 has a pocket 56
(FIGS. 8-10) which possesses the shape of an inverted four-sided
pyramid. The pocket 56 may also be in the shape of an inverted
cone, but the pyramidal configuration is preferred. The pockets 56
are separated by a planar intervening surface 58 which is parallel
to and disposed beneath the horizontal center plane of the lens
50.
The lens 50 functions similar to the lens 30, only the oblique zone
of high intensity illumination created beneath each spherical lens
segment 54 is generally conical instead of wing-shaped as is true
of the oblique zone located beneath each cylindrical lens segment
34 in the lens 30. By reason of this fact, the lens 50 is more
desirable where the positioning and orientation of work surfaces
and stations in the room 2 is not known in advance or is likely to
change. In other words, the lens 50 is suitable for universal
arrangement of work surfaces or stations, whereas more care must be
exercised in arranging work surfaces or stations beneath the lens
30.
With one exception the dimensions previously prescribed for the
lens 30 also apply to the lens 50, only their pertinence is three
dimensional instead of two dimensional as is true of the lens 30.
The single exception applies only to the pyramidal pockets 56, and
particularly to the included angle K between the opposing side
surface thereof. The maximum value of that angle should not exceed
66.degree. instead of 78.degree.. This resides in the fact that the
angle between the opposing surfaces at a cross-section taken
diagonally through the pyramidal pocket 56 (FIG. 9) will measure
78.degree. when the angle in a cross-section taken normal to the
surfaces (FIG. 8) measures 66.degree.. This also illustrates why
pockets 56 having a pyramidal shape are preferred to those of
conical shape. Indeed, if conically shaped pockets are employed,
the direct glare would increase along lines of sight extending
diagonally with respect to the grid created by the arrangement of
convex lens segments 54 and the pockets 56 and lamp images would
appear.
For point or concentrated sources of light such as incandescent
lamps, another modified lens 70 (FIG. 11) may be provided, and that
lens possesses the same cross-sectional shape as the lens 30, but
the lenticules close upon themselves. More particularly, the lens
70 possesses a series of circular lenticules 72 which are
concentric about a center spherical lenticule 74. Each lenticule 72
has a downwardly presented arcuate surface which is disposed in
front of a circular groove (not shown) of a V-shaped cross-section
located at the back surface of the lens 70. The center lenticule 72
is disposed in front of a conical pocket. Instead of being
circular, the lenticules 72 may also take the form of squares or
rectangles of increasing size.
It is possible to provide still another modified prismatic lens 80
which is similar to the lens 50, but possesses spherical lenticules
of two different sizes. In particular, the lens 80 on its
downwardly presented surface (FIG. 12) has a series of spaced minor
lenticules 82 which are separated by adjoining major lenticules 84.
Both the lenticules 82 and 84 are of the spherical variety, that is
their downwardly presented surfaces constitute segments of spheres.
However, in plan the minor lenticules 82 are square, while the
major lenticules 84 are octagonal. On its opposite side (FIG. 13),
the lens 80 has a planar intervening surface 86 which surrounds a
series of conical pockets 88 and 90. The pockets 88 are disposed
behind and centered on the minor lenticules 82, whereas the pockets
90 are disposed behind and centered on the major lenticules 84.
This invention is intended to cover all changes and modifications
of the example of the invention herein chosen for purposes of the
disclosure which do not constitute departures from the spirit and
scope of the invention.
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