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Description  |
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FIELD OF THE INVENTION
The present invention relates to projection systems or projectors,
particularly transmissive overhead projectors.
BACKGROUND OF THE INVENTION
With the increasing use of full-color, computer-generated and photographic
transparencies, and liquid crystal display (LCD) projection panels, there
is a need for projection systems of increased brightness. This has been
recently addressed by the use of higher wattage tungsten-halogen lamps,
metal-halide lamp technology, and high-efficiency anti-reflection coatings
on the optical components. The use of higher wattage tungsten filament
lamps increases the difficulty of cooling, and arc discharge lamps, such
as metal halide, are relatively expensive.
In the past, several attempts to increase the illumination level of
projection systems were characterized by the use of multiple lower wattage
lamps. In the case of episcopic projection, commonly practiced in opaque
projectors, it is simply necessary to illuminate the opaque copy with
light from several sources. The scattered light from the copy which enters
a projection lens is then directed to the screen. This type of projection
system is described, for example, in U.S. Pat. No. 4,979,813.
In diascopic projection, light from a lamp is collected by single or
multiple condensing lenses, passes through a projection transparency, and
is focused to the projection lens. This mode of projection is commonly
used in 35 millimeter and overhead projectors, and gives a brighter
projected image than episcopic projection. See, for example, U.S. Pat.
Nos. 3,547,530 and 3,979,160. However, since the condensing lens system
can only efficiently focus light from one single point (lamp position) to
another single point (projection lens position), diascopic projection is
usually limited to the use of a single lamp. This inherently limits the
brightness which may be achieved on the screen.
Several attempts have been made to efficiently combine the output of
multiple lamps and bring them to a common focus. U.S. Pat. No. 1,887,650
describes a system combining eight lamps, U.S. Pat. No. 3,770,344
describes an overhead projector combining four lamps, and Japanese patent
nos. 4-179046 and 5-199485 describe projectors combining two lamps. All of
these devices suffer from a common deficiency in that the combined output
from the lamps is not truly integrated. The combined lamp output beams are
contiguous, yet spatially separated. The result is that should one lamp
fail, the screen image brightness does not diminish uniformly, but rather
individual sections of the screen image become completely dark, making
part of the screen image unreadable.
True integration of the light from multiple sources, allowing them to be
focused to a common point, is a more demanding task. U.S. Pat. No.
4,952,053 describes an overhead projector combining two lamps, U.S. Pat.
No. 5,231,433 describes a method for integrating two collimated light
beams by means of a linear grooved reflector or a linear grooved
refracting element. Japanese patent no. 5-232399 describes a method for
combining and integrating the output of two lamps by means of a beam
splitter and multiple-pass reflections. The efficiency of these systems is
limited by the achievable reflectance of the reflector coatings, geometric
shading losses, and by the high chromatic dispersion of the refracting
elements.
SUMMARY OF THE INVENTION
The current invention avoids the deficiencies of the prior art, providing a
projection system with complete and efficient integration of the output of
multiple light sources, to increase screen brightness. This is
accomplished by a series of Fresnel collecting and focusing lenses, and a
linear beam combining prismatic film that utilizes total internal
reflection (TIR). The projection System can be in the form of an
integrated projector designed to project electronically generated or
stored information or in the form of an overhead projector adapted for
full-size overhead transparencies, or the reduced format of LCD projection
panels. The present invention further relates to a low profile overhead
projector.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a cross-sectional view of a linear prismatic film of the prior
art that deviates a beam of light by refraction and total internal
reflection.
FIG. 2 is a cross-sectional view of a 60.degree. apex angle linear
prismatic film of the current invention.
FIG. 3 is a cross-sectional view of the prismatic film of the present
invention and illustrates schematically the integration of two collimated
light beams.
FIG. 4 is a schematic illustration of a transmissive overhead projector
system that combines and integrates the output of two lamps.
FIG. 5 is a schematic illustration of an alternate arrangement of a
projection system that combines and integrates the output of two lamps.
FIG. 6 is a schematic illustration of a projection system that combines and
integrates the output of four lamps.
FIG. 7 is a perspective view showing desirable shapes of lenses for use in
the present invention.
FIG. 8 is a perspective schematic illustration showing condensing optics
used with the present invention to form an elliptical shaped beam at the
rectangular Fresnel lens collimator.
FIG. 9 is a schematic illustration of an integrated liquid crystal
projection system that combines and integrates the output of two lamps.
DETAILED DESCRIPTION OF THE INVENTION
U.S. Pat. No. 4,984,144 describes a dispersive linear prismatic film 1 that
deviates a beam of light by refraction and total internal reflection, as
shown in FIG. 1. The isosceles triangle micro prisms 2 have an apex angle
.alpha. of 69.degree.. An incident ray 3 enters facet 4 at an entrance
angle .theta. of about 75.degree., where it is refracted. It is then
totally internally reflected at facet 5, and ray 7 exits perpendicular to
the planar face 8. The large entrance angle .theta. of about 75.degree.was
a requirement for this prismatic lens in its intended use in a high aspect
ratio light fixture.
FIG. 2 shows the linear prismatic film 9 of the current invention,
consisting of a series of isosceles triangle shaped micro prisms 10 with
an apex angle .alpha. of 60.degree.. When an extended area collimated
light beam 11 enters the film perpendicular to facet 12 at the specific
entrance angle .theta. of 60.degree., then the light rays 13 exit
perpendicular to plano surface 14 with the deviation occurring entirely by
total internal refraction at facet 15. Since there is no refraction at
surfaces 12 or 14, there is no dispersion and the ray deviation is
independent of the refractive index of the material. Moreover, since ray
11 of the entrance beam touches both the peak and valley of adjacent
microgrooves, the entrance beam 11 completely fills the TIR facet 15, and
there are no geometric losses or spurious ray deviations.
For the 60.degree.apex angle film, FIG. 3 illustrates that two collimated
incident beams 16a and 16b can be efficiently and spatially combined. The
individual exiting ray bundles 17a and 17b from the left and right
incident beams 16a and 16b are interlaced on a micro scale, such that the
intensity of light over the total area of the film 9 is effectively
doubled.
For the linear prismatic beam-combining film 9 of the current: invention,
the following conditions need to be satisfied for most efficient
operation:
1) The incident light 16a and 16b must be collimated so that light rays
from each lamp enter the entire prismatic film 9 at the same entrance
angle .theta.;
2) The preferred vertex angle .alpha. of the linear prismatic
beam-combining film 9 is 60.degree. plus or minus 2.degree.; and
3) The preferred entrance angle .theta. of the collimated light entering
the linear beam combining film is 60.degree. plus or minus 3.5.degree..
If the prism vertex angle .alpha. is greater than 62.degree., less than 90%
of each reflecting facet is utilized. For example, for an acrylic plastic
prismatic film with a refractive index n=1.492, a vertex angle .alpha. of
62.degree., and an entrance angle .theta. of 63.5.degree., only about 90%
of each reflecting facet is utilized. Excessive underfilling of the
reflecting facets causes the collimated exit beams 17a and 17b produced by
each adjacent microprism to be spatially separated, and dark banding
begins to appear on the illuminated projection screen.
On the other hand, when the prism vertex angle .alpha. is less than
58.degree., less than 90% of the incident light rays 16a and 16b exit
perpendicular to the film. For example, for an acrylic plastic prismatic
film with a refractive index n=1.492, a vertex angle .alpha. of
58.degree., and an entrance angle .theta. of 56.5.degree., about 10% of
the incident rays miss each reflecting facet. The light missing the
reflecting facet exits the film in an uncollimated and uncontrolled
direction, and does not contribute to the illumination on the projection
screen.
Table 1 below illustrates the fraction of beam filling of each facet (BFF)
for various vertex angles .alpha. of the film 9. Values of BFF less than
unity represent underfilling of the reflecting facet, while values of BFF
greater than unity represent overspilling of the reflecting facet. As
explained above, more than 10% of the incident light is spatially
separated or wasted at vertex angles .theta. above 62.degree. or below
58.degree., upon exiting the film 9.
TABLE 1
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.alpha. .theta.
BFF
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50 42.3 1.55
58 56.5 1.11
59 58.3 1.05
60 60.0 1.0
61 61.7 0.947
62 63.5 0.895
.
70 77.7 0.446
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It will be seen from Table 1 that the entrance angle .theta. of the
collimated light 16a and 16b generally changes in a similar fashion as the
vertex angle .alpha. changes, but the relationship is not linear. This is
because at entrance angles .theta. other than 60.degree. the refractive
index n of the material of the film has an effect. The exact relationship
for the entrance angle .theta. necessary to produce maximum screen
illumination at a given vertex angle .alpha. is given by the equation:
##EQU1##
wherein: .theta.=said angle of inclination of said collimated light
.alpha.=said included angle of said prism sides
n=index of refraction of the material of said film.
FIG. 4 shows a projection system 18 that efficiently integrates the output
from two lamps 19a and 19b, providing uniform screen brightness when each
lamp 19a or 19b is individually on, and doubling the screen brightness
when both lamps 19a and 19b are on. Light sources 19a and 19b are
positioned at the focal point of rectangular-shaped Fresnel lenses 20a and
20b, respectively, which collimate the light beams. Each collimated beam
fills the stage aperture 21 at an entrance angle .theta. of 60.degree..
The stage aperture 21 can be square, to accommodate full-size overhead
transparencies, or a reduced size rectangular format, to accommodate LCD
projection panels. Near the stage aperture 21 is the 60.degree. linear
prismatic film 9. The integrated and collimated light exiting from the
60.degree. linear prismatic film 9 enters a circular Fresnel lens 22 which
focuses the light to the projection lens 23. A glass platen 24 is usually
placed above the Fresnel lens 22 to supports the overhead transparency or
LCD projection panel. If the projected facet widths of the linear
prismatic film 9 are less than the resolving power of the eye at normal
screen viewing distances, then each light source 19a and 19b appears to
fully illuminate the entire screen. With both lamps 19a and 19b on, the
screen brightness is effectively doubled over the brightness produced by a
single lamp 19a or 19b.
FIG. 5 shows an alternate arrangement using folding mirrors 25a, 25b, and
26, to combine the output of the two light sources 19a and 19b. An
additional 60.degree. beam combining linear prism 9a is required.
FIG. 6 shows a configuration that combines the output of four light sources
19a, 19b, 19c, and 19d. In this arrangement, the additional linear
prismatic film element 9b, additional Fresnel lens collimators 20c and
20d, and additional folding mirrors 25c and 25d are shown. This cascading
process can be further extended to integrate the output of additional
light sources.
The beam shaping requirements to fill rectangular optical elements in this
multiple lamp projection system are most easily achieved when these
optical elements have an aspect ratio L/W that is close to unity, e.g. a
square perimeter. To achieve this condition, it is preferable that the
each additional optical element be oriented along the shorter side of the
rectangular element preceding it. For the two lamp system shown in FIG. 4
and illustrated again in more detail in FIG. 7, with a rectangular linear
prismatic element 9 having a length L.sub.1 =8 units, and a width W.sub.1
=6 units (L.sub.1 /W.sub.1 =1.33), if the Fresnel lens collimators 20a and
20b (only 20a is shown) are oriented along the W.sub.1 dimension, then the
length L.sub.2 of the collimator is L.sub.2 =W.sub.1 =6 units, and the
width W.sub.2 of the collimator=L.sub.1 /2=4 units, giving an aspect ratio
L.sub.2 /W.sub.2 =6/4=1.5. If the Fresnel lens collimators were oriented
along the L.sub.1 dimension, then the collimator aspect ratio=L.sub.2
/W.sub.2 =8/3=2.67, and beam shaping is more difficult to achieve.
Similarly, for the four lamp system shown in FIG. 6, with a square
prismatic element 9 having a length L.sub.1 =12 units, and a width W.sub.1
=12 units, then the linear prismatic element 9a must have an aspect ratio
L.sub.2 /W.sub.2 =12/6=2. If the Fresnel lens collimators 20a and 20b are
oriented along the W.sub.2 dimension, then the aspect ratio of the
collimators=L.sub.3 /W.sub.3 =6/6=1, which is the ideal beam shaping
requirement.
It is also important to note that for each additional level of multiple
light sources, e.g. two lamps, four lamps, eight lamps, etc., that the
area of each additional linear prism element or Fresnel collimator, is
halved. This limits the achievable light collection and sets a practical
limit on the number of lamps that can be integrated.
FIG. 9 shows a projection system that efficiently integrates the output of
two lamps, as is also illustrated in FIG. 4, again providing uniform
screen brightness when each lamp is individually on, and doubling the
screen brightness when both lamps are on. A polarization-modulating
display 32, such as a liquid crystal display, is positioned between
Fresnel lens 22 and the 60.degree. linear prismatic film 9 to define an
optical window through which light from the lamps is directed. This liquid
crystal display panel 32 comprises a layer of liquid crystalline material
which can be of a twisted nematic or a supertwisted nematic enclosed
between two transparent substrates or plates. Each of these plates may
comprise a transparent control electrode which can be divided into a large
number of columns and rows; thus defining a large number of image elements
in the display panel. These image elements are controlled by driving the
electrodes, and the image display panel is referred to as passively
controlled. Alternatively, one of the substrates can be provided with an
electrode while the other is provided with semi-conductor drive
electronics. A device employing this type of control is referred to as an
actively controlled image display panel.
EXAMPLE
Described below with respect to FIG. 7, and further illustrated in FIG. 8,
is a specific arrangement that has been constructed for use as an LCD
overhead projector. The rectangular stage aperture size has a length
L.sub.1 =228.6 millimeters (9.0 inches) and a width W.sub.1 of 171.5
millimeters (6.75 inches), giving an aspect ratio of L.sub.1 /W.sub.1
=4/3, a common ratio for many LCD projection panels. The light source
filaments 26 (only one is shown) are positioned about 11 millimeters
behind a pair of glass condensers 27 which collect and direct light to the
Fresnel lens collimator a. The light sources 26 are 400 watt, 36 volt flat
mandrel capsule types, ANSI Code designation EVD. A spherical reflector 28
having a diameter of 60 millimeters and a radius of curvature of 32.5
millimeters focuses the back rays in the forward direction. An aspheric
symmetric Pyrex condenser 29, having an approximate focal length of 55
millimeters and a diameter of 60 millimeters, focuses the light from the
lamps 26 into a light cone of circular cross-section. A square optical
crown glass cylinder lens 30 having an approximate focal length of 175
millimeters, and dimensions of 82 by 82 millimeters, is placed in close
proximity to the Pyrex condenser 29. This cylinder lens 30 further
compresses this circular cone of light in one direction to form an
elliptical shaped beam 31. The single element Fresnel lens collimators 20a
have a focal length of 178 millimeters, operate between f/0.75 and f/1.0,
and are oriented symmetrically at 30.degree. from the vertical. The height
W.sub.2 of the Fresnel collimator 20a is half the length L.sub.1 of the
stage aperture, W.sub.2 =114.3 millimeters (4.5 inches), and the width
L.sub.2 of the Fresnel collimator 20a is the width of the stage aperture,
L.sub.2 =171.5 millimeters (6.75 inches). The aspect ratio L.sub.2
/W.sub.2 of the collimating Fresnel lens is 1.5. To efficiently fill the
rectangular aperture of the collimating Fresnel lens, the following
relationship should be approximated: L.sub.2 /W.sub.2 =A/B, where A and B
are the major and minor axes of the elliptic cross-section 31 of the light
beam at the plane of the Fresnel collimator as shown in FIG. 8.
As illustrated in FIG. 4, the 60.degree. linear prismatic film 9 was
fabricated in 2 millimeter thick acrylic plastic, with dimensions slightly
larger than the stage aperture, and the width of each individual prismatic
groove 10 was about 0.5 millimeters. A rectangular acrylic Fresnel lens
22, having a focal length of about 325 millimeters, groove widths between
0.5 and 0.125 millimeters, and approximately the same size as the linear
prismatic film 9, was placed between the linear prismatic film 9 and a
glass platen 21 defining the stage aperture. A triplet projection lens 23
of 330 millimeter focal length projected an image of the stage to fill a
60 inch wide screen at approximately 6.7X magnification.
With this configuration, an average screen illumination of 140 foot-candles
was measured from each individual lamp, and an average screen illumination
of 280 foot-candles with both lamps operating. This is equivalent to the
brightness of a 7000 lumen square aperture overhead projector projecting a
60 inch square image.
It can be appreciated by those skilled in the art, that by the use of
additional folding mirrors in the configurations described, modifications
of the arrangement of optical components can be achieved. These
modifications can reduce the base height of the projector by variation of
width and length of the projector base containing these components. It
will also be appreciated that although specific examples of the invention
have been illustrated, the invention is more generally applicable to any
device which requires collimated light in the optical path.
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