U.S. patent number 3,594,065 [Application Number 04/834,929] was granted by the patent office on 1971-07-20 for multiple iris raster.
Invention is credited to Alvin M. Marks.
United States Patent |
3,594,065 |
Marks |
July 20, 1971 |
MULTIPLE IRIS RASTER
Abstract
A variable light-transmitting panel is described having plural
spaced electrostatic control electrodes. The control electrodes can
be selectively energized to show a picture or other desired graphic
information by modulating transmitted light or by controlling
selected areas to alter the reflection coefficient of light. The
control electrodes are mounted adjacent to a thin layer of
nonconductive liquid containing a large number of minute crystal
dipoles. The opaque portions of the raster are due to the random
distribution of the dipoles caused by Brownian motion of the fluid
molecules. Application of an electric field by the electrodes
produces an alignment of the dipoles and permits the passage of
light. A small mask may be positioned over each electrode area to
block out any light produced by voltages below a threshold
voltage.
Inventors: |
Marks; Alvin M. (Whitestone,
NY) |
Family
ID: |
25268150 |
Appl.
No.: |
04/834,929 |
Filed: |
May 26, 1969 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
Issue Date |
|
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567456 |
Jul 25, 1966 |
3451742 |
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Current U.S.
Class: |
359/296 |
Current CPC
Class: |
G02F
1/172 (20130101) |
Current International
Class: |
G02F
1/01 (20060101); G02F 1/17 (20060101); G02f
001/34 () |
Field of
Search: |
;350/160,266,267,269,285 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Wibert; R. L.
Assistant Examiner: Rothenberg; J.
Parent Case Text
This application is a continuation-in-part of an application for
Multiple Iris Raster, filed July 25, 1966, Ser. No. 567,456, now
U.S. Pat. No. 3,451,742, by Alvin M. Marks.
Claims
Having thus fully described the invention, what I claim as new and
desire to be secured by Letters Patent of the United States,
is:
1. A multiple iris raster comprising; a first transparent
nonconductive plate forming one boundary of the raster, a second
transparent nonconductive plate spaced from the first plate and
forming the other boundary of the raster, a transparent
nonconductive fluid held between said first and second plates, a
plurality of dipole particles in said fluid, a plurality of spaced
parallel electrodes secured to said first plate with means for
connection to an external circuit, a plurality of spaced parallel
electrodes secured to said second plate and positioned at right
angles to the electrodes in the first plate with means for
connection to an external circuit, a plurality of conductive pins
secured in the first and second plates, each pin positioned along
said electrodes and in contact therewith, each of said pins mounted
normal to the surface of said plates and each pin in one plate
mounted opposite to a pin in the other plate, and threshold means
consisting of an opaque mask mounted at each of the pin positions
on one of the plates to prevent the passage of light through the
raster below a selected voltage.
2. A multiple iris raster as claimed in claim 1 wherein each of
said conductive electrodes in the first and second plates is
connected through a resistor to a common conductor to ground.
3. A raster as claimed in claim 1 wherein said conductive
electrodes in the first plate are sequentially connected to a
signal source of alternating current at the same time said
conductive electrodes in the second plate are sequently connected
to the same signal source but having a reversed polarity.
4. A raster as claimed in claim 1 wherein said dipole particles
have a length which is about one-third the wavelength of visible
light and a diameter which is less than one-tenth of said
wavelength.
5. A raster as claimed in claim 1 wherein said pins extend only
part of the distance through the plates and are not in contact with
the fluid.
6. A raster as claimed in claim 1 wherein said pins extend all the
way through the plates and make contact with the fluid between the
plates.
7. A raster as claimed in claim 1 wherein said first and second
plates are substantially flat and parallel to each other and
thereby define a fluid chamber having parallel surfaces.
8. A raster as claimed in claim 1 wherein said dipole particles are
elongated optically active dichroic crystals formed by
precipitation from a liquid solution.
9. A raster as claimed in claim 1 wherein said dipole particles are
made of Herapathite.
10. A raster as claimed in claim 1 wherein said dipole particles
are made of assymetric metal particles.
11. A raster as claimed in claim 1 wherein said pins are spaced
along said electrodes at a distance equal to the distance between
the electrodes on the other plate.
12. A multiple iris raster comprising a first transparent
nonconductive plate forming one boundary of the raster, a second
transparent nonconductive plate spaced from the first plate and
forming the other boundary of the raster, a transparent
nonconductive fluid held between said first and second plates, a
plurality of dipole particles in said fluid a layer of transparent
plastic material on the fluid side of each of the transparent
plates between the plates and the fluid, a plurality of
electrically conductive dipoles permanently aligned normal to the
plate faces and carried within the plastic layers, a plurality of
spaced parallel electrodes secured to the first plate with means
for connection to an external circuit, a plurality of spaced
parallel electrodes secured to the second plate and positioned at
right angles to the electrodes in the first plate with means for
connection to an external circuit, said electrically conductive
dipoles within the plastic layers providing a capacitive path to
control the electric field in the dipole layer between the plates,
and a threshold means to prevent passage of the light through the
raster below a selected voltage.
Description
BACKGROUND OF THE INVENTION
This invention relates to a multiple iris raster for selectively
passing portions of a light beam through desired minute areas. The
invention has particular reference to a simple system of energizing
the areas to form small well defined electrostatic fields and
thereby align a large number of dipoles suspended in a liquid layer
in said areas. The phenomena associated with the alignment of tiny
dipoles in an electric field and the dipole movements due to
Brownian bombardment have been known for some time and various
attempts have been made to control their positions to modulate
transmitted light. Generally, the results have not been
satisfactory because the application of the electric field was not
confined to a small area and the definition of the transmitted
light was poor. The present invention employs a plurality of
equally spaced crossed electrodes connected to a plurality of
conductive pins which extend toward the fluid layer forming a
plurality of axial point to point electrodes. The electric fields
produced by this arrangement are well defined and more intense than
those produced by prior art structures.
The dipoles used in the liquid cell should be quite small, having a
length of about one-third to one-half of the wavelength of the
transmitted light. Also, the dipole particles must have a width and
thickness which is less than one-tenth of the wavelength of the
incident light. Dipoles may be made of crystals such as Herapathite
or metal crystals which have a natural elongated or asymmetric
shape, such as a plate or rod. While larger dimensions may be used,
these are generally not preferred since the small particles serve
to pass or cut off the incident light and quickly respond to the
action of the fluid molecules to form an opaque mass due to their
statistical random position.
A minimum critical field intensity or threshold field must be
applied before any substantial alignment of the dipoles is
accomplished. When the field intensity is less than critical, the
Brownian motion of the liquid molecules is sufficient to provide a
random position to most of the dipoles so that very little light
can pass through the cell. When the field intensity across opposed
electrodes is greater than the critical voltage, a narrow
cylindrical space is filled with aligned dipoles and a small
quantity of light is transmitted. As the voltage increases, the
diameter of the cylindrical space is increased, passing more light.
It has been found that a linear relationship exists between the
diameter of the light spot, the transmitted light flux and the
applied voltage above the critical value. To provide a sharp
threshold in the light transmission at the critical voltage,
suitable masks have been added to the cell structure to eliminate
transmitted light below the threshold voltage.
With a dipolar suspension containing ions, the application of a
direct current voltage to the electrodes causes a temporary
alignment of dipoles and then disalignment causing a momentarily
transparent spot. The dipoles quickly disalign due to the formation
of a shield of positive ions at the negative electrode, and vice
versa. This shield can be avoided by the application of an
alternating current voltage having a half period which is less than
the relaxation time of the dipole particle. If the half period is
of the order of the relaxation time, the dipoles tend to disalign
during the time the electric field intensity is going through zero.
Such alternate alignment and disalignment produces turbulence in
the suspension and the result is a poorly defined transmitted light
beam. The frequency of the aligning voltage is preferably within
the range of 0.01 to 10 megahertz. With a nonionic dipolar
suspension, such as a metal dipole particle in a nonionic fluid
(silicone, aliphatic, aromatic, ester, fluoro carbon, or others, or
mixtures thereof) a DC field may be used and the pin electrodes may
be in contact with the fluid layer, as shown in FIG. 4. When ions
are present a transparent insulating layer must be employed between
the electrode pins and the dipole fluid layer, as shown in FIGS. 2
and 3.
The average energy applied to the dipoles by the impact of the
liquid molecules corresponding to a threshold voltage E.sub.r of
about 100 volts /cm. Since the dipole rod is about 2 .times.
10.sup..sup.-5 cm. long this provides a potential difference across
the dipole rod of about 2 .times. 10.sup..sup.-3 volts. The impacts
are random in direction, causing a random direction of the dipoles
thereby producing an opaque layer. The aligning field intensity
must exceed the critical value E.sub.r to produce light
transmission.
One of the features of the present invention is a plurality of
spots in a raster which operate to produce light transmission in a
time interval of the order of 1 microsecond.
Another feature of the invention is the provision of a large flat
display panel which can be used in connection with a television
receiving circuit.
For a better understanding of the present invention, together with
other details and features thereof, reference is made to the
following description taken in connection with the accompanying
drawings.
BRIEF DESCRIPTION OF THE FIGURES
FIG. 1 is an isometric view showing the raster, an external
illumination means, and two scanning circuits (shown in block)
which apply voltages to the raster electrodes.
FIG. 2 is a cross-sectional view on an enlarged scale showing a
portion of one of the raster plates indicating its construction and
the method of forming the plate prior to the positioning of the
conductive electrodes and pins.
FIG. 3 is a cross-sectional view on an enlarged scale showing a
portion of the raster cell with details of the pins, insulated from
a fluid layer containing a suspension of dipoles and free ions.
FIG. 4 is a cross-sectional view similar to FIG. 3 but showing the
pins penetrating the first and second transparent plates to contact
a nonionic fluid layer containing a suspension of dipoles.
FIG. 5 is a cross-sectional view of another arrangement showing the
raster, a diffusing plate, and an illumination means behind the
diffusing plate which may be a gaseous discharge device.
FIG. 6 is a plan view of a portion of the raster showing the
external connections of the crossed electrodes and the positions of
the masks.
FIG. 7 is a graph showing the relationship of the applied voltage
to the transmitted light flux.
FIG. 8 shows a means of employing a random aligned conducting
dipole suspension layer in lieu of the pins using capacitive
contact.
FIG. 9 shows light flux and spot diameter versus voltage applied
between pin pairs.
DESCRIPTION OF THE PREFERRED EMBODIMENT
Referring now to the figures, the raster includes two spaced
parallel plates 10 and 11, shown in detail in FIGS. 3 and 4. These
plates are made of transparent nonconductive material such as glass
or Lucite. Prior to assembly, each of the plates is formed with a
series of spaced parallel grooves 12, (best shown in FIG. 2) on the
outer faces thereof. A plurality of holes 13 are drilled or formed
in the plates normal to the faces to accommodate pins 15 which will
be inserted later. Each hole 13 is drilled or formed at the bottom
of a groove 12. After the pins 15 have been inserted into the
plates, electrical conductive material 16, 17 is deposited in the
grooves 12 to form the crossed electrodes. The plates are then
mounted adjacent to but spaced from each other and sealed around
their edges, with the grooves 12 of one plate mounted at 90.degree.
to the grooves on the other plate. The space between the plates is
then filled with a suspension of a nonconductive transparent fluid
and dipole particles 14. As shown in FIG. 6, the electrode material
16, 17 on each plate is connected to lead-in conductors 16A on one
side for one plate and to similar lead-in conductors 17A for the
other plate. In FIG. 3, these conductors are for the application of
alternating current signals to modulate the transmission of the
suspension 14. On the other side of plate 10 the electrodes 16A are
connected to resistors 20 and a grounded conductor 21. In a similar
manner the electrodes 17A in plate 11 are connected to resistors 22
and a grounded conductor 23.
Pins 15 on one plate are positioned along the length of the
electrode 16A and spaced apart from each other a distance equal to
the spacing of the electrodes 17A in the other plate. This
arrangement produces a pattern of pins and electrodes in which each
pin on one plate is opposite and in line with a pin on the other
plate. The pins 15 are generally arranged so that they penetrate
each plate 10, 11 for about 90 percent of the plate's thickness.
With this construction, the pins are not in direct contact with the
fluid between the plates. This construction is shown in FIGS. 2 and
3. In certain applications where longer pins are used, these pins,
as shown in FIG. 4, traverse the entire thickness of plates 10 and
11 and make contact with the fluid suspension 14.
Referring now specifically to FIG. 1, one of the uses of the iris
raster is shown. A source of illumination, such as an incandescent
lamp (not shown), is mounted within a lighttight container 24. The
light from this source is focused by a lens 25 onto the assembled
raster to provide substantially equal illumination over the entire
raster area. In this illustration light is reflected from a
reflective layer 26 at the rear of the raster forward to the
observer's eye 40. The electrodes 16A on one edge of the raster are
energized by pulse circuits and a delay line generally indicated in
FIG. 1 as vertical-scanning pulse circuit 28 as previously
described in my U.S. Pat. No. 2,670,402 issued Feb. 23, 1954. In a
similar manner, the electrodes 17A are connected to a
horizontal-scanning pulse circuit 31. Pulse circuit sources 28 and
31 may be a pulse circuit and delay line. The delay lines may be of
any suitable type, such as inductance-capacitance, diode or triode
transistors, preferably as miniature or microminiature circuits
capable of controlling voltage pulses in a predetermined sequential
manner.
It is obvious that this type of raster can be used for many
different purposes, one of them being the showing of a television
picture. When a television picture is to be shown, the picture
signal is fed in from a picture amplifier which is added to the
voltage pulse. Each electrode receives a voltage pulse in a timed
sequence which starts from the left-hand edge and moves to the
right-hand edge in synchronism with the received television signal.
During each horizontal application of pulses one of the electrodes
is energized by the applied pulse plus the picture signal. During
the next horizontal application of pulses, the next lower electrode
is energized. As the process continues, a complete pattern of the
entire raster is energized and at the end of the frame time
interval, all the pin pairs, where light is to be transmitted, will
then have received voltage pulses which establish an electrostatic
field between them thereby aligning dipoles in those areas. The
alignment varies according to the applied voltage so as to provide
a light flux proportional to the voltage above a threshold voltage.
The diameter of the light spot is also proportional to the applied
voltage in a certain range (see FIG. 9).
As explained above, a threshold voltage is preferably maintained
across opposite pin electrodes 15 by applying an alternating
voltage of the order of 10 to 100 volts. This voltage is the
minimum critical voltage (V/2 in FIG. 7) above which the dipoles
start to align, thus forming circular dots of transmitted light
between opposite pin electrodes 15. Upon the application of the
additional voltage from the television picture signal, the spot
diameter of aligned dipoles in the selected areas within the
suspension 14 increases to form small transparent annular areas
permitting light to pass through the raster at those places thus
modulating the spot transmission in accordance with the signal
voltage. An increase in voltage expands the annular areas and
permits more light to pass. When the voltage is removed, the
dipoles again are disaligned by Brownian action to form an opaque
nontransmitting area.
FIG. 5 shows an alternate means of illumination of the dipole
suspension from the rear to show a picture. A diffusing plate 33,
which may be ground glass, diffuses the light from a plurality of
gaseous discharge lamps 34, only one being shown in FIG. 5. This
form of display has very little thickness and may be used as a self
luminous "picture on the wall" "flat" television screen, or data
display screen.
FIGS. 3, 4, and 6, each show a small round mask 35 placed at each
electrode crossover. These masks cut off the light which might be
transmitted by the suspension below a chosen threshold voltage. As
explained above and shown graphically in FIG. 7, a voltage of about
half the maximum voltage of the sum of the signal and pulse
voltages produces a light cutoff. Below a given voltage (40 volts
as in FIG. 9) the tendency to align the dipoles is matched by the
energy of the liquid molecules to produce Brownian motion and this
provides cutoff. If a greater threshold voltage is required then a
circular mask of suitable diameter is used, for example, 0.3 mm. if
the electrode spacing is 0.6 mm. As might be expected, this voltage
is not definite and varies with electrode spacings, fluid
thickness, dipole concentration, and other factors.
When the display is operated, the applied voltage is not directly
proportional to the light values desired to be produced. Instead,
zero light transmission is denoted by a voltage of half the maximum
voltage. If the maximum voltage is set at 100 volts, then the
opaque condition must occur from 0 to 50 volts, half transmission
at 75 volts and full transmission at 100 volts. Such a system
results in a linear correspondence between signal voltage values
and light transmission as indicated by the straight portion of the
curve shown in FIG. 7.
The signal voltages are applied to conductors 16A and 17A (see FIG.
6) and thereby produce a voltage on the conductors because of the
potential drop across resistors 20 and 22. All those conductors
which receive no signal are at ground potential because they are
connected through resistors 20 and 22 to ground. Since each
conductor 16A receives a positive voltage at the same time a
conductor 17A receives an equal negative voltage, they are always
at a voltage which is V/2 reactive to ground.
Let it be assumed that the maximum signal voltages of +50 volts are
applied to vertical conductor 17B and -50 volts to horizontal
conductor 16B. Then only at the cross over position 37 is there a
potential difference of 100 volts, and a maximum light transmission
is thereby effected in the dipole suspension at the cross over
point shown as the area indicated by the circle 38. At the same
time a potential difference of 50 volts is applied to the
suspension at all other points on conductors 16B and 17B. This
series of voltages produces no light transmission, as indicated
below V/2 in FIG. 7, and in FIG. 4. The random distribution of
dipoles adjoining the vertical pencil of aligned dipoles blocks
light. At all other signal voltages less than the maximum value
there is no tendency to produce misplaced pencils since the side
voltages are always one-half the signal voltage, and elsewhere the
voltages between the pins are zero, except at the cross over where
the full voltage is applied, and the light spot appears.
With the device shown in FIG. 4, in which the pins contact the
fluid and when a nonionic fluid is preferably used, an AC or DC
voltage may be employed.
In the device shown in FIG. 3, in which the pins are insulated from
the fluid, the fluid may be ionic or nonionic and an AC voltage
preferably above 5 kHz. is then used to prevent ionic migration and
blocking of the voltage used to align the dipoles.
Herapathite dipole suspensions generally are ionic and require the
device shown in FIG. 3, while metal or other conductive materials
form dipoles without ions in a nonionic fluid and may be used with
the device of FIG. 4.
In the device shown in FIG. 8, a layer of transparent plastic or
glass material 50 is adhered to the faces of the plates 10, 11
facing the dipole suspension 14. A plurality of electrically
conductive dipoles 51 such as metal whiskers or elongated crystals
are embedded in the plastic material. The dipoles 51 are
permanently aligned normal to the major faces of the layer material
50 and parallel to the path of the light through the raster panel.
Alignment of the dipoles 51 can be achieved while the plastic or
glass is in a viscous state by the application of a suitable
electric or magnetic field.
The device shown in FIG. 8 is similar to that shown in FIG. 4 in
all other respects except that the pins 15 may now be omitted.
Contact is made at the cross over points by the capacitive effect
of the metal dipoles which is greatest where the distance between
the electrode lines is least.
In the above disclosure an iris raster has been described which is
operated by signal voltages applied to a series of vertical and
horizontal electrodes. Pins or aligned dipoles are used to
concentrate the field in the dipole fluid suspension at the cross
over points of the X and Y electrodes. Vertical and horizontal
electrodes are connected through resistors to ground. The dipolar
suspension is of a nature to respond by transmitting light above a
threshold electric field E.sub.r. At points where light must not be
transmitted an artificial threshold consisting of small masks 35
may be used over the center of the spot.
* * * * *