CA2092950A1 - High efficiency squarewave voltage driver - Google Patents
High efficiency squarewave voltage driverInfo
- Publication number
- CA2092950A1 CA2092950A1 CA 2092950 CA2092950A CA2092950A1 CA 2092950 A1 CA2092950 A1 CA 2092950A1 CA 2092950 CA2092950 CA 2092950 CA 2092950 A CA2092950 A CA 2092950A CA 2092950 A1 CA2092950 A1 CA 2092950A1
- Authority
- CA
- Canada
- Prior art keywords
- capacitive
- light valve
- voltage
- suspended particle
- circuit
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
Classifications
-
- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G3/00—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes
- G09G3/20—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters
- G09G3/34—Control arrangements or circuits, of interest only in connection with visual indicators other than cathode-ray tubes for presentation of an assembly of a number of characters, e.g. a page, by composing the assembly by combination of individual elements arranged in a matrix no fixed position being assigned to or needed to be assigned to the individual characters or partial characters by control of light from an independent source
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/0121—Operation of devices; Circuit arrangements, not otherwise provided for in this subclass
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/17—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on variable-absorption elements not provided for in groups G02F1/015 - G02F1/169
- G02F1/172—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on variable-absorption elements not provided for in groups G02F1/015 - G02F1/169 based on a suspension of orientable dipolar particles, e.g. suspended particles displays
-
- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09G—ARRANGEMENTS OR CIRCUITS FOR CONTROL OF INDICATING DEVICES USING STATIC MEANS TO PRESENT VARIABLE INFORMATION
- G09G2310/00—Command of the display device
- G09G2310/06—Details of flat display driving waveforms
Abstract
Presented is a device and method for providing a means of driving capacitive cells, such as those comprising suspended particle light valve windows, with a squarewave voltage signal at a select frequency with high efficiency and low power requirements. The invention uses an inductive circuit in parallel withthe capacitive load of the capacitive cell, a dc voltage source, and a fast switching means connected to timely control the polarity of the voltage source to the capacitive cell.
Description
20929~0 High Efficiency Squarewave Voltage Driver Background of the Invention A suspended particle light valve window consists of a thin cell whose 5 walls consist of glass or plastic sheets coated on their inner surfaces with transparent, electrically conducting films, and which is filled with a suspendedparticle fluid. The suspended particles within the fluid medium are responsive to the application of an electric field and change the optical properties of the fluid depending on the intensity and polarity of the applied electric field. Such light o valves must be electrically excited by applying ac voltage, preferably squarewave, to the two conducting films. Because of their construction, the light valves are electrically capacitive in nature.
Ddving them with a conventional power supply is very inefficient because the capacitance must be repeatedly charged, discharged, and recharged with 15 opposite polarity. frhis can be a serious disadvantage for low-power battery operation. Higher efficiency could be achieved by connecting an inductor to the ~ ;
cell, and operating the cell in a resonant circuit at the ddve frequency. Howeva, thc waveform in this case would be sinusoidal, not square.
It is an object of this invention to introduce a volhge drive means and 20 method for powering capacitive suspended particle light valve windows or other capacitive circuits or cells, and which requires low power level and produces anefficient squarewave volhge cycle.
It is a further object of this invention to utilize an LC circuit to efficiently ~
deliver a square wave voltage signal across a capacitive suspended particle light ~ ~ i 25 valve window or other capacitive circuit or cell using a low power dc primary volhge source.
~ ~.
.. . . . ,. ~ , - .
~` 2 ~ 9 2 ~
Summary of the Invention The invention provides a means of driving capacitive cells, such as those comprising suspended particle light valve windows, with a squarewave voltage signal at a select frequency with high efficiency and low power requirements. ~ -The invention uses an inductive circuit in parallel with the capacitive load of the capacitive cell, a dc voltage source, and a switching means connected to timely control the polarity of the voltage source to the capacitive cell. Energy ~ --conservation and rapid polarity reversal is accomplished with the switching means ~ ~ -by connecting the capacitive cell with the inductive circuit making an LC circuit o during times of making polarity changes.
A11 switches of the switching means would, in a typical application, be ~ ~
fast electronic switches comprising transistors, field effect transistors and other ~ ~ ;
microelectronic or optoelectronic devices. They are operated and controlled by acomputerized timing circuit. With the capacitive light valve cell represented by a capacitance C, and the inductance of the parallel circuit by L, the LC circuit formed by the switching means has a resonant frequency fLC = 1/2,~ J~ which is chosen to be higher (greater) than that of the squarewave voltage required todrive the light valve.
Brief Descri~tior~ Drawings Figure l shows a simplified schematic of the equiva1ent circuit for the invention.
Figure 2 is a voltage and current plot for an ideal LC circuit at resonance.
Figure 3 show8 the timing for the switches and the generated squarewave voltage applied to the light valvo shutter.
Figure 4 shows an embodiment of an optoelectronic switch circuit.
3 2~9~9~1~
Description of the Preferre~l Embodiment The invention, in general, comprises a dc power source, a capacitive light valve window, an inductance connected in parallel with the light valve, a first switching means for connecting or disconnecting the inductance from the light s valve, a second switching means connected between the light valve and the power source for reversing polarity to the light valve window, and a timing and control means for operating the switching means to a predetermined duty cycle. The preferred duty cycle is a cyclical squarewave which is optimized for operation of ~ ~;
the light valve window.
A preferred embodiment is shown in Fig. 1. The squarewave driver circuit 10 is shown compdsing a dc power source 12, connected through switches . .
14, 16, 18, and 20 to light valve 26. An inductance 28 is connected via switch ~ -24 in parallel with light valve 26. A timing and control unit 22 is connected to ;
provide programmed control of the operation of switches 14, 16, 18, 20, and 24.
15 In a typical application, all switches will be fast electronic switches. -The light valve 26, being capacitive and connected in parallel with -inductance 28, forms an LC circuit with inductance 28 when switch 24 is closed.
The resonant frequency of this circuit is fLC = 1/2~ ~. Fig. 2 shows an ideal plot for the voltage 46 and current 48 as functions of time for this LC circuit if it 20 were allowed to oscillate freely without loss.
:. ~ , . :.
The cyclical voltage desired to be applied at light vatve 26 is shown in Fig. 3. It is preferable that the voltage at light valve 26 be at some predeterrnined level +V, S4, for a half cycle, and then reversed to -V, 56, for the remaining half cycle. This procedure is repeated at some predetermined 25 frequency fO to establish the desired continuous squarewave voltagc signal. The voltagc level V, of course, is the level selected for dc power source 12.
- , , ~ . ,. . .. , ~ , ,, .,; . .. : :, . ... .
4 2~92 Switching polarity of the voltage level at 50 and 52 is desired to be close to simple step changes.
To accomplish rapid approximation to simple step changes at 50 and 52, ^ -and at a minimum of expended energy, it is necessary to adjust the LC circuit tos have a resonant freguency fLC chosen to be significantly greater than fO, perhaps by ten times or more. If we assume initially that controller 22 has all switchesopen e~ccept for switches 16 and 20, then light valve 26 is charged to power ~ -source voltage +V. This corresponds to the point 40 in Fig. 2 and to the level 54 in Figure 3. Switches 16 and 20 are kept closed by controller 22 for the 10 desired half pedod of the squarewave ddve signa1 to light valve 26. Dudng this timc the capacitance of light valve 26 is fully charged.
Then switches 16 and 20 are opened to remove source 12 from the capacitive cell 26. Immediately thereafter switch 24 is closed. The LC circuit is ~ i now formed and will start to ~resonate" or "dng", with the voltage across light 15 valve 26 falling along voltage curve 46 in Fig. 2, passing through zero, and ideally reach the valuc -V at point 42 in Fig. 2. In reality, because of losses in the resonant circuit, the volt~ge reached at point 42 will be numerically somewhat less than thc ideal valuc of -V. Now controller 22 opens switch 24 and the LC
circuit has oscillated through one half cycle of its resonant frequency fLC . What 20 has been achieved is a revcrsal of the pdadq of the voltage on the capacitance of light valvc 26 with only a smaU loss of stored energy and voltage due to the resistance of the LC circuit.
Immediately after opening switch 24, the controller 22 closes switches 14 and 18. This reconnects power source 12 to light valve 26 again, but with 25 opposite poladty. The capacitance of light valve 26 is now charged fully to thc -` s 2~9~5~3 voltage -V, 56 in Fig. 3, thereby making up for the small loss of energy which occurred during the voltage reversal cycle.
Now controller 22 keeps all switches open except for switches 14 and 18 ~ ~ ~
for the second half period of the squarewave drive signal to light valve 26. At ~ ;
the end of this period switches 14 and 18 are opened and switch 24 is immediately thereafter closed by controller 22. This allows the LC resonant circuit to execute the next ha1f cycle of its oscillation from point 42 to point 44 in Fig. 2, reversing the voltage across the capacitance of light valve 26 and bringing it back, ideally, to +V.
o Again, controller 22 opens switch 24 at completion of this half cycle for -: . ,.
the LC circuit, i.e., at point 44 of Fig. 2, and immediately thereafter closes switches 16 and 20 to start the squarewave cycle over again. At this point we have returned to the starting point of the square wave cycle; one full cycle of the squarewave drive signal on light valve 26 has been completed, and one full cycleof the LC resonant circuit has been completed, with each segment of the square wave cycle carefully timed and formed. ~ ;
Half cycles of the sinusoidal waveform of the LC resonant circuit make up the quasi-step transitions of the squarewave drive voltage, as shown at points 50 and 52, in Fig.3. The drive voltage of Fig. 3 is not a perfect or true squarewave, but is an excellent approximation to a squarewave drive signal needed for light valve 26, provided that fLC is sufficiently higher than fO.
This process is repeated under timing and control of the controller 22 to generate a continuous desired squarewave drive signal for light valve 26 at a high efficiency and with the capability of design for low power, portable operation. It should be further noted that switch 24 is always operated at times when the ,f,~, current in the LC circuit is zero because the LC loop current is 90 out phase with the voltage as shown by the current and voltage curves in Fig.2. ;-FiB. 4 shows an embodiment for the structure of an optoelectronic switching circuit to serve as one of the switches in the invention. This circuit is 5 comprised of a FET 62, a npn transistor 68, a high speed opto coupler 70, and resisters 64 and 66. The circuit to be controlled by the switch is represented by --60. The power source 12 connections are terminals 72, and connection to the timing and control means 22 occurs through terminals 72. In this embodiment the FET was an IRF530 transistor, the non transistor 68 was a 2N2222, and the 10 opto coupla was an ISO6 6N136 device. To those skilled in the art it is clearthat there are other choices of equivalent embodiments to accomplish the high speed switching required in the invention.
The preferred embodiment presented herein has focused on the development of a squarewave voltage driver; however, it should be clear that controller 22 is capable of being programmed to develop other waveform signals dependent only upon the choice of the components involved in this invention.
While these specific embodiments of the invention herein have been illustrated and described in detail, it will be appreciated that the invention is not limited thereto, sinco many modifications may be made by one skilled in the art which 20 fall within the true spirit and scope of the invention.
Ddving them with a conventional power supply is very inefficient because the capacitance must be repeatedly charged, discharged, and recharged with 15 opposite polarity. frhis can be a serious disadvantage for low-power battery operation. Higher efficiency could be achieved by connecting an inductor to the ~ ;
cell, and operating the cell in a resonant circuit at the ddve frequency. Howeva, thc waveform in this case would be sinusoidal, not square.
It is an object of this invention to introduce a volhge drive means and 20 method for powering capacitive suspended particle light valve windows or other capacitive circuits or cells, and which requires low power level and produces anefficient squarewave volhge cycle.
It is a further object of this invention to utilize an LC circuit to efficiently ~
deliver a square wave voltage signal across a capacitive suspended particle light ~ ~ i 25 valve window or other capacitive circuit or cell using a low power dc primary volhge source.
~ ~.
.. . . . ,. ~ , - .
~` 2 ~ 9 2 ~
Summary of the Invention The invention provides a means of driving capacitive cells, such as those comprising suspended particle light valve windows, with a squarewave voltage signal at a select frequency with high efficiency and low power requirements. ~ -The invention uses an inductive circuit in parallel with the capacitive load of the capacitive cell, a dc voltage source, and a switching means connected to timely control the polarity of the voltage source to the capacitive cell. Energy ~ --conservation and rapid polarity reversal is accomplished with the switching means ~ ~ -by connecting the capacitive cell with the inductive circuit making an LC circuit o during times of making polarity changes.
A11 switches of the switching means would, in a typical application, be ~ ~
fast electronic switches comprising transistors, field effect transistors and other ~ ~ ;
microelectronic or optoelectronic devices. They are operated and controlled by acomputerized timing circuit. With the capacitive light valve cell represented by a capacitance C, and the inductance of the parallel circuit by L, the LC circuit formed by the switching means has a resonant frequency fLC = 1/2,~ J~ which is chosen to be higher (greater) than that of the squarewave voltage required todrive the light valve.
Brief Descri~tior~ Drawings Figure l shows a simplified schematic of the equiva1ent circuit for the invention.
Figure 2 is a voltage and current plot for an ideal LC circuit at resonance.
Figure 3 show8 the timing for the switches and the generated squarewave voltage applied to the light valvo shutter.
Figure 4 shows an embodiment of an optoelectronic switch circuit.
3 2~9~9~1~
Description of the Preferre~l Embodiment The invention, in general, comprises a dc power source, a capacitive light valve window, an inductance connected in parallel with the light valve, a first switching means for connecting or disconnecting the inductance from the light s valve, a second switching means connected between the light valve and the power source for reversing polarity to the light valve window, and a timing and control means for operating the switching means to a predetermined duty cycle. The preferred duty cycle is a cyclical squarewave which is optimized for operation of ~ ~;
the light valve window.
A preferred embodiment is shown in Fig. 1. The squarewave driver circuit 10 is shown compdsing a dc power source 12, connected through switches . .
14, 16, 18, and 20 to light valve 26. An inductance 28 is connected via switch ~ -24 in parallel with light valve 26. A timing and control unit 22 is connected to ;
provide programmed control of the operation of switches 14, 16, 18, 20, and 24.
15 In a typical application, all switches will be fast electronic switches. -The light valve 26, being capacitive and connected in parallel with -inductance 28, forms an LC circuit with inductance 28 when switch 24 is closed.
The resonant frequency of this circuit is fLC = 1/2~ ~. Fig. 2 shows an ideal plot for the voltage 46 and current 48 as functions of time for this LC circuit if it 20 were allowed to oscillate freely without loss.
:. ~ , . :.
The cyclical voltage desired to be applied at light vatve 26 is shown in Fig. 3. It is preferable that the voltage at light valve 26 be at some predeterrnined level +V, S4, for a half cycle, and then reversed to -V, 56, for the remaining half cycle. This procedure is repeated at some predetermined 25 frequency fO to establish the desired continuous squarewave voltagc signal. The voltagc level V, of course, is the level selected for dc power source 12.
- , , ~ . ,. . .. , ~ , ,, .,; . .. : :, . ... .
4 2~92 Switching polarity of the voltage level at 50 and 52 is desired to be close to simple step changes.
To accomplish rapid approximation to simple step changes at 50 and 52, ^ -and at a minimum of expended energy, it is necessary to adjust the LC circuit tos have a resonant freguency fLC chosen to be significantly greater than fO, perhaps by ten times or more. If we assume initially that controller 22 has all switchesopen e~ccept for switches 16 and 20, then light valve 26 is charged to power ~ -source voltage +V. This corresponds to the point 40 in Fig. 2 and to the level 54 in Figure 3. Switches 16 and 20 are kept closed by controller 22 for the 10 desired half pedod of the squarewave ddve signa1 to light valve 26. Dudng this timc the capacitance of light valve 26 is fully charged.
Then switches 16 and 20 are opened to remove source 12 from the capacitive cell 26. Immediately thereafter switch 24 is closed. The LC circuit is ~ i now formed and will start to ~resonate" or "dng", with the voltage across light 15 valve 26 falling along voltage curve 46 in Fig. 2, passing through zero, and ideally reach the valuc -V at point 42 in Fig. 2. In reality, because of losses in the resonant circuit, the volt~ge reached at point 42 will be numerically somewhat less than thc ideal valuc of -V. Now controller 22 opens switch 24 and the LC
circuit has oscillated through one half cycle of its resonant frequency fLC . What 20 has been achieved is a revcrsal of the pdadq of the voltage on the capacitance of light valvc 26 with only a smaU loss of stored energy and voltage due to the resistance of the LC circuit.
Immediately after opening switch 24, the controller 22 closes switches 14 and 18. This reconnects power source 12 to light valve 26 again, but with 25 opposite poladty. The capacitance of light valve 26 is now charged fully to thc -` s 2~9~5~3 voltage -V, 56 in Fig. 3, thereby making up for the small loss of energy which occurred during the voltage reversal cycle.
Now controller 22 keeps all switches open except for switches 14 and 18 ~ ~ ~
for the second half period of the squarewave drive signal to light valve 26. At ~ ;
the end of this period switches 14 and 18 are opened and switch 24 is immediately thereafter closed by controller 22. This allows the LC resonant circuit to execute the next ha1f cycle of its oscillation from point 42 to point 44 in Fig. 2, reversing the voltage across the capacitance of light valve 26 and bringing it back, ideally, to +V.
o Again, controller 22 opens switch 24 at completion of this half cycle for -: . ,.
the LC circuit, i.e., at point 44 of Fig. 2, and immediately thereafter closes switches 16 and 20 to start the squarewave cycle over again. At this point we have returned to the starting point of the square wave cycle; one full cycle of the squarewave drive signal on light valve 26 has been completed, and one full cycleof the LC resonant circuit has been completed, with each segment of the square wave cycle carefully timed and formed. ~ ;
Half cycles of the sinusoidal waveform of the LC resonant circuit make up the quasi-step transitions of the squarewave drive voltage, as shown at points 50 and 52, in Fig.3. The drive voltage of Fig. 3 is not a perfect or true squarewave, but is an excellent approximation to a squarewave drive signal needed for light valve 26, provided that fLC is sufficiently higher than fO.
This process is repeated under timing and control of the controller 22 to generate a continuous desired squarewave drive signal for light valve 26 at a high efficiency and with the capability of design for low power, portable operation. It should be further noted that switch 24 is always operated at times when the ,f,~, current in the LC circuit is zero because the LC loop current is 90 out phase with the voltage as shown by the current and voltage curves in Fig.2. ;-FiB. 4 shows an embodiment for the structure of an optoelectronic switching circuit to serve as one of the switches in the invention. This circuit is 5 comprised of a FET 62, a npn transistor 68, a high speed opto coupler 70, and resisters 64 and 66. The circuit to be controlled by the switch is represented by --60. The power source 12 connections are terminals 72, and connection to the timing and control means 22 occurs through terminals 72. In this embodiment the FET was an IRF530 transistor, the non transistor 68 was a 2N2222, and the 10 opto coupla was an ISO6 6N136 device. To those skilled in the art it is clearthat there are other choices of equivalent embodiments to accomplish the high speed switching required in the invention.
The preferred embodiment presented herein has focused on the development of a squarewave voltage driver; however, it should be clear that controller 22 is capable of being programmed to develop other waveform signals dependent only upon the choice of the components involved in this invention.
While these specific embodiments of the invention herein have been illustrated and described in detail, it will be appreciated that the invention is not limited thereto, sinco many modifications may be made by one skilled in the art which 20 fall within the true spirit and scope of the invention.
Claims (7)
1. A high efficiency voltage driver for a capacitive cell such as a suspended particle light valve window which comprises:
a dc power source;
a capacitive cell;
an inductance connected in parallel with the capacitive cell;
a first switching means positioned between said capacitive cell and said inductance for connecting or disconnecting said inductance from said capacitive cell;
a second switching means positioned between said capacitive cell and said power source for connecting and reversing polarity of said dc power source to said capacitive cell; and a timing and control means for operating said first and second switching means according to a predetermined switching sequence.
a dc power source;
a capacitive cell;
an inductance connected in parallel with the capacitive cell;
a first switching means positioned between said capacitive cell and said inductance for connecting or disconnecting said inductance from said capacitive cell;
a second switching means positioned between said capacitive cell and said power source for connecting and reversing polarity of said dc power source to said capacitive cell; and a timing and control means for operating said first and second switching means according to a predetermined switching sequence.
2. A high efficiency voltage driver according to Claim 1 wherein said capacitive cell is a suspended particle light valve window.
3. A high efficiency voltage driver according to Claim 1 wherein said first and second switching means are fast electronic switches.
4. A high efficiency voltage driver according to Claim 3 wherein said timing and control means Is a computer.
5. A high efficiency voltage driver according to Claim 3 wherein said fast electronic switches are transistors.
6. A high efficiency voltage driver according to Claim 3 wherein said fast electronic switches are transistorized circuits.
7. A method for driving a capacitive suspended particle light valve window with an efficient squarewave voltage signal which comprises the steps of:
providing a dc voltage, V, across said capacitive suspended particle light valve window for one half cycle of a squarewave voltage signal with a predetermined period of frequency, fO;
disconnecting said dc voltage from said capacitive suspended particle light valve window and immediately thereafter connecting said capacitive suspended particle light valve window to an LC circuit with a predetermined resonant frequency, fLC, selected to be higher than the preselected frequency fO for said squarewave driver;
allowing said LC circuit to operate for one half of its natural cycle defined by its resonant frequency, fLC, thereby allowing the voltage applied to said light valve to be reversed to a value slightly lower in absolute value, because of slight resistive losses in the LC circuit, than the negative of the original voltage applied to said light valve;
disabling said LC circuit and immediately thereafter connecting in reverse polarity said dc voltage to said capacitive suspended particle light valve window and thereby establishing a dc voltage, -V, across said capacitive suspended particle light valve window for a second half of the squarewave period;
disconnecting said inverse dc voltage and immediately thereafter reconnecting said capacitive suspended particle light valve window to said LC circuit;
allowing said LC circuit to operate for one half of its natural cycle defined by its resonant frequency, fLC. thereby allowing the voltage applied to said capacitive suspended particle light valve window to again be reversed to a value slightly lower in absolute value, because of slight resistive losses in the LC circuit, than said original voltage applied to said capacitive suspended particle light valve window;
disabling said LC circuit and immediately thereafter reconnecting in original polarity said dc voltage to said capacitive suspended particle light valve window thereby establishing said original dc voltage, V, across said capacitive suspended particle light valve window; and repeating above steps to form a continuous square wave driving voltage signal across said capacitive suspended particle light valve window.
providing a dc voltage, V, across said capacitive suspended particle light valve window for one half cycle of a squarewave voltage signal with a predetermined period of frequency, fO;
disconnecting said dc voltage from said capacitive suspended particle light valve window and immediately thereafter connecting said capacitive suspended particle light valve window to an LC circuit with a predetermined resonant frequency, fLC, selected to be higher than the preselected frequency fO for said squarewave driver;
allowing said LC circuit to operate for one half of its natural cycle defined by its resonant frequency, fLC, thereby allowing the voltage applied to said light valve to be reversed to a value slightly lower in absolute value, because of slight resistive losses in the LC circuit, than the negative of the original voltage applied to said light valve;
disabling said LC circuit and immediately thereafter connecting in reverse polarity said dc voltage to said capacitive suspended particle light valve window and thereby establishing a dc voltage, -V, across said capacitive suspended particle light valve window for a second half of the squarewave period;
disconnecting said inverse dc voltage and immediately thereafter reconnecting said capacitive suspended particle light valve window to said LC circuit;
allowing said LC circuit to operate for one half of its natural cycle defined by its resonant frequency, fLC. thereby allowing the voltage applied to said capacitive suspended particle light valve window to again be reversed to a value slightly lower in absolute value, because of slight resistive losses in the LC circuit, than said original voltage applied to said capacitive suspended particle light valve window;
disabling said LC circuit and immediately thereafter reconnecting in original polarity said dc voltage to said capacitive suspended particle light valve window thereby establishing said original dc voltage, V, across said capacitive suspended particle light valve window; and repeating above steps to form a continuous square wave driving voltage signal across said capacitive suspended particle light valve window.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA 2092950 CA2092950A1 (en) | 1993-03-30 | 1993-03-30 | High efficiency squarewave voltage driver |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA 2092950 CA2092950A1 (en) | 1993-03-30 | 1993-03-30 | High efficiency squarewave voltage driver |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2092950A1 true CA2092950A1 (en) | 1994-10-01 |
Family
ID=4151387
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA 2092950 Abandoned CA2092950A1 (en) | 1993-03-30 | 1993-03-30 | High efficiency squarewave voltage driver |
Country Status (1)
| Country | Link |
|---|---|
| CA (1) | CA2092950A1 (en) |
-
1993
- 1993-03-30 CA CA 2092950 patent/CA2092950A1/en not_active Abandoned
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