Electrophoretic switch for a light pipe

• US 5,317,667 A
• Filed: 11/23/1992
• Issued: 05/31/1994
• Est. Priority Date: 11/23/1992
• Status: Expired due to Fees

• Current Assignee: Visteon Global Technologies Incorporated (Visteon Corporation)
• Original Assignee: Ford Motor Company
• Inventors: Weber, Willes H., Remillard, Jeffrey T., Ginder, John M.
• Primary Examiner(s): Lee, John D.
• Assistant Examiner(s): PALMER, PHAN T H
• Application Number:
  US07/980,066
• Time in Patent Office: 554 Days
• Field of Search: 385/147, 385/4, 385/11, 385/123-127, 359/296, 359/71
• US Class Current: 385/147
• CPC Class Codes: G02B 6/032 with non solid core or cladding G02B6/02295 takes precedence
• CPC Class Codes: G02B 6/3568 characterised by the actuating force
• CPC Class Codes: G02F 1/167 by electrophoresis
• CPC Class Codes: G02F 1/1677 Structural association of cells with optical devices, e.g. reflectors or illuminating devices
• CPC Class Codes: G02F 2203/026 attenuated or frustrated internal reflection

Abstract

An electrophoretic light switch is provided for controlling light in a light pipe having a transparent inner conductor, an outer conductor and a solution containing charged particles. Light is absorbed by the solution when the particles are attracted to the inner conductor causing the light intensity in the light pipe to be reduced.

Claims

1. A device for modulating light output of a light pipe comprising:

a light pipe having a first index of refraction;

a transparent first conductor coating said light pipe having a second index of refraction greater than said first index of refraction;

a cylindrical second conductor located substantially concentrically with respect to said light pipe and having a diameter greater than or equal to the diameter of said first conductor forming a space therebetween; and

a solution having a third index of refraction less than said first index of refraction containing charged particles having a fourth index of refraction greater than said third index of refraction filling the space between said first conductor and said second conductor, said charged particles adapted to move in response to a potential difference between said first conductor and said second conductor; and

retaining means for holding said second conductor in a fixed location with respect to said first conductor and for retaining said solution in said space.

2. A device as in claim 1 wherein said light pipe is comprised of glass.

3. A device as in claim 1 wherein said light pipe is comprised of plastic.

4. A device as in claim 1 wherein said transparent first conductor is comprised of an indium-tin oxide.

5. A device as in claim 1 wherein said second conductor has an inner surface coated with a light absorbing material.

6. A device as in claim 5 wherein said second conductor is comprised of stainless steel.

7. A device as in claim 1 wherein said solution is comprised of acetonitrile.

8. A device as in claim 7 wherein said charged particles are comprised of polystryene spheres.

9. A device as in claim 1 further comprising connection means for coupling respective voltages to said first conductor and said second conductor.

10. A device as in claim 1 further comprising a voltage source electrically connected to said first and second conductors providing a potential difference therebetween.

11. A method for controlling the light output of a light pipe comprising the steps of:

providing a transparent first conductor adjacent to and surrounding said light pipe, a second conductor located substantially concentrically with respect to said first conductor and forming a space therebetween and a solution containing charged particles filling said space;

applying a potential difference between said first conductor and said second conductor; and

controlling the movement of said charged particles in said solution by changing the potential difference of said first conductor with respect to said second conductor.

12. A method as in claim 11 further comprising the steps of:

creating a evanescent field by the interaction of the light in said light pipe with the charged particles contained in the solution; and

absorbing the light created by the evanescent field into said solution thereby reducing the light output of the light pipe.

13. A method as in claim 11 wherein said transparent first conductor has an index of refraction equal to or greater than that of said light pipe.

14. A method as in claim 11 wherein said solution has an index of refraction less than the index of refraction of said light pipe.

15. A method as in claim 11 wherein said charged particles have an index of refraction greater than the index of refraction of said solution.