Light homogenization
US-2017285348-A1 · Oct 5, 2017 · US
US11133455B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11133455-B2 |
| Application number | US-201916703291-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 4, 2019 |
| Priority date | Dec 11, 2018 |
| Publication date | Sep 28, 2021 |
| Grant date | Sep 28, 2021 |
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An example device includes a nanovoided polymer element, which may be located at least in part between the electrodes. In some examples, the nanovoided polymer element may include anisotropic voids, including a gas, and separated from each other by polymer walls. The device may be an electroactive device, such as an actuator having a response time for a transition between actuation states. The gas may have a characteristic diffusion time (e.g., to diffuse half the mean wall thickness through the polymer walls) that is less than the response time. The nanovoids may be sufficiently small (e.g., below 1 micron in diameter or an analogous dimension), and/or the polymer walls may be sufficiently thin, such that the gas interchange between gas in the voids and gas absorbed by the polymer walls may occur faster than the response time, and in some examples, effectively instantaneously.
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What is claimed is: 1. A device, comprising: a first electrode; a second electrode; and an anisotropic nanovoided polymer comprising anisotropic nanovoids within a polymer matrix, the anisotropic nanovoids separated from each other by polymer walls having a mean wall thickness, the anisotropic nanovoids comprising a gas, wherein: at least a portion of the anisotropic nanovoided polymer is located between the first electrode and the second electrode; the gas has a characteristic diffusion time to diffuse half the mean wall thickness through the polymer walls; the device is an electroactive device having a response time for a transition from a first state to a second state; and the characteristic diffusion time is less than the response time. 2. The device of claim 1 , wherein the mean thickness of the polymer walls is sufficiently thin so that the gas can diffuse through the polymer walls during the response time. 3. The device of claim 1 , wherein the characteristic diffusion time for the gas is less than approximately one millisecond. 4. The device of claim 1 , wherein the device is an actuator, and the response time is an actuation time for the transition from the first state to the second state in response to an electric field applied between the first electrode and the second electrode. 5. The device of claim 4 , wherein the first state is a generally uncompressed state. 6. The device of claim 4 , wherein the second state is compressed by at least 50%, relative to the first state, along a compression direction parallel to the electric field. 7. The device of claim 6 , wherein the anisotropic nanovoids in a generally uncompressed state are elongated along at least one direction perpendicular to the compression direction. 8. The device of claim 1 , wherein the mean wall thickness of the polymer walls is less than 1 micron. 9. The device of claim 1 , wherein the response time is less than approximately 1 millisecond. 10. The device of claim 1 , wherein the response time is at least ten times greater than the characteristic diffusion time. 11. The device of claim 1 , wherein the polymer matrix comprises an electroactive polymer. 12. The device of claim 11 , wherein the electroactive polymer shows appreciable electroconstriction when an electric field is applied between the first electrode and the second electrode. 13. The device of claim 11 , wherein the electroactive polymer comprises a silicone polymer. 14. The device of claim 13 , wherein the silicone polymer is polydimethylsiloxane, or a derivative thereof. 15. The device of claim 1 , wherein the gas comprises air. 16. The device of claim 1 , wherein the anisotropic nanovoids have an anisotropy ratio determined by a ratio of a first dimension measured along a first direction, and a second dimension measured along a second direction perpendicular to the first direction, wherein the anisotropy ratio is at least approximately 2 when the anisotropic nanovoided polymer is in a generally uncompressed state. 17. The device of claim 1 , wherein the device is sensor, and the response time is a deformation time for a mechanically-induced transition from the first state to the second state. 18. A method, comprising: applying an electric field between a first electrode and a second electrode to switch an actuator from a first state to a second state, wherein the actuator comprises a nanovoided polymer located between the first electrode and the second electrode, the nanovoided polymer comprising nanovoids enclosing a gas separated by polymer walls, the second state is compressed parallel to the electric field, relative to the first state, and a characteristic diffusion time of the gas through the polymer walls is less than a response time of the actuator. 19. The method of claim 18 , wherein the second state is at least 50% compressed along a compression direction of the electric field, relative to a generally uncompressed state. 20. The method of claim 18 , wherein the response time of the actuator is 1 millisecond or less.
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