PHASE CHANGE DEVICE

• US 20100225989A1
• Filed: 03/03/2010
• Published: 09/09/2010
• Est. Priority Date: 03/05/2009
• Status: Abandoned Application

• Current Assignee: Regents of the University of California (University of California)
• Original Assignee: Regents of the University of California (University of California)
• Inventors: Anders, Andre
• Application Number:
  US12/716,838
• Publication Number:
  US 20100225989A1
• Time in Patent Office: Days
• US Class Current: 359/288
• CPC Class Codes: G02F 1/0147 based on thermo-optic effects G02F1/132 takes precedence
• CPC Class Codes: G02F 1/19 based on variable-reflection or variable-refraction elements not provided for in groups G02F1/015 - G02F1/169

Abstract

A phase change material is applied as a very thin film to a transparent substrate such as glass, which material when switched from the amorphous to the crystalline state and back again can affect the reflectivity/transmittance of the combined substrate-coating system. When used with glass panels in the fabrication of relatively large area window glass, the change in spectrally selective transmittance can be used to modulate the amount of sunlight passing through the glass, and thus reduce the amount of cooling required for an interior space in the summertime, and the amount of heating required of that same interior space in the wintertime, while also optimizing the use of visible daylight. Exemplary of a suitable phase change material for glass coating is GeSb or BiSn. Heating of the phase change material to initiate a change in phase can be provided by the application of electric energy, such as supplied from a pulsed power supply, or radiant energy, such as from a laser.

Claims

1. An article comprising a transparent substrate upon which has been coated with a very thin layer of a phase-change material exhibiting high resistivity and low reflectance in the amorphous state, and low resistivity and high reflectivity in the crystalline state, wherein the difference between the crystallization temperature of the phase-change material and its melting temperature is in the order of 25°

C. to 50°

C.

2. The article of claim 1 wherein the transparent substrate is glass.

3. The article of claim 2 wherein the transparent substrate is a window glass.

4. The article of claim 2 wherein the phase-change material is selected from a semi metal, a metal or metalloid or metal alloy composition.

5. The article of claim 4 wherein the phase-change material has a melting temperature of between 120°

C. and 300°

C.

6. The article of claim 5 wherein the melting temperature is between 160°

C. and 250°

C.

7. The article of claim 1 further including a conductive layer which is in contact with both the transparent substrate and the phase change layer.

8. The article of claim 7 wherein the conductive layer is disposed between the transparent layer and the phase change layer.

9. The article of claim 7 wherein the article further includes a capping layer disposed on the side of the phase-change layer opposite the side facing the transparent layer.

10. A method for changing the transmittance of the article of claim 1 to incident light wherein the phase of the phase change material is changed from one phase to the other by the application of short heat pulse.

11. The method of claim 10 wherein heat is applied to the phase change material by the passage of a pulse of electric current.

12. The method of claim 11 wherein a pulsed power supply is used to supply the pulse of electric current.

13. The method of claim 12 wherein the duration of the electric current pulse is in the order of less than one to one or more micro seconds.

14. The method of claim 13 wherein the duration of the cool down of the phase change material, after pulsed heating is in the order of less than one to one or more micro seconds.

15. The method of claim 10 wherein the heat is supplied by the application of a radiant energy source.

16. The method of claim 15 wherein the radiant energy source is a laser.

17. The method of claim 16 wherein the wavelength of the infrared laser is longer than the absorptive wavelength of glass on which it is deposited.

18. The method of claim 16 wherein the laser is a UV laser.

19. The method of claim 16 wherein the radiant energy source is a pulsed flash light source.

20. The method of claim 10 wherein the conversion of the phase change material from the amorphous phase to the crystalline phase is achieved by heating the material above the crystalline temperature, but below the melting temperature, followed by cooling.

21. The method of claim 10 wherein the conversion of the phase change from crystalline to amorphous comprises the rapid, pulsed heating of the material to above its melting temperature, followed by rapid cooling to quench the material, wherein both the heating and cooling steps are carried out in the order of a few microseconds.

22. An insulated glass unit comprising a frame into which two parallel panes of glass are secured in opposing positions, spaced a distance one from the other, wherein, the interior surface of at least one of the panes of glass is coated with a phase change material, and a radiation heat source is positioned within the space between the panes of glass, said radiation heat source mounted to a movable fixture designed to move the radiation source over the coated area, such as to fully subject said coated area to the radiation of the source, when activated.