Non-imaging freeform optical device for use in a high concentration photovoltaic device

• US 8,553,338 B1
• Filed: 08/30/2010
• Issued: 10/08/2013
• Est. Priority Date: 08/28/2009
• Status: Expired due to Fees

• Current Assignee: Zheng Jason Geng
• Original Assignee: Zheng Jason Geng
• Inventors: Geng, Zheng Jason
• Primary Examiner(s): Harrington, Alicia M
• Application Number:
  US12/871,498
• Time in Patent Office: 1,135 Days
• Field of Search: 359/708, 359/742, 359/627, 359726-728, 359/712, 362/341, 362/347, 362/317
• US Class Current: 359/727
• CPC Class Codes: F24S 23/31 having discontinuous faces, e.g. Fresnel lenses
• CPC Class Codes: F24S 23/70 with reflectors
• CPC Class Codes: F24S 23/79 with spaced and opposed interacting reflective surfaces
• CPC Class Codes: G02B 19/0028 refractive and reflective surfaces, e.g. non-imaging catadioptric systems
• CPC Class Codes: G02B 19/0042 for use with direct solar radiation
• CPC Class Codes: G02B 3/02 with non-spherical faces G02B3/10 takes precedence
• CPC Class Codes: H01L 31/0543 comprising light concentrating means of the refractive type, e.g. lenses
• CPC Class Codes: H01L 31/0547 comprising light concentrating means of the reflecting type, e.g. parabolic mirrors, concentrators using total internal reflection
• CPC Class Codes: Y02E 10/40 Solar thermal energy, e.g. solar towers
• CPC Class Codes: Y02E 10/52 PV systems with concentrators

Abstract

A high concentration photovoltaic (HCPV) optics are described. In one example, an HCPV device can include a frame and a solar sensor cell attached to the frame. The solar cell can be configured to receive an optical beam and can further be configured to convert solar energy in the incident optical beam into electrical energy or power. The HCPV device can further include a non-imaging freeform optical device. The optical device can have an asymmetric surface profile with a predefined surface normal arranged to direct incident optical beams toward an entire solar sensor cell surface area. The freeform optical device can have a larger diameter than the solar sensor cell. Also, the freeform optical device can have an asymmetric surface profile shaped to concentrate the incident optical beams onto the solar sensor cell.

Claims

1. A method for forming a non-imaging freeform optical device for use in a high concentration photovoltaic device, comprising:

calculating surface normals for a plurality of locations on a surface of the non-imaging freeform optical device based on a half angular field of view of a sun and a predetermined distance from the non-imaging freeform optical device to a solar sensor cell;

shaping a mold for a substrate of the non-imaging freeform optical device, shaping further comprising forming a surface geometry of the mold according to the surface normals calculated for the non-imaging freeform optical device;

filling the mold with substrate material to form a substrate in the shape of the mold;

separating the mold and the substrate after the substrate material has conformed to the shape of the mold; and

polishing the substrate.

2. A method as in claim 1, wherein calculating surface normals for the plurality of locations on the surface of the non-imaging freeform optical device comprises calculating surface normals based on reflectance from the non-imaging freeform optical device to the solar sensor cell.

3. A method as in claim 1, wherein calculating surface normals for the plurality of locations on the surface of the non-imaging freeform optical device comprises calculating surface normals based on refraction from the non-imaging freeform optical device to the solar sensor cell.

4. A method for designing a non-imaging freeform optical device for use in a high concentration photovoltaic device, the method comprising:

identifying a concentration region relative the non-imaging freeform optical device for concentrating incident light from the non-imaging freeform optical device;

initiating a first ray from a first edge of the concentration region toward a predetermined point on the non-imaging freeform optical device using a ray-tracing model;

redirecting the first ray toward a first wavefront;

initiating a second ray from a second wavefront that impinges on the predetermined point offset from an angular impingement of the first wavefront at the predetermined point by an angular view of a sun;

redirecting the second ray from the non-imaging freeform optical device to a second edge of the non-imaging freeform optical device; and

calculating a surface normal at the predetermined point for the non-imaging freeform optical device such that the first and second wavefronts are redirected to a surface of the non-imaging freeform optical device.

5. A method as in claim 4, wherein the non-imaging freeform optical device is a second optical device and the method includes redirecting the first ray from a first optical device after initiaing the first ray and before redirecting the first ray.

6. A method as in claim 5, further comprising calculating a surface normal of the first optical device.

7. A method as in claim 4, wherein the non-imaging freeform optical device is a first optical device and the method includes redirecting the second ray from a second optical device after redirecting the second ray and before calculating the surface normal.

8. A method as in claim 7, further comprising calculating a surface normal of the second optical device.

9. A method as in claim 4, wherein at least one of redirecting the first ray and redirecting the second ray comprises redirecting using a mirror to reflect the first ray or the second ray.

10. A method as in claim 4, wherein at least one of redirecting the first ray and redirecting the second ray comprises redirecting using a lens to refract the first ray or the second ray.

11. A method as in claim 4, wherein the steps of identifying the concentration region, initiating the first ray, redirecting the first ray, initiating the second ray, redirecting the second ray, and calculating the surface normal are repeated for multiple points on the non-imaging freeform optical device.