Presentation is loading. Please wait.

Presentation is loading. Please wait.

J. Shawn Addington David T. Wagner

Similar presentations


Presentation on theme: "J. Shawn Addington David T. Wagner"— Presentation transcript:

1 A Study of the Effects of Processing Variations on the Performance of Silicon Solar Cells
J. Shawn Addington David T. Wagner Electrical and Computer Engineering Department Virginia Military Institute

2 Outline Photovoltaic Effect Solar Cell Fundamentals
Solar Cell Design and Fabrication Cell Performance Conclusions

3 Photovoltaic Effect 1839 French physicist Becquerel
Conversion of light to electricity Solar Cell

4 Solar Cell Structure and Operation
p-Si - E + n-Si

5 Solar Cell Structure and Operation
Isc I p-Si e- h+ + Voc - - E + h+ e- h+ e- h+ + V - RL e- h+ e- h+ e- e- h+ n-Si

6 Electrical Model of a Solar Cell
Rs RL I + V -

7 IV Characteristic of a Solar Cell

8 Series Resistance - Rs Rs = R front contact + Rp + Rn + R back contact
p-Si n-Si R front contact R back contact Rp Rn Rs = R front contact + Rp + Rn + R back contact

9 R front contact resistance is reduced by using a large contact area
BUT large contact area blocks more incoming light and lowers power output of cell Optimization? (contact design)

10 R back contact Entire back surface
Large surface area minimizes resistance Optimization? (back side doping)

11 Rn and Rp Rn depends on the Si wafer characteristics
p-Si n-Si R front contact R back contact Rp Rn Rn depends on the Si wafer characteristics Rp depends on the doping characteristics Optimization? (doping variations)

12 Effect of Processing on Rp
Dopant Diffusion p-Si n-Si

13 Effect of Doping Variations on Rs

14 IV Characteristic of a Solar Cell

15 Front Contact Design Optimization
A tapered design to address the trade-off between contact area and shadowing

16 Preliminary Results of Front Contact Design Optimization

17 Current Research in Back Side Doping
R front contact p-Si n-Si Rp Rn n+ - Si R back contact

18 Solar Radiation is Composed of a Range of Wavelengths

19 Solar Cell Performance as a Function of Incident Radiation
short wavelengths long wavelengths e- h+ p-Si - E + h+ h+ e- e- e- h+ n-Si

20 Tuning the “Target Window” through Process Variation
shorter doping times longer doping times p-Si - E + n-Si

21 Solar Cell Output Power vs Incident Wavelength
Maximum power output for 750nm incident wavelength 3 hour doping process Expect sensitivity to shift as doping process varies

22 Current Research Maximum power wavelength vs doping variations
Back-side doping Front contact design optimization Antireflective coatings

23 Conclusions Thanks! How solar cells work Why solar cells work that way
How design and processing affect solar cell performance Ongoing research


Download ppt "J. Shawn Addington David T. Wagner"

Similar presentations


Ads by Google