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UCSD Physics 12
Submitted by :- Gaurav (2k20/EE/102)
Submitted to:- Prof. Md. Gulam Mustafa
UCSD Physics 12
• Highly purified silicon (Si) from sand, quartz, etc. is “doped” with intentional
impurities at controlled concentrations to produce a p-n junction
– p-n junctions are common and useful: diodes, CCDs, photodiodes, transistors
• A photon incident on the p-n junction liberates an electron
– photon disappears, any excess energy goes into kinetic energy of electron (heat)
– electron wanders around drunkenly, and might stumble into “depletion region”
where electric field exists (electrons, being negative, move against field arrows)
– electric field sweeps electron across the junction, constituting a current
– more photons  more electrons  more current  more power
n-type silicon
p-type silicon
photon of light
liberated electron
electric field
Si doped with
boron, e.g.
Si doped with
phosphorous, e.g.
Photovoltaic (PV) Scheme
UCSD Physics 12
Spring 2013 3
PV types
• Single-crystal silicon
– 15–18% efficient, typically
– expensive to make (grown as big crystal)
• Poly-crystalline silicon
– 12–16% efficient, slowly improving
– cheaper to make (cast in ingots)
• Amorphous silicon (non-crystalline)
– 4–8% efficient
– cheapest per Watt
– called “thin film”, easily deposited on a wide range of
surface types
UCSD Physics 12
simulation
UCSD Physics 12
Spring 2013 5
Results
DC voltage, we get from solar panel
UCSD Physics 12
Pulsating AC supply
UCSD Physics 12
Pure AC
UCSD Physics 12

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ppe lab project.ppt

  • 1. UCSD Physics 12 Submitted by :- Gaurav (2k20/EE/102) Submitted to:- Prof. Md. Gulam Mustafa
  • 2. UCSD Physics 12 • Highly purified silicon (Si) from sand, quartz, etc. is “doped” with intentional impurities at controlled concentrations to produce a p-n junction – p-n junctions are common and useful: diodes, CCDs, photodiodes, transistors • A photon incident on the p-n junction liberates an electron – photon disappears, any excess energy goes into kinetic energy of electron (heat) – electron wanders around drunkenly, and might stumble into “depletion region” where electric field exists (electrons, being negative, move against field arrows) – electric field sweeps electron across the junction, constituting a current – more photons  more electrons  more current  more power n-type silicon p-type silicon photon of light liberated electron electric field Si doped with boron, e.g. Si doped with phosphorous, e.g. Photovoltaic (PV) Scheme
  • 3. UCSD Physics 12 Spring 2013 3 PV types • Single-crystal silicon – 15–18% efficient, typically – expensive to make (grown as big crystal) • Poly-crystalline silicon – 12–16% efficient, slowly improving – cheaper to make (cast in ingots) • Amorphous silicon (non-crystalline) – 4–8% efficient – cheapest per Watt – called “thin film”, easily deposited on a wide range of surface types
  • 5. UCSD Physics 12 Spring 2013 5 Results DC voltage, we get from solar panel

Editor's Notes

  1. Spring 2013
  2. Spring 2013
  3. Spring 2013