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Lesson 23: Introduction to Solar Energy and Photo Cells ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson 23 332a.pptx.

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Presentation on theme: "Lesson 23: Introduction to Solar Energy and Photo Cells ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson 23 332a.pptx."— Presentation transcript:

1 Lesson 23: Introduction to Solar Energy and Photo Cells ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson 23 332a.pptx

2 2 Learning Objectives After this presentation you will be able to:  Identify the solar spectrum  Determine the angle that captures the maximum solar energy  Explain the atomic difference between conductor, insulators, and semiconductors  Explain physics behind the photoelectric effect  Compute the open circuit voltage and short circuit current of a photocell

3 Lesson 23 332a.pptx3 Solar Energy and Photocells Solar Spectrum AM0 =1.36 kW/m 2 Incident on Atmosphere AM1.5-1.0 kW/m 2 Passing through Atmosphere Incident to 48 0 angle to vertical Includes absorption of water vapor, C0 2, methane.

4 Lesson 23 332a.pptx4 Solar Energy Conversion Direct Radiation depends on season, location, cloudiness. Yearly average 30% Average Intensity (W/m 2 ) 10% in lower Canada to 50% in tropics Solar Array Sun Defuse Radiation unfocusable. Long wavelengths scatter more color sky blue. Solar Radiation perpendicular to Array Surface

5 Lesson 23 332a.pptx5 Solar Intensity

6 Lesson 23 332a.pptx6 Solar Intensity

7 Lesson 23 332a.pptx7 Conductors, Insulators and Semiconductors Semiconductors – Valence electrons exist Bonded to other atoms Bonds broken by external energy like heat or light Examples: Silicon, Germanium Conductors – Free electrons in atomic structure Valence electrons form current when electric potential applied. Examples: copper, silver Insulators – No free electrons in valence band Examples: glass, plastics.

8 Lesson 23 332a.pptx8 Semiconductors Doped Semiconductors – Impurities added to increase conductance P-type semiconductor - excess holes (absent electrons) N-type semiconductor – excess electrons Charge drift forms Depletion Zone PN Junction

9 Lesson 23 332a.pptx9 Forward Biased PN Junction V lowers potential barrier for electrons upsets balance I flows Forward Bias

10 Lesson 23 332a.pptx10 Solar.ppt10 PN Junction-Diode Operation PN Junction Characteristic V  = cut-in voltage 0.6 V for silicon Junction conducts when forward biased V T = Voltage-equivalent of Temperature = 0.026 V at room temperature I s = saturation current depends on junction area and doping

11 Lesson 23 332a.pptx11 Photoelectric Effect Photon E >1.1 eV I C = cell current I L = reverse current Light striking a PN junction creates currents. Photons must have sufficient energy increase electron energy and create Electron/hole pairs

12 Lesson 23 332a.pptx12 Open Circuit Voltage/Short Circuit Current Open circuit means R= ∞ and I C =0, so open circuit voltage is V T = 0.026 V at room temperature I s = saturation current I L = reverse current Cell power output given by

13 END LESSON 23 ET 332a Dc Motors, Generators and Energy Conversion Devices Lesson 23 332a.pptx13


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