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Solar Photovoltaic Physics
Basic Physics and
Materials Science of Solar Cells
Syllabus • Chapter 1: Introduction
• Chapter 2: Solar Resource
• Chapter 3: Fundamental of Photovoltaic (Light absorption, Excitation and Transport)
• Chapter 4: PN Junctions
• Chapter 5: Solar Cells and Parameters
• Chapter 6: Design of Silicon Cells
• Chapter 7: Manufacturing Si Cells
• Chapter 8: Thin film Solar cells [CdS/CdTe, CdS/CIGS and GaAs].
• Chapter 9: Dye/Quantum dots sensitized solar cells
• Chapter 10: Modules, Arrays and Characterization
Books
http://www.pvcdrom.pveducation.org/
• Jenny Nelson: The Physics of Solar Cells:
Imperial College Press
• Peter Wurfel: Physics of Solar Cells: From Basic
Principles to Advanced Concepts: Viley -VCH
Books • Bube, R. H. Photovoltaic Materials. London, UK: Imperial College Press, 1998. ISBN:
9781860940651.
• Green, M. A. Solar Cells: Operating Principles, Technology and System Applications.
Upper Saddle River, NJ: Prentice Hall, 1981. ISBN: 9780138222703.
• Wenham, S. R., M. A. Green, M. E. Watt, R. Corkish. Applied Photovoltaics. 2nd ed.
New York, NY: Earthscan Publications Ltd., 2007. ISBN: 9781844074013.
• Green, M. A. Silicon Solar Cells: Advanced Principles and Practice. Sydney, Australia:
Centre for Photovoltaic Devices & Systems, 1995. ISBN: 9780733409943.
• Aberle, A. G. Crystalline Silicon Solar Cells - Advanced Surface Passivation &
Analysis. Sydney, Australia: University of New South Wales, 2004. ISBN:
9780733406454
• Poortmans, J., and V. Arkhipov. Thin Film Solar Cells: Fabrication, Characterization
and Applications. Hoboken, NJ: John Wiley & Sons, 2006. ISBN: 9780470091265.
• Green, M. A. Third Generation Photovoltaics: Advanced Solar Energy Conversion.
New York, NY: Springer-Verlag, 2007. ISBN: 9783540265627.
• Luque, A., and S. Hegedus. Handbook of Photovoltaic Science and Engineering.
Hoboken, NJ: John Wiley & Sons, 2003. ISBN: 9780471491965
Tests and Scores
• Mid Test : 30
• Final Test : 30
• Presentations [2] : 20
• Attendance : 20
Total : 100
A Brief History of Photovoltaic Technology
• 1839 – Photovoltaic effect discovered by Becquerel.
• 1870s – Hertz developed solid selenium PV (2%).
• 1905 – Photoelectric effect explained by A. Einstein.
• 1930s – Light meters for photography commonly employed cells of copper oxide or selenium.
• 1954 – Bell Laboratories developed the first crystalline silicon cell (4%).
• 1958 – PV cells on the space satellite U.S. Vanguard (better than expected).
Things Start To Get Interesting...
• Mid 1970s – World energy crisis started and millions of dollars spent in research and development of cheaper and more efficient solar cells.
• 1976 – First amorphous silicon cell developed by Wronski and Carlson.
• 1980’s - Steady progress towards higher efficiency and many new types introduced
• 1990’s - Large scale production of solar cells more than 10% efficient with the following materials: – Ga-As and other III-V’s – Crystalline, Polycrystalline, and Amorphous Silicon – CuInGaSe2 and CdTe – TiO2 Dye-sensitized (still under research and not yet
commercialized)
• Today prices continue to drop and new “3rd generation” solar cells are researched.
Types of Solar Photovoltaic Materials
Photovoltaic Materials
Electronic Structure of Semiconductors
• Silicon
• Group 4 elemental
semiconductor
• Silicon crystal forms the
diamond lattice
• Resulting in the use of four
valence electrons of each
silicon atom.
Crystalline
Silicon
Amorphous Silicon
Solar PV Materials: Crystalline & Polycrystalline Silicon
• Advantages:
– High Efficiency (14-22%)
– Established technology
(The leader)
– Stable
• Disadvantages:
– Expensive production
– Low absorption coefficient
– Large amount of highly
purified feedstock
Amorphous Silicon Advantages:
• High absorption (don’t need a lot of material)
• Established technology
• Ease of integration into buildings
• Excellent ecological balance sheet
• Cheaper than the glass, metal, or plastic you deposit it on
Disadvantages:
• Only moderate stabilized efficiency 7-10%
• Instability- It degrades when light hits it
– Now degraded steady state
The Sun
Solar Radiation In Space The solar irradiance on an object some distance D from the sun is found by dividing the
total power emitted from the sun by the surface area over which the sunlight falls
Solar Radiation Outside the Earth's Atmosphere
Blackbody Radiation
The total power density from a
blackbody is determined by
integrating the spectral irradiance
over all wavelengths which gives:
where is the Stefan-Boltzmann constant
and T is the temperature of the blackbody
(K).
The wavelength at which the spectral
irradiance is the highest, or, in other
words the wavelength where most of
the power is emitted.
The Solar Spectrum The spectral content of
the incident light;
• the radiant power density from the sun;
• the angle at which the incident solar radiation strikes a photovoltaic module; and
• the radiant energy from the sun throughout a year or day for a particular
surface.
The Solar Spectrum • the spectral content of
the incident light;
• the radiant power density from the sun;
• the angle at which the incident solar radiation strikes a photovoltaic module; and
• the radiant energy from the sun throughout a year or day for a particular
surface.
Atmospheric Effects
Atmospheric effects have several impacts on the solar
radiation at the Earth's surface. The major effects for
photovoltaic applications are:
• A reduction in the power of the solar radiation due to absorption, scattering and reflection in the atmosphere;
• A change in the spectral content of the solar radiation due to greater absorption or scattering of some wavelengths;
• The introduction of a diffuse or indirect component into the solar radiation; and
• Local variations in the atmosphere(such as water vapor, clouds and pollution) which have additional effects on the incident power, spectrum and directionality.
Atmospheric Effects
When dealing with "particles" such as
photons or electrons, a commonly
used unit of energy is the electron-
volt (eV) rather than the joule (J). An
electron volt is the energy required to
raise an electron through 1 volt, thus
1 eV = 1.602 x 10-19 J.
Spectral Irradiance
The spectral irradiance of xenon (green), halogen (blue) and mercury (red) light bulbs (left axis) are compared to the spectral irradiance from the sun (purple, which corresponds to the right axis).
Radiant Power Density
Quantifying Solar Power
Orbit Ellipticity
Air Mass
Standardized Solar Spectrum and Solar Irradiation
Average Monthly Solar Radiation
Attempts to Simulate Solar Spectra • Better matches: Xe lamps with air mass filters
The ideal illumination source would
have following features A spatial non uniformity of less than 1%.
A variation in total irradiance with time of
less than 1%, filtered for a given reference
spectrum to have a spectral mismatch error of
less than 1%.
These requirements are essential in obtaining
an accuracy of better than 2%
Testers are classified according to three criteria:
Spectral match
Irradiance inhomogeneity - spatial uniformity
over the illumination area
Temporal Instability - stability over time.
There are three classes within each of these
criteria where 'A' is the top rating an 'C' is the
lowest rating
Uniformity Spectral Fidelity Temporal Stability
Solar Simulator Standards
Estimating Solar Systems Outputs
Actual system outputs may be significantly lower, due to suboptimal system performance, design, installation, shading losses,
Estimating Solar Land Area Requirements
Test Case