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Dr. Mrinmoy Majumder
Topic of Renewable Energy Course of MTech in Hydroinformatics Engg.
at National Institute of Technology Agartala
Enrol for my course on MCDM :
More such tutorial in http://www.baipatra.ws
๏‚ง ๐ธ๐‘“ = ๐ธ๐‘ โˆ’ ๐‘˜๐‘‡ ln
๐‘ ๐‘
๐‘ ๐‘‘
๏‚ง For n type material
๏‚ง ๐‘๐‘‘ concentration of donor atom
๏‚ง ๐ธ๐‘“ = ๐ธ ๐‘ฃ โˆ’ ๐‘˜๐‘‡ ln
๐‘ ๐‘ฃ
๐‘ ๐‘Ž
๏‚ง For n type material
๏‚ง ๐‘๐‘‘ concentration of acceptor atom
๏‚ง When p and n type material is connected with each other then
๏‚ง Electron from the n type will flow to p type material and thus become positively
charged
๏‚ง Hole from p type will be compensated by the electron from n type material thus
become negatively charged
๏‚ง When there is no more free electrons and holes flow of current stops and the
potential at which this equilibrium is reached is known as Contact Potential
๏‚ง This condition is known as Unbiased Condition
๏‚งIf an external voltage ๐‘ฃ ๐‘“ is applied on P-N junction then
the contact potential V is reduced by V- ๐‘ฃ ๐‘“
๏‚งThe junction is said to be in Forward bias mode
๏‚งCurrent flow across the junction increases sharply
๏‚งIf a large reverse voltage ๐‘ฃ ๐‘ is applied on P-N junction
then the contact potential V is increased by V+ ๐‘ฃ ๐‘
๏‚งThe junction is said to be in Reverse bias mode
๏‚งCurrent flow is only due to minority carriers
๏‚งReverse bias condition increases the in-built potential
๏‚ง ๐ผ๐‘— = ๐ผ0 exp
โ…‡๐‘ฃ
๐‘˜๐‘‡
โˆ’ 1
๏‚ง ๐ผ0= saturation current or dark current under reverse bias and
๏‚ง e = electronic charge
๏‚ง When a p-n junction is illuminated by sunlight then new electronic-hole pairs are
generated and current I is obtained which is equal to :
๏‚ง ๐ผ = ๐ผ๐ฟ โˆ’ ๐ผ๐‘— which can be written as
๏‚ง ๐ผ = ๐ผ๐ฟ โˆ’ ๐ผ0 exp
โ…‡๐‘ฃ
๐‘˜๐‘‡
โˆ’ 1
๏‚ง where IL is solar light generated current
๏‚ง This phenomenon is known as Photovoltaic Effect
๏‚ง Figure besides depict the current-
voltage characteristic of a solar cell at
given illumination and temperature.
๏‚ง Voc,Isc are the open circuit and short
circuit voltage and current,
respectively.
๏‚ง Vm,Im are the voltage and current at
maximum power
๏‚ง With rise in temperature leakage
increases in cell
๏‚ง Cell quality is maximum when the
Fill Factor value approaches
๏‚ง ๐น๐น =
๐ผ ๐‘š ๐‘ฃ ๐‘š
๐ผ๐‘ ๐‘ ๐‘ฃ ๐‘œ๐‘
๐น๐น =
๐ผ ๐‘š ๐‘ฃ ๐‘š
๐ผ๐‘  ๐ด ๐‘
where Is is the incident solar flux
Ac is the cellโ€™s area
Dr. Majumder's Course on Renewable Energy

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Dr. Majumder's Course on Renewable Energy

  • 1. Dr. Mrinmoy Majumder Topic of Renewable Energy Course of MTech in Hydroinformatics Engg. at National Institute of Technology Agartala Enrol for my course on MCDM : More such tutorial in http://www.baipatra.ws
  • 2. ๏‚ง ๐ธ๐‘“ = ๐ธ๐‘ โˆ’ ๐‘˜๐‘‡ ln ๐‘ ๐‘ ๐‘ ๐‘‘ ๏‚ง For n type material ๏‚ง ๐‘๐‘‘ concentration of donor atom ๏‚ง ๐ธ๐‘“ = ๐ธ ๐‘ฃ โˆ’ ๐‘˜๐‘‡ ln ๐‘ ๐‘ฃ ๐‘ ๐‘Ž ๏‚ง For n type material ๏‚ง ๐‘๐‘‘ concentration of acceptor atom
  • 3. ๏‚ง When p and n type material is connected with each other then ๏‚ง Electron from the n type will flow to p type material and thus become positively charged ๏‚ง Hole from p type will be compensated by the electron from n type material thus become negatively charged ๏‚ง When there is no more free electrons and holes flow of current stops and the potential at which this equilibrium is reached is known as Contact Potential ๏‚ง This condition is known as Unbiased Condition
  • 4. ๏‚งIf an external voltage ๐‘ฃ ๐‘“ is applied on P-N junction then the contact potential V is reduced by V- ๐‘ฃ ๐‘“ ๏‚งThe junction is said to be in Forward bias mode ๏‚งCurrent flow across the junction increases sharply
  • 5. ๏‚งIf a large reverse voltage ๐‘ฃ ๐‘ is applied on P-N junction then the contact potential V is increased by V+ ๐‘ฃ ๐‘ ๏‚งThe junction is said to be in Reverse bias mode ๏‚งCurrent flow is only due to minority carriers ๏‚งReverse bias condition increases the in-built potential
  • 6. ๏‚ง ๐ผ๐‘— = ๐ผ0 exp โ…‡๐‘ฃ ๐‘˜๐‘‡ โˆ’ 1 ๏‚ง ๐ผ0= saturation current or dark current under reverse bias and ๏‚ง e = electronic charge
  • 7. ๏‚ง When a p-n junction is illuminated by sunlight then new electronic-hole pairs are generated and current I is obtained which is equal to : ๏‚ง ๐ผ = ๐ผ๐ฟ โˆ’ ๐ผ๐‘— which can be written as ๏‚ง ๐ผ = ๐ผ๐ฟ โˆ’ ๐ผ0 exp โ…‡๐‘ฃ ๐‘˜๐‘‡ โˆ’ 1 ๏‚ง where IL is solar light generated current ๏‚ง This phenomenon is known as Photovoltaic Effect
  • 8. ๏‚ง Figure besides depict the current- voltage characteristic of a solar cell at given illumination and temperature. ๏‚ง Voc,Isc are the open circuit and short circuit voltage and current, respectively. ๏‚ง Vm,Im are the voltage and current at maximum power ๏‚ง With rise in temperature leakage increases in cell ๏‚ง Cell quality is maximum when the Fill Factor value approaches
  • 9. ๏‚ง ๐น๐น = ๐ผ ๐‘š ๐‘ฃ ๐‘š ๐ผ๐‘ ๐‘ ๐‘ฃ ๐‘œ๐‘ ๐น๐น = ๐ผ ๐‘š ๐‘ฃ ๐‘š ๐ผ๐‘  ๐ด ๐‘ where Is is the incident solar flux Ac is the cellโ€™s area