Based on the equation:
J = JPH - J0[ exp(qV/kT) - 1 ]
When J = 0:
Voc = (kT/q) ln (JPH/J0 + 1)
When V = 0:
Jsc = JPH
This shows that Voc is dependent on JPH, T and J0. When more light is shone on the solar cell, meaning there's higher irradiance, the increase in JPH will increase Voc as well. When there's higher temperature T, J0 will be strongly affected and there will be more leakage current. This is not shown in the equation, and will overwhelm the increase in T in the equation and cause Voc to reduce.
The diagram above shows the power density curve, where a negative power density shows that the solar cell is generating power. A positive power density shows that the solar cell is consuming/dissipating power, and the solar cell heats up. There is a point of maximum power density generation called the maximum power point, where the power density is Pmax, with corresponding voltage Vmp and current density Jmp. The points where power density is zero is at Voc and Jsc.
Hence: Pmax = Vmp Jmp
And the shaded area in the diagram represents the power density generated.
Another external parameter called the fill factor FF is defined as follows:
FF = JmpVmp / JscVoc
Lastly, the conversion efficiency η of a solar cell is defined as follows:
η = Pmax/Pin = Jsc Voc FF / Pin
where Pin = 1000W/m2 = 100mW/cm2, the irradiance (power density of light) under STC (AM1.5, 25°C).
Hence, efficiency is expressed all in external parameters.
Reference:
3.2.1 External Parameters of an Ideal Solar Cell, Delft University of Technology, https://www.youtube.com/watch?v=ZyedIjJ6frI
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