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The Impact of Shunt Resistance on Solar Cell Performance
Shunt resistance (RSH) plays a significant role in the efficiency of solar cells. It is often caused by manufacturing defects and can lead to power losses in solar cells. Low shunt resistance provides an alternative current path for the light-generated current, reducing the current flow through the solar cell junction and lowering the voltage output. This effect is more pronounced at lower light levels, where the loss of current to the shunt has a greater impact.
Equation for Solar Cell with Shunt Resistance
The behavior of a solar cell with shunt resistance can be described by the equation:
I = IL – I0 exp(qV/nkT) – VRSH
Where I is the cell output current, IL is the light-generated current, V is the voltage across the cell terminals, T is the temperature, q and k are constants, n is the ideality factor, and RSH is the shunt resistance.
Impact on Fill Factor
The shunt resistance also affects the fill factor of the solar cell. The maximum power output can be approximated as the power without shunt resistance, minus the power lost in the shunt resistance. This leads to the equation:
PMP‘ = PMP(1 – RSH/RS)
Where PMP is the maximum power output, RS is the series resistance, and RSH is the shunt resistance.
Normalized Shunt Resistance
A normalized shunt resistance (rSH) can be defined as RSH/RS. Assuming that the open-circuit voltage and short-circuit current are not affected by the shunt resistance, the impact of shunt resistance on the fill factor can be determined as:
FF’ = FF(1 – 1/rSH)
Where FF is the fill factor unaffected by shunt resistance, and FF’ is the fill factor affected by shunt resistance.
Empirical Equation for Fill Factor
An empirical equation that relates the fill factor unaffected by shunt resistance (FF0) to the fill factor affected by shunt resistance (FFSH) is:
FFSH = FF0(1 – 1/rSH)
This equation is valid for rSH > 0.4.
Source: Siliconvlsi
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