# Detailed Balance

Detailed balance provides a technique to calculate the maximum efficiency of photovoltaic devices. Originally the method was proposed by Shockley and Queisser in 1961 1. An extended version was published in 1984 by Tiedje et al. 2.

1. The mobility is infinite, allowing collection of carriers no matter where they are generated.
2. Complete absorption of all photons above the band gap.

The calculations for detailed balance calculations involve calculating the particle flux for different configurations of the Plank’s equation. The general form of the equation is:

The general approach is to calculate the absorption flux and the flux emitted from the solar cell. The difference between these two  (multiplied by q恒大彩票网址是多少) is the current from the solar cell.

### Absorption flux

The absorption from the sun is given by:

$φsunEG,∞,0,Tsun=2πh3c2∫EG∞E2expEkTsun-1dE$

### Emission flux

The emission from the solar cell depends on the quasi-Fermi level separation (μ) of the solar cell. Under short circuit conditions, m is zero. The emission is calculated by:

$φ2EG,∞,μ,TEarth=2πh3c2∫EG∞E2expE-μkTEarth-1dE$

### Calculation of efficiency for a fixed Eg and black body

The power from the solar cell depends on the band gap and on the quasi-Fermi level separation. For a given band gap, the quasi-Fermi level separation must be varied to find the maximum power point, i.e., where

is at a maximum. This is done by varying m from 0 to close to the open circuit condition (where φ1 = φ2), and find where the power is at a maximum.

The efficiency is then defined as:

### Efficiency as a function of band gap

To find the efficiency as a function of band gap, the above procedure is repeated for each band gap. There is an range of bandgaps for the optimum cell efficiency as shown in the graph below.

Limiting solar cell efficiency as a function of the material bandgap for one-sun illumination. The calculations assume that the only recombination is radiative. In actual devices the efficiencies are lower due to other recombination mechanisms and losses in parasitic resistances.

### AM1.5 Spectrum

To find the efficiency under an AM1.5 spectra (or other measured spectra), φ1 is replaced by the summation of the photon flux for energies above the band gap, and the power from the sun is replaced by the summation of the power in the measured spectra.