The short-circuit current and the open-circuit voltage are the maximum current and voltage respectively from a solar cell. However, at both of these operating points, the power from the solar cell is zero. The "fill factor", more commonly known by its abbreviation "FF", is a parameter which, in conjunction with V_{oc} and I_{sc}, determines the maximum power from a solar cell. The FF is defined as the ratio of the maximum power from the solar cell to the product of V_{oc} and I_{sc} so that:

$$FF= \frac{P_{MP}}{V_{OC}\times I_{SC}}$$

## Fill Factor

$FF=\frac{{V}_{MP}{I}_{MP}}{{V}_{OC}{I}_{SC}}$

Graphically, the FF is a measure of the "squareness" of the solar cell and is also the area of the largest rectangle which will fit in the IV curve. The FF is illustrated below.

As FF is a measure of the "squareness" of the IV curve, a solar cell with a higher voltage has a larger possible FF since the "rounded" portion of the IV curve takes up less area. The maximum theoretical FF from a solar cell can be determined by differentiating the power from a solar cell with respect to voltage and finding where this is equal to zero. Hence:

$$\frac{d(I V)}{d V}=0$$

giving:

$$V_{MP} = V_{OC} - \frac{nkT}{q}ln(\frac{q V_{MP}}{nkT}+1)$$

The equation above requires Lambert functions to solve (see below) but a simpler approach is to use iteration to calculate V_{MP}. The equation above only relates V_{oc} to V_{MP} and extra equations are needed to find I_{MP} and FF. A more commonly used expression for the FF can be determined empirically as:1

## Fill Factor - Empirical

$FF=\frac{{v}_{oc}-\mathrm{ln}\left({v}_{oc}+0.72\right)}{{v}_{oc}+1}$

where v_{oc} is defined as a "normalized V_{oc}":

## Voc normalized

${v}_{oc}=\frac{q}{nkT}{V}_{oc}$

The above equations show that a higher voltage will have a higher possible FF. However, large variations in open-circuit voltage within a given material system are relatively uncommon. For example, at one sun, the difference between the maximum open-circuit voltage measured for a silicon laboratory device and a typical commercial solar cell is about 120 mV, giving maximum FF's respectively of 0.85 and 0.83. However, the variation in maximum FF can be significant for solar cells made from different materials. For example, a GaAs solar cell may have a FF approaching 0.89.

The above equation also demonstrates the importance of the ideality factor, also known as the "n-factor" of a solar cell. The ideality factor is a measure of the junction quality and the type of recombination in a solar cell. For the simple recombination mechanisms discussed in Types of Recombination, the n-factor has a value of 1. However, some recombination mechanisms, particularly if they are large, may introduce recombination mechanisms of 2. A high n-value not only degrades the FF, but since it will also usually signal high recombination, it gives low open-circuit voltages.

A key limitation in the equations described above is that they represent a maximum possible FF, although in practice the FF will be lower due to the presence of parasitic resistive losses, which are discussed in Effects of Parasitic Resistances. Therefore, the FF is most commonly determined from measurement of the IV curve and is defined as the maximum power divided by the product of I_{sc}*V_{oc}, i.e.:

## Fill Factor

$FF=\frac{{V}_{MP}{I}_{MP}}{{V}_{OC}{I}_{SC}}$

### Exact determination of V_{MP}

The equation for a solar cell is:

$$I = I_L-I_0\left[\exp\left(\frac{V}{nV_t}\right)-1\right]$$

\(Power = V \times I\) and in addition the -1 term has no effect at V_{MP}

$$P = V I_L- V I_0\exp\left(\frac{V}{nV_t}\right)$$

V_{MP} is when the derivative of the power with respect to V is zero:

$$0 = I_L- I_0\exp\left(\frac{V_{MP}}{nV_t}\right)\left(1+\frac{V_{MP}}{nV_t}\right)$$

V> > V_{t} and rearranging gives:

$$\frac{I_L}{I_0} =\exp\left(\frac{V_{MP}}{nV_t}\right)\left(\frac{V_{MP}}{nV_t}\right)$$

The Lambert W function provides the solution to a class of exponential functions.

$$Y = Xe^x \Leftrightarrow X = W (Y)$$

so we get:

$$\frac{V_{MP}}{nV_t} =W\left(\frac{I_L}{I_0}\right)$$

$$V_{MP} = nV_t W\left(\frac{I_L}{I_0}\right)$$

using the expression for V_{OC} we can also write:

$$V_{MP} = nV_t W\left(\exp\left(\frac{V_{OC}}{nV_t}\right)\right)$$

Since the expression inside the W() is always real and positive we only ever need the principle branch of the Lambert W function, W_{0}. The Lambert W function is a transcendental function much like logarithm function. While it is not available on most calculators, it is available on advanced mathematical packages such as Matlab or Python. With further analysis the Lambert W function can also be used for other solar cell terms and in the presence of parasitic resistances 2.

- 1. , “Solar cell fill factors: General graph and empirical expressions”, Solid-State Electronics, vol. 24, pp. 788 - 789, 1981.
- 2. , “Exact analytical solutions of the parameters of real solar cells using Lambert W-function”, Solar Energy Materials and Solar Cells, vol. 81, no. 2, pp. 269 - 277, 2004.