**Line to Line Fault (LL):**

Figure 11.7 shows a Line to Line Fault at F in a power system on phases b and c through a fault impedance Z* ^{f}*. The phases can always be relabelled, such that the fault is on phases b and c.

The currents and voltages at the fault can be expressed as

The symmetrical components of the fault currents are

from which we get

The symmetrical components of voltages at F under fault are

Writing the first two equations, we have

From which we get

Now

Substituting I_{b} from Eq. (11.15) in Eq. (11.14), we get

Equations (11.11) and (11.16) suggest parallel connection of positive and negative sequence networks through a series impedance Z* ^{f}* as shown in Figs. 11.8a and b. Since I

_{a0}= 0 as per Eq. (11.12), the zero sequence network is unconnected.

In terms of the Thvenin equivalents, we get from Fig. 11.8b

From Eq. (11.15), we get

Knowing I_{a1,}we can calculate V_{a1} and V_{a2} from which voltages at the fault can be found.

If the Line to Line Fault occurs from loaded conditions, the positive sequence network can be modified