**Bus Impedance Matrix Method for Analysis of Unsymmetrical Shunt Faults:**

Bus Impedance Matrix Method of fault analysis, given for symmetrical faults can be easily extended to the case of unsymmetrical faults. Consider for example an LG fault on the rth bus of a n-bus system. The connection of sequence networks to simulate the fault is shown in Fig. 11.25.

The positive sequence network has been replaced here by its Thevenin equivalent, i,e. prefault voltage V°_{1-r}, of bus r in series with the passive positive sequence network (all voltage sources short circuited). Since negative and zero sequence prefault voltages are zero, both these are passive networks only.

It may be noted that subscript *a *has been dropped in sequence currents and voltages, while integer subscript is introduced for bus identification. Superscripts *o *and *f *respectively, indicate prefault and postfault values.

For the passive positive sequence network

where

and

As per the sequence network connection, current –I^{f}_{1-r} is injected only at the faulted rth bus of the positive sequence network, we have therefore

Substituting Eq. (11.39) in Eq. (11.35), we can write the positive sequence voltage at the rth bus of the passive positive sequence network as

Thus the passive positive sequence network presents an impedance Z_{1-rr}, to the positive sequence current I^{f}_{1-r}.

For the negative sequence network

The negative sequence network is injected with current I^{f}_{2-r} at the *r*th bus only. Therefore,

The negative sequence voltage at the rth bus is then given by

Thus, the negative sequence network offers an impedance Z_{2-rr} to the negative sequence current I^{f}_{2-r}

Similarly, for the zero sequence network

and

That is, the zero sequence network offers an impedance Z_{0-rr} to the zero sequence current I^{f}_{0-r.}

From the sequence network connection of Fig. 11.25, we can now write

Sequence currents for other types of faults can be similarly computed using Z_{1-rr,}Z_{2-rr,}and Z_{0-rr} in place of Z_{1}, Z_{2} and Z_{0} in Eqs. (11.7), (11.17) and (11.24) with E_{a}=V°_{1-r}

Postfault sequence voltages at any bus can now be computed by superposing on prefault bus voltage, the voltage developed owing to the injection of appropriate sequence current at bus *r.*

For passive positive sequence network, the voltage developed at bus *i *owing to the injection of -I^{f}_{1-r} at bus *r *is

Hence postfault positive sequence voltage at bus *i *is given by

where

Since the prefault negative sequence bus voltages are zero, the postfault negative sequence bus voltages are given by

where

Similarly, the postfault zero sequence bus voltages are given by

where

With postfault sequence voltages known at the buses, sequence currents in lines can be computed as:

For line *uv, *having sequence admittances Y_{1-uv,}Y_{2-uv }and Y_{0-uv}

Knowing sequence voltages and currents, phase voltages and currents can be easily computed by the use of the symmetrical component transformation

It appears at first, as if this method is more laborious than computing fault currents from Thevenin impedances of the sequence networks, as it requires computation of bus impedance matrices of all the three sequence networks. It must, however, be pointed out here that once the bus impedance matrices have been assembled, fault analysis can be conveniently carried out for all the buses, which, in fact, is the aim of a fault study. Moreover, bus impedance matrices can be easily modified to account for changes in power network configuration.