To conduct a Load Flow Analysis, the components in a power system need to be modelled. The modelling is done by developing equivalent circuits of the components, such as the generator, transmission lines and line capacitances.

The Generator equivalent circuit is shown below.

The Thevenin equivalent circuit is as shown below.

This consists of a voltage source and a resistance and an inductance in series with the load.

E = V + IZ

where

Z is the steady stage impedance

V is the voltage and

I is the current

**The Norton equivalent circuit**

The Norton equivalent circuit consists of a power source and an admittance in parallel.

I

_{Norton}= V/Z

I

_{Norton}= YV

**Load**

The load is modelled as a resistance and inductance in a series circuit that is earth

**Transmission lines**

Transmission lines are modelled as

**Short transmission lines (less than 80 km)**

Short lines that are less than 80 kms long are modelled as a resistance and reactance in series with the load. The line capacitances are neglected.

**Medium (80 to 250 km)**

**Medium lines are modelled as a resistance and reactance in series. The admittance is in parallel in two sections.**

**Long lines ( 250 km and above)**

**Long lines are also modelled as a resistance and reactance in series. The admittance is in parallel in two sections.**