To obtain this characteristic, the generator is operated at a constant speed without any load connected. The field current is gradually increased, and the corresponding terminal voltage is recorded. This data is then plotted, with field current on the x-axis and generated voltage on the y-axis.
The generated EMF (Eg) is directly proportional to the flux (Φ), expressed by the equation Eg = KΦ, where K is a constant. Initially, as the field current increases, the generated voltage increases proportionally due to the increasing magnetic flux. However, once the magnetic field reaches saturation, the flux (Φ) essentially plateaus, regardless of further increases in field current. As a result, the generated voltage also levels off, resulting in a nearly straight-line portion on the saturation curve.
Even when the field current is zero, a small amount of EMF is generated due to residual magnetism in the field poles. This is represented by a non-zero intercept on the voltage axis in the graph of the no-load saturation characteristic.