5 Armature reaction - nptel - Indian Institute of Technology Madras
5 Armature reaction - nptel - Indian Institute of Technology Madras
5 Armature reaction - nptel - Indian Institute of Technology Madras
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Electrical Machines I Pr<strong>of</strong>. Krishna Vasudevan, Pr<strong>of</strong>. G. Sridhara Rao, Pr<strong>of</strong>. P. Sasidhara Rao<br />
<strong>Indian</strong> <strong>Institute</strong> <strong>of</strong> <strong>Technology</strong> <strong>Madras</strong><br />
Volts<br />
0<br />
Open circuit e.m.f<br />
Terminal voltage V<br />
Ohmic Drop IaRa<br />
C<br />
B<br />
A<br />
Load current,Ia<br />
Induced e.m.f<br />
Figure 34: External characteristics <strong>of</strong> a separately excited shunt generator<br />
pensating winding resistance.<br />
As seen from the equation E being function <strong>of</strong> speed and flux per pole it will<br />
also change when these are not held constant. Experimentally the external characteristics<br />
can be determined by conducting a load test. If the external characteristic is obtained by<br />
subtracting the armature drop from the no-load terminal voltage, it is found to depart from<br />
the one obtained from the load test. This departure is due to the armature <strong>reaction</strong> which<br />
causes a saturation at one tip <strong>of</strong> each pole. Modern machines are operated under certain<br />
degree <strong>of</strong> saturation <strong>of</strong> the magnetic path. Hence the reduction in the flux per pole with<br />
load is obvious. The armature drop is an electrical drop and can be found out even when<br />
the machine is stationary and the field poles are unexcited. Thus there is some slight droop<br />
in the external characteristics, which is good for parallel operation <strong>of</strong> the generators.<br />
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