A dynamometer-type wattmeter operates based on the electrodynamic principle. It utilizes the interaction between the magnetic fields produced by fixed current coils (current coils) and a moving coil.
In a dynamometer wattmeter:
The torque produced is proportional to the product of the currents in the two coils and the sine of the angle between them. For a resistive load, this torque is proportional to the instantaneous power consumed by the load.
For AC circuits, the instantaneous power ($p(t)$) fluctuates. The deflection of the wattmeter's pointer indicates the average value of this instantaneous power over a complete cycle. This average value corresponds to the true power or active power consumed by the load.
Mathematically, the average power ($P_{avg}$) measured is given by:
$P_{avg} = V_{rms} \times I_{rms} \times \cos(\phi)$
where $V_{rms}$ and $I_{rms}$ are the RMS voltage and current, and $\cos(\phi)$ is the power factor.
Therefore, the dynamometer-type wattmeter responds to the average value of the active power.
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