The current flowing through a pure inductor in an AC circuit lags the applied voltage by:
Quarter of a cycle
In an AC circuit containing an ideal (pure) inductor, the relationship between the voltage across the inductor and the current flowing through it is crucial.
The phase difference ($\phi$) between voltage and current in a pure inductive circuit is:
A full cycle in an AC waveform corresponds to $2\pi$ radians or $360^\circ$. To express the phase lag as a fraction of a cycle, we calculate:
Fraction = $\frac{\text{Phase Lag}}{\text{Full Cycle}} = \frac{\pi/2}{2\pi} = \frac{1}{4}$
Alternatively, using degrees:
Fraction = $\frac{90^\circ}{360^\circ} = \frac{1}{4}$
Therefore, the current flowing through a pure inductor in an AC circuit lags the applied voltage by a quarter of a cycle.
The total opposition offered to the flow of current in AC circuit is called-
A quantity whose magnitude has a definite repeating time cycle is called a-
The current drawn by a tungsten filament lamp is measured by an ammeter. The ammeter reading under steady state condition will be ______ the ammeter reading when the supply is switched on.
What is the average value of a sine wave Vm sinωt over a full cycle?
The peak factor of a sinusoidal waveform is: