The problem involves finding the average power consumed in an AC circuit given the instantaneous values of current and voltage. The expressions provided are:
Current: \( i = \frac{1}{\sqrt{2}} \sin(100\pi t) \text{ amp} \)
Voltage: \( e = \frac{1}{\sqrt{2}} \sin(100\pi t + \pi/3) \text{ volt} \)
The average power \( P \) consumed in an AC circuit is given by:
\( P = I_{\text{rms}} V_{\text{rms}} \cos\phi \)
Where:
From the expressions:
The phase difference \( \phi \) is \( \pi/3 \).
Substituting these values into the average power formula:
\( P = \left(\frac{1}{\sqrt{2}}\right) \left(\frac{1}{\sqrt{2}}\right) \cos\left(\frac{\pi}{3}\right) \)
We know that \( \cos(\pi/3) = \frac{1}{2} \). Thus:
\( P = \left(\frac{1}{\sqrt{2}}\right)^2 \times \frac{1}{2} \)
\( P = \frac{1}{2} \times \frac{1}{2} = \frac{1}{4} \times \frac{1}{2} = \frac{1}{8} \)
Therefore, the average power consumed in the circuit is \( \frac{1}{8} \) watts.
Draw the plots showing the variation of magnetic flux φ linked with the loop with time t and variation of induced emf E with time t. Mark the relevant values of E, φ and t on the graphs.
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: