In an AC circuit containing an inductor, the relationship between voltage and current is characterized by their phase difference. For an ideal inductor, the voltage (\( V \)) across it can be represented in terms of the current (\( I \)), using the inductive reactance and the phase shift caused by the inductance. This phase difference is given by:
\( V(t) = L \frac{dI(t)}{dt} \)
The sinusoidal expressions for voltage and current in an AC circuit are:
\( I(t) = I_0 \sin(\omega t + \phi_I) \)
\( V(t) = V_0 \sin(\omega t + \phi_V) \)
For an inductor, voltage leads the current by \(\frac{\pi}{2}\) radians (or 90 degrees), meaning the voltage reaches its maximum value one-quarter of a cycle before the current reaches its maximum. Therefore, the phase difference (\( \phi_V - \phi_I \)) is:
\( \phi_V - \phi_I = \frac{\pi}{2} \)
Therefore, in an inductor, voltage leads the current by \( \frac{\pi}{2} \).
In an inductive circuit, the voltage \( V \) and the current \( I \) are related through the inductance \( L \) and the frequency of the alternating current. The voltage across an inductor is given by: \[ V_L = L \frac{dI}{dt} \]
For an AC circuit, the current and voltage can be expressed as: \[ I = I_0 \sin(\omega t) \] \[ V_L = L I_0 \omega \cos(\omega t) \] Since \( \cos(\omega t) = \sin\left(\omega t + \frac{\pi}{2}\right) \), the voltage leads the current by \( \frac{\pi}{2} \) radians in an inductor.
Thus, the correct answer is: \[ \text{(B) } \text{voltage leads the current by } \frac{\pi}{2} \]
Show that the energy required to build up the current \( I \) in a coil of inductance \( L \) is \( \frac{1}{2} L I^2 \).
A circular coil of diameter 15 mm having 300 turns is placed in a magnetic field of 30 mT such that the plane of the coil is perpendicular to the direction of the magnetic field. The magnetic field is reduced uniformly to zero in 20 ms and again increased uniformly to 30 mT in 40 ms. If the EMFs induced in the two time intervals are \( e_1 \) and \( e_2 \) respectively, then the value of \( e_1 / e_2 \) is:
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: