We know the emf induced in an inductor is given by: \[ \mathcal{E} = L \frac{dI}{dt} \] where \( L \) is the inductance of the inductor, \( I \) is the current, and \( \frac{dI}{dt} \) is the rate of change of current. The current increases uniformly from 0 to 2 A in 40 seconds, so the rate of change of current is: \[ \frac{dI}{dt} = \frac{2 \, \text{A}}{40 \, \text{s}} = 0.05 \, \text{A/s} \] Substituting this into the equation for emf: \[ \mathcal{E} = L \times 0.05 \] Given that the induced emf is 5 mV or \( 5 \times 10^{-3} \, \text{V} \), we can solve for \( L \): \[ 5 \times 10^{-3} = L \times 0.05 \] \[ L = \frac{5 \times 10^{-3}}{0.05} = 10^{-1} \, \text{H} = 0.1 \, \text{H} \] Now, the flux \( \Phi \) linked with the inductor at any time \( t \) is given by: \[ \Phi = L \times I \] At \( t = 10 \) s, the current is: \[ I = \frac{2 \, \text{A}}{40 \, \text{s}} \times 10 \, \text{s} = 0.5 \, \text{A} \] Thus, the flux at \( t = 10 \, \text{s} \) is: \[ \Phi = 0.1 \times 0.5 = 0.05 \, \text{Wb} \]
Predict the direction of induced current in the situations described by the following Figs. 6.18(a) to (f ).
A long solenoid with 15 turns per cm has a small loop of area 2.0 cm2 placed inside the solenoid normal to its axis. If the current carried by the solenoid changes steadily from 2.0 A to 4.0 A in 0.1 s, what is the induced emf in the loop while the current is changing?
A rectangular wire loop of sides 8 cm and 2 cm with a small cut is moving out of a region of uniform magnetic field of magnitude 0.3 T directed normal to the loop. What is the emf developed across the cut if the velocity of the loop is 1 cm s-1 in a direction normal to the (a) longer side, (b) shorter side of the loop? For how long does the induced voltage last in each case?
A 1.0 m long metallic rod is rotated with an angular frequency of 400 rad s-1 about an axis normal to the rod passing through its one end. The other end of the rod is in contact with a circular metallic ring. A constant and uniform magnetic field of 0.5 T parallel to the axis exists everywhere. Calculate the emf developed between the centre and the ring.
A horizontal straight wire 10 m long extending from east to west is falling with a speed of 5.0 m s-1, at right angles to the horizontal component of the earth’s magnetic field, 0.30 \(\times\)10-4 Wb m-2 .