Consider two long coaxial solenoids \( S_1 \) and \( S_2 \), each of length \( l \) (\( l \gg r_2 \)) and radius \( r_1 \) and \( r_2 \) (\( r_2 > r_1 \)), respectively. The number of turns per unit length are \( n_1 \) and \( n_2 \), respectively. We will derive the expression for the mutual inductance \( M_{12} \) of solenoid \( S_1 \) with respect to solenoid \( S_2 \) and show that \( M_{21} = M_{12} \).
The magnetic field inside a long solenoid is given by:
\[ B_1 = \mu_0 n_1 I_1 \]
where: - \( \mu_0 \) is the permeability of free space, - \( n_1 \) is the number of turns per unit length of solenoid \( S_1 \), - \( I_1 \) is the current flowing through solenoid \( S_1 \). This magnetic field is directed along the axis of the solenoid and is uniform inside the solenoid.
The magnetic flux \( \Phi_2 \) through the area of one turn of solenoid \( S_2 \) is given by:
\[ \Phi_2 = B_1 A_2 \]
where: - \( A_2 = \pi r_2^2 \) is the cross-sectional area of solenoid \( S_2 \), - \( B_1 = \mu_0 n_1 I_1 \) is the magnetic field produced by solenoid \( S_1 \). Therefore, the total flux through \( N_2 \) turns of solenoid \( S_2 \) is given by:
\[ \Phi_2 = \mu_0 n_1 I_1 \pi r_2^2 l \]
where \( l \) is the length of solenoid \( S_2 \).
The induced EMF \( \mathcal{E}_2 \) in solenoid \( S_2 \) due to the time-varying magnetic flux is given by Faraday’s law:
\[ \mathcal{E}_2 = - \frac{d\Phi_2}{dt} = - \frac{d}{dt} \left( \mu_0 n_1 I_1 \pi r_2^2 l \right) \]
Since \( I_1 \) is the current in solenoid \( S_1 \), we can write:
\[ \mathcal{E}_2 = - M_{12} \frac{dI_1}{dt} \]
where \( M_{12} \) is the mutual inductance between solenoid \( S_1 \) and solenoid \( S_2 \). Thus, comparing both expressions for the induced EMF, we get:
\[ M_{12} = \mu_0 n_1 n_2 \pi r_1^2 l \]
This is the expression for the mutual inductance between the two solenoids.
From the above derivation, it is evident that the mutual inductance is symmetric. That is, the mutual inductance \( M_{12} \) of solenoid \( S_1 \) with respect to solenoid \( S_2 \) is equal to the mutual inductance \( M_{21} \) of solenoid \( S_2 \) with respect to solenoid \( S_1 \). Therefore, we can write:
\[ M_{21} = M_{12} \]
The mutual inductance between two coaxial solenoids is given by:
\[ M_{12} = \mu_0 n_1 n_2 \pi r_1^2 l \] and it is symmetric, i.e., \( M_{21} = M_{12} \).
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 .