To solve the problem of finding \( \frac{e_1}{e_2} \), we start with the formula for the EMF induced in a coil: \[ e = -N \frac{d\Phi}{dt} \] where \( N \) is the number of turns, \(\Phi\) is the magnetic flux, and \(t\) is time. The magnetic flux \(\Phi\) is given by \(\Phi = B \cdot A\), where \(B\) is the magnetic field and \(A\) is the area of the coil. For a circular coil, the area \(A\) is \(\pi r^2\). Given the diameter of the coil is 15 mm (0.015 m), the radius \(r\) is 0.0075 m, so: \[ A = \pi (0.0075)^2 \] \[ A = \pi \times 5.625 \times 10^{-5} \] The initial magnetic field \(B\) is 30 mT (0.03 T). Thus, the initial magnetic flux is: \[ \Phi_i = 0.03 \times \pi \times 5.625 \times 10^{-5} \] The coil then goes through two changes:
- Case 1: \(B\) reduces uniformly to 0 in 20 ms (0.02 s). The change in flux \(\Delta\Phi_1\) is: \[ \Delta\Phi_1 = -\Phi_i \]
- Case 2: \(B\) increases uniformly to 0.03 T in 40 ms (0.04 s). The change in flux \(\Delta\Phi_2\) is: \[ \Delta\Phi_2 = \Phi_i \]
Let's calculate the induced EMFs \(e_1\) and \(e_2\):
- \(e_1\) when \(B\) reduces to 0: \[ e_1 = -N \frac{\Delta\Phi_1}{\Delta t_1} = -300 \times \frac{-\Phi_i}{0.02} = 300 \times \frac{\Phi_i}{0.02} \]
- \(e_2\) when \(B\) increases to 0.03 T: \[ e_2 = -N \frac{\Delta\Phi_2}{\Delta t_2} = -300 \times \frac{\Phi_i}{0.04} = 300 \times \frac{-\Phi_i}{0.04} \]
Taking the ratio \(\frac{e_1}{e_2}\): \[ \frac{e_1}{e_2} = \frac{300 \times \Phi_i / 0.02}{300 \times \Phi_i / 0.04} = \frac{1/0.02}{1/0.04} = \frac{0.04}{0.02} = 2 \] The correct value of \(\frac{e_1}{e_2}\) is 2.