Step 1: Use the Self
-Inductance Formula The induced emf is given by: \[ V = L \frac{dI}{dt} \] where:
- \( V = 150 \) V,
- \( \Delta I = 14 - 4 = 10 \) A,
- \( \Delta t = 0.2 \) ms = \( 0.2 \times 10^{-3} \) s.
Step 2: Solve for \( L \) \[ L = \frac{V \cdot \Delta t}{\Delta I} \] \[ L = \frac{150 \times 0.2 \times 10^{-3}}{10} \] \[ L = 3 \times 10^{-3} = 3 \text{ mH} \]
A coil of area A and N turns is rotating with angular velocity \( \omega\) in a uniform magnetic field \(\vec{B}\) about an axis perpendicular to \( \vec{B}\) Magnetic flux \(\varphi \text{ and induced emf } \varepsilon \text{ across it, at an instant when } \vec{B} \text{ is parallel to the plane of the coil, are:}\)

If the roots of $\sqrt{\frac{1 - y}{y}} + \sqrt{\frac{y}{1 - y}} = \frac{5}{2}$ are $\alpha$ and $\beta$ ($\beta > \alpha$) and the equation $(\alpha + \beta)x^4 - 25\alpha \beta x^2 + (\gamma + \beta - \alpha) = 0$ has real roots, then a possible value of $y$ is: