
Step 1: Understanding Electromagnetic Induction
From Faraday's Law of electromagnetic induction, the induced emf (\(\mathcal{E}\)) in the loop is given by: \[ \mathcal{E} = B l v \] where: - \( B = 2 \, \text{Wb/m}^2 \) (magnetic field strength), - \( l = 0.1 \, \text{m} \) (side length of the loop), - \( v \) (velocity of the loop, to be determined).
Step 2: Applying Ohm's Law
The induced current \( I \) in the loop is given by: \[ I = \frac{\mathcal{E}}{R} \] where: - \( R = 10 \, \Omega \) (resistance of the loop), - \( I = 1 \) A (steady current in the loop).
Step 3: Solving for \( v \)
Substituting the values: \[ 1 = \frac{(2 \times 0.1 \times v)}{10} \] \[ 1 = \frac{0.2 v}{10} \] \[ v = \frac{10}{0.2} = 2 \text{ m/s} = 2 \text{ cm/s} \]
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: