We are given a solenoid of area \(A\), length \(\ell\), filled with a material of relative permeability \(\mu_r = 2\). We need to find the magnetic energy stored in it in terms of the magnetic field \(B\).
The magnetic energy density in a medium is given by:
\[ u = \frac{B^2}{2\mu}. \]
For a solenoid filled with material of relative permeability \(\mu_r\),
\[ \mu = \mu_r \mu_0. \]
The total magnetic energy stored in the solenoid of volume \(V = A\ell\) is:
\[ U = u \times V = \frac{B^2}{2\mu} \times A\ell = \frac{B^2 A \ell}{2\mu_r \mu_0}. \]
Step 1: Substitute \(\mu_r = 2\):
\[ U = \frac{B^2 A \ell}{2(2)\mu_0} = \frac{B^2 A \ell}{4\mu_0}. \]
Step 2: The question likely asks for the energy per unit length or the general dependence. Since \(\ell\) is constant, we can express the answer (per unit length) as:
\[ \frac{U}{\ell} = \frac{B^2 A}{4\mu_0}. \]
The magnetic energy stored in the solenoid is:
\[ \boxed{\frac{B^2 A}{4\mu_0}}. \]
Correct Option: \( \dfrac{B^2 A}{4\mu_0} \)
A proton is moving undeflected in a region of crossed electric and magnetic fields at a constant speed of \( 2 \times 10^5 \, \text{m/s} \). When the electric field is switched off, the proton moves along a circular path of radius 2 cm. The magnitude of electric field is \( x \times 10^4 \, \text{N/C} \). The value of \( x \) is \(\_\_\_\_\_\). (Take the mass of the proton as \( 1.6 \times 10^{-27} \, \text{kg} \)).
Due to presence of an em-wave whose electric component is given by \( E = 100 \sin(\omega t - kx) \, NC^{-1} \), a cylinder of length 200 cm holds certain amount of em-energy inside it. If another cylinder of same length but half diameter than previous one holds same amount of em-energy, the magnitude of the electric field of the corresponding em-wave should be modified as:

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by:
The Lagrangian of a particle of mass \( m \) and charge \( q \) moving in a uniform magnetic field of magnitude \( 2B \) that points in the \( z \)-direction, is given by: \[ L = \frac{m}{2} v^2 + qB(x v_y - y v_x) \] where \( v_x, v_y, v_z \) are the components of its velocity \( v \). If \( p_x, p_y, p_z \) denote the conjugate momenta in the \( x, y, z \)-directions and \( H \) is the Hamiltonian, which of the following option(s) is/are correct?

