A point charge \( q \) is placed at a distance \( d \) above an infinite, grounded conducting plate placed on the \( xy \)-plane at \( z = 0 \).
The electrostatic potential in the \( z > 0 \) region is given by \( \phi = \phi_1 + \phi_2 \), where:
\( \phi_1 = \frac{1}{4 \pi \epsilon_0} \cdot \frac{q}{\sqrt{x^2 + y^2 + (z - d)^2}} \)
\( \phi_2 = - \frac{1}{4 \pi \epsilon_0} \cdot \frac{q}{\sqrt{x^2 + y^2 + (z + d)^2}} \)
Which of the following option(s) is/are correct?
Step 1: The total electrostatic potential is the sum of the potentials due to the charge and the image charge. The image charge method is used to solve for the potential above the conducting plane.
Step 2: The force on the point charge \( q \) due to the image charge is given by Coulomb’s law. However, the question is focused on the potential and its properties, so the force magnitude and energy calculations are secondary and do not match the correct answer.
Step 3: The potential \( \phi_1 \) represents the potential of a charge above a grounded conducting plane, which satisfies Poisson’s equation for \( z > 0 \) since it corresponds to a solution of Laplace’s equation with boundary conditions at the plate.
Step 4: The potential \( \phi_2 \) represents the image charge, ensuring the boundary condition at the grounded conducting plane is satisfied.
A point particle of charge \( Q \) is located at \( P \) along the axis of an electric dipole 1 at a distance \( r \) as shown in the figure. The point \( P \) is also on the equatorial plane of a second electric dipole 2 at a distance \( r \). The dipoles are made of opposite charge \( q \) separated by a distance \( 2a \). For the charge particle at \( P \) not to experience any net force, which of the following correctly describes the situation?
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is: