
The particle moves under the influence of an electric field. We will use the work-energy principle to find its speed when it crosses the x-axis.
Step 1: The electric force acting on the particle is given by: \[ F_{\text{electric}} = qE \] where \( E \) is the electric field.
Step 2: The work done by this force in moving the particle a distance \( l \) along the x-axis is: \[ W = F_{\text{electric}} \times l = qEl \] Step 3: The kinetic energy gained by the particle is equal to the work done: \[ K = \frac{1}{2} m v^2 \] So, equating the work and kinetic energy: \[ qEl = \frac{1}{2} m v^2 \] Step 4: Solve for \( v \): \[ v = \sqrt{\frac{2qEI}{m}} \] Final Conclusion: The speed of the particle when it crosses the x-axis is \( \sqrt{\frac{2qEI}{m}} \), which is Option (2).
As shown below, bob A of a pendulum having massless string of length \( R \) is released from \( 60^\circ \) to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take \( g \) as acceleration due to gravity):

The magnitude of heat exchanged by a system for the given cyclic process ABC (as shown in the figure) is (in SI units):

A particle of mass \( m \) and charge \( q \) is fastened to one end \( A \) of a massless string having equilibrium length \( l \), whose other end is fixed at point \( O \). The whole system is placed on a frictionless horizontal plane and is initially at rest. If a uniform electric field is switched on along the direction as shown in the figure, then the speed of the particle when it crosses the x-axis is:
For \( \alpha, \beta, \gamma \in \mathbb{R} \), if \[ \lim_{x \to 0} \frac{x^2 \sin(\alpha x) + (\gamma - 1)e^{x^2}}{\sin(2x - \beta x)} = 3, \] then \( \beta + \gamma - \alpha \) is equal to:

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: