We are given the following information:
When the ball collides with the horizontally mounted spring, its kinetic energy is completely converted into potential energy stored in the spring. The potential energy stored in the spring at maximum compression is given by: \[ E_{\text{spring}} = \frac{1}{2} k x^2 \] Where: - \( k \) is the spring constant, - \( x \) is the maximum compression of the spring (0.5 m). Since all the kinetic energy is transferred to the spring, we equate the kinetic energy to the potential energy stored in the spring: \[ 10^3 \, \text{J} = \frac{1}{2} k (0.5)^2 \] Solving for \( k \): \[ 10^3 = \frac{1}{2} k (0.25) \] \[ 10^3 = 0.125 k \] \[ k = \frac{10^3}{0.125} = 8 \times 10^3 \, \text{N/m} \]
Correct Answer: (C) \( 8 \times 10^3 \, \text{N/m} \)
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Two similar metallic rods of the same length \( l \) and area of cross section \( A \) are joined and maintained at temperatures \( T_1 \) and \( T_2 \) (\( T_1>T_2 \)) at one of their ends as shown in the figure. If their thermal conductivities are \( K \) and \( \frac{K}{2} \) respectively. The temperature at the joining point in the steady state is:

According to equipartition principle, the energy contributed by each translational degree of freedom and rotational degree of freedom at a temperature T are respectively (\( k_B = \text{Boltzmann constant} \)):
Kepler's second law (law of areas) of planetary motion leads to law of conservation of