
Consider two blocks A and B of masses \( m_1 = 10 \) kg and \( m_2 = 5 \) kg that are placed on a frictionless table. The block A moves with a constant speed \( v = 3 \) m/s towards the block B kept at rest. A spring with spring constant \( k = 3000 \) N/m is attached with the block B as shown in the figure. After the collision, suppose that the blocks A and B, along with the spring in constant compression state, move together, then the compression in the spring is, (Neglect the mass of the spring)
To find the compression in the spring when blocks A and B move together after the collision, we can use the principles of conservation of momentum and energy.
Since there is no external force, the momentum before and after the collision is conserved. Initially, block A is moving and block B is at rest.
Initial momentum:
\(p_{\text{initial}} = m_1 \cdot v = 10 \, \text{kg} \cdot 3 \, \text{m/s} = 30 \, \text{kg m/s}\)
After collision, both blocks move together with velocity \(v_f\):
\(p_{\text{final}} = (m_1 + m_2) \cdot v_f = (10 + 5) \, \text{kg} \cdot v_f = 15 \, \text{kg} \cdot v_f\)
Equating initial and final momentum:
\(30 = 15 \cdot v_f \Rightarrow v_f = 2 \, \text{m/s}\)
The kinetic energy lost in the collision is converted into the potential energy of the compressed spring.
Initial kinetic energy:
\(KE_{\text{initial}} = \frac{1}{2} m_1 v^2 = \frac{1}{2} \cdot 10 \cdot 3^2 = 45 \, \text{J}\)
Final kinetic energy:
\(KE_{\text{final}} = \frac{1}{2} (m_1 + m_2) v_f^2 = \frac{1}{2} \cdot 15 \cdot 2^2 = 30 \, \text{J}\)
Energy stored in the spring (Potential energy):
\(\text{PE}_{\text{spring}} = KE_{\text{initial}} - KE_{\text{final}} = 45 - 30 = 15 \, \text{J}\)
The potential energy stored in the spring is given by \(\frac{1}{2} k x^2\), where \(x\) is the compression.
\(\frac{1}{2} \cdot 3000 \cdot x^2 = 15\)
Solving for \(x\):
\(1500 x^2 = 15 \Rightarrow x^2 = \frac{15}{1500} = 0.01\) \(x = \sqrt{0.01} = 0.1 \, \text{m}\)
Thus, the compression in the spring is 0.1 m.
Two projectile protons \( P_1 \) and \( P_2 \), both with spin up (along the \( +z \)-direction), are scattered from another fixed target proton \( T \) with spin up at rest in the \( xy \)-plane, as shown in the figure. They scatter one at a time. The nuclear interaction potential between both the projectiles and the target proton is \( \hat{\lambda} \vec{L} \cdot \vec{S} \), where \( \vec{L} \) is the orbital angular momentum of the system with respect to the target, \( \vec{S} \) is the spin angular momentum of the system, and \( \lambda \) is a negative constant in appropriate units. Which one of the following is correct?

Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: