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Question: A block of mass m moving towards right with a velocity V strikes (head on) another block of mass M w...

A block of mass m moving towards right with a velocity V strikes (head on) another block of mass M which is at rest connected to a spring. The coefficient of restitution for collision between the blocks is e = 0.5. Find the value of M for which the subsequent compression in the spring is maximum. There is no friction.

A

m

B

2m

C

m2\frac{m}{2}

D

m4\frac{m}{4}

Answer

m

Explanation

Solution

1. Collision Phase:

Let the mass of the first block be mm and its initial velocity be VV. Let the mass of the second block be MM and its initial velocity be 00. Let the velocities after collision be vmv_m and vMv_M for mm and MM respectively.

  • Conservation of Momentum: mV+M(0)=mvm+MvMm V + M(0) = m v_m + M v_M mV=mvm+MvMm V = m v_m + M v_M (Eq. 1)

  • Coefficient of Restitution (e = 0.5): e=(vMvm)/(V0)e = (v_M - v_m) / (V - 0) 0.5V=vMvm0.5 V = v_M - v_m vm=vM0.5Vv_m = v_M - 0.5 V (Eq. 2)

Substitute (Eq. 2) into (Eq. 1): mV=m(vM0.5V)+MvMm V = m (v_M - 0.5 V) + M v_M mV=mvM0.5mV+MvMm V = m v_M - 0.5 m V + M v_M 1.5mV=(m+M)vM1.5 m V = (m + M) v_M vM=(1.5mV)/(m+M)v_M = (1.5 m V) / (m + M)

2. Spring Compression Phase:

The spring compression is maximum when the kinetic energy of block MM (which is connected to the spring) is fully converted into elastic potential energy of the spring. This happens when the velocity of MM momentarily becomes zero. We need to maximize xmaxx_{max}, where (1/2)kxmax2=(1/2)MvM2(1/2) k x_{max}^2 = (1/2) M v_M^2. Therefore, we need to maximize MvM2M v_M^2. Substitute the expression for vMv_M: MvM2=M[(1.5mV)/(m+M)]2M v_M^2 = M * [(1.5 m V) / (m + M)]^2 MvM2=(2.25m2V2)[M/(m+M)2]M v_M^2 = (2.25 m^2 V^2) * [M / (m + M)^2] To maximize MvM2M v_M^2, we need to maximize the function f(M)=M/(m+M)2f(M) = M / (m + M)^2.

3. Maximizing f(M)f(M):

To find the maximum, we differentiate f(M)f(M) with respect to MM and set the derivative to zero: f(M)=d/dM[M/(m+M)2]f'(M) = d/dM [M / (m + M)^2] Using the quotient rule: f(M)=[1(m+M)2M2(m+M)]/[(m+M)2]2f'(M) = [1 * (m + M)^2 - M * 2(m + M)] / [(m + M)^2]^2 f(M)=[(m+M)2M]/(m+M)3f'(M) = [(m + M) - 2M] / (m + M)^3 f(M)=(mM)/(m+M)3f'(M) = (m - M) / (m + M)^3 Set f(M)=0f'(M) = 0: (mM)/(m+M)3=0(m - M) / (m + M)^3 = 0 This implies mM=0m - M = 0, so M=mM = m. (We can verify this is a maximum by checking the second derivative, which will be negative at M=mM=m).

4. Check for separation:

If M=mM = m, then vm=V(m0.5m)/(m+m)=V(0.5m)/(2m)=0.25Vv_m = V * (m - 0.5m) / (m + m) = V * (0.5m) / (2m) = 0.25 V. And vM=(1.5mV)/(m+m)=0.75Vv_M = (1.5 m V) / (m + m) = 0.75 V. Since vM>vmv_M > v_m, block mm separates from MM after the collision. Thus, the assumption that only MM's kinetic energy is converted to spring potential energy is valid.

The value of MM for which the subsequent compression in the spring is maximum is mm.