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Question: Two blocks, of masses $M$ and $2M$, are connected to a light spring of spring constant $K$ that has ...

Two blocks, of masses MM and 2M2M, are connected to a light spring of spring constant KK that has one end fixed, as shown in figure. The horizontal surface and the pulley are frictionless. The blocks are released from rest when the spring is non deformed. The string is light.

(I) Maximum extension in the spring is 4MgK\frac{4Mg}{K}.

(II) Maximum kinetic energy of the system is 2M2g2K\frac{2M^2g^2}{K}.

(III) Maximum extension in the spring is 2MgK\frac{2Mg}{K}.

(IV) Maximum kinetic energy of the system is 4M2g2K\frac{4M^2g^2}{K}.

Then which of the following option is correct?

A

I and IV

B

I and II

C

III and IV

D

None of these

Answer

(B)

Explanation

Solution

The problem involves a system of two blocks, a spring, and a pulley. We need to find the maximum extension of the spring and the maximum kinetic energy of the system. The system is released from rest with the spring non-deformed. Since the surfaces and pulley are frictionless, mechanical energy is conserved.

Let M1=MM_1 = M be the mass of the block on the horizontal surface, and M2=2MM_2 = 2M be the mass of the hanging block. Let KK be the spring constant.

1. Calculate the equilibrium extension (xeqx_{eq}):

The equilibrium position is where the net force on the system is zero. Let xx be the extension of the spring. The force exerted by the spring on M1M_1 is KxKx to the left. The tension in the string pulls M1M_1 to the right and M2M_2 upwards. For M1M_1 (horizontal motion): TKx=0    T=KxT - Kx = 0 \implies T = Kx. For M2M_2 (vertical motion): 2MgT=0    T=2Mg2Mg - T = 0 \implies T = 2Mg. Equating the tensions: Kxeq=2MgKx_{eq} = 2Mg xeq=2MgKx_{eq} = \frac{2Mg}{K}

This is the extension at which the system would remain at rest if placed there.

2. Calculate the maximum extension in the spring (xmaxx_{max}):

The system starts from rest at x=0x=0 (relaxed spring). It moves downwards, accelerating until it reaches the equilibrium position, and then continues to move until it momentarily comes to rest at the maximum extension. We can use the conservation of mechanical energy. Let the initial position of M2M_2 be the reference for gravitational potential energy (Ug=0U_g = 0). Initial state (released from rest): KEi=0KE_i = 0 Us,i=0U_{s,i} = 0 (spring relaxed) Ug,i=0U_{g,i} = 0 Total initial energy Ei=0E_i = 0.

Final state (maximum extension xmaxx_{max}): At maximum extension, the system momentarily comes to rest, so KEf=0KE_f = 0. The spring is extended by xmaxx_{max}, so Us,f=12Kxmax2U_{s,f} = \frac{1}{2}Kx_{max}^2. The block M2M_2 has descended by xmaxx_{max}, so Ug,f=2MgxmaxU_{g,f} = -2Mgx_{max}. Total final energy Ef=0+12Kxmax22MgxmaxE_f = 0 + \frac{1}{2}Kx_{max}^2 - 2Mgx_{max}.

By conservation of mechanical energy, Ei=EfE_i = E_f: 0=12Kxmax22Mgxmax0 = \frac{1}{2}Kx_{max}^2 - 2Mgx_{max} 12Kxmax2=2Mgxmax\frac{1}{2}Kx_{max}^2 = 2Mgx_{max} Since xmax0x_{max} \neq 0, we can divide by xmaxx_{max}: 12Kxmax=2Mg\frac{1}{2}Kx_{max} = 2Mg xmax=4MgKx_{max} = \frac{4Mg}{K}

This matches statement (I).

3. Calculate the maximum kinetic energy of the system (KEmaxKE_{max}):

The maximum kinetic energy occurs at the equilibrium position, where x=xeq=2MgKx = x_{eq} = \frac{2Mg}{K}. Let vmaxv_{max} be the speed of the blocks at this point. Using conservation of mechanical energy between the initial state and the equilibrium state: Initial energy Ei=0E_i = 0. Energy at equilibrium EeqE_{eq}: KEeq=12M1vmax2+12M2vmax2=12(M+2M)vmax2=12(3M)vmax2KE_{eq} = \frac{1}{2}M_1v_{max}^2 + \frac{1}{2}M_2v_{max}^2 = \frac{1}{2}(M + 2M)v_{max}^2 = \frac{1}{2}(3M)v_{max}^2. Us,eq=12Kxeq2U_{s,eq} = \frac{1}{2}Kx_{eq}^2. Ug,eq=2MgxeqU_{g,eq} = -2Mgx_{eq}. So, Eeq=KEmax+12Kxeq22MgxeqE_{eq} = KE_{max} + \frac{1}{2}Kx_{eq}^2 - 2Mgx_{eq}.

By conservation of mechanical energy, Ei=EeqE_i = E_{eq}: 0=KEmax+12Kxeq22Mgxeq0 = KE_{max} + \frac{1}{2}Kx_{eq}^2 - 2Mgx_{eq} KEmax=2Mgxeq12Kxeq2KE_{max} = 2Mgx_{eq} - \frac{1}{2}Kx_{eq}^2 Substitute xeq=2MgKx_{eq} = \frac{2Mg}{K}: KEmax=2Mg(2MgK)12K(2MgK)2KE_{max} = 2Mg\left(\frac{2Mg}{K}\right) - \frac{1}{2}K\left(\frac{2Mg}{K}\right)^2 KEmax=4M2g2K12K4M2g2K2KE_{max} = \frac{4M^2g^2}{K} - \frac{1}{2}K\frac{4M^2g^2}{K^2} KEmax=4M2g2K2M2g2KKE_{max} = \frac{4M^2g^2}{K} - \frac{2M^2g^2}{K} KEmax=2M2g2KKE_{max} = \frac{2M^2g^2}{K}

This matches statement (II).

Conclusion:

Statement (I) is correct: Maximum extension in the spring is 4MgK\frac{4Mg}{K}. Statement (II) is correct: Maximum kinetic energy of the system is 2M2g2K\frac{2M^2g^2}{K}. Statement (III) is incorrect. Statement (IV) is incorrect.

Therefore, the correct option is (B) I and II.