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Q.

Two bodies m1 and m2 are kept on a table with coefficient of friction ‘μ’ and are joined by a spring.  Initially, the spring is in its relaxed state. The minimum constant force F which will make the other block m2 move is ( k is the spring constant).

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a

large {F_{min }} = mu {m_1}g + frac{{mu {m_2}g}}{2}

b

large {F_{min }} = frac{{mu {m_1}g, + ,mu {m_2}g}}{2}

c

large {F_{min }} = frac{{mu {m_1}g, + ,mu {m_2}g}}{4}

d

large {F_{min }} = mu {m_1}g + mu {m_2}g

answer is A.

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Detailed Solution

Motion of  m2 starts when,  kx = μ m2.g    

Where  x = elongation in the spring

large x = frac{{mu {m_2}g}}{k}\\

The minimum force will be such that m1 has no kinetic energy.
    Applying work energy principle for m1

fn_cm large int_{,0}^{,x} {(F - mu {m_1}g - kx)} ,dx = 0 \\Fx - mu m_1 gx - frac12 kx^2 =0\\Rightarrow F = left[ {mu {m_1}g + frac{1}{2}kx} right] = left[ {mu {m_1}g + frac{{mu {m_2}g}}{2}} right]\\Rightarrow {F_{min }} = mu {m_1}g + frac{{mu {m_2}g}}{2}

Alternative solution :

Minimum spring force required to move the block m2 = µ m2 g

.: kx = µ m2 g ....................(1)

For minimum firce F , kinetic energy of the block will be negligibly small.

.: F X x = work done against frictional force on m1 + Elastic P.E strored .

= µ m1g X x + 1/2 kx2

.: kx = 2 F - 2 µ m1 g ....................(2)

From (1) and (2), F =(µ m1 g + 1/2 µ m2 g)

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