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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

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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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