
- ✓$\frac{{2Mm}}{{\left( {M - m} \right)}}\,\frac{l}{{{t^2}}}$
- B$\frac{{\left( {M - m} \right)}}{{2Mm}}\,\frac{l}{{{t^2}}}$
- C$\frac{{2Mm}}{{\left( {M + m} \right)}}\,\frac{l}{{{t^2}}}$
- D$\frac{{\left( {M + m} \right)}}{{2Mm}}\,\frac{l}{{{t^2}}}$

$M g-F=M a_{1}$ $...(i)$
$m g-F=m a_{2}$ $...(ii)$
Now, $\quad 1+\frac{1}{2} a_{2} t^{2}=\frac{1}{2} a_{1} t^{2}$
or $a_{1}=\frac{2 l}{t^{2}}+a_{2}$ $...(iii)$
Solving equations $( i ), (ii)\, and \,(iii),$ we get;
$F=\frac{2 M m}{(M-m)} \frac{l}{t^{2}}$
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$(i){\vec V_C} - {\vec V_A} = 2\left( {{{\vec V}_B} - {{\vec V}_C}} \right)$
$(ii){\vec V_C} - {\vec V_B} = {\vec V_B} - {\vec V_A}$
$(iii)\left| {{{\vec V}_C} - {{\vec V}_A}} \right| = 2\left| {{{\vec V}_B} - {{\vec V}_C}} \right|$
$(iv)\left| {{{\vec V}_C} - {{\vec V}_A}} \right| = 4\left| {{{\vec V}_B}} \right|$

$( g =$ acceleration due to gravity)
$(\theta=$ angle as shown in figure $)$
