In the figure shown, assume ideal pulleys and inextensible, massless strings. Find the acceleration of masses $M$ and $2M$ when the system is released from rest at an angle $\theta=60^\circ$. Take $g=10 m/s^2$. Solution If $M$ goes up by $h$ and $s$ is the length of the string on the right side of left pulley, $s^2 = h^2 + constant^2$ So, $s \frac {ds}{dt} = h \frac {dh}{dt}$ Or, $s v= h v'$ (here $v$ is instantaneous velocity of $2M$ and $v'$ is the instantaneous velocity of $M$) Or, $v = v' cos \theta$ Or, $a = a' cos \theta + v' \frac {d}{dt}cos \theta$ [Differentiating w.r.t. t. Here $a$ is instantaneous acceleration of $2M$ and $a'$ is the instantaneous acceleration of $M$.] Since the system is released from rest, $v' = 0$. So, $a = a' cos \theta$ or $a'=2a$ (Note that $a'=2a$ is valid only in the beginning of the motion and not throughout the motion.) Equation of motion for $2M$, $2Mg - T = 2Ma$ Equation of motion for $M$, $2Tcos 60^\circ -...
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