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- In the system shown in figure, masses of the blocks are such that when system is released, the acceleration of pulley P1 is a upward and acceleration of block A is a1 upward. It is found that the acceleration of block C is same as that of A both in magnitude and direction (a1 > a > a1 / 2). Then
Q.
In the system shown in figure, masses of the blocks are such that when system is released, the acceleration of pulley $P_{1}$ is $a$ upward and acceleration of block $A$ is $a_{1}$ upward. It is found that the acceleration of block $C$ is same as that of $A$ both in magnitude and direction $\left(a_{1} > a > a_{1} / 2\right)$. Then
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Solution:
The acceleration of block $A$, w.r.t pulley $P_{1}$;
$a_{A P_{1}}=\left(a_{1}-a\right) \uparrow$
$a_{B P_{1}}=\left(a_{B}-a\right) \downarrow$
The acceleration of block $B$, w.r.t pulley $P_{1}$;
But, $\left|\vec{a}_{AP_{1}}\right|=-\left|\vec{a}_{B P_1}\right|$
$a_{1}-a \equiv a_{B}+a$
Hence, $a_{B}=2 a-a_{1} \uparrow$
The acceleration of block $C$ w.r.t pulley $P_{2}$;
$a_{C P_{2}}=\left(a_{c}+a\right) \uparrow$
The acceleration of block $D$ w.r.t pulley $P_{2}$;
$a_{D P_{2}}=\left(a_{D}-a\right) \downarrow$
$a_{C}+a=a_{D}-a$
$a_{D}=\left(2 a+a_{1}\right) \downarrow$
Hence, $\vec{a}_{B C}=\vec{a}_{B}-\vec{a}_{c}=2\left(a_{1}-a\right) \downarrow$
and $\vec{a}_{\beta D}=\vec{a}_{\Delta}-\vec{a}_{D}=4 a \uparrow$
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