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A system of two light smooth pulleys and light inextensible strings, has two masses M1 and M2 , attached as shown. The pulley P2 is movable and pulley P1 is a fixed pulley. If the mass M2 moves up and the mass M1 moves down, the accelerations of the masses M1 and M2 , are, respectively

(1) \((\frac{4M_1-2M_2}{4M_1+M_2})\)g and \((\frac{2M_1-M_2}{4M_1+M_2})g\)

(2) \((\frac{4M_1-2M_2}{4M_1+M_1})\) g and \((\frac{2M_1-M_2}{4M_1+M_2})g\)

(3)  \((\frac{4M_1-2M_2}{4M_1+M_1})\) and \((\frac{2M_1-M_2}{4M_1+M_2})g\)

(4) \((\frac{4M_1-2M_2}{4M_1+M_2})\) g and   \((\frac{2M_1-M_2}{4M_1+M_2})g\)

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 (1) \((\frac{4M_1-2M_2}{4M_1+M_2})\)g and \((\frac{2M_1-M_2}{4M_1+M_2})g\)

Let T1 and T2 be the tensions in the strings, as shown. We see that

T1 = 2T2

Pulley P2 is massless. If there is a net force on it, acceleration will approach infinity. For the mass M2 , moving upward, the acceleration will be half that of the mass M1 , moving downwards. [This is because a downward displacement Δx , of mass Mwill result in an upward displacement of (Δx/2) of mass M2]

Hence the equations of motion of the two masses are

Adding (3) and (4), we get

The acceleration of mass M1 is, therefore,

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