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A block of mass `m` is connected to another block of mass `M` by a massless spring of spring constant `k`. the blocks are kept of a smooth horizontal plane and are at rest. The spring is unstretched when a constant force `F` starts acting on the block of mass `M` of pull it. Find the maximum extension of the spring
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We solve the situation in the reference frame of centre of mass As only `F` is the external force acting on the system, due to this force, the acceleration of the centre of mass is `F/(M+m)`. Thus, with respect to centre of mass, there is as pseudoforce on the two mases in the opposite direction,the free body digram of `m` and `M` with respect to centre of mass (taking centre of mass at rest) is shown in figure.
image
Taking centre of mass ast rest, if `m` moves maximum by a distance `x_(1)` and `M` moves maximum by a distance `x_(2)` then the work done by external forces (including pseudoforce) will be
`W=(mF)/(m+M)x_(1)+(F-(MF)/(m+M))x_(2)=(mF)/(m+M)(x_(1)+x_(2))`
this work is stored in the form of potential energy of the spring as `U=(1/2)k(x_(1)+x_(2))^(2)`.
Thus, on equation we get the maximum extension in the spring, as after this instant the sprig starts contracting.
`1/2k(x_(1)+x_(2))^(2)=(mF)/(m+M)(x_(1)+x_(2))`
`implies x_(max)=x_(1)+x_(2)=(2mF)/(k(m+M))`

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