InterviewSolution
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InterviewSolution
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Two point masses `m_1` and `m_2` are connected by a spring of natural length `l_0`. The spring is compressed such that the two point masses touch each other and then they are fastened by a string. Then the system is moved with a velocity `v_0` along positive x-axis. When the system reached the origin, the string breaks `(t=0)`. The position of the point mass `m_1` is given by `x_1=v_0t-A(1-cos omegat)` where A and `omega` are constants. Find the position of the second block as a function of time. Also, find the relation between A and `l_0`. |
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Answer» Correct Answer - `x_(2) = v_(0)t + (m_(1))/(m_(2)) A (1 - cos omegat), l_(0) = ((m_(1))/(m_(2)) + 1) A` The string snaps and the spring force comes into play. The spring force beings an internal force for the two mass-spring system will not be able to change the velocity of centre of mass. This means the location of centre of mass at time t will be `v_(0)t` `x_(cm) = (m_(1)x_(1) + m_(2)x_(2))/(m_(1) + m_(2)) = v_(0)t` `rArr m_(1)[v_(0)t - A(1 - cos omegat)] + m_(2)x_(2) = v_(0)tm_(1) + v_(0)tm_(2)` `rArr m_(2)x_(2) = v_(0)tm_(1) + v_(0)tm_(2) - v_(0)tm_(1) + m_(1)A (1 - cos omegat)` `rArr m_(2)x_(2) = v_(0)tm_(2) + m_(1)A(1 - cos omegat)` `rArr x_(2) = v_(0)t + (m_(1))/(m_(2)) A(1 - cos omegat)` (b) Given that `x_(1) = v_(0)t - A(1 - cos omegat)` `:. (dx_(1))/(dt) = v_(0) - Aomega sin omegat` `:. (d^(2)x_(1))/(dt^(2)) = -Aomega^(2) cos omegat` ....(i) This is the acceleration of mass `m_(1)`. When the spring comes to its natural length instantaneously then `(d^(2)x_(1))/(dt^(2)) = 0` and `x_(2) - x_(1) = l_(0)` `:. [v_(0)t + (m_(1))/(m_(2)) A(1 - cos omegat)] - [v_(0)t - A (1 - cos omegat)] = l_(0)` `((m_(1))/(m_(2)) + ) A ( 1 - cos omega t ) = l_(0)` Also when `(d^(2)x_(1))/(dt^(2)) = 0, cos omegat = 0` from (1) `:. l_(0) = ((m_(1))/(m_(2)) + 1) A` |
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