A block of mass m is attached to a pulley disc of equal mass m ,radius r by means of a slack string as shown.the pulley is hinged about its centre on a horizontal table and the block is projected with an initial velocity of 5 m/s.its velocity when the string becomes taut will be
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initial velocity of block, 
Let final velocity of block ,
from Newton's 2nd law,

we know, torque is the rate of change of angular momentum.
e.g.,
or,![-F.r=\frac{dL}{dt}<br /><br />here negative sign shows that force on the pulley is opposing to the force on the mass of the table. <br /><br />or, [tex]-\frac{m(v_2-v_1)}{dt}.r=\frac{I(\omega_2-\omega_1)}{dt} -F.r=\frac{dL}{dt}<br /><br />here negative sign shows that force on the pulley is opposing to the force on the mass of the table. <br /><br />or, [tex]-\frac{m(v_2-v_1)}{dt}.r=\frac{I(\omega_2-\omega_1)}{dt}](https://tex.z-dn.net/?f=-F.r%3D%5Cfrac%7BdL%7D%7Bdt%7D%3Cbr+%2F%3E%3Cbr+%2F%3Ehere+negative+sign+shows+that+force+on+the+pulley+is+opposing+to+the++force+on+the+mass+of+the+table.+%3Cbr+%2F%3E%3Cbr+%2F%3Eor%2C+%5Btex%5D-%5Cfrac%7Bm%28v_2-v_1%29%7D%7Bdt%7D.r%3D%5Cfrac%7BI%28%5Comega_2-%5Comega_1%29%7D%7Bdt%7D)
but Initial angular velocity ,
now,
moment of inertia of disc about an axis passing through centre of it and perpendicular to its plane is given by, I = mr²/2
so,
or,
or,
so,
hence,
therefore, velocity of block when the string becomes taut will be 10/3 m/s .
Let final velocity of block ,
from Newton's 2nd law,
we know, torque is the rate of change of angular momentum.
e.g.,
or,
but Initial angular velocity ,
now,
moment of inertia of disc about an axis passing through centre of it and perpendicular to its plane is given by, I = mr²/2
so,
or,
or,
so,
hence,
therefore, velocity of block when the string becomes taut will be 10/3 m/s .
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