A uniform chain of mass M and length L has a part L3 hanging over the edge of a table. If the friction between the table and the chain is neglected, the kinetic energy of the chain as it completely falls off the edge of the table is
A
2MgL3
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B
4MgL9
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C
32MgL
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D
MgL
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Solution
The correct option is B4MgL9 Mass per unit length of the chain is ML. Consider a small element of length dx at a distance x below the edge of the table. The mass of this element is m=(ML)dx. The potential energy of the hanging part of the chain is U=−∫L/30MgLxdx =−MgL∣∣∣x22∣∣∣L/30=−MgL18
Let us take the potential energy to be zero when the chain is on the table. Therefore, the total initial P.E. of the chain is Ut=0+U=−MgL18
If the full chain (of length L) were to fall, the P.E. would be Uf=∫L0MgLxdx=−MgL2 ∴ Loss in P.E = Ui−Uf=MgL2−MgL18=49MgL
Loss in P.E. = Gain in K.E. Kf−Ki=49MgL
But initially the chain was at rest. So Ki=0 Kf=49MgL