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A uniform chain of mass m and length l is on a smooth horizontal table with (1/n)^th part of its leght is hanging from one end of the table. The velocity of the chain, when it completely slips off the table is

Answer»

Solution :With respect to the TOP of the table, the initial potential energy of the chain,
`U_(1)`= PE of the chain lying on the table + PE of the hanging PART of the chain
`=L(1-(1)/(n))mg(0)+(m)/(n)g""((-L)/(2N))=-(MGL)/(2n^(2))`
P.E of the chain, when it just slips off the table,
`U_(2)= mg((-L)/(2))=-(mgL)/(2)`
From jaw of conservation of energy
`Delta K = - Delta U K_(f) - K_(i) = - (U_(f) - U _(i))`
`thereforeK_(i)=0,K_(f)=-[-(mgL)/(2)-(-(mgL)/(2n^(2)))]`
`K_(f)= (mgL)/(2)[1-(1)/(n^(2))]`
It .V. is the velocity of the chain, then, `(1)/(2)mv^(2)=(mgL)/(2)[1-(1)/(n^(2))]`
`thereforev=sqrt(gL[1-(1)/(n^(2))])`


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