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Question: A uniform rope of linear mass density \(\lambda \) and length \(l\) is coiled on a smooth horizontal...

A uniform rope of linear mass density λ\lambda and length ll is coiled on a smooth horizontal surface. One end is pulled up by an external agent with constant vertical velocity vv.Choose the correct option(s).
(A). Power developed by external agent as a function of xxis P=λxgvP = \lambda xgv
(B). Power developed by external agent as a function of xxis P=(λv2+λxg)vP = (\lambda {v^2} + \lambda xg)v
(C). Energy lost during the complete lift of the rope is zero.
(D). Energy lost during the complete lift of the rope is λlv22\dfrac{{\lambda l{v^2}}}{2}

Explanation

Solution

Here we apply the concept of average power which is defined as total work done per unit time.
Formula Used: Pavg=WtotalT{P_{avg}} = \dfrac{{{W_{total}}}}{T}

Complete step by step answer:
Average power is total work done per unit time.
Pavg=WtotalT=W1+W2T................(1){P_{avg}} = \dfrac{{{W_{total}}}}{T} = \dfrac{{{W_1} + {W_2}}}{T}................(1)
For W1{W_1},
dw=Fdx=λxgdxdw = Fdx = \lambda xgdx
W1=dw=0Lλxgdx=λgL22{W_1} = \int {dw = \int\limits_0^L {\lambda xgdx} } = \dfrac{{\lambda g{L^2}}}{2} (λ=mL)\left( {\because \lambda = \dfrac{m}{L}} \right)
From work energy theorem
W=ΔK.E=12Mv20=12Mv2W = \Delta K.E = \dfrac{1}{2}M{v^2} - 0 = \dfrac{1}{2}M{v^2}
Put the value of W1{W_1} and W2{W_2}in equation (1)
Pavg=λgv2+12λLv2Lv{P_{avg}} = \dfrac{{\lambda g{v^2} + \dfrac{1}{2}\lambda L{v^2}}}{{\dfrac{L}{v}}} (T=Lv)\left( {T = \dfrac{L}{v}} \right)
=λvgL2+12λv3= \dfrac{{\lambda vgL}}{2} + \dfrac{1}{2}\lambda {v^3}

Hence option B is correct.

Note: In this question it is said that a uniform rope of a length and a linear mass density which is coiled in on the horizontal smooth surface and from one side of the rope is pulled up with a constant velocity and we have to choose among the average power applied by the external agent in pulling the entire rope and the two condition of energy.
Other method,
The mass of the rope m=λdxm = \lambda dx
The force or weight of the rope F=λgdxF = \lambda gdx
The power acting on the rope P=λgdx×v=λgv0ldxP = \lambda gdx \times v = \lambda gv\int\limits_0^l {dx}
The average power P=λgv[x]0l=λgvlP = \lambda gv\left[ x \right]_0^l = \lambda gvl