No sliding.

In the arrangement shown in the figure mass of the block B and A are 2m,8m respectively and the floor is smooth. The block B is connected to block C by means of a pulley. If the whole system is released then the minimum value of mass of the block C so that block A remains stationary with respect to B is:

Details:
1.Co-efficient of friction between A and B is μ \mu
2.No friction between B and floor.

Please Post Solutions also.

10 m μ 1 \frac { 10m }{ \mu -1 } m μ \frac { m }{ \mu } 2 m μ + 1 \frac { 2m }{ \mu +1 } 10 m 1 μ \frac { 10m }{ 1-\mu }

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1 solution

For A to remain stationary with respect to B, friction and it's weight should cancel out i.e. μ N = ( 8 m ) g \mu N = (8m)g ; where N is the normal force by B's surface to A and they should have the same acceleration.

N will have the magnitude but opposite direction of pseudo force due to it's acceleration.

N = (8m) x ¨ \ddot{x} .

Thus,

μ ( 8 m ) x ¨ = ( 8 m ) g \mu (8m)\ddot{x} = (8m)g

x ¨ = g μ \ddot{x} = \frac{g}{\mu}

Now the system of A and B is connected to C by an inextensible string. So for A and B to accelerate at x ¨ \ddot{x} C should also accelerate at x ¨ \ddot{x} .

The force for the whole system A,B and C to accelerate at x ¨ \ddot{x} is thw weight of C.

So the force equation is

( 8 m + 2 m + M ) x ¨ = M g (8m + 2m + M)\ddot{x} = Mg ; M M is the mass of C.

x ¨ = M g 10 m + M \ddot{x} = \frac{Mg}{10m + M}

So,

g μ = M g 10 m + M \frac{g}{\mu} = \frac{Mg}{10m + M}

M = 10 m μ 1 M = \frac{10m}{\mu - 1} .

This is the minimal solution of M as increasing it will only cause to increase in the normal force N which increases limit of the friction then required.

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