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Question: Block A of mass 5 kg is kept between plank B of mass 10 kg and the inclined plane as shown below. Pl...

Block A of mass 5 kg is kept between plank B of mass 10 kg and the inclined plane as shown below. Plank B is attached to an inextensible string which is parallel to inclined plane. Block A slides with constant velocity between plank and fixed wedge. Friction coefficient between all surfaces is same as μ\mu. Find value of 20μ\mu.

A

15

B

20

C

10

D

5

Answer

15

Explanation

Solution

Block A slides with constant velocity, meaning the net force on it is zero. The forces acting on block A parallel to the inclined plane are its gravitational component (mAgsin(θ)m_A g \sin(\theta)) downwards, and friction forces from plank B (fBAf_{BA}) and the inclined plane (fAWf_{AW}) upwards. Perpendicular to the incline, the forces are the gravitational component (mAgcos(θ)m_A g \cos(\theta)) and the normal forces from plank B (NABN_{AB}) and the inclined plane (NAWN_{AW}).

For equilibrium along the incline: mAgsin(θ)=fBA+fAWm_A g \sin(\theta) = f_{BA} + f_{AW} Since f=μNf = \mu N, we have: mAgsin(θ)=μNAB+μNAW=μ(NAB+NAW)m_A g \sin(\theta) = \mu N_{AB} + \mu N_{AW} = \mu (N_{AB} + N_{AW})

For equilibrium perpendicular to the incline: NAB+NAW=mAgcos(θ)N_{AB} + N_{AW} = m_A g \cos(\theta)

Substituting the second equation into the first: mAgsin(θ)=μ(mAgcos(θ))m_A g \sin(\theta) = \mu (m_A g \cos(\theta))

Dividing by mAgcos(θ)m_A g \cos(\theta): tan(θ)=μ\tan(\theta) = \mu

Given θ=37\theta = 37^\circ, and tan(37)=34=0.75\tan(37^\circ) = \frac{3}{4} = 0.75. So, μ=0.75\mu = 0.75.

The question asks for 20μ20\mu: 20μ=20×0.75=1520\mu = 20 \times 0.75 = 15.