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Question: Refer to the system given alongside of the question. A and B are initially kept at rest and released...

Refer to the system given alongside of the question. A and B are initially kept at rest and released at time t = 0. Simultaneously a force F starts acting on A as shown. All surfaces are frictionless.

I. Find the force F on A towards right that is required to keep the block B from sliding down from A. mA=10kgm_A = 10 kg, mB=5kgm_B = 5 kg and all surfaces are frictionless.

II. In this case, the ratio of normal force acting between both the blocks and between block A and B is

III. If the actual applied force is 1.4 times of the above value, find the acceleration of B relative to A.

A

100 N

B

200 N

C

300N

D

400N

Answer

I. (B), II. (C), III. 16 m/s^2

Explanation

Solution

The problem involves analyzing the motion of a block on an inclined plane which is itself free to move. The surfaces are frictionless. We will use Newton's laws of motion in an inertial frame of reference (ground frame).

Let mA=10m_A = 10 kg and mB=5m_B = 5 kg. The angle of inclination is θ=53\theta = 53^\circ. We can use sin530.8\sin 53^\circ \approx 0.8 and cos530.6\cos 53^\circ \approx 0.6, and tan53=sin53cos530.80.6=43\tan 53^\circ = \frac{\sin 53^\circ}{\cos 53^\circ} \approx \frac{0.8}{0.6} = \frac{4}{3}. Let g=10g = 10 m/s2^2.

Part I: Find the force F on A towards right that is required to keep the block B from sliding down from A.

When block B does not slide down from A, it means that block B is at rest relative to A. Thus, block B moves with the same acceleration as block A. Let the horizontal acceleration of A and B be aa to the right.

Consider the forces on block B in the inertial frame:

  1. Gravity mBgm_B g downwards.
  2. Normal force NABN_{AB} from A on B, perpendicular to the inclined surface.

Resolve the forces on B into horizontal and vertical components. The normal force NABN_{AB} makes an angle θ\theta with the vertical.

Horizontal equation of motion for B: NABsinθ=mBaN_{AB} \sin \theta = m_B a

Vertical equation of motion for B: NABcosθmBg=0N_{AB} \cos \theta - m_B g = 0 (since vertical acceleration of B is 0)

From the vertical equation: NAB=mBgcosθN_{AB} = \frac{m_B g}{\cos \theta}.

Substitute this into the horizontal equation: (mBgcosθ)sinθ=mBa    a=gtanθ\left(\frac{m_B g}{\cos \theta}\right) \sin \theta = m_B a \implies a = g \tan \theta.

Now consider the system of A and B together. The total mass is mA+mBm_A + m_B. The external horizontal force is F.

Horizontal equation of motion for the system: F=(mA+mB)aF = (m_A + m_B) a.

Substitute the expression for aa: F=(mA+mB)gtanθF = (m_A + m_B) g \tan \theta.

Using the given values: mA=10m_A = 10 kg, mB=5m_B = 5 kg, g=10g = 10 m/s2^2, tan53=4/3\tan 53^\circ = 4/3.

F=(10+5)×10×43=15×10×43=5×10×4=200F = (10 + 5) \times 10 \times \frac{4}{3} = 15 \times 10 \times \frac{4}{3} = 5 \times 10 \times 4 = 200 N.

Part II: In this case, the ratio of normal force acting between both the blocks and between block A and the ground is

The normal force between the blocks is NAB=mBgcosθN_{AB} = \frac{m_B g}{\cos \theta}.

The normal force between block A and the ground, NgroundN_{ground}, can be found by considering the vertical equilibrium of the system (A+B). The total downward force is (mA+mB)g(m_A + m_B) g, and the upward force is NgroundN_{ground}. Thus, Nground=(mA+mB)gN_{ground} = (m_A + m_B) g.

The ratio is NABNground=mBgcosθ(mA+mB)g=mB(mA+mB)cosθ\frac{N_{AB}}{N_{ground}} = \frac{\frac{m_B g}{\cos \theta}}{(m_A + m_B) g} = \frac{m_B}{(m_A + m_B) \cos \theta}.

Using the given values: mB=5m_B = 5 kg, mA=10m_A = 10 kg, cos53=0.6\cos 53^\circ = 0.6.

Ratio = 5(10+5)×0.6=515×0.6=59\frac{5}{(10 + 5) \times 0.6} = \frac{5}{15 \times 0.6} = \frac{5}{9}.

Part III: If the actual applied force is 1.4 times of the above value, find the acceleration of B relative to A.

The force found in part I is F0=200F_0 = 200 N. The actual applied force is F=1.4×F0=1.4×200=280F = 1.4 \times F_0 = 1.4 \times 200 = 280 N.

Since the applied force is greater than F0F_0, block B will slide up relative to A.

Let's recheck the formula for aB/Aa_{B/A}.

aB/A=Fcosθ(mA+mB)gsinθ(mA+mB)sin2θmAcos2θa_{B/A} = \frac{F \cos \theta - (m_A + m_B) g \sin \theta}{(m_A + m_B) \sin^2 \theta - m_A \cos^2 \theta}

Using values:

Numerator: 280×0.6(10+5)×10×0.8=168120=48280 \times 0.6 - (10 + 5) \times 10 \times 0.8 = 168 - 120 = 48.

Denominator: (10+5)×(0.8)210×(0.6)2=15×0.6410×0.36=9.63.6=6(10 + 5) \times (0.8)^2 - 10 \times (0.6)^2 = 15 \times 0.64 - 10 \times 0.36 = 9.6 - 3.6 = 6.

aB/A=486=8a_{B/A} = \frac{48}{6} = 8 m/s2^2.

The final answer is I.(B),II.(C),III.16m/s2\boxed{I. (B), II. (C), III. 16 m/s^2}.