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Two particles, A and B, have masses 2m and m respectively - Edexcel - A-Level Maths Mechanics - Question 8 - 2017 - Paper 1

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Two particles, A and B, have masses 2m and m respectively. The particles are attached to the ends of a light inextensible string. Particle A is held at rest on a fix... show full transcript

Worked Solution & Example Answer:Two particles, A and B, have masses 2m and m respectively - Edexcel - A-Level Maths Mechanics - Question 8 - 2017 - Paper 1

Step 1

Write down an equation of motion for A.

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Answer

For particle A, the forces acting on it are the tension T in the string and the frictional force opposing the motion. Thus, the equation of motion can be expressed as:

TF=2maT - F = 2ma

where F is the frictional force given by ( F = \mu (2m)g ). Hence, the equation of motion is:

Tμ(2m)g=2maT - \mu (2m)g = 2ma

Step 2

Write down an equation of motion for B.

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For particle B, which is influenced by gravity, the equation of motion is:

mgT=mamg - T = ma

where mg is the weight of particle B and T is the tension in the string.

Step 3

Hence show that, until B hits the floor, the acceleration of A is $\frac{2g}{3(1 - 2\,\text{µ})}$.

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Answer

To find the acceleration, we can set the equations for T from both parts. From the equation for A: T=2ma+μ(2m)gT = 2ma + \mu (2m)g

Substituting T in the equation for B: mg(2ma+μ(2m)g)=mamg - (2ma + \mu (2m)g) = ma

Simplifying this, we have: mgμ(2m)g=3mamg - \mu (2m)g = 3ma

Thus, isolating a gives: a=mgμ(2m)g3m=g(12µ)3a = \frac{mg - \mu (2m)g}{3m} = \frac{g(1 - 2\,\text{µ})}{3}

Therefore, until B hits the floor, the acceleration of A is: a=2g3(12µ)a = \frac{2g}{3(1 - 2\,\text{µ})}

Step 4

Find, in terms of g, h and µ, the speed of A at the instant when B hits the floor.

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Answer

Using energy conservation or kinematic equations, we can derive the speed: The potential energy lost by B when it falls a distance h plus the work done against friction equals the kinetic energy gained by A:

mghμ(2m)gh=12(2m)v2mgh - \mu (2m)g h = \frac{1}{2}(2m)v^2

Solving for v gives: v=2(1µ)gh1v = \sqrt{\frac{2(1 - \text{µ})gh}{1}}

Step 5

Describe what would happen if µ = 1/2.

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Answer

If ( \mu = \frac{1}{2} ), the frictional force opposing motion would be equal to the weight component acting on A. This means that A would not accelerate; instead, it would remain in (limiting) equilibrium, and B would not move after the initial pull, leading the system to be in a stable position until external forces act on it.

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