Two particles, A and B, have masses 2m and m respectively - Edexcel - A-Level Maths Mechanics - Question 8 - 2017 - Paper 1
Question 8
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 in the string (T) and the frictional force (f). Hence, the equation of motion can be written as:
[ T - f = 2ma ]
Here, ( f = \mu \cdot (2m)g ), the equation can also be expressed as:
[ T - \mu \cdot (2mg) = 2ma ]
This simplifies to:
[ T = 2ma + 2\mu mg ]
Step 2
Write down an equation of motion for B.
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Answer
For particle B, the only forces acting on it are the weight (mg) acting downwards and the tension (T) acting upwards. Thus, the equation of motion is:
[ mg - T = ma ]
Step 3
Hence show that, until B hits the floor, the acceleration of A is \( \frac{g}{3}(1-2\mu) \).
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Answer
Using the equations from parts (i) and (ii), from particle B's equation, we can substitute T into A's equation:
[ T = mg - ma ].
Substituting into A's equation:
[ mg - ma = 2ma + 2\mu mg ]
Rearranging gives:
[ mg - 2\mu mg = 3ma ]
This yields:
[ a = \frac{g(1-2\mu)}{3} ]
Step 4
Find, in terms of g, h and \( \mu \), the speed of A at the instant when B hits the floor.
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Answer
Using the equation of motion for constant acceleration, we have:
[ v^2 = u^2 + 2as ]
Here, ( u = 0 ), ( a = \frac{g(1-2\mu)}{3} ) and ( s = h ).
Thus,
[ v^2 = 0 + 2 \cdot \frac{g(1-2\mu)}{3} \cdot h ]
This simplifies to:
[ v = \sqrt{\frac{2gh(1-2\mu)}{3}} ]
Step 5
Describe what would happen if \( \mu = \frac{1}{2} \).
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Answer
If ( \mu = \frac{1}{2} ), the coefficients involved in the calculation would lead to a neutral balance of forces at B. This means particle A would not move due to friction being equal to the tension in the string corresponding to its weight, resulting in A remaining stationary.