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One end of a light inextensible string is attached to a block P of mass 5 kg - Edexcel - A-Level Maths Mechanics - Question 7 - 2009 - Paper 1

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One end of a light inextensible string is attached to a block P of mass 5 kg. The block P is held at rest on a smooth fixed plane which is inclined to the horizontal... show full transcript

Worked Solution & Example Answer:One end of a light inextensible string is attached to a block P of mass 5 kg - Edexcel - A-Level Maths Mechanics - Question 7 - 2009 - Paper 1

Step 1

(i) the acceleration of the scale pan

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Answer

To find the acceleration of the scale pan, we can use Newton's second law for the system. The forces acting on block P along the incline are:

  • Weight component: 5gsinβ5g \sin \beta (down the incline)
  • Tension (T) in the string (up the incline)

Thus, we can set up the equation: T5gsinβ=5aT - 5g \sin \beta = 5a

From the problem, we have sinβ=35\sin \beta = \frac{3}{5}, hence: T5g35=5aT - 5g \cdot \frac{3}{5} = 5a T3g=5a(1)T - 3g = 5a \quad (1)

For the system of block Q and R, we have: 15gT=15a(2)15g - T = 15a \quad (2)

Now, we can express equation (1) as: T=3g+5aT = 3g + 5a

Substituting this in equation (2): 15g(3g+5a)=15a15g - (3g + 5a) = 15a 12g=20a12g = 20a a=12g20=0.6ga = \frac{12g}{20} = 0.6g

Step 2

(ii) the tension in the string

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Answer

We substitute a=0.6ga = 0.6g back into equation (1): T3g=5(0.6g)T - 3g = 5(0.6g) T3g=3gT - 3g = 3g T=6gT = 6g

Step 3

the magnitude of the force exerted on block Q by block R

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Answer

For block Q, the forces acting on it include its weight and the normal force exerted by block R. The weight of block Q is: WQ=15gW_Q = 15g

The normal force (N) acting on block Q can be calculated using: N=15gFN = 15g - F where FF is the force experienced by block Q due to block R. From the previous calculation, we have: F=5a=5×0.6g=3gF = 5a = 5 \times 0.6g = 3g Therefore, substituting: N=15g3g=12gN = 15g - 3g = 12g

Step 4

the magnitude of the force exerted on the pulley by the string

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Answer

To find the force exerted on the pulley by the string, we consider the tension in the string. The net force acting on the pulley due to the string is: F=2Tcos(90α)F = 2T \cos(90^{\circ} - \alpha)

With T=6gT = 6g and given that cos(90α)=sinα\cos(90^{\circ} - \alpha) = \sin \alpha: F=2×6gsinαF = 2 \times 6g \cdot \sin \alpha We need to evaluate sinα\sin \alpha which can be derived from sinβ\sin \beta as α=90β\alpha = 90^{\circ} - \beta and is equivalent to:\nF=12gsin(β)=12g45=9.6g(approx.105N).F = 12g \cdot \sin(\beta) = 12g \cdot \frac{4}{5} = 9.6g \, (approx. \, 105 \, N).

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