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Two particles A and B, of mass 7 kg and 3 kg respectively, are attached to the ends of a light inextensible string - Edexcel - A-Level Maths Mechanics - Question 7 - 2011 - Paper 1

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Two particles A and B, of mass 7 kg and 3 kg respectively, are attached to the ends of a light inextensible string. Initially B is held at rest on a rough fixed plan... show full transcript

Worked Solution & Example Answer:Two particles A and B, of mass 7 kg and 3 kg respectively, are attached to the ends of a light inextensible string - Edexcel - A-Level Maths Mechanics - Question 7 - 2011 - Paper 1

Step 1

Find the magnitude of the acceleration of B immediately after release.

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Answer

To find the acceleration of B, we start by analyzing the forces acting on both particles A and B.

Forces on A:

For particle A (mass = 7 kg), the forces acting are:

  • Weight: FA=7gF_A = 7g (downwards)
  • Tension in the string: TT (upwards)

From Newton's second law, we can write: 7gT=7aag17g - T = 7a ag{1}

Forces on B:

For particle B (mass = 3 kg), along the plane:

  1. Tension acting up the plane: TT
  2. Weight component down the plane: 3gsinθ3g \sin \theta
  3. Frictional force opposing the motion: Ffriction=μR=23×RF_{friction} = \mu R = \frac{2}{3} \times R

Where R=3gcosθR = 3g \cos \theta is the normal force acting on B.

Thus, along the plane: T3gsinθ23R=3aag2T - 3g \sin \theta - \frac{2}{3} R = 3a ag{2}

Substitute R:

Substituting for R:

ightarrow F_{friction} = \frac{2}{3}(3g \cos \theta) = 2g \cos \theta$$ So the equation for B becomes: $$T - 3g \sin \theta - 2g \cos \theta = 3a ag{3}$$ ### System of Equations: Now we can solve Equations (1) and (3). First, substituting $\sin \theta$ and $\cos \theta$ from $tan \theta = \frac{5}{12}$: - $\sin \theta = \frac{5}{13}$ - $\cos \theta = \frac{12}{13}$ Now substitute these into (3): 1. Substitute into Equation (1) to express T: \[ T = 7g - 7a \tag{4} \] 2. Substitute $\sin \theta$ and $\cos \theta$ into Equation (3) to get: \[ (7g - 7a) - 3g \cdot \frac{5}{13} - 2g \cdot \frac{12}{13} = 3a \tag{5} \] Rearranging gives: \[ 7g - 7a - \frac{15g}{13} - \frac{24g}{13} = 3a \rightarrow \frac{91g - 39g}{13} = 10a \] Simplifying leads to: \[ 52g = 10a\qquad a = \frac{26g}{5} \tag{6} \] Substituting $g \approx 9.8 ext{ m/s}^2$ results in: \[ a \approx 5.088 m/s^{2} ext{ or } 5.09 m/s^{2}.\]

Step 2

Find the speed of B when it has moved 1 m up the plane.

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Answer

Using the kinematic equation to determine the speed of B after moving 1 m up the plane, we apply:

v2=u2+2as,v^2 = u^2 + 2as, where:

  • u=0u = 0 (initial speed),
  • s=1s = 1 m (distance moved),
  • a=5.088m/s2a = 5.088 m/s^2 (acceleration found previously).

Thus, v2=0+25.0881=10.176,v^2 = 0 + 2 \cdot 5.088 \cdot 1 = 10.176, v=10.1763.19m/s.v = \sqrt{10.176} \approx 3.19 m/s.

Step 3

Find the time between the instants when the string breaks and when B comes to instantaneous rest.

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Answer

After the string breaks, the forces acting on particle B are:

F=(3g+Ffriction)=(3g+233gcosθ)F = - \left( 3g + F_{friction} \right) = -\left( 3g + \frac{2}{3} \cdot 3g \cos \theta \right)

This can be simplified to: F=3g(1+231213)3g(1+0.1846)3g1.1846=3.5538g,F = -3g \left(1 +\frac{2}{3}\cdot\frac{12}{13}\right) \approx -3g \cdot (1 + 0.1846) \approx -3g \cdot 1.1846 = -3.5538g, which is the deceleration B experiences.

Using the kinematic equation: v=u+at,v = u + at, where u=3.19m/su = 3.19 m/s, v=0v = 0 (final speed at rest), a=3g0.1846a = -3g \cdot 0.1846.

Thus, 0=3.193g(0.1846)t,0 = 3.19 - 3g (0.1846)t, which leads to solving for tt: $$t \approx \frac{3.19}{3g\cdot 0.1846} \approx 0.229 s.$

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