Particles P and Q have masses m kg and 2m kg respectively. The particles are initially held at rest 6.4 m apart on the same line of greatest slope of a rough plane inclined at an angle α to the horizontal, where sin α = 0.8 (see diagram). Particle P is released from rest and slides down the line of greatest slope. Simultaneously, particle Q is projected up the same line of greatest slope at a speed of 10 m s⁻¹. The coefficient of friction between each particle and the plane is 0.6. [Diagram]
- (a)Show that the acceleration of Q up the plane is –11.6 m s⁻².[4]
- (b)Find the time for which the particles are in motion before they collide.[5]
- (c)The particles coalesce on impact. Find the speed of the combined particle immediately after the impact.[4]
This question uses a diagram from the original paper, which isn't shown here. Open the full paper from the past papers archive to see it.
Mark scheme
Marking points from the official mark scheme (Oct/Nov 2021). The mark or mark type is shown in brackets.
- M1 Apply Newton's 2nd law along or perpendicular to the plane to particle Q. Must use values for α or sin α or cos α.
- A1 Both correct.
- M1 Using F = 0.6R where R is a component of 2mg only
- A1 AG Acceleration of Q up the plane while moving up the plane is a = -11.6 ms⁻²
- M1 Apply Newton's 2nd law to attempt to find the acceleration of particle P. Must use values for α or sin α.
- M1 For using constant acceleration equations to attempt to determine when v_Q = 0 .
- M1 Use constant acceleration equations to attempt to find either S_P(down) or S_Q(up) at time T_1.
- M1 For attempting to find the extra distance d[=0.455] needed to reach 6.4 m and using u_P =4.4T_1 at T_1 to find T_2 as d=(4.4T_1)T_2+1/2×4.4T_2²-1/2x4.4T_2².
- A1 t=0.98194357... Time before collision = [t = T_1 + T_2 = 0.862 +0.12 =]0.982
- Alternative method for Question 7(b)
- M1 Apply Newton's 2nd law to attempt to find the acceleration of particle P. Must use values for α or sin α.
- M1 For using constant acceleration equations to attempt to determine when v_Q = 0
- M1 Use constant acceleration equations to attempt to find either S_P(down) or S_Q(up) at time t where t is the total time before collision.
- M1 For applying (±) s_P + (±) s_Q = 6.4 using their expressions for s_P and s_Q to set up and solve a 3-term quadratic equation in t to obtain at least 1 solution.
- A1 t=0.98194357... Time before collision is t = 0.982 s
- Special case for those who do not take into account the fact that Q comes to rest and then changes its direction
- M1 Apply Newton's 2nd law to attempt to find the acceleration of particle P. Must use values for α or sin α.
- M1 For using constant acceleration equations to attempt to find either S_P(down) or S_Q(up).
- M1 For applying (±) s_P + (±) s_Q = 6.4 using their expressions for s_P and s_Q to set up and solve a 3-term quadratic equation in t to obtain at least 1 solution.
- A1 Must reject t = 16/9. Maximum mark 4 out of 5. Time that particles are in motion before collision t = 1 s
- B1 FT Allow ±4.4. FT on their 4.4 and their 0.982. U_P(down) = 0 + 4.4 × 0.982 [= 4.3208]
- B1 FT Allow ±4.4. FT on their 4.4 and their 0.12. U_Q(down) = 4.4 × 0.12 [= 0.528]
- M1 Apply conservation of momentum, 4 terms, using their u_P and u_Q values with m and 2m respectively. Velocity of P and Q after impact must be equal.
- A1 Must be positive. Speed of combined particle immediately after impact = v = 1.79 ms⁻¹
- Special case for those who do not take into account the fact that Q comes to rest and then changes its direction
- B1 FT Allow ±4.4, FT on their 1 and their 4.4. U_P(down) = 0 + 4.4 × 1 [= 4.4]
- B1 FT Allow ± (10 – 11.6 × 1), FT on their 1. U_Q(up) = 10 - 11.6 × 1 [= –1.6] so u_Q(down) = 1.6
- M1 Apply conservation of momentum, 4 terms, using their u_P and u_Q values with m and 2m respectively. Velocity of P and Q after impact must be equal.
- A1 Allow v = 38/15. Speed of combined particle immediately after impact = v = 2.53 ms⁻¹
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