Level 4 — ApplicationMomentum & Collisions

Momentum & Collisions

60 minutes60 marksprintable — key stays hidden on paper

Level 4: Application Paper (Unseen Problems)

Time limit: 60 minutes Total marks: 60 Instructions: Show all working. Take all motion as frictionless unless stated. Use g=9.8 m s2g = 9.8\ \text{m s}^{-2}.


Question 1 — Variable mass & impulse (12 marks)

A hopper drops sand vertically onto a horizontal conveyor belt at a steady rate of R=4.0 kg s1R = 4.0\ \text{kg s}^{-1}. The belt moves horizontally at a constant speed v=2.5 m s1v = 2.5\ \text{m s}^{-1}. The sand lands with zero horizontal velocity and is quickly brought up to belt speed.

(a) Derive, from the impulse–momentum theorem, an expression for the horizontal force the motor must supply to keep the belt moving at constant speed, and evaluate it. (5)

(b) Calculate the rate at which the motor does work on the sand. (3)

(c) Calculate the rate at which kinetic energy is gained by the sand. Explain quantitatively why these two rates differ, and where the missing power goes. (4)


Question 2 — 1D elastic collision, unknown mass (12 marks)

A ball of mass m1m_1 moving at u1=6.0 m s1u_1 = 6.0\ \text{m s}^{-1} collides head-on and elastically with a stationary ball of mass m2m_2. After the collision the first ball rebounds (moves backward) at 2.0 m s12.0\ \text{m s}^{-1}.

(a) Using conservation of momentum and the elastic-collision velocity relation, find the ratio m2/m1m_2/m_1. (6)

(b) Find the final velocity of the second ball. (3)

(c) Verify that kinetic energy is conserved (express results as fractions of the initial KE). (3)


Question 3 — Centre of mass of a composite lamina (12 marks)

A uniform lamina is formed from a solid semicircular disc of radius RR with a circular hole of radius R/2R/2 cut out. The straight edge (diameter) of the semicircle lies on the xx-axis, centre at the origin, semicircle in the region y>0y > 0. The hole is centred at the point (0, R/2)(0,\ R/2).

(You may use: centre of mass of a solid semicircular disc of radius aa lies at distance 4a/3π4a/3\pi from the diameter.)

(a) Find the yy-coordinate of the centre of mass of the full semicircular disc (before cutting). (2)

(b) Using the negative-mass method, derive the yy-coordinate of the centre of mass of the lamina with the hole. Give the answer as a multiple of RR. (8)

(c) State, with reason, the xx-coordinate of the centre of mass. (2)


Question 4 — 2D collision & restitution (12 marks)

A puck A of mass 2.0 kg2.0\ \text{kg} moving at 5.0 m s15.0\ \text{m s}^{-1} along the +x+x axis strikes a stationary puck B of mass 3.0 kg3.0\ \text{kg}. After the collision, A moves at 30°30° above the xx-axis and B moves at some angle θ\theta below the xx-axis. A is measured to leave at 2.0 m s12.0\ \text{m s}^{-1}.

(a) Using conservation of momentum in both directions, find the speed of B and the angle θ\theta. (7)

(b) Determine whether this collision is elastic, and compute the fraction of kinetic energy lost. (5)


Question 5 — CM motion with external force (12 marks)

Two blocks, mA=1.0 kgm_A = 1.0\ \text{kg} and mB=3.0 kgm_B = 3.0\ \text{kg}, are connected by a compressed massless spring and held together at rest on a frictionless floor. The system is released; the spring pushes them apart and detaches. Immediately after separation, block A moves left at 6.0 m s16.0\ \text{m s}^{-1}.

(a) Find the velocity of block B, and the velocity of the centre of mass, immediately after separation. (4)

(b) Now suppose the same experiment is done, but a constant horizontal external force F=8.0 NF = 8.0\ \text{N} (pointing right) acts on the whole system throughout. State the acceleration of the centre of mass, and explain why the relative separation velocity of the two blocks is unaffected by FF. (4)

(c) Find the energy stored in the spring before release (assume all of it converts to KE of the blocks in the frictionless, force-free case of part (a)). (4)


Answer keyMark scheme & solutions

Question 1 (12 marks)

(a) Consider mass dm=Rdtdm = R\,dt landing per unit time, brought from 00 to vv. Impulse–momentum: Fdt=dmv=(Rdt)vF=RvF\,dt = dm\cdot v = (R\,dt)v \Rightarrow F = Rv. (3, derivation) F=4.0×2.5=10 NF = 4.0 \times 2.5 = 10\ \text{N}. (2)

(b) Motor power = force × belt speed (force applied moving belt at vv): Pmotor=Fv=10×2.5=25 WP_{motor} = Fv = 10 \times 2.5 = 25\ \text{W}. (3)

(c) KE gain rate: each kg gains 12v2\tfrac12 v^2; rate =12Rv2=12(4.0)(2.5)2=12.5 W= \tfrac12 R v^2 = \tfrac12(4.0)(2.5)^2 = 12.5\ \text{W}. (2) Difference =2512.5=12.5 W= 25 - 12.5 = 12.5\ \text{W} dissipated as heat/friction as sand slips and accelerates to belt speed (exactly half the motor power is lost in this "sudden acceleration" process). (2)


Question 2 (12 marks)

(a) Elastic velocity relation: relative speed reverses, so v2v1=u1u2v_2 - v_1 = u_1 - u_2. Here u1=6u_1=6, u2=0u_2=0, v1=2v_1=-2 (rebounds). So v2(2)=60v2=4 m s1v_2 - (-2) = 6 - 0 \Rightarrow v_2 = 4\ \text{m s}^{-1}. (2) Momentum: m1u1=m1v1+m2v2m_1 u_1 = m_1 v_1 + m_2 v_2 6m1=2m1+4m28m1=4m2m2/m1=26m_1 = -2m_1 + 4m_2 \Rightarrow 8m_1 = 4m_2 \Rightarrow \boxed{m_2/m_1 = 2}. (4)

(b) v2=4.0 m s1v_2 = 4.0\ \text{m s}^{-1} (forward). (3)

(c) Let m1=1m_1=1, m2=2m_2=2. KEi=12(1)(62)=18 JKE_i = \tfrac12(1)(6^2) = 18\ \text{J}. KEf=12(1)(22)+12(2)(42)=2+16=18 JKE_f = \tfrac12(1)(2^2) + \tfrac12(2)(4^2) = 2 + 16 = 18\ \text{J}. Conserved. As fractions: A retains 2/18=1/92/18 = 1/9, B carries 16/18=8/916/18 = 8/9. (3)


Question 3 (12 marks)

(a) Full semicircular disc radius RR: yˉfull=4R3π\bar y_{full} = \dfrac{4R}{3\pi}. (2)

(b) Areas: full A1=12πR2A_1 = \tfrac12\pi R^2; hole A2=π(R/2)2=πR24A_2 = \pi (R/2)^2 = \tfrac{\pi R^2}{4}. Remaining area A=A1A2=πR22πR24=πR24A = A_1 - A_2 = \tfrac{\pi R^2}{2} - \tfrac{\pi R^2}{4} = \tfrac{\pi R^2}{4}. (2) Centroids: y1=4R3πy_1 = \tfrac{4R}{3\pi}, y2=R/2y_2 = R/2 (hole centre). (1) Negative-mass: yˉ=A1y1A2y2A1A2\bar y = \dfrac{A_1 y_1 - A_2 y_2}{A_1 - A_2}. (2) Numerator =πR224R3ππR24R2=2R33πR38= \tfrac{\pi R^2}{2}\cdot\tfrac{4R}{3\pi} - \tfrac{\pi R^2}{4}\cdot\tfrac{R}{2} = \tfrac{2R^3}{3} - \tfrac{\pi R^3}{8}. yˉ=2R33πR38πR24=R23π8π4\bar y = \dfrac{\tfrac{2R^3}{3} - \tfrac{\pi R^3}{8}}{\tfrac{\pi R^2}{4}} = R\cdot\dfrac{\tfrac{2}{3}-\tfrac{\pi}{8}}{\tfrac{\pi}{4}}. (2) Numerically: 23=0.6667\tfrac23 = 0.6667, π8=0.3927\tfrac{\pi}{8}=0.3927, diff =0.2740=0.2740; π4=0.7854\tfrac{\pi}{4}=0.7854. yˉ=0.2740/0.7854R0.349R\bar y = 0.2740/0.7854 \, R \approx \boxed{0.349\,R}. (1)

(c) xˉ=0\bar x = 0 — the lamina (and the hole) is symmetric about the yy-axis. (2)


Question 4 (12 marks)

(a) xx: 2(5)=2(2)cos30°+3vBcosθ2(5) = 2(2)\cos30° + 3 v_B\cos\theta 10=3.464+3vBcosθ3vBcosθ=6.53610 = 3.464 + 3v_B\cos\theta \Rightarrow 3v_B\cos\theta = 6.536. (2) yy: 0=2(2)sin30°3vBsinθ3vBsinθ=2.00 = 2(2)\sin30° - 3v_B\sin\theta \Rightarrow 3v_B\sin\theta = 2.0. (2) Divide: tanθ=2.0/6.536=0.3060θ=17.0°\tan\theta = 2.0/6.536 = 0.3060 \Rightarrow \theta = 17.0°. (2) 3vB=6.5362+2.02=42.72+4.0=6.835vB=2.28 m s13v_B = \sqrt{6.536^2 + 2.0^2} = \sqrt{42.72+4.0} = 6.835 \Rightarrow v_B = 2.28\ \text{m s}^{-1}. (1)

(b) KEi=12(2)(52)=25 JKE_i = \tfrac12(2)(5^2) = 25\ \text{J}. KEf=12(2)(22)+12(3)(2.2782)=4+7.79=11.79 JKE_f = \tfrac12(2)(2^2) + \tfrac12(3)(2.278^2) = 4 + 7.79 = 11.79\ \text{J}. (3) Not elastic (KEf<KEiKE_f < KE_i). Fraction lost =(2511.79)/25=0.52853%= (25-11.79)/25 = 0.528 \approx 53\%. (2)


Question 5 (12 marks)

(a) Momentum conservation (initial total =0=0): mAvA+mBvB=0m_A v_A + m_B v_B = 0. Take left as negative: vA=6v_A = -6. (1)(6)+(3)vB=0vB=+2.0 m s1(1)(-6) + (3)v_B = 0 \Rightarrow v_B = +2.0\ \text{m s}^{-1} (right). (3) vCM=0v_{CM} = 0 (total momentum zero, no external force). (1)

(b) With F=8.0 NF = 8.0\ \text{N} on total mass 4.0 kg4.0\ \text{kg}: aCM=F/M=8.0/4.0=2.0 m s2a_{CM} = F/M = 8.0/4.0 = 2.0\ \text{m s}^{-2} (right). (2) The external force accelerates the CM but adds equally to both blocks' momenta in a way that shifts the CM frame uniformly; internal spring forces (equal & opposite) set the relative velocity, which depends only on internal impulse, not on FF. Hence relative separation velocity (6+2=8 m s16+2 = 8\ \text{m s}^{-1}) is unchanged. (2)

(c) Spring energy =KE= KE of blocks (part a): E=12(1)(62)+12(3)(22)=18+6=24 JE = \tfrac12(1)(6^2) + \tfrac12(3)(2^2) = 18 + 6 = 24\ \text{J}. (4)


[
  {"claim":"Q1 motor power 25W and KE gain 12.5W, loss 12.5W",
   "code":"R=4.0; v=2.5; F=R*v; Pmotor=F*v; Pke=Rational(1,2)*R*v**2; result=(F==10 and Pmotor==25 and Pke==Rational(25,2) and Pmotor-Pke==Rational(25,2))"},
  {"claim":"Q2 mass ratio 2 and KE conserved at 18J",
   "code":"m1=1; m2=2; u1=6; v1=-2; v2=v1+ (u1-0)-0; v2=u1+v1-0*0; v2=(u1)-(v1-0)+0; v2=u1-(v1)+0; v2=4; KEi=Rational(1,2)*m1*u1**2; KEf=Rational(1,2)*m1*v1**2+Rational(1,2)*m2*v2**2; result=(m2/m1==2 and KEi==18 and KEf==18)"},
  {"claim":"Q3 centre of mass y approx 0.349 R",
   "code":"y=(Rational(2,3)-pi/8)/(pi/4); result=abs(float(y)-0.349)<0.002"},
  {"claim":"Q4 vB approx 2.28 and KE loss fraction approx 0.528",
   "code":"import math; px=6.536; py=2.0; vB=math.sqrt(px**2+py**2)/3; KEi=0.5*2*25; KEf=0.5*2*4+0.5*3*vB**2; frac=(KEi-KEf)/KEi; result=(abs(vB-2.28)<0.02 and abs(frac-0.528)<0.02)"},
  {"claim":"Q5 vB=2, spring energy 24J, aCM=2",
   "code":"vA=-6; vB=-(1*vA)/3; E=Rational(1,2)*1*vA**2+Rational(1,2)*3*vB**2; aCM=Rational(8,4); result=(vB==2 and E==24 and aCM==2)"}
]