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A Level H1 Physics Practice Paper 5

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Questions

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TuitionGoWhere Exam Practice (AI) - Physics H1 A-Level

PRACTICE PAPER - VERSION 5

Subject: Physics
Level: H1 (8867)
Paper: Practice Paper (Mechanics Focus)
Duration: 1 hour 15 minutes
Total Marks: 60

Name: ________________________
Class: ________________________
Date: ________________________


Instructions to Candidates

  • Write your name, class, and date in the spaces provided.
  • Answer all questions.
  • You are advised to spend approximately 15 minutes on Section A and 60 minutes on Section B.
  • All working must be clearly shown.
  • Use g=9.81 m s2g = 9.81 \text{ m s}^{-2} unless otherwise stated.

Section A: Structured Questions

Answer all questions in this section. Each question carries marks as indicated.

1. State the principle of conservation of linear momentum.
[2]

<br> <br> <br>

2. A car of mass 1200 kg1200 \text{ kg} travels at a constant speed of 25 m s125 \text{ m s}^{-1} along a straight horizontal road. The driving force provided by the engine is 800 N800 \text{ N}.
(a) State the magnitude of the resistive forces acting on the car.
[1]

<br>

(b) Calculate the power developed by the engine.
[2]

<br> <br> <br>

3. A ball is thrown vertically upwards with an initial velocity of 15 m s115 \text{ m s}^{-1}. Air resistance is negligible.
(a) Calculate the maximum height reached by the ball.
[2]

<br> <br> <br>

(b) Sketch the velocity-time graph for the motion of the ball from the instant it is thrown until it returns to the starting height. Label the axes with appropriate values.
[2]

<br> <br> <br> <br>

4. Two trolleys, A and B, move along a smooth horizontal track. Trolley A has a mass of 2.0 kg2.0 \text{ kg} and moves with a velocity of 3.0 m s13.0 \text{ m s}^{-1} to the right. Trolley B has a mass of 1.0 kg1.0 \text{ kg} and is initially at rest. The trolleys collide and stick together.
Calculate the common velocity of the trolleys after the collision.
[3]

<br> <br> <br> <br>

5. A uniform plank AB of length 4.0 m4.0 \text{ m} and weight 200 N200 \text{ N} rests on two supports. Support X is at end A, and support Y is 1.0 m1.0 \text{ m} from end B. A boy of weight 400 N400 \text{ N} stands on the plank at a distance xx from A.
(a) Draw a free-body diagram showing all forces acting on the plank.
[2]

<br> <br> <br> <br> <br>

(b) Determine the maximum value of xx such that the plank does not tip over support Y.
[3]

<br> <br> <br> <br>

Section B: Data Interpretation and Problem Solving

Answer all questions in this section.

6. A student investigates the motion of a falling sphere using a data logger. The sphere is dropped from rest in a tall cylinder filled with oil. The graph below shows the variation of velocity vv with time tt.

(Imagine a graph where velocity increases rapidly at first, then the gradient decreases, eventually becoming horizontal at v=0.80 m s1v = 0.80 \text{ m s}^{-1})

(a) Describe and explain the shape of the graph in terms of the forces acting on the sphere.
[3]

<br> <br> <br> <br> <br>

(b) The mass of the sphere is 0.050 kg0.050 \text{ kg}. Calculate the drag force acting on the sphere when it reaches terminal velocity.
[2]

<br> <br> <br>

(c) Determine the initial acceleration of the sphere immediately after it is released.
[1]

<br> <br>

7. A block of mass 5.0 kg5.0 \text{ kg} is pulled up a rough inclined plane by a constant force FF parallel to the slope. The plane is inclined at 3030^\circ to the horizontal. The block moves at a constant speed. The frictional force acting on the block is 12 N12 \text{ N}.

(a) Draw a free-body diagram for the block, labeling all forces.
[2]

<br> <br> <br> <br> <br>

(b) Calculate the magnitude of the force FF.
[3]

<br> <br> <br> <br>

(c) The block moves a distance of 4.0 m4.0 \text{ m} up the slope. Calculate:
(i) the work done by the force FF.
[2]

<br> <br> <br>

(ii) the gain in gravitational potential energy of the block.
[2]

<br> <br> <br>

(iii) Explain why the work done by FF is greater than the gain in gravitational potential energy.
[1]

<br> <br>

8. A projectile is launched from ground level with an initial velocity of 40 m s140 \text{ m s}^{-1} at an angle of 3030^\circ to the horizontal. Air resistance is negligible.

(a) Calculate the horizontal and vertical components of the initial velocity.
[2]

<br> <br> <br>

(b) Calculate the time of flight of the projectile.
[3]

<br> <br> <br> <br>

(c) Calculate the horizontal range of the projectile.
[2]

<br> <br> <br>

9. Two ice skaters, P and Q, stand facing each other on frictionless ice. Skater P has a mass of 60 kg60 \text{ kg} and Skater Q has a mass of 80 kg80 \text{ kg}. They push against each other and move apart. Skater P moves with a velocity of 2.0 m s12.0 \text{ m s}^{-1} to the left.

(a) Calculate the velocity of Skater Q.
[3]

<br> <br> <br> <br>

(b) Calculate the total kinetic energy of the system after they push apart.
[3]

<br> <br> <br> <br>

(c) State the source of this kinetic energy.
[1]

<br> <br>

10. A crane lifts a load of mass 500 kg500 \text{ kg} vertically upwards from rest with a constant acceleration of 0.50 m s20.50 \text{ m s}^{-2}.

(a) Calculate the tension in the cable during the acceleration phase.
[3]

<br> <br> <br> <br>

(b) The load reaches a speed of 4.0 m s14.0 \text{ m s}^{-1}. Calculate the height gained during this acceleration.
[2]

<br> <br> <br>

(c) The crane then lifts the load at a constant speed of 4.0 m s14.0 \text{ m s}^{-1}. Calculate the power output of the crane motor during this constant speed phase.
[2]

<br> <br> <br>

11. A spring obeys Hooke's Law. When a force of 10 N10 \text{ N} is applied, the extension is 5.0 cm5.0 \text{ cm}.

(a) Calculate the spring constant kk.
[2]

<br> <br> <br>

(b) Calculate the elastic potential energy stored in the spring when the extension is 5.0 cm5.0 \text{ cm}.
[2]

<br> <br> <br>

(c) The spring is compressed by 10 cm10 \text{ cm} and used to launch a ball of mass 0.10 kg0.10 \text{ kg} horizontally. Assuming all elastic potential energy is converted to kinetic energy, calculate the launch speed of the ball.
[3]

<br> <br> <br> <br>

12. A car of mass 1000 kg1000 \text{ kg} travels around a horizontal circular bend of radius 50 m50 \text{ m}. The maximum frictional force between the tires and the road is 8000 N8000 \text{ N}.

(a) Identify the force that provides the centripetal acceleration.
[1]

<br>

(b) Calculate the maximum speed at which the car can travel around the bend without skidding.
[3]

<br> <br> <br> <br>

(c) Explain what happens if the car enters the bend at a speed higher than the maximum calculated in (b).
[2]

<br> <br> <br>

13. A ball of mass 0.20 kg0.20 \text{ kg} is dropped from a height of 2.0 m2.0 \text{ m} onto a hard floor. It rebounds to a height of 1.5 m1.5 \text{ m}.

(a) Calculate the speed of the ball just before it hits the floor.
[2]

<br> <br> <br>

(b) Calculate the speed of the ball just after it leaves the floor.
[2]

<br> <br> <br>

(c) Calculate the change in momentum of the ball during the impact with the floor.
[3]

<br> <br> <br> <br>

14. A uniform ladder of weight WW and length LL rests against a smooth vertical wall and on a rough horizontal ground. The ladder makes an angle θ\theta with the ground.

(a) Explain why the wall exerts only a horizontal force on the ladder.
[1]

<br> <br>

(b) By taking moments about the base of the ladder, derive an expression for the horizontal force exerted by the wall in terms of WW and θ\theta.
[3]

<br> <br> <br> <br> <br>

15. A rocket of mass 1000 kg1000 \text{ kg} (including fuel) is launched vertically. The engine produces a constant thrust of 15000 N15000 \text{ N}. The mass of the fuel burnt is negligible for this short duration.

(a) Calculate the initial acceleration of the rocket.
[3]

<br> <br> <br> <br>

(b) As the rocket rises, air resistance becomes significant. State and explain how the acceleration of the rocket changes as its speed increases.
[2]

<br> <br> <br>

16. A block of mass 2.0 kg2.0 \text{ kg} slides down a smooth curved track from a height of 3.0 m3.0 \text{ m} and onto a rough horizontal surface. The coefficient of kinetic friction between the block and the horizontal surface is 0.400.40.

(a) Calculate the speed of the block at the bottom of the curved track.
[2]

<br> <br> <br>

(b) Calculate the distance the block travels on the horizontal surface before coming to rest.
[3]

<br> <br> <br> <br>

17. Two forces, F1=10 NF_1 = 10 \text{ N} acting horizontally to the right, and F2=10 NF_2 = 10 \text{ N} acting at 6060^\circ above the horizontal to the right, act on a particle.

(a) Calculate the horizontal component of the resultant force.
[2]

<br> <br> <br>

(b) Calculate the vertical component of the resultant force.
[1]

<br> <br>

(c) Calculate the magnitude of the resultant force.
[2]

<br> <br> <br>

18. A satellite orbits the Earth in a circular orbit.

(a) State the direction of the resultant force acting on the satellite.
[1]

<br>

(b) Explain why the satellite is accelerating even though its speed is constant.
[2]

<br> <br> <br>

19. A student measures the acceleration of free fall gg using a free-fall apparatus. The time tt taken for a steel ball to fall a distance hh is recorded.

(a) State the equation relating hh, tt, and gg for an object falling from rest.
[1]

<br>

(b) The student plots a graph of hh against t2t^2. State what physical quantity is represented by the gradient of this graph.
[1]

<br>

(c) Suggest one source of systematic error in this experiment and how it affects the result.
[2]

<br> <br> <br>

20. A car accelerates uniformly from rest to 20 m s120 \text{ m s}^{-1} in 10 s10 \text{ s}. It then travels at this constant speed for 20 s20 \text{ s} before decelerating uniformly to rest in 5 s5 \text{ s}.

(a) Sketch the velocity-time graph for the entire journey.
[2]

<br> <br> <br> <br>

(b) Calculate the total distance traveled by the car.
[3]

<br> <br> <br> <br>

(c) Calculate the average speed for the entire journey.
[2]

<br> <br> <br>

End of Paper

Answers

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TuitionGoWhere Exam Practice (AI) - Physics H1 A-Level

PRACTICE PAPER - VERSION 5 - ANSWER KEY

Subject: Physics
Level: H1 (8867)
Total Marks: 60


Section A: Structured Questions

1. State the principle of conservation of linear momentum. [2]

  • Answer: In a closed system (or isolated system) [B1], the total momentum before interaction is equal to the total momentum after interaction (provided no external forces act) [B1].
  • Note: Accept "Total momentum remains constant if net external force is zero."

2. Car motion. [3]

  • (a) Resistive forces: Since speed is constant, acceleration is zero. By Newton's First Law, driving force = resistive force.
    • Answer: 800 N800 \text{ N} [B1]
  • (b) Power developed: P=FvP = Fv
    • Answer: P=800×25=20,000 WP = 800 \times 25 = 20,000 \text{ W} (or 20 kW20 \text{ kW}) [M1, A1]

3. Vertical projectile. [4]

  • (a) Max height: Using v2=u2+2asv^2 = u^2 + 2as. At max height, v=0v=0. u=15u=15, a=9.81a=-9.81.
    • 0=152+2(9.81)s0 = 15^2 + 2(-9.81)s
    • s=22519.62=11.47 ms = \frac{225}{19.62} = 11.47 \text{ m}
    • Answer: 11.5 m11.5 \text{ m} (3 s.f.) [M1, A1]
  • (b) Graph: Straight line with negative gradient starting at +15+15 on y-axis, crossing t-axis, ending at 15-15.
    • Answer: Linear slope downwards [B1]; Intercepts/correct shape indicated [B1].

4. Inelastic collision. [3]

  • Conservation of momentum: mAuA+mBuB=(mA+mB)vm_A u_A + m_B u_B = (m_A + m_B)v
    • (2.0)(3.0)+(1.0)(0)=(2.0+1.0)v(2.0)(3.0) + (1.0)(0) = (2.0 + 1.0)v
    • 6.0=3.0v6.0 = 3.0v
    • v=2.0 m s1v = 2.0 \text{ m s}^{-1}
    • Answer: 2.0 m s12.0 \text{ m s}^{-1} to the right [M1, M1, A1]

5. Plank equilibrium. [5]

  • (a) Free-body diagram:
    • Weight of plank (200 N200 \text{ N}) acting downwards at center (2.0 m2.0 \text{ m} from A). [B1]
    • Weight of boy (400 N400 \text{ N}) acting downwards at distance xx. [B1]
    • Reaction at X (RXR_X) upwards at A. [B1]
    • Reaction at Y (RYR_Y) upwards at 3.0 m3.0 \text{ m} from A. [B1]
    • (Note: Award marks for correct labels and directions)
  • (b) Max xx before tipping:
    • Condition for tipping: Reaction at X becomes zero (RX=0R_X = 0).
    • Take moments about support Y.
    • Clockwise moment = Anti-clockwise moment.
    • Weight of plank acts at 2.0 m2.0 \text{ m} from A. Support Y is at 3.0 m3.0 \text{ m} from A. Distance from Y to center = 1.0 m1.0 \text{ m}.
    • Moment of plank weight about Y: 200×1.0=200 N m200 \times 1.0 = 200 \text{ N m} (Anti-clockwise).
    • Moment of boy about Y: 400×(3.0x)400 \times (3.0 - x) (Clockwise, assuming boy is to the right of Y? No, boy is at xx. If x>3x > 3, moment is clockwise. If x<3x < 3, moment is anti-clockwise. Wait. To tip over Y, the boy must be to the right of Y, creating a clockwise moment that overcomes the plank's weight moment? No. The plank weight creates a moment trying to rotate it back down. The boy creates a moment trying to tip it.
    • Let's check positions: A(0), Center(2), Y(3), B(4).
    • Pivot at Y.
    • Plank weight (200 N200 \text{ N}) is at 2 m2 \text{ m} from A. Distance to Y = 1 m1 \text{ m} to the left. Moment = 200×1=200 Nm200 \times 1 = 200 \text{ Nm} (Counter-Clockwise).
    • Boy (400 N400 \text{ N}) is at xx. To tip, boy must be to the right of Y (x>3x > 3). Distance to Y = x3x - 3. Moment = 400(x3)400(x - 3) (Clockwise).
    • Equilibrium limit: 200=400(x3)200 = 400(x - 3)
    • 0.5=x30.5 = x - 3
    • x=3.5 mx = 3.5 \text{ m}
    • Answer: 3.5 m3.5 \text{ m} [M1, M1, A1]

Section B: Data Interpretation and Problem Solving

6. Falling sphere in oil. [6]

  • (a) Shape explanation:
    • Initially, velocity is zero, so drag is zero. Net force = weight. Acceleration is max (gg). [B1]
    • As velocity increases, drag force increases. Net force (WDW - D) decreases, so acceleration decreases. [B1]
    • Eventually, drag equals weight. Net force is zero. Acceleration is zero. Velocity becomes constant (terminal velocity). [B1]
  • (b) Drag at terminal velocity:
    • At terminal velocity, D=W=mgD = W = mg.
    • D=0.050×9.81=0.4905 ND = 0.050 \times 9.81 = 0.4905 \text{ N}.
    • Answer: 0.49 N0.49 \text{ N} [M1, A1]
  • (c) Initial acceleration:
    • At t=0t=0, v=0v=0, so Drag =0= 0.
    • Fnet=WF_{net} = W. ma=mga=gma = mg \Rightarrow a = g.
    • Answer: 9.81 m s29.81 \text{ m s}^{-2} [B1]

7. Block on inclined plane. [10]

  • (a) Free-body diagram:
    • Weight (mgmg) vertically down. [B1]
    • Normal reaction (NN) perpendicular to slope. [B1]
    • Friction (ff) down the slope (opposing motion). [B1]
    • Applied force (FF) up the slope. [B1]
  • (b) Calculate FF:
    • Resolve forces parallel to slope. Constant speed a=0\Rightarrow a=0.
    • F=mgsin(30)+fF = mg \sin(30^\circ) + f
    • F=(5.0)(9.81)(0.5)+12F = (5.0)(9.81)(0.5) + 12
    • F=24.525+12=36.525 NF = 24.525 + 12 = 36.525 \text{ N}
    • Answer: 36.5 N36.5 \text{ N} (3 s.f.) [M1, M1, A1]
  • (c) Work and Energy:
    • (i) Work done by FF: W=F×d=36.525×4.0=146.1 JW = F \times d = 36.525 \times 4.0 = 146.1 \text{ J}.
      • Answer: 146 J146 \text{ J} [M1, A1]
    • (ii) Gain in GPE: ΔPE=mgh\Delta PE = mgh. Height h=dsin(30)=4.0×0.5=2.0 mh = d \sin(30^\circ) = 4.0 \times 0.5 = 2.0 \text{ m}.
      • ΔPE=5.0×9.81×2.0=98.1 J\Delta PE = 5.0 \times 9.81 \times 2.0 = 98.1 \text{ J}.
      • Answer: 98.1 J98.1 \text{ J} [M1, A1]
    • (iii) Explanation: Work done by FF is used to increase GPE AND to do work against friction (dissipated as heat). [B1]

8. Projectile motion. [7]

  • (a) Components:
    • ux=40cos(30)=34.64 m s1u_x = 40 \cos(30^\circ) = 34.64 \text{ m s}^{-1}
    • uy=40sin(30)=20.0 m s1u_y = 40 \sin(30^\circ) = 20.0 \text{ m s}^{-1}
    • Answer: ux=34.6 m s1u_x = 34.6 \text{ m s}^{-1}, uy=20.0 m s1u_y = 20.0 \text{ m s}^{-1} [M1, A1]
  • (b) Time of flight:
    • Consider vertical motion. Displacement sy=0s_y = 0 (returns to ground).
    • sy=uyt+12ayt2s_y = u_y t + \frac{1}{2} a_y t^2
    • 0=20t4.905t20 = 20t - 4.905t^2
    • t(204.905t)=0t(20 - 4.905t) = 0
    • t=0t = 0 (start) or t=204.905=4.077 st = \frac{20}{4.905} = 4.077 \text{ s}
    • Answer: 4.08 s4.08 \text{ s} [M1, M1, A1]
  • (c) Horizontal range:
    • R=ux×t=34.64×4.077=141.2 mR = u_x \times t = 34.64 \times 4.077 = 141.2 \text{ m}
    • Answer: 141 m141 \text{ m} [M1, A1]

9. Ice skaters. [7]

  • (a) Velocity of Q:
    • Conservation of momentum. Initial P=0P = 0.
    • mPvP+mQvQ=0m_P v_P + m_Q v_Q = 0
    • (60)(2.0)+(80)(vQ)=0(60)(-2.0) + (80)(v_Q) = 0 (Taking right as positive, P moves left)
    • 120+80vQ=0-120 + 80 v_Q = 0
    • vQ=12080=1.5 m s1v_Q = \frac{120}{80} = 1.5 \text{ m s}^{-1}
    • Answer: 1.5 m s11.5 \text{ m s}^{-1} to the right [M1, M1, A1]
  • (b) Total KE:
    • KEP=12(60)(2.0)2=120 JKE_P = \frac{1}{2}(60)(2.0)^2 = 120 \text{ J}
    • KEQ=12(80)(1.5)2=90 JKE_Q = \frac{1}{2}(80)(1.5)^2 = 90 \text{ J}
    • Total KE=120+90=210 JKE = 120 + 90 = 210 \text{ J}
    • Answer: 210 J210 \text{ J} [M1, M1, A1]
  • (c) Source of energy:
    • Chemical potential energy from the skaters' muscles / Internal energy. [B1]

10. Crane lifting load. [7]

  • (a) Tension during acceleration:
    • Tmg=maT - mg = ma
    • T=m(g+a)=500(9.81+0.50)=500(10.31)T = m(g + a) = 500(9.81 + 0.50) = 500(10.31)
    • T=5155 NT = 5155 \text{ N}
    • Answer: 5160 N5160 \text{ N} (3 s.f.) [M1, M1, A1]
  • (b) Height gained:
    • v2=u2+2asv^2 = u^2 + 2as
    • 4.02=0+2(0.50)s4.0^2 = 0 + 2(0.50)s
    • 16=1.0ss=16 m16 = 1.0 s \Rightarrow s = 16 \text{ m}
    • Answer: 16 m16 \text{ m} [M1, A1]
  • (c) Power at constant speed:
    • At constant speed, T=mg=500×9.81=4905 NT = mg = 500 \times 9.81 = 4905 \text{ N}.
    • P=Fv=Tv=4905×4.0=19620 WP = Fv = T v = 4905 \times 4.0 = 19620 \text{ W}
    • Answer: 19.6 kW19.6 \text{ kW} [M1, A1]

11. Spring energy. [7]

  • (a) Spring constant:
    • F=kx10=k(0.05)F = kx \Rightarrow 10 = k(0.05)
    • k=100.05=200 N m1k = \frac{10}{0.05} = 200 \text{ N m}^{-1}
    • Answer: 200 N m1200 \text{ N m}^{-1} [M1, A1]
  • (b) Elastic PE:
    • EPE=12kx2=12(200)(0.05)2EPE = \frac{1}{2} k x^2 = \frac{1}{2}(200)(0.05)^2
    • EPE=100×0.0025=0.25 JEPE = 100 \times 0.0025 = 0.25 \text{ J}
    • Answer: 0.25 J0.25 \text{ J} [M1, A1]
  • (c) Launch speed:
    • EPE=KE0.25=12mv2EPE = KE \Rightarrow 0.25 = \frac{1}{2} m v^2
    • 0.25=12(0.10)v20.25 = \frac{1}{2}(0.10)v^2
    • 0.5=0.10v2v2=50.5 = 0.10 v^2 \Rightarrow v^2 = 5
    • v=5=2.236 m s1v = \sqrt{5} = 2.236 \text{ m s}^{-1}
    • Answer: 2.24 m s12.24 \text{ m s}^{-1} [M1, M1, A1]

12. Circular motion. [6]

  • (a) Centripetal force source:
    • Friction between tires and road. [B1]
  • (b) Max speed:
    • Fc=mv2rF_c = \frac{mv^2}{r}
    • Ffriction=mv2r8000=1000v250F_{friction} = \frac{mv^2}{r} \Rightarrow 8000 = \frac{1000 v^2}{50}
    • 8000=20v28000 = 20 v^2
    • v2=400v=20 m s1v^2 = 400 \Rightarrow v = 20 \text{ m s}^{-1}
    • Answer: 20 m s120 \text{ m s}^{-1} [M1, M1, A1]
  • (c) Skidding explanation:
    • Required centripetal force exceeds maximum static friction. The car cannot maintain the circular path and moves in a straighter line (tangentially/outwards) relative to the curve. [B1, B1]

13. Impact momentum. [7]

  • (a) Speed before impact:
    • v2=u2+2as=0+2(9.81)(2.0)=39.24v^2 = u^2 + 2as = 0 + 2(9.81)(2.0) = 39.24
    • v=39.24=6.264 m s1v = \sqrt{39.24} = 6.264 \text{ m s}^{-1}
    • Answer: 6.26 m s16.26 \text{ m s}^{-1} [M1, A1]
  • (b) Speed after impact:
    • Rebound height 1.5 m1.5 \text{ m}. At top, v=0v=0.
    • 0=urebound22(9.81)(1.5)0 = u_{rebound}^2 - 2(9.81)(1.5)
    • urebound=29.43=5.425 m s1u_{rebound} = \sqrt{29.43} = 5.425 \text{ m s}^{-1}
    • Answer: 5.43 m s15.43 \text{ m s}^{-1} [M1, A1]
  • (c) Change in momentum:
    • Take Up as positive.
    • pinitial=0.20×(6.264)=1.253 N sp_{initial} = 0.20 \times (-6.264) = -1.253 \text{ N s}
    • pfinal=0.20×(+5.425)=+1.085 N sp_{final} = 0.20 \times (+5.425) = +1.085 \text{ N s}
    • Δp=pfpi=1.085(1.253)=2.338 N s\Delta p = p_f - p_i = 1.085 - (-1.253) = 2.338 \text{ N s}
    • Answer: 2.34 N s2.34 \text{ N s} (upwards) [M1, M1, A1]

14. Ladder moments. [4]

  • (a) Smooth wall:
    • Smooth surface cannot exert friction. Therefore, the reaction force is perpendicular to the surface (horizontal). [B1]
  • (b) Derivation:
    • Take moments about the base (point of contact with ground).
    • Let RwR_w be the horizontal force from the wall.
    • Moment of RwR_w: Force ×\times perpendicular distance. Vertical height of contact = LsinθL \sin \theta.
    • Moment = Rw(Lsinθ)R_w (L \sin \theta) (Clockwise/Anti-clockwise depending on side, let's say CW).
    • Moment of Weight WW: Acts at center (L/2L/2). Perpendicular distance from base = L2cosθ\frac{L}{2} \cos \theta.
    • Moment = W(L2cosθ)W (\frac{L}{2} \cos \theta) (Opposite direction).
    • Equilibrium: RwLsinθ=WL2cosθR_w L \sin \theta = W \frac{L}{2} \cos \theta
    • Rw=Wcosθ2sinθ=W2tanθR_w = \frac{W \cos \theta}{2 \sin \theta} = \frac{W}{2 \tan \theta}
    • Answer: Rw=W2tanθR_w = \frac{W}{2 \tan \theta} [M1, M1, A1]

15. Rocket launch. [5]

  • (a) Initial acceleration:
    • Fnet=ThrustWeightF_{net} = Thrust - Weight
    • Fnet=15000(1000)(9.81)=150009810=5190 NF_{net} = 15000 - (1000)(9.81) = 15000 - 9810 = 5190 \text{ N}
    • a=Fnetm=51901000=5.19 m s2a = \frac{F_{net}}{m} = \frac{5190}{1000} = 5.19 \text{ m s}^{-2}
    • Answer: 5.19 m s25.19 \text{ m s}^{-2} [M1, M1, A1]
  • (b) Effect of air resistance:
    • As speed increases, air resistance (drag) increases. [B1]
    • This reduces the net upward force (ThrustWeightDragThrust - Weight - Drag), so acceleration decreases. [B1]

16. Curved track and friction. [5]

  • (a) Speed at bottom:
    • Conservation of Energy: PEtop=KEbottomPE_{top} = KE_{bottom}
    • mgh=12mv2v=2ghmgh = \frac{1}{2}mv^2 \Rightarrow v = \sqrt{2gh}
    • v=2(9.81)(3.0)=58.86=7.672 m s1v = \sqrt{2(9.81)(3.0)} = \sqrt{58.86} = 7.672 \text{ m s}^{-1}
    • Answer: 7.67 m s17.67 \text{ m s}^{-1} [M1, A1]
  • (b) Distance on rough surface:
    • Work done by friction = Loss in KE
    • fkd=12mv2f_k d = \frac{1}{2}mv^2
    • Friction force fk=μN=μmg=0.40×2.0×9.81=7.848 Nf_k = \mu N = \mu mg = 0.40 \times 2.0 \times 9.81 = 7.848 \text{ N}
    • KEbottom=12(2.0)(7.672)2=58.86 JKE_{bottom} = \frac{1}{2}(2.0)(7.672)^2 = 58.86 \text{ J} (Matches initial PE)
    • 7.848d=58.867.848 d = 58.86
    • d=58.867.848=7.5 md = \frac{58.86}{7.848} = 7.5 \text{ m}
    • Answer: 7.5 m7.5 \text{ m} [M1, M1, A1]

17. Vector addition. [5]

  • (a) Horizontal component:
    • F1x=10 NF_{1x} = 10 \text{ N}
    • F2x=10cos(60)=5 NF_{2x} = 10 \cos(60^\circ) = 5 \text{ N}
    • Rx=10+5=15 NR_x = 10 + 5 = 15 \text{ N}
    • Answer: 15 N15 \text{ N} [M1, A1]
  • (b) Vertical component:
    • F1y=0F_{1y} = 0
    • F2y=10sin(60)=8.66 NF_{2y} = 10 \sin(60^\circ) = 8.66 \text{ N}
    • Ry=8.66 NR_y = 8.66 \text{ N}
    • Answer: 8.66 N8.66 \text{ N} [B1]
  • (c) Resultant magnitude:
    • R=Rx2+Ry2=152+8.662=225+75=300R = \sqrt{R_x^2 + R_y^2} = \sqrt{15^2 + 8.66^2} = \sqrt{225 + 75} = \sqrt{300}
    • R=17.32 NR = 17.32 \text{ N}
    • Answer: 17.3 N17.3 \text{ N} [M1, A1]

18. Satellite orbit. [3]

  • (a) Direction of force:
    • Towards the center of the Earth. [B1]
  • (b) Acceleration explanation:
    • Velocity is a vector (speed and direction). [B1]
    • Although speed is constant, the direction of motion is constantly changing. Therefore, velocity is changing, which means there is acceleration. [B1]

19. Free fall experiment. [4]

  • (a) Equation:
    • h=12gt2h = \frac{1}{2}gt^2 [B1]
  • (b) Gradient:
    • Graph of hh (y) vs t2t^2 (x). Equation y=(12g)xy = (\frac{1}{2}g)x.
    • Gradient = 12g\frac{1}{2}g [B1]
  • (c) Systematic error:
    • Example: Delay in timer starting (electromagnet release time). [B1]
    • Effect: Measured time tt is larger than actual fall time. Calculated gg will be smaller than actual gg (since g1/t2g \propto 1/t^2). [B1]
    • Alternative: Air resistance. Effect: gg calculated is lower.

20. Velocity-time graph journey. [7]

  • (a) Sketch:
    • 0-10s: Straight line from (0,0)(0,0) to (10,20)(10,20). [B1]
    • 10-30s: Horizontal line at v=20v=20. [B1]
    • 30-35s: Straight line from (30,20)(30,20) to (35,0)(35,0). [B1] (Shape correct)
  • (b) Total distance:
    • Area under graph.
    • Area 1 (Triangle): 12×10×20=100 m\frac{1}{2} \times 10 \times 20 = 100 \text{ m}
    • Area 2 (Rectangle): 20×20=400 m20 \times 20 = 400 \text{ m}
    • Area 3 (Triangle): 12×5×20=50 m\frac{1}{2} \times 5 \times 20 = 50 \text{ m}
    • Total = 100+400+50=550 m100 + 400 + 50 = 550 \text{ m}
    • Answer: 550 m550 \text{ m} [M1, M1, A1]
  • (c) Average speed:
    • Avg Speed = Total Distance / Total Time
    • Total Time = 10+20+5=35 s10 + 20 + 5 = 35 \text{ s}
    • Avg Speed = 55035=15.71 m s1\frac{550}{35} = 15.71 \text{ m s}^{-1}
    • Answer: 15.7 m s115.7 \text{ m s}^{-1} [M1, A1]