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A Level H1 Physics Mechanics Quiz

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Questions

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A-Level Physics H1 Quiz - Mechanics

Name: __________________________
Class: __________________________
Date: __________________________
Score: ________ / 45

Duration: 45 minutes
Total Marks: 45

Instructions:

  1. Answer all questions.
  2. Write your answers in the spaces provided.
  3. Show all working clearly. Numerical answers should be given to an appropriate number of significant figures.
  4. Take the acceleration of free fall g=9.81 m s2g = 9.81 \text{ m s}^{-2} unless otherwise stated.

Section A: Kinematics and Dynamics (Questions 1–5)

1. A car accelerates uniformly from rest to a speed of 24 m s124 \text{ m s}^{-1} in 6.0 s6.0 \text{ s}. It then travels at this constant speed for 10 s10 \text{ s} before decelerating uniformly to rest in 4.0 s4.0 \text{ s}.

(a) Calculate the acceleration of the car during the first 6.0 s6.0 \text{ s}.

<br><br><br> Answer: ____________________ m s2\text{m s}^{-2} [1]

(b) Calculate the total distance travelled by the car.

<br><br><br><br> Answer: ____________________ m\text{m} [2]

2. A stone is thrown horizontally from the top of a cliff with a speed of 15 m s115 \text{ m s}^{-1}. The cliff is 45 m45 \text{ m} high. Air resistance is negligible.

(a) Calculate the time taken for the stone to reach the ground.

<br><br><br> Answer: ____________________ s\text{s} [2]

(b) Calculate the horizontal distance from the base of the cliff where the stone lands.

<br><br> Answer: ____________________ m\text{m} [1]

3. State Newton’s Second Law of Motion in terms of momentum.

<br><br><br>


_________________________________________________________________________ [2]

4. A block of mass 5.0 kg5.0 \text{ kg} rests on a rough horizontal surface. A horizontal force of 20 N20 \text{ N} is applied to the block, causing it to accelerate at 2.0 m s22.0 \text{ m s}^{-2}.

Calculate the magnitude of the frictional force acting on the block.

<br><br><br> Answer: ____________________ N\text{N} [2]

5. Two trolleys, A and B, move along a straight frictionless track. Trolley A has mass 2.0 kg2.0 \text{ kg} and velocity 3.0 m s13.0 \text{ m s}^{-1} to the right. Trolley B has mass 1.0 kg1.0 \text{ kg} and velocity 2.0 m s12.0 \text{ m s}^{-1} to the left. They collide and stick together.

Calculate the common velocity of the trolleys after the collision. (Take right as positive).

<br><br><br><br> Answer: ____________________ m s1\text{m s}^{-1} [3]


Section B: Forces, Equilibrium, and Energy (Questions 6–12)

6. A uniform beam AB of length 4.0 m4.0 \text{ m} and weight 120 N120 \text{ N} is hinged at end A to a vertical wall. The beam is held horizontal by a cable attached to end B, which makes an angle of 3030^\circ with the beam.

(a) Draw a free-body diagram showing all forces acting on the beam. Label the forces clearly.

<br><br><br><br><br><br> [2]

(b) Calculate the tension in the cable.

<br><br><br><br> Answer: ____________________ N\text{N} [3]

7. Define the term work done by a force.

<br><br><br>


_________________________________________________________________________ [1]

8. A crane lifts a load of mass 500 kg500 \text{ kg} vertically upwards at a constant speed of 2.0 m s12.0 \text{ m s}^{-1}.

Calculate the power developed by the crane motor. (Ignore air resistance).

<br><br><br> Answer: ____________________ W\text{W} [2]

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

(a) Calculate the loss in gravitational potential energy during the fall and rebound process.

<br><br><br> Answer: ____________________ J\text{J} [2]

(b) Suggest what happens to the lost energy.

<br><br> _________________________________________________________________________ [1]

10. A car of mass 1200 kg1200 \text{ kg} travels up a slope inclined at 5.05.0^\circ to the horizontal at a constant speed of 20 m s120 \text{ m s}^{-1}. The resistive forces acting on the car total 400 N400 \text{ N}.

Calculate the driving force required to maintain this constant speed.

<br><br><br><br> Answer: ____________________ N\text{N} [3]

11. Explain why the principle of conservation of energy applies to a pendulum swinging in a vacuum, but not to one swinging in air.

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



_________________________________________________________________________ [2]

12. 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}.

Calculate the elastic potential energy stored in the spring when the extension is 5.0 cm5.0 \text{ cm}.

<br><br><br> Answer: ____________________ J\text{J} [2]


Section C: Momentum, Impulse, and Advanced Applications (Questions 13–20)

13. State the principle of conservation of linear momentum.

<br><br><br>


_________________________________________________________________________ [2]

14. A golf club strikes a stationary golf ball of mass 0.045 kg0.045 \text{ kg}. The club is in contact with the ball for 0.50 ms0.50 \text{ ms}. The ball leaves the club with a speed of 50 m s150 \text{ m s}^{-1}.

Calculate the average force exerted by the club on the ball.

<br><br><br><br> Answer: ____________________ N\text{N} [3]

15. Distinguish between an elastic collision and an inelastic collision in terms of kinetic energy.

<br><br><br>


_________________________________________________________________________ [2]

16. A particle of mass mm moves in a horizontal circle of radius rr with constant speed vv.

(a) State the direction of the resultant force acting on the particle.

<br> _________________________________________________________________________ [1]

(b) Derive the expression for the centripetal acceleration a=v2ra = \frac{v^2}{r}. (You may use vector diagrams or kinematic arguments).

<br><br><br><br><br><br> [3]

17. A box of mass 10 kg10 \text{ kg} is pushed across a horizontal floor by a force of 50 N50 \text{ N} acting at an angle of 3030^\circ below the horizontal. The coefficient of dynamic friction between the box and the floor is 0.200.20.

(a) Calculate the normal reaction force acting on the box.

<br><br><br> Answer: ____________________ N\text{N} [2]

(b) Calculate the acceleration of the box.

<br><br><br><br> Answer: ____________________ m s2\text{m s}^{-2} [3]

18. The graph below shows the variation of velocity vv with time tt for a falling object subject to air resistance.

(Imagine a graph starting at v=0, curving upwards with decreasing gradient, approaching a horizontal asymptote at vTv_T)

(a) Explain, in terms of forces, why the gradient of the graph decreases with time.

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


_________________________________________________________________________ [2]

(b) State the condition for the object to reach terminal velocity vTv_T.

<br> _________________________________________________________________________ [1]

19. A projectile is launched with speed uu at an angle θ\theta to the horizontal. Show that the maximum height HH reached is given by: H=u2sin2θ2gH = \frac{u^2 \sin^2 \theta}{2g}

<br><br><br><br><br><br> [3]

20. Two spheres, X and Y, undergo a head-on collision on a smooth surface.

  • Sphere X: mass 2m2m, initial velocity +u+u.
  • Sphere Y: mass mm, initial velocity u-u.

After the collision, sphere X moves with velocity +0.5u+0.5u.

(a) Calculate the velocity of sphere Y after the collision.

<br><br><br><br> Answer: ____________________ [3]

(b) Determine whether this collision is elastic or inelastic. Show your working.

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


_________________________________________________________________________ [3]


End of Quiz

Answers

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A-Level Physics H1 Quiz - Mechanics (Answer Key)

1. (a) a=vut=2406.0=4.0 m s2a = \frac{v - u}{t} = \frac{24 - 0}{6.0} = 4.0 \text{ m s}^{-2} [1] (b) Distance = Area under graph. Area 1 (triangle) = 12×6.0×24=72 m\frac{1}{2} \times 6.0 \times 24 = 72 \text{ m} Area 2 (rectangle) = 10×24=240 m10 \times 24 = 240 \text{ m} Area 3 (triangle) = 12×4.0×24=48 m\frac{1}{2} \times 4.0 \times 24 = 48 \text{ m} Total Distance = 72+240+48=360 m72 + 240 + 48 = 360 \text{ m} [2]

2. (a) Vertical motion: s=ut+12at2s = ut + \frac{1}{2}at^2. uy=0u_y = 0, a=g=9.81a = g = 9.81, s=45s = 45. 45=0+12(9.81)t245 = 0 + \frac{1}{2}(9.81)t^2 t2=909.81=9.174t^2 = \frac{90}{9.81} = 9.174 t=3.03 st = 3.03 \text{ s} (approx 3.0 s3.0 \text{ s}) [2] (b) Horizontal distance sx=uxt=15×3.03=45.45 ms_x = u_x t = 15 \times 3.03 = 45.45 \text{ m} (approx 45 m45 \text{ m}) [1]

3. The resultant force acting on an object is equal to the rate of change of its momentum. [1] Mathematically: F=ΔpΔtF = \frac{\Delta p}{\Delta t} or F=d(mv)dtF = \frac{d(mv)}{dt}. [1]

4. Resultant Force Fnet=ma=5.0×2.0=10 NF_{net} = ma = 5.0 \times 2.0 = 10 \text{ N}. [1] Fnet=FappliedFfrictionF_{net} = F_{applied} - F_{friction} 10=20Ffriction10 = 20 - F_{friction} Ffriction=10 NF_{friction} = 10 \text{ N} [1]

5. 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)(2.0)=(2.0+1.0)v(2.0)(3.0) + (1.0)(-2.0) = (2.0 + 1.0)v [1] 6.02.0=3.0v6.0 - 2.0 = 3.0v 4.0=3.0v4.0 = 3.0v v=+1.33 m s1v = +1.33 \text{ m s}^{-1} (to the right) [2]

6. (a) Diagram should show:

  • Weight WW acting downwards from the center of the beam. [1]
  • Tension TT acting from end B at 3030^\circ to the beam (upwards/left). [1]
  • Reaction force at hinge A (vertical/horizontal components or resultant). [Accept if implied or not explicitly asked to calculate, but good practice]. Note: Question asks for forces on beam. Weight and Tension are critical. (b) Take moments about hinge A. Clockwise Moment = Anticlockwise Moment W×(distance to center)=T×(length)W \times (\text{distance to center}) = T_{\perp} \times (\text{length}) 120×2.0=(Tsin30)×4.0120 \times 2.0 = (T \sin 30^\circ) \times 4.0 [1] 240=T(0.5)(4.0)240 = T(0.5)(4.0) 240=2.0T240 = 2.0 T T=120 NT = 120 \text{ N} [2]

7. Work done is the product of the force and the displacement moved in the direction of the force. [1] (W=FscosθW = F s \cos \theta)

8. Power P=FvP = F v. Since speed is constant, Driving Force F=Weight=mgF = \text{Weight} = mg. [1] F=500×9.81=4905 NF = 500 \times 9.81 = 4905 \text{ N} P=4905×2.0=9810 WP = 4905 \times 2.0 = 9810 \text{ W} (or 9.8 kW9.8 \text{ kW}) [1]

9. (a) Initial GPE =mgh1=0.20×9.81×2.0=3.924 J= mgh_1 = 0.20 \times 9.81 \times 2.0 = 3.924 \text{ J} Final GPE =mgh2=0.20×9.81×1.5=2.943 J= mgh_2 = 0.20 \times 9.81 \times 1.5 = 2.943 \text{ J} Loss =3.9242.943=0.981 J= 3.924 - 2.943 = 0.981 \text{ J} (approx 0.98 J0.98 \text{ J}) [2] (b) Energy is converted to thermal energy (heat) and sound upon impact with the ground / due to air resistance. [1]

10. Forces acting down the slope: Component of weight (mgsinθmg \sin \theta) + Resistive forces. Driving Force FDF_D acts up the slope. Since speed is constant, FD=mgsinθ+FresistF_D = mg \sin \theta + F_{resist}. [1] mgsin5.0=1200×9.81×sin5.0=1200×9.81×0.08716=1026 Nmg \sin 5.0^\circ = 1200 \times 9.81 \times \sin 5.0^\circ = 1200 \times 9.81 \times 0.08716 = 1026 \text{ N} [1] FD=1026+400=1426 NF_D = 1026 + 400 = 1426 \text{ N} (approx 1430 N1430 \text{ N}) [1]

11. In a vacuum, only gravity (conservative force) does work, so mechanical energy (KE + GPE) is conserved. [1] In air, air resistance (non-conservative force) does negative work, converting mechanical energy into thermal energy/heat, so total mechanical energy decreases. [1]

12. Spring constant k=Fx=100.05=200 N m1k = \frac{F}{x} = \frac{10}{0.05} = 200 \text{ N m}^{-1}. [1] Elastic PE E=12kx2=12(200)(0.05)2=100×0.0025=0.25 JE = \frac{1}{2} k x^2 = \frac{1}{2} (200) (0.05)^2 = 100 \times 0.0025 = 0.25 \text{ J}. (Alternatively E=12Fx=12(10)(0.05)=0.25 JE = \frac{1}{2} F x = \frac{1}{2} (10)(0.05) = 0.25 \text{ J}) [1]

13. In a closed/isolated system (no external forces), [1] the total linear momentum remains constant (or total momentum before collision = total momentum after collision). [1]

14. Impulse =Δp=m(vu)=0.045(500)=2.25 N s= \Delta p = m(v - u) = 0.045(50 - 0) = 2.25 \text{ N s}. [1] Impulse =FavgΔt= F_{avg} \Delta t 2.25=Favg×(0.50×103)2.25 = F_{avg} \times (0.50 \times 10^{-3}) [1] Favg=2.250.0005=4500 NF_{avg} = \frac{2.25}{0.0005} = 4500 \text{ N} [1]

15. In an elastic collision, total kinetic energy is conserved. [1] In an inelastic collision, total kinetic energy is not conserved (some is converted to other forms like heat/sound/deformation). [1]

16. (a) Towards the center of the circle. [1] (b) Consider velocity vectors v1\vec{v}_1 and v2\vec{v}_2 at times tt and t+Δtt+\Delta t. The change in velocity Δv\Delta \vec{v} points towards the center. Using similar triangles for velocity vector triangle and position triangle: Δvv=Δsr\frac{\Delta v}{v} = \frac{\Delta s}{r} Δv=vΔsr\Delta v = \frac{v \Delta s}{r} Divide by Δt\Delta t: ΔvΔt=vrΔsΔt\frac{\Delta v}{\Delta t} = \frac{v}{r} \frac{\Delta s}{\Delta t} As Δt0\Delta t \to 0, ΔvΔt=a\frac{\Delta v}{\Delta t} = a and ΔsΔt=v\frac{\Delta s}{\Delta t} = v. Therefore, a=v2ra = \frac{v^2}{r}. [3] (Award marks for logical steps/diagram)

17. (a) Resolve forces vertically. Upward forces = Downward forces. R=mg+Fsin30R = mg + F \sin 30^\circ [1] R=(10×9.81)+(50×0.5)=98.1+25=123.1 NR = (10 \times 9.81) + (50 \times 0.5) = 98.1 + 25 = 123.1 \text{ N} (approx 123 N123 \text{ N}) [1] (b) Frictional force Ff=μR=0.20×123.1=24.62 NF_f = \mu R = 0.20 \times 123.1 = 24.62 \text{ N}. Horizontal component of applied force Fx=Fcos30=50cos30=43.30 NF_x = F \cos 30^\circ = 50 \cos 30^\circ = 43.30 \text{ N}. Resultant horizontal force Fnet=FxFf=43.3024.62=18.68 NF_{net} = F_x - F_f = 43.30 - 24.62 = 18.68 \text{ N}. [1] a=Fnetm=18.6810=1.87 m s2a = \frac{F_{net}}{m} = \frac{18.68}{10} = 1.87 \text{ m s}^{-2} (approx 1.9 m s21.9 \text{ m s}^{-2}) [2]

18. (a) As speed increases, air resistance (drag) increases. [1] The resultant downward force (WeightDragWeight - Drag) decreases. Since F=maF=ma, acceleration (gradient) decreases. [1] (b) Air resistance equals weight (Resultant force is zero). [1]

19. At maximum height, vertical velocity vy=0v_y = 0. Initial vertical velocity uy=usinθu_y = u \sin \theta. Using v2=u2+2asv^2 = u^2 + 2as with a=ga = -g and s=Hs = H: 0=(usinθ)22gH0 = (u \sin \theta)^2 - 2gH [1] 2gH=u2sin2θ2gH = u^2 \sin^2 \theta [1] H=u2sin2θ2gH = \frac{u^2 \sin^2 \theta}{2g} [1]

20. (a) Conservation of Momentum: Pinitial=(2m)(u)+(m)(u)=2mumu=muP_{initial} = (2m)(u) + (m)(-u) = 2mu - mu = mu. Pfinal=(2m)(0.5u)+(m)(vY)=mu+mvYP_{final} = (2m)(0.5u) + (m)(v_Y) = mu + m v_Y. mu=mu+mvYmvY=0vY=0mu = mu + m v_Y \Rightarrow m v_Y = 0 \Rightarrow v_Y = 0. [3] (b) Check Kinetic Energy. KEinitial=12(2m)u2+12(m)(u)2=mu2+0.5mu2=1.5mu2KE_{initial} = \frac{1}{2}(2m)u^2 + \frac{1}{2}(m)(-u)^2 = mu^2 + 0.5mu^2 = 1.5mu^2. KEfinal=12(2m)(0.5u)2+12(m)(0)2=m(0.25u2)=0.25mu2KE_{final} = \frac{1}{2}(2m)(0.5u)^2 + \frac{1}{2}(m)(0)^2 = m(0.25u^2) = 0.25mu^2. KEinitialKEfinalKE_{initial} \neq KE_{final} (1.5mu2>0.25mu21.5mu^2 > 0.25mu^2). Therefore, the collision is inelastic. [3]