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A Level H2 Physics Practice Paper 1

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Questions

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TuitionGoWhere Practice Paper - Physics H2 A-Level

TuitionGoWhere Practice Paper (AI)

Subject: Physics H2
Level: A-Level
Paper: Practice Paper 1 (Version 1 of 5)
Topic Focus: Mechanics (Newtonian Mechanics, Energy, Momentum, Circular Motion)
Duration: 1 hour 30 minutes
Total Marks: 60

Name: __________________________
Class: __________________________
Date: __________________________


Instructions to Candidates

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

Section A: Structured Questions (40 Marks)

1. A car of mass 1200 kg1200 \text{ kg} travels along a straight horizontal road. The engine provides a constant driving force of 2400 N2400 \text{ N}. The total resistive force acting on the car is proportional to its speed vv, given by Fresist=kvF_{resist} = kv, where kk is a constant.

(a) The car reaches a terminal speed of 40 m s140 \text{ m s}^{-1}. Calculate the value of the constant kk.
[2]

<br> <br> <br>

(b) Calculate the initial acceleration of the car when it starts from rest.
[2]

<br> <br> <br>

(c) Explain, in terms of forces, why the acceleration of the car decreases as its speed increases.
[2]

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

2. A ball of mass 0.15 kg0.15 \text{ kg} is thrown vertically upwards with an initial speed of 12 m s112 \text{ m s}^{-1} from ground level. Air resistance is negligible.

(a) Calculate the maximum height reached by the ball.
[2]

<br> <br> <br>

(b) Determine the time taken for the ball to return to the ground.
[2]

<br> <br> <br>

(c) On the axes below, sketch the variation with time tt of the kinetic energy EkE_k of the ball from the moment it is thrown until it returns to the ground. Label the maximum value on the energy axis.
[3]

      E_k / J
        |
        |
        |
        |
        |
        |
        |________________________ t / s
        0

3. Two trolleys, A and B, move along a frictionless 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. They collide and stick together.

(a) State the principle of conservation of linear momentum.
[2]

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

(b) Calculate the common velocity of the trolleys after the collision.
[2]

<br> <br> <br>

(c) Determine the loss in kinetic energy during the collision.
[3]

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

4. A satellite orbits the Earth in a circular orbit of radius RR. The mass of the Earth is MM and the mass of the satellite is mm.

(a) Show that the orbital speed vv of the satellite is given by v=GMRv = \sqrt{\frac{GM}{R}}, where GG is the gravitational constant.
[3]

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

(b) The satellite moves to a higher circular orbit. State and explain the effect on: (i) the orbital speed of the satellite,
[2]

<br> <br> <br>
(ii) the total mechanical energy of the satellite.  
[2]
<br> <br> <br>

5. A simple pendulum consists of a bob of mass 0.50 kg0.50 \text{ kg} attached to a light inextensible string of length 1.2 m1.2 \text{ m}. The bob is pulled aside until the string makes an angle of 3030^\circ with the vertical and is released from rest.

(a) Calculate the change in gravitational potential energy of the bob as it moves from the release point to the lowest point of its swing.
[3]

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

(b) Calculate the speed of the bob at the lowest point of its swing.
[2]

<br> <br> <br>

(c) At the lowest point, calculate the tension in the string.
[3]

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

6. A cyclist travels around a horizontal circular bend of radius 25 m25 \text{ m}. The coefficient of static friction between the tires and the road is 0.800.80.

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

<br>

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

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

(c) The cyclist leans inwards while turning. Explain why leaning is necessary for stability.
[2]

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

Section B: Data-Based and Contextual Questions (20 Marks)

7. A student investigates the relationship between the extension xx of a spring and the load FF applied to it. The spring obeys Hooke's Law up to its limit of proportionality. The student obtains the following data:

Load FF / NExtension xx / cm
0.00.0
2.01.2
4.02.4
6.03.6
8.04.8
10.06.5
12.09.0

(a) Plot a graph of FF (y-axis) against xx (x-axis) on the grid below. Draw the line of best fit for the linear region.
[4]

      F / N
   12 |
      |
   10 |
      |
    8 |
      |
    6 |
      |
    4 |
      |
    2 |
      |
    0 |________________________________________ x / cm
      0    2    4    6    8    10   12

(b) Determine the spring constant kk of the spring.
[2]

<br> <br> <br>

(c) Estimate the elastic potential energy stored in the spring when the load is 8.0 N8.0 \text{ N}.
[2]

<br> <br> <br>

(d) Explain why the graph deviates from a straight line for loads greater than 8.0 N8.0 \text{ N}.
[2]

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

8. A projectile is launched from the top of a cliff 45 m45 \text{ m} high with an initial velocity of 20 m s120 \text{ m s}^{-1} at an angle of 3030^\circ above the horizontal. Air resistance is negligible.

(a) Calculate the time taken for the projectile to hit the ground.
[4]

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

(b) Calculate the horizontal distance from the base of the cliff to the point where the projectile lands.
[2]

<br> <br> <br>

(c) Determine the magnitude of the velocity of the projectile just before it hits the ground.
[4]

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

9. In a game of billiards, a white ball of mass mm moving with speed uu collides elastically with a stationary red ball of equal mass mm. After the collision, the white ball moves off at an angle of 3030^\circ to its original direction.

(a) State two quantities that are conserved in this elastic collision.
[2]

<br> <br>

(b) Show that the red ball moves off at an angle of 6060^\circ to the original direction of the white ball.
[3]

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

(c) If the initial speed uu was 2.0 m s12.0 \text{ m s}^{-1}, calculate the speed of the red ball after the collision.
[3]

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

10. A block of mass 5.0 kg5.0 \text{ kg} rests on a rough inclined plane that makes an angle of 2020^\circ with the horizontal. A force PP acts parallel to the plane and up the slope. The coefficient of dynamic friction between the block and the plane is 0.300.30.

(a) Calculate the component of the weight of the block acting down the slope.
[2]

<br> <br> <br>

(b) Calculate the normal reaction force acting on the block.
[2]

<br> <br> <br>

(c) The block is pulled up the slope at a constant speed. Calculate the magnitude of the force PP.
[3]

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

(d) The force PP is increased so that the block accelerates up the slope at 1.5 m s21.5 \text{ m s}^{-2}. Calculate the new value of PP.
[3]

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

Answers

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TuitionGoWhere Practice Paper - Physics H2 A-Level

Answer Key and Marking Scheme Version 1

Total Marks: 60


Section A: Structured Questions

1. Car Motion with Resistive Force

(a) At terminal speed, acceleration is zero, so driving force equals resistive force.
Fdrive=Fresist=kvF_{drive} = F_{resist} = kv
2400=k(40)2400 = k(40)
k=240040=60 N s m1k = \frac{2400}{40} = 60 \text{ N s m}^{-1} (or kg s1\text{kg s}^{-1})
[2 marks]: 1 for correct equation, 1 for correct answer with units.

(b) At start (v=0v=0), resistive force Fresist=k(0)=0F_{resist} = k(0) = 0.
Resultant force Fnet=Fdrive=2400 NF_{net} = F_{drive} = 2400 \text{ N}.
Fnet=ma2400=1200aF_{net} = ma \Rightarrow 2400 = 1200 a
a=2.0 m s2a = 2.0 \text{ m s}^{-2}
[2 marks]: 1 for identifying net force, 1 for correct answer.

(c) As speed vv increases, the resistive force Fresist=kvF_{resist} = kv increases.
The driving force is constant.
Therefore, the resultant force (FdriveFresistF_{drive} - F_{resist}) decreases.
Since a=Fnet/ma = F_{net}/m, the acceleration decreases.
[2 marks]: 1 for linking speed to increased resistive force, 1 for linking reduced net force to reduced acceleration.

2. Vertical Projectile Motion

(a) Using conservation of energy or kinematics:
v2=u2+2asv^2 = u^2 + 2as
At max height, v=0v=0, a=9.81 m s2a = -9.81 \text{ m s}^{-2}, u=12 m s1u = 12 \text{ m s}^{-1}.
0=122+2(9.81)h0 = 12^2 + 2(-9.81)h
19.62h=14419.62 h = 144
h=7.34 mh = 7.34 \text{ m}
[2 marks]: 1 for correct substitution, 1 for correct answer (7.34 or 7.35 m).

(b) Time to reach max height: v=u+at0=129.81tuptup=1.223 sv = u + at \Rightarrow 0 = 12 - 9.81 t_{up} \Rightarrow t_{up} = 1.223 \text{ s}.
Total time T=2×tup=2.45 sT = 2 \times t_{up} = 2.45 \text{ s}.
(Alternatively using s=ut+12at2s = ut + \frac{1}{2}at^2 with s=0s=0).
[2 marks]: 1 for method, 1 for correct answer (2.45 s).

(c) Graph shape: Parabola opening upwards (since Ekv2E_k \propto v^2 and vv varies linearly with tt, EkE_k is quadratic).

  • Starts at max value at t=0t=0.
  • Zero at t=1.22 st = 1.22 \text{ s} (halfway).
  • Returns to max value at t=2.45 st = 2.45 \text{ s}.
  • Symmetric about the time axis midpoint.
    Max Ek=12mv2=0.5(0.15)(122)=10.8 JE_k = \frac{1}{2}mv^2 = 0.5(0.15)(12^2) = 10.8 \text{ J}.
    [3 marks]: 1 for correct shape (U-shaped/parabolic), 1 for touching zero axis at midpoint, 1 for labeling max energy approx 10.8 J.

3. Inelastic Collision

(a) In a closed system (no external forces), the total momentum before collision equals the total momentum after collision.
[2 marks]: 1 for "closed system/no external forces", 1 for "total momentum constant/before=after".

(b) 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 = 3.0 v
v=2.0 m s1v = 2.0 \text{ m s}^{-1}
[2 marks]: 1 for correct equation, 1 for correct answer.

(c) Initial KE: KEi=12mAuA2=0.5(2.0)(3.02)=9.0 JKE_i = \frac{1}{2} m_A u_A^2 = 0.5(2.0)(3.0^2) = 9.0 \text{ J}.
Final KE: KEf=12(mA+mB)v2=0.5(3.0)(2.02)=6.0 JKE_f = \frac{1}{2} (m_A+m_B) v^2 = 0.5(3.0)(2.0^2) = 6.0 \text{ J}.
Loss in KE =9.06.0=3.0 J= 9.0 - 6.0 = 3.0 \text{ J}.
[3 marks]: 1 for initial KE, 1 for final KE, 1 for correct difference.

4. Satellite Orbit

(a) Gravitational force provides centripetal force:
GMmR2=mv2R\frac{GMm}{R^2} = \frac{mv^2}{R}
Cancel mm and one RR:
GMR=v2\frac{GM}{R} = v^2
v=GMRv = \sqrt{\frac{GM}{R}}
[3 marks]: 1 for equating forces, 1 for algebraic steps, 1 for final result.

(b) (i) Orbital speed decreases. Since v1Rv \propto \frac{1}{\sqrt{R}}, as RR increases, vv decreases.
[2 marks]: 1 for "decreases", 1 for explanation using formula.

(ii) Total mechanical energy increases (becomes less negative).
Work must be done against gravity to move to a higher orbit, increasing potential energy more than kinetic energy decreases.
Etotal=GMm2RE_{total} = -\frac{GMm}{2R}. As RR increases, EtotalE_{total} becomes closer to 0 (increases).
[2 marks]: 1 for "increases", 1 for explanation.

5. Simple Pendulum

(a) Vertical height change h=LLcosθ=L(1cosθ)h = L - L \cos \theta = L(1 - \cos \theta).
h=1.2(1cos30)=1.2(10.866)=1.2(0.134)=0.1608 mh = 1.2 (1 - \cos 30^\circ) = 1.2 (1 - 0.866) = 1.2(0.134) = 0.1608 \text{ m}.
ΔPE=mgh=0.50×9.81×0.1608=0.789 J\Delta PE = mgh = 0.50 \times 9.81 \times 0.1608 = 0.789 \text{ J}.
[3 marks]: 1 for height calculation, 1 for formula, 1 for answer (0.79 J).

(b) Conservation of energy: ΔPE=ΔKE\Delta PE = \Delta KE.
0.789=12mv20.789 = \frac{1}{2} m v^2
v2=2×0.7890.50=3.156v^2 = \frac{2 \times 0.789}{0.50} = 3.156
v=1.78 m s1v = 1.78 \text{ m s}^{-1}
[2 marks]: 1 for substitution, 1 for answer.

(c) At lowest point, forces are Tension (TT) up and Weight (mgmg) down. Resultant force is centripetal.
Tmg=mv2LT - mg = \frac{mv^2}{L}
T=mg+mv2L=(0.50)(9.81)+0.50(1.782)1.2T = mg + \frac{mv^2}{L} = (0.50)(9.81) + \frac{0.50(1.78^2)}{1.2}
T=4.905+1.5841.2=4.905+1.32=6.225 NT = 4.905 + \frac{1.584}{1.2} = 4.905 + 1.32 = 6.225 \text{ N}.
[3 marks]: 1 for correct force equation, 1 for substitution, 1 for answer (6.23 N).

6. Circular Motion (Cyclist)

(a) Frictional force between tires and road.
[1 mark]

(b) Max friction provides centripetal force:
Ffric=μR=μmgF_{fric} = \mu R = \mu mg
mv2r=μmg\frac{mv^2}{r} = \mu mg
v2=μgrv^2 = \mu g r
v=0.80×9.81×25=196.2=14.0 m s1v = \sqrt{0.80 \times 9.81 \times 25} = \sqrt{196.2} = 14.0 \text{ m s}^{-1}.
[3 marks]: 1 for equation setup, 1 for substitution, 1 for answer.

(c) Leaning creates a horizontal component of the normal reaction force (or torque balance) that provides the necessary centripetal force/moment to prevent toppling outwards. It aligns the resultant force of gravity and normal reaction through the center of mass.
[2 marks]: 1 for mentioning torque/moment or component of force, 1 for stability/preventing toppling.


Section B: Data-Based and Contextual Questions

7. Spring Experiment

(a) Graph:

  • Points plotted correctly.
  • Straight line drawn through origin up to (8.0, 4.8).
  • Curve drawn for points beyond 8.0 N.
    [4 marks]: 1 for axes labels/units, 1 for all points correct, 1 for linear fit, 1 for curve at end.

(b) Gradient of linear section:
k=ΔFΔx=8.000.0480=166.67 N m1k = \frac{\Delta F}{\Delta x} = \frac{8.0 - 0}{0.048 - 0} = 166.67 \text{ N m}^{-1}.
k167 N m1k \approx 167 \text{ N m}^{-1}.
[2 marks]: 1 for gradient method, 1 for answer (167 N/m). Note: x must be in meters.

(c) Energy = Area under graph up to 8.0 N.
E=12Fx=0.5×8.0×0.048=0.192 JE = \frac{1}{2} F x = 0.5 \times 8.0 \times 0.048 = 0.192 \text{ J}.
[2 marks]: 1 for formula/area concept, 1 for answer.

(d) The limit of proportionality has been exceeded. The spring undergoes plastic deformation or the material structure is changing, so Hooke's Law no longer applies.
[2 marks]: 1 for "limit of proportionality exceeded", 1 for elaboration.

8. Projectile from Cliff

(a) Vertical motion:
sy=45 ms_y = -45 \text{ m} (down is negative), uy=20sin30=10 m s1u_y = 20 \sin 30^\circ = 10 \text{ m s}^{-1}, ay=9.81 m s2a_y = -9.81 \text{ m s}^{-2}.
s=ut+12at2s = ut + \frac{1}{2}at^2
45=10t4.905t2-45 = 10t - 4.905t^2
4.905t210t45=04.905t^2 - 10t - 45 = 0
Using quadratic formula: t=10±1004(4.905)(45)2(4.905)t = \frac{10 \pm \sqrt{100 - 4(4.905)(-45)}}{2(4.905)}
t=10±100+882.99.81=10±31.359.81t = \frac{10 \pm \sqrt{100 + 882.9}}{9.81} = \frac{10 \pm 31.35}{9.81}
Positive root: t=41.359.81=4.215 st = \frac{41.35}{9.81} = 4.215 \text{ s}.
[4 marks]: 1 for resolving uyu_y, 1 for correct equation, 1 for quadratic handling, 1 for answer (4.22 s).

(b) Horizontal motion:
ux=20cos30=17.32 m s1u_x = 20 \cos 30^\circ = 17.32 \text{ m s}^{-1}.
Distance =ux×t=17.32×4.215=73.0 m= u_x \times t = 17.32 \times 4.215 = 73.0 \text{ m}.
[2 marks]: 1 for uxu_x, 1 for distance calculation.

(c) Vertical velocity at impact:
vy=uy+at=10+(9.81)(4.215)=1041.35=31.35 m s1v_y = u_y + at = 10 + (-9.81)(4.215) = 10 - 41.35 = -31.35 \text{ m s}^{-1}.
Horizontal velocity vx=17.32 m s1v_x = 17.32 \text{ m s}^{-1} (constant).
Magnitude v=vx2+vy2=17.322+(31.35)2v = \sqrt{v_x^2 + v_y^2} = \sqrt{17.32^2 + (-31.35)^2}
v=299.98+982.82=1282.8=35.8 m s1v = \sqrt{299.98 + 982.82} = \sqrt{1282.8} = 35.8 \text{ m s}^{-1}.
[4 marks]: 1 for vyv_y calc, 1 for stating vxv_x, 1 for Pythagorean combination, 1 for answer.

9. Elastic Collision (Billiards)

(a) 1. Kinetic Energy. 2. Linear Momentum.
[2 marks]: 1 for each.

(b) For equal masses in elastic collision, the angle between final velocity vectors is 9090^\circ.
Alternatively, use conservation equations:
x-mom: mu=mv1cos30+mv2cosθmu = mv_1 \cos 30 + mv_2 \cos \theta
y-mom: 0=mv1sin30mv2sinθ0 = mv_1 \sin 30 - mv_2 \sin \theta
KE: u2=v12+v22u^2 = v_1^2 + v_2^2
From vector triangle, since u2=v12+v22u^2 = v_1^2 + v_2^2, the triangle is right-angled.
Thus 30+θ=90θ=6030^\circ + \theta = 90^\circ \Rightarrow \theta = 60^\circ.
[3 marks]: 1 for citing equal mass/elastic property or equations, 1 for logical deduction of 90 deg separation, 1 for final angle.

(c) From the right-angled velocity vector triangle:
vred=usin30v_{red} = u \sin 30^\circ (component opposite to white ball's angle? No, geometry: vwhitev_{white} is adjacent to 30, vredv_{red} is opposite? Let's check).
Vector sum u=v1+v2\vec{u} = \vec{v}_1 + \vec{v}_2.
Angle of v1\vec{v}_1 is 30 to u\vec{u}. Angle of v2\vec{v}_2 is 60 to u\vec{u}.
vred=ucos60v_{red} = u \cos 60^\circ or usin30u \sin 30^\circ.
vred=2.0×0.5=1.0 m s1v_{red} = 2.0 \times 0.5 = 1.0 \text{ m s}^{-1}.
[3 marks]: 1 for correct trigonometric relation, 1 for substitution, 1 for answer.

10. Inclined Plane

(a) Component down slope =mgsinθ= mg \sin \theta.
Wparallel=5.0×9.81×sin20=49.05×0.342=16.78 NW_{parallel} = 5.0 \times 9.81 \times \sin 20^\circ = 49.05 \times 0.342 = 16.78 \text{ N}.
[2 marks]: 1 for formula, 1 for answer (16.8 N).

(b) Normal reaction R=mgcosθR = mg \cos \theta.
R=5.0×9.81×cos20=49.05×0.940=46.1 NR = 5.0 \times 9.81 \times \cos 20^\circ = 49.05 \times 0.940 = 46.1 \text{ N}.
[2 marks]: 1 for formula, 1 for answer.

(c) Constant speed means equilibrium. Forces up slope = Forces down slope.
P=Wparallel+FfrictionP = W_{parallel} + F_{friction}
Ffriction=μR=0.30×46.1=13.83 NF_{friction} = \mu R = 0.30 \times 46.1 = 13.83 \text{ N}.
P=16.78+13.83=30.61 NP = 16.78 + 13.83 = 30.61 \text{ N}.
[3 marks]: 1 for friction calc, 1 for equilibrium equation, 1 for answer (30.6 N).

(d) Newton's 2nd Law: Fnet=maF_{net} = ma.
PWparallelFfriction=maP' - W_{parallel} - F_{friction} = ma
P16.7813.83=5.0×1.5P' - 16.78 - 13.83 = 5.0 \times 1.5
P30.61=7.5P' - 30.61 = 7.5
P=38.11 NP' = 38.11 \text{ N}.
[3 marks]: 1 for net force equation, 1 for substitution, 1 for answer (38.1 N).