IB Practice / Physics HL / A. Space, time and motion

Kinematics and projectile motion: practice worksheet

6 questions · 44 marks · about 52 minutes

This worksheet practises reading motion graphs, using the uniform-acceleration equations with a clear sign convention, resolving projectiles launched horizontally, above and below the horizontal, and explaining qualitatively the effects of fluid resistance. Questions 5(d) and 6(d) also draw on A.2 (forces and momentum).

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  1. Question 1warm-up · calculator

    A ball is thrown vertically upwards from the ground with an initial speed of 20 m s−120\ \text{m s}^{-1}. Air resistance is negligible. Take g=10 m s−2g = 10\ \text{m s}^{-2} for this question.

    (a)Find the time taken for the ball to reach its maximum height.[1]

    Markscheme
    v=u+at⇒0=20−10tv = u + at \Rightarrow 0 = 20 - 10t so t=2 st = 2\ \text{s} ✔1

    Answer: t=2 st = 2\ \text{s}

    (b)Find the maximum height reached by the ball.[1]

    Markscheme
    v2=u2+2as⇒0=400−20sv^{2} = u^{2} + 2as \Rightarrow 0 = 400 - 20s so s=20 ms = 20\ \text{m} ✔1

    Accept s=(u+v)t2=20×22=20 ms = \frac{(u+v)t}{2} = \frac{20 \times 2}{2} = 20\ \text{m} or any other correct equation of motion.

    Answer: s=20 ms = 20\ \text{m}

    (c)State the acceleration of the ball at the instant it is at its maximum height.[1]

    Markscheme
    10 m s−210\ \text{m s}^{-2} directed downwards / towards the ground ✔1

    Both magnitude and direction required. Do not accept zero.

    Answer: 10 m s−210\ \text{m s}^{-2} downwards

    (d)Write down the velocity of the ball when it returns to the point from which it was thrown.[1]

    Markscheme
    20 m s−120\ \text{m s}^{-1} downwards ✔1

    Accept −20 m s−1-20\ \text{m s}^{-1} with upwards taken as positive. Direction must be given.

    Answer: 20 m s−120\ \text{m s}^{-1} downwards (i.e. −20 m s−1-20\ \text{m s}^{-1} taking upwards as positive)

  2. Question 2warm-up · calculator

    A tram moves along a straight track. Its velocity–time graph consists of three straight-line segments: from t=0t = 0 to t=4 st = 4\ \text{s} the velocity increases uniformly from 00 to 6 m s−16\ \text{m s}^{-1}; from t=4 st = 4\ \text{s} to t=10 st = 10\ \text{s} the velocity is constant at 6 m s−16\ \text{m s}^{-1}; from t=10 st = 10\ \text{s} to t=12 st = 12\ \text{s} the velocity decreases uniformly to 00.

    (a)Find the acceleration of the tram during the first 4 s4\ \text{s}.[1]

    Markscheme
    gradient =6−04=1.5 m s−2= \frac{6 - 0}{4} = 1.5\ \text{m s}^{-2} ✔1

    Answer: 1.5 m s−21.5\ \text{m s}^{-2}

    (b)Determine the total displacement of the tram between t=0t = 0 and t=12 st = 12\ \text{s}.[2]

    Markscheme
    recognises displacement as area under the graph, e.g. 12(4)(6)+(6)(6)+12(2)(6)\frac{1}{2}(4)(6) + (6)(6) + \frac{1}{2}(2)(6) ✔1
    12+36+6=54 m12 + 36 + 6 = 54\ \text{m} ✔1

    Accept a single trapezium: 12(12+6)(6)=54 m\frac{1}{2}(12 + 6)(6) = 54\ \text{m}.

    Answer: 54 m54\ \text{m}

    (c)Hence find the average velocity of the tram over the 12 s12\ \text{s} journey.[1]

    Markscheme
    vˉ=5412=4.5 m s−1\bar v = \frac{54}{12} = 4.5\ \text{m s}^{-1} ✔1

    ECF from (b). Do not accept 0+62=3 m s−1\frac{0 + 6}{2} = 3\ \text{m s}^{-1}.

    Answer: 4.5 m s−14.5\ \text{m s}^{-1}

  3. Question 3exam-style · calculator

    A stone is thrown horizontally from the top of a vertical sea cliff with a speed of 12.0 m s−112.0\ \text{m s}^{-1}. The top of the cliff is 45.0 m45.0\ \text{m} above the sea. Air resistance is negligible. Take g=9.8 m s−2g = 9.8\ \text{m s}^{-2}.

    (a)State the horizontal component of the acceleration of the stone while it is in flight.[1]

    Markscheme
    zero ✔1

    Answer: zero

    (b)Show that the time taken for the stone to reach the sea is about 3 s3\ \text{s}.[1]

    Markscheme
    45.0=12(9.8)t2⇒t=2×45.09.8=3.03 s45.0 = \frac{1}{2}(9.8)t^{2} \Rightarrow t = \sqrt{\frac{2 \times 45.0}{9.8}} = 3.03\ \text{s} ✔1

    Award the mark for the substituted expression with an unrounded result of 3.03 s3.03\ \text{s}.

    Answer: t=3.03 st = 3.03\ \text{s}

    (c)Calculate the horizontal distance from the base of the cliff to the point where the stone enters the sea.[1]

    Markscheme
    x=12.0×3.03=36.4 mx = 12.0 \times 3.03 = 36.4\ \text{m} ✔1

    Accept 36 m36\ \text{m} if t=3.0 st = 3.0\ \text{s} is used.

    Answer: 36.4 m36.4\ \text{m}

    (d)Determine the speed of the stone and the angle its velocity makes with the horizontal at the instant it enters the sea.[3]

    Markscheme
    vertical component vy=9.8×3.03=29.7 m s−1v_{y} = 9.8 \times 3.03 = 29.7\ \text{m s}^{-1} (or vy=2×9.8×45.0=29.7 m s−1v_{y} = \sqrt{2 \times 9.8 \times 45.0} = 29.7\ \text{m s}^{-1}) ✔1
    v=12.02+29.72=32.0 m s−1v = \sqrt{12.0^{2} + 29.7^{2}} = 32.0\ \text{m s}^{-1} ✔1
    θ=tan⁡−1(29.712.0)=68.0∘\theta = \tan^{-1}\left(\frac{29.7}{12.0}\right) = 68.0^{\circ} below the horizontal ✔1

    Accept v2=12.02+2(9.8)(45.0)v^{2} = 12.0^{2} + 2(9.8)(45.0) giving 32.0 m s−132.0\ \text{m s}^{-1} directly. Accept 22∘22^{\circ} to the vertical. ECF from (b).

    Answer: v=32.0 m s−1v = 32.0\ \text{m s}^{-1} at 68.0∘68.0^{\circ} below the horizontal

  4. Question 4exam-style · calculator

    A ball is kicked from the flat roof of a building. The ball leaves the roof at a height of 15.0 m15.0\ \text{m} above horizontal ground with a speed of 18.0 m s−118.0\ \text{m s}^{-1} at an angle of 30∘30^{\circ} above the horizontal. Air resistance is negligible. Take g=9.8 m s−2g = 9.8\ \text{m s}^{-2}.

    (a)Show that the maximum height of the ball above the ground is about 19 m19\ \text{m}.[2]

    Markscheme
    uy=18.0sin⁡30∘=9.0 m s−1u_{y} = 18.0 \sin 30^{\circ} = 9.0\ \text{m s}^{-1} ✔1
    rise above roof =9.022×9.8=4.13 m= \frac{9.0^{2}}{2 \times 9.8} = 4.13\ \text{m}, so height above ground =15.0+4.13=19.1 m= 15.0 + 4.13 = 19.1\ \text{m} ✔1

    Award the second mark only if the 15.0 m15.0\ \text{m} is added and an unrounded value is shown.

    Answer: 19.1 m19.1\ \text{m}

    (b)Determine the time taken for the ball to reach the ground.[3]

    Markscheme
    uses s=ut+12at2s = ut + \frac{1}{2}at^{2} with a consistent sign convention, e.g. −15.0=9.0t−4.9t2-15.0 = 9.0t - 4.9t^{2} ✔1
    solves the quadratic: t=9.0+9.02+4(4.9)(15.0)2×4.9t = \frac{9.0 + \sqrt{9.0^{2} + 4(4.9)(15.0)}}{2 \times 4.9} ✔1
    t=2.89 st = 2.89\ \text{s} ✔1

    ALTERNATIVE: time to top 0.918 s0.918\ \text{s} ✔, fall of 19.1 m19.1\ \text{m} from rest takes 2×19.19.8=1.98 s\sqrt{\frac{2 \times 19.1}{9.8}} = 1.98\ \text{s} ✔, total 2.89 s2.89\ \text{s} ✔. ECF from (a).

    Answer: t=2.89 st = 2.89\ \text{s}

    (c)Calculate the horizontal distance travelled by the ball before it reaches the ground.[1]

    Markscheme
    x=18.0cos⁡30∘×2.89=45.1 mx = 18.0 \cos 30^{\circ} \times 2.89 = 45.1\ \text{m} ✔1

    ECF from (b).

    Answer: 45.1 m45.1\ \text{m}

    (d)In reality, air resistance acts on the ball. Explain how air resistance affects the horizontal distance travelled by the ball.[2]

    Markscheme
    air resistance acts opposite to the velocity so there is a horizontal component of force / horizontal deceleration ✔1
    horizontal component of velocity decreases during flight (is no longer constant) ✔1
    so the horizontal distance is smaller / the trajectory is asymmetric and steeper on the way down ✔1

    Award [max 2]. OWTTE.

    Answer: The horizontal distance is reduced because the horizontal component of velocity now decreases during the flight.

  5. Question 5exam-style · calculator

    A skydiver of mass 75 kg75\ \text{kg} steps from a stationary balloon and falls vertically. The table gives the downward velocity vv of the skydiver at time tt after leaving the balloon.

    t / sv / m s−1001.09.72.018.53.025.84.031.65.035.86.038.98.042.310.043.912.044.515.044.920.045.0\begin{array}{c|c} t\ /\ \text{s} & v\ /\ \text{m s}^{-1} \\ \hline 0 & 0 \\ 1.0 & 9.7 \\ 2.0 & 18.5 \\ 3.0 & 25.8 \\ 4.0 & 31.6 \\ 5.0 & 35.8 \\ 6.0 & 38.9 \\ 8.0 & 42.3 \\ 10.0 & 43.9 \\ 12.0 & 44.5 \\ 15.0 & 44.9 \\ 20.0 & 45.0 \end{array}

    (a)State the terminal speed of the skydiver.[1]

    Markscheme
    45 m s−145\ \text{m s}^{-1} ✔1

    Answer: 45 m s−145\ \text{m s}^{-1}

    (b)Estimate the instantaneous acceleration of the skydiver at t=4.0 st = 4.0\ \text{s}.[2]

    Markscheme
    acceleration identified as gradient of the velocity–time graph at t=4.0 st = 4.0\ \text{s}, e.g. uses 35.8−25.85.0−3.0\frac{35.8 - 25.8}{5.0 - 3.0} ✔1
    a≈5.0 m s−2a \approx 5.0\ \text{m s}^{-2} ✔1

    Accept values in the range 4.54.5 to 5.5 m s−25.5\ \text{m s}^{-2} from a tangent or symmetric chord about t=4.0 st = 4.0\ \text{s}.

    Answer: approximately 5.0 m s−25.0\ \text{m s}^{-2}

    (c)Estimate the distance fallen by the skydiver during the first 6.0 s6.0\ \text{s}.[3]

    Markscheme
    distance identified as area under the velocity–time graph ✔1
    area found by trapezia (or counting strips), e.g. 1.0×(02+9.7+18.5+25.8+31.6+35.8+38.92)1.0 \times \left(\frac{0}{2} + 9.7 + 18.5 + 25.8 + 31.6 + 35.8 + \frac{38.9}{2}\right) ✔1
    s≈141 ms \approx 141\ \text{m} ✔1

    Accept values in the range 135135 to 147 m147\ \text{m}. Do not award the final mark for 12(9.8)(6.0)2=176 m\frac{1}{2}(9.8)(6.0)^{2} = 176\ \text{m}, which ignores fluid resistance.

    Answer: approximately 140 m140\ \text{m}

    (d)Explain, with reference to the forces acting on the skydiver, why the acceleration decreases with time and why the velocity eventually becomes constant.[3]

    Markscheme
    at t=0t = 0 the only force is the weight so the acceleration is gg / 9.8 m s−29.8\ \text{m s}^{-2} ✔1
    air resistance (fluid resistance / drag) increases as the speed increases ✔1
    net force == weight −- air resistance decreases, so the acceleration decreases ✔1
    when air resistance equals the weight the net force is zero, so acceleration is zero and the velocity is constant (terminal speed) ✔1

    Award [max 3]. OWTTE.

    Answer: The air resistance increases with speed, so the net downward force (weight minus air resistance) decreases and the acceleration decreases; when air resistance equals the weight the net force is zero and the velocity is constant.

  6. Question 6challenge · calculator

    A ball of mass 0.150 kg0.150\ \text{kg} is thrown from a balcony that is 8.00 m8.00\ \text{m} above horizontal ground. The ball leaves the hand with a speed of 14.0 m s−114.0\ \text{m s}^{-1} at an angle of 25∘25^{\circ} below the horizontal. Air resistance is negligible unless stated otherwise. Take g=9.8 m s−2g = 9.8\ \text{m s}^{-2}.

    (a)Determine the time taken for the ball to reach the ground.[3]

    Markscheme
    vertical component uy=14.0sin⁡25∘=5.92 m s−1u_{y} = 14.0 \sin 25^{\circ} = 5.92\ \text{m s}^{-1} downwards ✔1
    taking downwards as positive: 8.00=5.92t+4.9t28.00 = 5.92t + 4.9t^{2} ✔1
    t=−5.92+5.922+4(4.9)(8.00)2×4.9=0.809 st = \frac{-5.92 + \sqrt{5.92^{2} + 4(4.9)(8.00)}}{2 \times 4.9} = 0.809\ \text{s} ✔1

    ALTERNATIVE: find vyv_{y} from vy2=uy2+2gsv_{y}^{2} = u_{y}^{2} + 2gs giving 13.8 m s−113.8\ \text{m s}^{-1} ✔, then t=vy−uygt = \frac{v_{y} - u_{y}}{g} ✔, t=0.809 st = 0.809\ \text{s} ✔. Accept 0.81 s0.81\ \text{s}.

    Answer: t=0.809 st = 0.809\ \text{s}

    (b)Show that the speed of the ball just before it hits the ground is about 19 m s−119\ \text{m s}^{-1}.[2]

    Markscheme
    v2=u2+2gh=14.02+2(9.8)(8.00)v^{2} = u^{2} + 2gh = 14.0^{2} + 2(9.8)(8.00) (or vx=12.7 m s−1v_{x} = 12.7\ \text{m s}^{-1} and vy=13.8 m s−1v_{y} = 13.8\ \text{m s}^{-1} combined in quadrature) ✔1
    v=352.8=18.8 m s−1v = \sqrt{352.8} = 18.8\ \text{m s}^{-1} ✔1

    An unrounded value must be shown for the second mark. Accept an energy argument 12mv2=12mu2+mgh\frac{1}{2}mv^{2} = \frac{1}{2}mu^{2} + mgh.

    Answer: 18.8 m s−118.8\ \text{m s}^{-1}

    (c)A second identical ball is thrown from the same balcony with the same speed of 14.0 m s−114.0\ \text{m s}^{-1}, but at 25∘25^{\circ} above the horizontal. Without further calculation, state and explain how the impact speed and the time of flight of the second ball compare with those of the first ball.[3]

    Markscheme
    impact speed is the same ✔1
    because v2=u2+2ghv^{2} = u^{2} + 2gh (or the energy transferred, mghmgh) depends only on the initial speed and the height fallen, not on the launch direction ✔1
    time of flight is longer because the second ball first rises and returns to the balcony height (with the same downward vertical velocity component 5.92 m s−15.92\ \text{m s}^{-1}) before repeating the motion of the first ball ✔1

    OWTTE. Do not award the third mark for 'it travels further' without reference to the vertical motion.

    Answer: The impact speed is the same (18.8 m s−118.8\ \text{m s}^{-1}); the time of flight is longer for the second ball.

    (d)On hitting the ground the first ball sinks into soft mud and comes to rest in 25 ms25\ \text{ms}. Determine the magnitude of the average net force acting on the ball while it is being brought to rest.[3]

    Markscheme
    change in momentum Δp=0.150×18.8=2.82 kg m s−1\Delta p = 0.150 \times 18.8 = 2.82\ \text{kg m s}^{-1} ✔1
    converts time to seconds: Δt=0.025 s\Delta t = 0.025\ \text{s} and uses F=ΔpΔtF = \frac{\Delta p}{\Delta t} ✔1
    F=2.820.025=113 NF = \frac{2.82}{0.025} = 113\ \text{N} ✔1

    Accept 110110 to 115 N115\ \text{N} depending on rounding of vv. ECF from (b). Accept an equivalent approach using a=ΔvΔta = \frac{\Delta v}{\Delta t} and F=maF = ma.

    Answer: F≈113 NF \approx 113\ \text{N}

    (e)In reality air resistance acts on the first ball during its flight. Explain how air resistance affects the time of flight and the impact speed of the ball.[2]

    Markscheme
    air resistance acts opposite to the velocity so the (vertical) acceleration is less than gg and the ball gains speed more slowly / kinetic energy is transferred to the air ✔1
    so the impact speed is lower than 18.8 m s−118.8\ \text{m s}^{-1} ✔1
    the vertical component of velocity is smaller at every instant, so the ball takes longer to fall 8.00 m8.00\ \text{m} / time of flight increases ✔1

    Award [max 2]. OWTTE.

    Answer: Both are affected: the impact speed is lower and the time of flight is longer.

Common errors

  • Mixing sign conventions within one calculation, for example using +9.8+9.8 for gg with an upward initial velocity taken as positive, which gives the wrong root when a projectile lands below its launch point.
  • Treating the maximum height or range as the full vertical displacement when the projectile is launched from a height, forgetting to add the launch height or to use a negative displacement.
  • Using the average of initial and final velocities to find average velocity when the acceleration is not uniform, or reading distance from a velocity–time graph as gradient rather than area.
  • Assuming the horizontal component of velocity is constant even when air resistance is present, and describing the effect of air resistance on range only through the change in time of flight.
  • Confusing distance with displacement and speed with velocity, for example stating that the average velocity of a ball thrown up and caught at the same point is non-zero.

Original questions and notes written by Pietro Meloni, PhD, from the IB syllabus. Not endorsed by or affiliated with the International Baccalaureate Organization. Found a mistake? Please tell me privately at pietro@pietromeloni.com. More questions on this topic: A. Space, time and motion practice.

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