9702/21

Physics 9702/21May/June 2022

Cambridge AS Level · AS Level Structured Questions · worked solutions for every part, with the mark scheme

7
questions
60
marks
75
minutes

Topics Dynamics · Kinematics · Forces, Density and Pressure · Work, Energy and Power · Physical Quantities and Units · Deformation of Solids · +5 more

Q1KinematicsDynamicsFree sample
(a)

Define velocity.

1M
DifficultyEasy
Worked solution

Answer

Velocity is the rate of change of displacement with time.

Final answer

Rate of change of displacement with time.

Detailed explanation

Background Concept

Velocity is a vector quantity that tells you how quickly and in what direction the position of an object is changing. It is defined in terms of displacement (also a vector).

Instantaneous velocity is defined by

v=dsdtv = \frac{\mathrm{d}s}{\mathrm{d}t}

and average velocity is

average v=ΔsΔt.\text{average } v = \frac{\Delta s}{\Delta t}.

Understanding the Question

You are asked to define velocity (1 mark). This requires a clear definition linking velocity to displacement and time, and (ideally) indicating it is a vector.

Approach

Use the standard definition: velocity is the rate of change of displacement with time.

Step-by-Step Reasoning

  • “Rate of change” means “change per unit time”.
  • For velocity we must use displacement (not distance), because velocity has direction.
  • So velocity is change in displacement divided by time taken.

Key Takeaways

  • Velocity uses displacement, not distance.
  • Velocity is a vector (direction matters).

Common Mistakes

  • Defining velocity as “rate of change of distance” (that is speed).
  • Writing only “displacement divided by time” without making clear it is a rate (usually still accepted, but less precise).

Things to Be Careful About

  • If asked for a definition, do not substitute numbers or talk about graphs.
  • If you add extra detail, ensure it is correct (e.g. do not say velocity is scalar).
Techniques used
state velocity as a vector rate of changeuse the definition of displacement change per unit time
(b)

A rock of mass 7.5 kg7.5\text{ kg} is projected vertically upwards from the surface of a planet. The rock leaves the surface of the planet with a speed of 4.0 m s14.0\text{ m s}^{-1} at time t=0t = 0. The variation with time tt of the velocity vv of the rock is shown in Fig. 1.1.

Assume that the planet does not have an atmosphere and that the viscous force acting on the rock is always zero.

(i)

Determine the height of the rock above the surface of the planet at time t=4.0 st = 4.0\text{ s}.

height = ______ m\text{m}

3M
DifficultyMedium-Easy
Worked solution

Working

Displacement from t=0t=0 to 2.5s2.5\,\text{s}:

A1=12×2.5×4.0=5.0 mA_1 = \tfrac{1}{2} \times 2.5 \times 4.0 = 5.0\ \text{m}

Displacement from t=2.5t=2.5 to 4.0s4.0\,\text{s} (negative):

A2=(0+(2.4))2×1.5=1.8 mA_2 = \tfrac{(0 + (-2.4))}{2} \times 1.5 = -1.8\ \text{m}

Net height above surface at t=4.0st=4.0\,\text{s}:

5.0+(1.8)=3.2 m5.0 + (-1.8) = 3.2\ \text{m}

Answer

3.2 m3.2\ \text{m}

Final answer

3.2 m

Detailed explanation

Background Concept

For a velocity–time graph, the displacement over a time interval is the area under the graph:

Δs=vdt.\Delta s = \int v\,\mathrm{d}t.

Key sign idea:

  • If vv is positive, the area contributes a positive displacement (upwards here).
  • If vv is negative, the area contributes a negative displacement (downwards here).

Understanding the Question

The rock is thrown upwards with initial velocity 4.0 m s14.0\ \text{m s}^{-1}. From the graph, vv decreases linearly, crosses v=0v=0 at t=2.5 st=2.5\ \text{s} (top of the motion), and becomes negative by t=4.0 st=4.0\ \text{s} (rock is moving downward). You must find its height above the surface at t=4.0 st=4.0\ \text{s}, i.e. the net vertical displacement from t=0t=0 to t=4.0 st=4.0\ \text{s}.

Approach

Find the area under the vvtt graph from 00 to 4.0 s4.0\ \text{s}. Because the graph crosses the axis, split it into:

  1. a positive triangle from 00 to 2.5 s2.5\ \text{s},
  2. a negative triangle/trapezium from 2.52.5 to 4.0 s4.0\ \text{s},
    then add them (including the negative sign).

Step-by-Step Reasoning

  1. From t=0t=0 to 2.5 s2.5\ \text{s}, velocity goes from 4.04.0 to 00, making a triangle.
A1=12×base×height=12×2.5×4.0=5.0 m.A_1 = \tfrac{1}{2} \times \text{base} \times \text{height} = \tfrac{1}{2} \times 2.5 \times 4.0 = 5.0\ \text{m}.

This is the upward displacement to the highest point.

  1. From t=2.5t=2.5 to 4.0 s4.0\ \text{s}, velocity goes from 00 to 2.4 m s1-2.4\ \text{m s}^{-1}. The area is below the axis, so it is negative. Treat it as a trapezium (or a triangle here):

Time interval:

Δt=4.02.5=1.5 s.\Delta t = 4.0 - 2.5 = 1.5\ \text{s}.

Average velocity over that interval (since the graph is a straight line):

vˉ=0+(2.4)2=1.2 m s1.\bar v = \frac{0 + (-2.4)}{2} = -1.2\ \text{m s}^{-1}.

So displacement:

A2=vˉΔt=(1.2)×1.5=1.8 m.A_2 = \bar v\,\Delta t = (-1.2)\times 1.5 = -1.8\ \text{m}.
  1. Net displacement (height above the surface at t=4.0 st=4.0\ \text{s}):
Δs=A1+A2=5.0+(1.8)=3.2 m.\Delta s = A_1 + A_2 = 5.0 + (-1.8) = 3.2\ \text{m}.

So at 4.0 s4.0\ \text{s} the rock is still above the launch point, but is on its way back down.

Key Takeaways

  • Area under a vvtt graph gives displacement.
  • Areas below the time axis count as negative displacement.
  • When the graph is linear, using average velocity over an interval is quick and accurate.

Common Mistakes

  • Adding the magnitudes of areas and forgetting the negative sign after vv becomes negative.
  • Using the gradient instead of the area (gradient gives acceleration, not displacement).
  • Using t=4.0 st=4.0\ \text{s} as the base for the first triangle (should be 2.5 s2.5\ \text{s} where v=0v=0).

Things to Be Careful About

  • Read the correct intercepts from the graph: v=0v=0 at t=2.5 st=2.5\ \text{s} and v=2.4 m s1v=-2.4\ \text{m s}^{-1} at t=4.0 st=4.0\ \text{s}.
  • Keep consistent units: area units are (m s1)×s=m(\text{m s}^{-1})\times \text{s} = \text{m}.
Techniques used
find displacement from the area under a velocity-time graphsplit the area into simple shapes and include negative area
(ii)

Determine the change in the momentum of the rock from time t=0t = 0 to time t=4.0 st = 4.0\text{ s}.

change in momentum = ______ N s\text{N s}

2M
DifficultyMedium-Easy
Worked solution

Working

Initial momentum:

p0=7.5×4.0=30 kg m s1p_0 = 7.5 \times 4.0 = 30\ \text{kg m s}^{-1}

Final momentum at t=4.0st=4.0\,\text{s}:

p4=7.5×(2.4)=18 kg m s1p_4 = 7.5 \times (-2.4) = -18\ \text{kg m s}^{-1}

Change in momentum:

Δp=p4p0=1830=48 N s\Delta p = p_4 - p_0 = -18 - 30 = -48\ \text{N s}

Answer

48 N s-48\ \text{N s}

Final answer

-48 N s

Detailed explanation

Background Concept

Linear momentum pp is

p=mvp = mv

and is a vector (it has direction because vv has direction). The change in momentum is

Δp=pfinalpinitial=m(vfinalvinitial).\Delta p = p_\text{final} - p_\text{initial} = m(v_\text{final} - v_\text{initial}).

The unit kg m s1\text{kg m s}^{-1} is equivalent to N s\text{N s}.

Understanding the Question

You are asked for the change in momentum from t=0t=0 to t=4.0 st=4.0\ \text{s}.

  • Mass m=7.5 kgm = 7.5\ \text{kg}.
  • From the graph: v0=+4.0 m s1v_0 = +4.0\ \text{m s}^{-1} and v4=2.4 m s1v_4 = -2.4\ \text{m s}^{-1}.
    The negative final velocity indicates the rock is moving downward at t=4.0 st=4.0\ \text{s}.

Approach

Use

Δp=m(v4v0)\Delta p = m(v_4 - v_0)

and keep the sign of velocities to show direction.

Step-by-Step Reasoning

  1. Find momentum at t=0t=0:
p0=mv0=7.5×4.0=30 kg m s1.p_0 = mv_0 = 7.5 \times 4.0 = 30\ \text{kg m s}^{-1}.
  1. Find momentum at t=4.0 st=4.0\ \text{s}:
p4=mv4=7.5×(2.4)=18 kg m s1.p_4 = mv_4 = 7.5 \times (-2.4) = -18\ \text{kg m s}^{-1}.
  1. Subtract to get change in momentum:
Δp=p4p0=1830=48 kg m s1=48 N s.\Delta p = p_4 - p_0 = -18 - 30 = -48\ \text{kg m s}^{-1} = -48\ \text{N s}.

The negative sign means the momentum has changed in the negative (downward) direction.

Key Takeaways

  • Use Δp=mΔv\Delta p = m\Delta v with correct signs.
  • Negative velocity gives negative momentum (direction matters).

Common Mistakes

  • Using p0p4p_0 - p_4 instead of p4p0p_4 - p_0.
  • Ignoring the negative sign on v4v_4.
  • Writing the unit as N\text{N} (momentum change is N s\text{N s}, not N\text{N}).

Things to Be Careful About

  • State or imply direction through the sign; if you choose to give a magnitude instead, you should state “downwards”.
  • Do not round intermediate momenta too aggressively; here values are simple so it is fine.
Techniques used
use change in momentum \(\Delta p = m\Delta v\)substitute velocities from a velocity-time graph with sign
(iii)

Determine the weight WW of the rock on this planet.

WW = ______ N\text{N}

2M
DifficultyMedium
Worked solution

Working

Acceleration is the gradient of the vv-tt graph:

a=04.02.50=1.6 m s2a = \frac{0 - 4.0}{2.5 - 0} = -1.6\ \text{m s}^{-2}

So g=1.6 m s2g = 1.6\ \text{m s}^{-2} and

W=mg=7.5×1.6=12 NW = mg = 7.5 \times 1.6 = 12\ \text{N}

Answer

12 N12\ \text{N}

Final answer

12 N

Detailed explanation

Background Concept

On a planet with no air resistance (as stated), the only significant force on the rock in flight is its weight W=mgW = mg acting downward.

The rock’s acceleration is then constant and equal to the gravitational field strength (taking upward as positive):

a=g.a = -g.

From a velocity–time graph:

  • the gradient is acceleration:
a=ΔvΔt.a = \frac{\Delta v}{\Delta t}.

Understanding the Question

You are given a straight-line vv-–tt graph, so acceleration is constant. You must determine the weight WW of the 7.5 kg7.5\ \text{kg} rock on this planet.

Because there is no atmosphere in this part, the only force is weight, so the acceleration found from the graph is the gravitational acceleration gg (in magnitude).

Approach

  1. Calculate the gradient of the vv-–tt graph to find aa.
  2. Use a=ga = -g (upwards taken as positive) to get gg.
  3. Calculate weight using W=mgW = mg.

Step-by-Step Reasoning

  1. Choose two clear points on the straight line. From the graph:
  • at t=0t=0, v=4.0 m s1v=4.0\ \text{m s}^{-1},
  • at t=2.5 st=2.5\ \text{s}, v=0v=0.

Gradient:

a=04.02.50=4.02.5=1.6 m s2.a = \frac{0 - 4.0}{2.5 - 0} = \frac{-4.0}{2.5} = -1.6\ \text{m s}^{-2}.

So the magnitude of gravitational acceleration is

g=1.6 m s2.g = 1.6\ \text{m s}^{-2}.
  1. Weight:
W=mg=7.5×1.6=12 N.W = mg = 7.5 \times 1.6 = 12\ \text{N}.

(Weight acts downward.)

Key Takeaways

  • Gradient of a vv-–tt graph gives acceleration.
  • With no air resistance, acceleration is constant and equals g-g.
  • Weight is W=mgW=mg.

Common Mistakes

  • Using area under the graph (displacement) instead of gradient (acceleration).
  • Forgetting that the gradient is negative; gg is the magnitude of acceleration due to gravity.
  • Writing W=maW = ma with aa negative and giving a negative weight (weight is a force magnitude; direction is downward).

Things to Be Careful About

  • Use two well-separated points for the gradient to reduce reading error.
  • Quote weight in newtons, N\text{N}, and use consistent significant figures (here 2 s.f. is appropriate).
Techniques used
find acceleration from the gradient of a velocity-time graphapply Newton's second law to relate weight to mass and acceleration
(c)

In practice, the planet in (b) does have an atmosphere that causes a viscous force to act on the moving rock.

State and explain the variation, if any, in the resultant force acting on the rock as it moves vertically upwards.

2M
DifficultyMedium-Easy
Worked solution

Answer

As the rock rises, both weight and viscous (drag) force act downward, so the resultant force is downward.
The viscous force decreases as the speed decreases, so the resultant downward force decreases in magnitude (tending to just WW as v0v \to 0).

Final answer

Resultant force is downward and decreases in magnitude as the rock slows (drag decreases), tending to W at the top.

Detailed explanation

Background Concept

When an object moves through an atmosphere, it experiences a viscous/drag force that acts opposite to its direction of motion.

  • Weight W=mgW=mg acts downward and is (approximately) constant near the surface.
  • Drag FDF_D depends on speed: it increases with speed (often proportional to vv at low speeds and to v2v^2 at higher speeds).

Resultant force is the vector sum of all forces:

Fres=F.F_\text{res} = \sum F.

Understanding the Question

The rock is moving vertically upwards. You are asked to state and explain how the resultant force changes as it goes up, when there is an atmosphere.

Key point: while moving upward, both weight and drag are downward; but drag changes because the rock’s speed changes.

Approach

  1. Draw a free-body diagram for the upward motion.
  2. Write the resultant (taking upward as positive).
  3. Use the fact that as the rock rises it slows down, so its speed decreases, hence drag decreases.
  4. Deduce how this changes the resultant force.

Step-by-Step Reasoning

  1. Forces while moving upward:
  • Weight WW downward (constant).
  • Drag FDF_D downward (because motion is upward).
  1. Taking upward as positive, the resultant force is
Fres=(W+FD).F_\text{res} = -(W + F_D).

So the resultant is downward.

  1. As the rock rises, it slows: its speed vv decreases. Since FDF_D depends on speed, FDF_D decreases as vv decreases.

  2. Therefore W+FDW + F_D decreases, so the magnitude of the resultant downward force decreases as the rock rises.

At the highest point, v=0v=0 so drag is zero, leaving resultant force just the weight WW downward.

Key Takeaways

  • Drag always opposes motion.
  • During upward motion: drag and weight act in the same (downward) direction.
  • As speed decreases, drag decreases, so the resultant force becomes less downward (approaches WW).

Common Mistakes

  • Saying the resultant force is constant (it is not, because drag changes with speed).
  • Saying drag acts upward during upward motion (it acts downward then; it would act upward on the way down).
  • Saying the resultant becomes zero at the top (only drag becomes zero; weight remains).

Things to Be Careful About

  • Distinguish between direction of force and direction of motion.
  • “Resultant force decreases” must be interpreted as “magnitude decreases”; direction remains downward throughout the upward part of the motion.
Techniques used
identify forces acting on an object moving through a fluidrelate drag magnitude to speeddeduce how the resultant force changes as speed decreases

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