9702/43

Physics 9702/43October/November 2014

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

13
questions
100
marks
120
minutes

Topics Magnetic Fields · Oscillations · Thermodynamics · Electric Fields · Capacitance · Quantum Physics · +8 more

Q1OscillationsMagnetic FieldsTemperatureFree sample

A light spring is suspended from a fixed point. A bar magnet is attached to the end of the spring, as shown in Fig. 1.1.

In order to shield the magnet from draughts, a cardboard cup is placed around the magnet but does not touch it.
The magnet is displaced vertically and then released. The variation with time tt of the vertical displacement yy of the magnet is shown in Fig. 1.2.

The mass of the magnet is 130 g130\ \text{g}.

(a)

For the oscillations of the magnet, use Fig. 1.2 to

(i)

determine the angular frequency ω\omega,

ω\omega = ______ rad s1\text{rad s}^{-1}

2M
DifficultyMedium-Easy
Worked solution

Working

From Fig. 1.2, time between successive maxima:

T=0.30 sT = 0.30\ \text{s} ω=2πT=2π0.30=2.09×101 rad s1\omega = \frac{2\pi}{T} = \frac{2\pi}{0.30} = 2.09\times 10^{1}\ \text{rad s}^{-1}

Answer

ω21 rad s1\omega \approx 21\ \text{rad s}^{-1}
Final answer

21 rad s^-1

Detailed explanation

Background Concept

For simple harmonic motion (SHM), the displacement varies sinusoidally with time and repeats after one period TT. The angular frequency ω\omega (in rad s1\text{rad s}^{-1}) is related to the period by

ω=2πT.\omega = \frac{2\pi}{T}.

Here, 2π rad2\pi\ \text{rad} corresponds to one complete cycle.

Understanding the Question

You are given a displacement–time graph for the vertical oscillations of the magnet. The task is to use the graph to find the period TT and hence calculate ω\omega.

Approach

  1. Identify two identical points one cycle apart (e.g. two successive maxima).
  2. Read the time difference to get TT.
  3. Substitute into ω=2π/T\omega = 2\pi/T.

Step-by-Step Reasoning

  • From the graph description, there is a maximum at t=0t = 0 and the next maximum at t=0.30 st = 0.30\ \text{s}. Hence
T=0.30 s.T = 0.30\ \text{s}.
  • Then
ω=2π0.30=20.94 rad s121 rad s1.\omega = \frac{2\pi}{0.30} = 20.94\ \text{rad s}^{-1} \approx 21\ \text{rad s}^{-1}.

Key Takeaways

  • The period is read from repeated points on the displacement–time graph.
  • Angular frequency is found using ω=2π/T\omega = 2\pi/T.

Common Mistakes

  • Using half a cycle (e.g. max to min) as the period.
  • Forgetting the factor of 2π2\pi and using ω=1/T\omega = 1/T.

Things to Be Careful About

  • Choose clearly identifiable points (two maxima or two minima) to reduce reading error.
  • Keep units consistent: TT in seconds gives ω\omega in rad s1\text{rad s}^{-1}.
Techniques used
read the period from a displacement–time graphuse \(\omega = 2\pi/T\) to calculate angular frequency
(ii)

show that the maximum kinetic energy of the oscillating magnet is 6.4 mJ6.4\ \text{mJ}.

2M
DifficultyMedium-Easy
Worked solution

Working

From Fig. 1.2, amplitude

A=1.5 cm=1.5×102 mA = 1.5\ \text{cm} = 1.5\times 10^{-2}\ \text{m}

Mass of magnet m=130 g=0.130 kgm = 130\ \text{g} = 0.130\ \text{kg}.

Using ω21 rad s1\omega \approx 21\ \text{rad s}^{-1},

vmax=ωA=21×1.5×102=0.315 m s1v_{\max} = \omega A = 21\times 1.5\times 10^{-2} = 0.315\ \text{m s}^{-1} Ek,max=12mvmax2=12(0.130)(0.315)2=6.45×103 JE_{k,\max} = \frac{1}{2}mv_{\max}^2 = \frac{1}{2}(0.130)(0.315)^2 = 6.45\times 10^{-3}\ \text{J}

Answer

Ek,max6.4 mJE_{k,\max} \approx 6.4\ \text{mJ}
Final answer

6.4 mJ

Detailed explanation

Background Concept

In SHM, the speed is greatest as the object passes through the equilibrium position (displacement y=0y = 0). The maximum speed is related to amplitude AA and angular frequency ω\omega by

vmax=ωA.v_{\max} = \omega A.

The maximum kinetic energy occurs at this point:

Ek,max=12mvmax2.E_{k,\max} = \frac{1}{2}mv_{\max}^2.

(Equivalently, the total energy in SHM is E=12mω2A2E = \frac{1}{2}m\omega^2A^2, which equals the maximum kinetic energy.)

Understanding the Question

From the displacement–time graph you read the amplitude. You already found ω\omega in part (a)(i). With the given mass m=0.130 kgm = 0.130\ \text{kg}, you must show that the maximum kinetic energy is 6.4 mJ6.4\ \text{mJ}.

Approach

  1. Read amplitude AA from the graph and convert to metres.
  2. Use vmax=ωAv_{\max} = \omega A.
  3. Substitute into Ek,max=12mv2E_{k,\max} = \tfrac{1}{2}mv^2.

Step-by-Step Reasoning

  • The graph shows peaks at about +1.5 cm+1.5\ \text{cm} and 1.5 cm-1.5\ \text{cm}, so
A=1.5 cm=0.015 m.A = 1.5\ \text{cm} = 0.015\ \text{m}.
  • With ω21 rad s1\omega \approx 21\ \text{rad s}^{-1},
vmax=ωA=21×0.015=0.315 m s1.v_{\max} = \omega A = 21\times 0.015 = 0.315\ \text{m s}^{-1}.
  • Then
Ek,max=12(0.130)(0.315)2=6.45×103 J=6.45 mJ6.4 mJ.E_{k,\max} = \frac{1}{2}(0.130)(0.315)^2 = 6.45\times 10^{-3}\ \text{J} = 6.45\ \text{mJ} \approx 6.4\ \text{mJ}.

Key Takeaways

  • In SHM, maximum kinetic energy occurs at equilibrium where speed is maximum.
  • Use vmax=ωAv_{\max} = \omega A and then 12mv2\tfrac{1}{2}mv^2.

Common Mistakes

  • Using amplitude in cm without converting to m, giving an answer 10410^4 too large.
  • Using the peak-to-peak displacement (3.0 cm3.0\ \text{cm}) instead of the amplitude (1.5 cm1.5\ \text{cm}).
  • Using E=mv2E = mv^2 instead of E=12mv2E = \tfrac{1}{2}mv^2.

Things to Be Careful About

  • Check units: ω\omega in rad s1\text{rad s}^{-1}, AA in m\text{m} gives vv in m s1\text{m s}^{-1}.
  • Significant figures: 6.4 mJ6.4\ \text{mJ} is appropriate given graph readings.
Techniques used
extract the amplitude from a displacement–time graphuse \(v_{\max} = \omega A\) for SHMcalculate kinetic energy using \(E_k = \tfrac{1}{2}mv^2\)
(b)

The cardboard cup is now replaced with a cup made of aluminium foil.
During 10 complete oscillations of the magnet, the amplitude of vibration is seen to decrease to 0.75 cm0.75\ \text{cm} from that shown in Fig. 1.2. The change in angular frequency is negligible.

(i)

Use Faraday’s law of electromagnetic induction to explain why the amplitude of the oscillations decreases.

3M
DifficultyMedium
Worked solution

Answer

As the magnet oscillates, the magnetic flux linkage through the aluminium cup changes, so an e.m.f. is induced (Faraday’s law).

This produces induced (eddy) currents in the aluminium. The magnetic field due to these currents opposes the change / motion of the magnet (Lenz’s law), giving a damping force.

Work is done against this force and the electrical energy is dissipated as thermal energy in the cup, so the oscillation energy decreases and the amplitude falls.

Final answer

Induced eddy currents oppose the motion (Faraday + Lenz), dissipating energy as heat so amplitude decreases.

Detailed explanation

Background Concept

Faraday’s law states that an e.m.f. is induced when the magnetic flux linkage changes:

E=d(NΦ)dt.\mathcal{E} = -\frac{\mathrm{d}(N\Phi)}{\mathrm{d}t}.

The negative sign is Lenz’s law: the induced effect opposes the change that produced it. In a bulk conductor (like an aluminium cup), induced currents circulate in closed loops; these are called eddy currents. Eddy currents cause heating because the conductor has resistance, so electrical energy is dissipated at a rate P=I2RP = I^2R.

Understanding the Question

Replacing cardboard with aluminium introduces a conducting material near the oscillating magnet. The magnet’s motion changes the magnetic flux through the metal, so induction occurs. The question asks you to explain why this causes the amplitude to decrease (i.e. why the motion is damped).

Approach

  1. State that magnet motion causes changing flux linkage in the conductor.
  2. Use Faraday’s law to conclude an induced e.m.f. and current.
  3. Use Lenz’s law to explain the induced magnetic field opposes the magnet’s motion, creating a resistive (damping) force.
  4. Link the damping force to energy loss (work done) and heating in the cup.

Step-by-Step Reasoning

  • When the magnet moves up and down, the magnetic field pattern relative to the aluminium changes. That means the magnetic flux Φ\Phi through loops in the cup is changing with time.
  • By Faraday’s law, a changing flux induces an e.m.f. around those loops. Since aluminium is conducting, this e.m.f. drives circulating eddy currents.
  • By Lenz’s law, the magnetic field produced by the eddy currents acts so as to oppose the change in flux. In practice, this opposition manifests as a force opposing the magnet’s velocity (a “magnetic drag”).
    • On the downward motion, the induced field acts to oppose the increase of flux (and so opposes the downward motion).
    • On the upward motion, it opposes the decrease of flux (and again opposes the upward motion).
  • Because there is a force opposite to the motion, the magnet does work against this force each cycle. That energy is transferred to the eddy currents and then dissipated as heat in the aluminium (resistive heating).
  • As a result, the mechanical energy of the oscillation decreases, so the amplitude steadily falls (damped oscillation).

Key Takeaways

  • Changing magnetic flux induces an e.m.f. (Faraday’s law).
  • Induced currents create fields that oppose the motion/change (Lenz’s law).
  • The opposition does negative work on the oscillator, reducing its energy and amplitude.

Common Mistakes

  • Saying “the aluminium attracts the magnet” rather than opposing its motion.
  • Describing induction but not linking it to energy dissipation (must mention loss as heat / I2RI^2R).
  • Confusing the role of the cardboard cup: cardboard is an insulator so eddy currents cannot flow.

Things to Be Careful About

  • The damping is strongest when the magnet moves fastest because dΦ/dt\mathrm{d}\Phi/\mathrm{d}t is largest then.
  • The question states the change in angular frequency is negligible: so you should focus on energy loss (amplitude reduction), not changing ω\omega.
Techniques used
apply Faraday’s law to a changing magnetic flux linkageuse Lenz’s law to determine the direction of induced effectslink induced currents to energy dissipation and damping
(ii)

Show that the loss in energy of the oscillating magnet is 4.8 mJ4.8\ \text{mJ}.

2M
DifficultyMedium-Easy
Worked solution

Working

Total energy in SHM:

E=12mω2A2A2E = \frac{1}{2}m\omega^2A^2 \propto A^2

Initial amplitude from Fig. 1.2: A0=1.5 cmA_0 = 1.5\ \text{cm}.
After 10 oscillations: A1=0.75 cmA_1 = 0.75\ \text{cm}.

E1E0=(A1A0)2=(0.751.5)2=0.25\frac{E_1}{E_0} = \left(\frac{A_1}{A_0}\right)^2 = \left(\frac{0.75}{1.5}\right)^2 = 0.25

With E0=6.4 mJE_0 = 6.4\ \text{mJ},

E1=0.25×6.4=1.6 mJE_1 = 0.25\times 6.4 = 1.6\ \text{mJ}

Energy lost:

ΔE=E0E1=6.41.6=4.8 mJ\Delta E = E_0 - E_1 = 6.4 - 1.6 = 4.8\ \text{mJ}

Answer

loss in energy=4.8 mJ\text{loss in energy} = 4.8\ \text{mJ}
Final answer

4.8 mJ

Detailed explanation

Background Concept

For SHM with angular frequency ω\omega and amplitude AA, the total mechanical energy is

E=12mω2A2.E = \frac{1}{2}m\omega^2A^2.

So if mm and ω\omega are constant (the question says the change in ω\omega is negligible), then

EA2.E \propto A^2.

This is why damping that reduces amplitude also reduces energy.

Understanding the Question

The magnet starts with the amplitude shown in Fig. 1.2 (about 1.5 cm1.5\ \text{cm}). With an aluminium cup, after 10 complete oscillations the amplitude is 0.75 cm0.75\ \text{cm}. You must find how much energy has been lost over those 10 oscillations.

You can use the maximum kinetic energy from part (a)(ii) as the initial total energy E0E_0.

Approach

  1. Use EA2E \propto A^2 to find the fraction of energy remaining.
  2. Multiply that fraction by the initial energy to get final energy.
  3. Subtract to get the loss.

Step-by-Step Reasoning

  • Initial amplitude A0=1.5 cmA_0 = 1.5\ \text{cm}, final amplitude A1=0.75 cmA_1 = 0.75\ \text{cm}.
  • Energy ratio:
E1E0=(A1A0)2=(0.751.5)2=(0.5)2=0.25.\frac{E_1}{E_0} = \left(\frac{A_1}{A_0}\right)^2 = \left(\frac{0.75}{1.5}\right)^2 = (0.5)^2 = 0.25.

So the oscillation has 25%25\% of its original energy after 10 oscillations.

  • With E0=6.4 mJE_0 = 6.4\ \text{mJ}:
E1=0.25×6.4=1.6 mJ.E_1 = 0.25\times 6.4 = 1.6\ \text{mJ}.
  • Energy lost:
ΔE=6.41.6=4.8 mJ.\Delta E = 6.4 - 1.6 = 4.8\ \text{mJ}.

Key Takeaways

  • In SHM (fixed mm and ω\omega), energy scales with A2A^2.
  • Halving the amplitude reduces the energy to one quarter.

Common Mistakes

  • Assuming energy is proportional to amplitude AA rather than A2A^2.
  • Using A0=3.0 cmA_0 = 3.0\ \text{cm} (peak-to-peak) instead of amplitude.
  • Treating 6.4 mJ6.4\ \text{mJ} as “energy lost” rather than initial energy.

Things to Be Careful About

  • The result depends on ω\omega being effectively constant (stated in the question).
  • Keep consistent units: because you use an energy ratio, cm is acceptable for the amplitude ratio (the conversion cancels).
Techniques used
use proportionality of SHM energy to amplitude squaredcalculate initial and final energies and take the differenceuse a previously found value as the total SHM energy
(c)

The mass of the aluminium cup in (b) is 6.2 g6.2\ \text{g}. The specific heat capacity of aluminium is 910 J kg1 K1910\ \text{J kg}^{-1}\ \text{K}^{-1}.
The energy in (b)(ii) is transferred to the cup as thermal energy.
Calculate the mean rise in temperature of the cup.

temperature rise = ______ K\text{K}

2M
DifficultyMedium-Easy
Worked solution

Working

Energy transferred to cup:

Q=4.8 mJ=4.8×103 JQ = 4.8\ \text{mJ} = 4.8\times 10^{-3}\ \text{J}

Mass of cup:

m=6.2 g=6.2×103 kgm = 6.2\ \text{g} = 6.2\times 10^{-3}\ \text{kg}

Specific heat capacity c=910 J kg1 K1c = 910\ \text{J kg}^{-1}\ \text{K}^{-1}.

Q=mcΔTΔT=Qmc=4.8×103(6.2×103)(910)Q = mc\Delta T \Rightarrow \Delta T = \frac{Q}{mc} = \frac{4.8\times 10^{-3}}{(6.2\times 10^{-3})(910)} ΔT=8.5×104 K\Delta T = 8.5\times 10^{-4}\ \text{K}

Answer

temperature rise=8.5×104 K\text{temperature rise} = 8.5\times 10^{-4}\ \text{K}
Final answer

8.5×10^-4 K

Detailed explanation

Background Concept

The thermal energy required to raise the temperature of a mass mm by ΔT\Delta T is

Q=mcΔT,Q = mc\Delta T,

where cc is the specific heat capacity in J kg1 K1\text{J kg}^{-1}\ \text{K}^{-1}. This relationship applies when there is no change of state and the temperature rise is small enough that cc can be treated as constant.

Understanding the Question

You are told that the energy lost from the oscillations (found in part (b)(ii) as 4.8 mJ4.8\ \text{mJ}) is transferred as thermal energy to the aluminium cup of mass 6.2 g6.2\ \text{g}. With c=910 J kg1 K1c = 910\ \text{J kg}^{-1}\ \text{K}^{-1}, you must find the mean temperature rise of the cup.

Approach

  1. Convert QQ from mJ to J and mass from g to kg.
  2. Rearrange Q=mcΔTQ = mc\Delta T to ΔT=Q/(mc)\Delta T = Q/(mc).
  3. Substitute values and calculate.

Step-by-Step Reasoning

  • Convert units:
Q=4.8 mJ=4.8×103 J,Q = 4.8\ \text{mJ} = 4.8\times 10^{-3}\ \text{J}, m=6.2 g=6.2×103 kg.m = 6.2\ \text{g} = 6.2\times 10^{-3}\ \text{kg}.
  • Rearrangement:
ΔT=Qmc.\Delta T = \frac{Q}{mc}.
  • Substitute:
ΔT=4.8×103(6.2×103)(910).\Delta T = \frac{4.8\times 10^{-3}}{(6.2\times 10^{-3})(910)}.

Compute the denominator: (6.2×103)(910)=5.642(6.2\times 10^{-3})(910) = 5.642.

So

ΔT=4.8×1035.642=8.5×104 K.\Delta T = \frac{4.8\times 10^{-3}}{5.642} = 8.5\times 10^{-4}\ \text{K}.

Key Takeaways

  • Use Q=mcΔTQ = mc\Delta T for heating with no phase change.
  • Always convert g to kg and mJ to J before substituting.

Common Mistakes

  • Using m=6.2m = 6.2 instead of 6.2×1036.2\times 10^{-3} (forgetting grams to kilograms).
  • Using Q=4.8Q = 4.8 instead of 4.8×1034.8\times 10^{-3} (forgetting mJ to J).
  • Quoting the answer without units.

Things to Be Careful About

  • The temperature rise is very small; writing it in standard form avoids rounding to zero.
  • Units check: J/(kgJ kg1 K1)=K\text{J}/(\text{kg}\cdot \text{J kg}^{-1}\ \text{K}^{-1}) = \text{K}.
Techniques used
use \(\Delta E = mc\Delta T\) to relate thermal energy to temperature changeconvert masses from grams to kilogramsrearrange for temperature rise

The rest of this paper

12 more questions
  • Q2Gravitational Fields · Magnetic Fields · Alternating Currents7M
  • Q3Ideal Gases · Thermodynamics7M
  • Q4Oscillations10M
  • Q5Electric Fields · Capacitance10M
  • Q6Capacitance4M
  • Q7Electric Fields · Magnetic Fields5M
  • Q8Quantum Physics10M
  • Q9Nuclear Physics · Quantum Physics · Thermodynamics6M
  • Q10Electronics8M
  • Q11Medical Physics9M
  • Q12Communication7M
  • Q13Communication6M
Loading the full paper…