AQA A-Level Physics Paper 2, June 2025: Question 4

8 marks · Medium difficulty · Short Answer

Calculate the orbital period of Enceladus using Kepler's third law and determine gravitational properties and the mass of Titan from a potential-distance graph.

Practise this question

Question

Question 4 presents data about moons of Saturn: Mimas orbits at 1.28 × 10^8 m above Saturn's surface with a period of 0.94 Earth days; Enceladus orbits at 1.80 × 10^8 m above the surface; Saturn's radius is 5.8 × 10^7 m. Part 04.1 asks to calculate the orbital period of Enceladus. Figure 2 displays a graph of gravitational potential (from -3.5 × 10^7 to -3.1 × 10^7 J/kg) against distance from Saturn (from 11.7 × 10^8 to 12.2 × 10^8 m). A dashed line shows potential from Saturn alone, while a solid curved line shows the combined potential of Saturn and Titan, peaking near 12.03 × 10^8 m and dropping sharply at the surface of Titan. Parts 04.2 to 04.4 ask to explain why Saturn's field strength is approximately constant, find the distance where the resultant field is zero, and determine the mass of Titan.

Mark scheme

Show the mark scheme Mark scheme for Question 4. 04.1 awards 3 marks: 1 for calculating orbital radii by adding Saturn's radius (1.86 × 10^8 m and 2.38 × 10^8 m), 1 for using Kepler's third law T^2 proportional to r^3, and 1 for 1.36 Earth days. 04.2 awards 1 mark for stating the dashed line has a constant/linear gradient and gravitational field strength equals potential gradient. 04.3 awards 1 mark for distance between 12.025 × 10^8 and 12.045 × 10^8 m where the gradient is zero. 04.4 awards 3 marks: 1 for calculating potential from Titan by subtracting dashed and solid curve values (~ -6.5 × 10^5 J/kg), 1 for distance from Titan (1.4 × 10^7 m) and using V = -GM/r, and 1 for mass of Titan in the range 1.36 × 10^23 kg to 1.47 × 10^23 kg.

How to answer it

Gravitational Fields: Moons of Saturn & Potential Wells

📌 What this question tests

This question assesses your understanding of circular orbits and gravitational potential fields in a multi-body planetary system:

  • Kepler's Third Law (T² ∝ r³): Calculating orbital radius from surface height and finding orbital period.
  • Potential Gradient & Field Strength: Linking gravitational field strength to the gradient of a gravitational potential vs. distance graph (g = -ΔV/Δr).
  • Neutral Points: Identifying where the resultant gravitational field strength is zero from the maximum (turning point) on a V-r curve.
  • Superposition of Potential: Subtracting background potential to isolate an individual body's potential, and calculating planetary mass using V = -GM/r.

Question 04.1

Orbital Period of Enceladus [3 Marks]

📐 Step-by-Step Calculation

  1. Find orbital radii from the centre of Saturn:
    Orbital radius = radius of planet + height above surface
    r_Mimas = 5.8 × 10⁷ + 1.28 × 10⁸ = 1.86 × 10⁸ m
    r_Enceladus = 5.8 × 10⁷ + 1.80 × 10⁸ = 2.38 × 10⁸ m
  2. Apply Kepler's Third Law:
    T² / r³ = constant  or  T_E / T_M = (r_E / r_M)^(3/2)
    T_E = 0.94 × (2.38 × 10⁸ / 1.86 × 10⁸)^(3/2)
    T_E = 0.94 × (1.2796)^(1.5) = 0.94 × 1.4474
  3. Calculate final period:
    T_E = 1.36 Earth days (to 2 or 3 s.f.)

✅ Mark Scheme Breakdown

  • Mark 1: Adding the radius of Saturn to orbital height for at least one moon ( r_Mimas = 1.86 × 10⁸ m or r_Enceladus = 2.38 × 10⁸ m ).
  • Mark 2: Correct use of T₁² / r₁³ = T₂² / r₂³ OR finding proportionality constant k = T / r^(1.5) .
  • Mark 3: Final answer of 1.36 Earth days (allow ecf to 1.57 days if radius of Saturn was omitted in both radii).

❌ Common Errors

  • Forgetting planet radius: Using height directly as orbital radius ( r = h ). In gravity calculations, r is ALWAYS measured from the centre of mass of the central body.
  • Converting time units unnecessarily: Converting 0.94 days to seconds and back again. While not incorrect, it adds unnecessary arithmetic steps where calculator errors can occur.

🧠 Exam Technique

Notice the question states "at a height ... above the surface". Train your eyes to spot "height" vs "orbital radius". Whenever you see "height", immediately write down: r = R_planet + h .

Question 04.2

Uniform Field Approximation [1 Mark]

✅ Correct Answer

The variation of gravitational potential with distance is approximately a straight line / linear / has a constant gradient

AND gravitational field strength equals the potential gradient ( g = -ΔV/Δr ).

💡 Key Knowledge

  • The relationship between field strength and potential is:
    g = - dV/dr (field strength is the negative gradient of the V-r curve).
  • A constant gradient directly implies a constant field strength.

❌ Common Errors & Examiner Warnings

  • Saying "potential is directly proportional to distance": A straight line with a non-zero intercept is linear, NOT directly proportional. Saying "directly proportional" loses the mark.
  • Incomplete reasoning: Only mentioning that the line is straight, without stating that field strength is equal to the gradient. Both elements are required for the single mark.

Question 04.3

Location of Zero Field Strength Point P [1 Mark]

✅ Correct Answer

distance = 12.025 × 10⁸ m to 12.045 × 10⁸ m

Mark Scheme Note: At least 4 significant figures required (e.g. 12.03 × 10⁸ m). Do not accept 12.02 or 12.05 (too imprecise).

🧠 Exam Technique: Reading the Maximum

  • Resultant gravitational field strength g = 0 where the gradient of the total potential curve (solid line) is zero: dV/dr = 0 .
  • Locate the crest/turning point of the solid line on Figure 2.
  • Look at grid divisions: 1 major square = 0.1 × 10⁸ m, subdivided into 10 small squares. Therefore, 1 small square = 0.01 × 10⁸ m .
  • The peak lies between 3 and 4 small squares past 12.0, giving 12.03 × 10⁸ m to 12.04 × 10⁸ m .

Question 04.4

Gravitational Potential & Mass of Titan [3 Marks]

📐 Step-by-Step Calculation

  1. Isolate potential due to Titan at 12.08 × 10⁸ m:
    Read both curves at distance = 12.08 × 10⁸ m (8 small squares past 12.0):
    • Dashed line (Saturn alone): V_Saturn ≈ -3.135 × 10⁷ J kg⁻¹ (allow -3.135 to -3.138)
    • Solid line (Total potential): V_total ≈ -3.200 × 10⁷ J kg⁻¹ (allow -3.200 to -3.203)
    V_Titan = V_total - V_Saturn
    V_Titan = -3.200 × 10⁷ - (-3.135 × 10⁷) = -0.065 × 10⁷ = -6.5 × 10⁵ J kg⁻¹
    (Matches the "show that ... is about -7 × 10⁵ J kg⁻¹")
  2. Find distance from the centre of Titan:
    Centre of Titan is at 12.22 × 10⁸ m from Saturn.
    r_Titan = 12.22 × 10⁸ - 12.08 × 10⁸ = 0.14 × 10⁸ m = 1.4 × 10⁷ m
  3. Calculate Titan's Mass using V = -GM / r:
    M = |V| × r / G
    Using calculated V = -6.5 × 10⁵ J kg⁻¹ :
    M = (6.5 × 10⁵ × 1.4 × 10⁷) / (6.67 × 10⁻¹¹) = 1.36 × 10²³ kg
    (Or using given value -7 × 10⁵ J kg⁻¹: M = 1.47 × 10²³ kg)

✅ Mark Scheme Breakdown

  • Mark 1: Gravitational potential from Titan = solid line - dashed line read at 12.08 × 10⁸ m:
    Shows calculation giving a value in range -6.2 × 10⁵ to -6.8 × 10⁵ J kg⁻¹ .
  • Mark 2: Correct distance from Titan ( 1.4 × 10⁷ m ) OR correct substitution into V = -GM/r .
  • Mark 3: Final answer consistent with their V :
    • If using -6.5 × 10⁵ : 1.36 × 10²³ kg (range 1.3 × 10²³ to 1.4 × 10²³)
    • If using "show that" value -7 × 10⁵ : 1.47 × 10²³ kg

❌ Common Errors

  • Using distance from Saturn instead of distance from Titan: Using r = 12.08 × 10⁸ m instead of the distance to Titan's centre ( 1.4 × 10⁷ m ). Gravitational potential of a body depends on distance from that body's centre.
  • Reading off the wrong distance on the graph: Not checking grid square scaling carefully (each small square = 0.01 × 10⁸ m).
  • Sign confusion in subtraction: Subtracting negative numbers incorrectly, e.g. -3.20 - 3.14 = -6.34 × 10⁷ instead of -3.20 - (-3.14) .

🧠 Exam Technique: "Show that... go on to determine"

When an exam paper says "Show that [X] is about -7 × 10⁵ J kg⁻¹; go on to determine...":

  • You must show your own full calculation for the first mark to get a value close to -7 × 10⁵ .
  • If you get stuck on the first step, you can still gain the subsequent marks by using the provided value ( -7 × 10⁵ J kg⁻¹ ) in the second part!

Topics

Physics · 3.7 Fields and their consequences (A-level only)

Question and mark scheme from the AQA A-Level Physics examination, Paper 2, June 2025. QuestionVault is an independent revision resource; questions remain the copyright of the awarding body.