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## ERQ · 12 marks · Topics: B.3 Gas laws + A.2 Forces and momentum · Archetype: theory_application
**Integration:** primary=B.3 Gas laws, secondary=A.2 Forces and momentum (strength: co_equal)
**Stem.** A compressed-air cannon is used to launch a small plastic projectile horizontally from a frictionless trolley. The cannon's cylindrical chamber has an internal cross-sectional area of 4.5 × 10⁻⁴ m² and an initial gas volume of 9.0 × 10⁻⁵ m³. Before firing, the chamber contains 3.6 × 10⁻³ mol of dry air at a temperature of 295 K. When the trigger is released, the gas expands and pushes the projectile of mass 25 g along a barrel of length 0.20 m. Assume that the expansion is adiabatic with adiabatic index γ = 1.40, that the projectile leaves the barrel at the instant the gas occupies twice its initial volume, and that atmospheric pressure outside the barrel is 1.0 × 10⁵ Pa.
### Part (a) State [2 marks] · AO1 · Topic: B.3
State the ideal gas equation and identify what each symbol represents.
### Part (b)(i) Show that [2 marks] · AO2 · Topic: B.3
Show that the initial pressure of the gas in the chamber is approximately 9.81 × 10⁴ Pa.
### Part (b)(ii) Determine [3 marks] · AO2 · Topic: B.3
For an adiabatic process the relation pV^γ = constant applies. Determine the pressure of the gas at the instant the projectile leaves the barrel.
### Part (c) Calculate [3 marks] · AO2+AO3 · Topic: B.3+A.2
The work done by the expanding gas on the projectile is W = (p₁V₁ − p₂V₂)/(γ − 1), where subscripts 1 and 2 refer to the initial and final states of the gas. The cannon and trolley together have mass 1.80 kg and are initially at rest on a frictionless surface. Using the work–energy theorem together with conservation of momentum, determine the speed of the projectile **relative to the ground** as it leaves the barrel.
### Part (d) Suggest [2 marks] · AO3 · ASSUMPTIONS DISCRIMINATOR · Topic: B.3+A.2
The speed measured in a real test of the cannon is found to be lower than the value calculated in (c). Suggest **two** physically distinct reasons for this discrepancy. For each reason, state whether neglecting it caused your calculated speed to be an over- or under-estimate.
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## Mark Scheme
### Part (a) [2 marks] — State
- M1: writes pV = nRT [no ECF]
- M2: identifies all symbols correctly — p = pressure (Pa), V = volume (m³), n = amount in moles, R = molar/ideal gas constant, T = absolute temperature (K) [no ECF]
### Part (b)(i) [2 marks] — Show that
- M1: correct substitution into pV = nRT, e.g. p = (3.6 × 10⁻³ × 8.31 × 295) / (9.0 × 10⁻⁵) [no ECF]
- M2: evaluates to p ≈ 9.81 × 10⁴ Pa (accept 9.80–9.82 × 10⁴ Pa; must show working since value is given) [no ECF]
### Part (b)(ii) [3 marks] — Determine (Calculate per §4.3)
- M1: applies adiabatic relation p₂ = p₁(V₁/V₂)^γ with V₂/V₁ = 2 [no ECF]
- M2: substitutes p₂ = 9.81 × 10⁴ × (1/2)^1.40 [ECF from (b)(i)]
- M3: p₂ ≈ 3.72 × 10⁴ Pa (accept 3.7–3.8 × 10⁴ Pa) [ECF from (b)(i)]
### Part (c) [3 marks] — Calculate (co_equal cross-topic)
Use p₁ = 9.81 × 10⁴ Pa, V₁ = 9.0 × 10⁻⁵ m³, p₂ = 3.72 × 10⁴ Pa, V₂ = 1.8 × 10⁻⁴ m³.
- M1: computes work done by gas W = (p₁V₁ − p₂V₂)/(γ − 1) = (8.83 − 6.70)/0.40 ≈ 5.3 J **(B.3 contribution)** [ECF from (b)(i),(b)(ii)]
- M2: applies momentum conservation: m_p v_p = m_c v_c, so projectile and cannon kinetic energies satisfy W = ½ m_p v_p² + ½ m_c v_c² = ½ m_p v_p² (1 + m_p/m_c) **(A.2 contribution — both topics required)** [ECF]
- M3: solves v_p = √[2W / (m_p(1 + m_p/m_c))] = √[2 × 5.3 / (0.025 × 1.0139)] ≈ 20.4 m s⁻¹ (accept 20–21 m s⁻¹) [ECF]
*Alternative valid path:* compute v_p assuming stationary cannon (≈ 20.6 m s⁻¹) then correct via momentum conservation; full marks if both physics inputs are evident.
### Part (d) [2 marks] — Suggest (proposal + warrant + direction per §4.4.1)
Award 1 mark per bullet. Each bullet requires (i) identification of a physically distinct mechanism with a brief physics warrant **and** (ii) a correctly reasoned direction (over- or under-estimate). Both elements must be present for the mark.
- **M1 (1 mark):** identifies ONE mechanism with warrant AND states direction. Examples (any one):
- Friction between projectile and barrel wall dissipates energy as heat, so less work is converted to kinetic energy → calculation **over**-estimates the real speed.
- "Blow-by" gas leakage past the projectile reduces the effective pressure acting over the barrel length → calculation **over**-estimates the speed.
- **M2 (1 mark):** identifies a SECOND, physically distinct mechanism with warrant AND states direction. Must not duplicate M1. Examples (any one):
- Air in front of the projectile must be pushed aside (drag / atmospheric back-pressure ≈ 1.0 × 10⁵ Pa acting on the projectile face), opposing motion → **over**-estimate.
- Real expansion is not perfectly adiabatic — some heat is conducted to barrel walls, lowering p₂ and W below the calculated value → **over**-estimate.
- Real gas behaviour / finite molecular volume at the elevated initial density modifies pV^γ slightly; typically the work output is reduced → **over**-estimate.
### Marker notes
- Show-that target in (b)(i): 9.81 × 10⁴ Pa given to 3 sf; student-derived 9.80–9.82 × 10⁴ Pa acceptable.
- Part (c): full marks require BOTH the thermodynamic work expression (B.3) AND momentum conservation (A.2) to appear in the solution. A solution using only one topic earns at most M1.
- Part (d): do NOT award a mark for a correct mechanism without direction, or a direction without a physics-based warrant. Do NOT award two marks for two variants of the same mechanism (e.g. "friction in barrel" and "air resistance" count as distinct; "heat loss to walls" and "non-adiabatic expansion" count as the same).
- Cannon recoil is NOT accepted as a (d) answer because it has already been included in the part (c) calculation.
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