Generated ERQ

✓ passed C.2 Wave model × D.2 Electric and magnetic fields 12 marks HL 3 passes 112.22s $0.6983
## ERQ · 12 marks · Topics: C.2 Wave model + D.2 Electric and magnetic fields · Archetype: theory_application **Integration:** primary=C.2 Wave model, secondary=D.2 Electric and magnetic fields (strength: supporting) **Stem.** A student sets up a Young's double-slit experiment in a sealed chamber. Coherent monochromatic light of wavelength 550 nm illuminates two narrow slits separated by 0.25 mm, and the interference pattern is observed on a screen 1.5 m beyond the slits. The chamber is initially evacuated and a sharp pattern of bright and dark fringes is recorded. The chamber is then filled with low-pressure air, and a uniform horizontal electric field of magnitude E is applied across the region between the slits and the screen, perpendicular to the direction of light propagation. Stray ionization (from background radiation) produces a low density of singly-charged positive ions (mass m = 4.8 × 10⁻²⁶ kg, charge +e) within the light path. As the field strength is increased above ~1.0 × 10⁵ V m⁻¹, the student observes that the fringes progressively lose contrast and eventually disappear. ### Part (a) State [2 marks] · AO1 · Topic: C.2 State two conditions that the light sources at the two slits must satisfy in order for a stable interference pattern to be observed on the screen. ### Part (b)(i) Calculate [3 marks] · AO2 · Topic: C.2 Calculate the fringe spacing on the screen when the chamber is evacuated. ### Part (b)(ii) Determine [2 marks] · AO2 · Topic: C.2 Determine the path difference, in nm, between waves arriving at the centre of the first dark fringe from the two slits. ### Part (c) Explain [3 marks] · AO3 · Topic: C.2 + D.2 The applied electric field accelerates the positive ions along the field direction. Using F = qE, the ions reach a typical kinetic energy of order 10⁻¹⁸ J before recombining or colliding. Explain how the work done on these charged particles by the field, together with their interaction with the light passing through the medium, leads to a loss of fringe visibility. ### Part (d) Evaluate [2 marks] · AO3 · ASSUMPTIONS DISCRIMINATOR Evaluate the assumption, used in part (b), that the air in the chamber can be treated as an undisturbed optical medium when the field is applied. --- ## Mark Scheme ### Part (a) [2 marks] — State - M1: the two sources must be coherent / maintain a constant phase difference [no ECF] - M2: the two sources must have the same frequency/wavelength (OR comparable amplitude / same polarization) [no ECF] ### Part (b)(i) [3 marks] — Calculate - M1: identifies s = λD/d and substitutes: s = (550 × 10⁻⁹)(1.5)/(0.25 × 10⁻³) [no ECF] - M2: correct evaluation of numerator/denominator, e.g. 8.25 × 10⁻⁷ / 2.5 × 10⁻⁴ [ECF from M1] - M3: s = 3.3 × 10⁻³ m (3.3 mm) [ECF from M1, M2] ### Part (b)(ii) [2 marks] — Determine - M1: identifies that first minimum corresponds to path difference = λ/2 [no ECF] - M2: path difference = 275 nm (accept 2.75 × 10⁻⁷ m) [ECF from M1] ### Part (c) [3 marks] — Explain (causal chain per §4.4.1) - M1: the electric force F = qE does work on the ions, giving them kinetic energy and accelerating them along randomly-distributed trajectories (since ions originate at random positions/times) [fact] - M2: the moving ions (and the field-induced dipoles in neutral molecules along the field direction) locally and time-dependently alter the refractive index of the air along each light path, therefore the optical path length traversed by light reaching the screen from each slit fluctuates randomly in time [linking — therefore] - M3: therefore the phase difference between waves from the two slits at any screen point fluctuates randomly, so on time-averaging the bright and dark fringes wash out and fringe visibility is reduced [linking — therefore + consequence] ### Part (d) [2 marks] — Evaluate (position + supporting + limiting per §4.4.1) - M1: position + supporting: the assumption is justified for the evacuated/field-free case — the wave model with a uniform medium correctly predicts the observed fringe spacing in (b), showing it captures the essential interference physics - M2: limiting consideration: however, once the field ionizes/polarizes the medium the refractive index is no longer uniform or static, so the wave model can only describe this regime by adding ad-hoc coupling between the field (D.2) and the optical phase — a limitation the simple model in (b) does not contain ### Marker notes - (b)(i): accept answers 3.2–3.4 mm; penalise missing units once only across paper. - (b)(ii): ECF — if student used incorrect fringe-spacing equation in (b)(i), still award full marks here for λ/2 reasoning and correct numerical value 275 nm. - (c): accept equivalent descriptions invoking density fluctuations, scintillation, or randomly-varying optical path; M2 requires explicit link between charged-particle motion in the field and an optical-medium property; M3 requires explicit link between random phase and loss of visibility. - (d) accept any of: medium is not truly uniform once ionized; refractive index becomes field-dependent (Kerr-type response); scattering by ions reduces coherence; thermal motion from ion–neutral collisions broadens phase distribution.