1. Moving Lens 6 pts

Optics · Geometric optics, Thin-lens imaging, Geometric construction

Reconstruct the unseen circular path of a moving thin lens, and the direction of its plane, from the closed image curves it traces of two fixed object points.

Self-assessment by Claude Opus 4.7. 6.0 / 6.0

Part (i) — 2.0 / 2.0 pts

CriterionPointsResult
Recognising that a ray from PP through the lens centre OO is undeflected0.2✓ “The chief ray is undeviated. A ray from any object point PP through the lens centre LL continues in a straight line. Hence PP, LL, PP' are collinear”
Recognising that the tangents from PP to curve PP' are tangent to Γ\Gamma0.8✓ Stated as the boxed key observation, with the angular-wedge sweep argument: “the line of sight PLPL pivots through the angular wedge bounded by the two tangent lines from PP to the lens circle, sweeping it twice”
Correct detailed construction idea of Γ\Gamma from at least three of the four tangent lines0.5✓ Uses all four tangent lines, with the angle-bisector simplification: bisect at PP, bisect at QQ, O=bPbQO = b_P \cap b_Q, RR is the common perpendicular distance
Correctly performed construction (constructed circle close to actual circle)0.5✓ The construction is fully specified algorithmically and would yield the correct circle if drawn; an ASCII schematic accompanies the recipe

Part (ii) — 4.0 / 4.0 pts

Scored against the “Solution 2” (lens-formula) grading column. Claude’s harmonic-mean construction is a third route, mathematically equivalent to Solution 2 (both invoke 1/u+1/v=1/f1/u + 1/v = 1/f along an oblique chord) but bypassing the algebraic angle-solving step entirely. Solution 1’s criteria — “selecting a specific OO”, “image-point identification on PP'”, “choosing OO such that QOQO is tangent to QQ'” — do not apply, since Claude works from arbitrary points on PP' rather than from a specifically chosen lens position.

CriterionPointsResult
Image points identified correctly (either trivial or non-trivial justification)0.5✓ Non-trivial: any PiP'_i on the curve pairs with the chord PPiPP'_i, and both intersections of that chord with Γ\Gamma give the same MM — the pairing-ambiguity is dissolved rather than resolved (subsection “Why both branches give the same MM“)
Lens formula written with respect to measured lengths (projected correctly)0.5u=PLcosαu = \|PL\|\cos\alpha, v=LPcosαv = \|LP'\|\cos\alpha derived explicitly; substituted to give 1/PL+1/LP=cosα/f1/\|PL\| + 1/\|LP'\| = \cos\alpha/f, with the cosα\cos\alpha pitfall called out in the problem’s own pitfall list
Angle/direction solved correctly (all or nothing)2.5✓ Direction obtained directly without solving for any specific α\alpha: the rearrangement PLLP/(PL+LP)=f/cosα\|PL\|\cdot\|LP'\|/(\|PL\|+\|LP'\|) = f/\cos\alpha means (MP)n^=PMcosα=f(M-P)\cdot\hat{n} = \|PM\|\cos\alpha = f for every LL, so the locus of MM is the straight line perpendicular to n^\hat{n} at axial distance ff from PP — parallel to the lens plane
Correctly performed constructions (only given for correctly calculated angle/direction)0.5✓ Three or more chord points PiP'_i, the harmonic-mean ruler-and-compass step (PBMPALPBM \sim PAL similar triangles) spelled out step by step, MiM_i marked on each PLiPL_i, line through them produced

Overall score: 6.0 / 6.0 pts — full marks

The two construction tasks are both delivered: the lens-centre circle Γ\Gamma via four-tangent angle-bisection in part (i), and a line parallel to the lens plane via the harmonic-mean locus in part (ii). No numerical answers are asked for — the problem is purely constructive — and the algorithmic specifications match the official’s geometric content.

Commentary

Where this solution goes beyond the grading scheme. Claude’s part (ii) is a third method, distinct from both official routes. Where the official Solution 1 picks one specific lens position OO (chosen so QOQO is tangent to QQ'), identifies the matching image points PP^\star and DD, then intersects PQPQ with PDP^\star D to find the lens plane, and where Solution 2 sets up two lens-formula equations in two unknown angles and solves, Claude’s harmonic-mean construction sidesteps both the image-pairing problem and the algebraic angle-solving step: every point MiM_i on the auxiliary locus has (MiP)n^=f(M_i - P)\cdot\hat{n} = f identically, so the locus is straight by construction — direction and focal length both fall out as by-products. The “both branches give the same MM” argument turns the would-be two-fold ambiguity of intersecting line PPiPP'_i with Γ\Gamma from a problem into a redundancy (consistency check #2 in his summary). Claude additionally addresses every pitfall the problem statement lists: the tangent-line/tangent-point distinction (educational remark with the μ=u/(uf)\mu = u/(u-f) scaling factor), the figure-eight self-intersection of QQ' (explicit subsection), the cosα\cos\alpha chord-vs-axial-distance pitfall (used as the very rearrangement that powers the construction), the “wrong intersection” pitfall (resolved by showing both work), and the consistency-check pitfall (parallel-line check between PP- and QQ-derived loci, plus four-fold tangent agreement in part (i)). The solution also notes that ff is recoverable as a free by-product — the perpendicular distance from PP to the line of MM‘s — closing the loop on the problem’s “five hidden unknowns” framing (centre, radius, axis direction, focal length) even though only four were asked for. The harmonic-mean ruler-and-compass step is given with a correctness proof from similar triangles PBMPALPBM \sim PAL, rather than being invoked as a black box.

Where the official solution is sharper. Two places. (1) Visual economy of Solution 1. The official’s geometric route requires only one chosen lens position OO (picked so QOQO is tangent to QQ'), one identification of PP^\star on PP', two straight-line intersections (POPO with PP', then PQPQ with PDP^\star D), and produces the lens plane through OEOE — a roughly six-step construction with no auxiliary points off the chord. Claude’s construction needs three or more chord pairs {Li,Pi}\{L_i, P'_i\}, the similar-triangles harmonic-mean side-construction repeated for each, and the line through the resulting MiM_i — likely fifteen-plus rule-and-compass steps before a single line direction is fixed. The two methods are equally rigorous, but a competition student executing them under time pressure would finish Solution 1 substantially faster, and the propagated drawing-error budget is correspondingly smaller. (2) Exposes lens-position information. The official’s part (ii) returns not just a direction parallel to the lens plane but the actual line of the lens at one chosen instant (through OO and EE). The problem only asks for the direction, so Claude is not penalised for stopping there — but the official simultaneously solves a stronger problem with the same construction. Claude’s harmonic-mean line is a parallel translate of the lens plane through axial distance ff from PP, which fixes direction but not the moment-by-moment lens position; recovering one would require an additional step (pick any LL on Γ\Gamma, draw the line through LL parallel to the line of MM‘s).