MATH40007 Seven Year Effective Coverage Matrix REVISED
English review edition prepared on 4 October 2026 from a preserved source copy. It is a later presentation, not the historical study interface. Source checks and difficulty judgements describe the original material author's own process; they do not indicate Imperial College London endorsement.
Source SHA-256: 64e9cae7b1c3700efc8e466138e99272a6914340593aa5d77502c6ed234de951Source date: 2026-08-06
Summary
Source cell order and numeric values are retained; prose labels are translated. Scroll within the table to view all rows and columns.
| MATH40007 Revised Historical-Coverage Audit | |||||||
| Metric | Value | Core correction | |||||
| Official question-level ability units | 28 | 2026 determines difficulty, not content slots. | |||||
| Old effective A/B units | 16 | 2020-2026 determines knowledge, entry cues and method chains. | |||||
| Old label-only/missing C/D units | 12 | C = label-only false coverage; excluded from effective coverage. | |||||
| New effective A/B units | 28 | Only Paper 1 remains a 2026-structure reinforcement paper. | |||||
| Paper-level difficulty | A32 / B20 / C12 / D16 | Papers 2-6 rotate historical ability families. | |||||
OfficialAbilityUnits
Source cell order and numeric values are retained; prose labels are translated. Scroll within the table to view all rows and columns.
| Year | Question | Ability unit / subparts | Recognition cue | First key step | Course method chain | Old grade | New paper coverage | New grade |
| 2020 | Q1 | Circuit Laplacian; Dirichlet voltages; unit-current response | large symmetric network / terminal data | write KCL or Lx=f | Laplacian -> symmetry -> voltages -> currents | C | Paper 4 Q1 | B |
| 2020 | Q2 | Random walk with competing targets and changed graph | journey stops at target/return | set harmonic boundary values | harmonic equations -> first-step conditioning | C | Paper 4 Q1 + Paper 5 Q2 | B |
| 2020 | Q3 | Four-mass spring network; constrained modes; modal equilibrium | fixed nodes and external forces | form reduced K/M | generalised eigenproblem -> modal expansion | B | Paper 5 Q3 + Paper 6 Q2 | B |
| 2020 | Q4 | First-quadrant complex potential; two grounded walls; boundary flux | log potential in quadrant | check boundary modulus | differentiate log -> boundary current -> integrate flux | B | Paper 6 Q1 | A |
| 2021 | Q1 | Cycle graph; circulant eigenvectors; effective conductance; voltage expansion | cycle/circulant symmetry | write Fourier modes | circulant spectrum -> modal voltage -> conductance | C | Paper 2 Q1 + Paper 3 Q3 | B |
| 2021 | Q2 | Subway random walk; escape and hitting a set | uniform choices on graph | assign hitting probabilities | harmonic system -> starting-edge average | C | Paper 2 Q2 + Paper 5 Q2 | A |
| 2021 | Q3 | Incidence and Laplacian null spaces; symmetry-built eigenvectors | incidence/nullity request | use rank-nullity and graph components | null spaces -> explicit L -> symmetry eigenspaces | C | Paper 5 Q1 | A |
| 2021 | Q4 | Upper-half-plane source/sink; insulated boundary; cross-line current | source-sink image form | differentiate h(z) | boundary component -> line integral -> conservation | B | Paper 3 Q4 | A |
| 2022 | Q1 | Grounded path Green matrix; reciprocity; inverse reduced Laplacian | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | B | Paper 4 Q2 | A |
| 2022 | Q2 | Incidence nullity; random-walk escape; internal hitting probability | graph plus multiple absorbing events | set different boundary values for each part | rank-nullity -> harmonic equations -> first-step average | C | Paper 2 Q2 | A |
| 2022 | Q3 | Six-node block Laplacian; symmetric/antisymmetric eigenvectors | two repeated blocks | try (e,e) and (e,-e) | base spectrum -> block lifting | B | Paper 4 Q3 | A |
| 2022 | Q4 | Circular electrode near grounded wall; limiting point source | Möbius log and circle boundary | identify constant-modulus boundary | geometry -> derivative -> wall current -> flux -> limit | B | Paper 4 Q4 | A |
| 2023 | Q1 | Tree conductance recurrence; generation voltages; infinite profiles | regular branching by generation | replace each layer by parallel resistance | layer resistances -> series sum -> limits | B | Paper 3 Q2 | A |
| 2023 | Q2 | Large ladder/chain spectral expansion and effective conductance | long structured graph | use supplied sine/circulant modes | spectral coefficients -> voltage/current observable | C | Paper 4 Q2 + Paper 6 Q4 | B |
| 2023 | Q3 | Non-uniform mass-spring generalised eigenproblem; symmetry reduction | unequal masses and commuting symmetry | mass-scale K and split parity spaces | M^-1/2 K M^-1/2 -> symmetry -> modes | D | Paper 5 Q3 | A |
| 2023 | Q4 | Grounded slit/electrode complex map; edge singularity | square-root branch at electrode endpoint | choose branch and check boundary | log derivative -> source check -> endpoint asymptotics | C | Paper 5 Q4 | A |
| 2024 | Q1 | Parameter-weighted circuit; limiting regimes; network substitution | conductance parameter c | solve KCL symbolically | weighted L -> limits -> exact C(c) -> substitute module | B | Paper 3 Q1 | A |
| 2024 | Q2 | Incidence/Laplacian null spaces; edge deletion; random walk | topology change after deleting edge | count components/cycles first | rank-nullity -> modified graph -> harmonic probabilities | C | Paper 5 Q1 + Paper 2 Q2 | B |
| 2024 | Q3 | Complete graph spectrum; effective conductance; voltage expansion | complete graph symmetry | use L=nI-J | orthogonal complement spectrum -> current expansion | C | Paper 3 Q3 | A |
| 2024 | Q4 | Multiple sources in half-plane; wall-current graph and total flux | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | B | Paper 3 Q4 | A |
| 2025 | Q1 | Tridiagonal/circulant spectra; Thomson minimisation and check | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | B | Paper 2 Q1 | A |
| 2025 | Q2 | Incidence dimensions; escape probability; internal hitting Q2(c) | same graph, different absorbing sets | reset boundary values for each part | incidence rank -> distinct harmonic systems | C | Paper 2 Q2 | A |
| 2025 | Q3 | Two-mass equilibrium, reaction, frequencies and full perturbation | equilibrium then perturbation | separate x=x_e+hat{x} | force balance -> eigenmodes -> initial-value projection | B | Paper 2 Q3 | A |
| 2025 | Q4 | Piecewise 1D conductor with source jump; interfaces; no-current condition | piecewise F(x) and interface | integrate J'=F and enforce continuity | piecewise integration -> interface -> parameter condition -> sketch | B | Paper 2 Q4 | A |
| 2026 | Q1 | Four fundamental spaces plus weighted circuit | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | A | Paper 1 Q1 | A |
| 2026 | Q2 | Two conductance reductions plus escape-before-return | two networks and random walk | reduce networks then use C/degree | series-parallel -> effective C -> escape identity | A | Paper 1 Q2 | A |
| 2026 | Q3 | Forced path diffusion; steady/transient modal solution | linear diffusion with boundaries | subtract steady state | K eigensystem -> initial deviation -> exponentials | A | Paper 1 Q3 | A |
| 2026 | Q4 | Uniform electrothermal rod and insulated-end variant | electrical heating drives thermal BVP | solve current first | phi/J -> heat source -> BVP -> energy balance | A | Paper 1 Q4 | A |
OldMockDisposition
Source cell order and numeric values are retained; prose labels are translated. Scroll within the table to view all rows and columns.
| Old file role | Question | Old content | Disposition | Reason |
| Old Paper 1 | Q1 | 2026 subspaces/circuit | RETAIN as 2026 reinforcement | Directly serves the single permitted 2026-structure role. |
| Old Paper 1 | Q2 | 2026 conductance/random walk | RETAIN as 2026 reinforcement | Directly serves the single permitted 2026-structure role. |
| Old Paper 1 | Q3 | 2026 diffusion | RETAIN as 2026 reinforcement | Directly serves the single permitted 2026-structure role. |
| Old Paper 1 | Q4 | 2026 electrothermal rod | RETAIN as 2026 reinforcement | Directly serves the single permitted 2026-structure role. |
| Old Paper 2 | Q1 | incidence/circuit | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 2 | Q2 | bridge/random walk | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 2 | Q3 | spring modes | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 2 | Q4 | half-plane source | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 3 | Q1 | spectra/Thomson | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 3 | Q2 | tree/random walk | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 3 | Q3 | block spectrum | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 3 | Q4 | piecewise rod | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 4 | Q1 | inverse Laplacian/circuit | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 4 | Q2 | bridge/random walk | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 4 | Q3 | forced diffusion | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 4 | Q4 | complex half-plane | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 5 | Q1 | subspaces/circuit | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 5 | Q2 | ladder/random walk | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 5 | Q3 | coupled oscillation | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 5 | Q4 | variable rod | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 6 | Q1 | incidence/circuit | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 6 | Q2 | cube/random walk | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 6 | Q3 | forced diffusion | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
| Old Paper 6 | Q4 | source-sink potential | REPLACE/REMAP | Usable mathematics, but the system fixed the same four 2026 slots and overcounted label coverage. |
NewSixPaperMap
Source cell order and numeric values are retained; prose labels are translated. Scroll within the table to view all rows and columns.
| Paper | Role | Historical basis | Coverage purpose |
| 1 | 2026 structure reinforcement | 2026 Q1-Q4 | Controlled familiarity only; explicitly not seven-year coverage |
| 2 | 2025 historical bridge | 2025 Q1-Q4 | Direct coverage of spectra/Thomson, internal hitting, springs, piecewise conduction |
| 3 | 2023-2024 historical abilities | 2023 Q1; 2024 Q1,Q3,Q4 | Tree recurrence, parameter circuits, complete-graph spectrum, multi-source potential |
| 4 | 2020-2022 historical abilities | 2020 Q1; 2022 Q1,Q3,Q4 | Large network response, Green matrix, block lifting, electrode limit |
| 5 | Seven-year gap closing | 2021 Q3; 2023 Q3,Q4; 2024 Q2 | Wheel nullspaces, generalised modes, slit singularity, changed-graph hitting |
| 6 | Mixed transfer pressure test | 2020 Q4; 2021/22/23 mixed | Topic order deliberately breaks the 2026 slot-recognition habit |
DifficultyCalibration
Source cell order and numeric values are retained; prose labels are translated. Scroll within the table to view all rows and columns.
| Paper | A marks | B marks | C marks | D marks | Total | Role |
| 1 | 32 | 20 | 12 | 16 | 80 | 2026 structure reinforcement |
| 2 | 32 | 20 | 12 | 16 | 80 | 2025 historical bridge |
| 3 | 32 | 20 | 12 | 16 | 80 | 2023-2024 historical abilities |
| 4 | 32 | 20 | 12 | 16 | 80 | 2020-2022 historical abilities |
| 5 | 32 | 20 | 12 | 16 | 80 | gap closing |
| 6 | 32 | 20 | 12 | 16 | 80 | mixed transfer pressure test |
| Six-paper total | 192 | 120 | 72 | 96 |
VersionMap
Source cell order and numeric values are retained; prose labels are translated. Scroll within the table to view all rows and columns.
| Old artifact | Status | Replacement | Website instruction |
| MATH40007_All_6_Questions_FINAL_V6.pdf | OBSOLETE - over-anchored | MATH40007_6_Papers_REVISED_HISTORICAL_COVERAGE_Questions.pdf | Remove from active whitelist; preserve in quarantine |
| MATH40007_All_6_Solutions_FINAL_V6.pdf | OBSOLETE - over-anchored | MATH40007_6_Papers_COURSE_METHOD_AUDITED_Solutions.pdf | Remove from active whitelist; preserve in quarantine |
| MATH40007_Six_Paper_Coverage_FINAL.pdf | OBSOLETE - label coverage | MATH40007_Seven_Year_Effective_Coverage_Matrix.xlsx | Do not display old coverage claim |
| MATH40007_Coverage_and_Use_Plan.pdf | HISTORICAL RECORD | MATH40007_Over_Anchoring_Diagnosis_and_Correction.pdf | Keep only as audit trail |
| MATH40007 Q2(c) Specialist practice package | MERGED | Revised Paper 2 Q2 | Retain only if clearly labelled optional bridge |
| Tony Paper 1 marking report | RETAIN | unchanged | Keep in feedback section |
OfficialSubpartMap
Source cell order and numeric values are retained; prose labels are translated. Scroll within the table to view all rows and columns.
| Year | Question | Part | Marks | Subpart ability | Recognition cue | First key step | Course method chain | New paper coverage | New grade |
| 2020 | Q1 | a | 4 | graph Laplacian | large symmetric network / terminal data | write KCL or Lx=f | Laplacian -> symmetry -> voltages -> currents | Paper 4 Q1 | B |
| 2020 | Q1 | b | 8 | Dirichlet voltages and effective conductance | large symmetric network / terminal data | write KCL or Lx=f | Laplacian -> symmetry -> voltages -> currents | Paper 4 Q1 | B |
| 2020 | Q1 | c | 8 | unit-current response and edge current | large symmetric network / terminal data | write KCL or Lx=f | Laplacian -> symmetry -> voltages -> currents | Paper 4 Q1 | B |
| 2020 | Q2 | a | 6 | best starting station for target before stop | journey stops at target/return | set harmonic boundary values | harmonic equations -> first-step conditioning | Paper 4 Q1 + Paper 5 Q2 | B |
| 2020 | Q2 | b | 6 | escape probability after leaving start | journey stops at target/return | set harmonic boundary values | harmonic equations -> first-step conditioning | Paper 4 Q1 + Paper 5 Q2 | B |
| 2020 | Q2 | c | 8 | changed graph after station closure | journey stops at target/return | set harmonic boundary values | harmonic equations -> first-step conditioning | Paper 4 Q1 + Paper 5 Q2 | B |
| 2020 | Q3 | a | 4 | mass-spring graph Laplacian | fixed nodes and external forces | form reduced K/M | generalised eigenproblem -> modal expansion | Paper 5 Q3 + Paper 6 Q2 | B |
| 2020 | Q3 | b | 6 | fixed-mass natural modes | fixed nodes and external forces | form reduced K/M | generalised eigenproblem -> modal expansion | Paper 5 Q3 + Paper 6 Q2 | B |
| 2020 | Q3 | c | 6 | modal equilibrium setup | fixed nodes and external forces | form reduced K/M | generalised eigenproblem -> modal expansion | Paper 5 Q3 + Paper 6 Q2 | B |
| 2020 | Q3 | d | 4 | equilibrium displacements | fixed nodes and external forces | form reduced K/M | generalised eigenproblem -> modal expansion | Paper 5 Q3 + Paper 6 Q2 | B |
| 2020 | Q4 | a | 5 | harmonicity and source | log potential in quadrant | check boundary modulus | differentiate log -> boundary current -> integrate flux | Paper 6 Q1 | A |
| 2020 | Q4 | b | 2 | grounded x-axis boundary | log potential in quadrant | check boundary modulus | differentiate log -> boundary current -> integrate flux | Paper 6 Q1 | A |
| 2020 | Q4 | c | 2 | grounded y-axis boundary | log potential in quadrant | check boundary modulus | differentiate log -> boundary current -> integrate flux | Paper 6 Q1 | A |
| 2020 | Q4 | d | 5 | boundary current component | log potential in quadrant | check boundary modulus | differentiate log -> boundary current -> integrate flux | Paper 6 Q1 | A |
| 2020 | Q4 | e | 6 | integrated boundary flux | log potential in quadrant | check boundary modulus | differentiate log -> boundary current -> integrate flux | Paper 6 Q1 | A |
| 2021 | Q1 | a | 3 | cycle Laplacian | cycle/circulant symmetry | write Fourier modes | circulant spectrum -> modal voltage -> conductance | Paper 2 Q1 + Paper 3 Q3 | B |
| 2021 | Q1 | b | 5 | circulant eigenvectors/eigenvalues | cycle/circulant symmetry | write Fourier modes | circulant spectrum -> modal voltage -> conductance | Paper 2 Q1 + Paper 3 Q3 | B |
| 2021 | Q1 | c | 5 | effective conductance | cycle/circulant symmetry | write Fourier modes | circulant spectrum -> modal voltage -> conductance | Paper 2 Q1 + Paper 3 Q3 | B |
| 2021 | Q1 | d | 7 | voltage eigen-expansion | cycle/circulant symmetry | write Fourier modes | circulant spectrum -> modal voltage -> conductance | Paper 2 Q1 + Paper 3 Q3 | B |
| 2021 | Q2 | a | 5 | hit A before B from X | uniform choices on graph | assign hitting probabilities | harmonic system -> starting-edge average | Paper 2 Q2 + Paper 5 Q2 | A |
| 2021 | Q2 | b | 8 | escape A to B before return | uniform choices on graph | assign hitting probabilities | harmonic system -> starting-edge average | Paper 2 Q2 + Paper 5 Q2 | A |
| 2021 | Q2 | c | 4 | hit any of B,Y,Z before return | uniform choices on graph | assign hitting probabilities | harmonic system -> starting-edge average | Paper 2 Q2 + Paper 5 Q2 | A |
| 2021 | Q2 | d | 3 | qualitative probability comparison | uniform choices on graph | assign hitting probabilities | harmonic system -> starting-edge average | Paper 2 Q2 + Paper 5 Q2 | A |
| 2021 | Q3 | a | 2 | incidence left-null dimension | incidence/nullity request | use rank-nullity and graph components | null spaces -> explicit L -> symmetry eigenspaces | Paper 5 Q1 | A |
| 2021 | Q3 | b | 2 | Laplacian null dimension | incidence/nullity request | use rank-nullity and graph components | null spaces -> explicit L -> symmetry eigenspaces | Paper 5 Q1 | A |
| 2021 | Q3 | c | 3 | explicit Laplacian | incidence/nullity request | use rank-nullity and graph components | null spaces -> explicit L -> symmetry eigenspaces | Paper 5 Q1 | A |
| 2021 | Q3 | d | 10 | four symmetry-form eigenvectors | incidence/nullity request | use rank-nullity and graph components | null spaces -> explicit L -> symmetry eigenspaces | Paper 5 Q1 | A |
| 2021 | Q3 | e | 3 | remaining two eigenvectors | incidence/nullity request | use rank-nullity and graph components | null spaces -> explicit L -> symmetry eigenspaces | Paper 5 Q1 | A |
| 2021 | Q4 | a | 4 | identify point source | source-sink image form | differentiate h(z) | boundary component -> line integral -> conservation | Paper 3 Q4 | A |
| 2021 | Q4 | b | 5 | no-flux boundary | source-sink image form | differentiate h(z) | boundary component -> line integral -> conservation | Paper 3 Q4 | A |
| 2021 | Q4 | c | 5 | current across finite y-axis interval | source-sink image form | differentiate h(z) | boundary component -> line integral -> conservation | Paper 3 Q4 | A |
| 2021 | Q4 | d | 6 | total cross-line current | source-sink image form | differentiate h(z) | boundary component -> line integral -> conservation | Paper 3 Q4 | A |
| 2022 | Q1 | a.i | 2 | node-1 unit-voltage response | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q1 | a.ii | 2 | node-1 effective conductance | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q1 | b.i | 2 | node-2 unit-voltage response | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q1 | b.ii | 2 | node-2 effective conductance | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q1 | c.i | 2 | node-3 unit-voltage response | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q1 | c.ii | 2 | node-3 effective conductance | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q1 | d | 4 | reciprocity identity | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q1 | e | 4 | Green matrix/inverse reduced Laplacian | multiple unit-voltage experiments | write reduced K | response columns -> symmetry reciprocity -> K inverse | Paper 4 Q2 | A |
| 2022 | Q2 | a | 4 | incidence dimensions/nullity | graph plus multiple absorbing events | set different boundary values for each part | rank-nullity -> harmonic equations -> first-step average | Paper 2 Q2 | A |
| 2022 | Q2 | b | 8 | escape N to S before return | graph plus multiple absorbing events | set different boundary values for each part | rank-nullity -> harmonic equations -> first-step average | Paper 2 Q2 | A |
| 2022 | Q2 | c | 8 | internal hitting N before S | graph plus multiple absorbing events | set different boundary values for each part | rank-nullity -> harmonic equations -> first-step average | Paper 2 Q2 | A |
| 2022 | Q3 | a | 2 | explicit block-graph Laplacian | two repeated blocks | try (e,e) and (e,-e) | base spectrum -> block lifting | Paper 4 Q3 | A |
| 2022 | Q3 | b | 3 | block form | two repeated blocks | try (e,e) and (e,-e) | base spectrum -> block lifting | Paper 4 Q3 | A |
| 2022 | Q3 | c | 5 | base 3x3 eigensystem | two repeated blocks | try (e,e) and (e,-e) | base spectrum -> block lifting | Paper 4 Q3 | A |
| 2022 | Q3 | d | 10 | symmetric/antisymmetric eigenvectors | two repeated blocks | try (e,e) and (e,-e) | base spectrum -> block lifting | Paper 4 Q3 | A |
| 2022 | Q4 | a | 3 | grounded wall | Möbius log and circle boundary | identify constant-modulus boundary | geometry -> derivative -> wall current -> flux -> limit | Paper 4 Q4 | A |
| 2022 | Q4 | b | 6 | constant-voltage circular electrode | Möbius log and circle boundary | identify constant-modulus boundary | geometry -> derivative -> wall current -> flux -> limit | Paper 4 Q4 | A |
| 2022 | Q4 | c | 3 | wall current density | Möbius log and circle boundary | identify constant-modulus boundary | geometry -> derivative -> wall current -> flux -> limit | Paper 4 Q4 | A |
| 2022 | Q4 | d | 2 | maximum current point | Möbius log and circle boundary | identify constant-modulus boundary | geometry -> derivative -> wall current -> flux -> limit | Paper 4 Q4 | A |
| 2022 | Q4 | e | 3 | total wall current | Möbius log and circle boundary | identify constant-modulus boundary | geometry -> derivative -> wall current -> flux -> limit | Paper 4 Q4 | A |
| 2022 | Q4 | f | 3 | point-source limiting process | Möbius log and circle boundary | identify constant-modulus boundary | geometry -> derivative -> wall current -> flux -> limit | Paper 4 Q4 | A |
| 2023 | Q1 | a | 1 | tree incidence dimensions | regular branching by generation | replace each layer by parallel resistance | layer resistances -> series sum -> limits | Paper 3 Q2 | A |
| 2023 | Q1 | b.i | 4 | finite tree effective conductance | regular branching by generation | replace each layer by parallel resistance | layer resistances -> series sum -> limits | Paper 3 Q2 | A |
| 2023 | Q1 | b.ii | 6 | generation voltages | regular branching by generation | replace each layer by parallel resistance | layer resistances -> series sum -> limits | Paper 3 Q2 | A |
| 2023 | Q1 | b.iii | 1 | infinite unit-conductance limit | regular branching by generation | replace each layer by parallel resistance | layer resistances -> series sum -> limits | Paper 3 Q2 | A |
| 2023 | Q1 | c | 4 | profile c_j=1/j | regular branching by generation | replace each layer by parallel resistance | layer resistances -> series sum -> limits | Paper 3 Q2 | A |
| 2023 | Q1 | d | 4 | profile c_j=j | regular branching by generation | replace each layer by parallel resistance | layer resistances -> series sum -> limits | Paper 3 Q2 | A |
| 2023 | Q2 | a | 2 | block matrix construction for ladder | long structured graph | use supplied sine/circulant modes | spectral coefficients -> voltage/current observable | Paper 4 Q2 + Paper 6 Q4 | B |
| 2023 | Q2 | b | 4 | spectral coefficients | long structured graph | use supplied sine/circulant modes | spectral coefficients -> voltage/current observable | Paper 4 Q2 + Paper 6 Q4 | B |
| 2023 | Q2 | c | 6 | two-parameter recurrence representation | long structured graph | use supplied sine/circulant modes | spectral coefficients -> voltage/current observable | Paper 4 Q2 + Paper 6 Q4 | B |
| 2023 | Q2 | d | 4 | closed-form response | long structured graph | use supplied sine/circulant modes | spectral coefficients -> voltage/current observable | Paper 4 Q2 + Paper 6 Q4 | B |
| 2023 | Q2 | e | 4 | effective conductance | long structured graph | use supplied sine/circulant modes | spectral coefficients -> voltage/current observable | Paper 4 Q2 + Paper 6 Q4 | B |
| 2023 | Q3 | a | 1 | symmetry matrix square | unequal masses and commuting symmetry | mass-scale K and split parity spaces | M^-1/2 K M^-1/2 -> symmetry -> modes | Paper 5 Q3 | A |
| 2023 | Q3 | b | 4 | symmetry eigensystem | unequal masses and commuting symmetry | mass-scale K and split parity spaces | M^-1/2 K M^-1/2 -> symmetry -> modes | Paper 5 Q3 | A |
| 2023 | Q3 | c | 3 | mass-scaled eigenproblem | unequal masses and commuting symmetry | mass-scale K and split parity spaces | M^-1/2 K M^-1/2 -> symmetry -> modes | Paper 5 Q3 | A |
| 2023 | Q3 | d | 2 | commutation calculation | unequal masses and commuting symmetry | mass-scale K and split parity spaces | M^-1/2 K M^-1/2 -> symmetry -> modes | Paper 5 Q3 | A |
| 2023 | Q3 | e | 2 | commuting-eigenvector argument | unequal masses and commuting symmetry | mass-scale K and split parity spaces | M^-1/2 K M^-1/2 -> symmetry -> modes | Paper 5 Q3 | A |
| 2023 | Q3 | f | 8 | natural frequencies | unequal masses and commuting symmetry | mass-scale K and split parity spaces | M^-1/2 K M^-1/2 -> symmetry -> modes | Paper 5 Q3 | A |
| 2023 | Q4 | a | 6 | grounded slit electrode | square-root branch at electrode endpoint | choose branch and check boundary | log derivative -> source check -> endpoint asymptotics | Paper 5 Q4 | A |
| 2023 | Q4 | b | 6 | verify finite point source | square-root branch at electrode endpoint | choose branch and check boundary | log derivative -> source check -> endpoint asymptotics | Paper 5 Q4 | A |
| 2023 | Q4 | c | 4 | complex current density | square-root branch at electrode endpoint | choose branch and check boundary | log derivative -> source check -> endpoint asymptotics | Paper 5 Q4 | A |
| 2023 | Q4 | d | 4 | endpoint singularity | square-root branch at electrode endpoint | choose branch and check boundary | log derivative -> source check -> endpoint asymptotics | Paper 5 Q4 | A |
| 2024 | Q1 | a | 2 | weighted Laplacian | conductance parameter c | solve KCL symbolically | weighted L -> limits -> exact C(c) -> substitute module | Paper 3 Q1 | A |
| 2024 | Q1 | b | 2 | c to zero limit | conductance parameter c | solve KCL symbolically | weighted L -> limits -> exact C(c) -> substitute module | Paper 3 Q1 | A |
| 2024 | Q1 | c | 2 | c to infinity limit | conductance parameter c | solve KCL symbolically | weighted L -> limits -> exact C(c) -> substitute module | Paper 3 Q1 | A |
| 2024 | Q1 | d | 5 | internal voltages as functions of c | conductance parameter c | solve KCL symbolically | weighted L -> limits -> exact C(c) -> substitute module | Paper 3 Q1 | A |
| 2024 | Q1 | e | 4 | general effective conductance | conductance parameter c | solve KCL symbolically | weighted L -> limits -> exact C(c) -> substitute module | Paper 3 Q1 | A |
| 2024 | Q1 | f | 5 | substitution into six-node circuit | conductance parameter c | solve KCL symbolically | weighted L -> limits -> exact C(c) -> substitute module | Paper 3 Q1 | A |
| 2024 | Q2 | a | 2 | incidence left-null dimension | topology change after deleting edge | count components/cycles first | rank-nullity -> modified graph -> harmonic probabilities | Paper 5 Q1 + Paper 2 Q2 | B |
| 2024 | Q2 | b | 2 | Laplacian null dimension | topology change after deleting edge | count components/cycles first | rank-nullity -> modified graph -> harmonic probabilities | Paper 5 Q1 + Paper 2 Q2 | B |
| 2024 | Q2 | c | 2 | edge deletion raising components | topology change after deleting edge | count components/cycles first | rank-nullity -> modified graph -> harmonic probabilities | Paper 5 Q1 + Paper 2 Q2 | B |
| 2024 | Q2 | d | 7 | escape from W | topology change after deleting edge | count components/cycles first | rank-nullity -> modified graph -> harmonic probabilities | Paper 5 Q1 + Paper 2 Q2 | B |
| 2024 | Q2 | e | 7 | hit E before W from X | topology change after deleting edge | count components/cycles first | rank-nullity -> modified graph -> harmonic probabilities | Paper 5 Q1 + Paper 2 Q2 | B |
| 2024 | Q3 | a | 2 | complete-graph Laplacian | complete graph symmetry | use L=nI-J | orthogonal complement spectrum -> current expansion | Paper 3 Q3 | A |
| 2024 | Q3 | b | 4 | effective conductance | complete graph symmetry | use L=nI-J | orthogonal complement spectrum -> current expansion | Paper 3 Q3 | A |
| 2024 | Q3 | c | 6 | real orthonormal eigensystem | complete graph symmetry | use L=nI-J | orthogonal complement spectrum -> current expansion | Paper 3 Q3 | A |
| 2024 | Q3 | d | 6 | voltage expansion under unit current | complete graph symmetry | use L=nI-J | orthogonal complement spectrum -> current expansion | Paper 3 Q3 | A |
| 2024 | Q3 | e | 2 | conductance check | complete graph symmetry | use L=nI-J | orthogonal complement spectrum -> current expansion | Paper 3 Q3 | A |
| 2024 | Q4 | a | 2 | grounded wall | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | Paper 3 Q4 | A |
| 2024 | Q4 | b | 2 | source locations and strengths | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | Paper 3 Q4 | A |
| 2024 | Q4 | c | 3 | complex current density | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | Paper 3 Q4 | A |
| 2024 | Q4 | d | 1 | zero tangential/normal component | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | Paper 3 Q4 | A |
| 2024 | Q4 | e | 2 | wall-current formula | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | Paper 3 Q4 | A |
| 2024 | Q4 | f | 4 | total wall current | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | Paper 3 Q4 | A |
| 2024 | Q4 | g | 6 | wall-current sketch | product/ratio of image factors | locate every log singularity | differentiate -> boundary restriction -> integrate and sketch | Paper 3 Q4 | A |
| 2025 | Q1 | a.i | 1 | tridiagonal rank | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | Paper 2 Q1 | A |
| 2025 | Q1 | a.ii | 3 | tridiagonal eigenvalues | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | Paper 2 Q1 | A |
| 2025 | Q1 | b.i | 1 | circulant rank | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | Paper 2 Q1 | A |
| 2025 | Q1 | b.ii | 4 | circulant eigenvalues | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | Paper 2 Q1 | A |
| 2025 | Q1 | c.i | 4 | Thomson minimisation | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | Paper 2 Q1 | A |
| 2025 | Q1 | c.ii | 3 | equivalent conductance | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | Paper 2 Q1 | A |
| 2025 | Q1 | c.iii | 4 | energy/conductance check | two matrix structures plus current energy | use standard spectra then parameterise flows | spectrum -> energy minimisation -> equivalent circuit check | Paper 2 Q1 | A |
| 2025 | Q2 | a.i | 1 | incidence dimensions | same graph, different absorbing sets | reset boundary values for each part | incidence rank -> distinct harmonic systems | Paper 2 Q2 | A |
| 2025 | Q2 | a.ii | 2 | right/left null dimensions | same graph, different absorbing sets | reset boundary values for each part | incidence rank -> distinct harmonic systems | Paper 2 Q2 | A |
| 2025 | Q2 | b | 8 | escape W to S | same graph, different absorbing sets | reset boundary values for each part | incidence rank -> distinct harmonic systems | Paper 2 Q2 | A |
| 2025 | Q2 | c | 9 | internal hitting W before S from N | same graph, different absorbing sets | reset boundary values for each part | incidence rank -> distinct harmonic systems | Paper 2 Q2 | A |
| 2025 | Q3 | a | 4 | static equilibrium | equilibrium then perturbation | separate x=x_e+hat{x} | force balance -> eigenmodes -> initial-value projection | Paper 2 Q3 | A |
| 2025 | Q3 | b | 2 | ceiling reaction | equilibrium then perturbation | separate x=x_e+hat{x} | force balance -> eigenmodes -> initial-value projection | Paper 2 Q3 | A |
| 2025 | Q3 | c | 6 | natural frequencies | equilibrium then perturbation | separate x=x_e+hat{x} | force balance -> eigenmodes -> initial-value projection | Paper 2 Q3 | A |
| 2025 | Q3 | d | 8 | full perturbation solution | equilibrium then perturbation | separate x=x_e+hat{x} | force balance -> eigenmodes -> initial-value projection | Paper 2 Q3 | A |
| 2025 | Q4 | a | 3 | piecewise differential equations/interfaces | piecewise F(x) and interface | integrate J'=F and enforce continuity | piecewise integration -> interface -> parameter condition -> sketch | Paper 2 Q4 | A |
| 2025 | Q4 | b | 8 | piecewise voltage solution | piecewise F(x) and interface | integrate J'=F and enforce continuity | piecewise integration -> interface -> parameter condition -> sketch | Paper 2 Q4 | A |
| 2025 | Q4 | c | 3 | zero-current condition | piecewise F(x) and interface | integrate J'=F and enforce continuity | piecewise integration -> interface -> parameter condition -> sketch | Paper 2 Q4 | A |
| 2025 | Q4 | d | 2 | specialised solution | piecewise F(x) and interface | integrate J'=F and enforce continuity | piecewise integration -> interface -> parameter condition -> sketch | Paper 2 Q4 | A |
| 2025 | Q4 | e | 4 | voltage sketch | piecewise F(x) and interface | integrate J'=F and enforce continuity | piecewise integration -> interface -> parameter condition -> sketch | Paper 2 Q4 | A |
| 2026 | Q1 | a.i | 1 | column space | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | Paper 1 Q1 | A |
| 2026 | Q1 | a.ii | 3 | right null space | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | Paper 1 Q1 | A |
| 2026 | Q1 | a.iii | 1 | row space | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | Paper 1 Q1 | A |
| 2026 | Q1 | a.iv | 3 | left null space | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | Paper 1 Q1 | A |
| 2026 | Q1 | b.i | 4 | internal voltage | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | Paper 1 Q1 | A |
| 2026 | Q1 | b.ii | 4 | edge current and direction | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | Paper 1 Q1 | A |
| 2026 | Q1 | b.iii | 4 | effective conductance | subspaces and small circuit | rank-nullity then KCL | linear spaces -> harmonic voltages -> current | Paper 1 Q1 | A |
| 2026 | Q2 | a | 8 | effective conductance network 1 | two networks and random walk | reduce networks then use C/degree | series-parallel -> effective C -> escape identity | Paper 1 Q2 | A |
| 2026 | Q2 | b | 6 | effective conductance network 2 | two networks and random walk | reduce networks then use C/degree | series-parallel -> effective C -> escape identity | Paper 1 Q2 | A |
| 2026 | Q2 | c | 6 | escape-before-return probability | two networks and random walk | reduce networks then use C/degree | series-parallel -> effective C -> escape identity | Paper 1 Q2 | A |
| 2026 | Q3 | a | 4 | steady/transient decomposition | linear diffusion with boundaries | subtract steady state | K eigensystem -> initial deviation -> exponentials | Paper 1 Q3 | A |
| 2026 | Q3 | b | 4 | steady-state modal coefficients | linear diffusion with boundaries | subtract steady state | K eigensystem -> initial deviation -> exponentials | Paper 1 Q3 | A |
| 2026 | Q3 | c | 8 | explicit transient solution | linear diffusion with boundaries | subtract steady state | K eigensystem -> initial deviation -> exponentials | Paper 1 Q3 | A |
| 2026 | Q3 | d | 4 | sketch and limiting values | linear diffusion with boundaries | subtract steady state | K eigensystem -> initial deviation -> exponentials | Paper 1 Q3 | A |
| 2026 | Q4 | a | 2 | electrical BVP | electrical heating drives thermal BVP | solve current first | phi/J -> heat source -> BVP -> energy balance | Paper 1 Q4 | A |
| 2026 | Q4 | b | 4 | thermal BVP with dissipation | electrical heating drives thermal BVP | solve current first | phi/J -> heat source -> BVP -> energy balance | Paper 1 Q4 | A |
| 2026 | Q4 | c | 6 | solve voltage and temperature | electrical heating drives thermal BVP | solve current first | phi/J -> heat source -> BVP -> energy balance | Paper 1 Q4 | A |
| 2026 | Q4 | d | 4 | heat fluxes | electrical heating drives thermal BVP | solve current first | phi/J -> heat source -> BVP -> energy balance | Paper 1 Q4 | A |
| 2026 | Q4 | e | 3 | insulated-end temperature | electrical heating drives thermal BVP | solve current first | phi/J -> heat source -> BVP -> energy balance | Paper 1 Q4 | A |
| 2026 | Q4 | f | 1 | insulated-end heat flux | electrical heating drives thermal BVP | solve current first | phi/J -> heat source -> BVP -> energy balance | Paper 1 Q4 | A |