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E&M formula · equation · reference sheet

AP Physics C E&M Formula Sheet 2027

A reference-first Electricity & Magnetism equation system covering electrostatics through LC circuits, with exam-reference relationships separated from derived models and special cases.

∫MechanicsE & M
Reference-first equation system

What is actually given—and what you still have to know?

The exam supplies reference information, so this resource is organized around a more useful distinction than “memorize everything.” Exam reference marks relationships present in the current course reference information. Derived / course marks relationships, special cases, or model extensions that are useful for the course but are not being treated here as printed equation entries.

118E&M unique relationships
41exam-reference relationships
77derived / course relationships
2027exam-prep target
The equation is not the model.

Before substitution, identify the system or source, representation/geometry, governing law, assumptions, sign convention, and limiting behavior. On Physics C problems, the missing step is often deciding what to differentiate or integrate—not recalling the final algebraic form.

E&M equation-selection map

Source → field

Identify charge/current geometry. Use superposition generally; use Gauss or Ampère as calculation tools only when symmetry is strong enough.

Field → potential

Potential is scalar, field is vector, and ΔV=−∫E⃗·dℓ⃗ controls the sign relationship.

Boundary → capacitance

For conductors/capacitors, establish electrostatic boundary conditions and geometry before choosing a capacitance result.

Circuits need topology

Series/parallel reduction, Kirchhoff rules, and RC/LR/LC differential models solve different structures and time regimes.

Flux needs orientation

Electric/magnetic flux depend on an area vector; induction also requires the sign logic of Lenz’s law.

Magnetic force is directional

Cross products determine direction. Magnetic force on a point charge is perpendicular to velocity and therefore does no work.

Current exam-reference toolkit

More than an equation list: know the reference information around the equations

The current Physics C reference information supplied for exam use includes equations plus supporting constants, unit symbols, prefixes, standard modeling conventions, vector/calculus identities, and geometry/trigonometry. This page reorganizes those tools for learning rather than copying the official booklet layout.

Core E&M constants

k = 1/(4πε₀) ≈ 9.0×10⁹ N·m²/C², ε₀ ≈ 8.85×10⁻¹² C²/(N·m²), μ₀ = 4π×10⁻⁷ T·m/A, e = 1.60×10⁻¹⁹ C, c = 3.00×10⁸ m/s, plus particle masses, eV/u conversions, G, and g.

Default E&M conventions

Use an inertial frame; neglect friction/drag unless stated; treat strings, springs, pulleys, batteries, wires, and meters as ideal; take conventional current as positive-charge drift; treat resistors/lightbulbs as ohmic and capacitors as air-filled unless stated; isolated-point-charge potential is zero at infinity.

Vector identities

Resolve components first. Dot products control work/flux-type projections; cross products control torque and magnetic-force directions. Magnitude and unit-vector notation are part of the supplied mathematical toolkit.

Calculus identities

The reference information supports standard derivative/integral identities, but it does not choose limits, signs, paths, surfaces, or the physical integrand for you. Those decisions remain part of the physics.

Geometry + trigonometry

Area/volume relations, right-triangle relations, arc-length geometry, and common-angle trig values are reference aids. They are most useful after you draw and label the geometry correctly.

Formula-family coverage on this sheet

Formula familyExam-referenceDerived / courseRole
Potential65Searchable formula family
Circuits49Searchable formula family
Capacitors54Searchable formula family
Electrostatics45Searchable formula family
Current32Searchable formula family
RC Circuits15Searchable formula family
Dielectrics14Searchable formula family
Biot–Savart13Searchable formula family
Magnetism12Searchable formula family
Magnetic Force on Wires11Searchable formula family
Faraday’s Law10Searchable formula family
Charged Particle Motion02Searchable formula family
Lorentz Force01Searchable formula family
Crossed Fields01Searchable formula family

The table shows the largest formula families first. Use the category filter below to reach every smaller family without scrolling through the full library.

High-value derivation routes

Source → electric field

Use Coulomb superposition generally. Replace the direct integral with Gauss’s law only when symmetry lets E be treated simply on the Gaussian surface.

Electric field ↔ potential

Use ΔV=−∫E⃗·dℓ⃗; recover a field component from a spatial derivative of V. Decide whether vector field or scalar energy is the more efficient language.

Potential → capacitance/energy

Apply conductor boundary conditions and geometry first, then C=Q/|ΔV|. Build stored-energy forms from charging work rather than treating them as unrelated equations.

Charge flow → circuits

Start from I=dQ/dt and material/circuit constraints. Kirchhoff equations depend on topology and sign choices; RC behavior follows from a first-order differential equation.

Current → magnetic field/force

Use Biot–Savart generally; use Ampère only with suitable symmetry. Magnetic-force direction comes from a cross product and provides an immediate no-work check for point charges.

Flux change → induction

Define Φ_B with an area-vector orientation, then apply Faraday–Lenz. Add circuit laws for induced currents, or inductance for LR/LC differential models.

Symbol collisions that cause avoidable errors

SymbolMeaning hereHow to disambiguate
Ielectric currentDo not confuse with rotational inertia when crossing to Mechanics.
R / rresistance vs radius/distanceUse capitalization and context; both may occur in one circuit/geometry problem.
ε / ε₀emf vs permittivityEMF is a voltage-like source/induced quantity; ε₀ is a material constant of vacuum.
ρresistivity or charge densityUnits and the integral/constitutive relation identify which meaning is intended.
Φelectric or magnetic fluxAlways attach the field label and define the area-vector orientation.
k / κCoulomb constant vs dielectric constantκ is dimensionless relative permittivity; Coulomb k carries N·m²/C².
Search · filter · recall · print

Interactive equation library

Search by quantity, equation, unit, model, or purpose. Switch between exam-reference and derived/course relationships, isolate a formula family, or hide equations for active-recall practice.

E&M · ElectrostaticsExam reference
F⃗ = (1/4πε₀)(q₁q₂/r²)r̂Variables / units: q C; r mUse / condition: Coulomb force
E&M · ElectrostaticsDerived / course
E⃗ = F⃗/qVariables / units: E N/CUse / condition: electric-field definition
E&M · ElectrostaticsDerived / course
dE⃗ = (1/4πε₀)(dq/r²)r̂Variables / units: dq CUse / condition: continuous charge distribution
E&M · ElectrostaticsExam reference
∮E⃗·dA⃗ = Q_enc/ε₀Variables / units: flux N·m²/CUse / condition: Gauss's law
E&M · PotentialExam reference
ΔV = −∫E⃗·dr⃗Variables / units: V voltsUse / condition: potential difference from field
E&M · PotentialExam reference
U = qVVariables / units: U JUse / condition: electric potential energy
E&M · PotentialDerived / course
E⃗ = −∇VVariables / units: gradient of potentialUse / condition: field from potential
E&M · CapacitorsDerived / course
C = Q/ΔVVariables / units: C faradsUse / condition: capacitance definition
E&M · CapacitorsExam reference
C_parallel plate = εA/dVariables / units: ε F/mUse / condition: ideal parallel-plate capacitor
E&M · CapacitorsExam reference
U_C = ½CV² = Q²/(2C)Variables / units: U JUse / condition: stored capacitor energy
E&M · CurrentExam reference
I = dQ/dtVariables / units: I A; Q C; t sUse / condition: instantaneous electric current
E&M · CircuitsExam reference
R = ρL/AVariables / units: R ΩUse / condition: resistance of uniform conductor
E&M · CircuitsExam reference
V = IRVariables / units: V volts; I A; R ΩUse / condition: Ohmic resistor model
E&M · CircuitsDerived / course
P = IV = I²R = V²/RVariables / units: P WUse / condition: resistive/electric power
E&M · CircuitsDerived / course
ΣΔV_loop = 0Variables / units: voltsUse / condition: Kirchhoff loop rule
E&M · CircuitsDerived / course
ΣI_in = ΣI_outVariables / units: amperesUse / condition: Kirchhoff junction rule
E&M · CircuitsDerived / course
Q(t)=Cε(1−e^(−t/RC))Variables / units: τ=RCUse / condition: RC charging
E&M · CircuitsDerived / course
Q(t)=Q₀e^(−t/RC)Variables / units: τ=RCUse / condition: RC discharging
E&M · MagnetismDerived / course
F⃗_B = q v⃗×B⃗Variables / units: B teslaUse / condition: magnetic force on moving charge
E&M · MagnetismDerived / course
dB⃗ = (μ₀/4π) I dℓ⃗×r̂/r²Variables / units: B TUse / condition: Biot–Savart law
E&M · MagnetismExam reference
∮B⃗·dℓ⃗ = μ₀ I_encVariables / units: B TUse / condition: Ampère law in symmetric steady-current cases
E&M · Magnetic FieldsExam reference
Φ_B = ∫B⃗·dA⃗Variables / units: Φ_B Wb; B T; A m²Use / condition: magnetic flux through an oriented surface
E&M · InductionDerived / course
ε = −dΦ_B/dtVariables / units: ε voltsUse / condition: Faraday-Lenz induction
E&M · InductionDerived / course
L = NΦ_B/IVariables / units: L henryUse / condition: inductance definition
E&M · Inductor EMFExam reference
ε_L = −L dI/dtVariables / units: ε V; L H; dI/dt A/sUse / condition: self-induced back emf of an ideal inductor
E&M · Inductor EnergyExam reference
U_L = ½LI²Variables / units: U J; L H; I AUse / condition: magnetic energy stored by a linear inductor
E&M · ElectrostaticsDerived / course
Q = NeVariables / units: N integer; e CUse / condition: charge quantization
E&M · ElectrostaticsDerived / course
dq = λdℓ, σdA, or ρdVVariables / units: λ C/m; σ C/m²; ρ C/m³Use / condition: differential source charge
E&M · ElectrostaticsExam reference
Φ_E = ∫E⃗·dA⃗Variables / units: Φ_E N·m²/CUse / condition: electric flux through an oriented surface
E&M · ElectrostaticsDerived / course
Φ_E = EA cosθVariables / units: uniform E and flat area AUse / condition: uniform-field flux special case
E&M · ElectrostaticsExam reference
Q_enc = ∫λdℓ, ∫σdA, or ∫ρdVVariables / units: integrate enclosed region onlyUse / condition: enclosed charge for Gauss law
E&M · PotentialExam reference
U_E = kq₁q₂/rVariables / units: q C; r m; U_E JUse / condition: pair electric potential energy
E&M · PotentialDerived / course
U_E,total = Σ_(i<j) kq_iq_j/r_ijVariables / units: all pair separations r_ij mUse / condition: discrete multi-charge system energy
E&M · PotentialDerived / course
V = kq/rVariables / units: V volts; q C; r mUse / condition: point-charge electric potential
E&M · PotentialDerived / course
V = kΣ_i q_i/r_iVariables / units: V voltsUse / condition: scalar superposition for point charges
E&M · PotentialExam reference
V = k∫dq/rVariables / units: dq C; r mUse / condition: continuous-distribution electric potential
E&M · PotentialExam reference
E_x = −dV/dxVariables / units: E_x V/mUse / condition: field component from potential slope
E&M · PotentialExam reference
ΔU_E = qΔVVariables / units: U J; q C; V voltsUse / condition: potential-energy change
E&M · PotentialDerived / course
ΔK = −qΔVVariables / units: K JUse / condition: electrostatic-only work-energy relation
E&M · ConductorsDerived / course
E = 0 inside conducting materialVariables / units: E N/CUse / condition: electrostatic equilibrium
E&M · ConductorsDerived / course
V = constant on a connected conductorVariables / units: V voltsUse / condition: electrostatic equilibrium / equipotential conductor
E&M · ConductorsDerived / course
E_out = σ/ε₀Variables / units: σ C/m²Use / condition: field immediately outside a conductor surface in vacuum
E&M · ConductorsDerived / course
V₁ = V₂Variables / units: V voltsUse / condition: connected conductors at final equilibrium
E&M · ConductorsDerived / course
Q₁/Q₂ = R₁/R₂Variables / units: Q C; R mUse / condition: far-separated connected spherical conductors
E&M · CapacitorsExam reference
C = Q/|ΔV|Variables / units: C F; Q C; ΔV VUse / condition: definition of capacitance
E&M · CapacitorsExam reference
C = κε₀A/dVariables / units: A m²; d mUse / condition: ideal parallel-plate capacitor
E&M · CapacitorsDerived / course
E = Q/(κε₀A)Variables / units: E N/CUse / condition: uniform field between ideal parallel plates
E&M · CapacitorsExam reference
U_C = Q²/(2C) = ½C(ΔV)² = ½Q|ΔV|Variables / units: U JUse / condition: stored capacitor energy
E&M · CapacitorsDerived / course
C_sph = 4πκε₀ab/(b−a)Variables / units: a,b mUse / condition: concentric spherical capacitor
E&M · CapacitorsDerived / course
C_coax = 2πκε₀L/ln(b/a)Variables / units: L,a,b mUse / condition: long coaxial cylindrical capacitor
E&M · DielectricsExam reference
κ = ε/ε₀Variables / units: ε,ε₀ F/mUse / condition: relative permittivity / dielectric constant
E&M · DielectricsDerived / course
C = κC₀Variables / units: C FUse / condition: fully filled linear dielectric, unchanged geometry
E&M · DielectricsDerived / course
E = E₀/κVariables / units: E N/CUse / condition: isolated fully filled parallel-plate capacitor
E&M · DielectricsDerived / course
Q fixed: ΔV=ΔV₀/κ, U=U₀/κVariables / units: ΔV V; U JUse / condition: isolated capacitor dielectric insertion
E&M · DielectricsDerived / course
ΔV fixed: Q=κQ₀, U=κU₀Variables / units: Q C; U JUse / condition: battery-connected capacitor dielectric insertion
E&M · CurrentDerived / course
I = nqv_dAVariables / units: n m⁻³; q C; v_d m/s; A m²Use / condition: uniform carrier drift through cross section
E&M · CurrentDerived / course
J⃗ = nqv⃗_dVariables / units: J A/m²Use / condition: current density from carrier drift
E&M · CurrentExam reference
I = ∫J⃗·dA⃗Variables / units: I AUse / condition: total current from current-density field
E&M · CurrentExam reference
E⃗ = ρJ⃗Variables / units: E V/m; ρ Ω·mUse / condition: local ohmic material relation
E&M · CircuitsDerived / course
R = ∫ρ(ℓ)dℓ/AVariables / units: R Ω; ρ Ω·m; ℓ m; A m²Use / condition: constant-area resistor with position-dependent resistivity
E&M · CircuitsExam reference
R_eq,s = ΣR_iVariables / units: R ΩUse / condition: series equivalent resistance
E&M · CircuitsExam reference
1/R_eq,p = Σ(1/R_i)Variables / units: R ΩUse / condition: parallel equivalent resistance
E&M · CircuitsDerived / course
ΔV_terminal = ℰ − IrVariables / units: V; ℰ V; I A; r ΩUse / condition: nonideal battery during discharge
E&M · CircuitsDerived / course
ΔU = qΔVVariables / units: ΔU J; q C; ΔV VUse / condition: energy change per charge crossing a circuit element
E&M · CircuitsDerived / course
dQ_node/dt = ΣI_in − ΣI_outVariables / units: Q C; I A; t sUse / condition: general node charge-accounting relation
E&M · Capacitor NetworksExam reference
C_eq,p = ΣC_iVariables / units: C FUse / condition: parallel equivalent capacitance
E&M · Capacitor NetworksExam reference
1/C_eq,s = Σ(1/C_i)Variables / units: C FUse / condition: series equivalent capacitance
E&M · RC CircuitsExam reference
τ = RCVariables / units: τ s; R Ω; C FUse / condition: first-order RC time constant
E&M · RC CircuitsDerived / course
q_charge = Cℰ(1−e^(−t/RC))Variables / units: q C; ℰ V; t sUse / condition: simple initially uncharged series RC charging
E&M · RC CircuitsDerived / course
I_charge = (ℰ/R)e^(−t/RC)Variables / units: I AUse / condition: simple series RC charging current
E&M · RC CircuitsDerived / course
q_discharge = Q₀e^(−t/RC)Variables / units: q CUse / condition: simple RC discharge
E&M · RC CircuitsDerived / course
V_C,discharge = V₀e^(−t/RC)Variables / units: VUse / condition: simple RC discharge voltage
E&M · RC CircuitsDerived / course
X(t)=X_f+(X_i−X_f)e^(−t/τ)Variables / units: X; t sUse / condition: general first-order exponential approach to equilibrium
E&M · Magnetic FieldsExam reference
∮ B⃗·dA⃗ = 0Variables / units: B T; A m²Use / condition: Gauss’s law for magnetism over any closed surface
E&M · Magnetic FieldsExam reference
∇·B⃗ = 0Variables / units: B T; ∇ 1/mUse / condition: local differential form of Gauss’s law for magnetism
E&M · Magnetic MaterialsDerived / course
μ_r = μ/μ₀Variables / units: μ H/m; μ_r dimensionlessUse / condition: relative permeability ratio when a material model is specified
E&M · Moving ChargesDerived / course
B⃗ = (μ₀/4π) q(v⃗×r̂)/r²Variables / units: B T; q C; v m/s; r mUse / condition: nonrelativistic moving-point-charge magnetic field
E&M · Magnetic ForceExam reference
F⃗_B = q(v⃗×B⃗)Variables / units: F N; q C; v m/s; B TUse / condition: magnetic force on a moving charged particle
E&M · Lorentz ForceDerived / course
F⃗ = q(E⃗+v⃗×B⃗)Variables / units: F N; E N/C; B TUse / condition: combined electric and magnetic force
E&M · Charged Particle MotionDerived / course
r = m v_⊥/(|q|B)Variables / units: r m; m kg; v m/s; q C; B TUse / condition: nonrelativistic gyroradius in uniform magnetic field
E&M · Charged Particle MotionDerived / course
ω_c = |q|B/m; T = 2πm/(|q|B)Variables / units: ω rad/s; T sUse / condition: cyclotron angular frequency and period
E&M · Crossed FieldsDerived / course
v = E/BVariables / units: v m/s; E V/m; B TUse / condition: ideal crossed-field velocity selector
E&M · Biot–SavartExam reference
dB⃗ = (μ₀/4π) I(dℓ⃗×r̂)/r²Variables / units: B T; I A; dℓ m; r mUse / condition: magnetic field contribution from a steady-current element
E&M · Biot–SavartDerived / course
B_center = μ₀NI/(2R)Variables / units: B T; I A; R mUse / condition: field at center of N-turn circular loop
E&M · Biot–SavartDerived / course
B_axis = μ₀NI R²/[2(R²+z²)^(3/2)]Variables / units: B T; R,z mUse / condition: field on central axis of circular loop
E&M · Biot–SavartDerived / course
B_bisector = μ₀I L/[2πa√(a²+L²)]Variables / units: B T; L,a mUse / condition: field on perpendicular bisector of finite straight wire from −L to +L
E&M · Magnetic Force on WiresExam reference
dF⃗ = I(dℓ⃗×B⃗)Variables / units: F N; I A; dℓ m; B TUse / condition: differential force on current element in external field
E&M · Magnetic Force on WiresDerived / course
F⃗ = I(L⃗×B⃗)Variables / units: F N; I A; L m; B TUse / condition: straight wire in uniform external magnetic field
E&M · Current Density / Enclosed CurrentDerived / course
I_enc = ∫J⃗·dA⃗Variables / units: I A; J A/m²; A m²Use / condition: enclosed current for distributed current density
E&M · Long Straight WireDerived / course
B = μ₀I/(2πr)Variables / units: B T; I A; r mUse / condition: magnetic field outside a very long straight wire
E&M · Uniform Cylindrical CurrentDerived / course
B(r<R)=μ₀Ir/(2πR²)Variables / units: B T; I A; r,R mUse / condition: field inside a solid wire with uniform current density
E&M · Long SolenoidExam reference
B ≈ μ₀nIVariables / units: B T; n turns/m; I AUse / condition: ideal long-solenoid interior field
E&M · Ampère–Maxwell LawDerived / course
∮B⃗·dℓ⃗ = μ₀I + μ₀ε₀ dΦ_E/dtVariables / units: B T; I A; Φ_E N·m²/CUse / condition: conceptual complete magnetic-circulation law
E&M · Magnetic FluxDerived / course
Φ_B = B⃗·A⃗ = BA cosθVariables / units: Φ_B Wb; B T; A m²Use / condition: uniform-field flux through a flat oriented surface
E&M · Faraday’s LawExam reference
ε = −N dΦ_B/dtVariables / units: ε V; N dimensionless; Φ_B WbUse / condition: induced emf for N linked turns
E&M · Changing Uniform FieldDerived / course
ε = −NA dB_⊥/dtVariables / units: ε V; A m²; B TUse / condition: fixed loop with changing normal magnetic field
E&M · Changing AreaDerived / course
ε = −NB dA_⊥/dtVariables / units: ε V; B T; A m²Use / condition: constant field with changing threaded area
E&M · Rotating CoilDerived / course
ε = NBAω sinθVariables / units: ε V; B T; A m²; ω rad/sUse / condition: instantaneous rotating-coil emf with θ measured from area vector
E&M · Maxwell–Faraday LawExam reference
∮E⃗·dℓ⃗ = −dΦ_B/dtVariables / units: E V/m; ℓ m; Φ_B WbUse / condition: circulating electric field from changing magnetic flux
E&M · Induced CurrentDerived / course
I_ind = ε_ind/RVariables / units: I A; ε V; R ΩUse / condition: induced current when the loop is modeled as resistive
E&M · Motional EMFDerived / course
|ε| = BℓvVariables / units: ε V; B T; ℓ m; v m/sUse / condition: straight conductor moving perpendicular to its length and B
E&M · Magnetic BrakingDerived / course
F_drag = B²ℓ²v/RVariables / units: F N; B T; ℓ m; v m/s; R ΩUse / condition: simple resistive sliding-bar or entering-loop drag magnitude
E&M · Induction PowerDerived / course
F_drag v = εI = I²RVariables / units: P WUse / condition: energy-rate check for constant-speed resistive magnetic braking
E&M · Self-InductanceDerived / course
λ = NΦ_B = LIVariables / units: λ Wb-turn; L H; I AUse / condition: flux-linkage definition for a linear inductor
E&M · Solenoid InductanceExam reference
L = μ_core N²A/ℓVariables / units: L H; μ H/m; A m²; ℓ mUse / condition: ideal long-solenoid inductance
E&M · LR CircuitDerived / course
ε = IR + L dI/dtVariables / units: ε V; I A; R Ω; L HUse / condition: series LR growth differential equation
E&M · LR Time ConstantExam reference
τ = L/R_eqVariables / units: τ s; L H; R ΩUse / condition: characteristic time for an LR transient
E&M · LR Current GrowthDerived / course
I = (ε/R)(1−e^(−t/τ))Variables / units: I A; ε V; R Ω; t,τ sUse / condition: growth from zero current with constant source
E&M · LR Current DecayDerived / course
I = I₀e^(−t/τ)Variables / units: I A; I₀ A; t,τ sUse / condition: source-free LR current decay
E&M · LR Inductor VoltageDerived / course
|V_L| = εe^(−t/τ)Variables / units: V V; ε V; t,τ sUse / condition: inductor voltage magnitude during standard growth from zero
E&M · LC Loop EquationDerived / course
q/C + L dI/dt = 0Variables / units: q C; C F; L H; dI/dt A/sUse / condition: ideal source-free capacitor-inductor loop
E&M · LC Charge Differential EquationDerived / course
d²q/dt² = −q/(LC)Variables / units: q C; t s; L H; C FUse / condition: simple-harmonic charge model for an ideal LC circuit
E&M · LC Angular FrequencyExam reference
ω = 1/√(LC)Variables / units: ω rad/s; L H; C FUse / condition: natural angular frequency of ideal LC oscillation
E&M · LC PeriodDerived / course
T = 2π√(LC)Variables / units: T s; L H; C FUse / condition: period of charge and current oscillation
E&M · LC ChargeDerived / course
q(t) = Q_max cos(ωt+φ)Variables / units: q,Q C; ω rad/s; t s; φ radUse / condition: general sinusoidal ideal-LC charge solution
E&M · LC CurrentDerived / course
I(t) = −ωQ_max sin(ωt+φ)Variables / units: I A; Q C; ω rad/s; t s; φ radUse / condition: current from differentiating the charge solution
E&M · LC Energy ConservationDerived / course
q²/(2C) + ½LI² = constantVariables / units: q C; C F; L H; I AUse / condition: electric plus magnetic stored energy in ideal LC circuit
E&M · LC Maximum CurrentDerived / course
I_max = Q_max/√(LC) = ωQ_maxVariables / units: I A; Q C; L H; C FUse / condition: maximum current from conservation of energy

Five-step equation check before you calculate

1

Represent

Draw or label the graph, free-body diagram, field/circuit geometry, axis, path, surface, or state variables.

2

Choose the model

Name the governing law or definition before choosing a special-case result.

3

State conditions

Check symmetry, constancy, idealizations, system isolation, no-slip constraints, or transient endpoint assumptions.

4

Set signs/orientation

Fix axes, loop directions, area vectors, torque signs, current directions, and potential references before substitution.

5

Verify

Check units, direction, t=0/∞ endpoints, zero-angle/zero-field limits, and whether the result matches the original qualitative prediction.

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