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AP Physics C: E&M

Physics C: E & M

AP Physics C: Electricity & Magnetism Complete Notes

Exam: 1 hour 30 minutes - 35 MCQ (70 min, 50%) + 3 FRQ (45 min, 50%) Calculator: Allowed (graphing calculator required) Note: Calculus-based; can be taken alongside or after Physics C: Mechanics

SectionFormatQuestionsTimeWeight
Section IMultiple Choice (MCQ)3570 min50%
Section IIFree Response (FRQ)345 min50%

Science Practices (Skills Tested)

SkillNameExam Weight
1Visual Representations12%-18%
2Question and Methods8%-12%
3Representing Data and Phenomena12%-18%
4Data Analysis12%-18%
5Theoretical Arguments8%-12%
6Mathematical Routines18%-24%
7Connection Across Topics12%-18%

FRQ Types

TypeDescription
Quantitative/QualitativeTranslation
Paragraph ArgumentLong-form written justification
Lab DesignExperimental procedure and analysis

FRQ Tips

  • Gauss's Law problems: Always check symmetry first - spherical, cylindrical, or planar -> choose right Gaussian surface
  • Circuit analysis: For RC/RL/RLC transients, state initial and final conditions clearly before writing expressions
  • Faraday's Law: Be precise about sign convention; Lenz's Law is tested every year
  • E&M FRQs often combine multiple chapters: e.g., motional emf (Ch. 3) + circuits (Ch. 2) -> look for connections
  • Use calculus notation correctly: dΦB/dtd\Phi_B/dt vs. ΔΦB/Δt\Delta\Phi_B/\Delta t - state which you're using
  • Maxwell's Equations: Be able to write all four in both integral and differential forms (displacement current is key addition)
  • Partials are real: Even if you can't finish, show correct setup for partial credit

Unit 1: Electrostatics

Types Of Electric Charge

Electric charge is a fundamental property of matter. Two types of electric charge:

  • Positive charge (protons)

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Practice

Law Of Conservation Of Charge

The total electric charge in an isolated system remains constant. qinitial=qfinal\sum q_{initial} = \sum q_{final} Implications:

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Practice
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Unit 2: Gauss's Law

Definition Of Electric Flux

Electric flux through a surface is measure of electric field passing through it. ΦE=EdA=EdAcosθ\Phi_E = \int \vec{E} \cdot d\vec{A} = \int E\,dA\cos\theta Where:

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Practice

Scalar Product In Flux Calculation

The dot product EdA\vec{E} \cdot d\vec{A} projects E onto surface normal. EdA=EdAcosθ\vec{E} \cdot d\vec{A} = |\vec{E}||d\vec{A}|\cos\theta Physical meaning:

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Practice
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Unit 3: Electric Potential

Definition Of Electric Potential Energy

Energy of system of charges due to their positions relative to each other. U=potential energy of charge systemU = \text{potential energy of charge system} For two point charges:

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Practice

Work Done By Conservative Force

Electric force is conservative (path-independent work). WAB=ΔU=UAUBW_{A \to B} = -\Delta U = U_A - U_B For electric field:

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Practice
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Unit 4: Conductors, Capacitors, Dielectrics

Charge Distribution On Conductors

When conductors reach electrostatic equilibrium: Properties:

  • All excess charge resides on surface

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Practice

Faraday Cages

Hollow conductor shields interior from external electric fields. Properties:

  • E = 0 inside hollow conductor

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Practice
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Unit 5: Electric Circuits

Definition Of Current

Electric current is rate of charge flow through a cross-section. I=dqdtI = \frac{dq}{dt} Units: Amperes (A) = Coulombs/second (C/s)

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Practice

Current Density And Drift Velocity

Current density (vector): J=nqvd\vec{J} = nq\vec{v}_d Units: A/m2

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Practice
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Unit 6: Magnetic Fields

Lorentz Force Law

Force on moving charge in electric and magnetic fields: F=q(E+v×B)\vec{F} = q(\vec{E} + \vec{v} \times \vec{B}) For magnetic field only:

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Practice

Motion Of A Charged Particle In A Uniform Magnetic Field

Perpendicular to field (v ⊥ B):

  • Circular motion (magnetic force provides centripetal)
  • Speed constant (force ⟂ velocity -> no work)

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Practice
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Unit 7: Electromagnetism

Induced Emf In Moving Conductors And Changing Magnetic Fields

Changing magnetic flux induces electromotive force (emf). Motional emf (conductor moving in static field): E=(v×B)dl\mathcal{E} = \oint (\vec{v} \times \vec{B}) \cdot d\vec{l}

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Practice

Self-inductance And Mutual Inductance

Self-inductance L:

  • Changing current in coil induces emf in same coil
  • E=LdIdt\mathcal{E} = -L\frac{dI}{dt}

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Practice
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