AP Physics C: Electricity & Magnetism Unit 7 - Electrostatics

Electric Charge

  • Charge is a fundamental property of matter, measured in Coulombs (C).

  • Types of charge: Positive (protons) and Negative (electrons). They are equal in magnitude: e=1.60imes1019Ce = 1.60 imes 10^{-19} C.

  • Charge transfer occurs by electron movement: Positive charge indicates an electron deficit.

Atomic Structure

  • Nucleus contains protons (positive) and neutrons (neutral). Electrons are found in orbitals around the nucleus.

  • Protons and neutrons are held together by the strong force.

Conductors vs. Insulators

  • Conductors: Materials (e.g., metals) with free-moving electrons facilitating charge transfer.

  • Insulators: Materials (e.g., rubber, glass) where electrons are tightly bound, preventing charge flow.

Electroscope

  • Device to detect charge; diverging leaves indicate presence of charge.

Charging Methods

  • Conduction: Charging by direct contact (e.g., charged rod touching electroscope).

  • Induction: Charging without contact by bringing a charged object near and grounding the electroscope.

Coulomb's Law

  • Electrostatic forces between charges: extbfF=kracQ1Q2r2extbf{F} = k rac{|Q_1 Q_2|}{r^2}, where k=8.99imes109Nm2/C2k = 8.99 imes 10^9 N m^2/C^2.

  • The direction of the force is determined by the signs of the charges.

Electric Fields

  • Electric fields (E) created by charges: E=FqE = \frac{F}{q} and E=kQr2E = \frac{kQ}{r^2}.

  • Field lines indicate the direction of force on a positive test charge, originating from positive charges and terminating at negative charges.

Gauss’s Law

  • Net electric flux through a closed surface: Φ=Qencε0Φ = \frac{Q_{enc}}{ε_0}.

  • Useful in calculating electric fields for symmetrical charge distributions.

Applications of Gauss’s Law

  1. Infinite Sheets: Electric field due to uniform charge density is E=σ2ε0E = \frac{σ}{2ε_0}.

  2. Parallel Plates: The electric field inside the plates is uniform, outside is zero.

  3. Long Cylinders: Electric field from an infinite line charge characterized as E=λ2πrε0E = \frac{λ}{2πrε_0}.