Gauss' Law and Applications (Review & Summary)

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A set of vocabulary flashcards covering Gauss's Law, Coulomb's Law, and the classic results for conductors, lines, sheets, and spherical charges.

Last updated 4:01 PM on 9/16/25
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17 Terms

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Gauss's Law

The net electric flux through any closed surface equals the enclosed charge divided by ε0: \oint E\cdot dA=\frac{q_{_{}enclosed}}{\varepsilon_0}

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Electric flux

ΦE, the amount of electric field crossing a surface, given by ΦE = ∮ E · dA.

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Gaussian surface

An imaginary closed surface used to apply Gauss's Law and exploit symmetry in electrostatics.

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Charge enclosed

q_enclosed, the net charge contained inside a Gaussian surface.

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Net flux

The total flux through a closed surface, equal to ∮ E · dA.

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Coulomb's law

Description of the force between point charges; F = k q1 q2 / r^2; E = F/q; k = 1/(4π ε0). Coulomb's law can be derived from Gauss's Law.

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Conducting surface

A surface of a conductor; in electrostatic equilibrium, excess charge resides on the outer surface.

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E outside a conductor

The electric field just outside a charged conducting surface is perpendicular to the surface with magnitude E = σ/ε0 (n̂ direction outward for positive σ).

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E inside a conductor

Inside a perfect conductor, the electric field E = 0 in electrostatic equilibrium.

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Infinite line of charge

A straight line with uniform linear charge density λ, producing E = λ/(2π ε0 r) radially outward from the line.

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Linear charge density

λ, the amount of charge per unit length along a line.

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Infinite sheet of charge

An infinite plane with uniform surface charge density σ, producing E = σ/(2ε0) on each side, perpendicular to the sheet.

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Surface charge density

σ, the amount of charge per unit area on a surface.

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Spherical shell of charge

A thin spherical shell of radius R with total charge q; external field behaves as if all charge is at the center; internal field is zero for r < R.

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Exterior field of a spherical shell

For r ≥ R, E(r) = (1/(4π ε0)) q / r^2, directed radially.

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Interior field of a spherical shell

For r < R, E(r) = 0 (field inside a thin spherical shell).

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Uniform solid sphere of charge

A solid sphere with uniform volume charge density ρ; inside field E = (ρ r)/(3 ε0) ; outside E = (1/(4π ε0)) Q / r^2 .