Electric fields exhibit fascinating symmetries that simplify complex calculations. By recognizing spherical, cylindrical, or planar symmetry in charge distributions, we can apply Gauss's law more efficiently to determine electric field strengths.
Gauss's law connects electric flux through a closed surface to the enclosed charge . This powerful tool, combined with symmetry, allows us to solve electric field problems that would otherwise be challenging using Coulomb's law alone.
Symmetry in Electric Field Systems
Symmetry types in electric fields
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Spherical symmetry occurs when charge distribution is uniform and radially symmetric around a central point (point charge, uniformly charged sphere )
Electric field magnitude depends only on distance from the center
Electric field direction always radial, pointing towards or away from the center
Cylindrical symmetry occurs when charge distribution is uniform and radially symmetric along the axis of a cylinder (infinite line of charge , uniformly charged cylinder)
Electric field magnitude depends only on distance from the cylinder's axis
Electric field direction always perpendicular to the cylinder's axis, pointing towards or away from the axis
Planar symmetry occurs when charge distribution is uniform and symmetric across a plane (infinite sheet of charge , uniformly charged parallel plates )
Electric field magnitude constant at any given distance from the plane
Electric field direction always perpendicular to the plane, pointing towards or away from the plane
Identifying electric field symmetry
Identify shape and distribution of charge(s) in the system
Determine if charge distribution is uniform and symmetric
Spherical: Radially symmetric around a central point (point charge, uniformly charged sphere)
Cylindrical: Radially symmetric along the axis of a cylinder (infinite line of charge, uniformly charged cylinder)
Planar: Symmetric across a plane (infinite sheet of charge, uniformly charged parallel plates)
Applying Gauss's Law
Gauss's law for symmetrical charges
Gauss's law: ∮ E ⃗ ⋅ d A ⃗ = Q e n c ϵ 0 \oint \vec{E} \cdot d\vec{A} = \frac{Q_{enc}}{\epsilon_0} ∮ E ⋅ d A = ϵ 0 Q e n c
E ⃗ \vec{E} E : Electric field (a vector field representing the force per unit charge)
d A ⃗ d\vec{A} d A : Infinitesimal area element
Q e n c Q_{enc} Q e n c : Total charge enclosed by the Gaussian surface
ϵ 0 \epsilon_0 ϵ 0 : Permittivity of free space (8.85 × 1 0 − 12 C 2 N ⋅ m 2 8.85 \times 10^{-12} \frac{C^2}{N \cdot m^2} 8.85 × 1 0 − 12 N ⋅ m 2 C 2 )
Choose Gaussian surface that exploits symmetry of charge distribution
Spherical: Use concentric spherical surface
Cylindrical: Use coaxial cylindrical surface
Planar: Use parallel planar surface
Simplify integral by taking advantage of symmetry
Spherical: E ⃗ \vec{E} E constant in magnitude and perpendicular to surface at all points
Cylindrical: E ⃗ \vec{E} E constant in magnitude and perpendicular to curved surface
Planar: E ⃗ \vec{E} E constant in magnitude and perpendicular to surface
Solve for electric field magnitude using simplified integral
Spherical: E = Q e n c 4 π r 2 ϵ 0 E = \frac{Q_{enc}}{4\pi r^2 \epsilon_0} E = 4 π r 2 ϵ 0 Q e n c
Cylindrical: E = λ 2 π r ϵ 0 E = \frac{\lambda}{2\pi r \epsilon_0} E = 2 π r ϵ 0 λ (λ \lambda λ is linear charge density)
Planar: E = σ 2 ϵ 0 E = \frac{\sigma}{2\epsilon_0} E = 2 ϵ 0 σ (σ \sigma σ is surface charge density)
Electric Flux and Closed Surfaces
Electric flux is the measure of the electric field passing through a given surface
Gauss's law relates the electric flux through a closed surface to the enclosed charge
The closed surface used in Gauss's law is called a Gaussian surface
In electrostatics , the electric field and flux are time-independent
The superposition principle allows for the addition of electric fields from multiple charges