Calculate electric flux and electric field using Gauss's law Φ = Q/ε₀. Supports spherical, cylindrical, and planar symmetries with dielectric materials.
Gauss's law is one of Maxwell's four equations and provides the most elegant way to calculate electric fields when high symmetry is present. It states that the total electric flux through any closed surface equals the enclosed charge divided by the permittivity of the medium: Φ = Q_enc / ε.
This calculator applies Gauss's law for the three fundamental symmetries — spherical (point charges, charged spheres), cylindrical (long wires, coaxial cables), and planar (infinite sheets, parallel plates). For each geometry, it computes the electric flux, the electric field magnitude at the Gaussian surface, the electric potential (for spherical symmetry), and the energy density of the field.
Understanding Gauss's law is essential for physics students, electrical engineers designing capacitors and shielding, and anyone working with electrostatics. The calculator also accounts for dielectric materials through the relative permittivity (κ), showing how insulators reduce electric fields — a critical concept for capacitor design and high-voltage insulation engineering.
Gauss's law problems require choosing the right Gaussian surface and performing surface integrals. While the math simplifies beautifully with symmetry, setting up the calculation correctly and handling scientific notation (charges in microcoulombs, fields in kV/m) is error-prone. This calculator automates the geometry selection, unit handling, and derived quantity computation, letting you focus on physics rather than arithmetic.
Gauss's Law (integral form): Φ_E = ∮ E · dA = Q_enc / ε Spherical: E = Q / (4πεr²) Cylindrical: E = λ / (2πεr) where λ = Q/L Planar: E = σ / (2ε) where σ = Q/A Permittivity: ε = κε₀ ε₀ = 8.854 × 10⁻¹² F/m κ = relative permittivity (dielectric constant) Energy density: u = ½εE²
Result: E = 8.988 × 10⁵ N/C, Φ = 1.129 × 10⁵ N·m²/C
A +1 μC point charge enclosed by a spherical Gaussian surface of radius 0.1 m produces an electric flux of Q/ε₀ = 10⁻⁶/8.854×10⁻¹² ≈ 1.129×10⁵ N·m²/C. The electric field at the surface is E = Q/(4πε₀r²) ≈ 8.988×10⁵ N/C.
Gauss's law for electricity is the first of Maxwell's four equations. In differential form it reads ∇ · E = ρ/ε₀, connecting the divergence of the electric field to the local charge density. Together with Gauss's law for magnetism (∇ · B = 0), Faraday's law, and Ampère's law, it forms the complete description of classical electromagnetism.
Capacitor design relies heavily on Gauss's law. The field between parallel plates follows from planar symmetry: E = σ/ε, leading to capacitance C = εA/d. Coaxial cable shielding exploits cylindrical symmetry to confine fields between conductors. Faraday cages use the principle that enclosed charge determines interior flux — with no enclosed charge, the interior field is zero regardless of external fields.
While Gauss's law is easiest to apply in electrostatics, it holds for time-varying fields as well. The total flux through a closed surface still equals the enclosed charge even when fields change with time. However, in dynamic situations Faraday's law and the displacement current in Ampère's law also play essential roles, requiring the full set of Maxwell's equations.
Gauss's law says the total electric flux through any closed surface is proportional to the total charge enclosed within that surface. More charge means more flux lines passing through the surface.
Use Gauss's law when the charge distribution has high symmetry (spherical, cylindrical, or planar). Coulomb's law works for any configuration but requires summing contributions from each charge element, which can be very complex.
It is an imaginary closed surface you choose to apply Gauss's law. The surface should be chosen so that the electric field is either constant or zero over its entire area, making the flux integral trivial.
No. The total flux depends only on the enclosed charge, regardless of the surface shape. However, choosing a surface aligned with the field symmetry makes calculating E straightforward.
Electric flux measures the total number of electric field lines passing through a surface. Mathematically, it is the surface integral of E · dA. In SI units it is measured in N·m²/C or equivalently V·m.
A dielectric material with relative permittivity κ reduces the electric field by a factor of κ compared to vacuum. For example, water (κ ≈ 80) reduces the field to about 1/80th of the vacuum value, which is why water is an effective electrostatic shield.