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Intro. to Elect 04
CO1_Introduction to Electricity - Gauss’ Law and Applications - #4
| Question | Answer |
|---|---|
| Electric Flux (Definition) | A measure of how many electric field lines pass through a surface. |
| Electric Flux Formula | Φ = E·A cosθ, where θ is the angle between E and the surface normal. |
| Positive vs Negative Flux | Positive flux: field lines leaving a surface; negative flux: entering a surface. |
| Closed Surface (Gaussian Surface) | An imaginary closed boundary used to apply Gauss’ Law. |
| Gauss’ Law (Statement) | The net electric flux through a closed surface equals the enclosed charge divided by ε₀. |
| Gauss’ Law Formula | Φ = Q_enclosed / ε₀. |
| Purpose of Gaussian Surfaces | Used to exploit symmetry to simplify electric field calculations. |
| Isolated Conductor (Definition) | A conductor not connected to other conductors or ground. |
| Charge on an Isolated Conductor | Excess charge resides entirely on the outer surface. |
| Electric Field Inside a Conductor | The electric field inside a conductor in electrostatic equilibrium is zero. |
| Cylindrical Symmetry (Example) | Infinite line of charge produces a radial electric field depending only on distance r. |
| Field from Cylindrical Symmetry | E = λ / (2π ε₀ r) for a long line of charge. |
| Planar Symmetry (Example) | Infinite charged plane produces a uniform electric field. |
| Field from Planar Symmetry | E = σ / (2ε₀) for an infinite sheet of charge. |
| Spherical Symmetry (Example) | A uniformly charged sphere behaves like a point charge outside the sphere. |
| Field from Spherical Symmetry | E = kQ/r² outside the sphere; inside, E ∝ r for uniform charge. |