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Applications of Gauss's Law to Wire, Sheet and Shell

Applications of Gauss's law use symmetry to find electric field due to charge distributions such as an infinitely long line charge, an infinite plane sheet, and a uniformly charged spherical shell.

In one line: Line uses cylinder, sheet uses pillbox, shell uses sphere.

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Understand it

  • Gauss's law is most useful when a Gaussian surface can be chosen so that electric field is either constant and parallel to area vectors, or perpendicular to area vectors and gives zero flux.
  • For an infinitely long line charge, a coaxial cylinder is used and E = λ/(2πε0r).
  • For an infinite plane sheet, a pillbox surface gives E = σ/(2ε0) on either side.
  • For a spherical shell, a concentric sphere shows E = 0 inside the shell and outside field behaves as if total charge were concentrated at the centre.

Example

For a long straight line charge with λ = 4 × 10−6 C m−1 at r = 0.20 m, E = λ/(2πε0r) = (2kλ)/r = (2)(9 × 109)(4 × 10−6)/0.20 = 3.6 × 105 N C−1 radially outward for positive λ.

Formula and rule

Infinite line charge: E = λ/(2πε0r), λ in C m−1, r in m.

Infinite plane sheet: E = σ/(2ε0), σ in C m−2, independent of distance for an ideal infinite sheet.

Spherical shell: E = 0 inside; outside E = (1/4πε0)(Q/r2), as if charge were at centre.

Conditions: ideal symmetry, electrostatic equilibrium where applicable, and suitable Gaussian surface.

See it worked out

Follow the example line by line, then use the same method on new questions.

Worked example

A uniformly charged infinite plane sheet has σ = 3.54 × 10−6 C m−2.

  1. 1Electric field on either side is E = σ/(2ε0) = (3.54 × 10−6)/(2 × 8.85 × 10−12) = 2.0 × 105 N C−1.
  2. 2For positive σ, field is normal to the sheet and away from it on both sides.

Method you can reuse

  1. 1Identify symmetry of charge distribution.
  2. 2Choose matching Gaussian surface.
  3. 3Mark direction of E and dA.
  4. 4Find where E·dA contributes and where it is zero.
  5. 5Write flux in simplified form.
  6. 6Put qenclosed in terms of λ, σ, or Q.
  7. 7Solve for E and state direction and valid region.

Visual tip

Useful diagrams: cylindrical Gaussian surface around line charge, pillbox crossing plane sheet, and concentric spherical Gaussian surfaces inside and outside a charged shell. Labels should show symmetry axis, radius r, area vectors, enclosed charge, and field direction.

Check yourself

Answer the question in your head before opening the answer.

Try it yourself

Why is the electric field inside a uniformly charged spherical shell zero?

Think first, then show answer
Choose a spherical Gaussian surface inside the shell. It encloses no charge, so by Gauss's law the net flux is zero. By spherical symmetry, the only possible constant radial field on that surface must therefore be zero.

Common wrong answer

Using E = σ/ε0 for a single infinite non-conducting sheet is wrong in this context; the standard result is E = σ/(2ε0) on each side.

Don't mix this up

Students memorize formulas but use them for finite wires, finite sheets, or non-uniform charge distributions without the required symmetry.

Exam tip

Name the Gaussian surface in derivations: cylinder for line charge, pillbox for sheet, concentric sphere for shell. This shows why the flux integral becomes simple.

Write it in the exam

Each point is worth about one mark. Write point 1 for a 1-mark question and keep adding points as the marks go up.

How CBSE asks it

Asked mainly as derivations and comparison questions: field variation with distance for line, sheet, and shell; field inside a shell; and selecting the correct Gaussian surface.
  1. 1

    Enough for 1 mark

    Applications of Gauss's law use symmetry to find electric field due to charge distributions such as an infinitely long line charge, an infinite plane sheet, and a uniformly charged spherical shell.

  2. 2

    Add for 2 marks

    Example: For a long straight line charge with λ = 4 × 10−6 C m−1 at r = 0.20 m, E = λ/(2πε0r) = (2kλ)/r = (2)(9 × 109)(4 × 10−6)/0.20 = 3.6 × 105 N C−1 radially outward for positive λ.

  3. 3

    Add for 3 marks

    Gauss's law is most useful when a Gaussian surface can be chosen so that electric field is either constant and parallel to area vectors, or perpendicular to area vectors and gives zero flux.

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