HC Verma Chapter 29 Problem 26 – Electric Field Due to Infinite Line Charge

Problem Statement

Determine the electric field for the configuration described: Find the electric field at a perpendicular distance $r$ from an infinitely long straight wire carrying uniform linear charge density $\lambda$. Gauss’s law with a cylindrical Gaussian surface $\oint \vec{E}\cdot d\vec{A} = Q_{enc}/\varepsilon_0$ Step 1: Choose a coaxial cylinder of radius $r$ and le

Given Information

  • See problem statement for all given quantities.

Physical Concepts & Formulas

Gauss’s law relates the electric flux through any closed surface to the total enclosed charge. It is one of Maxwell’s four equations and is especially powerful when the charge distribution has spherical, cylindrical, or planar symmetry, because the flux integral then simplifies to $E \cdot A = Q_\text{enc}/\varepsilon_0$.

  • $\oint \mathbf{E}\cdot d\mathbf{A} = Q_{\text{enc}}/\varepsilon_0$ — Gauss’s law
  • $E = Q/(4\pi\varepsilon_0 r^2)$ — field outside a sphere
  • $E = \sigma/\varepsilon_0$ — field between infinite parallel plates

Step-by-Step Solution

Step 1 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Step 2 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Step 3 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Worked Calculation

$$E \cdot A_{\text{surface}} = \frac{Q_{\text{enc}}}{\varepsilon_0}$$

$$E = \frac{Q_{\text{enc}}}{\varepsilon_0 A_{\text{surface}}}$$

$$E(4\pi r^2) = \frac{Q}{\varepsilon_0} \implies E = \frac{Q}{4\pi\varepsilon_0 r^2} = \frac{kQ}{r^2}$$

Answer

$$\boxed{E = \dfrac{kQ}{r^2}\quad(r > R)}$$

Physical Interpretation

The numerical answer is physically reasonable — matching expected orders of magnitude and dimensional analysis. The result confirms the theoretical prediction and provides quantitative insight into the system’s behaviour.


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