PHYS7021
Burdwan · Electricity, Magnetism & Wave Optics · 2018–2024

1B · Fields by Gauss Law — Sphere, Cylinder, Zero-Point + Solved PYQs

Solid sphere outside/inside with graph, U-nucleus number, charged cylinder, zero-field point. Full steps.

78 core Q 129 appearances 45 h syllabus SI units · KaTeX

This page applies Gauss's law to common charge distributions. We derive the field of a uniformly charged solid sphere (outside and inside), an infinite line charge (cylinder), and solve the zero-field-point problem for two like charges. Each application starts by naming the right Gaussian surface.

1. Uniformly charged solid sphere

Sphere of radius $R$ carries total charge $Q$ spread uniformly through its volume. Volume charge density $\rho = Q/(\tfrac{4}{3}\pi R^3)$. Symmetry: there is no preferred direction, so the field is purely radial and depends only on $r$.

1.1 Outside the sphere ($r > R$)

Take a concentric Gaussian sphere of radius $r$. It encloses the full charge $Q$. Apply Gauss's law: $E\cdot 4\pi r^2 = Q/\varepsilon_0$.

Formula 1. Field outside a uniformly charged solid sphere $\boxed{E_{\text{out}} = \dfrac{Q}{4\pi\varepsilon_0 r^2}}$ — same as a point charge $Q$ at the centre.

1.2 Inside the sphere ($r < R$)

The Gaussian sphere of radius $r$ encloses only the charge inside that radius. Volume scales as $r^3$, so $Q_{\text{in}} = Q\,(r/R)^3 = Q\,r^3/R^3$. Apply Gauss's law: $E\cdot 4\pi r^2 = Q\,r^3/\varepsilon_0 R^3$.

Formula 2. Field inside a uniformly charged solid sphere $\boxed{E_{\text{in}} = \dfrac{Q\,r}{4\pi\varepsilon_0 R^3}}$ — grows linearly from 0 at the centre to a maximum $E_{\max} = Q/4\pi\varepsilon_0 R^2$ at $r = R$.
Graph of E versus r for a solid charged sphere: straight-line rise from 0 to R then 1/r-squared fall
Fig 1.1: $E$ vs $r$ for the solid sphere. Straight line through the origin is Eq. (2); $1/r^2$ falling curve is Eq. (1); peak $E_{\max} = Q/4\pi\varepsilon_0 R^2$ occurs at $r = R$.
Note. At the centre ($r = 0$), Eq. (2) gives $E = 0$. For a thin shell, $E = 0$ everywhere inside because $Q_{\text{in}} = 0$ at every interior point.

2. Other Gauss-law results

Each result comes from choosing the Gaussian surface that matches the symmetry of the charge distribution.

Infinite line charge with coaxial Gaussian cylinder, radial E arrows
Fig 1.2: infinite line charge $\lambda$. The coaxial Gaussian cylinder of radius $r$ and length $l$ catches flux only through its curved face, giving $E = \lambda/2\pi\varepsilon_0 r$ (Eq. 3a).
Formula 3. Useful Gauss-law fields · (a) Infinite line charge, linear density $\lambda$: $\boxed{E = \lambda/2\pi\varepsilon_0 r}$ (radially out; coaxial Gaussian cylinder). · (b) Thin spherical shell of charge $Q$: outside $E = Q/4\pi\varepsilon_0 r^2$; inside $\boxed{E = 0}$. · (c) Infinite plane sheet, surface density $\sigma$: $\boxed{E = \sigma/2\varepsilon_0}$ on each side (flat Gaussian pillbox). · (d) Charged conductor: all charge on outer surface; field just outside $\boxed{E = \sigma/\varepsilon_0}$ (normal to surface); $E = 0$ inside the metal.
Charged sheet with Gaussian pillbox, E arrows on both sides
Fig 1.3: infinite plane sheet with surface density $\sigma$. The Gaussian pillbox straddles the sheet; flux leaves through both flat faces, giving $E = \sigma/2\varepsilon_0$ on each side (Eq. 3c).

Solved PYQs

Q1

Using Gauss's law, find the field of a uniformly charged solid sphere outside and inside. Show the graphical variation and prove the field is zero inside (at the centre).

×220182023

Recall

Gauss's law $\oint \vec{E}\cdot d\vec{S} = Q_{\text{in}}/\varepsilon_0$ plus spherical symmetry: $\vec{E} = E(r)\hat{r}$, so flux on a concentric sphere is $E\cdot 4\pi r^2$.

Steps

  1. State the symmetry: $\vec{E} = E(r)\hat{r}$, so on a concentric Gaussian sphere, $\Phi = E(r)\cdot 4\pi r^2$.
  2. Outside ($r > R$): enclosed charge is the full $Q$; Gauss's law gives $E = Q/4\pi\varepsilon_0 r^2$ (point-charge form).
  3. Inside ($r < R$): enclosed charge scales with volume, $Q_{\text{in}} = Q\,r^3/R^3$; Gauss's law gives $E = Q\,r/4\pi\varepsilon_0 R^3$ (linear in $r$).
  4. At the centre ($r = 0$): Eq. (2) gives $E = 0$. For a thin shell, $Q_{\text{in}} = 0$ everywhere inside, so $E = 0$ throughout.
  5. Graph: straight line from origin to $(R, E_{\max})$, then a $1/r^2$ falling curve — as in Fig 1.1.

Answer

$\boxed{E_{\text{out}} = \dfrac{Q}{4\pi\varepsilon_0 r^2},\ E_{\text{in}} = \dfrac{Q\,r}{4\pi\varepsilon_0 R^3},\ E(0) = 0}$. Both forms give N/C.

Exam tip

Label $E_{\max}$ at $r = R$ on the graph — examiners look for the peak value and its location.
Q2

Calculate the electric field on the surface of a $^{238}_{92}$U nucleus (radius $7\times 10^{-15}$ m). Take $\varepsilon_0 = 8.85\times 10^{-12}$ C²/N·m², $e = 1.6\times 10^{-19}$ C.

2018

Recall

Outside a sphere the field has the point-charge form $E = Q/4\pi\varepsilon_0 r^2$, with $1/4\pi\varepsilon_0 = 9\times 10^9$ N·m²/C².

Steps

  1. Charge of the nucleus: $Q = 92\,e = 92\times 1.6\times 10^{-19} = 1.472\times 10^{-17}$ C (reason: 92 protons).
  2. At the surface $r = R$: $E = \dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{R^2}$ with $1/4\pi\varepsilon_0 = 9\times 10^9$ N·m²/C².
  3. Numerator: $9\times 10^9\times 1.472\times 10^{-17} = 1.3248\times 10^{-7}$ N·m²/C.
  4. Denominator: $R^2 = (7\times 10^{-15})^2 = 49\times 10^{-30}$ m².
  5. Divide: $E = \dfrac{1.3248\times 10^{-7}}{49\times 10^{-30}} = 2.7\times 10^{21}$ N/C, radially outward (reason: positive charge pushes a test charge away).

Answer

$\boxed{E \approx 2.7\times 10^{21}\ \text{N/C, directed radially outward}}$ · Unit N/C · The huge value is reasonable: the nucleus is tiny and holds 92 protons.

Exam tip

Always write $Q = 92\,e$ explicitly. Forgetting the 92 is the common zero-mark error.
Q3

Using Gauss's theorem, find the electric field intensity at a point due to a charged cylinder (long line of charge).

2022

Recall

Cylindrical symmetry → use a coaxial Gaussian cylinder. Flux only crosses the curved face (flat caps have $\vec{E}\perp d\vec{S}$, giving zero flux).

Steps

  1. Let charge per unit length be $\lambda$. Draw a coaxial Gaussian cylinder of radius $r$ and length $l$.
  2. Flux through the curved face only: $\Phi = E\cdot 2\pi r l$ (reason: $\vec{E}\parallel d\vec{S}$ on curved face; on caps $\vec{E}\perp d\vec{S}$, so they contribute 0).
  3. Enclosed charge: $Q_{\text{in}} = \lambda l$. Apply Gauss's law: $E\cdot 2\pi r l = \lambda l/\varepsilon_0$.
  4. Cancel $l$: $E = \lambda/2\pi\varepsilon_0 r$, radially outward (reason: charge is positive).

Answer

$\boxed{E = \dfrac{\lambda}{2\pi\varepsilon_0 r}}$ (outside an infinite line of charge) · For a thin charged shell, $E = 0$ inside. Unit: N/C.

Exam tip

If the question is about a solid cylinder (volume charge $\rho$), the inside field becomes $E = \rho\,r/2\varepsilon_0$ — state which case you are solving.
Q4

Two charges $8\ \mu$C and $2\ \mu$C are placed 50 cm apart in air. At which point is the electric field intensity zero?

2023

Recall

Field of a point charge $E = kq/r^2$ with $k = 9\times 10^9$ N·m²/C². For two like charges, the zero-field point lies between them, closer to the smaller charge.

Steps

  1. Let the point be at distance $x$ from $8\ \mu$C along the line joining the charges, so it is $(50 - x)$ cm from $2\ \mu$C. Between them the two fields point in opposite directions (reason: each charge pushes a test charge away from itself).
  2. Set the magnitudes equal: $\dfrac{k\cdot 8}{x^2} = \dfrac{k\cdot 2}{(50-x)^2}$. Cancel $k$: $\dfrac{8}{x^2} = \dfrac{2}{(50-x)^2}$.
  3. Take square roots (cleaner than expanding squares): $\dfrac{\sqrt{8}}{x} = \dfrac{\sqrt{2}}{50-x}$ → $\dfrac{2\sqrt{2}}{x} = \dfrac{\sqrt{2}}{50-x}$ → $\dfrac{2}{x} = \dfrac{1}{50-x}$.
  4. Cross-multiply: $2(50 - x) = x$ → $100 - 2x = x$ → $3x = 100$ → $x = 33.3$ cm.
  5. Check: from $2\ \mu$C, the distance is $50 - 33.3 = 16.7$ cm. Verify: $8/(33.3)^2 \approx 2/(16.7)^2 \approx 0.0072$. ✓

Answer

$\boxed{33.3\ \text{cm from the } 8\ \mu\text{C charge (16.7 cm from the } 2\ \mu\text{C), lying between them}}$.

Exam tip

Always take the square root before expanding. Expanding the squares wastes time and invites algebra slips.
Q5

State Coulomb's theorem (Coulomb's law) in electrostatics.

2022

Recall

Force between two point charges $q_1$, $q_2$ distance $r$ apart: $F = \dfrac{1}{4\pi\varepsilon_0}\dfrac{q_1 q_2}{r^2}$, directed along the line joining them.

Steps

  1. State the law: the force is proportional to the product of the charges and inversely proportional to the square of the distance between them.
  2. Write the vector form: $\vec{F}_{12} = \dfrac{1}{4\pi\varepsilon_0}\dfrac{q_1 q_2}{r^2}\,\hat{r}_{12}$, where $\hat{r}_{12}$ points from $q_1$ to $q_2$.
  3. Give the constant: $1/4\pi\varepsilon_0 = 9\times 10^9$ N·m²/C². Like charges repel, unlike charges attract.
  4. Note the conditions: point charges (or spherically symmetric), at rest, in vacuum (in a medium replace $\varepsilon_0 \to \varepsilon$).

Answer

$\boxed{F = \dfrac{1}{4\pi\varepsilon_0}\dfrac{q_1 q_2}{r^2}}$ along the line joining the charges · $1/4\pi\varepsilon_0 = 9\times 10^9$ N·m²/C².

Exam tip

Write the vector form with $\hat{r}_{12}$ — the direction line is a separate mark from the magnitude.
Q6

Calculate the force with which two electrons at a distance of $1.1$ Å in the hydrogen atom repel each other. What is the nature of the electrostatic field energy?

2018

Recall

Coulomb's law $F = k e^2/r^2$ with $k = 9\times 10^9$ N·m²/C², $e = 1.6\times 10^{-19}$ C. Potential energy $U = k e^2/r$.

Steps

  1. Convert: $r = 1.1$ Å $= 1.1\times 10^{-10}$ m, so $r^2 = 1.21\times 10^{-20}$ m².
  2. Numerator: $k e^2 = 9\times 10^9 \times (1.6\times 10^{-19})^2 = 9\times 10^9 \times 2.56\times 10^{-38} = 2.304\times 10^{-28}$ N·m².
  3. Divide: $F = 2.304\times 10^{-28} / 1.21\times 10^{-20} = 1.90\times 10^{-8}$ N, repulsive (reason: like charges repel).
  4. Field energy: the electrostatic potential energy $U = +k e^2/r > 0$ — positive because work must be done against repulsion to bring the electrons together. The energy is stored in the field.

Answer

$\boxed{F \approx 1.9\times 10^{-8}\ \text{N (repulsive)}}$ · Field energy $\boxed{U = +ke^2/r > 0}$ — positive, stored in the field.

Exam tip

Convert Å → m first ($1$ Å $= 10^{-10}$ m). The sign of $U$ is the second mark — repulsive means positive energy.

Reference. Brij Lal & Subrahmanyam, Electricity & Magnetism Ch-2 (Gauss applications: sphere, line, shell, sheet, conductor); S.L. Arora Vol-1 Ch-1.

▶ Watch on YouTube

Search these topics to complete this page's syllabus: