Notes
Coulomb's law and fields
- $\displaystyle F = \frac{1}{4\pi\varepsilon_0}\frac{|q_1q_2|}{r^2}$, where $\displaystyle \frac{1}{4\pi\varepsilon_0} = k = 9.0 \times 10^9$ N·m²/C².
- $\displaystyle \vec E = \frac{\vec F}{q_0}$. Point charge: $\displaystyle E = \frac{kq}{r^2}$.
- Continuous distributions: $\displaystyle \vec E = \int\frac{k\,dq}{r^2}\hat r$, with $dq = \lambda\,dx$, $\sigma\,dA$, or $\rho\,dV$. Use symmetry to cancel components first.
- On the axis of a ring of charge $Q$, radius $a$: $\displaystyle E = \frac{kQx}{(x^2 + a^2)^{3/2}}$.
Electric flux and Gauss's law
- Flux: $\Phi_E = \oint\vec E \cdot d\vec A$.
- Gauss's law: $\displaystyle \oint\vec E \cdot d\vec A = \frac{Q_{enc}}{\varepsilon_0}$.
- Choose a Gaussian surface that matches the symmetry so $E$ is constant on it:
| Charge distribution | Gaussian surface | Result |
|---|---|---|
| Point charge or sphere (outside) | Sphere | $\displaystyle E = \frac{kQ}{r^2}$ |
| Long line of charge $\lambda$ | Cylinder | $\displaystyle E = \frac{\lambda}{2\pi\varepsilon_0r}$ |
| Infinite plane $\sigma$ | Pillbox | $\displaystyle E = \frac{\sigma}{2\varepsilon_0}$ |
| Uniform solid sphere, inside ($r < R$) | Sphere | $\displaystyle E = \frac{kQr}{R^3}$ |
- Flux through a closed surface depends only on enclosed charge, not on the surface's shape or charges outside.
Practice
$\displaystyle \frac{(9.0 \times 10^9)(4.0 \times 10^{-6})}{4.0}$.
Only enclosed charge counts.
A cylinder matches the line's symmetry.
$\displaystyle E = \frac{\lambda}{2\pi\varepsilon_0r}$.
By symmetry, contributions from opposite sides cancel; also $x = 0$ in the formula.
$Q_{enc} \propto r^3$, so $\displaystyle E \propto \frac{r^3}{r^2} = r$.
An infinite plane gives a field independent of distance.
Flux in equals flux out; there's no enclosed charge.
Free response
Write your answer first, then open the scoring guide.
Free-response question
A solid insulating sphere of radius $R$ has a volume charge density $\rho(r) = \beta r$, where $\beta$ is a positive constant.
(a) Find the total charge $Q$ of the sphere.
Show the answer and scoring guide
$\displaystyle Q = \int_0^R \beta r(4\pi r^2)\,dr = 4\pi\beta\frac{R^4}{4} = \pi\beta R^4$.
Check off the points you earned:
(b) Use Gauss's law to find $E$ inside the sphere ($r < R$).
Show the answer and scoring guide
$Q_{enc} = \pi\beta r^4$. $\displaystyle E(4\pi r^2) = \frac{\pi\beta r^4}{\varepsilon_0} \Rightarrow E = \frac{\beta r^2}{4\varepsilon_0}$.
Check off the points you earned:
(c) Find $E$ outside the sphere ($r > R$).
Show the answer and scoring guide
$\displaystyle E(4\pi r^2) = \frac{\pi\beta R^4}{\varepsilon_0} \Rightarrow E = \frac{\beta R^4}{4\varepsilon_0r^2}$.
Check off the points you earned: