#+STARTUP: entitiespretty fold inlineimages #+LATEX_HEADER: \usepackage{ dsfont } \usepackage{amsmath} \usepackage[a4paper,margin=1in,portrait]{geometry} #+LATEX: #+OPTIONS: toc:nil * a ** 26 *** B from x_{dist} On axis of a current loop of radius a $B = \frac{\mu_0 I a^2}{2(x_{dist}_{}^2 + a^2)^{3/2}}$ *** B on axis from magnetic dipole $B = \frac{\mu_0}{2 \pi} \frac{\mu}{x^3}$ *** Net Torque on closed loop with area A at orientation \theta $\tau = I A B \text{sin}(\theta)$ *** Field outside, inside any current distribution with line symmetry $B = \frac{\mu_0 I}{2 \pi r}$ $B = \frac{\mu_0 I r_{inside}}{2 \pi R_{outside}^2}$ *** Sheet with uniform current density J *** Solenoid with turns n per unit length ** 27 *** Flux through solenoid with n turns per unit length $\phi_B = BA = \mu_0 n I \pi R^2$ *** Flux through rectangular loop with $l$ parallel to wire at distance $a$ $\phi_B = \int B dA = \int_{a}^{a+w} \frac{\mu_0 I}{2 \pi r} l dr = \frac{\mu_0 I l}{2 \pi} \text{ln}(\frac{a+w}{a})$ *** Induced current through circuit with bars at distance $l$ and moving bar velocity $v$ $I = \frac{Blv} {r}$ *** Flux through coil with $N$ turns turning at frequency $f$ in field $B$ $\phi_B = N B \pi r^2 \text{cos}(2 \pi f t)$ $E = - \frac{d \phi_B}{dt}$ *** Inductance of a solenoid $L = \frac{\phi_B}{I} = \mu_0 n^2 A l$ *** Electric field of a solenoid of radius $R$ at loop radius $r$ with $B = bt$ $E = \frac{R^2 b}{2r}$