# a14 - \documentclass[12pt]cfw_article % BB Apr 06 2009....

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\documentclass[12pt]{article} % BB Apr 06 2009. \usepackage{epsfig} \textheight 9.0in \textwidth 6.0in \topmargin -0.4in \headsep 0.4in \oddsidemargin 0.25in \evensidemargin 0.25in \def\sqr#1#2{{\vcenter{\hrule height.#2pt \hbox{\vrule width.#2pt height#1pt \kern#1pt \vrule width.#2pt} \hrule height.#2pt}}} \def\square{{\mathchoice\sqr64\sqr64\sqr{4.2}3\sqr{3.0}3}} \def\undertext#1{$\underline{\smash{\hbox{#1}}}$} \pagestyle{empty} \begin{document} \begin{center} {\bf ADVANCED DYNAMICS --- PHY 4241/5227}\\\vspace {2mm} {\bf HOME AND CLASS WORK -- SET 14}\\% \vspace {3mm} (April 13, 2009) \\ \end{center} \setcounter{equation}{0} \begin{description} \item{(58)} The electromagnetic field tensor transforms according to $$F'^{\, \alpha\beta} = a^{\alpha}_{\ \gamma} a^{\beta}_{\ \delta} F^{\gamma\delta}\, .$$ \begin{enumerate} \item Choose the particular case of a Lorentz boost in $x^1$-direction, $\vec{v}=v\, \hat{e}_1$, and write down the transformation law for the electric field $\vec{E}$ and the magnetic induction

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## This note was uploaded on 11/10/2011 for the course PHY 4241 taught by Professor Berg during the Spring '11 term at University of Florida.

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a14 - \documentclass[12pt]cfw_article % BB Apr 06 2009....

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