# HW4 - \documentclass[12pt]cfw_article \textheight 9.0in...

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\documentclass[12pt]{article} \textheight 9.0in \textwidth 6.0in \topmargin -0.4in \headsep 0.4in \oddsidemargin 0.25in \evensidemargin 0.25in \def\pmbf#1{{\mbox{\boldmath${#1}$}}} \def\undertext#1{$\underline{\smash{\hbox{#1}}}$} \pagestyle{empty} \begin{document} %----------------------------------------------------% %%%%%%%%%%%%%%%%% CLASSICAL MECHANICS %%%%%%%%%%%%%%%% %----------------------------------------------------% \begin{center} {\bf ADVANCED DYNAMICS --- PHY--4241/5227}\\\vspace {2mm} {\bf HOMEWORK 4}\\% \vspace {3mm} (\today) \\ \vspace {1mm}{Due on Monday, February 3, 2003} \\ \end{center} \setcounter{equation}{0} \bigskip %%%%%%%%%%%%%%%%%%%%%%%%%% \centerline{\bf PROBLEM 10} \medskip A particle of mass $m$ and electric charge $q$ moves under the influence of a constant magnetic field of the form ${\bf B}({\bf r})\!=\!B_0\hat{\bf z}$. Obtain the most general solution for the velocity ${\bf v}(t)$ using Newton's second law of motion in combination with the Lorentz force. That is,

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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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HW4 - \documentclass[12pt]cfw_article \textheight 9.0in...

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