From 3686efed92c14691be54cbd387f093de148585e8 Mon Sep 17 00:00:00 2001 From: "W. Trevor King" Date: Wed, 11 Apr 2012 17:54:02 -0400 Subject: [PATCH] Update MetaPost to Asymptote in Serway and Jewett v4's problem 19.13. --- .../Serway_and_Jewett_4/problem19.13.tex | 84 +++++++++---------- 1 file changed, 40 insertions(+), 44 deletions(-) diff --git a/latex/problems/Serway_and_Jewett_4/problem19.13.tex b/latex/problems/Serway_and_Jewett_4/problem19.13.tex index b722de8..598b314 100644 --- a/latex/problems/Serway_and_Jewett_4/problem19.13.tex +++ b/latex/problems/Serway_and_Jewett_4/problem19.13.tex @@ -1,63 +1,59 @@ \begin{problem*}{19.13} Three point charges are arranged as shown in Figure P19.13.\\ -%\begin{center} -% \begin{tabular}{|l|r|r|r|} -% Name & Charge (nC) & x (m) & y (m) \\ -% \hline -% $q_1$ & $5.00$ & $0$ & $0$ \\ -% $q_2$ & $6.00$ & $0.300$ & $0$ \\ -% $q_3$ & $-3.00$ & $0$ & $-0.100$ \\ -% \hline -% \end{tabular} -%\end{center} \Part{a} Find the vector electric field \vect{E} that $q_2$ and $q_3$ together create at the origin. \Part{b} Find the vector force \vect{F} on $q_1$. \end{problem*} % problem 19.13 -\empaddtoprelude{ - numeric a; - pair A, B, C; - a := 3cm; - A := origin; % q1 - B := (a,0); % q2 - C := (0,-a/3); % q3 - def drawB = - label.top(btex 0.300\mbox{ m} etex, draw_length(B, A, 8pt)); - label.lft(btex 0.100\mbox{ m} etex, draw_length(A, C, 8pt)); - labeloffset := 6pt; - draw_pcharge(A, 4pt); - label.rt(btex $q_1 = 5\mbox{ nC}$ etex, A); - draw_pcharge(B, 4.2pt); - label.rt(btex $q_2 = 6\mbox{ nC}$ etex, B); - draw_ncharge(C, 3pt); - label.rt(btex $q_3 = -3\mbox{ nC}$ etex, C); - enddef; -} - \begin{nosolution} \begin{center} -\begin{empfile}[2p] -\begin{emp}(0cm,0cm) - drawB; -\end{emp} -\end{empfile} +\begin{asy} +import ElectroMag; + +real u = 20cm; +draw_ijhat(); +Charge a = aCharge((0, 0), q=5, Label("$q_1=5.00\U{nC}$", align=W)); +a.draw(); +Charge b = aCharge((0.3u, 0), q=6, Label("$q_2=6.00\U{nC}$", align=S)); +b.draw(); +Charge c = aCharge((0, -0.1u), q=-3, Label("$q_3=-3.00\U{nC}$", align=S)); +c.draw(); +Distance dab = Distance(a.center(), b.center(), offset=-24pt, L="$0.300\U{m}$"); +dab.draw(); +Distance dac = Distance(a.center(), c.center(), L="$0.100\U{m}$"); +dac.draw(); +\end{asy} \end{center} \end{nosolution} \begin{solution} \begin{center} -\begin{empfile}[2] -\begin{emp}(0cm,0cm) - label.lft(btex $E_{21}$ etex, draw_Efield(B, A, a/8)); - label.rt(btex $E_{31}$ etex, draw_Efield(C, A, -a/5)); - draw_ijhats(-(a, a/3), 0, a/6); - drawB; -\end{emp} -\end{empfile} +\begin{asy} +import ElectroMag; + +real u = 20cm; +draw_ijhat(); +Charge a = aCharge((0, 0), q=5, Label("$q_1=5.00\U{nC}$", align=dir(160))); +a.draw(); +Charge b = aCharge((0.3u, 0), q=6, Label("$q_2=6.00\U{nC}$", align=S)); +b.draw(); +Charge c = aCharge((0, -0.1u), q=-3, Label("$q_3=-3.00\U{nC}$", align=S)); +c.draw(); +Distance dab = Distance(a.center(), b.center(), offset=-24pt, L="$0.300\U{m}$"); +dab.draw(); +Distance dac = Distance(a.center(), c.center(), offset=-24pt, + L=Label("$0.100\U{m}$", align=LeftSide)); +dac.draw(); +Charge cs[] = {b, c}; +string subscripts[] = {"2", "3"}; +CoulombEFields(a.center(), cs, subscripts, scale=0.1u, unit=0.03u); +Vector F = CoulombForce(b, a, scale=0.1u, unit=0.006u) + + CoulombForce(c, a, scale=0.1u, unit=0.006u); +F.label = Label("$F$", position=EndPoint, align=RightSide); +F.draw(); +\end{asy} \end{center} \Part{a} -\begin{equation} \begin{equation} \vect{E} = k_e \sum_i \frac{q_i}{r_i^2}\rhat_i = k_e \left[\frac{q_2}{x_2^2}(-\ihat) + \frac{q_3}{y_3^2}\jhat\right] -- 2.26.2