Edits to “Statement”, “Solution”, “Answer”

JAMF edited
revision #18726 parent #18725 ← older
@@ -1,56 +1,28 @@
### Statement
−$14.3.7.$ [Insert the problem statement]
−
−### Solution
−
−\documentclass[12pt,a4paper]{article}
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−\usepackage{subcaption}
−
−\begin{document}
$14.3.7$ a. When moving at the speed $\vec{\beta c}$ of a state in which there was only an electric field, a magnetic field with induction $\vec{B}$
arises , associated with the new electric field $\vec{E}$ by the relation $\vec{B} = [\vec{\beta} \times \vec{E}]$. Prove this relation in the case
−when the old $\vec{E}$ is perpendicular to the velocity $\vec{\beta c}$\\
+when the old $\vec{E}$ is perpendicular to the velocity $\vec{\beta c}$
b. What magnetic field occurs when the electric field of intensity $\vec{E}$ moves at
the speed $\beta c$ if, $\beta = 1$?
−\begin{center}
− solution
−\end{center}
+### Solution
−a) In the moving frame there is no magnetic field, only a electric field. But in the Earth frame there are a electric field $\vec{E}$ and a magnetic field $\vec{B}$.
−For prove the relation we will use the loretnz transformation of the magnetic field for calculate the magnetic field in the moving field, this is zero:
+a) In the moving frame there is no magnetic field, only an electric field. But in the Earth frame there are an electric field $\vec{E}$ and a magnetic field $\vec{B}$.
+To prove the relation we will use the Lorentz transformation of the magnetic field to calculate the magnetic field in the moving frame; this is zero:
\begin{equation}
\vec{B}' = 0 = \frac{\vec{B} - [\vec{\beta} \times \vec{E}]}{\sqrt{1-\beta^2}} \rightarrow \vec{B} = [\vec{\beta} \times \vec{E}]
\end{equation}
−In the equations of before I set $c=1$ for simplify the calculations, fixing the equation of before:
+In the equations above I set $c=1$ to simplify the calculations. Restoring the equation to include $c$:
\begin{equation}
\vec{B} = \frac{[\vec{\beta} \times \vec{E}]}{c}
\end{equation}
−b) Using the equation of before we can calculate the magnetic fields in each case:
+b) Using the previous equation we can calculate the magnetic field in each case:
\begin{equation}
\vec{B} = \frac{[\vec{\beta} \times \vec{E}]}{c}
@@ -64,10 +36,18 @@Solution
\vec{B_c} = \frac{[\hat{\beta} \times \vec{E}]}{c}
\end{equation}
−Where $\hat{\beta}$ is the unitary vector in the direction of velocity. The magnetic field will be zero when the velocity were parallel to the electric field.
−
−\end{document}
+Where $\hat{\beta}$ is the unit vector in the direction of velocity. The magnetic field will be zero when the velocity is parallel to the electric field.
#### Answer
−[Insert a concise answer or boxed result]
+\begin{equation}
+ \vec{B} = \frac{[\vec{\beta} \times \vec{E}]}{c}
+\end{equation}
+
+\begin{equation}
+ \vec{B_1} = \frac{[\vec{\beta_1} \times \vec{E}]}{c}
+\end{equation}
+
+\begin{equation}
+ \vec{B_c} = \frac{[\hat{\beta} \times \vec{E}]}{c}
+\end{equation}