<?xml version="1.0" encoding="UTF-8"?>

<record version="8" id="201">
 <title>Vector Identities</title>
 <name>VectorIdentities</name>
 <created>2006-07-20 18:59:21</created>
 <modified>2008-05-27 16:18:20</modified>
 <type>Definition</type>
 <creator id="1" name="bloftin"/>
 <modifier id="1" name="bloftin"/>
 <author id="1" name="bloftin"/>
 <classification>
	<category scheme="msc" code="02."/>
 </classification>
 <synonyms>
	<synonym concept="Vector Identities" alias="vector relationships"/>
 </synonyms>
 <keywords>
	<term>Vector Identities</term>
 </keywords>
 <preamble>% this is the default PlanetMath preamble.  as your knowledge
% of TeX increases, you will probably want to edit this, but
% it should be fine as is for beginners.

% almost certainly you want these
\usepackage{amssymb}
\usepackage{amsmath}
\usepackage{amsfonts}

% used for TeXing text within eps files
%\usepackage{psfrag}
% need this for including graphics (\includegraphics)
%\usepackage{graphicx}
% for neatly defining theorems and propositions
%\usepackage{amsthm}
% making logically defined graphics
%\usepackage{xypic}

% there are many more packages, add them here as you need them

% define commands here</preamble>
 <content>It is difficult to get anywhere in physics without a firm understanding of vectors and their common operations.  Here, we will give vector identities as a reference.  Basic terminology to keep straight.

\begin{table}[t]
\begin{center}
\begin{tabular}{cc}
\\ [.3ex] \hline \\ [.3ex]

{\bf Operation} &amp; {\bf Symbol} \\ [0.5ex]
%heading
\hline \\ [.3ex]

Gradient &amp; $\nabla f$ \\
Laplacian &amp; $\nabla^2$ \\
Divergence &amp; $\nabla \cdot$ \\
Curl &amp; $\nabla \times$ \\

\hline
\end{tabular}
\end{center}
\end{table}

{\bf Vector Magnitude}

$ A =  \left | \mathbf{A} \right | = \sqrt{{A_x}^2 + {A_y}^2 + {A_z}^2 }$\\
$ A =  \sqrt{\mathbf{A} \cdot \mathbf{A}} $

{\bf Scalar Product (Dot Product)}

$ \mathbf{A} \cdot \mathbf{B} = A_x B_x + A_y B_y + A_z B_z$ \\
$ \mathbf{A} \cdot \mathbf{B} = \left | \mathbf{A} \right | \left | \mathbf{B} \right | \cos \theta$


{\bf Vector Product (Cross Product)}

$ \mathbf{A} \times \mathbf{B} = \left ( A_y B_z - A_z B_y \right ) \mathbf{\hat{i}} + \left ( A_z B_x - A_x B_z \right ) \mathbf{\hat{j}} + \left ( A_x B_y - A_y B_x \right ) \mathbf{\hat{k}}$

It can be easier to remember with determinant formulation

$ \mathbf{A} \times \mathbf{B} = \left| \begin{matrix}
\mathbf{\hat{i}} &amp; \mathbf{\hat{j}} &amp; \mathbf{\hat{k}} \\
A_x &amp; A_y &amp; A_z \\
B_x &amp; B_y &amp; B_z
\end{matrix}\right| = \left ( A_y B_z - A_z B_y \right ) \mathbf{\hat{i}} + \left ( A_z B_x - A_x B_z \right ) \mathbf{\hat{j}} + \left ( A_x B_y - A_y B_x \right ) \mathbf{\hat{k}}$

{\bf Vector Triple Product, aka. BAC CAB}

$ \mathbf{A} \times \left ( \mathbf{B} \times \mathbf{C} \right ) = \mathbf{B} \left( \mathbf{A} \cdot \mathbf{C} \right ) - \mathbf{C} \left ( \mathbf{A} \cdot \mathbf{B} \right) $

{\bf Scalar Triple Product}

$ \mathbf{A} \cdot \left ( \mathbf{B} \times \mathbf{C} \right ) = \mathbf{B} \cdot \left ( \mathbf{C} \times \mathbf{A} \right ) = \mathbf{C} \cdot \left ( \mathbf{A} \times \mathbf{B} \right ) $

{\bf Gradient}

$ \nabla f = \frac{\partial f}{\partial x} \mathbf{\hat{i}} + \frac{\partial f}{\partial y} \mathbf{\hat{j}} + \frac{\partial f}{\partial z} \mathbf{\hat{k}} $

{\bf Gradient Identities}

$ \nabla \left ( f + g \right ) = \nabla f + \nabla g $ \\
$ \nabla \left ( \alpha f \right ) = \alpha \nabla f $ \\
$ \nabla \left ( f \, g \right ) = f \nabla g + g \nabla f $ \\
$ \nabla \left ( f/g \right ) = \frac{\left ( g \nabla f - f \nabla g \right )}{g^2} $ \\

{\bf Divergence}

$ \nabla \cdot \mathbf{A} =  \frac{\partial A_x}{\partial x} +
\frac{\partial A_y}{\partial y} +\frac{\partial A_z}{\partial z} $

{\bf Divergence of the cross product}

$ \nabla \cdot \left ( \mathbf{A} \times \mathbf{B} \right ) = \mathbf{B} \cdot \left ( \nabla \times \mathbf{A} \right ) - \mathbf{A} \cdot \left ( \nabla \times \mathbf{B} \right ) $

{\bf Divergence of the curl}

$ \nabla \cdot \left ( \nabla \times \mathbf{A} \right ) = 0 $

{\bf Laplacian Identities}

$ \nabla \times \left ( \nabla \times \mathbf{A} \right ) = \nabla \left ( \nabla \cdot \mathbf{A} \right ) - \nabla^2 \mathbf{A} $</content>
</record>
