Latex: Equations
Dr. Tom V. Mathew
4 October 2006
In line equation is produced by giving $ sign before and after an equation.
Few simple equation are given below.
\documentclass{article}
\begin{document}
A simple equation with english alphabets $z=x+y$,
another simple equation with greek alphabets $\alpha=\beta+\gamma$,
and an equation with some special notation $\sum z=\frac{\delta}{y^2}$.
\end{document}
This will produce equations like this:
A simple equation with english alphabets
,
another simple equation with greek alphabets
,
and an equation with some special notation
.
A simple equation with english alphabets
, another simple equation with
greek alphabets
, and
.
Note that the equation number is generated automatically.
The equation environment will create an equation similar to above, but not in-line.
The equation will be placed next line, justified middle, places some space
above and below; and auotmatically generate an equation number.
To get the equation below, use the source code in:
\begin{equation}
\Pi_{i=0}^{n^{2}}=\frac{\alpha^{\sqrt{y}}}{\sqrt{y-x}}
\end{equation}
 |
(1) |
The eqnarray environment is similar to the equation; but it can support
equation spanning to many lines.
\begin{eqnarray}
z = (x+1)+(y-2) \\
= x+y+1-2 \\
= x+y-1\\
\end{eqnarray}
Note that this environment has generated equation on all lines.
However, the aligment of the equation is not proper. See the follwoing example
which shows a nice alignment as well numbering for only once.
\begin{eqnarray}
\Pi_{i=0}^{n^{2}}&=&\frac{\alpha^{\sqrt{y}}}{\sqrt{y-x}}\\
&=&e^{25\beta}-1\nonumber\\
&=&\Delta+\Gamma\nonumber
\end{eqnarray}
This code will produce the follwing output.
%
\begin{equation}
%
\newcommand{\cellaa}{\frac{\partial^2{f(\bar{x})}}{\partial{x_1^2}}}
%
\newcommand{\cellab}{\frac{\partial^2{f(\bar{x})}}{\partial{x_1x_2}}}
%
\newcommand{\cellac}{\frac{\partial^2{f(\bar{x})}}{\partial{x_1x_3}}}
%
\newcommand{\cellan}{\frac{\partial^2{f(\bar{x})}}{\partial{x_1x_n}}}
%
\newcommand{\cellba}{\frac{\partial^2{f(\bar{x})}}{\partial{x_2x_1}}}
%
\newcommand{\cellbb}{\frac{\partial^2{f(\bar{x})}}{\partial{x_2^2}}}
%
\newcommand{\cellbc}{\frac{\partial^2{f(\bar{x})}}{\partial{x_2x_3}}}
%
\newcommand{\cellbn}{\frac{\partial^2{f(\bar{x})}}{\partial{x_2x_n}}}
%
\newcommand{\cellna}{\frac{\partial^2{f(\bar{x})}}{\partial{x_nx_1}}}
%
\newcommand{\cellnb}{\frac{\partial^2{f(\bar{x})}}{\partial{x_nx_2}}}
%
\newcommand{\cellnc}{\frac{\partial^2{f(\bar{x})}}{\partial{x_nx_3}}}
%
\newcommand{\cellnn}{\frac{\partial^2{f(\bar{x})}}{\partial{x_n^2}}}
%
a=\left(
%
\begin{array}{ccccc}
%
\cellaa&\cellab&\cellac&\dots&\cellan\\
\cellba&\cellbb&\cellbc&\dots&\cellbn\\
\dots &\dots & \dots &\dots&\dots\\\hline
\cellna&\cellnb&\cellnc&\dots&\cellnn\\
%
\end{array}
%
\right)
%
\end{equation}
 |
(6) |
Prof. Tom V. Mathew
2006-10-04