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1 | initial version |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = mc^2$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor.
2 | No.2 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = mc^2$$m \cdot c^2$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor.
3 | No.3 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. m \cdot c^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor.
4 | No.4 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = m \cdot c^2$. mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor.
5 | No.5 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
You can also do more:
$$ \left{ \begin{array}{c} a_1x+b_1y+c_1z=d_1 \ a_2x+b_2y+c_2z=d_2 \ a_3x+b_3y+c_3z=d_3 \end{array} \right. $$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor.. This StackExchange's MathMeta tutorial is quite informative too.
6 | No.6 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
You can also do more:
$$
\left{ $$\left{
\begin{array}{c}
a_1x+b_1y+c_1z=d_1 \
a_2x+b_2y+c_2z=d_2 \
a_3x+b_3y+c_3z=d_3
\end{array}
\right.
$$\right$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor. This StackExchange's MathMeta tutorial is quite informative too.
7 | No.7 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
You can also do more:UnmetHours doesn't have support for all of MathJax, but the essential stuff is there:
$$\left{
\begin{array}{c}
a_1x+b_1y+c_1z=d_1 \
a_2x+b_2y+c_2z=d_2 \
a_3x+b_3y+c_3z=d_3
\end{array}
\right$$$$m\dot C_p \frac{x}{y} \Delta T$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor. This StackExchange's MathMeta tutorial is quite informative too.
8 | No.8 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
UnmetHours doesn't have support for all of MathJax, but the essential stuff is there:
$$m\dot $$\dot m C_p \frac{x}{y} \Delta T$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor. This StackExchange's MathMeta tutorial is quite informative too.
9 | No.9 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
UnmetHours doesn't have support for all of MathJax, but the essential stuff is there:
$$\dot m C_p \frac{x}{y} \Delta T$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there are handy tools such as this online equation editor. This StackExchange's MathMeta tutorial is quite informative too.
$$\begin{cases} a_1x+b_1y+c_1z=d_1 \ a_2x+b_2y+c_2z=d_2 \ a_3x+b_3y+c_3z=d_3 \end{cases} $$
10 | No.10 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
UnmetHours doesn't have support for all of MathJax, but the essential stuff is there:
$$\dot m C_p \frac{x}{y} \Delta T$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with, there with it, please read this post here (basic) Equation support on unmethours. There are also handy tools such as this online equation editor. This StackExchange's MathMeta tutorial is quite informative too..
$$\begin{cases} a_1x+b_1y+c_1z=d_1 \ a_2x+b_2y+c_2z=d_2 \ a_3x+b_3y+c_3z=d_3 \end{cases} $$
11 | No.11 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
UnmetHours doesn't have support for all of MathJax, but the essential stuff is there:
$$\dot m C_p \frac{x}{y} \Delta T$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with it, please read this post here (basic) Equation support on unmethours. There are also handy tools such as this online equation editor.
$$\begin{cases}
a_1x+b_1y+c_1z=d_1 \
a_2x+b_2y+c_2z=d_2 \
a_3x+b_3y+c_3z=d_3
\end{cases}
$$UnmetHours doesn't have support for all of MathJax, but the essential stuff is there:
$$\dot m C_p \frac{x}{y} \Delta T$$
12 | No.12 Revision |
UnmetHours uses MathJax. You surround inline equations by a single $
sign: $e = mc^2$. To put an equation on its own line and centered, use $$
$$ e = m \cdot c^2$$
For the format of the equations, it's like LaTeX. If you are unfamiliar with it, please read this post here (basic) Equation support on unmethours. There are also handy tools such as this online equation editor.
UnmetHours doesn't have support for all of MathJax, MathJax (on the post I linked to, there are a few things that aren't working in my answer), but the essential stuff is there:
$$\dot m C_p \frac{x}{y} \Delta T$$