This is an equation environment:

\[ \int_\Omega d\omega = \int_{\partial\Omega} \omega \qquad\mbox{Stokes's Theorem} \]

This should be a centered equation with no numbering.

We also want to support equation environments:

\begin{equation} \int_\Omega d\omega = \int_{\partial\Omega} \omega \qquad\mbox{Stokes's Theorem} \end{equation}

We’ll probably have to handle numbering and cross-references in a post-processing step.

Lorem ipsum dolor sit amet, consectetur adipisicing elit, sed do eiusmod tempor incididunt ut labore et dolore magna aliqua. Ut enim ad minim veniam, quis nostrud exercitation ullamco laboris nisi ut aliquip ex ea commodo consequat. Duis aute irure dolor in reprehenderit in voluptate velit esse cillum dolore eu fugiat nulla pariatur. Excepteur sint occaecat cupidatat non proident, sunt in culpa qui officia deserunt mollit anim id est laborum.

Of course, inline math like \( \Omega > 0 \) and \( x^2 - 2 \equiv 0 \) should also work fine.

\begin{align} x^2 + y^2 &= 1 \\ y &= \sqrt{1 - x^2}. \end{align}

Maxwell’s Equations:

\begin{equation} \begin{aligned} \nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t} & = \frac{4\pi}{c}\vec{\mathbf{j}} \\ \nabla \cdot \vec{\mathbf{E}} & = 4 \pi \rho \\ \nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} & = \vec{\mathbf{0}} \\ \nabla \cdot \vec{\mathbf{B}} & = 0 \end{aligned} \end{equation}

\begin{equation*} \left.\begin{aligned} dE &= \rho \\ d*E &= -\dot{B} \\ dB &= 0 \\ d*B &= J + \dot{E} \end{aligned} \right\} \qquad \text{Maxwell's equations} \end{equation*}

\begin{multline} a+b+c+d+e+f\\ +i+j+k+l+m+n \end{multline}