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post1.md 838 B
title: Example Blog Post
author: Stephen Diehl
date: 2013-11-13
mathjax: on

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Some math:

×B1cEt=4πcjE=4πρ×E+1cBt=0B=0 \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}

Some code:

newtype MonadMonoid m a = MonadMonoid { unMonad :: a -> m a }

instance Monad m => Monoid (MonadMonoid m a) where
  mempty = MonadMonoid return
  mappend f g = MonadMonoid (f >=> g)

Fin.