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13.4.15
LaTeX en Blogger usando MathJax (II)
$$\oint_{S}\vec{E}\cdot d\vec{S}=\frac{1}{\varepsilon_{o}}\int_{V}\rho \; dV$$
$$E=mc^{2}$$
$$\vec{a}=\frac{\vec{F}}{m}$$
$$i\hbar\frac{\partial}{\partial t}\left|\Psi(t)\right>=H\left|\Psi(t)\right>$$
$$
i \hbar \frac{\partial}{\partial t} \Psi = H \Psi
$$
\begin{equation}
L' = {L}{\sqrt{1-\frac{v^2}{c^2}}}
\end{equation}
$$
\frac{1}{\displaystyle 1+
\frac{1}{\displaystyle 2+
\frac{1}{\displaystyle 3+x}}} +
\frac{1}{1+\frac{1}{2+\frac{1}{3+x}}}
$$
$$\int_0^\infty e^{-x^2} dx=\frac{\sqrt{\pi}}{2}$$
\begin{align}
B'&=-\nabla \times E,\\
E'&=\nabla \times B - 4\pi j,
\end{align}
\[ f(n) = \left\{
\begin{array}{l l}
n/2 & \quad \text{if $n$ is even}\\
-(n+1)/2 & \quad \text{if $n$ is odd}
\end{array} \right.\]
\begin{equation}
\left.\begin{aligned}
B'&=-\partial \times E,\\
E'&=\partial \times B - 4\pi j,
\end{aligned}
\right\}
\qquad \text{Maxwell's equations}\end{equation}
\begin{equation}\label{eq:gravt}
F=G\frac{mM}{r^2}.
\end{equation}
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