2.6.3 Caso particular: Campo transversal

$\fbox{\parbox[b]{5cm}{ \begin{eqnarray} u^\mu &=&W(1,v^x,0,v^z) \nonumber \\ b^\mu &=&(0,0,b,0) \nonumber \end{eqnarray}}}$

$\fbox{\parbox[b]{14cm}{ {\bf Campos caracter\'{\i}sticos:} \begin{eqnarray*} \la... ...2)[1-(v^x)^2-(v^2-(v^x)^ 2)\omega^2]}}{1-v^2\omega^2} [2ex] \end{eqnarray*}}}$

$\begin{eqnarray*} \omega^2=c_s^2+c_A^2-c_s^2c_A^2 \end{eqnarray*}$

(velocidad local del sonido) : $\displaystyle{hc_s^2=\chi+\frac{p}{\rho^2}\kappa}$

$\begin{eqnarray*} \chi=\left( \frac{\partial p}{\partial \rho}\right) _{\varepsi... ...a=\left( \frac{\partial p}{\partial \varepsilon }\right) _{\rho} \end{eqnarray*}$
(velocidad de Alfvén relativista): $\displaystyle{c_A^2=\frac{\mu\vert b\vert^2}{\rho h^*}}$