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Update URE_1.md

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Riccardo Giuntoli 2020-11-14 17:01:48 +01:00
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es.telecomlobby.com/radio_aficion/URE_1.md
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@ -62,12 +62,7 @@ Siendo lambda λ un coeficiente de conductividad propio de cada materia podemos
$$
\begin{align*}
y = y(x,t) &= A e^{i\theta} \\
&= A (\cos \theta + i \sin \theta) \\
&= A (\cos(kx - \omega t) + i \sin(kx - \omega t)) \\
&= A\cos(kx - \omega t) + i A\sin(kx - \omega t) \\
&= A\cos \Big(\frac{2\pi}{\lambda}x - \frac{2\pi v}{\lambda} t \Big) + i A\sin \Big(\frac{2\pi}{\lambda}x - \frac{2\pi v}{\lambda} t \Big) \\
&= A\cos \frac{2\pi}{\lambda} (x - v t) + i A\sin \frac{2\pi}{\lambda} (x - v t)
Conductancia = \frac{λxsuperficie(cm^2)}{longitud(cm)}\\
\end{align*}
$$