- #1
philmolz
- 2
- 0
Hi,
I'm a second year undergrad and we've covered the heat equation,
\begin{equation}
∇^{2}\Psi = \frac{1}{c^{2}}\frac{\partial^2 \Psi}{\partial t^2}
\end{equation}
and the wave equation,
\begin{equation}
D∇^{2}u= \frac{\partial u}{\partial t}
\end{equation}
in our differential equations course. Both Diffusion and wave propagation have wave like solutions, for example,
\begin{equation}
u= Ce^{-\sqrt{w/2D} x } \sin{(\sqrt{w/2D} x - wt)}
\end{equation}
\begin{equation}
\Psi = \Psi_{0} e^{i(kx-wt)}
\end{equation}
but are quite different phenomena. Could someone briefly explain the similarities/ differences in the phenomena and the solutions and how this relates to the differential equations please? Thanks.
I'm a second year undergrad and we've covered the heat equation,
\begin{equation}
∇^{2}\Psi = \frac{1}{c^{2}}\frac{\partial^2 \Psi}{\partial t^2}
\end{equation}
and the wave equation,
\begin{equation}
D∇^{2}u= \frac{\partial u}{\partial t}
\end{equation}
in our differential equations course. Both Diffusion and wave propagation have wave like solutions, for example,
\begin{equation}
u= Ce^{-\sqrt{w/2D} x } \sin{(\sqrt{w/2D} x - wt)}
\end{equation}
\begin{equation}
\Psi = \Psi_{0} e^{i(kx-wt)}
\end{equation}
but are quite different phenomena. Could someone briefly explain the similarities/ differences in the phenomena and the solutions and how this relates to the differential equations please? Thanks.