# The Wave Equation-Derivation and Physical Applications and Wave Speed Determination

The wave equation, given by $$\partial\_t^2 u-c^2 \nabla^2 u=f$$, is a crucial partial differential equation in physics defined by its second-order time derivative, which enables the description of propagating waves unlike the diffusion equation. Its application depends on the physical context: for transversal waves on a string or a membrane, the equation arises from applying Newton's second law under a small deviation approximation ( $$|\nabla u| \ll 1$$ ), with the wave speed squared determined by the ratio of tension to density ( $$c^2=S / \rho\_{\ell}$$ or $$c^2=\sigma / \rho\_A$$ ). In contrast, for electromagnetic fields, the wave equation for the magnetic field $B$ is a direct and exact consequence of Maxwell's equations, where the wave speed is precisely the speed of light, $$c=1 / \sqrt{\varepsilon\_0 \mu\_0}$$.

### :clapper:Demos

{% embed url="<https://www.youtube.com/playlist?list=PLG2qYtL4WVLddzLceu5EGelSTQBs-L6Wa>" %}

### :bubbles:Cue Column

{% embed url="<https://viadean.notion.site/The-Wave-Equation-Derivation-and-Physical-Applications-and-Wave-Speed-Determination-2a81ae7b9a3280018d0cf43f1608b117?source=copy_link>" %}
