(Waves)
We seek a law in the form of an equation which yields a new position in any independent coordinate as a function of the old ones \[``="\] differential equation
The disturbance is a function of 2 variables which can be varied independently (holding the respective other fixed): \[ \frac{\partial\Psi}{\partial x}=\frac{\partial f}{\partial x}=\frac{\partial f(x\pm vt)}{\partial(x\pm vt)}\frac{\partial(x\pm vt)}{\partial x}=\frac{\partial f}{\partial(x\pm vt)} \] and \[ \frac{\partial\Psi}{\partial t}=\frac{\partial f}{\partial t}=\frac{\partial f(x\pm vt)}{\partial(x\pm vt)}\frac{\partial(x\pm vt)}{\partial t}=\pm v\frac{\partial f}{\partial(x\pm vt)} \] \[ \Rightarrow \frac{\partial\Psi}{\partial t}=\pm v\frac{\partial\Psi}{\partial x} \] Repeat to find the 1-dimansional, fixed-profile (free) wave equation:
\[ \frac{\partial^2\Psi}{\partial t^2}=v^2\frac{\partial^2\Psi}{\partial x^2} \]