The phase velocity \(v_{p}\) is the speed at which a point of constant phase of the wave will travel for a discrete frequency and is given as
\begin{align}
v_{p} &= \frac{x}{t} \\
&= \frac{\lambda}{T} \\
&= \frac{\omega}{k} \\
\end{align}
\(\lambda\) is the wave length and T is the period. \(\omega\) is the angular frequency, \(k\) is the wavenumber. Formally, the phase is defined as follows
\begin{equation}
\Phi = k x - \omega t
\end{equation}
Then the phase velocity is given as follows
\begin{align}
v_{p} &= \frac{dx}{dt} \\
&= \frac{d \Phi}{dt} / \frac{d \Phi}{dx} \\
&= \omega / k
\end{align}
And the angular frequency is related to the wavenumber through the dispersion relationship.
\begin{equation}
\omega = \Omega(k)
\end{equation}
The group velocity is the speed at which a wave packet from a narrow range of frequencies will travel and is determined from the gradient of the dispersion relation
\begin{equation}
v_{g} = \frac{\partial \omega}{\partial k}
\end{equation}
The group velocity is often thought of as the velocity at which energy or information is conveyed along a wave.
In quantum theory, there is a concept of incoming and outgoing wave. They distinguish with each by \(e^{ikr}\) and \(e^{-ikr}\). It seems that if \(r\) increases then \(e^{ikr}\) increases while \(e^{-ikr}\) decreases with respect to positive \(k\). However, in flow instability theory, things seem to be opposite.
Oscillation is the repetitive variation, typically in time, of some measure about a central value, often a point of equilibrium, or between two or more different states.
It’s the system where the restoring force on a body is directly proportional to its displacement. And in this system, the regular motion is referred as simple harmonic motion.
The simple harmonic oscillator has a single degree of freedom. Coupled oscillator has more degrees of freedom and deeper interpretation is given by resolving the motion into normal modes.
Waves can be regarded as systems with an infinite number of degrees of freedom and normal modes.