Phase of traveling wave¶
The phase of a wave or other periodic function of some real variable \(t\) is an angle-like quantity representing the fraction of the cycle covered up to \(t\). As the variable \(t\) completes a full period, the phase increases by \(360^\circ\) or \(2 \pi\).
If a function \(h(x, t)\) describes a traveling wave, then position \(x\) and time \(t\) can only appear in the form of the wave phase described below.
Notes:
\(\omega = (\vec \omega \cdot {\vec e}_x)\), i.e. the angular frequency is a positive quantity if the wave travels in the positive direction of the \(x\)-axis. Here \({\vec e}_x\) is the unit vector pointing in the positive direction of the \(x\)-axis.
Conditions:
This law applies to a 1-dimensional traveling wave.
The constant phase shift is not taken into account.
Links:
- angular_wavenumber¶
angular_wavenumber
of the wave.- Symbol:
k
- Latex:
\(k\)
- Dimension:
angle/length
- angular_frequency¶
angular_frequency
of the wave.- Symbol:
w
- Latex:
\(\omega\)
- Dimension:
angle/time
- law¶
phi = k * x - w * t
- Latex:
- \[\varphi = k x - \omega t\]