Vector Wavenumber
Mathematically, a sinusoidal plane wave, as in Fig.B.9 or Fig.B.10, can be written as
where p(t,x) is the pressure at time (seconds) and position (3D Euclidean space). The amplitude , phase , and radian frequency are ordinary sinusoid parameters [451], and is the vector wavenumber:
- (unit) vector of direction cosines
- (scalar) wavenumber along travel direction
- wavenumber along the travel direction in its magnitude
- travel direction in its orientation
To see that the vector wavenumber has the claimed properties, consider that the orthogonal projection of any vector onto a vector collinear with is given by [451].^{B.35}Thus, is the component of lying along the direction of wave propagation indicated by . The norm of this component is , since is unit-norm by construction. More generally, is the signed length (in meters) of the component of along . This length times wavenumber gives the spatial phase advance along the wave, or, .
For another point of view, consider the plane wave , which is the varying portion of the general plane-wave of Eq.(B.48) at time , with unit amplitude and zero phase . The spatial phase of this plane wave is given by
As we know from elementary vector calculus, the direction of maximum phase advance is given by the gradient of the phase :
Since the wavenumber is the spatial frequency (in radians per meter) along the direction of travel, we should be able to compute it as the directional derivative of along , i.e.,
Scattering of plane waves is discussed in §C.8.1.
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