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{{DefineConcept
{{DefineConcept
|parameter_name=<math>\Psi</math>
|description=Shows how the variance of a signal is distributed with respect to frequency or wavenumber
|description=Shows how the variance of a signal is distributed with respect to frequency or wavenumber
|article_type=Fundamentals
|article_type=Fundamentals
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The units of frequency can be cyclic such as <math>\mathrm{Hz}</math> (previously called cycles per second), or they can be angular such as <math>\mathrm{rad\, s^{-1}}</math>.
The units of frequency can be cyclic such as <math>\mathrm{Hz}</math> (previously called cycles per second), or they can be angular such as <math>\mathrm{rad\, s^{-1}}</math>.
The units should never be expressed as <math>\mathrm{s^{-1}}</math> because this usage is ambiguous, even though the units of radians is technically dimensionless.
The units should never be expressed as <math>\mathrm{s^{-1}}</math> because this usage is ambiguous, even though the units of radians is technically dimensionless.
These two measures of frequency differ by a factor of <math>2\pi</math}.
The angular measures of frequency is larger than the cyclic measure of frequency by a factor of <math>2\pi</math>.




Thus, the units of a spectrum, <math>\Psi</math> are the square of the units of <math>u</math> per unit of frequency, <math>f</math>.
Thus, the units of a spectrum, <math>\Psi</math> are the square of the units of <math>u</math> per unit of frequency, <math>f</math>.
If the signal is a space series, such as <math>u(x)</math>, where <math>x</math> is the distance along a direction, then this signal also has a spectrum, but this spectrum provides the distribution of variance with respect to wavenumber, <math>k</math>.
The wavenumber can be cyclic [<math>\mathrm{cpm}</math>] (cycles per meter) or it can be angular [<math>\mathrm{rad\, m^{-1}}</math>].
To avoid ambiguity, one should never express the units of wavenumber as <math>\mathrm{m^{-1}}</math>.
The same properties apply to wavenumber spectrum, such as
<math>\overline{u^2} = \int_0^{\infty} \Psi_u(k)\, \mathrm{d}k  \ \ .</math>
If the signal <math>u</math> is discretely sampled, then the upper frequency (or wavenumber) limit is reduced from <math>f=\infty</math> to the Nqyquist frequency, <math>f=f_N=f_s/2</math>, where <math>f_s</math> is the sampling rate of the signal.

Latest revision as of 21:25, 13 July 2021


Short definition of Spectrum (Ψ)
Shows how the variance of a signal is distributed with respect to frequency or wavenumber

This is the common definition for Spectrum, but other definitions may be discussed within the wiki.




The spectrum of a signal, say u(t), shows how the variance of this signal is distributed with respect to frequency. If the spectrum of u is Ψu(f), then the spectrum has the property that the variance of u is

u2‾=∫0∞Ψu(f)df  .

and the variance located between two frequencies f1 and f2 is

∫f1f2Ψu(f)df  .

The units of frequency can be cyclic such as Hz (previously called cycles per second), or they can be angular such as rads−1. The units should never be expressed as s−1 because this usage is ambiguous, even though the units of radians is technically dimensionless. The angular measures of frequency is larger than the cyclic measure of frequency by a factor of 2π.


Thus, the units of a spectrum, Ψ are the square of the units of u per unit of frequency, f.

If the signal is a space series, such as u(x), where x is the distance along a direction, then this signal also has a spectrum, but this spectrum provides the distribution of variance with respect to wavenumber, k. The wavenumber can be cyclic [cpm] (cycles per meter) or it can be angular [radm−1]. To avoid ambiguity, one should never express the units of wavenumber as m−1. The same properties apply to wavenumber spectrum, such as

u2‾=∫0∞Ψu(k)dk  .

If the signal u is discretely sampled, then the upper frequency (or wavenumber) limit is reduced from f=∞ to the Nqyquist frequency, f=fN=fs/2, where fs is the sampling rate of the signal.