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In ], the reference value is usually the sampling frequency, denoted <math>f_s,\,</math>&nbsp; in '''samples per second''', because the frequency content of a sampled signal is completely defined by the content within a span of <math>f_s\,</math> ], at most. In other words, the frequency distribution is periodic with period <math>f_s.\,</math>&nbsp; When the actual frequency<math>, f,\,</math> has units of ] (] units), the normalized frequencies, also denoted by <math>f,\,</math>&nbsp; have units of '''cycles per sample''', and the periodicity of the normalized distribution is 1. &nbsp;And when the actual frequency<math>, \omega,\,</math> has units of radians per second (]), the normalized frequencies have units of '''radians per sample''', and the periodicity of the distribution is 2п. In ], the reference value is usually the sampling frequency, denoted <math>f_s,\,</math>&nbsp; in '''samples per second''', because the frequency content of a sampled signal is completely defined by the content within a span of <math>f_s\,</math> ], at most. In other words, the frequency distribution is periodic with period <math>f_s.\,</math>&nbsp; When the actual frequency<math>, f,\,</math> has units of ] (] units), the normalized frequencies, also denoted by <math>f,\,</math>&nbsp; have units of '''cycles per sample''', and the periodicity of the normalized distribution is 1. &nbsp;And when the actual frequency<math>, \omega,\,</math> has units of radians per second (]), the normalized frequencies have units of '''radians per sample''', and the periodicity of the distribution is 2п.



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In digital signal processing, the reference value is usually the sampling frequency, denoted f s , {\displaystyle f_{s},\,}   in samples per second, because the frequency content of a sampled signal is completely defined by the content within a span of f s {\displaystyle f_{s}\,} hertz, at most. In other words, the frequency distribution is periodic with period f s . {\displaystyle f_{s}.\,}   When the actual frequency , f , {\displaystyle ,f,\,} has units of hertz (SI units), the normalized frequencies, also denoted by f , {\displaystyle f,\,}   have units of cycles per sample, and the periodicity of the normalized distribution is 1.  And when the actual frequency , ω , {\displaystyle ,\omega ,\,} has units of radians per second (angular frequency), the normalized frequencies have units of radians per sample, and the periodicity of the distribution is 2п.

If a sampled waveform is real-valued, such as a typical filter impulse response, the periodicity of the frequency distribution is still f s . {\displaystyle f_{s}.\,}   But due to symmetry, it is completely defined by the content within a span of just f s / 2. {\displaystyle f_{s}/2.\,}   Accordingly, some filter design procedures/applications use that as the normalization reference (and the resulting units are half-cycles per sample). A filter design can be used at different sample-rates, resulting in different frequency responses. Normalization produces a distribution that is independent of the sample-rate. Thus one plot is sufficient for all possible sample-rates.

The following table shows examples of normalized frequencies for a 1 kHz signal, and a sample rate f s {\displaystyle f_{s}} = 44.1 kHz.

Type Computation Value
Radians/sample 2 pi 1000 / 44100 0.1425
w.r.t. fs 1000 / 44100 0.02676
w.r.t. Nyquist 1000 / 22050 0.04535
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