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Frequency divided by a characteristic frequency

In digital signal processing (DSP), a normalized frequency is a ratio of a variable frequency (πŸ‘ {\displaystyle f}
) and a constant frequency associated with a system (such as a sampling rate, πŸ‘ {\displaystyle f_{s}}
). Some software applications require normalized inputs and produce normalized outputs, which can be re-scaled to physical units when necessary. Mathematical derivations are usually done in normalized units, relevant to a wide range of applications.

Examples of normalization

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A typical choice of characteristic frequency is the sampling rate (πŸ‘ {\displaystyle f_{s}}
) that is used to create the digital signal from a continuous one. The normalized quantity, πŸ‘ {\displaystyle f'={\tfrac {f}{f_{s}}},}
has the unit cycle per sample regardless of whether the original signal is a function of time or distance. For example, when πŸ‘ {\displaystyle f}
is expressed in Hz (cycles per second), πŸ‘ {\displaystyle f_{s}}
is expressed in samples per second.[1]

Some programs (such as MATLAB toolboxes) that design filters with real-valued coefficients prefer the Nyquist frequency πŸ‘ {\displaystyle (f_{s}/2)}
as the frequency reference, which changes the numeric range that represents frequencies of interest from πŸ‘ {\displaystyle \left[0,{\tfrac {1}{2}}\right]}
cycle/sample to πŸ‘ {\displaystyle [0,1]}
half-cycle/sample. Therefore, the normalized frequency unit is important when converting normalized results into physical units.

πŸ‘ Image
Example of plotting samples of a frequency distribution in the unit "bins", which are integer values. A scale factor of 0.7812 converts a bin number into the corresponding physical unit (hertz).

A common practice is to sample the frequency spectrum of the sampled data at frequency intervals of πŸ‘ {\displaystyle {\tfrac {f_{s}}{N}},}
for some arbitrary integer πŸ‘ {\displaystyle N}
(see Β§ Sampling the DTFT). The samples (sometimes called frequency bins) are numbered consecutively, corresponding to a frequency normalization by πŸ‘ {\displaystyle {\tfrac {f_{s}}{N}}.}
[2]:β€Šp.56 eq.(16)β€Š[3] The normalized Nyquist frequency is πŸ‘ {\displaystyle {\tfrac {N}{2}}}
with the unit ⁠1/N⁠th cycle/sample.

Angular frequency, denoted by πŸ‘ {\displaystyle \omega }
and with the unit radians per second, can be similarly normalized. When πŸ‘ {\displaystyle \omega }
is normalized with reference to the sampling rate as πŸ‘ {\displaystyle \omega '={\tfrac {\omega }{f_{s}}},}
the normalized Nyquist angular frequency is Ο€ radians/sample.

The following table shows examples of normalized frequency for πŸ‘ {\displaystyle f=1}
kHz, πŸ‘ {\displaystyle f_{s}=44100}
samples/second (often denoted by 44.1 kHz), and 4 normalization conventions:

Quantity Numeric range Calculation Reverse
πŸ‘ {\displaystyle f'={\tfrac {f}{f_{s}}}}
  [0, ⁠1/2⁠] cycle/sample 1000 / 44100 = 0.02268 πŸ‘ {\displaystyle f=f'\cdot f_{s}}
πŸ‘ {\displaystyle f'={\tfrac {f}{f_{s}/2}}}
  [0, 1] half-cycle/sample 1000 / 22050 = 0.04535 πŸ‘ {\displaystyle f=f'\cdot {\tfrac {f_{s}}{2}}}
πŸ‘ {\displaystyle f'={\tfrac {f}{f_{s}/N}}}
  [0, ⁠N/2⁠] bins 1000 Γ— N / 44100 = 0.02268 N πŸ‘ {\displaystyle f=f'\cdot {\tfrac {f_{s}}{N}}}
πŸ‘ {\displaystyle \omega '={\tfrac {\omega }{f_{s}}}}
  [0, Ο€radians/sample 1000 Γ— 2Ο€ / 44100 = 0.14250 πŸ‘ {\displaystyle \omega =\omega '\cdot f_{s}}

See also

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References

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  1. ^ Carlson, Gordon E. (1992). Signal and Linear System Analysis. Boston, MA: Β©Houghton Mifflin Co. pp. 469, 490. ISBN 8170232384.
  2. ^ Harris, Fredric J. (Jan 1978). "On the use of Windows for Harmonic Analysis with the Discrete Fourier Transform" (PDF). Proceedings of the IEEE. 66 (1): 51–83. Bibcode:1978IEEEP..66...51H. CiteSeerX 10.1.1.649.9880. doi:10.1109/PROC.1978.10837. S2CID 426548.
  3. ^ Taboga, Marco (2021). "Discrete Fourier Transform - Frequencies", Lectures on matrix algebra. https://www.statlect.com/matrix-algebra/discrete-Fourier-transform-frequencies.