Normalized frequency (signal processing)

From HandWiki
(Redirected from Physics:Cycles per sample)
Short description: Frequency divided by a characteristic frequency


In digital signal processing (DSP), a normalized frequency is a ratio of a variable frequency (f) and a constant frequency associated with a system (such as a sampling rate, fs). 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

A typical choice of characteristic frequency is the sampling rate (fs) that is used to create the digital signal from a continuous one. The normalized quantity, f′=ffs, has the unit cycle per sample regardless of whether the original signal is a function of time or distance. For example, when f is expressed in Hz (cycles per second), fs is expressed in samples per second.[1]

Some programs (such as MATLAB toolboxes) that design filters with real-valued coefficients prefer the Nyquist frequency (fs/2) as the frequency reference, which changes the numeric range that represents frequencies of interest from [0,12] cycle/sample to [0,1] half-cycle/sample. Therefore, the normalized frequency unit is important when converting normalized results into physical units.

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 fsN, for some arbitrary integer N (see § Sampling the DTFT). The samples (sometimes called frequency bins) are numbered consecutively, corresponding to a frequency normalization by fsN.[2]: p.56 eq.(16)  The normalized Nyquist frequency is N2 with the unit ⁠1/N⁠th cycle/sample.

Angular frequency, denoted by ω and with the unit radians per second, can be similarly normalized. When ω is normalized with reference to the sampling rate as ω′=ωfs, the normalized Nyquist angular frequency is π radians/sample.

The following table shows examples of normalized frequency for f=1 kHz, fs=44100 samples/second (often denoted by 44.1 kHz), and 4 normalization conventions:

Quantity Numeric range Calculation Reverse
f′=ffs   [0, ⁠1/2⁠] cycle/sample 1000 / 44100 = 0.02268 f=f′⋅fs
f′=ffs/2   [0, 1] half-cycle/sample 1000 / 22050 = 0.04535 f=f′⋅fs2
f′=ffs/N   [0, ⁠N/2⁠] bins 1000 × N / 44100 = 0.02268 N f=f′⋅fsN
ω′=ωfs   [0, π] radians/sample 1000 × 2π / 44100 = 0.14250 ω=ω′⋅fs

See also

References

  1. ↑ Carlson, Gordon E. (1992). Signal and Linear System Analysis. Boston, MA: ©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". Proceedings of the IEEE 66 (1): 51–83. doi:10.1109/PROC.1978.10837. Bibcode: 1978IEEEP..66...51H. http://web.mit.edu/xiphmont/Public/windows.pdf.