|
|
Line 1: |
Line 1: |
| {{notability|date=February 2012}}
| | Myrtle Benny is how I'm called and I feel comfortable when individuals use the complete title. Puerto Rico is home std test exactly where he's been residing for many years and he home [http://www.nytimes.com/ref/health/healthguide/esn-herpes-ess.html std test] kit will by no [http://www.associazioneitalianafotografi.it/community/gruppi/points-to-know-when-confronted-with-candidiasis/ over the counter std test] means move. For many years he's been operating as a receptionist. One of the very best issues in the world for me is to do aerobics and I've been performing it for fairly a while.<br><br>My web page: std testing at [http://immbooks.com/blogs/post/44599 home std test kit], [http://www.escuelavirtual.registraduria.gov.co/user/view.php?id=140944&course=1 mouse click for source], |
| | |
| The '''autocorrelation technique''' is a method for estimating the dominating frequency in a [[Complex number|complex]] signal, as well as its variance. Specifically, it calculates the first two moments of the power spectrum, namely the mean and variance. It is also known as the '''pulse-pair algorithm''' in [[radar]] theory.
| |
| | |
| The algorithm is both computationally faster and significantly more accurate compared to the [[discrete Fourier transform|Fourier transform]], since the resolution is not limited by the number of samples used.
| |
| | |
| == Derivation ==
| |
| The [[autocorrelation]] of lag 1 can be expressed using the inverse Fourier transform of the power spectrum <math>S(\omega)</math>:
| |
| :<math> R(1) = \frac{1}{2\pi} \int_{-\pi}^{\pi} S(\omega) e^{i\,\omega\,1} d\omega. </math>
| |
| If we model the power spectrum as a single frequency <math>S(\omega) \ \stackrel{\mathrm{def}}{=}\ \delta(\omega - \omega_0)</math>, this becomes:
| |
| :<math> R(1) = \frac{1}{2\pi} \int_{-\pi}^{\pi} \delta(\omega - \omega_0) e^{i\,\omega} d\omega </math>
| |
| :<math> R(1) = \frac{1}{2\pi} e^{i\,\omega_0} </math>
| |
| where it is apparent that the phase of <math>R(1)</math> equals the signal frequency.
| |
| | |
| == Implementation ==
| |
| The mean frequency is calculated based on the [[autocorrelation]] with lag one, evaluated over a signal consisting of N samples:
| |
| :<math>\omega = \angle R_N(1) = \tan^{-1}\frac{im\{ R_N(1) \}}{re\{ R_N(1) \}}. </math>
| |
| The spectral variance is calculated as follows:
| |
| :<math>var\{ \omega \} = \frac{2}{N} \left( 1 - \frac{|R_N(1)|}{R_N(0)} \right). </math>
| |
| | |
| == Applications ==
| |
| * Estimation of blood velocity and turbulence in ''color flow imaging'' used in [[medical ultrasonography]].
| |
| * Estimation of target velocity in [[pulse-doppler radar]]
| |
| | |
| {{inline|date=February 2012}}
| |
| | |
| == External links ==
| |
| * [http://ieeexplore.ieee.org/xpl/abs_free.jsp?arNumber=1054886 A covariance approach to spectral moment estimation], Miller et al., IEEE Transactions on Information Theory. {{full|date=November 2012}}
| |
| * Doppler Radar Meteorological Observations [http://www.ofcm.gov/fmh11/fmh11partb/2005pdf/fmh-11B-2005.pdf Doppler Radar Theory].{{full|date=November 2012}} Autocorrelation technique described on p.2-11
| |
| * [http://server.oersted.dtu.dk/31655/documents/kasai_et_al_1985.pdf Real-Time Two-Dimensional Blood Flow Imaging Using an Autocorrelation Technique], by Chihiro Kasai, Koroku Namekawa, Akira Koyano, and Ryozo Omoto, IEEE Transactions on sonics and ultrasonics, May 1985 {{full|date=November 2012}}
| |
| | |
| [[Category:Radar theory]]
| |
| [[Category:Signal processing]]
| |
| [[Category:Time series analysis]]
| |
Myrtle Benny is how I'm called and I feel comfortable when individuals use the complete title. Puerto Rico is home std test exactly where he's been residing for many years and he home std test kit will by no over the counter std test means move. For many years he's been operating as a receptionist. One of the very best issues in the world for me is to do aerobics and I've been performing it for fairly a while.
My web page: std testing at home std test kit, mouse click for source,