The bias induced by the Goodman algorithm: Difference between revisions
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The bias induced by the Goodman routine | The bias induced by the Goodman routine | ||
<ref> | <ref name="goodmanetal2006">{{Cite journal | ||
|authors= L. Goodman, E. Levine and R. Lueck | |||
|journal_or_publisher= J. Atmos. Oceanic Technol. | |||
|paper_or_booktitle= On measuring the terms of the turbulent kinetic energy budget from an AUV | |||
|year= 2006 | |||
|volume= 23 | |||
|pages= 977-990 | |||
|doi= 10.1175/JTECH1889.1 | |||
}}</ref> | |||
vibration-coherent corrections algorithm is corrected by dividing the spectrum by <math>1-\frac{1.02N_v}{N_f}</math> where <math>N_v</math> is the number of signals that are used to remove coherent signals in the shear-probe signals and <math>N_f</math> is the number of fft-segments that are used to estimate the shear-spectra | |||
<ref name="luecketal2022">{{Cite journal | |||
|authors= R. G. Lueck, D. MacIntyre, and J. MacMillan | |||
|journal_or_publisher= J. Atmos. Oceanic Technol. | |||
|paper_or_booktitle= The bias in coherent noise removal | |||
|year= 2022 | |||
|doi=TBD | |||
}}</ref>. | |||
Revision as of 22:09, 19 November 2021
The bias induced by the Goodman routine [1] vibration-coherent corrections algorithm is corrected by dividing the spectrum by <math>1-\frac{1.02N_v}{N_f}</math> where <math>N_v</math> is the number of signals that are used to remove coherent signals in the shear-probe signals and <math>N_f</math> is the number of fft-segments that are used to estimate the shear-spectra [2].
References
- ↑ {{#arraymap:L. Goodman, E. Levine and R. Lueck|,|x|x|, |and}}. 2006. On measuring the terms of the turbulent kinetic energy budget from an AUV. J. Atmos. Oceanic Technol.. doi:10.1175/JTECH1889.1
- ↑ {{#arraymap:R. G. Lueck, D. MacIntyre, and J. MacMillan|,|x|x|, |and}}. 2022. The bias in coherent noise removal. J. Atmos. Oceanic Technol.. doi:TBD
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