The bias induced by the Goodman algorithm - Revision history

CynthiaBluteau: Categorization

2021-11-23T15:20:39Z

Categorization

← Older revision		Revision as of 15:20, 23 November 2021
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	return to [[Flow chart for shear probes]]		return to [[Flow chart for shear probes]]


			[[Category:Shear probes]]

Rolf at 22:13, 19 November 2021

2021-11-19T22:13:20Z

← Older revision		Revision as of 22:13, 19 November 2021
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	\|doi= 10.1175/JTECH1889.1		\|doi= 10.1175/JTECH1889.1
	}}</ref>		}}</ref>
	vibration-coherent noise removal 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 noise in the shear-probe ~~signals~~ and <math>N_f</math> is the number of fft-segments that are used to estimate the shear spectrum		vibration-coherent noise removal 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 noise in the shear-probe spectrum and <math>N_f</math> is the number of fft-segments that are used to estimate the shear spectrum
	<ref name="luecketal2022">{{Cite journal		<ref name="luecketal2022">{{Cite journal
	\|authors= R. G. Lueck, D. MacIntyre, and J. MacMillan		\|authors= R. G. Lueck, D. MacIntyre, and J. MacMillan

Rolf at 22:12, 19 November 2021

2021-11-19T22:12:33Z

← Older revision		Revision as of 22:12, 19 November 2021
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	\|doi= 10.1175/JTECH1889.1		\|doi= 10.1175/JTECH1889.1
	}}</ref>		}}</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 noise in the shear-probe signals and <math>N_f</math> is the number of fft-segments that are used to estimate the shear spectrum		vibration-coherent noise removal 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 noise in the shear-probe signals and <math>N_f</math> is the number of fft-segments that are used to estimate the shear spectrum
	<ref name="luecketal2022">{{Cite journal		<ref name="luecketal2022">{{Cite journal
	\|authors= R. G. Lueck, D. MacIntyre, and J. MacMillan		\|authors= R. G. Lueck, D. MacIntyre, and J. MacMillan

Rolf at 22:11, 19 November 2021

2021-11-19T22:11:54Z

← Older revision		Revision as of 22:11, 19 November 2021
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	The bias induced by the Goodman ~~routine~~		The bias induced by the Goodman
	<ref name="goodmanetal2006">{{Cite journal		<ref name="goodmanetal2006">{{Cite journal
	\|authors= L. Goodman, E. Levine and R. Lueck		\|authors= L. Goodman, E. Levine and R. Lueck

Rolf at 22:11, 19 November 2021

2021-11-19T22:11:32Z

← Older revision		Revision as of 22:11, 19 November 2021
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	\|doi= 10.1175/JTECH1889.1		\|doi= 10.1175/JTECH1889.1
	}}</ref>		}}</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~~		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 noise in the shear-probe signals and <math>N_f</math> is the number of fft-segments that are used to estimate the shear spectrum
	<ref name="luecketal2022">{{Cite journal		<ref name="luecketal2022">{{Cite journal
	\|authors= R. G. Lueck, D. MacIntyre, and J. MacMillan		\|authors= R. G. Lueck, D. MacIntyre, and J. MacMillan

Rolf at 22:09, 19 November 2021

2021-11-19T22:09:59Z

@@ Line 1: / Line 1: @@
 The bias induced by the Goodman routine
-<ref> Goodman, L., Levine, E. R., & Lueck, R. G. (2006). On measuring the terms of the turbulent kinetic energy budget from an AUV. Journal of Atmospheric and Oceanic Technology, 23(7), 977-990. </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="goodmanetal2006">{{Cite journal
+|authors= L. Goodman, E. Levine and R. Lueck

Rolf at 22:07, 19 November 2021

2021-11-19T22:07:23Z

← Older revision		Revision as of 22:07, 19 November 2021
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	The bias induced by the Goodman routine ~~<ref name="goodmanetal2006">,~~		The bias induced by the Goodman routine

	<ref> Goodman, L., Levine, E. R., & Lueck, R. G. (2006). On measuring the terms of the turbulent kinetic energy budget from an AUV. Journal of Atmospheric and Oceanic Technology, 23(7), 977-990. </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> Goodman, L., Levine, E. R., & Lueck, R. G. (2006). On measuring the terms of the turbulent kinetic energy budget from an AUV. Journal of Atmospheric and Oceanic Technology, 23(7), 977-990. </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.

Rolf at 22:05, 19 November 2021

2021-11-19T22:05:01Z

← Older revision		Revision as of 22:05, 19 November 2021
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	The bias induced by the Goodman<ref> Goodman, L., Levine, E. R., & Lueck, R. G. (2006). On measuring the terms of the turbulent kinetic energy budget from an AUV. Journal of Atmospheric and Oceanic Technology, 23(7), 977-990. </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.		The bias induced by the Goodman routine <ref name="goodmanetal2006">,

			<ref> Goodman, L., Levine, E. R., & Lueck, R. G. (2006). On measuring the terms of the turbulent kinetic energy budget from an AUV. Journal of Atmospheric and Oceanic Technology, 23(7), 977-990. </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.

Rolf at 22:03, 19 November 2021

2021-11-19T22:03:11Z

← Older revision		Revision as of 22:03, 19 November 2021
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	==References==		==References==
	<references />		<references />



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			return to [[Flow chart for shear probes]]

Aleboyer at 16:24, 22 September 2021

2021-09-22T16:24:40Z

← Older revision		Revision as of 16:24, 22 September 2021
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	The bias induced by the Goodman 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.		The bias induced by the Goodman<ref> Goodman, L., Levine, E. R., & Lueck, R. G. (2006). On measuring the terms of the turbulent kinetic energy budget from an AUV. Journal of Atmospheric and Oceanic Technology, 23(7), 977-990. </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.




			==References==
			<references />