User contributions for Aleboyer
From Atomix
5 November 2021
- 03:4103:41, 5 November 2021 diff hist +118 Dataset requirements for shear probes No edit summary
- 03:3803:38, 5 November 2021 diff hist +1,997 Dataset requirements for shear probes No edit summary
- 03:2803:28, 5 November 2021 diff hist +76 Shear probes quality control metrics No edit summary
- 03:2803:28, 5 November 2021 diff hist +74 Dissipation rate estimates No edit summary
- 03:2703:27, 5 November 2021 diff hist +76 Processing parameters No edit summary
- 03:2603:26, 5 November 2021 diff hist +76 Minimum duration No edit summary
- 03:2603:26, 5 November 2021 diff hist +77 Maximum pitch and roll No edit summary
- 03:2503:25, 5 November 2021 diff hist +75 Minimum depth No edit summary
- 03:2503:25, 5 November 2021 diff hist +74 Direction of the vertical velocity No edit summary
- 03:2503:25, 5 November 2021 diff hist +76 Minimum speed No edit summary
- 03:2403:24, 5 November 2021 diff hist +7 Convert the shear probe data No edit summary
- 03:2403:24, 5 November 2021 diff hist +23 Convert the shear probe data No edit summary
- 03:2303:23, 5 November 2021 diff hist +43 Convert the shear probe data No edit summary
- 03:2303:23, 5 November 2021 diff hist +45 Determine the speed of profiling No edit summary
- 03:2103:21, 5 November 2021 diff hist +1 Flow chart for shear probes No edit summary
- 03:2003:20, 5 November 2021 diff hist +54 Flow chart for shear probes No edit summary
23 October 2021
- 04:1204:12, 23 October 2021 diff hist −18 ATOMIX Gallery No edit summary
- 04:1104:11, 23 October 2021 diff hist +154 ATOMIX Gallery No edit summary
- 04:1004:10, 23 October 2021 diff hist +71 N File:Epsilometer EpsiFish FastCTDWinch.jpg No edit summary current
5 October 2021
- 16:0816:08, 5 October 2021 diff hist +199 Wavenumber response of the shear probe No edit summary
22 September 2021
- 16:5716:57, 22 September 2021 diff hist +32 Iterative spectral integration algorithm No edit summary
- 16:5716:57, 22 September 2021 diff hist +819 Iterative spectral integration algorithm No edit summary
- 16:2416:24, 22 September 2021 diff hist +237 The bias induced by the Goodman algorithm No edit summary
- 16:2316:23, 22 September 2021 diff hist +236 The Goodman algorithm No edit summary
- 16:2216:22, 22 September 2021 diff hist +235 Frequency spectra and cross-spectra of shear and vibrations No edit summary
- 16:1916:19, 22 September 2021 diff hist +352 Vibration-coherent noise removal No edit summary
20 August 2021
- 22:5222:52, 20 August 2021 diff hist +535 N Vibration-coherent noise removal Created page with "All platforms vibrate. The shear-probe, like nearly all other velocity sensors, measures the velocity of the fluid relative to the platform that holds the probe. Thus, platfor..."
- 22:5122:51, 20 August 2021 diff hist +572 N De-spiking parameters Created page with "The shear probe will collide with plankton and other particulates in the water, and it will occasionally hit jellyfish and even some fish that do not get out of its path. Thes..."
- 22:5122:51, 20 August 2021 diff hist +670 N High-pass filter cut-off frequency Created page with "The shear probe does not respond to a constant cross-axis velocity. It typically responds to fluctuations of cross-axis velocity with a frequency of 0.1 Hz and higher. Additio..."
- 22:5022:50, 20 August 2021 diff hist +343 N Nearest power-of-two number Created page with "The rate of sampling can then be used to convert these two durations into a number of samples. Although many fast Fourier transform algorithms can transform data of any number..."
- 22:5022:50, 20 August 2021 diff hist +4 Processing parameters No edit summary
- 22:4922:49, 20 August 2021 diff hist +205 N Duration Created page with "Data are invariably sampled regularly in time and not in space. Thus, there is an equivalent duration of time for the chosen diss-length and fft-length, and this duration depe..."
- 22:4922:49, 20 August 2021 diff hist +1,543 N Fft-length Created page with "fft-length – the lowest wavenumber that one wishes to resolve in a spectrum is determined by the length of the segments of data that are processed by a fast Fourier transfor..."
- 22:4622:46, 20 August 2021 diff hist +237 N Diss-length Created page with "diss-length -- Choosing the length of data, in units of meters, for the estimation of dissipation rates makes this choice fairly platform and vehicle independent, and allows i..."
- 22:4622:46, 20 August 2021 diff hist +24 Processing parameters No edit summary
- 22:1922:19, 20 August 2021 diff hist +785 Iterative spectral integration algorithm No edit summary
- 21:4521:45, 20 August 2021 diff hist +1,911 Iterative spectral integration algorithm No edit summary
- 21:3921:39, 20 August 2021 diff hist +1,235 Iterative spectral integration algorithm No edit summary
- 21:3521:35, 20 August 2021 diff hist +1,400 Iterative spectral integration algorithm No edit summary
- 21:1621:16, 20 August 2021 diff hist −1 Iterative spectral integration algorithm No edit summary
- 21:1621:16, 20 August 2021 diff hist +501 N Iterative spectral integration algorithm Created page with "Spectral integration is an iterative procedure because the bandwidth required to estimate the variance of shear depends on the rate of dissipation, the level of electronic noi..."
- 20:5520:55, 20 August 2021 diff hist +594 N Wavenumber response of the shear probe Created page with "The probe-response correction depends on the dimensions of the shear probe. For a commonly used shear probe the spectrum is corrected for the spatial averaging of the shear pr..."
- 19:0519:05, 20 August 2021 diff hist +360 N The bias induced by the Goodman algorithm Created page with "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..."
- 18:5918:59, 20 August 2021 diff hist +4 Dissipation rate estimates No edit summary
- 18:5418:54, 20 August 2021 diff hist +381 N The high-pass filter Created page with "The high-pass filter correction is obtained by multiplying the spectrum by <math>1+\left( \frac{f_c}{f} \right)^2</math> where <math>f_c</math> is the high-pass cut-off freque..."
- 18:3318:33, 20 August 2021 diff hist +65 The Goodman algorithm No edit summary
- 18:2918:29, 20 August 2021 diff hist +71 The Goodman algorithm No edit summary
- 18:2818:28, 20 August 2021 diff hist +872 N The Goodman algorithm Created page with "The procedure is well described in Goodman2006. Focusing on one specific direction, one can simply: - compute the coherence squared <math>toto</math> between the observed v..."
- 18:2218:22, 20 August 2021 diff hist +4 Dissipation rate estimates No edit summary
- 18:1618:16, 20 August 2021 diff hist +27 Dissipation rate estimates No edit summary