Velocity despiking

Any measured signal may be contaminated by spikes. These spikes are typically short-lived and transient, which result in sudden change in the measured velocities. These spikes must be removed because they can alter quite dramatically the velocity spectra, which is then used for fitting inertial subrange model.

Overview

Spikes in velocities measured by acoustic-Doppler velocimeters can result from aliasing of the Doppler signal, in particular when pulses become contaminated by reflecting from complex objects and boundaries . Several techniques exist for despiking. The most used with acoustic-Doppler velocimeters are the phase-space thresholding techniques . Other techniques currently being investigated by the subgroup are those used in atmospheric turbulence studies , in particular the median filter despiking technique .

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  Example velocities measured by an acoustic-Doppler velocimeters

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  Example velocity spectra before and after removing spikes. The variance of the despiked signal has reduced by 12% even though there were 30 spikes

Filter based methods

This category of methods is quite common in the literature and have been reviewed extensively by others . These methods compare the original signal against a smoothed version, and values exceeding a threshold [math]\displaystyle{ T }[/math] are deemed to be spikes. Most commonly, the threshold is applied to the timeseries of velocity differences obtained by subtracting the smoothed velocities from the original spiky signal.

Example velocities before and after smoothing (top). Filter-based despiking methods use the difference between these two signals to identify spikes (bottom).

Filter choice

In the 1970s, scientists developed methods based on nonlinear median filters . These filters are less biased by spikes than other linear operations such as low-pass butterworth filters. The moving median filter, for example, only requires a window size, i.e, the number of points over which to calculate the median. This size must be longer than the duration of spikes, which can span consecutive samples. This number must also be sufficiently short to compute a reasonable local median (see Table 1 of Starkenburg et al 2016). The challenge then becomes determining the threshold for identifying spikes.

Identifying the threshold

Some filter-based methods use thresholds based on a factor of the original timeseries' standard deviation (e.g., Tukey method discussed by Goring & Nikora). The results of the analysis then becomes sensitive to this choice of factor. A more automated means to identify the threshold was proposed by Brock (1986) using a histogram of velocity differences. The local minimums on either side from the center defines the positive and negative thresholds. Velocity differences exceeding these thresholds are deemed to be spikes.

Histogram of velocity differences. The local minimum denotes the lower and upper thresholds [math]\displaystyle{ T }[/math] for identifying spikes. The standard deviation of the original timeseries is 2 cm/s, while the thresholds are -4.8 and 5.3 cm/s.

Phase-space thresholding methods

Elaborate here on the methods of Goring and Nikora, which was developed specifically for acoustic-doppler velocity measurements. The other papers referenced above include methods for turbulence measurements for other systems such as eddy-correlation. The JTECH paper by Starkenburg et al. (2016) review a number of methods, including those of Goring and Nikora. Starkenburg et al. (2016) deemed median based filtering a more robust means of filtering data since it can handle missing points more easily, and handles better timeseries with evidence of low-frequency coherent turbulent structures.

• Requires first detrending the time serie
• Recursive/iterative process
• Universal threshold based on ..

Notes

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