Decomposing velocity measurements: Difference between revisions

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The quality-controlled velocities are first [[Detrending time series|detrended]] before being further analysed to determine [[Velocity past the sensor|mean flow past the sensor]] and [[Surface wave statistics|surface wave statistics]]. These quantities  are necessary for later choosing the appropriate [[Velocity inertial subrange model| inertial subrange model]] for [[Spectral fitting|spectral fitting]].
The quality-controlled velocities can be [[Detrending time series|detrended]] before being further analysed to determine [[Velocity past the sensor|mean flow past the sensor]] and [[Surface wave statistics|surface wave statistics]]. These quantities  are necessary for later choosing the appropriate [[Velocity inertial subrange model| inertial subrange model]] for [[Spectral fitting|spectral fitting]].
   
   
==Methods for detrending==
==Methods for detrending==
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There is no exact definition for what consists of a "trend", nor any set algorithm for identifying the trend. The following techniques can be used for detrending <ref name=Wuetal_PNAS/>:
There is no exact definition for what consists of a "trend", nor any set algorithm for identifying the trend. The following techniques can be used for detrending <ref name=Wuetal_PNAS/>:
# Linear trend removal
# Linear trend removal
# Low-pass linear filters (e.g., butterworth filter)
# Low-pass linear filters  
# Empirical modal decomposition
# Empirical modal decomposition


The first two methods presume the original time series is [[Stationarity|stationary]] and linear, while the third is adaptive and applicable to nonlinear and non-stationary timeseries.  
The first two methods presume the original time series is [[Stationarity|stationary]] and linear, while the third is adaptive and applicable to nonlinear and non-stationary timeseries.


[[File:Long timeseries.png|400px|thumb|Measured velocities at 4 Hz from an [[Acoustic-Doppler Velocimeters]] have been detrended using three different techniques. Empirical modal decomposition (EMD) <ref name="Wuetal_PNAS">{{Cite journal
[[File:Long timeseries.png|400px|thumb|Measured velocities at 4 Hz from an [[Acoustic-Doppler Velocimeters]] have been detrended using three different techniques. Empirical modal decomposition (EMD) <ref name="Wuetal_PNAS">{{Cite journal
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}}</ref>, linear trend, and a 2nd order low-pass Butterworth filter. A cut-off period of 10 min was targeted by both the filter and EMD]]
}}</ref>, linear trend, and a 2nd order low-pass Butterworth filter. A cut-off period of 10 min was targeted by both the filter and EMD]]


===Long continuous sampling===
==Application to measured velocities==
'''Info needs simplifying after convening as a subgroup'''
Measurements are typically collected in the following two ways:
Different techniques dependent on whether measurements were collected continuously or in long bursts.
* continuously, or in such long bursts that they can be considered continuous
* short bursts that are typically  at most 2-3x the expected largest turbulence time scales.  


===Short burst sampling===
As a rule of thumb, turbulence estimates from the inertial subrange of velocity rely on 5 to 15 min long-[[Segmenting datasets|segments]].
A short burst is typically at most 2-3x the expected largest turbulence time scales. As a rule of thumb, turbulence estimates from the inertial subrange of velocity rely on 5 to 15 min long-segments.


==Segmenting==
==Segmenting==

Revision as of 20:50, 29 November 2021


The quality-controlled velocities can be detrended before being further analysed to determine mean flow past the sensor and surface wave statistics. These quantities are necessary for later choosing the appropriate inertial subrange model for spectral fitting.

Methods for detrending

There is no exact definition for what consists of a "trend", nor any set algorithm for identifying the trend. The following techniques can be used for detrending [1]:

  1. Linear trend removal
  2. Low-pass linear filters
  3. Empirical modal decomposition

The first two methods presume the original time series is stationary and linear, while the third is adaptive and applicable to nonlinear and non-stationary timeseries.

Measured velocities at 4 Hz from an Acoustic-Doppler Velocimeters have been detrended using three different techniques. Empirical modal decomposition (EMD) [1], linear trend, and a 2nd order low-pass Butterworth filter. A cut-off period of 10 min was targeted by both the filter and EMD

Application to measured velocities

Measurements are typically collected in the following two ways:

  • continuously, or in such long bursts that they can be considered continuous
  • short bursts that are typically at most 2-3x the expected largest turbulence time scales.

As a rule of thumb, turbulence estimates from the inertial subrange of velocity rely on 5 to 15 min long-segments.

Segmenting

Chopping timeseries into smaller segments is essentially a form of filtering (box-car).

Notes

  1. Jump up to: 1.0 1.1 Zhaohua Wu, Norden E. Huang, Steven R. Long and and Chung-Kang Peng. 2007. On the trend, detrending, and variability of nonlinear and nonstationary time series. PNAS. doi:10.1073/pnas.0701020104

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