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Decomposition nonstationary turbulence velocity in open channel flow

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Presentation on theme: "Decomposition nonstationary turbulence velocity in open channel flow"— Presentation transcript:

1 Decomposition nonstationary turbulence velocity in open channel flow
Ying-Tien Lin

2 Background Laminar flow and turbulent flow

3 Background Flow velocity profile

4 Background Turbulent flow occurs in our daily life.
put cube sugar into a cup of coffee Turbulent model Assume Turbulent velocity or Fluctuated velocity Mean velocity

5 Background Reynolds shear stress Sediment particles Shear stress River

6 Background Stationary turbulence flow
Nonstationary turbulence flow (occurs in flooding period) Mean velocity How to find its time-varying mean velocity?

7 Decomposition method Fourier decomposition method
Wavelet transformation Empirical mode decomposition

8 Fourier decomposition method
DFT LF Inv. DFT It is unable to show how the frequencies vary with time in the spectrum.

9 Wavelet transformation
DWT Threshold Inv. DWT Linear combinations of small wave Be able to show the frequency varies with time

10 Empirical Mode Decomposition (EMD)
The upper and lower envelopes of U(t) are constructed by connecting its local maxima and minima. Upper envelope Velocity Instantaneous velocity Lower envelope Time

11 Empirical mode decomposition (EMD)
The mean value of the two envelopes is then computed. The difference between the instantaneous velocity and the mean value is called the first intrinsic mode function (IMF), c1(t). IMF is a function that: 1. has only one extreme between zero crossings. 2. has a mean value of zero. This is called the Sifting Process

12 C1(t) C5(t) C12(t) residual(t)

13 Results Add noise Denoising

14 Results Add noise Denoising

15 Summary These three decomposition methods perform good fitting with the original functions. EMD seems better than the other two methods.


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