introduction : time-frequency analysis hht, wigner-ville and wavelet

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Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

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Page 1: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Introduction : Time-Frequency Analysis

HHT, Wigner-Ville and Wavelet

Page 2: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Motivations

• The frequency and energy level of data from real world phenomena are seldom constant. For example our speech, music, weather and climate are highly variable.

• Traditional frequency analysis is inadequate. • To describe such phenomena and understand

the underlying mechanisms we need the detailed time frequency analysis.

• What is Time-Frequency Analysis?

Page 3: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Traditional Methodsfor Time Series Analysis

• Various probability distributions

• Spectral analysis and Spectrogram

• Wavelet Analysis

• Wigner-Ville Distributions

• Empirical Orthogonal Functions aka Singular Spectral Analysis

Page 4: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Time-Frequency Analysis

• All time-frequency-energy representations should be classified as time-frequency analysis; thus, wavelet, Wigner-Ville Distribution and spectrogram should all be included.

• Almost by default, the term, ‘time-frequency analysis’, was monopolized by the Wagner-Ville distribution.

Page 5: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Conditions for Time-Frequency Analysis

• To have a valid time-frequency representation, we have to have frequency and energy functions varying with time.

• Therefore, the frequency and energy functions should have instantaneous values.

• Ideally, separated event should not influence each other and be treated independently.

Page 6: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Morlet Wavelet Spectrum

1 / 2

where

( ) is the Basic Wavelet function; for

Morlet Wavelet , it is the Gaussian modulated

sine and cosine fu

1 t bW ( a,b; x , ) x( t ) dt .

aa

a is the dilation factor , 1 / a is the frequen

nct

cy.

b is the translatio

ions

t

.

n fac

or , b is the time.

Page 7: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Wigner-Ville Distribution

i

2 i

wher

1W ( ,t ) x ( t ) x ( t ) e d

e

1S( ) x ( t ) x(

2

2

2

) e d

2

t

Wigner-Ville Distribution, W(ω, t), is defined as

WV Distribution has to be identical to the Fourier Power spectrum; therefore, the mean of Wigner-Ville Spectrum is the same as the Fourier spectrum, | S(ω) |2 .

Page 8: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

VW Instantaneous Frequency

i1W ( ,t ) x ( t )

W ( ,t

x ( t ) e d2 2 2

)d( t )

W ( , ).

t d

Therefore, at any given time, there is only one instantaneous frequency value.

What if there are two independent components? In this case, VW gives the weighted mean.

Page 9: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Spectrogram : Short-Time-Fourier Transform

2 i1S( : t , t ) x ( t ) x( t ) G( t , t )e d

2

Spectrogram is defined as

Note 1. G(t, Δt) is a window with zero value outside the duration of Δt.

Note 2. The spectrogram represents power density.

Page 10: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Addativity of Fourier Transforms (Spectra)

1 2

1 2

i t

t

If x( t ) x ( t ) x ( t ) then

S( ) S ( ) S ( ) ,

1where S( ) x( t ) e d t .

2

Page 11: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity of Power Spectral Properties

2 2 22

1 2 1 2 1 2

2 2

1 2

S S S S S 2 S S

S S .

Therefore, for Wigner-Ville Distribution, it is impossible to have two events occur at different time independently with different frequency to be totally independent of each other.

Both Wavelet and Spectrogram can separate events.

But, Sum of Spectrogram is not the Fourier Spectrum.

Page 12: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Marginal Requirement• Discrete Wavelet analysis with orthogonal basis should satisfy this requirement; Continuous Wavelet with redundancy and leakage would not satisfy this requirement.

• As the Wigner-Ville distributions have the marginal distribution identical to that of Power Spectral Density, there is the extra requirement that the marginal spectrum has to be PSD.

• A genuine instantaneous frequency distribution will also not satisfy this requirement (i.e. sum equals PSD). But the energy is conserved.

•Spectrogram does not satisfy this requirement, for it suffers the poor frequency resolution due to the limitation of the window length.

• This is not a very reasonable requirement. If PSD is inadequate to begin with, why should it be used as a standard?

Page 13: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Data 2 Waves

Page 14: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Fourier Spectra

Page 15: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Hilbert Spectrum

Page 16: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Wavelet Spectrum

Page 17: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Wigner-Ville Spectrum and Components

Page 18: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Wigner-Ville Spectrum

Page 19: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Fourier Components

Page 20: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Hilbert,Wigner-Ville & Wavelet Spectra

Page 21: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Marginal Hilbert and Fourier Spectra

Page 22: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Non-addativity Example : Marginal Hilbert and Fourier Spectra Details

Page 23: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

New Example : Data LOD 1962-1972

Page 24: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

New Example : Spectrogram (730)

Page 25: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

New Example : Spectrogram Details

Page 26: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

New Example : Wigner-Ville

Page 27: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

New Example : Morlet wavelet

Page 28: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

New Example : Hilbert Spectrum

Page 29: Introduction : Time-Frequency Analysis HHT, Wigner-Ville and Wavelet

Summary

• Wavelet, Spectrogram and HHT can all separate simultaneous events with different degrees of fidelity, but WV cannot.

• The instantaneous frequency defined by moments in WV is crude and illogical; it gives only one weighted mean IF value at any given time.

• Though WV satisfies the marginal energy requirement, it does not give WV any advantage in time-frequency analysis or even as an analysis tool.