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An Introduction to HHT: Instantaneous Frequency, Trend, Degree of Nonlinearity and Non- stationarity. Norden E. Huang Research Center for Adaptive Data Analysis Center for Dynamical Biomarkers and Translational Medicine NCU, Zhongli , Taiwan, China. - PowerPoint PPT Presentation
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An Introduction to HHT: Instantaneous Frequency, Trend,
Degree of Nonlinearity and Non-stationarity
Norden E. Huang
Research Center for Adaptive Data AnalysisCenter for Dynamical Biomarkers and Translational Medicine
NCU, Zhongli, Taiwan, China
OutlineRather than the implementation details,
I will talk about the physics of the method.
• What is frequency?
• How to quantify the degree of nonlinearity?
• How to define and determine trend?
What is frequency?
It seems to be trivial.
But frequency is an important parameter for us to understand many physical phenomena.
Definition of Frequency
Given the period of a wave as T ; the frequency is defined as
1.
T
Instantaneous Frequency
distanceVelocity ; mean velocity
time
dxNewton v
dt
1Frequency ; mean frequency
period
dHH
So that both v and
T defines the p
can appear in differential equations.
hase functiondt
Other Definitions of Frequency : For any data from linear Processes
j
Ti t
j 0
1. Fourier Analysis :
F( ) x( t ) e dt .
2. Wavelet Analysis
3. Wigner Ville Analysis
Definition of Power Spectral Density
Since a signal with nonzero average power is not square integrable, the Fourier transforms do not exist in this case.
Fortunately, the Wiener-Khinchin Theroem provides a simple alternative. The PSD is the Fourier transform of the auto-correlation function, R(τ), of the signal if the signal is treated as a wide-sense stationary random process:
2i 2S( ) R( )e d S( )d ( t )
Fourier Spectrum
Problem with Fourier Frequency• Limited to linear stationary cases: same
spectrum for white noise and delta function.
• Fourier is essentially a mean over the whole domain; therefore, information on temporal (or spatial) variations is all lost.
• Phase information lost in Fourier Power spectrum: many surrogate signals having the same spectrum.
Surrogate Signal:Non-uniqueness signal vs. Power Spectrum
I. Hello
The original data : Hello
The surrogate data : Hello
The Fourier Spectra : Hello
The Importance of Phase
To utilize the phase to define
Instantaneous Frequency
Prevailing Views onInstantaneous Frequency
The term, Instantaneous Frequency, should be banished forever from the dictionary of the communication engineer.
J. Shekel, 1953
The uncertainty principle makes the concept of an Instantaneous Frequency impossible.
K. Gröchennig, 2001
The Idea and the need of Instantaneous Frequency
k , ;
t
tk
0 .
According to the classic wave theory, the wave conservation law is based on a gradually changing φ(x,t) such that
Therefore, both wave number and frequency must have instantaneous values and differentiable.
p
2 2 1 / 2 1
i ( t )
For any x( t ) L ,
1 x( )y( t ) d ,
t
then, x( t )and y( t ) form the analytic pairs:
z( t ) x( t ) i y( t ) ,
wherey( t )
a( t ) x y and ( t ) tan .x( t )
a( t ) e
Hilbert Transform : Definition
The Traditional View of the Hilbert Transform for Data Analysis
Traditional Viewa la Hahn (1995) : Data LOD
Traditional Viewa la Hahn (1995) : Hilbert
Traditional Approacha la Hahn (1995) : Phase Angle
Traditional Approacha la Hahn (1995) : Phase Angle Details
Traditional Approacha la Hahn (1995) : Frequency
The Real World
Mathematics are well and good but nature keeps dragging us around by the nose.
Albert Einstein
Why the traditional approach does not work?
Hilbert Transform a cos + b : Data
Hilbert Transform a cos + b : Phase Diagram
Hilbert Transform a cos + b : Phase Angle Details
Hilbert Transform a cos + b : Frequency
The Empirical Mode Decomposition Method and Hilbert Spectral Analysis
Sifting
(Other alternatives, e.g., Nonlinear Matching Pursuit)
Empirical Mode Decomposition: Methodology : Test Data
Empirical Mode Decomposition: Methodology : data and m1
Empirical Mode Decomposition: Methodology : data & h1
Empirical Mode Decomposition: Methodology : h1 & m2
Empirical Mode Decomposition: Methodology : h3 & m4
Empirical Mode Decomposition: Methodology : h4 & m5
Empirical Mode DecompositionSifting : to get one IMF component
1 1
1 2 2
k 1 k k
k 1
x( t ) m h ,h m h ,
.....
.....h m h
.h c
.
The Stoppage Criteria
The Cauchy type criterion: when SD is small than a pre-set value, where
T2
k 1 kt 0
T2
k 1t 0
h ( t ) h ( t )SD
h ( t )
Or, simply pre-determine the number of iterations.
Empirical Mode Decomposition: Methodology : IMF c1
Definition of the Intrinsic Mode Function (IMF): a necessary condition only!
Any function having the same numbers ofzero cros sin gs and extrema,and also havingsymmetric envelopes defined by local max imaand min ima respectively is defined as anIntrinsic Mode Function( IMF ).
All IMF enjoys good Hilbert Transfo
i ( t )
rm :
c( t ) a( t )e
Empirical Mode Decomposition: Methodology : data, r1 and m1
Empirical Mode DecompositionSifting : to get all the IMF components
1 1
1 2 2
n 1 n n
n
j nj 1
x( t ) c r ,r c r ,
x( t ) c r
. . .r c r .
.
Definition of Instantaneous Frequency
i ( t )
t
The Fourier Transform of the Instrinsic ModeFunnction, c( t ), gives
W ( ) a( t ) e dt
By Stationary phase approximation we have
d ( t ) ,dt
This is defined as the Ins tan taneous Frequency .
An Example of Sifting &
Time-Frequency Analysis
Length Of Day Data
LOD : IMF
Orthogonality Check
• Pair-wise % • 0.0003• 0.0001• 0.0215• 0.0117• 0.0022• 0.0031• 0.0026• 0.0083• 0.0042• 0.0369• 0.0400
• Overall %
• 0.0452
LOD : Data & c12
LOD : Data & Sum c11-12
LOD : Data & sum c10-12
LOD : Data & c9 - 12
LOD : Data & c8 - 12
LOD : Detailed Data and Sum c8-c12
LOD : Data & c7 - 12
LOD : Detail Data and Sum IMF c7-c12
LOD : Difference Data – sum all IMFs
Traditional Viewa la Hahn (1995) : Hilbert
Mean Annual Cycle & Envelope: 9 CEI Cases
Mean Hilbert Spectrum : All CEs