Frequency and Instantaneous Frequency A Totally New View of Frequency

Frequency and Instantaneous Frequency

A Totally New View of Frequency

Definition of Frequency

Given the period of a wave as T ; the frequency is defined as

T.

1

Equivalence :

• The definition of frequency is equivalent to defining velocity as

Velocity = Distance / Time

• But velocity should be

V = dS / dt .

Traditional Definition of Frequency

• frequency = 1/period.

• Definition too crude• Only work for simple sinusoidal waves• Does not apply to nonstationary processes• Does not work for nonlinear processes • Does not satisfy the need for wave

equations

Definitions of Frequency : 1For 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

Jean-Baptiste-Joseph Fourier

1807 “On the Propagation of Heat in Solid Bodies”

1812 Grand Prize of Paris Institute

“Théorie analytique de la chaleur”

‘... the manner in which the author arrives at these equations is not exempt of difficulties and that his analysis to integrate them still leaves something to be desired on the score of generality and even rigor.’

1817 Elected to Académie des Sciences

1822 Appointed as Secretary of Académie

paper published

Fourier’s work is a great mathematical poem. Lord Kelvin

Fourier Spectrum

Random and Delta Functions

Fourier Components : Random Function

Fourier Components : Delta Function

Problems with Integral methods

• Frequency is not a function of time within the integral limit; therefore, the frequency variation could not be found in any differential equation, other than a constant.

• The integral transform pairs suffer the limitation imposed by the uncertainty principle.

Definitions of Frequency : 2For Simple Dynamic System

TC

0

4. Dynamic System through Hamiltonian :

H( p,q,t ) and A( t ) pdq ;

H.

A

This is an system analysis but not a data analysis method.

Definitions of Frequency : 3Instantaneous Frequency for IMF

only

5. Teager Energy Operator

6. Period between zero cros sin gs and extrema

Teager Energy Operator : the Idea

H. M. Teager, 1980: Some observations on oral air flow during phonation, IEEE Trans. Acoustics, Speech, Signal Processing, ASSP-28-5, 599-601.

2c

2 2c

2 4c

c c

c c

[ x( t ) ] x ( t ) x( t ) x( t ) :

For x( t ) A sin t , then

[ x( t ) ] A .

[ x( t ) ] A .

[ x( t )] [ x( t )]; A

[ x( t )] [ x( t )]

Generalized Zero-Crossing :By using intervals between all combinations of zero-crossings and

extrema.

T1

T2

T4

Generalized Zero-Crossing :Computing the weighted frequency.

1 11

1 21 22 41 42

2i 2i2i

4 i 4 i

4

4 i

3 44

At any location, there are7 different int erval values :

11 T f ; we assign weight a factor 4

4T

12 T f ; we assigna weight factor 2

2T

14 T f ; we assigna weight facto

4 f 2( f f ) f f f ff

r

.2

1T

1

Problems with TEO and GZC

• TEO has super time resolution but it is strictly for linear processes.

• GZC is robust but its resolution is too crude.

Definitions of Frequency : 4Instantaneous Frequency for IMF only

ji ( t )

2 1

jj

j

8.Quadrature method

yNormalized x ; y

7. HHT Analysis :

dx( t ) a( t ) e .

dt

1 x ; ( t ) tanx

d ( t )( t ) .

dt

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

Instantaneous Frequency is indispensable for nonlinear Processes

xx t

dtx

d 22

2 c( os1 ) .

x

The Idea and the need of Instantaneous Frequency

k , ;

t

t

k0 .

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. But how to find φ(x, t)?

Prevailing Views

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

Ideal case for Instantaneous Frequency

• Obtain the analytic signal based on real valued function through Hilbert Transform.

• Compute the Instantaneous frequency by taking derivative of the phase function from AS.

• This is true only if the function is an IMF, and its imaginary part of the analytic signal is identical to the quadrature of the real part. Unfortunately, this is true only for very special and simple cases.

p

i ( t )

2 2 1 / 2 1

For any x( t ) L ,

1 x( )y( t ) d ,

t

then, x( t )and y( t )are complex conjugate :

z( t ) x( t ) i y( t ) a( t ) e ,

where

y( t )a( t ) x y and ( t ) tan .

x( t )

Hilbert Transform : Definition

Limitations for IF computed through Hilbert Transform

• Data must be expressed in terms of Intrinsic Mode Function. (Note : Traditional applications using band-pass filter distorts the wave form; therefore, it can only be used for linear processes.) IMF is only necessary but not sufficient.

• Bedrosian Theorem: Hilbert transform of a(t) cos θ(t) might not be exactly a(t) sin θ(t). Spectra of a(t) and cos θ(t) must be disjoint.

• Nuttall Theorem: Hilbert transform of cos θ(t) might not be sin θ(t) for an arbitrary function of θ(t). Quadrature and Hilbert Transform of arbitrary real functions are not necessarily identical.

• Therefore, a simple derivative of the phase of the analytic function for an arbitrary function may not work.

Data : Hello

Empirical Mode Decomposition

Sifting to produce IMFs

Bedrosian Theorem

Let f(x) and g(x) denotes generally complex functions in L2(-∞, ∞) of the real variable x. If

(1) the Fourier transform F(ω) of f(x) vanished for │ω│> a and the Fourier transform G(ω) of g(x) vanishes for │ω│< a, where a is an arbitrary positive constant, or

(2) f(x) and g(x) are analytic (i. e., their real and imaginary parts are Hilbert pairs),

then the Hilbert transform of the product of f(x) and g(x) is given

H { f(x) g(x) } = f(x) H { g(x) } .

Bedrosian, E., 1963: A Product theorem for Hilbert Transform, Proceedings of the IEEE, 51, 868-869.

Nuttall Theorem

For any function x(t), having a quadrature xq(t), and a Hilbert transform xh(t); then,

where Fq(ω) is the spectrum of xq(t).

Nuttall, A. H., 1966: On the quadrature approximation to the Hilbert Transform of modulated signal, Proc. IEEE, 54, 1458

2

0

02

q

E xq( t ) xh( t ) dt

2 F ( ) d ,

Difficulties with the Existing Limitations

• Data are not necessarily IMFs.

• Even if we use EMD to decompose the data into IMFs. IMF is only necessary but not sufficient because of the following limitations:

• Bedrosian Theorem adds the requirement of not having strong amplitude modulations.

• Nuttall Theorem further points out the difference between analytic function and quadrature.

• The discrepancy, however, is given in term of the quadrature spectrum, which is an unknown quantity. Therefore, it cannot be evaluated. Nuttall Theorem provides a constant limit not a function of time; therefore, it is not very useful for non-stationary processes.

Analytic vs. Quadrature

X(t)

Y(t) Z(t) Analytic

Hilbert Transform

Q(t) Quadrature, not analytic

No Known general method

Analytic functions satisfy Cauchy-Reimann equation, but may be x2+ y2 ≠ 1. Then the arc-tangent would not recover the true phase function.

Quadrature pairs are not analytic, but satisfy strict 90o phase shift; therefore, x2+ y2 = 1, and the arc-tangent always gives the true phase function.

For cosθ(t) with arbitrary function of θ(t) :

Normalization

To overcome the limitation imposed by Bedrosian Theorem

Why do we need Decomposition and Normalization :

We need a method to reduce the data to Intrinsic Mode Functions; then we also need a method for AM FM decomposition to over

come the difficulties stated in Bedrosian Theorem.

An Example : Step-function with Carrier

Data : Step-function with Carrier

Fourier Spectra for Step-function and Carrier

Hilbert Spectrum : Step-function with Carrier

Morlet Wavelet : Step-function with Carrier

Spectrogram : Step-function with Carrier

Data : Step-function with Carrier III

Hilbert Spectrum : Step-function with Carrier III

Problems with Hilbert Transform method

• If there is any amplitude change, the Fourier Spectra for the envelope and carrier are not separable. Thus, we violated the limitations stated in the Bedrosian Theorem; drastic amplitude change produce drastic deteriorating results.

• Once we cannot separate the envelope and the carrier, the analytic signal through Hilbert Transform would not give the phase function of the carrier alone without the influence of the variation from the envelope.

• Therefore, the instantaneous frequency computed through the analytic signal ceases to have full physical meaning; it provides an approximation only.

Effects of Normalization

Normalization method can give a true AM FM decomposition to over come

the difficulties stated in Bedrosian Theorem, and also provide a sharper

error index than Nuttall Theorem.

NHHT : Procedures • Obtain IMF representation of the data from siftings. • Find local maxima of the absolute value of IMF (to take

advantage of using both upper and lower envelopes) and fix the end values as maxima to ameliorate the end effects.

• Construct a Spline Envelope (SE) through the maxima.• When envelope goes under the data, straight line envelope

will be used for that section of the SE.• Normalize the data using SE : N-data = Data/SE. This steps

can be repeated.• Compute IF (FM) and Absolute Value (AV) from Hilbert

Transform of N-data.• Definition : Error Index = (AV-1)2.• Compute Instantaneous Frequency for SE (AM).

NHHT Procedures : 1. IMF from Data through siftings

NHHT Procedures : 2. Locate local maxima and fix the ends

NHHT Procedures : 3. Construct the Cubic Spline Envelope (CSE)

NHHT procedures:i

nn

n

n

F t f t is the empi

For an IMF x t withenvelope e t

x tf t

e t

x tf t e t x t

f te t e t e t e t

x tf t

e t e t e t

rical FM signal

A t e t e t e t is t

11

1 12

2 2 1 2

1 2

1 2

, ( ), ( ) :

( )( ) ;

( )

( )( ) ( ) ( )

( ) = ; ..

( ) ( ) ;

( ) ( )

.( ) ( ) ( ) ( )

( ) ...

( )( )

( ) ( ) ... (

( )

.)

he empirical AM signal .

NHHT Procedures : 4. Normalize the IMF through CSE

NHHT Procedures : 5. Compute IF through Hilbert Transform

NHHT Procedures : 6. Comparison of Hilbert Transforms of Data and

Normalized data

NHHT Procedures : 7. Define the Error Index = (AV – 1)2.

NHHT Procedures : 8. Define the IMF of Envelope

NHHT Procedures : 9. AM and FM of y=c3y(7001:8000,9)

NHHT : Procedures • Obtain IMF representation of the data from siftings. • Find local maxima of the absolute value of IMF (to take

advantage of using both upper and lower envelopes) and fix the end values as maxima to ameliorate the end effects.

• Construct a Spline Envelope (SE) through the maxima.• When envelope goes under the data, straight line envelope

will be used for that section of the SE.• Normalize the data using SE : N-data = Data/SE. This steps

can be repeated.• Compute IF (FM) and Absolute Value (AV) from Hilbert

Transform of N-data.• Definition : Error Index = (AV-1)2.• Compute Instantaneous Frequency for SE (AM).

Example : Exponentially Decaying Cubic Chirp

Model function

Exponentially decaying cubic chirp :Equation

3t t

x( t ) exp cos 2 ;128 512

t 0 : 1024 .

Exponentially decaying cubic chirp : Data

Exponentially decaying cubic chirp :Normalizing function

Exponentially decaying cubic chirp :Normalized carrier

Exponentially decaying cubic chirp :Phase Diagram

Exponentially decaying cubic chirp :Instantaneous Frequency

Exponentially decaying cubic chirp :Error Indices

Quadrature

To circumvent the limitation imposed by Nuttall Theorem

Nuttall Theorem

For any function x(t), having a quadrature xq(t), and a Hilbert transform xh(t); then,

where Fq(ω) is the spectrum of xq(t).

Nuttall, A. H., 1966: On the quadrature approximation to the Hilbert Transform of modulated signal, Proc. IEEE, 54, 1458

2

0

02

q

E xq( t ) xh( t ) dt

2 F ( ) d ,

Why do we need Quadrature :

To over come the difficulties stated in Nuttall Theorem for complicate phase

functions.

An Example : Duffing Pendulum

Duffing : Model Equation

Duffing type wave mod el :

t 0 : 1024;

t tx( t ) cos 0.3 sin( ) .

128 64

Duffing : Expansions of the Model Equation

For 1, the Model equationcanbe expanded as

x( t ) cos t sin 2 t

cos t cos sin 2 t sin t sin sin 2 t

cos t sin 2 t sin t ..

1 cos t cos 3 t .

.

...2 2

.

Duffing : Data

Duffing : Data, Quadrature & Hilbert

Duffing : Amplitude

Duffing : Phase

Duffing : Frequency truth is given by quadrature

Quadrature : Procedures

• Normalize the IMFs as in the NHHT method.

• Compute IF (FM) from Quadrature of N-data as follows:

2 1

Quadrature method

yNormalized x ; y 1 x ; ( t ) tan

x

d ( t )( t ) .

dt

Validation of NHHT and Quadrature Methods

Through examples using• NHHT• HHT• GZC• TEO

• Quadrature

Example : Duffing Equation

Model function

Damped Chirp Duffing Model

2 2t t tx( t ) exp cos 32 0.3 sin 32 ,

256 64 512 32 512

with t 0 : 1024 .

Example : Speech Signal ‘Hello’

Real Data

Data : Hello

Data : Hello IMF

Hello : Data c3y(8)

Hello : Check Bedrosian Theorem

Hello : Instantaneous Frequency & data c3y(8)

Hello : Instantaneous Frequency & data Details c3y(8)

A Physical Example : Water Surface Waves

Real Laboratory Data


k , ;

t

t

k0 .

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.


g

g j

j

EC E 0 ; Energy

t x

C EE0 ; Action

t x

According to the classic wave theory, there are other more important wave conservation laws for Energy and Action:

Therefore, if frequency is a function of time, it has to satisfy certain condition for both laws to be valid.

Data

Governing Equations I:

2

22 2

2

, 0,

1, 0,

2

, .

z

z gt z t

zt z

Governing Equations II:

2

2

2

2

2 22 22

2

0, 0,

10, 0,

2

, , , 0 ,

1 1.

2 2

h h h h

h

z L L Qz t

zt z z

where L gt z x y

Q Lz t z

Governing Equations III:

2 22

22

..... . .

.... . .

.

kz i kz i

i i

Ae e A e e c c

Be B e c c

wherer k x t

Governing Equations IV: The 4th order Nonlinear Schrodinger

Equation

2 22

2 2

3 3

2 3

2

1 1 12

2 2 4

1 36

8 2

1.

2

A A A Ai A A

t x y x

A A A Ai iA A A

x y x x x

Ai A A i

x x z

Dysthe, K. B., 1979: Note on a modification to the nonlinear Schrodinger equation for

application to deep water waves. Proc. R. Soc. Lond., 369, 105-114.

Equation by perturbation up to 4th order.

But ω = constant.

Data and IF : Station #1



Phase Averaged Data and IF : Station #1




Summary

• Instantaneous frequency could be highly variable with high gradient.

• The assumption used in the classic wave theory might not be totally attainable.

• Coupled with the fusion of waves, we might need a new paradigm for water wave studies.

Comparisons of Different Methods

• TEO extremely local but for linear data only.• GZC most stable but offers only smoothed

frequency over ¼ wave period at most.• HHT elegant and detailed, but suffers the

limitations of Bedrosian and Nuttall Theorems.• NHHT, with Normalized data, overcomes

Bedrosian limitation, offers local, stable and detailed Instantaneous frequency and Error Index for nonlinear and nonstationary data.

• Quadrature is the best, but the sampling rate has to be sufficiently high.

Conclusions

• Instantaneous Frequency could be calculated routinely from the normalized IMFs through quadrature (for high data density) or Hilbert Transform (for low data density).

• For any signal, there might be more than one IF value at any given time.

• For data from nonlinear processes, there has to be intra-wave frequency modulations; therefore, the Instantaneous Frequency could be highly variable.

Documents

Frequency and Instantaneous Frequency A Totally New View of Frequency