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    Wavelet Transform and

    Some Applications in Time

    Series Analysis andForecasting

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    A little bit of history.

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    Jean Baptiste Joseph Fourier (1768 1830)

    1787: Train for priest (Left but Never married!!!).

    1793: Involved in the local Revolutionary Committee.1974: Jailed for the first time.

    1797: Succeeded Lagrange as chair of analysis andmechanics at cole Polytechnique.

    1798: Joined Napoleon's army in its invasion of Egypt.

    1804-1807: Political Appointment. Work on Heat.Expansion of functions as trigonometrical series.Objections made by Lagrange and Laplace.

    1817: Elected to the Acadmie des Sciences in andserved as secretary to the mathematical section.Published his prize winning essay Thorie analytique de

    la chaleur.1824: Credited with the discovery that gases in theatmosphere might increase the surface temperature ofthe Earth (sur les tempratures du globe terrestre et desespaces plantaires ). He established the concept ofplanetary energy balance. Fourier called infrared

    radiation "chaleur obscure" or "dark heat.

    MGP: Leibniz - Bernoulli - Bernoulli - Euler - Lagrange - Fourier Dirichlet - .

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    Windowed (Short-Time) Fourier Transform (1946)

    James W. Cooley and John W. Tukey, "An algorithmfor the machine calculation of complex Fourier series,"Math. Comput.19, 297301 (1965).

    Independently re-invented an algorithm known to CarlFriedrich Gauss around 1805

    Fast Fourier Transform

    Dennis Gabor

    James W. Cooley and John W. Tukey

    Winner of the 1971 Nobel Prize for contributions to the principlesunderlying the science of holography, published his now-famous paperTheory of Communication.2

    C. F. Gauss

    Stephane Mallat, Yves Meyer

    Jean Morlet

    Presented the concept of wavelets (ondelettes) in its present theoretical formwhen he was working at the Marseille Theoretical Physics Center (France).

    (Continuous Wavelet Transform)

    (Discrete Wavelet Transform) The main algorithm datesback to the work of Stephane Mallat in 1988. Then joined Y.Meyer.

    http://euler.ciens.ucv.ve/matematicos/images/gauss.gif
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    Motivation.

    Earthquake

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    Fourier Transform

    1

    0

    /21N

    k

    Nink

    in efN

    f

    2,.....,1

    2

    NNn

    dfdttf22

    dtetff ti 2

    deftf ti2

    Fourier Transform

    Inverse Fourier Transform

    Parseval Theorem

    Discrete Fourier Transform

    Phase!!!

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    Limitations???

    Non-Stationary SignalsFourier does not provide information about when different periods(frequencies)where important: No localization in time

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    has the same support for everyand , but the number of cycles varieswith frequency.

    dttgtfuGf u,,

    Windowed (Short-Time) Fourier Transform

    tiu eutgtg

    2

    ,

    tg u, u

    Estimates locally around , the amplitude ofa sinusoidal wave of frequency

    2412ueug D. Gabor

    u ug Function with local support.

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    Limitations??

    Fixed resolution.

    Related to the Heisenberg uncertainty principle. The product of the standard deviationin time and frequency is limited.

    The width of the windowing function relates to the how the signal is represented itdetermines whether there is good frequency resolution (frequency components closetogether can be separated) or good time resolution (the time at which frequencies change).

    Selection of determines and . ug g g

    ggt

    00 Localization:

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    Example.

    x(t) = cos(210t) for

    x(t) = cos(225t) for

    x(t) = cos(250t) for

    x(t) = cos(2100t) for

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    Wavelet Transform

    dtttfuW u,, 0

    utt

    u

    1,

    Gives good time resolution for high frequency events, and good frequency resolution for lowfrequency events, which is the type of analysis best suited for many real signals.

    0dtt

    dtt

    12dttMother wavelet

    properties

    0

    2

    ,

    0

    2

    ,

    0

    ,

    d

    d

    t

    t

    t

    0,10,1

    0,1

    0

    0

    t

    t,

    t,

    t,

    0,1

    0

    0

    0,1

    ,

    t

    .

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    Wavelet Transform

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    Some Continuous Wavelets

    241

    2

    0

    eei

    Morlet

    ut

    tu

    1,

    tiu eutgtg

    2

    ,

    2412

    ueug Gabor

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    Torrence and Compo (1998)

    Continuous Wavelet

    Transform

    For Discrete Data

    Time series

    Wavelet

    Defined as the convolution with a scaledand translated version of

    DFT (FFT) of the time series

    N times for each s: Slow!

    Using the convolution theorem,the wavelet transform is theinverse Fourier transform

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    Mallat's multiresolution framework

    Design method of most of thepractically relevant discrete

    wavelet transforms (DWT)

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    Doppler Signal

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    sin(5t)+sin(10t) sin(5t) sin(10t)

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    Earthquake

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    Sun Spots

    Power 9-12 years

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    Length of Day

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    Filtering (Inverse Wavelet Transform)

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    Wavelet Coherency

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    Wavelet Cross-SpectrumWavelet Coherency

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    Forecasting South-East AsiaIntraseasonalVariability

    Webster, P. J, and C. Hoyos, 2004: Prediction of Monsoon

    Rainfall and River Discharge on 15-30 day Time Scales.

    Bul l . Amer. Met. Soc., 85 (11), 1745-1765.

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    Indian Monsoon: Spatial-Temporal Variability

    Active and Break Periods1. Strong annual cycle. Strong spatial variability.2. Intraseasonal Variability >>> Interannual Variability

    3. Strong impact in Indias economy

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    OLR Composites based

    on active periods.

    Selection of Active phases

    Regional Structure of the Monsoon Intraseasonal Variability MISO

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    OLR Composites

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    Development of an empirical scheme

    Choice of the predictors: These are physicallybased and strongly related the MISO evolution(identified from diagnostic studies).

    Time series are separated through identification ofsignificant bands from wavelet analysis of thepredictand (Same separation made for predictors).

    Coefficients of the Multi-linear regression change

    are time-dependent.

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    Predictors

    OLR Field Predictors

    Central India

    Central IO

    Somali Jet Intensity

    Tropical Easterly Jet IndexSea-level pressure

    Central India

    Surface Wind Predictors

    U-comp

    U, V-comp 200mb U-comp

    Upper-tropospheric predictors

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    Predictands

    1. Central India Precipitation. 2. Regional Precipitation3. River Discharge

    St ti ti l S h W l t B di

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    Statistical Scheme: Wavelet Banding

    Statistical scheme uses wavelets to determine

    spectral structure of predictand.

    Based on the definition of the bands in the

    predictand, the predictors are also banded identically

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    Statistical Scheme: Regression Scheme

    Linear regression sets

    are formed betweenpredictand and predictor

    and advanced in time.

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    20-day forecasts for Central India

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    Error Estimation

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    All schemes use identical

    predictors

    Only the WB method

    appears to capture the

    intraseasonal variability

    So why does WB appear

    to work?

    Comparison of Schemes

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    Consider predictand made up oftwo periodic modes:

    F(t)2sin(t) sin(6t)

    Consider two predictors:

    G(t) sin(t 20) sin(3t)

    H(t) sin(6t 20) sin(4t)

    We can solve problem using:

    A regression technique

    Or

    Wavelet banding then

    regression

    The reason wavelet banding works can be seen from a simple example:

    R i A l i

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    With simple regression

    technique, the waves

    in the predictors (noise)

    that do not match the

    harmonics of the

    predictand introduce

    errors

    Compare blue and red

    curves. Correlation is

    reasonable but signalis degraded

    Regression Analysis

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    Filtering the predictors

    relative to the signature ofthe predictands eliminates

    noise.

    In this simple case the

    forecast is perfect.

    In complicated geophysical

    time series where coefficients

    vary with time, spurious

    modes are eliminated andBayesian statistical schemes

    are less confused.

    Wavelet Banding