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Laboratory in Oceanography: Data and Methods

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Title: Laboratory in Oceanography: Data and Methods


1
Laboratory in Oceanography Data and Methods
Methods for Non-Stationary Means
  • MAR599, Spring 2009
  • Miles A. Sundermeyer

2
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Recall, for OA
  • Assumed field is homogeneous and isotropic.
  • Assumed errors do not co-vary with themselves or
    with observations, and that errors have zero
    mean.
  • Estimated field based on observations and
    correlation matrix (assumes the observations are
    correlated with each other).
  • Computed expected error variances (Note, as long
    as stations dont change w/ time, errors also
    dont change with time. Can use this to explore
    possible station schemes to minimize error in
    maps.)

3
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Types of kriging
  • Simple kriging (OA, OI) known constant mean,
    µ(x) 0.
  • Ordinary kriging - unknown but constant mean,
    µ(x) µ, and enough observations to estimate the
    variogram/correlation function
  • Universal kriging - assumes mean is unknown but
    linear combination of known functions,
  • Extensions
  • Lognormal kriging
  • Vector fields (incorporate non-divergence, or
    geostrophy)
  • Non-isotropic (challenge for coastal OA see OAX
    from Bedford Institute of Oceanography)
  • Multivariate

4
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Extensions of simple kriging (OI,OA)
  • Consider problem of a localized tracer, such as
    dye-release experiment, river plume, or other
    localized field.
  • Suppose non-zero mean can always subtract the
    mean
  • Suppose non-isotropic can scale different
    directions (assuming correlation function is
    still the same)
  • Suppose spatially varying mean ... need universal
    kriging for this

5
Methods for Non-Stationary Means OA (contd) and
Kriging
Example Dye mapping during Coastal Mixing
Optics Experiment (CMO)
6
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Example CMO
  • Dye concentration varies spatially approx.
    Gaussian in x and y at large scales.
  • Wish to map small-scale variability capture
    variability within patch

7
Methods for Non-Stationary Means OA (contd) and
Kriging
Example CMO
8
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Example CMO
  • Start with large-scale interpolation

9
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Example CMO
  • Start with large-scale interpolation (b6 km,
    a2)
  • interpolate smoothed map onto observation
    points as spatially varying mean.

10
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Example CMO
  • compute covariance function of residual from
    first pass kriging (data minus spatially varying
    mean).

11
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Example CMO
  • Do 2nd pass kriging on residual
  • Obtain kriging estimate and error map

12
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Example CMO
  • Do 2nd pass kriging on residual
  • Obtain kriging estimate and error map

13
Methods for Non-Stationary Means OA (contd) and
Kriging
Nugget Effect Though correlation at zero lag is
theoretically 1, sampling error and small scale
variability may cause observations separated by
small distances to be dissimilar. This causes a
discontinuity at the origin of the correlation
function called the nugget effect.
14
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Anisotropy
  • Kriging/OA can handle different correlation
    length scales in different coordinate directions.
  • Can also handle time correlations for
    spatio-temporal data
  • Example OAX (developed by Bedford Institute of
    Oceanography)

15
Methods for Non-Stationary Means OA (contd) and
Kriging
  • Block Kriging
  • Use only data within certain range to estimate
    value at particular location. Minimizes size of
    inversion required for OA.

16
Methods for Non-Stationary Means OA (contd) and
Kriging
Subjective Objective analysis Need to be
mindful of decisions made during OA / kriging
analysis
http//people.seas.harvard.edu/leslie/MBST98/ll_a
nalysis.html
17
Methods for Non-Stationary Means OA (contd) and
Kriging
  • References
  • A. G. Journel and CH. J. Huijbregts " Mining
    Geostatistics", Academic Press 1981

18
Laboratory in Oceanography Data and Methods
Methods for Non-Stationary Means (contd)
  • MAR599, Spring 2009
  • Miles A. Sundermeyer

19
Methods for Non-Stationary Means Complex
Demodulation
  • Basics idea of Complex Demodulation
  • Complex demodulation can be thought of as a type
    of band-pass filter that gives the time variation
    of amplitude and phase of a time series in a
    specified frequency band.
  • To implement
  • Frequency-shift time series by multiply by e-iwt,
    where w is the central frequency of interest.
  • Low-pass filter to remove frequencies greater
    than the central frequency. The low pass acts as
    a band-pass filter when the time series is
    reconstructed (unshifted).
  • Express complex time series as a time-varying
    amplitude and phase of variability in band near
    the central frequency that is, X(t) A(t)
    cos(wt -(ft)), where A(t) is the amplitude and
    f(t) the phase for a central frequency w, and
    X(t) is the reconstructed band-passed time
    series.
  • (Note the phase variation can also be thought
    of as a temporal compression or expansion of a
    nearly sinusoidal time series, which is
    equivalent to a time variation of frequency. )

20
Methods for Non-Stationary Means Complex
Demodulation
  • Example Idealized signal
  • 7 day record
  • Signal has period of ½ day (w2 cpd)
  • A(t) has period of 3.5 days
  • f(t) has period of 7 days

21
Methods for Non-Stationary Means Complex
Demodulation
  • The Math (simplified) ...
  • Time series is assumed to be a combination of
    nearly periodic signal with nominal frequency w,
    plus everything else, Z(t).
  • Amplitude, A(t), and phase f(t), of the periodic
    signal are assumed to vary slowly in time
    compared to base frequency, w.
  • Can write
  • Step 1 Multiply by e-iwt gt Y(t)
    X(t)e-iwt, which can be written as
  • 1st term varies slowly, with no power at or above
    w
  • 2nd term varies at freq 2w
  • 3rd term varies at freq w (and none at zero freq)

22
Methods for Non-Stationary Means Complex
Demodulation
  • Step 2 Low-pass filter to remove frequencies at
    or above frequency w. This smoothes the 1st
    term, and nearly removes 2nd and 3rd terms,
    giving
  • where prime indicates smoothing. The choice of
    filter determines what frequency band remains.
  • Step 3 Isolate A(t) and f(t)

see also http//www.pmel.noaa.gov/maillists/tmap/
ferret_users/fu_2007/msg00180.html
23
Methods for Non-Stationary Means Complex
Demodulation
  • Example Coastal Mixing and Optics Shipboard
    Velocity

time (days)
24
Methods for Non-Stationary Means Complex
Demodulation
25
Methods for Non-Stationary Means Complex
Demodulation
26
Methods for Non-Stationary Means Complex
Demodulation
27
Methods for Non-Stationary Means Complex
Demodulation
28
Methods for Non-Stationary Means Complex
Demodulation
29
Methods for Non-Stationary Means Complex
Demodulation
30
Methods for Non-Stationary Means Complex
Demodulation
31
Methods for Non-Stationary Means Complex
Demodulation
32
Methods for Non-Stationary Means Complex
Demodulation
33
Methods for Non-Stationary Means Complex
Demodulation
34
Methods for Non-Stationary Means Complex
Demodulation
  • Useful Tidbits
  • Bloomfield, P. 1976. Fourier decomposition of
    time series An introduction, 258 pp., John
    Wiley, New York.
  • Matlab has a communications toolbox with many
    implementations/functions
  • fmmod, fmdemod - frequency modulation and
    demodulation
  • pmmod, pmdemod - phase modulation and
    demodulation
  • References
  • Chelton, D. B. and R. E. Davis, 1982. Monthly
    mean sea level variability along the west coast
    of North America, J. Phys. Oceanogr., 21,
    757-784.
  • Bingham, C., M. D. Godfrey, and J. W. Tukey,
    "Modern Techniques of Power Spectrum
    Estimation,"  IEEE Transactions on Audio and
    Electro-acoustics, Volume AU-15, Number 2, June
    1967, pp. 56-66.

35
Methods for Non-Stationary Means Complex
Demodulation
  • Example Applications
  • J. Hyatt and R. C. Beardsley - Observations of
    near-inertial motions in sea ice and the upper
    ocean mixed layer in Marguerite Bay, western
    Antarctic Peninsula shelf, Geophysical Research
    Abstracts, Vol. 7, 04162, 2005.
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