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Title: Problems in Atmospheric Sciences:


1
Problems in Atmospheric Sciences Potential
Utility of Infrasound Data
  • Midlatitude Cyclones
  • Tropical Cyclones
  • WW3 Microbaroms

2
Forecast Errors over Pacific
West Coast Forecast Bust a Costly Embarrassment
in Eugene, Ore.
3
Forecast Errors over Pacific
L
976
NCEP Eta model 24-hr (solid) and 48-hr (dashed)
SLP forecast (mb) for 00 UTC on 3 March 1999 and
GOES infrared satellite image.
4
Forecast Errors over Pacific
24-hr (top) and 48-hr (bottom) SLP forecast
errors (mb) for period 11/01-04/02.
5
Forecast Busts
Model 48-hr forecast (solid) and analysis
(dashed) of Sea Level Pressure (every 2 mb) for
14 December 2001
Eta
AVN
NOGAPS
UKMO
6
Forecast Errors over Pacific
Model storm forecast central SLP errors (mb) and
storm position errors for period 00 UTC 14 Dec
2001.
7
Lightning Detection
This noise can be detected by a network of
special receivers located on remote Pacific
islands.
8
Lightning Detection Project (ONR)
Noise from lightning measured by PACNET can be
used to estimate the rainfall rate.
9
Sea-level Pressure Map at 18 UTC (left panel) and
Long Range Cloud-to-ground Lightning Detected
between 1453 and 1753 UTC (right panel) 18
December 2002.
Pacific Extratropical Cyclone
10
Sea-level Pressure Map at 3 UTC (left panel) and
Long Range Cloud-to-ground Lightning Detected
between 2353 and 0253 UTC (right panel) 18-19
December 2002.
Pacific Extratropical Cyclone
11
Sea-level Pressure Map at 6 UTC (left panel) and
Long Range Cloud-to-ground Lightning Detected
between 0253 and 0553 UTC (right panel) 19
December 2002.
Pacific Extratropical Cyclone
12
Sea-level Pressure Map at 9 UTC (left panel) and
Long Range Cloud-to-ground Lightning Detected
between 0553 and 0853 UTC (right panel) 19
December 2002.
Pacific Extratropical Cyclone
13
Sea-level Pressure Map at 12 UTC (left panel) and
Long Range Cloud-to-ground Lightning Detected
between 0853 and 1153 UTC (right panel) 19
December 2002.
Pacific Extratropical Cyclone
14
Sea-level Pressure (SLP) Map at 12 UTC (left
panel) and Eta SLP Forecasts valid at 12 UTC (24
and 12 hr forecasts shown in middle and far right
panels, respectively) 19 December 2002.
Pacific Extratropical Cyclone
15
Forecasting a Kona low
AVN Forecast Pressure Traces
16
Winter Storm Summary
  • Large short-term (0-48 hr) forecast errors (gt10
    mb) occur 10-15 times each winter over the
    northeast Pacific in the Eta model.
  • Large initialization errors over the Pacific
    still occur in all operational forecast systems
    and are major contributors to short-term forecast
    failures.
  • Occasionally small initial errors grow into large
    forecast errors.
  • Large position errors of surface low centers
    contribute to large forecast errors of SLP at
    coastal locations.
  • Forecast failures over the eastern Pacific Ocean
    propagate downstream and can contribute to large
    forecast errors over the eastern half of the U.S.
  • Is there a role for infrasound in toward solving
    this problem?

17
The Hurricane Problem
What do we know about hurricanes?
18
Hurricane Track Forecasting
Track forecasts from numerical and statistical
models are compared to come up with the best
forecast track.
19
Hurricane Track Forecasting
Hurricanes track forecasting has made significant
gains in the past 30 years due to faster
computers and better observations of storm
steering currents by aircraft and satellite
instruments.
20
Hurricane Intensity Forecasting
Hurricanes intensity forecasting has made almost
no gains in the past 30 years despite faster
computers and better observations of storm
environment by aircraft and satellite
instruments. Part of problem is a lack of
understanding of energy transfer from ocean to
atmosphere, which in turn depends on the
particulars of the boundary layer structure and
circulation.
21
Radar Analysis
Doppler Velocity
A residual velocity for each elevation is
obtained by subtracting the 0th order
(sinusoidal) component of the velocity field as
observed by the radar along a conical scan of set
elevations.
Residual Velocity
VAD Velocity
22
Animation of Velocity Residuals in Hurricane
Bonnie
23
Boundary Layer Rolls Characteristics
Schematic depicting hurricane boundary layer
rolls, showing the mean values for 142 BL rolls
observed during four hurricane landfalls (142
cases).
24
Developing a Hurricane Balloon to study
Lagrangian enegetics of airflow
25
Developing a Hurricane Balloon
  • GPS position
  • Satellite cellular telephone for communication
  • Lift control
  • Lots of sensors
  • Microphone?

26
Developing a Hurricane Balloon
Release in Hawaii
27
What are microbaroms?
  • Microbaroms signals, like microseisms, are
    believed to be created by the nonlinear
    interaction of ocean surface waves
  • The microbarom peak near 0.2 Hz is right on the
    detection frequency band for 1 kt explosions
  • IMS arrays with large apertures (gt 1 km) were
    supposed to render microbaroms incoherent, but
    distinct coherent bursts may still be detected
  • Microbaroms may be generated in open ocean or by
    reflections with coastline and islands, and are
    prominent on island stations
  • Theoretical energy peak of microbarom radiation
    is near vertical, but this energy is lost
  • Sufficient energy is radiated near the
    horizontal, where most microbarom arrivals are
    detected
  • Study microbarom statistics at I59US and global
    distribution of microbarom signal levels

28
Microbaroms 2002
N Swells, Aleutians
Trade and S Swells
29
Theory Arendt and Fritz, 2000
  • Assumptions
  • Wave height small relative to wavelength of ocean
    wave
  • Distance greater than acoustic wavelength
  • Solution
  • For a prescribed surface wave displacement g(x,t)
    and vertical velocity uz(x,t), the acoustic
    pressure is

30
Theory
  • Consider a ocean surface wave displacement
    spectrum A,

The radiated acoustic spectrum would be
31
Wave Watch 3 (WW3)
  • WAVEWATCH III (Tolman 1997, 1999a) is a third
    generation wave model developed at NOAA/NCEP.
  • WAVEWATCH III solves the spectral action density
    balance equation for wavenumber-direction
    spectra. The implicit assumption of these
    equations is that the medium (depth and current)
    as well as the wave field vary on time and space
    scales that are much larger than the
    corresponding scales of a single wave.
    Furthermore, the physics included in the model do
    not cover conditions where the waves are severely
    depth-limited. This implies that the model can
    generally by applied on spatial scales (grid
    increments) larger than 1 to 10 km, and outside
    the surf zone.

http//polar.ncep.noaa.gov/waves/wavewatch/
32
Young Swell case (0-4 days old)
33
Middle Age Swell case (4-6 days old) All with
identical forcing
34
Old Swell case (6-10 days old) All with identical
forcing
35
Atmospheric Forcing
Surface winds associated with January 2003 Case
36
Wave Watch 3 (WW3)
Wave height and dominant period
37
January 2003 Case
Wave Spectra
38
January 2003 Case
Microbarom arrivals
39
Fig. 2 Observed infrasonic arrival azimuth for
microbarom signals (0.1-0.5Hz) in comparison with
azimuth from Hawaii to Hurricane Daniels core
(Red Line).
Fig. 1 Hurricane Daniel as seen by GOES 10 on
July 26, 2000. ISLA will attempt to accurately
depict the wind/wave field produced by Hurricane
Daniel in order to model microbaroms produced by
the nonlinear interaction of Daniels ocean
surface waves.
40
Evaluating the Theoretical Model
The Wave Watch 3 model outputs the variance
density , F, of the surface wave field as a
function of frequency, f, and propagation
direction,q. The variance density can be
integrated over angle and frequency to provide
the total wave energy E,
The peak source pressure occurs when k -k, w
w
For preliminary amplitude estimates, we use
Whitakers relationship
41
Global Pressure Field Frequency steps of 0.01 Hz
42
Predicted vs Observed
43
Microbarom Conclusions and future work
  • All IMS infrasound arrays, and particularly those
    close to the ocean, are susceptible to
    microbaroms
  • Surface wave spectrum from Wave Watch 3 global
    model
  • Algorithm to evaluate a theoretical source
    pressure field induced by the open ocean surface
    wave field
  • Used simple relationship to estimate global
    infrasonic field
  • Need to add atmospheric specifications,
    attenuation losses, and direction of arrival
    information
  • Need to incorporate better propagation algorithms
    to provide time dependent and frequency dependent
    estimates of the propagating infrasonic field
  • Need to add reflections with coastline and
    islands mesoscale problem, site dependent and
    not trivial
  • Approach can be adapted to microseisms

44
Time for Barnstorming?
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