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Operational Oceanography: Modeling EM Propagation Characteristics

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Compare and contrast upper air sounding TDA inputs for the purpose of modeling ... Target: R/V Cypress Sea (small/medium sized vessel) with a regular ESM receiver ... – PowerPoint PPT presentation

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Title: Operational Oceanography: Modeling EM Propagation Characteristics


1
Operational OceanographyModeling EM Propagation
Characteristics
  • LT Erin OMarr
  • 7 Sept 2007

2
Purpose of the Study
  • Compare and contrast upper air sounding TDA
    inputs for the purpose of modeling EM propagation
    characteristics
  • In situ
  • Model
  • Identification of trapping layers and ducting
    layers affecting shipboard sensor propagation
    characteristics
  • Surface Search Radars

3
Operational Significance
  • As a Navy METOC Officer, we will be assigned
    to/support various deployable assets
  • Critical decisions about variations in
    capabilities of platform sensors, as well as,
    counter-detection
  • Fire Control Systems
  • Surface Search Radars
  • Communications
  • OPTEMPO in the littoral battlespace
  • Coastal region is becoming evermore important
  • Criticality of ship-to-ship and ship-to-shore
    radar and communications
  • The environment effects system performance
  • Proper characterization of the environment

4
Advanced Refractive Effects Prediction System
(AREPS)
  • Tactical Decision Aids (TDA)
  • Qualitative assessment of system performance
    given existing environmental conditions
  • AREPS is most widely used TDA for the prediction
    of radar ranges and signal propagation
    characteristics
  • Advanced Propagation Model (APM)
  • Extreme sensitivity to model inputs such as SST
    and RH
  • Quality input quality output
  • Critical area of research
  • Obtain an understanding of typical duct height
    values
  • Understand procedures for accurately estimating
    duct heights from routine measurements

5
Review Refraction Categories
Figure and Table courtesy of Davidson,
Assessment of Atmospheric Factors in EM/EO
Propagation, pp 3-18 .
6
Review Types of Ducting
Figure and Table courtesy of Davidson,
Assessment of Atmospheric Factors in EM/EO
Propagation, pp 3-21.
7
Evaporation Duct
  • The ED is one of an operators primary concerns
    over water
  • Can significantly enhance the range and strength
    of signal propagation
  • Radar
  • communications
  • The rapid, vertical decrease in relative
    humidity, at the surface, results in a
    simultaneous rapid decrease in the refractive
    index.
  • Primarily concerned with water vapor content
    however, RH is readily measured and
    representative of the amount of water vapor
    (pressure/specific humidity) present and
    coincident gradient
  • The gradient of the refractive index causes
    significant bending of the ray geometry
  • The EDH fluctuates throughout the day and is
    highly dependent of Tair, Tsea, q, and the wind
    component(s)
  • Local mixing above the sea surface
  • Surface-based duct with typical depths of 2-30m
  • EDH 10m is significant for surface radars with
    frequencies above 5GHz
  • Ducts 30m are significant for almost all radar
    frequencies

8
Data and Methodology
  • First leg of the Operational Oceanography cruise
  • Standard meteorological observations
  • Rawinsondes were launched to collect upper air
    soundings
  • Regional AF MM5 vertical profile forecasts
  • 15km horizontal resolution, 25mb vertical
    resolution, and 3-hr time step.
  • Vertical sounding data was extracted at or as
    close as possible to the soundings times and on
    the precise location of the in situ sounding
    launch point.
  • Calculated Evaporation Duct Height (EDH) and it
    added to environmental profile
  • Paulus/Jeske (P/J) model
  • In situ SST
  • Organic SWS, SWD, pressure, and Tair
  • AREPS standard project
  • Platform R/V Point Sur with standard 10GHz
    (X-band) radar at 15ft height.
  • Target R/V Cypress Sea (small/medium sized
    vessel) with a regular ESM receiver

9
Rawinsonde
MM5
Ship rawinsonde 18191313ZJUL07
Evidence of a shallow ED (17.98ft thick) present
at time of ship sounding. MM5 does not reflect
the ED however, does forecast the presence of a
subrefraction layer once SST is added (31.53ft
thick).
10
Ship rawinsonde 18191313ZJUL07
Range-height cross section of probability of
detection (Pd) using a near surface radar against
a small/medium-sized vessel target. Pd is
indicated by the color scale on the bottom.
Extended near-surface ranges due to ED.
11
Rawinsonde
MM5
Ship rawinsonde 20114219ZJUL07
Evidence of an ED layer at surface (30.2ft) and
various elevated ducts on the in situ sounding.
MM5 forecasts a deeper ED (58.12ft) however, no
elevated ducts.
12
Extended near-surface ranges due to ED.
ED almost 2x as thick as 18JUL
Ship rawinsonde 20114219ZJUL07
Range-height cross section of probability of
detection (Pd) using a near surface radar against
a small/medium-sized vessel target. Pd is
indicated by the color scale on the bottom.
Extended near-surface ranges due to ED.
13
Model has little to no skill in predicting ED
when observed SST is used for extrapolating the
ED. No further statistics were looked at.
14
Quality of input into TDA- APM is very sensitive
to SST and RH. Graphic shows in situ/model RH
differences. My hypothesis Observed SST (not
shown) created a discontinuous profile and
erroneous model predictions of propagation
characteristics.
15
Discussion
  • Value of observed surface variables added to
    rawinsonde/model
  • Knowledge of near surface atmosphere
    significantly aids the modeling of the existence,
    depth, and intensity of ducts
  • Need either both measured or both modeled to
    yield proper coupling between the SST and Air T
  • If adding obs SST to model sounding, must pay
    attention to the temperatures measured
  • If the SST is warmer than the lowest levels, the
    atmosphere would be less stable than it
    actually is
  • If model RH is off, the ED will be off
  • Underprediction or overprediction!
  • Appending an ED profile to an upper air profile
    takes manipulation
  • Gradients at the top of the EDH profile and the
    first gradient of the upper air profile cannot be
    too discontinuous
  • Focused on surface ranges, but no ducts shown in
    model
  • Model uses significant levels
  • Could be important for ducting situations at
    height and range

16
What do we do???
  • Vertical high resolution model fields
  • Use a model with SST fields
  • Make in situ SST observations to use
  • 2m wind and Air T/another level and extrapolate
    down
  • In Situ or land vertical sounding
  • Need to remove levels/add levels for ED over
    water (smoothing)
  • Climo?
  • AREPS has the capability to automatically append
    the EDH profile to upper air refractivity
    profiles from COAMPS files
  • COAMPS has the surface parameters to compute EDH
    profiles using bulk models (P/J, NPS)

17
Current Research-Models
  • Models of similar resolution proved to be useful
    in predicting the spatial distributions and
    diurnal variations of refractivity, but missed
    the fine vertical structure (which is critical)
  • In the case of our AO, the model resolution is
    not fine enough to accurately depict the
    localized processes caused by the San Nicolas
    islands
  • Further manipulation of vertical profile
  • The sfc obs represent the lower 1km and the
    profile above
  • Experiment have shown improvement using the
    technique.

Courtesy of Atkinson et al, 2000.
18
Current Research-Predicting EDH
  • Cannot be determined by rawinsondes (near-surface
    resolution is too coarse)
  • Atmospheric surface layer theory
  • Nomogram (TA, TS, RH, WS)
  • Model predictions of path losses
  • ED models developed that use bulk atmospheric
    measurements at a single altitude to blend with
    refractivity data measured at higher altitudes
  • As many measurements as possible at levels 10m
    and less
  • Minimum of two levels to extrapolate
  • AREPS
  • Automatically append the EDH profile to upper air
    refractivity profiles from COAMPS files

Courtesy of Babin et al, 1996.
19
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