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Differential O2 Absorption Barometric Pressure Radar (DIAR_BAR):
Improvements in Tropical Storm Forecasts
Qilong Min1, Bing Lin2, Yongxiang Hu2 , Wei Gong1, Steven Harrah2, Wes Lawrence3, Dion Fralick2,
1State University of New York, Albany, NY
2NASA Langley Research Center, Hampton, VA3Old Dominion University, Norfolk, VA
Spatial coverage: very limited Costs: high Uncertainty: ~1 mb
Existing techniques: in-situ
drift buoy
moored buoy
dropsonde
No remote sensing technique is available.
Sea surface pressure measurements
Atmospheric pressure : the primary driving force for atmospheric dynamics and generates wind fields that transport mass, moisture and momentum.
Historical studies
• Active & passive O2 A-band instruments
active: high stable laser system --- difficult
passive: daytime, cloud free, aerosol loading
• Microwave sounder
25 ~ 75GHz: multiple channels (6)
absorption: LW, WV
atmospheric and cloud temperature
footprints, sea surface reflectivities
Oxygen is uniformly mixed in the atmosphere, and attenuates the transmitted signal – less at lower freq. and more at higher freq.
The amount of attenuation is directly related to
barometric pressure and altitude.
f or 1/GHz)
PPRecRec
Atten
uation
Calibrated PRec
w/o Attenuation
Aircraft/Spacecraft-BasedQ-Band (50-56GHz) Radar
Measurement Concept
Pr () = PTAe2(, )0(, , )/(4R2()) (1)
Pr: radar received power; T: transmittance
() exp (OLV) = exp (OOLLVV) (2) where O = MP0/g, M: mixing ratio; P0: sea surface pressure
Pr(1)/Pr(2)=C(1)C(2)-1exp(-2 (O(1)-O(2))MOPO/g). (3) power ratio of two frequency channels at the O2-band
Similar LW & WV absorption (50~56GHz)
Almost the same in footprint & reflectivity
P0 C0(1, 2) + C1(1, 2) loge(Pr(1)Pr-1(2)) (4)
A very simple near-linear relationship between surface air pressure and radar
power ratio of two different frequencies (or differential absorption index) is expected from the O2 band radar data.
Theoretical basis
Radar simulated results
Most of the variability is due to global atmospheric profile variations: temperature, water vapor, clouds, etc.
PoC Instrument Development
Agilent8362BPNA
50-56 GHz Transceiver
15 GHx PLOX 5 = 45GHz
Port 1
Port 2
10 MHz Ref
5-11 GHz IF
5-11 GHz IF 50-56 GHz
TransmitAntenna
ReceiveAntenna
5-11 GHz IF
5-11 GHz IF
15 GHz PLO
50-56 GHz
Agilent8362BPNA
50-56 GHz Transceiver
15 GHx PLOX 5 = 45GHz
Port 1
Port 2
10 MHz Ref
5-11 GHz IF
5-11 GHz IF 50-56 GHz
TransmitAntenna
ReceiveAntenna
5-11 GHz IF
5-11 GHz IF
15 GHz PLO
50-56 GHz
Agilent 8362BNetwork Analyzer
SpaceK Labs 45GHz Up/Down
Converter
Quinstar 24"Cassegrain Antennas
Ground tests
Radar Installed in/on Mobile Radar Lab
relatively isolated radar reflector
• nearly spherical reflector• ~300m clear range
ProjectedBeamwidth
Varina-Enon BridgeI-295 South of Richmond, VA
Approx. 150’ above James River
Ground tests
Measure Water NRCS Over Wide Inc. Ang.Support Satellite Design
Supported by VDOT
PATAUXENT RIVER NAVAL AIR STATION
Flight tests
Observed and simulated Differential absorption
LEO SatelliteInstrument
• COTS & Lab Equip.• Demo Concept
• Operational Design• Op. Perf. Assessment• Technology Readiness
Level from 3 to 7
• GlobalMeasurements
15 ~ 22 km
0 – 3 km >220 kmAirborne
Instrument
Proof-of-ConceptInstrument
Technology Roadmap
Sea level pressure (SLP) assimilation (WRF)
“Simulated satellite SLP” using surface pressure measurements during first landing of Katrina
Model configuration
Advanced Research WRF (ARW) dynamic solver
CCM3 Radiation
Thompson cloud microphysics and Kain-Fristch convective parameterization
Mellor-Yamada PBL
36 and 12 km horizontal resolution and 28 layers, 261×181 grid mesh
84 -hour simulation
276 278 280 28224
25
26
27
28
29
30
276 278 280 28224
26
28
30
Case Assimilation Pattern Scale Length Factor
CTL No
Ga Area 0.25-1.00
Gl Lowest Pressure 0.25-1.00
Gc Area without lowest pressure 0.25-1.00
Gb A 2 degree band 0.25-1.00
Sea level pressure (SLP) assimilation (WRF)
e
f
987 993 999 1005 1011 1018 1024
276 278 280 28224
25
26
27
28
29
30
987 993 999 1005 1011 1018 1024
276 278 280 28224
25
26
27
28
29
30
987 993 999 1005 1011 1018 1024
276 278 280 28224
25
26
27
28
29
30
987 993 999 1005 1011 1018 1024
276 278 280 28224
25
26
27
28
29
30
987 993 999 1005 1011 1018 1024
276 278 280 28224
25
26
27
28
29
30
987 993 999 1005 1011 1018 1024
276 278 280 28224
25
26
27
28
29
30
OBS
NCEP-FNL
Gl_.25
Gl_1.0
Ga_.25
Ga_1.0
Sea-Level Pressure at 00 UTC August 26, 2005
Sea level pressure (SLP) assimilation (WRF)
CTL Gl(.25) Ga(1.0)
Ga(1.0)-CTLGl(.25)-CTL
•The assimilation runs symmetrically strengthen the cyclonic flow and enhances the westward and southward mean flow.
•Due to deepening of the hurricane vortex, the convective heating is enhanced
Initial column wind vector (m/s) in the experiments
Ga
Hurricane Katrina tracks
• Single point assimilations have large spread in track when different length scales are used
• All points assimilations have small spread in track and produce close track and landing position
Gl
Thick Black soild—best estimateBlack dashed—CTLSensitivity to scale length factorBlack –1; Red—0.75; Green—0.5 and Black—0.25
900
920
940
960
980
1000
26 27 28 29
Date
Min
SL
P (
hP
a)
Gl(.25)
Gb(.75)
Gc(1.0)
Ga(1.0)
best
12km
30
60
90
120
150
26 27 28 29
Date
Max
Win
d (
Kn
ots
)
Gl(.25)
Gb(.75)
Gc(1.0)
Ga(1.0)
best
12km
Hurricane Katrina Intensity (84-hour: Gl, Ga, Gc and Gb)
Without center pressure, Gc simulates comparable results as Ga, indicating the effect of pressure horizontal distribution in assimilation.
Exp(36km)
Distance (km)
Minimum Pressure (hPa)
Maximum Wind (Knot)
CTL 360 24 49
Ga 71 7 26
Gl 120 11 28
Gb 38 6 28
Gc 66 9 27
Summary
The differential O2 absorption pressure radar will provide the first remote sensing barometric data! The accuracy of instantaneous surface air pressure measurements could be ~4mb. (grid averages: errors ~1mb)
Lab, ground, and flight tests of current prototype instrument indicate that it works
Next generation radar: operational capability This effort will lead significant improvements in predictions of
hurricane intensities and tracks.
This differential O2 absorption radar technique may dramatically extend the current, limited-point barometric capability over oceans with airborne and spaceborne instruments.