Transcript
Page 1: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

AVAPS Flight Summary

HS3 2012

NOAA ESRL

Gary WickRyan SpackmanDarren Jackson

Dave Costa

NCAR

Terry HockDean LauritsenCharlie MartinXuanyong Xu

NOAA AOML

Michael BlackJason Dunion

Page 2: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

Dropsonde Observations

Flight Target Sondes Comments

5-6 Sep 2012 Leslie 30 Transit, Limited Ku

11-12 Sep Nadine 34 System fault -– parachute cap anomaly;RF noise issue emerges in flight

14-15 Sep Nadine 70 RFI continues

19-20 Sep Nadine 76 RFI continues

22-23 Sep Nadine 58 RFI continues

26-27 Sep Nadine 75 RFI improves

Total Sondes 343

Page 3: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

Dropsonde Observations

Page 4: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

Dropsonde Achievements

• First operations with Ku communications:

Download raw D-files from AV-6 in flight

Real-time ASPEN processing

Near real-time posting of skew-T plot to MTS

Near real-time transmission to GTS

Reference to HS3 sonde data in NHC forecast discussions for Nadine

• Plans for parallel GFS model runs• Dropsonde deployment flexibility in various Atlantic

FIRs (e.g., box module insertion in real time)

Page 5: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

AVAPS Lessons LearnedFlight Ops

1 – Two AVAPS team members required in the PMOF:

Dedicated drop operator necessary because of intensive comms

AVAPS science seat coordinates drop pattern and any changes with mission scientists and shuttles data to processing team

2 – Additional team required for real-time processing

Instrument Issues

1 - Parachute cap manufacturing anomaly being addressed

2 – RF noise interference issue is under investigation

Page 6: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

Science Directions• Tropical-extratropical transition: trough interactions• Aerosol-cloud-precipitation interactions: Role of SAL• HS3 science investigations: Build collaborations with

investigator teams that are using the dropsonde data

Courtesy of G. Wick, NOAA

Page 7: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

Sep 26 Nadine Mission

Dry, stable SAL

Dry, stable continental air

Moist core

How could Nadine survive and even flourish in such a dry, stable environment? Is the core within a “protected pouch”? How does convection overcome the stable low-level environment and inversion? Are differences in SST and surface air temperature important to enhance surface fluxes?

Courtesy of M. Black, NOAA

Page 8: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

NASA Global Hawk – HS3 2012

Page 9: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

• Dropsonde RF Signal Strength vs Time for First 6 dropsHS3 2012: Case 1 – Science Flight #1 (transit)

Normal AVAPS ‘no signal’ noise floor

Page 10: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

• Dropsonde RF Signal Strength vs Time for First 6 dropsHS3 2012: Case 2 – Science Flight #2

Why has the ‘no signal’ noise floor increased on Drops 2 through 6 (shown here) and all subsequent drops?

Drop 1, the ‘Bermuda’ drop

Page 11: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

HS3 2012: Case 1 – Science Flight #1 (transit)• Two AVAPS 400 MHz Spectrum Analyzer data frames prior to takeoff• Note average noise floor jump from ~ -110 dBm to ~ -102 dBm• These plots are 6 seconds apart in time

UTC Time - 20:16:00 UTC Time - 20:16:06

approx mean: -110 dBmapprox mean: -102 dBm

Page 12: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

HS3 2012: Case 1 – Science Flight #1 (transit)• GH IWG1 data

prior to takeoff

UTC Time of cursor20:16:06

(same UTC time as 2nd AVAPS Spectrum Analyzer plot)

GH Takeoff ^

GH Pressure Altitude

GH Aircraft Heading 20:16:06 Z ground taxi begins

Page 13: AVAPS F LIGHT S UMMARY HS3 2012 NOAA ESRL G ARY W ICK R YAN S PACKMAN D ARREN J ACKSON D AVE C OSTA NCAR T ERRY H OCK D EAN L AURITSEN C HARLIE M ARTIN

HS3 2012: Case 1 – Science Flight #1 (transit)• Zoomed-in detail of previous IWG1 aircraft data slide UTC Time = 20:16:06

GH Aircraft Heading 20:16:06 Z ground taxi begins


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