multi-frequency radar/passive microwave observations and … · 2016-11-02 · apr-3 land/ocean...

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Multi-Frequency Radar/Passive Microwave Observations and Simulations of Cold Season Precipitation from GPM and OLYMPEX F. Joseph (Joe) Turk 1 [email protected] S. Tanelli 1 , S. Durden 1 , O. Sy 1 , G. Liu 2 , A. Battaglia 3 1) Jet Propulsion Laboratory, California Institute of Technology 2) Florida State University, Tallahassee, FL 3) Univ. of Leicester, UK Summary There has been considerable recent activity towards improving the understanding of scattering properties of frozen precipitation at mm-wave frequencies, associated computational methods, scattering/emission tables, and multi-frequency (three frequencies or more) radar measurement concepts. However, there are limited real-world observations to test and evaluate their use for space-based precipitation measurements and techniques. Two datasets have been prepared for these and other studies, such as future space-based cloud process studies, such as the Cloud and Precipitation Processes concept (CAPPM): https://pmm.nasa.gov/cappm. Contact J. Turk (email above) for more information and availability. Dataset Name Satellite Description Date Available 2A.GPM.DPR GPM DPR Ku and Ka-band radar reflectivity profile and radar-based precipitation retrievals, Version 04A 2014/03/08-current 1B.GPM.GMI GPM GMI Level 1B brightness temperatures, Version 04A 2014/03/05-current 2B-GEOPROF CloudSat CloudSat vertical reflectivity profile 2006/06/15-2016/07/31 Daylight-only operations since January 2012. ECMWF-AUX CloudSat ECMWF forecast analysis interpolated to each vertical CloudSat bin 2006/06/15-2016/07/31 1C.NOAA18.MHS NOAA-18 MHS Level 1C intercalibrated brightness temperatures 2006/06/15-2016/07/31 2C-SNOW-PROFILE CloudSat Snow water and snow rate profile at each vertical CloudSat bin 2006/06/15-2016/07/31 3x3 DPR profiles surrounding each GMI min-detectable cloud cloud DPR for Radiometer Scene Discrimination 4x4-km, 250-m vertical Z(Ku) < 15 dB and Z(Ka) < 15 dB and Z(Ka-HS) < 15 dB (all bins) è “no cloud” N bins where Z(Ku) > 20 dB as a proxy for increased level of cloudiness and precipitation N > 20 è “low probability” N > 50 è “medium probability” N > 100 è “high probability” 37-GHz resolution increased likelihood cloudiness increasing cloud levels Gulf of Mexico, ocean 17 June 2014 T vap = 36.9 T sfc = 301.2 DJF MAM JJA SON West Texas, bare soil 2 October 2014 T vap = 11.6 T sfc =304.7 DJF MAM JJA SON Search GPM database for nearby entries in leading PC-space: r = 1 N [(u obs u i sim )/σ i ] 2 N = 3 (latitude, longitude and date only used to plot points on the map) environmental state covariance emissivity covariance Minnesota, snow-cover 1 March 2015 T vap =1.8 T sfc = 259.1 DJF MAM JJA SON Estimating Non-Raining Surface Parameters to Assist GPM Constellation Radiometer-Based Precipitation Techniques F. Joseph (Joe) Turk 1 , Y. You 2 , Z. S. Haddad 1 1) Jet Propulsion Laboratory, California Institute of Technology 2) ESSIC/Univ. of Maryland-College Park, MD Summary One of the key challenges for GPM is how to link the information from the single DPR across all passive MW sensors in the constellation, to produce a globally consistent precipitation product. Currently, the surface and environmental conditions at the satellite observation time are interpolated from one or more global forecast models and a surface emissivity climatology, and used for radiative transfer simulations and cataloging/indexing the brightness temperature (TB) observations and simulations, within a common MW precipitation retrieval framework. Since the constellation MW radiometers routinely observe many more non-precipitating conditions than precipitating, here the information content within the non-precipitating GMI observations is studied as a means to characterize the emissivity state and to dynamically track the associated environmental conditions, regardless of underlying surface type. While not a cloud radar, the three DPR radars are used to separate “no-cloud” scenes from “low”, “medium” and “high” probability of cloudiness (not necessarily rain). Extension to SSMIS: Heritage 7- channel (no 10 GHz) radiometers such as SSMI and SSMIS do not have the same level of separation as a 9-channel (GMI); the raining and non-raining radiometer scenes will have more “overlap”. Cloud/No-Cloud Separation N(Ku) > 20 dB in column N>0 N>20 N>50 N>100 As more DPR cloud bins are present within the GMI radiometer scene, the PC structure shifts from the ”no-cloud” range (PC6-7 shown at right). As the cloud level further increases, the a-priori database search moves towards PC domains where more precipitating profiles are present. 37H vs 10H 89H vs 37H T vap vs T sfc Self-similar land locations and seasons appear, no ocean/coast areas Western US Southern Spain, southern Africa environmental state covariance emissivity covariance 37H vs 10H 89H vs 37H T vap vs T sfc Self-similar snow- cover locations and hemisphere seasons appear N Zealand south island (SH winter) Andes (SH winter) Alps (NH winter) Atlas Mtns (NH winter) environmental state covariance emissivity covariance 37H vs 10H 89H vs 37H T vap vs T sfc Airborne: OLYMPEx APR-3 + COSMIR + MASC + AMPR + MERRA2 During the Nov-Dec 2015 OLYMPEx campaign, there were fifteen flight dates where the NASA DC-8 collected simultaneous Ku/Ka/W-band APR-3 radar profiles (W-band unavailable 11/14 and 12/8), sounding radiometer observations from the Conically Scanning Millimeter-wave Imaging Radiometer (COSMIR) and the Microwave Atmosphere Sounder on Cubesat (MASC). On many dates, coincident Advanced Microwave Precipitation Radiometer (AMPR) data are available from coordinated ER-2 overpasses. MERRA2 atmosphere and surface reanalysis data was interpolated to each APR3 beam location to provide environmental context. Rachel Kroodsma (GSFC), Sharmila Padmanabhan (JPL) and Tim Lang (MSFC) are acknowledged for COSMIR, MASC and AMPR data, respectively. APR-3 Land/Ocean Ku/Ka 0 All Flights DPR Land/Ocean Ku/Ka 0 Nov-Dec 2015 OLYMPEx Region (no clouds) Box-and-whiskers plots of the APR-3 and corresponding GPM-DPR Ku/Ka- band surface backscattering cross section 0 under no-cloud scenes. All DPR overpasses in Nov-Dec 2015 covering the 46.9-48.5N 125.2-122.7W domain (1.5 x 2.5 degree) were used for comparison. The Ku/Ka radars agree within 1-3 dB, without accounting for any resolution differences, or offset time coincidence effects. The method relies upon a nonlinear transformation of TB into emissivity principal component (PC) space, to probabilistically separate “no-cloud” and increasingly cloudy scenes (Turk et. al., JTech, 2016). Transforming each TB observation into PC space, the GPM radiometer a-priori databases are searched globally (indexed into non-equal spaced bins according to the histogram of each PC, for computational efficiency) and inversely weighted in PC distance. The method appears to identify “self-similar” surface locations from the TB observations, without requiring any knowledge of geographical location, surface or environmental/temperature conditions. As the precipitation develops, the PC structure shifts from its “no-cloud” state, shifting and widening the database search region, from which the PDF of rain is obtained and the probability of precipitation. F-17 SSMIS GMI Relative operating characteristic (ROC) curve moves closer to upper left hand corner than for SSMIS Both the December 1 and 3 DC-8 flight lines were focused on flying up/down the Quinault river basin and that was covered by the NPOL and D3R radars. On December 1, moderately heavy stratiform rain was produced by a baroclinic system, where the structure was modified by the high elevation terrain and gradual change in the freezing level. On December 3, more convective cloud systems were overflown, with evidence in both the 166 and 183±7 channels on COSMIR and MASC. 3 December 2015 1 December 2015 Satellite: GPM-DPR/GMI + CloudSat + MHS + ECMWF + (Products) ±15-minute time coincidences between GPM and CloudSat (NOAA-19 MHS when it meets this threshold) are assembled with the data products listed in the table below. The current dataset spans the period between 8 March 2014 and 31 July 2016. A total of 7102 orbit coincidences occurred within this time span, but since CloudSat only operates on the daytime orbit, this cuts that number by approximately one-half. The next version will include CloudSat snow and rain profile products, and various DPR rain, sigma0 and PIA products, as requested by PMM and CloudSat investigators. Coincidence files are in HDF5 (< 40GB entire dataset), with quick-look graphics. Acknowledgments to Erich Stocker (PPS) for hosting as a GPM product and Phil Partain (CSU) for timely CloudSat data processing. https://storm.pps.eosdis.nasa.gov/storm (Search for 2BCSATGPM) 17 Jan 2016 1201 UTC Coast of Norway DPR swaths CloudSat snow CloudSat under GMI swath freezing level freezing level (AMPR only during DC8- ER2 coordination) (AMPR only during DC8- ER2 coordination) Self-similar areas of ocean or inland water SST and vapor appear, no land Copyright 2016 California Institute of Technology. U.S. government sponsorship acknowledged. This work was carried out at the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration. Support from the NASA under the Precipitation Measuring Missions (PMM) program is gratefully acknowledged.

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Page 1: Multi-Frequency Radar/Passive Microwave Observations and … · 2016-11-02 · APR-3 Land/Ocean Ku/Ka!0 All Flights DPR Land/Ocean Ku/Ka!0 Nov-Dec 2015 OLYMPEx Region (no clouds)

Multi-Frequency Radar/Passive Microwave Observations and Simulations of Cold Season Precipitation from GPM and OLYMPEX

F. Joseph (Joe) Turk1 [email protected]. Tanelli1, S. Durden1, O. Sy1, G. Liu2, A. Battaglia3

1) Jet Propulsion Laboratory, California Institute of Technology2) Florida State University, Tallahassee, FL

3) Univ. of Leicester, UKSummaryThere has been considerable recent activity towards improving theunderstanding of scattering properties of frozen precipitation at mm-wavefrequencies, associated computational methods, scattering/emission tables,and multi-frequency (three frequencies or more) radar measurementconcepts. However, there are limited real-world observations to test andevaluate their use for space-based precipitation measurements andtechniques. Two datasets have been prepared for these and other studies,such as future space-based cloud process studies, such as the Cloud andPrecipitation Processes concept (CAPPM): https://pmm.nasa.gov/cappm.Contact J. Turk (email above) for more information and availability.

Dataset Name Satellite Description Date Available

2A.GPM.DPR GPMDPR Ku and Ka-band radar reflectivity profile and radar-based precipitation

retrievals, Version 04A2014/03/08-current

1B.GPM.GMI GPM GMI Level 1B brightness temperatures, Version 04A 2014/03/05-current

2B-GEOPROF CloudSat CloudSat vertical reflectivity profile2006/06/15-2016/07/31

Daylight-only operations since January 2012.

ECMWF-AUX CloudSat ECMWF forecast analysis interpolated to each vertical CloudSat bin 2006/06/15-2016/07/31

1C.NOAA18.MHS NOAA-18 MHS Level 1C intercalibratedbrightness temperatures

2006/06/15-2016/07/31

2C-SNOW-PROFILE CloudSat Snow water and snow rate profile at each vertical CloudSat bin 2006/06/15-2016/07/31

3x3 DPR profiles surrounding each

GMI

min-detectable cloud

cloud

DPR for Radiometer Scene Discrimination

4x4-km, 250-m vertical

Z(Ku) < 15 dB andZ(Ka) < 15 dB andZ(Ka-HS) < 15 dB

(all bins) è “no cloud”

N bins where Z(Ku) > 20 dB as a proxy for increased level of cloudiness and precipitation

N > 20 è “low probability”N > 50 è “medium probability”

N > 100 è “high probability”

37-GHz resolution

increased likelihood cloudiness increasing

cloud levels

Gulf of Mexico, ocean17 June 2014

Tvap= 36.9 Tsfc= 301.2

DJF MAMJJA SON

West Texas, bare soil2 October 2014

Tvap= 11.6 Tsfc=304.7

DJF MAMJJA SON

Search GPM database for nearby entries in leading PC-space:

!!r = 1

N[(uobs∑ −ui

sim)/σ i ]2 N =3(latitude, longitude and date only used to plot points on the map)

environmental state covariance

emissivity covariance

Minnesota, snow-cover1 March 2015

Tvap=1.8 Tsfc= 259.1

DJF MAMJJA SON

Estimating Non-Raining Surface Parameters to Assist GPM Constellation Radiometer-Based Precipitation Techniques

F. Joseph (Joe) Turk1, Y. You2, Z. S. Haddad1

1) Jet Propulsion Laboratory, California Institute of Technology2) ESSIC/Univ. of Maryland-College Park, MD

SummaryOne of the key challenges for GPM is how to link theinformation from the single DPR across all passive MWsensors in the constellation, to produce a globallyconsistent precipitation product. Currently, the surfaceand environmental conditions at the satellite observationtime are interpolated from one or more global forecastmodels and a surface emissivity climatology, and used forradiative transfer simulations and cataloging/indexing thebrightness temperature (TB) observations andsimulations, within a common MW precipitation retrievalframework. Since the constellation MW radiometersroutinely observe many more non-precipitating conditionsthan precipitating, here the information content within thenon-precipitating GMI observations is studied as a meansto characterize the emissivity state and to dynamicallytrack the associated environmental conditions, regardlessof underlying surface type.

While not a cloud radar, the three DPR radars are used toseparate “no-cloud” scenes from “low”, “medium” and “high”probability of cloudiness (not necessarily rain).

Extension to SSMIS: Heritage 7-channel (no 10 GHz) radiometerssuch as SSMI and SSMIS do nothave the same level of separationas a 9-channel (GMI); the rainingand non-raining radiometerscenes will have more “overlap”.

Cloud/No-Cloud Separation N(Ku) > 20 dB in columnN>0 N>20 N>50 N>100

As more DPR cloud bins arepresent within the GMI radiometerscene, the PC structure shifts fromthe ”no-cloud” range (PC6-7shown at right). As the cloud levelfurther increases, the a-prioridatabase search moves towardsPC domains where moreprecipitating profiles are present.

37H vs 10H 89H vs 37H

Tvap vs Tsfc

Self-similar land locations and

seasons appear, no ocean/coast

areas

Western US

Southern Spain, southern Africa

environmental state covariance emissivity covariance

37H vs 10H 89H vs 37H

Tvap vs Tsfc

Self-similar snow-cover locations and hemisphere seasons appear

N Zealand south island (SH winter)

Andes(SH winter)

Alps(NH winter)

Atlas Mtns(NH winter)

environmental state covariance emissivity covariance

37H vs 10H 89H vs 37HTvap vs Tsfc

Airborne: OLYMPEx APR-3 + COSMIR + MASC + AMPR + MERRA2During the Nov-Dec 2015 OLYMPEx campaign, there were fifteen flightdates where the NASA DC-8 collected simultaneous Ku/Ka/W-band APR-3radar profiles (W-band unavailable 11/14 and 12/8), sounding radiometerobservations from the Conically Scanning Millimeter-wave ImagingRadiometer (COSMIR) and the Microwave Atmosphere Sounder on Cubesat(MASC). On many dates, coincident Advanced Microwave PrecipitationRadiometer (AMPR) data are available from coordinated ER-2 overpasses.MERRA2 atmosphere and surface reanalysis data was interpolated to eachAPR3 beam location to provide environmental context.

Rachel Kroodsma (GSFC), Sharmila Padmanabhan (JPL) and TimLang (MSFC) are acknowledged for COSMIR, MASC and AMPR data,respectively.

APR-3 Land/Ocean Ku/Ka 𝞼0

All FlightsDPR Land/Ocean Ku/Ka 𝞼0

Nov-Dec 2015 OLYMPEx Region

(no clouds)

Box-and-whiskers plots of the APR-3 and corresponding GPM-DPR Ku/Ka-band surface backscattering cross section 𝞼0 under no-cloud scenes. AllDPR overpasses in Nov-Dec 2015 covering the 46.9-48.5N 125.2-122.7Wdomain (1.5 x 2.5 degree) were used for comparison. The Ku/Ka radarsagree within 1-3 dB, without accounting for any resolution differences, oroffset time coincidence effects.

The method relies upon a nonlinear transformation of TB intoemissivity principal component (PC) space, to probabilisticallyseparate “no-cloud” and increasingly cloudy scenes (Turk et.al., JTech, 2016). Transforming each TB observation into PCspace, the GPM radiometer a-priori databases are searchedglobally (indexed into non-equal spaced bins according to thehistogram of each PC, for computational efficiency) andinversely weighted in PC distance. The method appears toidentify “self-similar” surface locations from the TBobservations, without requiring any knowledge ofgeographical location, surface or environmental/temperatureconditions. As the precipitation develops, the PC structureshifts from its “no-cloud” state, shifting and widening thedatabase search region, from which the PDF of rain isobtained and the probability of precipitation.

F-17SSMIS GMI

Relative operating characteristic (ROC) curve moves closer to upper left hand corner than for SSMIS

Both the December 1 and 3 DC-8 flight lines were focused on flyingup/down the Quinault river basin and that was covered by the NPOL andD3R radars. On December 1, moderately heavy stratiform rain wasproduced by a baroclinic system, where the structure was modified bythe high elevation terrain and gradual change in the freezing level. OnDecember 3, more convective cloud systems were overflown, withevidence in both the 166 and 183±7 channels on COSMIR and MASC.

3 December 20151 December 2015

Satellite: GPM-DPR/GMI + CloudSat + MHS + ECMWF + (Products)±15-minute time coincidences between GPM and CloudSat (NOAA-19MHS when it meets this threshold) are assembled with the data productslisted in the table below. The current dataset spans the period between 8March 2014 and 31 July 2016. A total of 7102 orbit coincidences occurredwithin this time span, but since CloudSat only operates on the daytimeorbit, this cuts that number by approximately one-half. The next version willinclude CloudSat snow and rain profile products, and various DPR rain,sigma0 and PIA products, as requested by PMM and CloudSatinvestigators. Coincidence files are in HDF5 (< 40GB entire dataset), withquick-look graphics. Acknowledgments to Erich Stocker (PPS) for hostingas a GPM product and Phil Partain (CSU) for timely CloudSat dataprocessing.

https://storm.pps.eosdis.nasa.gov/storm (Search for 2BCSATGPM) 17 Jan 2016 1201 UTCCoast of Norway

DPR swaths

CloudSat

snow

CloudSat under GMI swath

freezing levelfreezing level

(AMPR only during DC8-

ER2 coordination)

(AMPR only during DC8-

ER2 coordination)

Self-similar areas of ocean or inland water SST and vapor appear, no land

Copyright 2016 California Institute of Technology. U.S. government sponsorship acknowledged. This work was carried out at the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration. Support from the NASA under

the Precipitation Measuring Missions (PMM) program is gratefully acknowledged.