+ All Categories
Home > Documents > Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Date post: 13-Jan-2016
Category:
Upload: thomas-bennett
View: 215 times
Download: 3 times
Share this document with a friend
Popular Tags:
9
Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014
Transcript
Page 1: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Active Microwave Physics and Basics

1

Simon YuehJPL, Pasadena, CA

August 14, 2014

Page 2: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

How Deep Can the Radio Waves Penetrate• 10 to17 GHz microwave can penetrate dry

snowpack with a broad range of depth (1 to 5 m)

2

• Experiment, Radio Laboratory, Helsinki University of Technology in 1987• Theoretical simulations from bicontinuous medium/NMM3D, Xu et al, 2012

Frequency Penetration Depth

10 GHz (X) ~5 m14 GHz (Ku)

~1 m

18 GHz (K) ~0.5 m37 GHz (Ka)

~0.1 m

0.01m

0.1m

1m

10m

Page 3: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Radar Sounding of SnowSurface Scattering

• Surface scattering dominates at near nadir looking• Early demonstration by late Prof. Hal Boyne (CSU)

• Current Status – A well-developed tool for probing the snow stratigraphy– Marsahll et al., ground-based FMCW Radar – Gogineni et al., aircraft-based Snow Radar

Courtesy of Boyne

• What is the resolution?– ΔR=Range resolution=C/2B– ΔH=H(1/cosθ-1) for rough interface

• Beamwidth (2θ) and height (H)

– Horizontal resolution=2Hθ – limited by beamwidth ΔRΔH

B ΔR

1 GHz 15 cm

5 GHz 3 cm

H ΔH

1000 m, 10deg 3.8m

10 m, 5 deg 1 cm

Page 4: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Off-nadir Looking RadarVolume Scattering

SAR processing can achieve horizontal resolution of a few meters from space

Backscatter contributions:

Volume, surface, and interaction terms.

Observed backscatter coefficient σ° :

asgvvg '0

At off-nadir angles (30-50 degrees incidence angles)

Volume scattering starts to dominate

Surface scattering diminishes

Main parameters for snow backscatter:

Dry snow• Snow water equivalent • Grain size (d)• Density (ρ)• Soil background signal

Wet snow• Liquid water content (radar signal does not

penetrate)

Page 5: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

One example of data and theoryMore data acquired through CLPX2, SnowScat and SnowSAR campaigns

• Snow

50 60 70 80 90 100 110 120-20

-18

-16

-14

-12

-10

-8

-6

SWE (mm)

VV

(dB

)

SnowSCAT backscatter against SWE, 40, 16.7GHz

10.2GHz

13.3GHz16.7GHz

03/01/201112/28/2010

SnowSCAT backscatter time series σvv with 40∘ incidence angle against SWE. Data taken from at Sodankylä between 12/28 /2010 and 03/01/2011.

Simulated radar backscatter using the DMRT/QCA for snow volume scattering at three frequencies. All three frequencies show response to snow water equivalent for moderate and large grain size.

Page 6: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

SAR Snow TomographySide-looking radar with multiple baselines

• Snow stratigraphy - Metamorphism and environmental factors create complex layering structures in the snow pack

• SAR Tomography will provide insight into snow and ice – Lack of comprehensive theoretical

development and experimental testing for snow

• SAR Tomography – Tested for 3-D forest canopy mapping– Coherence and multiple baselines– Demosntrated by GB-SAR, K Morrison of Cranfield U.

Measurements at Reynolds Creek study site, 200 meters from tower - 116 manual probe depth measurements. (Marshall et al. of BSU)

Leln

r

dr

Hei

ght

(m)

Sla

nt

Ran

ge (

m)

Polarimetric tomographic profile over a forested area using DLR’s E-SAR system at L-band [Moreira et al., IEEE GRS magazine, 2013].

Page 7: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Recent campaigns covering main snow regimes

Churchill, Canada, Tundra

(Near-)Coincident Ku-band and X-band scatterometers and SAR used

Sodankylä, Finland, Taiga

Innsbruck, Austria, Alpine

Colorado, USA Alpine/Tundra/ Taiga/Prairie

Inuvik, Canada, Tundra

Kuparuk, Alaska, Tundra

Page 8: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Radar backscatter versus SWE – from Sodankylä, Finland, Taiga

Backscatter versus observed SWE, Sodankylä, Finland

, SnowScat measurements for winter I , for winter II

radiative transfer model calculation for 3 different values of grain size

SnowScat measurements at 40° for two winters

Page 9: Active Microwave Physics and Basics 1 Simon Yueh JPL, Pasadena, CA August 14, 2014.

Radar backscatter versus SWE – from Rocky Mountain, Colorado

Backscatter for VV, HH, and VH polarizations shows sensitivity to SWE for three sampling sites

Yueh et al., Airborne Ku-band Polarimetric Radar Remote Sensing of Terrestrial Snow Cover, IEEE TGRS, Vol. 47, No. 10, 3347-3364, 2009.

NASA/JPL POLSCAT measurements


Recommended