Evolution of a three body scattering signature: 26 May 2010: Difference between revisions

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==Overview==
[[Image:26may2010 3 body anot.png|250px|right]]
[[Image:26may2010 3 body anot.png|250px|right]]
Three body scattering patterns were observed in association with a severe hailstorm on 26 May 2010.  Plots of the time evolution of the three body scattering patterns are shown.
Three body scattering patterns were observed in association with a severe hailstorm on 26 May 2010.  Plots of the time evolution of the three body scattering patterns are shown.


==Introduction==
==Introduction==
Echoes due to three body scattering are typically seen down-range of thunderstorms that contain high reflectivity regions located at heights of several km above the ground. When these high reflectivity areas are illuminated by the radar pulse, they re-radiate a scattered component of the incident energy in all directions. Some of this scattered energy is reflected off of the underlying ground surface, producing a re-illumination of particles in the pulse volume. A portion of this re-scattered energy is directed back towards the radar where it may result in a detectable echo. The lengthened path travelled by these signals (radar -> hydrometeors -> ground -> back to hydrometeors -> back to the radar) causes them to appear as down-range extensions of the generating thunderstorm echo. The presence of hailstones aloft with significant diameters and concentrations can cause the appearance of the three body signature.  During CSU-CHILL operations on 26 May 2010, an intensifying hailstorm was observed to develop an increasingly well defined three body signature.
Echoes due to three body scattering are typically seen down-range of thunderstorms that contain high reflectivity regions located at heights of several kilometers above the ground. When these high reflectivity areas are illuminated by the radar pulse, they re-radiate a scattered component of the incident energy in all directions. Some of this scattered energy is reflected off of the underlying ground surface, producing a re-illumination of particles in the pulse volume. A portion of this re-scattered energy is directed back towards the radar where it may result in a detectable echo. The lengthened path travelled by these signals (radar -> hydrometeors -> ground -> back to hydrometeors -> back to the radar) causes them to appear as down-range extensions of the generating thunderstorm echo.
 
[[Image:Three-body-scattering.png|300px|center]]
 
The presence of hailstones aloft with significant diameters and concentrations can cause the appearance of the three body signature.  During CSU-CHILL operations on 26 May 2010, an intensifying hailstorm was observed to develop an increasingly well defined three body signature.


==RHI Data==
==RHI Data==
The following sequence of RHI scans were all collected on an azimuth of
The following sequence of RHI scans were all collected on an azimuth of 191 degrees.  In each image frame the upper panel is reflectivity and the lower panel is differential reflectivity.  The development and descent of the intense reflectivity area is apparent.  In the differential reflectivity data, a region of anomalously positive <math>Z_{dr}</math> values develops in the three body scattering region down range of the storm. This is one of the differential reflectivity characteristics of three body echoes that were reported in Hubbert and Bringi (J. Atmos. Oceanic Tech., January, 2000, 51-61).
191 degrees.  In each image frame the upper panel is reflectivity and the
 
lower panel is differential reflectivity.  The development and descent of
the intense reflectivity area is apparent.  In the differential
reflectivity data, a region of anomalously positive Zdr values develops in
the three body scattering region down range of the storm. This is one of
the differential reflectivity characteristics of three body echoes that
were reported in Hubbert and Bringi (J. Atmos. Oceanic Tech., January, 2000, 51-61).
<center>
<center>
<imgloop delay=400 imgprefix="http://www.chill.colostate.edu/anim/26may2010_three_body/" width=308 height=608>
<imgloop delay=400 imgprefix="http://www.chill.colostate.edu/anim/26may2010_three_body/" width=308 height=608>
26may2010_1918_RHI.png
26may2010_1918_RHI.png|1918 UTC
26may2010_1924_RHI.png
26may2010_1924_RHI.png|1924 UTC
26may2010_1930_RHI.png
26may2010_1930_RHI.png|1930 UTC
26may2010_1932_RHI.png
26may2010_1932_RHI.png|1932 UTC
</imgloop>
</imgloop>
</center>
</center>
<hr>
 
The next plot includes the radial velocity field observed in the final RHI
The next plot includes the radial velocity field observed in the final RHI of the above time lapse sequence.  The spatial variability of the radial velocities is relatively smooth in the thunderstorm echo; the velocity
of the above time lapse sequence.  The spatial variability of the radial
variability is visibly greater in the three body region.  Due to the large fall velocity of the hailstones, the radial velocities in the three body echo are also predominately negative (Wilson and Reum, J. Atmos. Oceanic Tech., April 1988, 197-205).
velocities is relatively smooth in the thunderstorm echo; the velocity
 
variability is visibly greater in the three body region.  Due to the large
fall velocity of the hailstones, the radial velocities in the three body
echo are also predominately negative (Wilson and Reum, J. Atmos. Oceanic Tech., April 1988, 197-205).
<center>
<center>
[[Image:26may2010 3 body VT anot.png]]
[[Image:26may2010 3 body VT anot.png]]
</center>
</center>
<hr>
 
==PPI Data==
==PPI Data==
A short loop of 0.5 degree elevation PPI scans that bracket the RHI image
A short loop of 0.5 degree elevation PPI scans that bracket the RHI image loop period is shown below.  In these images, the upper panel is reflectivity and the lower panel is linear depolarization ratio (LDR). As
loop period is shown below.  In these images, the upper panel is
hail becomes an increasingly large component of the precipitation, the reflectivity levels approach 70 dBZ and the LDR values increase to ~ -15 dB. The final PPI image time is 1932:37 UTC. The SPC severe weather report records contain an observation of damage-producing 2 inch diameter hail from this storm in Commerce City at 1933 UTC.
reflectivity and the lower panel is linear depolarization ratio (Ldr). As
 
hail becomes an increasingly large component of the precipitation, the
reflectivity levels approach 70 dBZ and the Ldr values increase to ~ -15
dB. The final PPI image time is 1932:37 UTC. The SPC severe weather
report records contain an observation of damage-producing 2 inch diameter
hail from this storm in Commerce City at 1933 UTC.
<center>
<center>
<imgloop delay=400 imgprefix="http://www.chill.colostate.edu/anim/26may2010_three_body/" width=300 height=600>
<imgloop delay=400 imgprefix="http://www.chill.colostate.edu/anim/26may2010_three_body/" width=300 height=600>
PPI_26may2010_1916.png
PPI_26may2010_1916.png|1916 UTC
PPI_26may2010_1920.png
PPI_26may2010_1920.png|1920 UTC
PPI_26may2010_1926.png
PPI_26may2010_1926.png|1926 UTC
PPI_26may2010_1933.png
PPI_26may2010_1933.png|1933 UTC
</imgloop>
</imgloop>
</center>
</center>
==References==
* J. C. Hubbert, and V. N. Bringi, 2000: [http://journals.ametsoc.org/doi/abs/10.1175/1520-0426(2000)017%3C0051:TEOTBS%3E2.0.CO;2 The Effects of Three-Body Scattering on Differential Reflectivity Signatures]. ''Journal of Atmospheric and Oceanic Technology''., '''17''', 1 (January 2000) pp 51-61.
* James W. Wilson, Darelyn Reum, 1988: [http://journals.ametsoc.org/doi/abs/10.1175/1520-0426%281988%29005%3C0197%3ATFERAV%3E2.0.CO%3B2 The Flare Echo: Reflectivity and Velocity Signature]. ''Journal of Atmospheric and Oceanic Technology''., '''5''', 2 (April 1988) pp 197-205.
* [http://en.wikipedia.org/wiki/Three_body_scatter_spike Three Body Scattering] on Wikipedia


[[Category:Featured Articles]]
[[Category:Featured Articles]]
[[Category:Three Body Scattering]]
[[Category:Three Body Scattering]]

Latest revision as of 15:41, 22 March 2011

Three body scattering patterns were observed in association with a severe hailstorm on 26 May 2010. Plots of the time evolution of the three body scattering patterns are shown.


Introduction

Echoes due to three body scattering are typically seen down-range of thunderstorms that contain high reflectivity regions located at heights of several kilometers above the ground. When these high reflectivity areas are illuminated by the radar pulse, they re-radiate a scattered component of the incident energy in all directions. Some of this scattered energy is reflected off of the underlying ground surface, producing a re-illumination of particles in the pulse volume. A portion of this re-scattered energy is directed back towards the radar where it may result in a detectable echo. The lengthened path travelled by these signals (radar -> hydrometeors -> ground -> back to hydrometeors -> back to the radar) causes them to appear as down-range extensions of the generating thunderstorm echo.

The presence of hailstones aloft with significant diameters and concentrations can cause the appearance of the three body signature. During CSU-CHILL operations on 26 May 2010, an intensifying hailstorm was observed to develop an increasingly well defined three body signature.

RHI Data

The following sequence of RHI scans were all collected on an azimuth of 191 degrees. In each image frame the upper panel is reflectivity and the lower panel is differential reflectivity. The development and descent of the intense reflectivity area is apparent. In the differential reflectivity data, a region of anomalously positive values develops in the three body scattering region down range of the storm. This is one of the differential reflectivity characteristics of three body echoes that were reported in Hubbert and Bringi (J. Atmos. Oceanic Tech., January, 2000, 51-61).


Click play to begin animation

Delay: ms

Linear
Rock

The next plot includes the radial velocity field observed in the final RHI of the above time lapse sequence. The spatial variability of the radial velocities is relatively smooth in the thunderstorm echo; the velocity variability is visibly greater in the three body region. Due to the large fall velocity of the hailstones, the radial velocities in the three body echo are also predominately negative (Wilson and Reum, J. Atmos. Oceanic Tech., April 1988, 197-205).

PPI Data

A short loop of 0.5 degree elevation PPI scans that bracket the RHI image loop period is shown below. In these images, the upper panel is reflectivity and the lower panel is linear depolarization ratio (LDR). As hail becomes an increasingly large component of the precipitation, the reflectivity levels approach 70 dBZ and the LDR values increase to ~ -15 dB. The final PPI image time is 1932:37 UTC. The SPC severe weather report records contain an observation of damage-producing 2 inch diameter hail from this storm in Commerce City at 1933 UTC.


Click play to begin animation

Delay: ms

Linear
Rock

References