On Turbulence Measurements with Phased Array Radar

Isotropic and homogeneous turbulence can be characterized via the eddy dissipation rate ε and a correlation scale length, Λ. Weather radars have been used to estimate ε (assuming a fixed length scale) in precipitation from the Doppler spectrum width, which is a measure of the spread of radial velocities within the radar resolution volume. Pointed herein are differences between turbulence measurements by conventional pencil bean antenna and electronically steering phased array radar (PAR) antennas. Differences are caused by the shape and orientation of the beam cross section on phased array antenna because these depend on the pointing direction. A formalism applicable to pencil beams of circular cross section is extended to elliptic beam cross sections. For lateral dimensions of the radar resolution volume larger than its range extent an approximate formula is suggested for computing ε. Eddy dissipation rate computed along a radial pointing at a 40° of an all-digital PAR is presented.

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Publication Details

Published
2024-10-15
DOI
https://doi.org/10.1109/array58370.2024.10880344
Citations
1
Primary Topic
Radio Wave Propagation Studies
Type
article
Field-Weighted Citation Impact
1.30

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article

On Turbulence Measurements with Phased Array Radar

David Schvartzman, Larry Cornman, Dúsan S. Zrnić, Djordje Mirković
1 citations
Radio Wave Propagation Studies
1.30
article

On Turbulence Measurements with Phased Array Radar

David Schvartzman, Larry Cornman, Dúsan S. Zrnić, Djordje Mirković
article en
1 citations

Abstract

Isotropic and homogeneous turbulence can be characterized via the eddy dissipation rate ε and a correlation scale length, Λ. Weather radars have been used to estimate ε (assuming a fixed length scale) in precipitation from the Doppler spectrum width, which is a measure of the spread of radial velocities within the radar resolution volume. Pointed herein are differences between turbulence measurements by conventional pencil bean antenna and electronically steering phased array radar (PAR) antennas. Differences are caused by the shape and orientation of the beam cross section on phased array antenna because these depend on the pointing direction. A formalism applicable to pencil beams of circular cross section is extended to elliptic beam cross sections. For lateral dimensions of the radar resolution volume larger than its range extent an approximate formula is suggested for computing ε. Eddy dissipation rate computed along a radial pointing at a 40° of an all-digital PAR is presented.

NSF National Center for Atmospheric Research (US), NOAA National Severe Storms Laboratory (US), Radar (United States) (US), University of Oklahoma (US)
U.S. Department of Commerce
Affordable and clean energy
Openalex Percentile: Top 11%
Radio Wave Propagation Studies
1.30
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On Turbulence Measurements with Phased Array Radar — David Schvartzman, Larry Cornman, et al. · (2024) | TGRS Research Map | TGRS