Spatially Variable Advection Correction of Doppler Radial Velocity Data

Author:

Shapiro Alan12,Gebauer Joshua G.1,Dahl Nathan A.34,Bodine David J.5,Mahre Andrew15,Potvin Corey K.61

Affiliation:

1. a School of Meteorology, University of Oklahoma, Norman, Oklahoma

2. b Center for Analysis and Prediction of Storms, University of Oklahoma, Norman, Oklahoma

3. c Cooperative Institute for Mesoscale Meteorological Studies, University of Oklahoma, Norman, Oklahoma

4. d NOAA/NWS/Storm Prediction Center, University of Oklahoma, Norman, Oklahoma

5. e Advanced Radar Research Center, University of Oklahoma, Norman, Oklahoma

6. f NOAA/National Severe Storms Laboratory, University of Oklahoma, Norman, Oklahoma

Abstract

AbstractTechniques to mitigate analysis errors arising from the nonsimultaneity of data collections typically use advection-correction procedures based on the hypothesis (frozen turbulence) that the analyzed field can be represented as a pattern of unchanging form in horizontal translation. It is more difficult to advection correct the radial velocity than the reflectivity because even if the vector velocity field satisfies this hypothesis, its radial component does not—but that component does satisfy a second-derivative condition. We treat the advection correction of the radial velocity (υr) as a variational problem in which errors in that second-derivative condition are minimized subject to smoothness constraints on spatially variable pattern-translation components (U, V). The Euler–Lagrange equations are derived, and an iterative trajectory-based solution is developed in which U, V, and υr are analyzed together. The analysis code is first verified using analytical data, and then tested using Atmospheric Imaging Radar (AIR) data from a band of heavy rainfall on 4 September 2018 near El Reno, Oklahoma, and a decaying tornado on 27 May 2015 near Canadian, Texas. In both cases, the analyzed υr field has smaller root-mean-square errors and larger correlation coefficients than in analyses based on persistence, linear time interpolation, or advection correction using constant U and V. As some experimentation is needed to obtain appropriate parameter values, the procedure is more suitable for non-real-time applications than use in an operational setting. In particular, the degree of spatial variability in U and V, and the associated errors in the analyzed υr field are strongly dependent on a smoothness parameter.

Publisher

American Meteorological Society

Subject

Atmospheric Science

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