Doppler radar spectral width broadening due to beamwidth and wind shear

The spectral width observed by Doppler radars can be due to several effects including the atmospheric turbulence within the radar sample volume plus effects associated with the background flow and the radar geometry and configuration. This study re-examines simple models for the effects due to finite beam-width and vertical shear of the horizontal wind. Analytic solutions of 1- and 2-dimensional models are presented. Comparisons of the simple 2-dimensional model with numerical integrations of a 3-dimensional model with a symmetrical Gaussian beam show that the 2-dimensional model is usually adequate. The solution of the 2-dimensional model gives a formula that can be applied easily to large data sets. Analysis of the analytic solutions of the 2-dimensional model for off-vertical beams reveals a term that has not been included in mathematical formulas for spectral broadening in the past. This term arises from the simultaneous effects of the changing geometry due to curvature within a finite beamwidth and the vertical wind shear. The magnitude of this effect can be comparable to that of the well-known effects of beam-broadening and wind shear, and since it can have either algebraic sign, it can significantly reduce (or increase) the expected spectral broadening, although under typical conditions it is smaller than the beam-broadening effect. The predictions of this simple model are found to be consistent with observations from the VHP radar at White Sands Missile Range, NM.

[1]  W. Hocking Observation and measurement of turbulence m the middle atmosphere with a VHF radar , 1986 .

[2]  W. Hocking,et al.  An assessment of the effect of gravity waves on the width of radar Doppler spectra , 1994 .

[3]  Stephen A. Cohn,et al.  Radar Measurements of Turbulent Eddy Dissipation Rate in the Troposphere: A Comparison of Techniques , 1995 .

[4]  G. D. Nastrom,et al.  Variations of Winds and Turbulence Seen by the 50-MHz Radar at White Sands Missile Range, New Mexico , 1995 .

[5]  R. C. Srivastava,et al.  Wind Shear and Reflectivity Gradient Effects on Doppler Radar Spectra: II. , 1969 .

[6]  G. D. Nastrom,et al.  The Coupling of Gravity Waves and Turbulence at White Sands, New Mexico, from VHF Radar Observations , 1993 .

[7]  M. Yamamoto,et al.  Seasonal variability of vertical eddy diffusivity in the middle atmosphere: 1. Three‐year observations by the middle and upper atmosphere radar , 1994 .

[8]  P. W. Sloss,et al.  Wind Shear and Reflectivity Gradient Effects on Doppler Radar Spectra , 1968 .

[9]  W. Hocking Mesospheric turbulence intensities measured with a HF radar at 35°S - II , 1983 .

[10]  W. Hocking Two years of continuous measurements of turbulence parameters in the upper mesosphere and lower thermosphere made with a 2‐MHz radar , 1988 .

[11]  Wayne K. Hocking,et al.  Measurement of turbulent energy dissipation rates in the middle atmosphere by radar techniques: A review , 1985 .

[12]  Earl E. Gossard Radar Research on the Atmospheric Boundary Layer , 1990 .

[13]  D. Zrnic,et al.  Doppler Radar and Weather Observations , 1984 .

[14]  G. D. Nastrom,et al.  Turbulence eddy dissipation rates from radar observations at 5-20 km at White Sands Missile Range, New mexico , 1997 .

[15]  T. Tsuda,et al.  A systematic error in MST/ST radar wind measurement induced by a finite range volume effect: 2. Numerical considerations , 1988 .

[16]  Wayne K. Hocking,et al.  On the extraction of atmospheric turbulence parameters from radar backscatter Doppler spectra—I. Theory , 1983 .

[17]  Earl E. Gossard,et al.  Radar observation of clear air and clouds , 1983 .

[18]  R. Doviak,et al.  Meteorological radar signal intensity estimation , 1973 .

[19]  D. Atlas Advances in Radar Meteorology , 1964 .

[20]  Susumu Kato,et al.  A systematic error in MST/ST radar wind measurement induced by a finite range volume effect: 1. Observational results , 1988 .