A brief climatology of eddy diffusivities over White Sands Missile Range, New Mexico

Observations of the Doppler spectral width made using the VHF profiler radar at White Sands Missile Range, New Mexico, are used to estimate the eddy diffusion coefficient Kz at 5–20 km on an hourly basis. The data used span the period 1991–1995. Medians of the hourly values of Kz range from ∼3 m2/s near 5km to about 0.3 m2/s near 14km. The logarithms of the individual hourly values are approximately normally distributed. Seasonal median values of log Kz are nearly the same at all heights during autumn through spring, while the summer values are about twice as large as the values for other seasons. Hourly values of log Kz are negatively correlated with the static stability, are positively correlated with the vertical shear of the horizontal wind, and show weak negative correlation with the Richardson number during all seasons. The correlation of log Kz with the horizontal wind speed is positive in the winter, indicating that the magnitude of Kz is determined by synoptic weather systems then, and negative in the summer, indicating that convective processes are most important in determining Kz in the summer. The autocorrelation of log Kz as a function of vertical separation decreases more slowly with increasing vertical separation in the troposphere than in the stratosphere. The median values of log Kz that we find compare very well with those of past studies near the tropopause level and above, but in the troposphere they are significantly larger than those reported from the middle and upper atmosphere radar in Japan; this difference is discussed in terms of differences in the local terrain and the climate of the troposphere.

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

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

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

[4]  S. Clifford,et al.  A Study of Convection Capped by a Stable Layer Using Doppler Radar and Acoustic Echo Sounders , 1974 .

[5]  M. F. Larsen,et al.  Observations of Low-Frequency Inertia-Gravity Waves in the Lower Stratosphere over Arecibo , 1989 .

[6]  Frank D. Eaton,et al.  Comparisons of VHF radar, optical, and temperature fluctuation measurements ofCn2,r0 andθ0 , 1988 .

[7]  I. S. Bowen The Ratio of Heat Losses by Conduction and by Evaporation from any Water Surface , 1926 .

[8]  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 .

[9]  D. Lilly,et al.  Stratospheric Mixing Estimated from High-Altitude Turbulence Measurements , 1974 .

[10]  Toru Sato,et al.  Fine Altitude Resolution Observations of Stratospheric Turbulent Layers by the Arecibo 430 MHz Radar , 1982 .

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

[12]  V. Schilling,et al.  Vertical mixing of passive scalars owing to breaking gravity waves , 1996 .

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

[14]  B. B. Balsley,et al.  Doppler Radar Probing of the Clear Atmosphere , 1978 .

[15]  T. Tsuda,et al.  Zenith-angle dependence of VHF specular reflection echoes in the lower atmosphere , 1997 .

[16]  R. Woodman,et al.  Evaluation of effective eddy diffusive coefficients using radar observations of turbulence in the stratosphere , 1984 .

[17]  D. Hunten,et al.  Stratospheric eddy diffusion coefficients from tracer data , 1981 .

[18]  J.R. Hines,et al.  The Us Army Atmospheric Profiler Research Facility: Description And Capabilities , 1992, [Proceedings] IGARSS '92 International Geoscience and Remote Sensing Symposium.

[19]  M. Novello,et al.  Geodesic motion and confinement in Gödel's universe , 1983 .

[20]  S. Fukao,et al.  Vertical eddy diffusivity in the lower and middle atmosphere: A climatology based on the MU radar observations during 1986–1992 , 1996 .

[21]  R. Stull An Introduction to Boundary Layer Meteorology , 1988 .

[22]  W. Y. Chen,et al.  Structure functions of turbulence in the atmospheric boundary layer over the ocean , 1970, Journal of Fluid Mechanics.

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

[24]  W. Hocking An assessment of the capabilities and limitations of radars in measurements of upper atmosphere turbulence , 1996 .

[25]  G. D. Nastrom,et al.  Doppler radar spectral width broadening due to beamwidth and wind shear , 1997 .

[26]  U. Schumann,et al.  Estimate of diffusion parameters of aircraft exhaust plumes near the tropopause from nitric oxide and turbulence measurements , 1995 .

[27]  J. Weinstock Energy Dissipation Rates of Turbulence in the Stable Free Atmosphere , 1981 .

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