Radar observations of two‐dimensional turbulence in the equatorial electrojet, 3. Nighttime observations of Type 1 waves

The large vertically directed 50-MHz radar at Jicamarca has sufficient sensitivity to study nighttime echoes from the equatorial electrojet in detail with good resolution. Here we concentrate on type 1 (‘two-stream’) echoes. We find that (1) these echoes sometimes dominate the spectrum (which is never the case in daytime for a vertically directed radar), (2) they are observed over a much wider range of altitudes than they are during daytime, (3) they show an asymmetry which reverses from day to night (downgoing waves are more common at night), (4) the magnitude of the mean Doppler shift appears to increase somewhat with altitude, and (5) there is evidence of large-scale (kilometers) structure as well as intermediate (tens or hundreds of meters) and small (the wavelengths of meters or less which are directly responsible for radar echoes). We describe a model which qualitatively accounts for all the important characteristics of the observations. Long and intermediate waves with roughly horizontal k are initially unstable, and a complicated two-dimensional energy cascade process develops, with energy transfers probably going in both directions in k space. The asymmetry in the echoes can be explained if either the density depletions at the intermediate wavelengths are stronger than the enhancements or the positive density gradients are steeper than the negative.

[1]  R. Sudan,et al.  Temporal and spatial power spectrum studies of numerical simulations of Type II gradient drift irregularities in the equatorial electrojet , 1978 .

[2]  T. H. Dupree,et al.  Renormalized dielectric function for collisionless drift wave turbulence , 1978 .

[3]  J. Hoffman,et al.  Plasma bubbles and irregularities in the equatorial ionosphere , 1977 .

[4]  R. Sudan,et al.  Numerical simulations of type II gradient drift irregularities in the equatorial electrojet , 1977 .

[5]  R. Sudan,et al.  Theory of strongly turbulent two-dimensional convection of low-pressure plasma , 1977 .

[6]  Anthony J. Scannapieco,et al.  Nonlinear equatorial spread F , 1976 .

[7]  Warner L. Ecklund,et al.  Evidence for a Rayleigh-Taylor type instability and upwelling of depleted density regions during equatorial spread F , 1976 .

[8]  Tetsuya Sato,et al.  Self‐consistent studies of two‐dimensional large‐scale (∼100 m) electrojet irregularities , 1976 .

[9]  D. T. Farley,et al.  Radar measurements of neutral winds and temperatures in the equatorial E region , 1976 .

[10]  D. T. Farley,et al.  The effect of the gradient drift term on type 1 electrojet irregularities , 1975 .

[11]  H. Pécseli,et al.  The K spectrum of ionospheric irregularities , 1975 .

[12]  D. T. Farley,et al.  Vertical structure of the VHF backscattering region in the equatorial electrojet and the gradient drift instability , 1975 .

[13]  T. Rognlien,et al.  Nonlinear saturation and angular rotation of instabilities in the E layer , 1975 .

[14]  R. Sudan,et al.  Numerical studies of type 2 equatorial electrojet irregularity development , 1975 .

[15]  T. Rognlien,et al.  Theory of the nonlinear spectrum of the gradient drift instability in the equatorial electrojet , 1974 .

[16]  D. T. Farley Irregularities in the equatorial ionosphere: The Berkner Symposium , 1974 .

[17]  D. T. Farley,et al.  Radar observations of two dimensional turbulence in the equatorial electrojet, 2 , 1973 .

[18]  T. Rognlien,et al.  Nonlinear saturation of the gradient drift instability in the equatorial electrojet , 1973 .

[19]  Tetsuya Sato Unified theory of type I and II irregularities in the equatorial electrojet , 1973 .

[20]  P. Kaw Wave propagation effects on observation of irregularities in the equatorial electrojet , 1972 .

[21]  B. Balsley A longitudinal variation of electron drift velocity in the equatorial electrojet , 1970 .

[22]  N. D’angelo,et al.  Type II irregularities in the equatorial electrojet , 1970 .

[23]  Douglas K. Lilly,et al.  Numerical Simulation of Two‐Dimensional Turbulence , 1969 .

[24]  M. Sugiura,et al.  An improved model equatorial electrojet with a meridional current system , 1969 .

[25]  C. Leith Diffusion Approximation for Two‐Dimensional Turbulence , 1968 .

[26]  J. Untiedt A model of the equatorial electrojet involving meridional currents , 1967 .

[27]  R. Kraichnan Inertial Ranges in Two‐Dimensional Turbulence , 1967 .

[28]  R. Cohen,et al.  Secondary irregularities in the equatorial electrojet , 1967 .

[29]  P. Catto Adiabatic modifications to plasma turbulence theories , 1978 .

[30]  C. Kennel,et al.  On the marginally stable saturation spectrum of unstable type I equatorial electrojet irregularities , 1974 .

[31]  D. T. Farley,et al.  Instabilities in the equatorial electrojet , 1973 .

[32]  D. T. Farley,et al.  GENERATION OF SMALL-SCALE IRREGULARITIES IN THE EQUATORIAL ELECTROJET. , 1973 .