Gravity wave initiation of equatorial spread F/plasma bubble irregularities based on observational data from the SpreadFEx campaign

Abstract. The data from ground based experiments conducted during the 2005 SpreadFEx campaign in Brazil are used, with the help of theoretical model calculations, to investigate the precursor conditions, and especially, the role of gravity waves, in the instability initiation leading to equatorial spread F development. Data from a digisonde and a 30 MHz coherent back-scatter radar operated at an equatorial site, Sao Luis (dip angle: 2.7°) and from a digisonde operated at another equatorial site (dip angle: −11.5°) are analyzed during selected days representative of differing precursor conditions of the evening prereversal vertical drift, F layer bottom-side density gradients and density perturbations due to gravity waves. It is found that radar irregularity plumes indicative of topside bubbles, can be generated for precursor vertical drift velocities exceeding 30 m/s even when the precursor GW induced density oscillations are marginally detectable by the digisonde. For drift velocities ≤20 m/s the presence of precursor gravity waves of detectable intensity is found to be a necessary condition for spread F instability initiation. Theoretical model calculations show that the zonal polarization electric field in an instability development, even as judged from its linear growth phase, can be significantly enhanced under the action of perturbation winds from gravity waves. Comparison of the observational results with the theoretical model calculations provides evidence for gravity wave seeding of equatorial spread F.

[1]  E. Bonelli,et al.  The prereversal enhancement of the zonal electric field in the equatorial ionosphere , 1986 .

[2]  I. Batista,et al.  Thermospheric meridional wind control of equatorial spread F and evening prereversal electric field , 2006 .

[3]  P. C. Kendall,et al.  Electrical coupling of the E- and F-regions and its effect on F-region drifts and winds , 1974 .

[4]  P. J. Sultan,et al.  Linear theory and modeling of the Rayleigh‐Taylor instability leading to the occurrence of equatorial spread F , 1996 .

[5]  I. Batista,et al.  Vertical ionization drift velocities and range type spread F in the evening equatorial ionosphere , 1983 .

[6]  E. R. Paula,et al.  Effects of the vertical plasma drift velocity on the generation and evolution of equatorial spread F , 1999 .

[7]  David L. Hysell,et al.  Collisional shear instability in the equatorial F region ionosphere , 2004 .

[8]  I. Batista,et al.  Onset conditions of equatorial (range) spread F at Fortaleza, Brazil, during the June solstice , 1997 .

[9]  Raphaël F. Garcia,et al.  Response of the ionosphere to the seismic trigerred acoustic waves: Electron density and electromagnetic fluctuations , 2009 .

[10]  M. Larsen,et al.  Gravity wave initiation of equatorial spread F: A case study , 1981 .

[11]  F. Kamalabadi,et al.  Gravity wave and tidal influences on equatorial spread F based on observations during the Spread F Experiment (SpreadFEx) , 2008 .

[12]  F. S. Johnson,et al.  Occurrence of equatorial F region irregularities: Evidence for tropospheric seeding , 1998 .

[13]  D. Fritts,et al.  The impact of gravity waves rising from convection in the lower atmosphere on the generation and nonlinear evolution of equatorial bubble , 2009 .

[14]  M. A. Abdu,et al.  Equatorial F region vertical plasma drifts: Seasonal and longitudinal asymmetries in the American sector , 1986 .

[15]  B. L. Cragin,et al.  The effect of vertical drift on the equatorial F-region stability , 1986 .

[16]  Ronald F. Woodman,et al.  Average vertical and zonal F region plasma drifts over Jicamarca , 1991 .

[17]  Ronald F. Woodman,et al.  Equatorial spread F: Implications of VHF radar observations , 1970 .

[18]  T. Maruyama A diagnostic model for equatorial spread F, 1, Model description and application to electric field and neutral wind effects , 1988 .

[19]  R. Woodman,et al.  Seeding and layering of equatorial spread F by gravity waves , 1990 .

[20]  B. Reinisch,et al.  Conjugate Point Equatorial Experiment (COPEX) Campaign in Brazil: Electrodynamics highlights on spread F development conditions and day-to-day variability , 2009 .

[21]  David L. Hysell,et al.  Equatorial spread-F initiation: Post-sunset vortex, thermospheric winds, gravity waves , 2007 .

[22]  Jürgen Röttger,et al.  Equatorial spread-F by electric fields and atmospheric gravity waves generated by thunderstorms , 1981 .

[23]  H. Takahashi,et al.  Simultaneous observation of ionospheric plasma bubbles and mesospheric gravity waves during the SpreadFEx Campaign , 2009 .

[24]  Erhan Kudeki,et al.  Postsunset vortex in equatorial F‐region plasma drifts and implications for bottomside spread‐F , 1999 .

[25]  Bodo W. Reinisch,et al.  Vertical electron density profiles from the Digisonde network , 1996 .

[26]  M. Kelley,et al.  Nonlinear evolution of equatorial spread F 4. Gravity waves, velocity shear, and day-to-day variability , 1996 .

[27]  Sidney L. Ossakow,et al.  Nonlinear equatorial spread F: The effect of neutral winds and background Pedersen conductivity , 1982 .

[28]  S. Vadas,et al.  Gravity wave penetration into the thermosphere: sensitivity to solar cycle variations and mean winds , 2008 .

[29]  M. A. Abdu,et al.  Outstanding problems in the equatorial ionosphere–thermosphere electrodynamics relevant to spread F , 2001 .

[30]  John W. MacDougall,et al.  Presunrise spread F at Fortaleza , 1998 .

[31]  L. Linson,et al.  Formation of striations in ionospheric plasma clouds , 1970 .

[32]  M. Kelley,et al.  Nonlinear evolution of equatorial spread F: 2. Gravity wave seeding of Rayleigh‐Taylor instability , 1996 .

[33]  Thomas Dautermann,et al.  Overview and summary of the Spread F Experiment (SpreadFEx) , 2009 .

[34]  C. Hines INTERNAL ATMOSPHERIC GRAVITY WAVES AT IONOSPHERIC HEIGHTS , 1960 .

[35]  Sidney L. Ossakow,et al.  Three‐dimensional nonlinear evolution of equatorial ionospheric spread‐F bubbles , 2003 .

[36]  Bodo W. Reinisch,et al.  Coordinated digisonde and incoherent scatter radar F region drift measurements at Sondre Stromfjord , 1995 .

[37]  B. Reinisch,et al.  A comparison of ionospheric vertical drift velocities measured by Digisonde and Incoherent Scatter Radar at the magnetic equator , 2006 .

[38]  Henry Rishbeth,et al.  Polarization fields produced by winds in the equatorial F-region , 1971 .

[39]  S. Prakash Production of electric field perturbations by gravity wave winds in the E region suitable for initiating equatorial spread F , 1999 .

[40]  R. Sekar,et al.  Effects of vertical winds and electric fields in the nonlinear evolution of equatorial spread F , 1994 .

[41]  H. Takahashi,et al.  Magnetospheric disturbance induced equatorial plasma bubble development and dynamics: A case study in Brazilian sector , 2003 .

[42]  B. Reinisch,et al.  Equatorial F region evening vertical drift, and peak height, during southern winter months: A comparison of observational data with the IRI descriptions , 2006 .