Statistical characterization of SAPS velocities

B. S. R. Kunduri, J. B. H. Baker, J. M. Ruohoniemi, S. G. Shepherd, P. J. Erickon, A. J. Coster and E. G. Thomas

Introduction - SD SAPS Location model

Kunduri et al [2017], under review.

Introduction - Velocity characterization

Kunduri et al [2017], under review.

Problem statement

  • In Kunduri et al., [2017] (under review), we
    • ​developed SuperDARN based SAPS location model
    • discussed SAPS speeds using gridded line-of-sight velocities assuming SAPS were perfectly westwards.
  • A detailed characterization of SAPS velocities is required to complete the SAPS model. In this study
    • we analyze variations in SAPS flow direction with MLT.
    • we analyze mean SAPS velocities at different Dst bins and MLTs.
    • we derive kernel density estimates of SAPS velocities.

Traditional L-shell fitting approach [Clausen et al., 2012]

  • Clausen et al [2012] approach was to derive one L-shell fit for each radar pair. The approach was ideally suitable for case studies.
  • Not directly adaptable to statistical studies.
  • Three L-shell fit velocities (3 radar pairs) for data spanning more than 7 hours in MLT would be under utilization of resources.
  • The first step is make L-shell fitting applicable to statistical studies.

Optimized use of regions with "good" scatter

  • Instead of one velocity for each radar pair. We search the entire "map" to detect locations where L-shell fitting can be applied (irrespective of radars).
  • Regions where common volume measurements are available (highlighted above) are especially suited for applying L-shell fitting technique.

Identify all regions with "good" scatter

  • Apply a standard grid over SAPS observations.
  • Each cell in the grid is 1 hour MLT, 0.5 degrees MLAT (SAID features have narrow latitudinal range).
  • Cells with "good" scatter will:
    • ​have measurements with l-o-s azimuth range > 35.
    • Atleast have 3 unique azimuth measurements.
    • When fitting a sinusoid, determined SAPS azimuth should be within -90 +/- 20 degrees.
    • Fitting error should be less than 25%.
  • NOTE : L-o-s velocities below 150 m/s are discarded.

L-shell map (April 9, 2011 0840 UT)

  • Solid lines indicate velocities where "good" L-shell fit could be derived,
  • Dashed lines indicate velocities whose directions were assumed to be same as the nearest "good" fit.
  • Results are comparable to Clausen et al, [2012].
  • The L-shell map approach is suitable for statistical studies. - 1) results are standardized for all events. 2) not impacted by data availability at radar pairs.

L-shell map movie : Apr-9-2011

Mean velocities by Dst bins

  • Mean SAPS velocities at each Dst bin.
  • Velocities are higher in the dusk sector.
  • Velocities are higher at lower Dst levels.

Azimuths (and linear fits) by Dst bins

  • Mean  and std. dev. of SAPS velocity directions at different Dst bins.  -90 is perfectly westwards. The solid lines represent a linear fit to mean azimuths.
  • Flow direction becomes increasingly polewards towards dusk. Indicative of SAPS merging with auroral flows eventually? The pattern is also observed (not discussed) in Clausen et al [2012] event.

Kernel density estimates of velocities

  • The Figure presents histograms, kernel density estimates (red) and fitted skewed gaussian curves (dashed blue) for SAPS velocities for different Dst bins at a selected location.
  • Skewed gaussian appears to be a better fit for the KDEs (after trying several others).
  • The likelihood of observing higher velocities increases with geomagnetic activity.
  • With decreasing Dst gaussian curve changes from right skewed to left skewed.

Modeling the kernel density estimates

  • Figure shows KDEs of velocities for lowest dst bin at different MLTs.
  • Likelihood of observing higher velocities increases near dusk.
  • Each KDE can be modeled separately, but a universal model (function of Dst, MLAT, MLT) like SAPS location model is difficult.

Conclusions

  • Used L-shell fitting to estimate SAPS velocities
  • The mean SAPS velocities increased as we move towards dusk and at higher disturbance levels.
  • Flow direction was more polewards near dusk than near mid-night.
  • Kernel density estimates of velocities at a given location and dst-bin suggest a skewed gaussian distribution of velocities.
  • Developing a dst and geomagnetic location based common model is proving difficult. Tried different fits/distributions - skewed gaussian, rayleigh etc.

L-shell fitting

By Bharat Kunduri

L-shell fitting

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