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SuperDARN and reversed flow events in the cusp

SD2011. SuperDARN and reversed flow events in the cusp. K. Oksavik 1 , J. Moen 1,2 , E. H. Rekaa 2 , H. C. Carlson 3 , and M. Lester 4 1) UNIS, Longyearbyen, Norway 2) Department of Physics, Univ. Oslo, Oslo, Norway 3) CASS, Utah State University, USA

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SuperDARN and reversed flow events in the cusp

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  1. SD2011 SuperDARN and reversed flow events in the cusp K. Oksavik1, J. Moen1,2 , E. H. Rekaa2, H. C. Carlson3, and M. Lester4 1) UNIS, Longyearbyen, Norway 2) Department of Physics, Univ. Oslo, Oslo, Norway 3) CASS, Utah State University, USA 4) Department of Physics & Astronomy, Univ. Leicester, UK

  2. Background on RFE Reversed flow events (RFEs): • First seen with the EISCAT Svalbard radar • Longitudinally elongated, segments of transiently enhanced ion flow, in the direction opposite to the background flow • For both RFE and background flow: |Vlos| > 250 m/s (but in opposite directions) • Size: >400 km in longitude • Form one by one (not in pairs) Rinne et al. [2007]

  3. Three events will be studied • Solar wind is stable: • By positive • Bz negative • SD coverage: • 700-800 data points • VPC = 50-60 kV

  4. RFE seen by SuperDARN • The RFE flow channel (red color) is located in an area of sunward flow (blue color) in the postnoon sector • This is the first report of RFE in SD data!

  5. RFEs seem to occur in areas of high backscatter power and wide Doppler spectra The backscatter power / spectral width is often highest along one edge of RFEs, and low along the other edge Several examples of RFEs

  6. Events 1 and 2 were part of an interval of prolonged activity A transition took place at 09:05 UT The poleward edge of event 3 coincided with wide Doppler spectra and growing backscatter power Are RFE important for the formation of irregularities? 1 2 3 Time development of RFEs

  7. Formation of plasma irregularities via flow shears • The KH growth rate is [Keskinen et al., 1988]: • Most ∆VLOS are small, but some reach 800 m/s (i.e. growth time of 300 s) • A 42˚ angle between the radar beam and the large-scale flow decreases the net growth time to 200 s • Rinne et al. [2007] found examples of L = 12 km (i.e. growth time of 60 s) • KH may be efficient at producing irregularities! ∆VLOS Neighboring range gates

  8. Offset between SD and optics There appears to be an offset in latitude between RFE and the aurora

  9. Flow vorticity and FACs [Sofko et al., 1995]

  10. Determination of ground range • The clockwise flow reversal (i.e. upward FAC) aligns with the aurora, if we shift the Hankasalmi radar echoes equatorward by 140 km • Consistent with other studies [Yeoman et al., 1997]

  11. Conclusions • We have documented several examples of RFE channels seen by SuperDARN • The location of RFE flow shears relative to auroral arcs shows that the SD ground range was overestimated by 140 km • RFEs may be important for the formation of plasma irregularities via flow shear instabilities (Kelvin Helmholtz) • The large SuperDARN dataset offers new opportunities to learn more about RFEs

  12. From June 01, 2011 New address: Department of Physics and Technology, University of Bergen, P.B. 7803, NO-5020 Bergen, NORWAY. E-mail: kjellmar.oksavik@uib.no

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