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Polar observations of the characteristics of the dayside high altitude cusp T. A. FRITZ, J. CHEN, J. NIEHOF r for Space Physics at Boston Universit Polar PI conference call December 3, 2004

Polar observations of the characteristics of the dayside high altitude cusp

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Polar observations of the characteristics of the dayside high altitude cusp. Polar PI conference call December 3, 2004. T. A. FRITZ, J. CHEN, J. NIEHOF Center for Space Physics at Boston University. The Chapman Ferraro Cusp. - PowerPoint PPT Presentation

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Page 1: Polar observations of the characteristics of the dayside high altitude cusp

Polar observations of the characteristics of the dayside high altitude cusp

T. A. FRITZ, J. CHEN, J. NIEHOFCenter for Space Physics at Boston University

Polar PI conference callDecember 3, 2004

Page 2: Polar observations of the characteristics of the dayside high altitude cusp

The Chapman Ferraro Cusp

Observationally Polar has shown that the cusp is a large region and is the site of continuous large fluxes of energetic particles.

At BU we feel that we have established that these energetic particles are produced there and we are searching for the mechanism that does that.

10

10

Page 3: Polar observations of the characteristics of the dayside high altitude cusp

Cusp Energy Density comparison published by Chang et al., 1998

June 20, 1996

Page 4: Polar observations of the characteristics of the dayside high altitude cusp

8/27/96

Total Pressure (x10)

Magnetic Pressure

Plasma Prep. Pressure

Page 5: Polar observations of the characteristics of the dayside high altitude cusp

8/27/96 9/18/96

4/20/99 4/24/99

Page 6: Polar observations of the characteristics of the dayside high altitude cusp

8/27/96

Btotal

Vx

MICS He++

MICS O+6

MICS H+

Hydra ions

Page 7: Polar observations of the characteristics of the dayside high altitude cusp

Btotal

P prep (electrons)

P prep (ions)

Ion Density (Hydra)

Ion Density (Tide)

EFI Density

8/27/96

Page 8: Polar observations of the characteristics of the dayside high altitude cusp

Btotal

Vx (km/s)

MICS He++

MICS O+6

MICS H+

Hydra ions

9/18/96

Page 9: Polar observations of the characteristics of the dayside high altitude cusp

Btotal

P prep (electrons)

P prep (ions)

Ion Density (Hydra)

Ion Density (Tide)

EFI Density

Page 10: Polar observations of the characteristics of the dayside high altitude cusp

Btotal

Vx (km/s)

MICS He++

MICS O+6

MICS H+

Hydra ions

4/20/99

Page 11: Polar observations of the characteristics of the dayside high altitude cusp

Btotal

P prep (electrons)

P prep (ions)

Ion Density (Hydra)

Ion Density (Tide)

EFI Density

Page 12: Polar observations of the characteristics of the dayside high altitude cusp

Btotal

Vx (km/s)

MICS He++

MICS O+6

MICS H+

Hydra ions

4/24/99

Page 13: Polar observations of the characteristics of the dayside high altitude cusp

Btotal

P prep (electrons)

P prep (ions)

Ion Density (Hydra)

Ion Density (Tide)

EFI Density

Page 14: Polar observations of the characteristics of the dayside high altitude cusp

Ions Electrons

9/18/96

R=-0.86 R=-0.87

R=-0.93 R=-0.95

Page 15: Polar observations of the characteristics of the dayside high altitude cusp

Ions Electons

8/27/99

R=-0.90 R=-0.95

R=-0.83 R=-0.91

Page 16: Polar observations of the characteristics of the dayside high altitude cusp
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Page 21: Polar observations of the characteristics of the dayside high altitude cusp

Conclusions:

We have attempted to understand the components that must provide the energy density within the high-altitude cusp.

With the advertised data from the Polar team there is a deficiency of the measured plasma pressure in creating a balance.

The local plasma from the solar wind creates the diamagnetic cavity.

The perpendicular pressure provided by both the ions and electrons are highly anti-correlated with the turbulence as expected but the electrons surprisingly show a higher level of anti-correlation.

The sense of the polarization of the observed electric component of the turbulence in the direction perpendicular to B can provide resonate acceleration of ions rapidly to high energies.