Investigation of the Magnetosphere of Ganymede with Galileo's Energetic Particle Detector

Ph.D. dissertation by Shawn M. Stone, University of Kansas, 1999.

Copyright 1999 by Shawn M. Stone.  Used with permission.

List of Figures (Part 4, Appendix B)

• Figure B1 ZX projection of the G7 encounter in GSII coordinates
• Figure B2 ZY projection of the G7 encounter in GSII coordinates.
• Figure B3 Radial distance to the center of Ganymede for the G7 encounter as a function of encounter time
• Figure B4 Angle of deviation between the measured magnetic field vector with that of the model field vector
• Figure B5 Model 1 field line tracing for the G7 encounter
• Figure B6 Model 2 field line tracing for the G7 encounter
• Figure B7 A: Rate profile for feature G7-07:06:33 for the electrons as measured by the EPD instrument during the G7 encounter. B: The pitch (a) and phase (f) values of the particles as measured by the EPD detector.
• Figure B8 A: Rate profile for feature G7-07:11:33 for the electrons as measured by the EPD instrument during the G7 encounter. B: The pitch (a) and phase (f) values of the particles as measured by the EPD detector.
• Figure B9 A: Rate profile for feature G7-07:22:13 for the electrons as measured by the EPD instrument during the G7 encounter. B: The pitch (a) and phase (f) values of the particles as measured by the EPD detector.
• Figure B10 A: Simulated M1 and real (Re) rate profile for the feature G7-07:06:33 of channel E1 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B11 A: Simulated M1 and real (Re) rate profile for the feature G7-07:06:33 of channel E3 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B12 A: Simulated M1 and real (Re) rate profile for the feature G7-07:06:33 of channel F2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B13 A: Simulated M1 and real (Re) rate profile for the feature G7-07:06:33 of channel A2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B14 A: Simulated M1 and real (Re) rate profile for the feature G7-07:06:33 of channel A4 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B15 A: Simulated M1 and real (Re) rate profile for the feature G7-07:06:33 of channel A6 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B16 A: Simulated M2 and real (Re) rate profile for the feature G7-07:06:33 of channel E1 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B17 A: Simulated M2 and real (Re) rate profile for the feature G7-07:06:33 of channel E3 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B18 A: Simulated M2 and real (Re) rate profile for the feature G7-07:06:33 of channel F2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B19 A: Simulated M2 and real (Re) rate profile for the feature G7-07:06:33 of channel A2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B20 A: Simulated M2 and real (Re) rate profile for the feature G7-07:06:33 of channel A4 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B21 A: Simulated M2 and real (Re) rate profile for the feature G7-07:06:33 of channel A6 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B22 A: Simulated M1 and real (Re) rate profile for the feature G7-07:11:13 of channel E1 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B23 A: Simulated M1 and real (Re) rate profile for the feature G7-07:11:13 of channel E3 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B24 A: Simulated M1 and real (Re) rate profile for the feature G7-07:11:13 of channel F2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B25 A: Simulated M1 and real (Re) rate profile for the feature G7-07:11:13 of channel A2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B26 A: Simulated M1 and real (Re) rate profile for the feature G7-07:11:13 of channel A4 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B27 A: Simulated M1 and real (Re) rate profile for the feature G7-07:11:13 of channel A6 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B28 A: Simulated M2 and real (Re) rate profile for the feature G7-07:11:13 of channel E1 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B29 A: Simulated M2 and real (Re) rate profile for the feature G7-07:11:13 of channel E3 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B30 A: Simulated M2 and real (Re) rate profile for the feature G7-07:11:13 of channel F2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B31 A: Simulated M2 and real (Re) rate profile for the feature G7-07:11:13 of channel A2 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B32 A: Simulated M2 and real (Re) rate profile for the feature G7-07:11:13 of channel A4 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B33 A: Simulated M2 and real (Re) rate profile for the feature G7-07:11:13 of channel A6 normalized to 90º of pitch. B: The pitch and phase angles as calculated from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B34 A: Simulated M1 and real (Re) rate profile for the feature G7-07:22:14 of channel E1 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 50 and 10. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B35 A: Simulated M1 and real (Re) rate profile for the feature G7-07:22:14 of channel E1 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 50 and 0. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B36 A: Simulated M1 and real (Re) rate profile for the feature G7-07:22:14 of channel E3 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 50 and 10. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B37 A: Simulated M1 and real (Re) rate profile for the feature G7-07:22:14 of channel E3 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 50 and 0. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B38 A: Simulated M1 and real (Re) rate profile for the feature G7-07:22:14 of channel F2 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 50 and 10. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B39 A: Simulated M1 and real (Re) rate profile for the feature G7-07:22:14 of channel F2 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 50 and 0. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B40 A: Simulated M2 and real (Re) rate profile for the feature G7-07:22:14 of channel E1 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 30 and 10. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B41 A: Simulated M2 and real (Re) rate profile for the feature G7-07:22:14 of channel E1 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 30 and 0. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B42 A: Simulated M2 and real (Re) rate profile for the feature G7-07:22:14 of channel E3 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 30 and 10. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B43 A: Simulated M2 and real (Re) rate profile for the feature G7-07:22:14 of channel E3 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 30 and 0. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B44 A: Simulated M2 and real (Re) rate profile for the feature G7-07:22:14 of channel F2 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 5 and 1. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.
• Figure B45 A: Simulated M2 and real (Re) rate profile for the feature G7-07:22:14 of channel F2 normalized to 90º of pitch. The simulated runs are done in extended bounce mode with scattering included. Scattering coefficients are 1 and 0. B: The pitch and phase angles are computed from the look direction of the EPD detector and the appropriate magnetic field vector R for real and S for simulated.

Figures, continued 

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