GALILEO

**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.

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Updated 8/23/19, Cameron Crane

## QUICK FACTS

**Manufacturer:**The Galileo Spacecraft was manufactured by the Jet Propulsion Laboratory, Messerschmitt-Bölkow-Blohm, General Electric, and the Hughes Aircraft Company.

**Mission Duration:**Galileo was planned to have a mission duration of around 8 years, but was kept in operation for 13 years, 11 months, and 3 days, until it was destroyed in a controlled impact with Jupiter on September 21, 2003.

**Destination:**Galileo's destination was Jupiter and its moons, which it orbitted for 7 years, 9 months, and 13 days.