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Fundamental Technologies
Galileo Spacecraft Pages
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Investigation of the Magnetosphere of Ganymede with Galileo's Energetic Particle Detector
Ph.D. dissertation by Shawn M. Stone, University of Kansas, 1999.
List of Tables
- Table 1.1 Planets discovered to have an intrinsic magnetic
field by visiting spacecraft
- Table 1.2 Closest approach of the Voyager spacecraft to the
Galilean moons
- Table 1.3 Comparison between the times of the
observed microsignatures at Saturn for Voyager 1 and 2 and the times predicted by the dipole and
Z3+ current models
- Table 1.4 The magnetopause crossing and closest
approach times for the G2 and G7 encounters
- Table 3.1 Galileo EPD statistics
- Table 3.2 LEMMS A channels and passband energies
- Table 3.3 LEMMS E and F channels and passband energies
- Table 3.4 LEMMS geometrical factors for A,
E, and F channels
- Table 3.5 The standard equatorial coordinates for the north
pole of the respective body in J1950
- Table 3.6 The motor position index (0-7) is shown
with their corresponding angle q with respect to the SC Z axis
- Table 3.7 Spin sector index (1-16) with their
corresponding phase angle f
- Table 4.1 Schmidt quasi-normalized Legendre
functions to nmax=3
- Table 4.2 The coefficients aj
in the series expansion of the spherical harmonic coefficients Knm(l), of the scalar magnetic potential for the magnetopause field up to
nmax=2
- Table 4.3 The coefficients in the series
expansion of the spherical harmonics for the tail field Lnm(l)
up to nmax=2
- Table 4.4 The Jupiter O6 magnetic field model
Schmidt-Normalized spherical harmonic coefficients in Gauss as given by Connerney [1993]
- Table 4.5 The best fit parameters to Equations [4.25] and
[4.26] for the three Jovian outbound encounters
- Table 4.6 Values in nT of the uniform Jovian background field
used in model 1 calculated from the KK96 model [Khurana, 1997]
- Table 4.7 The mean and standard deviation of the first 100
magnetic field components in GSII Cartesian coordinates
- Table 4.8 Coefficients resulting from the minimization of
Equation [4.33] for G2 for r0=2.0 Rg
- Table 4.9 Coefficients for G7 resulting from
the minimization of Equation [4.33] with the internal multipole model of Ganymede specified
from Table 4.8
- Table 4.10 The boundary parameters for G2
and G7 derived from the fit of Equation [4.35]
- Table 4.11 Aberration angles of the
corotational plasma flow as ascertained from the look directions of the maximum and minimum
rates
- Table 5.1 The Rm values in Rg
beyond which particles in extended bound mode are considered to have convected past the Ganymede
interaction region
- Table 5.2 Bounce times between the Ganymede
region and the Jupiter bounce point for electrons
- Table 6.1 Summary of the time reversed particle
trace presented in Figures 6.12 through 6.17 for subenergy 400 keV sublook direction 1 for model M1
channel A4
- Table 6.2 Summary of Figures 6.18 through 6.23 for subenergy
400 keV sublook direction 5 for model M1 channel A4
- Table 6.3 Summary of Figures 6.26 through 6.31
for subenergy 1110 keV sublook direction 5 for model M2 channel A6
- Table 6.4 Summary of Figures 6.32 through 6.37
for subenergy 1110 keV sublook direction 7 for model M2 channel A6
- Table 6.5 Summary of features of model M1
and M2 not included in the main body of the text. The corresponding graphs are presented
in Appendix C.
- Table 6.6 Summary of Figures 6.40 through
6.45 for subenergy 74 keV sublook direction 1 for model M1 channel E3
- Table 6.7 Summary of Figures 6.48 through 6.53
for subenergy 74 keV sublook direction 1 for model M2 channel E3
- Table 6.8 Summary of the time-reversed particle
trace presented in Figures 6.70 through 6.75 for subenergy 74 keV sublook direction 3 for model M1 channel
E3. (This table still under construction.)
- Table 6.9 Summary of the time-reversed
particle trace presented in Figures 6.77 through 6.82 for subenergy 74 keV sublook direction 3
for model M2 channel E3. (This table still under construction.)
- Table 6.10 Summary of features of model M1
and M2 not included in the main body of the text for the closest approach portion of the
G2 encounter.
- Table 6.11 Summary of the time-reversed
particle trace presented in Figures 6.130 through 6.135 for subenergy 400 keV sublook direction 9 for
model M1 channel A4
- Table 6.12 Summary of the time-reversed
particle trace presented in Figures 6.137 through 6.142 for subenergy 400 keV sublook direction 10 for
model M2 channel A4
- Table 6.13 Summary of features of model M1
and M2 not included in the main body of the text for the outbound portion of the G2
encounter. The corresponding graph is presented in Appendix C.
- Table 7.1 Addition of corotational electric field. Summary of
Figures 7.1 through 7.6 for model M1
- Table 7.2 Addition of corotational electric field.
Summary of Figures 7.7 through 7.12 for model M2
- Table 7.3 Summary of the time-reversed particle
trace presented in Figures 7.15 through 7.20 for subenergy 37 keV sublook direction 1 for model M1
channel E1 at 25% of full corotation
- Table 7.4 Summary of the time-reversed particle
trace presented in Figures 7.23 through 7.28 for subenergy 37 keV sublook direction 1 for model
M1 channel E1 at 50% of full corotation
- Table 7.5 Summary of the time-reversed particle
trace presented in Figures 7.32 through 7.37 for subenergy 37 keV sublook direction 1 for model
M2 channel E1 at 25% of full corotation
- Table 7.6 Summary of the time-reversed particle
trace presented in Figures 7.38 through 7.43 for subenergy 37 keV sublook direction 1 for model
M2 channel E1 at 50% of full corotation
- Table 7.7 Inclusion of anti-parallel electric field for
feature G2-19:10:51; summary of Figures 7.44 through 7.49 for model M1
- Table 7.8 Inclusion of anti-parallel electric
field for feature G2-19:10:51: summary of Figures 7.50 through 7.55 for model M2
- Table 8.1 Comparison of magnetic field model
M1 and M2 at the G2 encounter
- Table 8.2 Comparison of magnetic field model M1
and M2 at the G7 encounter
- Table 8.3 Closest approach feature G2-18:56:31
- Table 8.4 Closest approach feature G2-18:58:31
- Table 8.5 Outbound feature G2-19:08:51
- Table 8.6 Outbound feature G2-19:10:51
- Table 8.7 Inbound feature G7-07:06:33
- Table 8.8 Inbound feature G7-07:11:13
- Table 8.9 Closest approach feature G2-18:56:31
- Table 8.10 Closest approach feature G2-18:58:31
- Table 8.11 Outbound feature G2-19:08:51
- Table 8.12 Outbound feature G2-19:10:51
- Table 8.13 Outbound feature G7-07:22:14
- Table 8.14 Scattering coefficients for
the G2 and G7 loss cone and anti-loss cone features derived from the correlations in chapter 6
- Table 8.15 Outbound feature G2-18:56:31
- Table 8.16 Outbound feature G2-19:10:51
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Updated 8/27/2007, T. Hunt-Ward
tizby@ftecs.com