Ganymede presents a unique example of an internally magnetized moon wh
ose intrinsic magnetic field excludes the plasma present at its orbit,
thereby forming a magnetospheric cavity. We describe some of the prop
erties of this mini-magnetosphere, embedded in a sub-Alfvenic flow and
formed within a planetary magnetosphere. A vacuum superposition model
(obtained by adding the internal field of Ganymede to the field impos
ed by Jupiter) organizes the data acquired by the Galileo magnetometer
on four close passes in a useful, intuitive fashion. The last field l
ine that links to Ganymede at both ends extends to similar to 2 Ganyme
de radii, and the transverse scale of the magnetosphere is similar to
5.5 Ganymede radii. Departures from this simple model arise from curre
nts flowing in the Alfven wings and elsewhere on the magnetopause. The
four passes give different cuts through the magnetosphere from which
we develop a geometric model for the magnetopause surface as a functio
n of the System Ln location of Ganymede. On one of the passes, Ganymed
e was located near the center of Jupiter's plasma disk. For this pass
we identify probable Kelvin-Helmholtz surface waves on the magnetopaus
e, After entering the relatively low-latitude upstream magnetosphere,
Galileo apparently penetrated the region of closed field lines (ones t
hat link to Ganymede at both ends), where we identify predominantly tr
ansverse fluctuations at frequencies reasonable for field line resonan
ces. We argue that magnetic field measurements, when combined with flo
w measurements, show that reconnection is extremely efficient. Downstr
eam reconnection, consequently, may account for heated plasma observed
in a distant crossing of Ganymede's wake. We note some of the ways in
which Ganymede's unusual magnetosphere corresponds to familiar planet
ary magnetospheres (viz., the magnetospheric topology and an electron
ring current). We also comment on some of the ways in which it differs
from familiar planetary magnetospheres (viz., relative stability and
predictability of upstream plasma and field conditions, absence of a m
agnetotail plasma sheet and of a plasmasphere, and probable instabilit
y of the ring current).