The front boundary of the magnetic cloud at day 291.79 was well-defined. The magnetic field strength increased, the magnetic field direction rotated southward, the density decreased by a large amount, and the temperature decreased (Figure 1). The large abrupt changes in the field and plasma parameters suggest that the boundary was a tangential discontinuity in the MHD limit.
A higher resolution profile shows that the boundary
was a magnetic hole (a small-scale structure in which
the magnetic field strength is low and across which
the total pressure was approximately constant), which
is not unusual at magnetic clouds [see, e.g., Burlaga,
1995]. If one takes the beginning and end times of
the magnetic hole at 18:51:25.5 UT and 19:01:04.5 UT,
respectively, the magnetic field direction rotated
through 2220 in
a plane. A minimum variance analysis using the unnormalized
magnetic field vectors shows that the normal to this
plane had the direction (
n =
230.30,
n = 1.70).
Recall that the axis of the magnetic cloud was approximately (
c
= 2910,
n = -100),
so that the angle
between the normal to the front boundary of the magnetic
cloud and its axis was approximately 60S0. The component of the magnetic
field normal to the plane of rotation of the field
at the front boundary is 0.09 nT
0.40 nT
(two sigma uncertainty), consistent with
zero, which is additional evidence that the boundary
was a tangential discontinuity.
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