TY - GEN
T1 - 3d magnetic reconnection
AU - Parnell, Clare E.
AU - Maclean, Rhona C.
AU - Haynes, Andrew L.
AU - Galsgaard, Klaus
PY - 2010/6/1
Y1 - 2010/6/1
N2 - Magnetic reconnection is an important process that is prevalent in a wide range of astrophysical bodies. It is the mechanism that permits magnetic fields to relax to a lower energy state through the global restructuring of the magnetic field and is thus associated with a range of dynamic phenomena such as solar flares and CMEs. The characteristics of threedimensional reconnection are reviewed revealing how much more diverse it is than reconnection in two dimensions. For instance, three-dimensional reconnection can occur both in the vicinity of null points, as well as in the absence of them. It occurs continuously and continually throughout a diffusion volume, as opposed to at a single point, as it does in two dimensions. This means that in three-dimensions field lines do not reconnect in pairs of lines making the visualisation and interpretation of three-dimensional reconnection difficult. By considering particular numerical 3D magnetohydrodynamic models of reconnection, we consider how magnetic reconnection can lead to complex magnetic topologies and current sheet formation. Indeed, it has been found that even simple interactions, such as the emergence of a flux tube, can naturally give rise to 'turbulent-like' reconnection regions.
AB - Magnetic reconnection is an important process that is prevalent in a wide range of astrophysical bodies. It is the mechanism that permits magnetic fields to relax to a lower energy state through the global restructuring of the magnetic field and is thus associated with a range of dynamic phenomena such as solar flares and CMEs. The characteristics of threedimensional reconnection are reviewed revealing how much more diverse it is than reconnection in two dimensions. For instance, three-dimensional reconnection can occur both in the vicinity of null points, as well as in the absence of them. It occurs continuously and continually throughout a diffusion volume, as opposed to at a single point, as it does in two dimensions. This means that in three-dimensions field lines do not reconnect in pairs of lines making the visualisation and interpretation of three-dimensional reconnection difficult. By considering particular numerical 3D magnetohydrodynamic models of reconnection, we consider how magnetic reconnection can lead to complex magnetic topologies and current sheet formation. Indeed, it has been found that even simple interactions, such as the emergence of a flux tube, can naturally give rise to 'turbulent-like' reconnection regions.
KW - (magnetohydrodynamics:) MHD
KW - Magnetic fields
UR - http://www.scopus.com/inward/record.url?scp=84861926552&partnerID=8YFLogxK
U2 - 10.1017/S1743921311017650
DO - 10.1017/S1743921311017650
M3 - Conference contribution
AN - SCOPUS:84861926552
SN - 9780521197397
T3 - Proceedings of the International Astronomical Union
SP - 227
EP - 238
BT - Astrophysical Dynamics
ER -