TY - JOUR
T1 - Ion and electron heating characteristics of magnetic reconnection in tokamak plasma merging experiments
AU - Ono, Y.
AU - Tanabe, H.
AU - Yamada, T.
AU - Inomoto, M.
AU - Ii, T.
AU - Inoue, S.
AU - Gi, K.
AU - Watanabe, T.
AU - Gryaznevich, M.
AU - Scannell, R.
AU - Michael, C.
AU - Cheng, C. Z.
PY - 2012/12
Y1 - 2012/12
N2 - Recently, the TS-3 and TS-4 tokamak merging experiments revealed significant plasma heating during magnetic reconnection. A key question is how and where ions and electrons are heated during magnetic reconnection. Two-dimensional measurements of ion and electron temperatures and plasma flow made clear that electrons are heated inside the current sheet mainly by the Ohmic heating and ions are heated in the downstream areas mainly by the reconnection outflows. The outflow kinetic energy is thermalized by the fast shock formation and viscous damping. The magnetic reconnection converts the reconnecting magnetic field energy mostly to the ion thermal energy in the outflow region whose size is much larger than the current sheet size for electron heating. The ion heating energy is proportional to the square of the reconnection magnetic field component B2p.This scaling of reconnection heatingindicates the significant ion heating effect of magnetic reconnection, which leads to a new high-field reconnection heating experiment for fusion plasmas.
AB - Recently, the TS-3 and TS-4 tokamak merging experiments revealed significant plasma heating during magnetic reconnection. A key question is how and where ions and electrons are heated during magnetic reconnection. Two-dimensional measurements of ion and electron temperatures and plasma flow made clear that electrons are heated inside the current sheet mainly by the Ohmic heating and ions are heated in the downstream areas mainly by the reconnection outflows. The outflow kinetic energy is thermalized by the fast shock formation and viscous damping. The magnetic reconnection converts the reconnecting magnetic field energy mostly to the ion thermal energy in the outflow region whose size is much larger than the current sheet size for electron heating. The ion heating energy is proportional to the square of the reconnection magnetic field component B2p.This scaling of reconnection heatingindicates the significant ion heating effect of magnetic reconnection, which leads to a new high-field reconnection heating experiment for fusion plasmas.
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U2 - 10.1088/0741-3335/54/12/124039
DO - 10.1088/0741-3335/54/12/124039
M3 - Article
AN - SCOPUS:84870185791
SN - 0741-3335
VL - 54
JO - Plasma Physics and Controlled Fusion
JF - Plasma Physics and Controlled Fusion
IS - 12
M1 - 124039
ER -