TY - JOUR
T1 - Momentum losses by charge exchange with neutral particles in H-mode discharges at JET
AU - Versloot, T. W.
AU - de Vries, P. C.
AU - Giroud, C.
AU - Brix, M.
AU - von Hellermann, M. G.
AU - Lomas, P. J.
AU - Moulton, D.
AU - O'Mullane, M.
AU - Nunes, I. M.
AU - Salmi, Antti
AU - Tala, Tuomas
AU - Voitsekhovitch, I.
AU - Zastrow, K.-D.
AU - JET-EFDA contributors
PY - 2011
Y1 - 2011
N2 - The effect of a neutral density background on the toroidal angular
momentum and kinetic energy profiles has been investigated in JET. Under
equivalent conditions but with increasing gas fuelling during the flat
top phase, it has been observed that both the edge rotation and
temperature decrease. The increase in electron density was not
sufficient to compensate the rotation and temperature loss such that
both energy and momentum confinement times are significantly reduced.
The edge localized mode behaviour is observed to be significantly
affected by the increased neutral influx. A simple 1.5D fluid model has
been used to qualitative capture the neutral transport response within
the plasma, followed by a forward model of the passive charge-exchange
(CX) emission of carbon to obtain a corrected radial neutral density
profile. It has been found that the neutral density is sharply
attenuated over the edge region, with similar edge magnitudes in both
the non-fuelled (Γ0/ne ~ 1.2 m s−1) and maximum fuelled case (Γ0/ne ~ 2.5 m s−1). Discharges with reversed-B
operation exhibited even higher normalized neutral fluxes related to
first orbit effects and increased wall interactions. Over the full
neutral influx range, a decrease in pedestal thermal Mach number from
0.25 to 0.14 was observed. Increased neutral penetration up to the
pedestal top (r/a ~ 0.9) due to multiple CX interactions
is obtained from the interpretive model. Under these multiple
neutral–ion interactions, the impact on the CX loss of angular momentum
is larger compared with the CX energy loss. The drag torque was seen to
increase up to 10% of the total applied torque, while energy losses
appeared to be smaller. The accuracy of this global approach method is
unfortunately limited; however, the estimated momentum sink was found
comparable to the torque required to explain the discrepancy between
observed global energy and momentum confinement.
AB - The effect of a neutral density background on the toroidal angular
momentum and kinetic energy profiles has been investigated in JET. Under
equivalent conditions but with increasing gas fuelling during the flat
top phase, it has been observed that both the edge rotation and
temperature decrease. The increase in electron density was not
sufficient to compensate the rotation and temperature loss such that
both energy and momentum confinement times are significantly reduced.
The edge localized mode behaviour is observed to be significantly
affected by the increased neutral influx. A simple 1.5D fluid model has
been used to qualitative capture the neutral transport response within
the plasma, followed by a forward model of the passive charge-exchange
(CX) emission of carbon to obtain a corrected radial neutral density
profile. It has been found that the neutral density is sharply
attenuated over the edge region, with similar edge magnitudes in both
the non-fuelled (Γ0/ne ~ 1.2 m s−1) and maximum fuelled case (Γ0/ne ~ 2.5 m s−1). Discharges with reversed-B
operation exhibited even higher normalized neutral fluxes related to
first orbit effects and increased wall interactions. Over the full
neutral influx range, a decrease in pedestal thermal Mach number from
0.25 to 0.14 was observed. Increased neutral penetration up to the
pedestal top (r/a ~ 0.9) due to multiple CX interactions
is obtained from the interpretive model. Under these multiple
neutral–ion interactions, the impact on the CX loss of angular momentum
is larger compared with the CX energy loss. The drag torque was seen to
increase up to 10% of the total applied torque, while energy losses
appeared to be smaller. The accuracy of this global approach method is
unfortunately limited; however, the estimated momentum sink was found
comparable to the torque required to explain the discrepancy between
observed global energy and momentum confinement.
U2 - 10.1088/0741-3335/53/6/065017
DO - 10.1088/0741-3335/53/6/065017
M3 - Article
SN - 0741-3335
VL - 53
JO - Plasma Physics and Controlled Fusion
JF - Plasma Physics and Controlled Fusion
IS - 6
M1 - 065017
ER -