Fullwave simulations of ICRF heating regimes in toroidal plasmas with nonMaxwellian distribution functions
Abstract
At the power levels required for significant heating and current drive in magneticallyconfined toroidal plasma, modification of the particle distribution function from a Maxwellian shape is likely [T. H. Stix, Nucl. Fusion, 15 737 (1975)], with consequent changes in wave propagation and in the location and amount of absorption. In order to study these effects computationally, both the finiteLarmorradius and the highharmonic fast wave (HHFW), versions of the fullwave, hotplasma toroidal simulation code TORIC [M. Brambilla, Plasma Phys. Control. Fusion 41, 1 (1999) and M. Brambilla, Plasma Phys. Control. Fusion 44, 2423 (2002)], have been extended to allow the prescription of arbitrary velocity distributions of the form f(v, v_perp, psi , theta). For hydrogen (H) minority heating of a deuterium (D) plasma with anisotropic Maxwellian H distributions, the fractional H absorption varies significantly with changes in parallel temperature but is essentially independent of perpendicular temperature. On the other hand, for HHFW regime with anisotropic Maxwellian fast ion distribution, the fractional beam ion absorption varies mainly with changes in the perpendicular temperature. The evaluation of the wavefield and power absorption, through the full wave solver, with the ion distribution function provided by either aMonteCarlo particle and FokkerPlanck codes is also examinedmore »
 Authors:

 Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
 Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
 Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States). Plasma Science and Fusion Center
 XCEL Engineering Inc., 1066 Commerce Park Drive, Oak Ridge, TN 37830, United States of America
 Publication Date:
 DOE Contract Number:
 AC02CH0911466; FC0201ER54648
 Product Type:
 Dataset
 Research Org.:
 Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States); Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
 Sponsoring Org.:
 USDOE Office of Science (SC), Fusion Energy Sciences (FES)
 Subject:
 70 PLASMA PHYSICS AND FUSION TECHNOLOGY
 Keywords:
 NSTXU
 OSTI Identifier:
 1356364
 DOI:
 10.11578/1356364
Citation Formats
Bertelli, N., Valeo, E.J., Green, D.L., Gorelenkova, M., Phillips, C.K., Podesta, M., Lee, J.P., Wright, J.C., and Jaeger, E.F. Fullwave simulations of ICRF heating regimes in toroidal plasmas with nonMaxwellian distribution functions. United States: N. p., 2017.
Web. doi:10.11578/1356364.
Bertelli, N., Valeo, E.J., Green, D.L., Gorelenkova, M., Phillips, C.K., Podesta, M., Lee, J.P., Wright, J.C., & Jaeger, E.F. Fullwave simulations of ICRF heating regimes in toroidal plasmas with nonMaxwellian distribution functions. United States. doi:10.11578/1356364.
Bertelli, N., Valeo, E.J., Green, D.L., Gorelenkova, M., Phillips, C.K., Podesta, M., Lee, J.P., Wright, J.C., and Jaeger, E.F. 2017.
"Fullwave simulations of ICRF heating regimes in toroidal plasmas with nonMaxwellian distribution functions". United States. doi:10.11578/1356364. https://www.osti.gov/servlets/purl/1356364. Pub date:Mon May 01 00:00:00 EDT 2017
@article{osti_1356364,
title = {Fullwave simulations of ICRF heating regimes in toroidal plasmas with nonMaxwellian distribution functions},
author = {Bertelli, N. and Valeo, E.J. and Green, D.L. and Gorelenkova, M. and Phillips, C.K. and Podesta, M. and Lee, J.P. and Wright, J.C. and Jaeger, E.F.},
abstractNote = {At the power levels required for significant heating and current drive in magneticallyconfined toroidal plasma, modification of the particle distribution function from a Maxwellian shape is likely [T. H. Stix, Nucl. Fusion, 15 737 (1975)], with consequent changes in wave propagation and in the location and amount of absorption. In order to study these effects computationally, both the finiteLarmorradius and the highharmonic fast wave (HHFW), versions of the fullwave, hotplasma toroidal simulation code TORIC [M. Brambilla, Plasma Phys. Control. Fusion 41, 1 (1999) and M. Brambilla, Plasma Phys. Control. Fusion 44, 2423 (2002)], have been extended to allow the prescription of arbitrary velocity distributions of the form f(v, v_perp, psi , theta). For hydrogen (H) minority heating of a deuterium (D) plasma with anisotropic Maxwellian H distributions, the fractional H absorption varies significantly with changes in parallel temperature but is essentially independent of perpendicular temperature. On the other hand, for HHFW regime with anisotropic Maxwellian fast ion distribution, the fractional beam ion absorption varies mainly with changes in the perpendicular temperature. The evaluation of the wavefield and power absorption, through the full wave solver, with the ion distribution function provided by either aMonteCarlo particle and FokkerPlanck codes is also examined for Alcator CMod and NSTX plasmas. NonMaxwellian effects generally tends to increase the absorption with respect to the equivalent Maxwellian distribution.},
doi = {10.11578/1356364},
journal = {},
number = ,
volume = ,
place = {United States},
year = {2017},
month = {5}
}
Works referencing / citing this record:
Fullwave simulations of ICRF heating regimes in toroidal plasma with nonMaxwellian distribution functions
journal, April 2017
 Bertelli, N.; Valeo, E. J.; Green, D. L.
 Nuclear Fusion, Vol. 57, Issue 5, Article No. 056035
Fullwave simulations of ICRF heating regimes in toroidal plasma with nonMaxwellian distribution functions
journal, April 2017
 Bertelli, N.; Valeo, E. J.; Green, D. L.
 Nuclear Fusion, Vol. 57, Issue 5, Article No. 056035