SLM 2/29/2000 WAH 13 Mar 2002 1 NBI Driven Neoclassical Effects W. A. Houlberg ORNL K.C. Shaing, J.D. Callen U. Wis-Madison NSTX Meeting 25 March 2002.

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SLM 2/29/2000 WAH 13 Mar NBI Driven Neoclassical Effects W. A. Houlberg ORNL K.C. Shaing, J.D. Callen U. Wis-Madison NSTX Meeting 25 March 2002 Princeton, New Jersey

SLM 2/29/2000 WAH 13 Mar NBI Forces on Thermal Species Drive Particle and Heat Fluxes and Viscous Heating Unbalanced neutral beam injection can influence the interpretation of the particle and ion power balances through: –Thermal-NBI friction –Viscous heating –Thermal-NBI heat friction (needs evaluation) The NBI friction and viscous heating effects alone can exceed standard ion neoclassical heat conduction (e.g., works of Stacey, Hinton) The NBI heat friction was estimated by Callen in 1974 to have an influence comparable to the NBI friction, and therefore needs to be revisited Note that NBI heat friction on electrons a major contributor to the electron shielding current in NBCD More thorough quantitative analyses of these NBI effects are suggested when ion turbulence is suppressed: –NSTX negative effective ion thermal conductivity with co-NBI –Observations of ion thermal conductivity below standard neoclassical in ITBs

SLM 2/29/2000 WAH 13 Mar Neoclassical Parallel Force Balances with NBI Hirshman and Sigmar, Nucl. Fusion 21 (1981) 1079 Houlberg, Shaing, Hirshman and Zarnstorff, Phys. Plasmas 4 (1997) 3230 Parallel momentum and heat force balance equations for species j: Classical parallel friction forces between thermal particles: Neoclassical parallel viscous forces: ViscousOhmic Beam Friction Thermal Friction Function of parallel flows of all species Function of poloidal flows of own species

SLM 2/29/2000 WAH 13 Mar Neoclassical Particle and Heat Fluxes with NBI The banana plateau fluxes are related to the poloidal flows: –Importance relative to standard neoclassical is governed by the ratio of induced poloidal flows The Pfirsch-Schlüter fluxes are related directly to the forces: –Importance relative to standard neoclassical governed by the ratio of forces All of the NBI terms are outward with co-injection, inward with counter- injection (testable by co-/counter-NBI comparisons)

SLM 2/29/2000 WAH 13 Mar The Radial Force Balances with NBI Radial force balance equations: NBI effects on poloidal rotation should be considered when: –Determining the radial electric field using the radial force balance with theoretical models for the poloidal rotation –Comparing measured poloidal rotation with theoretical models

SLM 2/29/2000 WAH 13 Mar Viscous Heating with NBI The neoclassical viscous heating is enhanced as the square of the poloidal flow velocities: In addition to this are heating terms from classical (small) and toroidal viscosity (e.g., Stacey’s gyroviscosity, turbulence induced viscosity, …) Viscous heating is likely important for: –ITBs with strong pressure gradients –Strong toroidal rotation

SLM 2/29/2000 WAH 13 Mar Summary of NBI Driven Neoclassical Effects There is an extensive literature on the theory for NBI driven neoclassical fluxes and viscous heating Various of these analyses have shown the effects are comparable to the standard neoclassical effects Much of that literature considers individual effects and approximations that can be treated more comprehensively These effects should be most visible in experiments with unbalanced NBI when turbulence induced transport is suppressed –NSTX cases where negative effective ion thermal conductivity is inferred –DIII-D QDB plasmas –ITBs The primary work for a quantitative study would be to evaluate the parallel NBI friction and heat friction in an NBI package (only the toroidal torque is presently evaluated in TRANSP and other codes)

SLM 2/29/2000 WAH 13 Mar A Selection of References on NBI Driven Effects Introductory assessment including momentum and heat flux torques: J.D. Callen, et al, “Neutral beam injection into tokamaks,” 5 th IAEA, Tokyo (1974), Vol 1, 645 Momentum torque and viscous heating: S.P. Hirshman, D.J. Sigmar, “Neoclassical transport of impurities in tokamak plasmas,” Nucl. Fusion 21 (1981) 1079 W.M. Stacey, Jr., “The effects of neutral beam injection on impurity transport in tokamaks,” Phys. Fluids 27 (1984) 2076 W.M. Stacey, Jr., “Rotation and Impurity Transport in a tokamak plasma with directed neutral- beam injection,” Nucl. Fusion 25 (1985) 463 W.M. Stacey, Jr., “Convective and viscous fluxes in strongly rotating tokamak plasmas,” Nucl. Fusion 30 (1990) 2453 W.M. Stacey, Jr., “Poloidal rotation and density asymmetries in a tokamak plasma with strong toroidal rotation,” Phys. Fluids B 4 (1992) 3302 F.L. Hinton, Y.-B. Kim, “Effects of neutral beam injection on poloidal rotation and energy transport in tokamaks,” Phys. Fluids B 5 (1993) 3012 W.M. Stacey, “Comments on ‘Effects of neutral beam injection on poloidal rotation and energy transport in tokamaks,’ ” Phys. Fluids B 5 (1993) 4505 Momentum and heat flux torques included in formal development of equations (no applications): J.P. Wang, et al, “Momentum and heat friction forces between fast ions and thermal plasma species,” Nucl. Fusion 34 (1994) 231 W.A. Houlberg, et al, “Bootstrap current and neoclassical transport in tokamaks of arbitrary collisionality and aspect ratio,” Phys. Plasmas 4 (1997) 3230