Progress on Optimization Results for Steady-State Plasma Solutions

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Progress on Optimization Results for Steady-State Plasma Solutions A.D. Turnbull, H. St John, R. Buttery, M. Choi, L.L Lao, S. Smith General Atomics ARIES Team Meeting Gaithersburg Md May 31 June 1 2012

Previous Progress Through January 2012: Profiles Collapsed Using GLF23 Transport Model GLF23 Model predicted collapse of standard ARIES ACT1B scenario: - EPED1 pedestal model incorporated in profiles consistent with model for peeling-ballooning stability - Collapse could only be avoided with an increase in density by a factor 80% o Collapse apparently due to large transport flux in outer part o Transport resulted in edge collapse to boundary condition value which then propagated inward - Collapse appears to be a feature of alpha-heated scenarios TGLF model with real geometry was much more optimistic: - Collapse avoided with small peaking of density: - Appears to better represent the transport in the strongly shaped outer region - Issue with TGLF is it is extremely slow compared to GLF23 Proposed to implement Multi-Mode model: - Claimed to be as high fidelity as TGLF but an order of magnitude faster

Progress Made in Implementing Planned Self Consistent Simulation for ARIES-AT Baseline Implemented Multi-Mode Gyrofluid transport Model: - Ten times slower than GLF23 but ten times faster than TGLF Main Result: - Successful simulation of ARIES base case to steady state o No collapse - Two cases considered with different density: o For n e = 1.67 x 10 20 m -3 P DT = 1.1 GW and Q DT = 28.7 o For n e = 1.78 x 10 20 m -3 P DT = 1.5 GW and Q DT = 39.7 - Major issue with considerable evolution of q profile: o Axis temperature overheats causing large on-axis current density despite small residual steady-state electric field o q 0 drops well below unity and is probably unstable o Requires large RF current drive on axis to maintain q 0 > 1 Future plans: - Eliminate overheating of axis temperatures and excess axis current density - Evolve to steady state - Iterate using steady state as new starting equilibrium

Two Cases Considered With Different Line Averaged Density Obtained by Varying Broadness Axis density kept fixed at standard density value but line averaged value is varied: n e =1.67 10 20 m 3 and n e =1.78 10 20 m 3

Electron and Ion Species Temperatures Evolved According to Multi-Mode Species Transport Coefficients Profiles initialized with T e = T i and species evolved separately to steady state with Multi-Mode model Initial temperature profiles Density profiles fixed in time in these simulations

Multi-Mode Theory-based Anomalous Transport Model Predicts Temperature, Density and Rotation Profiles ONETWO transport code evolves temperatures and densities for each individual species s under heat and particle diffusion and sources: ( ) t n s T s n s t = ( D 1 s n s T s ) + ν 1 1 ( s n s T s ) + S s = ( D 2 s n s ) + ν 2 2 ( s n s ) + S s Multi-mode calculates particle diffusion, D 1,2, heat convection ν 1,2, and sources S 1,2 from: - Weiland model for ITG, TEM, and MHD modes: J. Weiland, Plasma Physics. Institute of Physics Publishing, 2000 - Drift-resistive-inertial ballooning modes (DRIBM): T. Rafiq, et al., Physics of Plasmas, 17 082511, 2010 - Horton model for short wavelength ETG anomalous transport with threshold obtained from Jenko threshold: W. Horton, et al.,, Physics of Plasmas, vol. 7, no. 5, pp. 1494 1510, 2000 F. Jenko, et al. Physics of Plasmas, 8, 4096 4104, 2001

Temperatures Evolved to Steady State for Both Density Cases Without Collapse Both cases overheat core electron temperature: - High T e leads to other issues

Steady State Electron Temperatures Above 40 kev While Profile Integrity Maintained to Edge Boundary Condition Slight mismatch at edge boundary condition: - Can probably be eliminated on further iterations

Comparison of Steady State Fluxes With GLF23 Shows Multi-Mode Has Much Reduced Flux in Outer Region Both species fluxes outside r/a = 0.6 are reduced by almost an order of magnitude

Electron Transport in GLF23 Simulations Showed Apparently Large Trapped Electron Mode Contribution TEM is believed to be dominant non-etg contribution: - GLF23 does not further isolate individual contributions

Diagnosis of Transport Shows ETG as Dominant Electron Transport Mechanism in Multi-Mode Model Trapped electron mode contribution is smaller than but comparable to ETG transport: - Included in Weiland electron transport model

Diagnosis of Ion Transport Shows ITG Modes Contained in Weiland Model is Largest Contribution Drift ballooning modes are also significant: - These are not included in GLF23 or TGLF

Evolution to Steady State with Small Residual Electric Field (~ µv) Flat electric field profile indicates steady state: B t = E ψ t = re φ + V loop

Safety Factor on Axis Evolves to a Value Below Unity Even With Small Residual Electric Field Likely to be unstable to internal kink modes: - Expected sawtoothing discharge High axis T e implies local current density can be large: j ~ E 0 η ~ E 0 T e 3 2

Current Density Requires Further Iteration to Remove Residual Ohmic Contribution With Moderate RF Power Large local axis RF driven current is required to eliminate Ohmic axis current density: n e =1.67 10 20 m 3 I RF = 2.6MA n e =1.78 10 20 m 3 I RF = 2.5MA I Boot = 4.9MA I Ohm = 3.1MA I Boot = 6.6MA I Ohm =1.4MA

Multi-Mode Transport Package Implemented in ONETWO Code First iteration finds reasonable steady state solutions: - Ten times faster than TGLF model - Profile collapse found with GLF23 is avoided Future Steps Benchmark solution with previous successful TGLF simulation Eliminate axis overheating and excess axis current density: - May or may not be a bug in implementation of Multi-mode model - May resort to pellet fuelling to maintain axis density and simultaneously suppress overheating in the core Evolve to steady state: - GENRAY calculation of current drive needed to maintain profiles Iterate using steady state as new starting equilibrium: - Transport coefficients are based on initial equilibrium - Need to be updated to reflect quite different steady state profiles - Then evolved to new steady state - Further iteration may be necessary

Backup Slides

Summary Data: n e = 1.67 x 10 20 m -3 Minor radius a (cm): 139.9 b/a: 2.29 Nominal Rmajor (cm): 550.0 R at geom. cent. (cm): 548.2 R at mag. axis (cm): 580.1 Z at mag. axis (cm): 0.0 Volume (cm**3): 4.22E+08 Pol. circum. (cm): 1519.0 surface area (cm**2): 4.90E+06 cross. sect area: 1.28E+05 Bt (G): 5.54E+04 Ip (A): 1.06E+07 Bt at Rgeom (G): 5.56E+04 r(q = 1)/a: 0.40 Line-avg den (1/cm**3): 1.85E+14 Tau-particle-dt (s): 2.000 profiles ucenter uedge ucen/uav elec. den. (1/cm**3): 1.96E+14 7.95E+13 1.38 elec. temp. (kev): 42.94 0.02 2.89 ion temp. (kev): 24.55 0.02 2.16 current (A/cm**2): 584.16 3.92 6.73 Zeff: 1.27 1.44 0.97 q: 0.24 14.36 q* at edge: 4.29 ang. speed (1/sec): 9.00E+01 1.00E+00 1.86E+00

Summary Data: n e = 1.67 x 10 20 m -3 exper. code Surface voltage : 0.00 0.01 Volts Average voltage : 0.00 0.00 Volts Ohmic power: 0.00E+00 1.86E+04 Watts Beam power-torus: 0.00E+00 0.00E+00 Watts Neutron rate D(D,N): 0.00E+00 1.14E+18 #/s Computed quantities Beam power elec. (W): 0.00E+00 ke at a/2 (1/cm-s): 1.08E+18 Beam power ions (W): 0.00E+00 ki at a/2 (1/cm-s): 2.57E+18 Beam power cx loss (W): 0.00E+00 ki/kineo at a/2: 98.77 Shinethrough (%): 0.00 chi electrons at a/2: 6.59E+03 RF power absorbed: 3.83E+07 chi ions at a/2: 1.73E+04 Radiated power (W): 6.67E+07 r*/a: Te = (Te(0)+Te(a))/2 0.46 Brems prim ions (W): 2.26E+07 Brems imp ions : 4.39E+07 Poloidal B field (G): 8.77E+03 Beta-poloidal: 2.400 beam torque (nt-m) 0.00E+00 total torque (nt-m): -3.05E-03 stored ang mtm (kg*m2/s): 4.39E-01 momt inertia (kg*m**2): 7.15E-03 kinetic energy of rotation (j) : 2.00E+01

Summary Data: n e = 1.67 x 10 20 m -3 electrons ions thermal total Stored Energy (J) 2.451E+08 1.667E+08 4.117E+08 4.684E+08 de/dt (W): 6.596E+03-1.192E-06 6.596E+03 6.596E+03 Input power (W): 1.819E+08 2.568E+08 2.568E+08 Energy conf. time (s): 1.3471 1.6033 1.8239 H(89p) = 2.61 H(89pm) = 3.03 H_ITER98y2 = 1.26 H_Petty = 0.80 Beta-toroidal volume-avg center electrons: 3.147E-02 1.097E-01 ions: 2.140E-02 5.583E-02 beam: 0.000E+00 0.000E+00 alphas: 7.274E-03 4.345E-02 total: 6.014E-02 2.090E-01 Normalized beta 4.413E+00 total power input (W) = 3.831E+07 time = 1.0000E+06 Itot = 1.06E+07 Iohm = 3.08E+06 Iboot = 4.89E+06 Ibeam = 0.00E+00 Irf = 2.63E+06 genray cd,amps qe,watts qi, watts 2.632E+06 3.804E+07 2.548E+05 QDD = 0.03 QDT = 28.67 QTT = 0.05 P DD = 1.2772E+06 P DT = 1.0986E+09 P TT = 2.0263E+06 W D(D,n) = 1.1365E+18 D(T,n) = 3.8966E+20 T(T,2n) = 1.1194E+18 #/sec paux (MW) = 3.83E+01 palpha = 2.18E+02 prad = 6.67E+01 Ptransport = 1.90E+02

Summary Data: n e = 1.78 x 10 20 m -3 Minor radius a (cm): 139.9 b/a: 2.29 Nominal Rmajor (cm): 550.0 R at geom. cent. (cm): 548.2 R at mag. axis (cm): 580.1 Z at mag. axis (cm): 0.0 Volume (cm**3): 4.22E+08 Pol. circum. (cm): 1519.0 surface area (cm**2): 4.90E+06 cross. sect area: 1.28E+05 Bt (G): 5.54E+04 Ip (A): 1.06E+07 Bt at Rgeom (G): 5.56E+04 r(q = 1)/a: 0.07 Line-avg den (1/cm**3): 1.90E+14 Tau-particle-dt (s): 2.000 profiles ucenter uedge ucen/uav elec. den. (1/cm**3): 1.97E+14 7.95E+13 1.27 elec. temp. (kev): 47.48 0.02 2.85 ion temp. (kev): 27.24 0.02 2.17 current (A/cm**2): 239.33 3.91 2.76 Zeff: 1.28 1.44 0.98 q: 0.59 14.36 q* at edge: 4.29 ang. speed (1/sec): 9.00E+01 1.00E+00 1.86E+00

Summary Data: n e = 1.78 x 10 20 m -3 exper. code Surface voltage : 0.00 0.00 Volts Average voltage : 0.00 0.00 Volts Ohmic power: 0.00E+00 2.83E+03 Watts Beam power-torus: 0.00E+00 0.00E+00 Watts Neutron rate D(D,N): 0.00E+00 1.63E+18 #/s computed quantities Beam power elec. (W): 0.00E+00 ke at a/2 (1/cm-s): 1.34E+18 Beam power ions (W): 0.00E+00 ki at a/2 (1/cm-s): 2.84E+18 Beam power cx loss (W): 0.00E+00 ki/kineo at a/2: 49.26 Shinethrough (%): 0.00 chi electrons at a/2: 6.96E+03 RF power absorbed: 3.86E+07 chi ions at a/2: 1.62E+04 Radiated power (W): 7.35E+07 r*/a: Te = (Te(0)+Te(a))/2 0.46 Brems prim ions (W): 2.90E+07 Brems imp ions : 4.43E+07 Poloidal B field (G): 8.77E+03 Beta-poloidal: 2.987 beam torque (nt-m) 0.00E+00 total torque (nt-m): -3.35E-03 stored ang mtm (kg*m2/s): 4.87E-01 momt inertia (kg*m**2): 7.84E-03 kinetic energy of rotation (j) : 2.20E+01

Summary Data: n e = 1.78 x 10 20 m -3 electrons ions thermal total Stored Energy (J) 3.017E+08 2.021E+08 5.038E+08 5.829E+08 de/dt (W): 1.263E+04-3.576E-06 1.263E+04 1.263E+04 Input power (W): 2.350E+08 3.435E+08 3.435E+08 Energy conf. time (s): 1.2838 1.4666 1.6969 H(89p) = 2.80 H(89pm) = 3.15 H_ITER98y2 = 1.37 H_Petty = 0.83 Beta-toroidal volume-avg center electrons: 3.873E-02 1.220E-01 ions: 2.595E-02 6.194E-02 beam: 0.000E+00 0.000E+00 alphas: 1.016E-02 5.235E-02 total: 7.484E-02 2.363E-01 Normalized beta 5.491E+00 total power input (W) = 3.862E+07 time = 1.0000E+06 Itot = 1.06E+07 Iohm = 1.46E+06 Iboot = 6.61E+06 Ibeam = 0.00E+00 Irf = 2.53E+06 cd,amps qe,watts qi, watts genray 2.534E+06 3.847E+07 1.493E+05 QDD = 0.05 QDT = 39.69 QTT = 0.07 P DD = 1.8286E+06 P DT = 1.5331E+09 P TT = 2.8514E+06 W D(D,n) = 1.6310E+18 D(T,n) = 5.4373E+20 T(T,2n) = 1.5751E+18 #/sec paux (MW) = 3.86E+01 palpha = 3.05E+02 prad = 7.35E+01 Ptransport = 2.70E+02