RAPTOR Exercise 1: Ramp-up current diffusion with varying heating
In this exercise you will test the effect of differently timed heating during a plasma current ramp.
Contents
ITER simulation setup
First we set up the RAPTOR simulation.
clear run ../../RAPTOR_path.m % load the default parameters for ITER config = RAPTOR_config('ITER'); % load default params config.grid.tgrid = [0:0.1:1,3:2:140]; % tranport model: choose empirical model with % transport reduction at low shear. config.chi_e = chi_e('FF'); config.chi_e.params.cano = 4; config.chi_e.params.cneo = 0.1; % Heating actuators: EC and NBI config.nbhcd = nbhcd('nbhcd_gaussian'); config.nbhcd.params.active = true; config.nbhcd.params.rdep = [0.26]; % config.nbhcd.params.wdep = [0.15]; % broad heating config.nbhcd.params.wdep_out = [0.75]; % broad heating config.nbhcd.params.cd_eff = [5]; % current drive config.nbhcd.params.uindices = [2];% index in input vector config.echcd = echcd('echcd_gaussian'); config.echcd.params.active = true; config.echcd.params.rdep = [0.2 0.4 0.55 ]; % two actuators, set rdep=0 for first, rdep=0.4 for second config.echcd.params.wdep = [.05 .05 .05 ]; % wdep =0.35 for each config.echcd.params.cd_eff = [10 10 10]; % current drive efficiency factor: pure ECH for first, co-ECCD for second config.echcd.params.uindices = [3 4 5]; % index of power for each actuator in input vector % radiation modules etc config.prad.active = false; config.pei.active = true; config.palpha.active = false; [~,model,params,init] = RAPTOR_config(config); % generate model structure for these params. params.debug.iterdisp = 10; % display every 10 % Plasma current ramp rampfun = @(t,tmin,ymin,tmax,ymax) max(ymin,min((ymax-ymin)/(tmax-tmin)*(t-tmin),ymax-ymin)+ymin); % anonymous function for ramps U(1,:) = rampfun(params.tgrid.tgrid,0,4e6,100,12e6); % input Ip trace U(2,:) = zeros(size(U(1,:))); % placeholder, will replace this with heating later. U(3,:) = zeros(size(U(1,:))); % placeholder, will replace this with heating later. U(4,:) = zeros(size(U(1,:))); % placeholder, will replace this with heating later. U(5,:) = zeros(size(U(1,:))); % placeholder, will replace this with heating later. % initial conditions init.te0 = 2e3; init.ne0 = 1e19; [x0,g0,v0] = RAPTOR_initial_conditions(U(1),model,init); % Define the initial condition v0 = v0*ones(1,params.tgrid.nt); % specify density ramp: multiply initial profile by ne0(t) negauss = model.te.LamTegauss*v0(model.ne.ind,1); ne0 = rampfun(params.tgrid.tgrid,0,1,100,5); negauss_varying = negauss*ne0; v0(model.ne.ind,:) = model.te.LamTegauss \ negauss_varying; v0(model.ni.ind,:) = 0.9*v0(model.ne.ind,:); % Run the simulation simres = RAPTOR_predictive(x0,g0,v0,U,model,params); out = RAPTOR_out(simres,model,params); RAPTOR_plot_GUI(out);
Loading default configuration for ITER
loading CHEASE equilibrium from /Users/ffelici/Dropbox/4K480 - Dropbox/Exercises/Week7/RAPTOR_exercise/chease_equils/ITER_hybrid_citrin_equil_cheasedata
Scaling Te initial condition to match edge value boundary value (200)
istep telaps newt res t[ s] dt[ s] Ip[MA] Icd[MA] Ibs[MA] Ioh[MA] qe qmin q0 Vl[V] Te0[keV] ne0[e19] Wi[MJ] We[MJ] f_ss
1 0.03 4 1.2e-10 0 0.1 4 0 0.0559 3.95 14.7 3.68 3.68 6.6e-01 1.58 1.00 22.69 0.57 9.2e+00
11 0.26 3 1.9e-10 1 2 4.08 0 0.0358 4.05 14.5 2.6 2.6 1.3e+00 1.17 1.04 24.41 0.46 4.3e+00
21 0.46 2 9.5e-11 21 2 5.68 0 0.0535 5.63 10.4 1.2 1.2 1.5e+00 1.56 1.84 53.82 0.97 3.4e+00
31 0.64 2 4.6e-11 41 2 7.28 0 0.0713 7.21 8.1 0.851 0.851 1.5e+00 1.88 2.64 95.55 1.63 3.5e+00
41 0.81 2 5.3e-11 61 2 8.88 0 0.0883 8.8 6.64 0.657 0.657 1.6e+00 2.16 3.44 149.89 2.41 3.5e+00
51 1 2 5.5e-11 81 2 10.5 0 0.104 10.4 5.63 0.533 0.533 1.6e+00 2.43 4.24 217.17 3.32 3.5e+00
61 1.2 3 8.3e-11 101 2 12 0 0.119 11.9 4.92 0.448 0.448 1.6e+00 2.69 5.00 296.17 4.30 3.3e+00
71 1.4 2 7.7e-10 121 2 12 0 0.121 11.9 4.92 0.381 0.381 1.3e+00 3.07 5.00 334.19 4.59 1.9e+00
EXERCISES
- By varying U(1,:), investigate the effect of different plasma current ramp rates on the speed of penetration of inductive current, the evolution of the loop voltage profile U_{pl}, and the q profile.
- Returning to the original Ip time trace, now use U(2,:) to add 16MW of NBI power starting at different times during the ramp-up. Examine the effect on the T_e q and jpar profiles and explain the results.
- Vary U(3:5,:) to add at most 20MW of off-axis EC current drive at different times, and try to obtain a transport barrier by getting a reversed-shear q profile.
- Find a combination of timing for heating and current drive to keep qmin above 1 for as long as possible.