An integrated model of a complete discharge in the FIRE experiment has been developed based on the TSC simulation code. The complete simulation model includes a choice of several models for core transport, combined with an edge pedestal model and the Porcelli sawtooth model. Burn control is provided by feedback on the auxiliary heating power. We find that with the GLF23 and MMM95 transport models, Q >10 operation should be possible for H-mode pedestal temperatures in the range of 4-5 keV.
Introduction:The proposed Fusion Ignition Research Experiment (FIRE) is a $1B class facility that will be capable of exploring many of the burning plasma physics issues of interest to our community. The device dimensions can be "derived" from an optimization algorithm where we seek the most compact configuration that utilizes wedged copper alloy toroidal field coils pre-cooled to 80 o K and without active cooling [1]. The constraints imposed during the optimization include ELMy H-mode ITER98(y,2) scaling for the energy confinement time, a density limit of n 20 < 0.75 n GW , sufficient power to exceed the H-mode power threshold, a normalized stability parameter of β N < 1.8, and a pulse length exceeding (by a factor of 2) that required for the plasma current profile to fully equilibrate to a stationary state. This leads to a reference design with R 0 = 2.14 m, a = 0.595 m, B t (R 0 ) = 10 T, I P = 7.7 MA with a flattop time at full parameters of 20 s, and with150 MW of fusion power. The strong shaping (δ X = 0.7, κ X = 2.0) and low normalized density can be expected to improve the confinement to a multiplier of 1.1 applied to the H98(y,2) global confinement time scaling, projecting to a fusion gain Q ~ 10 [2].