MANTA: A Negative-Triangularity NASEM-Compliant Fusion Pilot Plant

MANTA Collaboration, G. Rutherford, H. S. Wilson, A. Saltzman, D. Arnold, J. L. Ball, S. Benjamin, R. Bielajew, N. de Boucaud, M. Calvo-Carrera, R. Chandra, H. Choudhury, C. Cummings, L. Corsaro, N. DaSilva, R. Diab, A. R. Devitre, S. Ferry,S. J. Frank, C. J. Hansen, J. Jerkins, J. D. Johnson, P. Lunia, J. van de Lindt, S. Mackie, A. D. Maris, N. R. Mandell, M. A. Miller, T. Mouratidis, A. O. Nelson, M. Pharr, E. E. Peterson, P. Rodriguez-Fernandez, S. Segantin, M. Tobin, A. Velberg, A. M. Wang, M. Wigram, J. Witham, C. Paz-Soldan, D. G. Whyte

arxiv(2024)

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Abstract
The MANTA (Modular Adjustable Negative Triangularity ARC-class) design study investigated how negative-triangularity (NT) may be leveraged in a compact, fusion pilot plant (FPP) to take a “power-handling first" approach. The result is a pulsed, radiative, ELM-free tokamak that satisfies and exceeds the FPP requirements described in the 2021 National Academies of Sciences, Engineering, and Medicine report “Bringing Fusion to the U.S. Grid". A self-consistent integrated modeling workflow predicts a fusion power of 450 MW and a plasma gain of 11.5 with only 23.5 MW of power to the scrape-off layer (SOL). This low P_SOL together with impurity seeding and high density at the separatrix results in a peak heat flux of just 2.8 MW/m^2. MANTA's high aspect ratio provides space for a large central solenoid (CS), resulting in ∼15 minute inductive pulses. In spite of the high B fields on the CS and the other REBCO-based magnets, the electromagnetic stresses remain below structural and critical current density limits. Iterative optimization of neutron shielding and tritium breeding blanket yield tritium self-sufficiency with a breeding ratio of 1.15, a blanket power multiplication factor of 1.11, toroidal field coil lifetimes of 3100 ± 400 MW-yr, and poloidal field coil lifetimes of at least 890 ± 40 MW-yr. Following balance of plant modeling, MANTA is projected to generate 90 MW of net electricity at an electricity gain factor of ∼2.4. Systems-level economic analysis estimates an overnight cost of US$3.4 billion, meeting the NASEM FPP requirement that this first-of-a-kind be less than US$5 billion. The toroidal field coil cost and replacement time are the most critical upfront and lifetime cost drivers, respectively.
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