@article{9177,
  author = {C. Bachmann and M. Siccinio and E. Acampora and G. Aiello and J. Bajari and J. Boscary and A. Bruschi and V. Claps and A. Cufar and S. Wiesen and J. Elbez-Uzan and G. Federici and T. Franke and G. Germano and L. Giannini and C. Gliss and et al.},
  title = {Engineering concept of the VNS - a beam-driven tokamak for component testing},
  abstract = {<p>The qualification of in-vessel components for a fusion power plant requires a test environment with a high flux of 14 MeV neutrons over a sufficiently large surface and volume. Performance testing and qualification of the complex design and technologies of fusion nuclear components is needed, in particular that of the tritium breeding blanket (BB). Testing in relevant conditions over a relevant time will also allow gaining the necessary confidence regarding the build-up and control of tritium inventories inside the BB, which will be an important radioactive source. An option of such a volumetric neutron source (VNS) is a beam-driven tokamak. A feasibility study of the main machine components and associated plant systems is described in this article. The machine has a major radius of 2.53 m, a single-null divertor configuration, and four tangential 120 keV beamlines that generate a fusion power of approximately 30 MW and provide current drive for a steady-state plasma scenario. The plasma is small with a minor radius of a = 0.55 m to maximize the neutron wall load, up to 0.5 MW/m2, similar to what is targeted in ITER. Approximately 25 m2 are available for blanket testing including 4 port plugs, which offer flexibility regarding the test module operating conditions and the implementation of instrumentation. Given the small plasma, much of the tokamak's volume is made up by the neutron shielding structures that are similarly sized as in ITER. To reduce the construction risk, ITER-like concepts were adopted for many components. In some cases, however, lessons learned from ITER led to the development of customized or innovative concepts. Due to the modest fusion power the plasma will burn &lt;1 kg of tritium per year, which can be provided from external sources.</p>},
  year = {2025},
  journal = {Fusion Engineering and Design},
  volume = {211},
  pages = {114796},
  doi = {10.1016/j.fusengdes.2024.114796},
  language = {eng},
}