Assessment of the beam–target interaction of IFMIF: A state of the art

Abstract The main requirement for an efficient and safe operation of the IFMIF plant is the stability of the Li jet. The stability is related to the thermohydraulic behaviour and can be affected by the beam–target interaction. The waviness of the jet must stay within rather narrow limits to protect the backwall from beam impact and to maintain stable irradiation conditions in the test modules. Thermal and momentum transfer of the beam may destabilize the flow structure, cause shock waves and increased evaporation or aerosol formation. Different aspects of beam interaction have been analyzed in the past, but a comprehensive assessment is still lacking. This contribution provides an overview of the IFMIF related beam–free lithium surface interaction studies including a description of the underlying basics. As it comes out from numerical analyses that the impact of thermal expansion and of the momentum transfer caused by the beam are still small enough to be ineffective for constructive interferences, beam–target interaction is not to be expected to have a critical impact on jet stability.

[1]  E. Wakai,et al.  Evaluation of applicability of laser-based distance meter to measure Li-jet thickness for IFMIF/EVEDA project , 2014 .

[2]  M. Mizumoto,et al.  Selective energy neutron source based on the D-Li stripping reaction , 1989 .

[3]  S. Dudarev,et al.  An integrated model for materials in a fusion power plant: transmutation, gas production, and helium embrittlement under neutron irradiation , 2012 .

[4]  Ulrich Fischer,et al.  Evaluation and validation of d-Li cross section data for the IFMIF neutron source term simulation , 2007 .

[5]  A. Ibarra,et al.  IFMIF: overview of the validation activities , 2013 .

[6]  E. A. Farber,et al.  Heat Transfer to Water Boiling Under Pressure , 1948, Journal of Fluids Engineering.

[7]  Masayoshi Sugimoto,et al.  Measurement of Neutron Emission Spectra in Li(d,xn) Reaction with Thick and Thin Targets for 40-MeV Deuterons , 2005 .

[8]  P. Plotkin,et al.  Behavior of liquid lithium jet irradiated by 1 MeV electron beams up to 20 kW , 2005 .

[9]  S. Bankoff Entrapment of gas in the spreading of a liquid over a rough surface , 1958 .

[10]  Ahmed Hassanein Deuteron beam interaction with lithium jet in a neutron source test facility , 1996 .

[11]  Ulrich Grigull,et al.  Progress in heat and mass transfer , 1969 .

[12]  I. Michiyoshi Boiling Heat Transfer in Liquid Metals , 1988 .

[13]  S. Goldman Generalizations of the Young-Laplace equation for the pressure of a mechanically stable gas bubble in a soft elastic material. , 2009, The Journal of chemical physics.

[14]  Eiichi Wakai,et al.  Completion of IFMIF/EVEDA lithium test loop construction , 2012 .

[15]  Tobias Heupel,et al.  Overview of results of the first phase of validation activities for the IFMIF High Flux Test Module , 2012 .

[16]  E. W. Pottmeyer,et al.  The fusion materials irradiation test facility at Hanford , 1979 .

[17]  G. A. Esteban,et al.  Hydraulics and heat transfer in the IFMIF liquid lithium target: CFD calculations , 2009 .

[18]  M. Robinson,et al.  A proposed method of calculating displacement dose rates , 1975 .

[19]  M. Ida,et al.  Hydraulic analysis on effects of back-plate deformation upon stability of high-speed free-surface lithium flow for IFMIF target design , 2011 .

[20]  Satoshi Fukada,et al.  Tritium removal by Y hot trap for purification of IFMIF Li target , 2010 .

[21]  T. Terai,et al.  Fabrication of nitrogen trapping test loop for IFMIF-EVEDA , 2011 .

[22]  M. Muzzarelli,et al.  Lifus (lithium for fusion) 6 loop design and construction , 2013 .

[23]  S. Nukiyama The maximum and minimum values of the heat Q transmitted from metal to boiling water under atmospheric pressure , 1966 .

[24]  R. M. Singer,et al.  On the role of inert gas in incipient boiling liquid metal experiments , 1969 .

[25]  Eiichi Wakai,et al.  The start-up and observation of the Li target in the EVEDA Li test loop , 2014 .