Tomi Vuoriheimo

Tomi Vuoriheimo


Research Focus & Metrics

Academic Career Length

8Years (2019-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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23 September 2021 in Nuclear Fusion
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AHAntti Hakola
Antti Hakola
JLJari Likonen
Jari Likonen
ALAki Lahtinen
Aki Lahtinen
TVTomi Vuoriheimo
Tomi Vuoriheimo
MGMathias Groth
Mathias Groth
TCThe Eurofusion Wp Pfc Contributors
The Eurofusion Wp Pfc Contributors

2 December 2021 in Nuclear Fusion
Verified
Journal Article
Open access
SBS. Brezɩnsek
S. Brezɩnsek
CDC.P. Dhard
C.P. Dhard
MJM. Jakubowski
M. Jakubowski
RKR. König
R. König
SMS. Masuzaki
S. Masuzaki
TTthe W7-X Team
the W7-X Team
W7-X completed its plasma operation in hydrogen with island divertor and inertially cooled test divertor unit (TDU) made of graphite. A substantial set of plasma-facing components (PFCs), including in particular marker target elements, were extracted from the W7-X vessel and analysed post-mortem. The analysis provided key information about underlying plasma–surface interactions (PSI) processes, namely erosion, transport, and deposition as well as fuel retention in the graphite components. The net carbon (C) erosion and deposition distribution on the horizontal target (HT) and vertical target (VT) plates were quantified and related to the plasma time in standard divertor configuration with edge transform ι = 5/5, the dominant magnetic configuration of the two operational phases (OP) with TDU. The operation resulted in integrated high net C erosion rate of 2.8 mg s−1 in OP1.2B over 4809 plasma seconds. Boronisations reduced the net erosion on the HT by about a factor 5.4 with respect to OP1.2A owing to the suppression of oxygen (O). In the case of the VT, high peak net C erosion of 11 μm at the strike line was measured during OP1.2B which converts to 2.5 nm s−1 or 1.4 mg s−1 when related to the exposed area of the target plate and the operational time in standard divertor configuration. PSI modelling with ERO2.0 and WallDYN-3D is applied in an interpretative manner and reproduces the net C erosion and deposition pattern at the target plates determined by different post-mortem analysis techniques. This includes also the 13C tracer deposition from the last experiment of OP1.2B with local 13CH4 injection through a magnetic island in one half module. The experimental findings are used to predict the C erosion, transport, and deposition in the next campaigns aiming in long-pulse operation up to 1800 s and utilising the actively cooled carbon-fibre composite (CFC) divertor currently being installed. The CFC divertor has the same geometrical design as the TDU and extrapolation depends mainly on the applied plasma boundary. Extrapolation from campaign averaged information obtained in OP1.2B reveals a net erosion of 7.6 g per 1800 s for a typical W7-X attached divertor plasma in hydrogen.

25 February 2023 in Nuclear Materials and Energy
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Journal Article
Open access
MDM. Diez
M. Diez
MBM. Balden
M. Balden
SBS. Brezinsek
S. Brezinsek
YCY. Corre
Y. Corre
NFN. Fedorczak
N. Fedorczak
TVTomi Vuoriheimo
Tomi Vuoriheimo

1 May 2019 in Nuclear Materials and Energy
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Journal Article
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KHKalle Heinola
Kalle Heinola
Tommy Ahl­grenTommy Ahl­gren
Tommy Ahl­gren
SBSebastijan Brezinsek
Sebastijan Brezinsek
TVTomi Vuoriheimo
Tomi Vuoriheimo
SWS. Wiesen
S. Wiesen

5 January 2023 in Journal of Nuclear Engineering
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IJIndrek Jõgi
Indrek Jõgi
PPPeeter Paris
Peeter Paris
EBElodie Bernard
Elodie Bernard
MDMathilde Diez
Mathilde Diez
ETEmmanuelle Tsitrone
Emmanuelle Tsitrone
ECEurofusion Wp Pfc/Pwie Contributors
Eurofusion Wp Pfc/Pwie Contributors
Fuel retention monitoring in tokamak walls requires the development of remote composition analysis methods such as laser-induced breakdown spectroscopy (LIBS). The present study investigates the feasibility of the LIBS method to analyse the composition and fuel retention in three samples from WEST divertor erosion marker tiles after the experimental campaign C3. The investigated samples originated from tile regions outside of strong erosion and deposition regions, where the variation of thin deposit layers is relatively small and facilitates cross-comparison between different analysis methods. The depth profiles of main constituents W, Mo and C were consistent with depth profiles determined by other composition analysis methods, such as glow-discharge optical emission spectroscopy (GDOES) and secondary ion mass spectrometry (SIMS). The average LIBS depth resolution determined from depth profiles was 100 nm/shot. The averaging of the spectra collected from multiple spots of a same sample allowed us to improve the signal-to-noise ratio, investigate the presence of fuel D and trace impurities such as O and B. In the investigated tile regions with negligible erosion and deposition, these impurities were clearly detectable during the first laser shot, while the signal decreased to noise level after a few subsequent laser shots at the same spot. LIBS investigation of samples originating from the deposition regions of tiles may further clarify LIBS’ ability to investigate trace impurities.

27 May 2024 in Materials
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Journal Article
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ALAnna Liski
Anna Liski
TVTomi Vuoriheimo
Tomi Vuoriheimo
JBJesper Byggmästar
Jesper Byggmästar
KMKenichiro Mizohata
Kenichiro Mizohata
KHKalle Heinola
Kalle Heinola
FTFilip Tuomisto
Filip Tuomisto
The WMoTaNbV alloy has shown promise for applications as a solid state hydrogen storage material. It absorbs significant quantities of H directly from the atmosphere, trapping it with high energy. In this work, the dynamics of the absorption of hydrogen isotopes are studied by determining the activation energy for the solubility and the solution enthalpy of H in the WMoTaNbV alloy. The activation energy was studied by heating samples in a H atmosphere at temperatures ranging from 20 °C to 400 °C and comparing the amounts of absorbed H. The solution activation energy EA of H was determined to be EA=0.22±0.02 eV (21.2 ± 1.9 kJ/mol). The performed density functional theory calculations revealed that the neighbouring host atoms strongly influenced the solution enthalpy, leading to a range of theoretical values from −0.40 eV to 0.29 eV (−38.6 kJ/mol to 28.0 kJ/mol).