Deuterium Inventory in Tore Supra (DITS): 2nd post-mortem analysis campaign and fuel retention in the gaps

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Abstract

A dedicated study on fuel retention has been launched in Tore Supra, which includes a D wall-loading campaign and the dismantling of the main limiter (Deuterium Inventory in Tore Supra, DITS project). This paper presents new results from a second post-mortem analysis campaign on 40 tiles with special emphasis on the D retention in the gaps. SIMS analysis reveals that only 1/3 of the thickness of deposits in the plasma shadowed zones are due to the DITS wall-loading campaign. As pre-DITS deposits contain less D than DITS deposits, the contribution of DITS to the D inventory is about 30–50%. The new estimate for the total amount of D retained in the Tore Supra limiter is 1.7 × 1024 atoms, close to the previous estimate, with the gap surfaces contributing about 33%. NRA measurements show a stepped decrease of D along the gap with strong asymmetries between different gap orientations.

Introduction

High performance plasma discharges in modern magnetic confinement devices lead to the development of plasma facing components with castellated surfaces in order to reduce mechanical stress induced by heat loads or transient magnetic fields. However, the enlarged surface of these castellated plasma facing components raised concerns about the possibility of increased fuel retention. In order to assess the fuel retention in gaps and on castellated structures, several dedicated studies were performed (e.g. [1], [2], [3]). In most of these studies, the individual discharges lasted only a few seconds and no active control of the sample temperature during the discharges was attempted. This gap can be breached in Tore Supra as it can achieve long plasma durations combined with castellated, actively cooled plasma facing components (PFCs). The Deuterium Inventory in Tore Supra (DITS) project was launched to study fuel retention in true steady state from a plasma wall interaction point of view.

The DITS project consists of three phases: a dedicated campaign of repetitive discharges to load the walls with deuterium, the extraction of representative parts of the PFCs (namely one sector of the toroidal pump limiter (TPL), and tiles from different inboard and outboard protection PFCs), and an extensive analysis program in collaboration with European partners. Prior to the DITS loading campaign, 13C and 11B marker layers were deposited inside the vacuum vessel via glow discharges, using a mixture of He and 13CH4 or 11B2D6, respectively. For the actual D wall-loading campaign, more than 160 long (>1 min), identical discharges were performed for a total of ∼5 h of plasma operation [4]. Gas balance measurements showed a constant, non-saturating D-retention rate of 1.7 × 1020 D atoms s−1 resulting in a total increment of the D vessel inventory of ∼3.1 × 1024 D atoms [4].

An extensive post-mortem analysis program on the extracted PFC samples has been established to estimate the retained D. A first analysis campaign on 10 TPL tiles gave a first overview of the D content in the TPL and tested the technical procedures (e.g. sample cutting and handling, relevant analysis techniques) [5], [6]. A second analysis campaign, with 40 additional tiles has been started to address specific questions regarding retention and to broaden the statistical basis for the D quantification. Particularly, special care was taken for the detection of the 13C and 11B marker layers, in order to identify the part of the D inventory specifically due to the DITS loading campaign and to allow a more accurate comparison between the amount of retained fuel deduced from post-mortem analysis and from particle balance measurements. This article presents first results from this second post-mortem analysis campaign with special emphasis on the contribution of the gap surfaces to the D retention.

Section snippets

Available samples

Fig. 1 shows a picture of the dismounted TPL sector. Each finger is composed of 21 tiles (2.2 × 2.2–2.8 × 0.6 cm3), the width of the gaps being 2 and 0.6 mm in the poloidal and toroidal directions, respectively (the tile numbering convention is FxTy for tile y on finger x). One clearly sees the erosion/deposition pattern after the wall-loading campaign. Its shape results from self shadowing effects due to magnetic ripple structure: erosion zones are found in the directly plasma loaded areas; thin to

Results and discussion

The SIMS measurements on the samples in this second analysis campaign give a good indication of the position of the DITS start markers. The analyses were focused on samples from the thin, non-flaking zones since charging effects of the flaked deposits on samples from the thick deposit zones prevented effective measurements with the used magnetic sector SIMS apparatus. Fig. 2 presents a typical depth profile from the top surface of the tiles in the plasma shadowed zones. A broad feature of

Conclusion

In the case of Tore Supra, gap surfaces account for a significant amount of the retained D, but the connection between retention and magnetic configuration needs further investigation. Although the amount of D found in the post-mortem analysis (from the TPL and other PFCs) comes close to the amount of retained D estimated with particle balance measurements during the DITS campaign, the position of the DITS start markers within the deposits show that probably only 30–50% of the found deuterium

Acknowledgements

This work was carried out within the framework of the EFDA Task Force on Plasma–Wall Interactions. The views and opinions expressed herein do not necessarily reflect those of the European Commission.

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Presenting author. Address: CEA Cadarache, IRFM Bat. 508, 13108 Saint-Paul-lèz-Durance, France.

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