2013
DOI: 10.1088/0029-5515/53/7/073001
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Wall conditioning and density control in the reversed field pinch RFX-mod

Abstract: In the reversed field pinch RFX-mod at the highest plasma current of 2 MA, when error fields are not effectively feedback controlled, localized thermal loads up to tens of MW m−2 can be produced. The graphite tiles withstand such high power loads, but the high hydrogen retention makes density control extremely difficult. Several wall conditioning techniques have been optimized in the last campaigns, including helium glow discharge cleaning and wall boronization by diborane glow discharges. More recently, lithi… Show more

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Cited by 19 publications
(22 citation statements)
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“…Since the RFP heating is ohmic, multiplying equation ( 1) by n G , we get (V − V dyn ) I p = V G πa 2 n 0 , which is a linear dependence of the central density on heating power (input power minus the dynamo term). This dependence has indeed been reported for RFX [23]: with larger input power, larger densities can be accessed. This is a result reminiscent of the Sudo scaling, and it has been shown in the past also in the TEXTOR tokamak [24].…”
Section: Density Limit Phenomenology In the Rfx Rfpsupporting
confidence: 76%
See 1 more Smart Citation
“…Since the RFP heating is ohmic, multiplying equation ( 1) by n G , we get (V − V dyn ) I p = V G πa 2 n 0 , which is a linear dependence of the central density on heating power (input power minus the dynamo term). This dependence has indeed been reported for RFX [23]: with larger input power, larger densities can be accessed. This is a result reminiscent of the Sudo scaling, and it has been shown in the past also in the TEXTOR tokamak [24].…”
Section: Density Limit Phenomenology In the Rfx Rfpsupporting
confidence: 76%
“…This is a result reminiscent of the Sudo scaling, and it has been shown in the past also in the TEXTOR tokamak [24]. In the same paper [23], it was reported that, with lithization, the power required to get to the same density is half as much as in standard RFX discharges. According to equation (1), this means that also V G can be greatly reduced with wall conditioning.…”
Section: Density Limit Phenomenology In the Rfx Rfpmentioning
confidence: 71%
“…On the other hand, as the density is increased, its profile becomes hollow, due to the lack of continuous core fuelling (the only central fuelling is by pellet injection, whose effectiveness is limited by the short particle confinement time [42]), combined with an outward pinch and a high recycling [6]. In order to improve density control, in addition to boronization, lithization by different techniques has been applied, including evaporation and lithization by a liquid lithium limiter [43] and, recently, solid Li multi-pellet injection [44]. The latter technique allowed a more uniform Li deposition on the plasma wall, as shown in figure 12, where Li influxes at different toroidal positions as obtained after Li evaporation and by multipellet injection are compared.…”
Section: Density Control and Pwi Studiesmentioning
confidence: 99%
“…In RFX-mod, the carbon wall, due to its high hydrogen retention, dominates the behaviour of the plasma density, leading to uncontrolled H release in the presence of a strong plasma-wall interaction (PWI). Experiments testing several techniques of first wall lithization led to the reduction of recycling and improvement of density control [4] (section 3.2). (b) Feedback control of MHD stability.…”
Section: Advances In Active Controlmentioning
confidence: 99%