Suppression of Erosion in the DIII-D Divertor with Detached Plasmas

Suppression of Erosion in the DIII-D Divertor with Detached Plasmas PDF Author:
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ISBN:
Category :
Languages : en
Pages : 16

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The ability to withstand disruptions makes carbon-based materials attractive for use as plasma-facing components in divertors. However, such materials suffer high erosion rates during attached plasma operation which, in high power long pulse machines, would give short component lifetimes and high tritium inventories. The authors present results from recent experiments in DIII-D, in which the Divertor Materials Evaluation System (DiMES) was used to examine erosion and deposition during short exposures to well defined plasma conditions. These studies show that during operation with detached plasmas, produced by gas injection, net erosion is suppressed everywhere in the divertor. Net deposition of carbon with deuterium was observed at the inner and outer strikepoints and in the private-flux region between strikepoints. For these low temperature plasmas (T{sub e}

Divertor Erosion in DIII-D.

Divertor Erosion in DIII-D. PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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Net erosion rates of carbon target plates have been measured in situ for the DIII-D lower divertor. The principal method of obtaining this data is the DiMES sample probe. Recent experiments have focused on erosion at the outer strike-point (OSP) of two divertor plasma conditions: attached (T[sub e]> 40 eV) ELMing plasmas, and detached (T[sub e]2 eV) ELMing plasmas. For the attached cases, the erosion rates exceed 10 cm/exposure-year, even with incident heat flux

The Influence of Carbon in the Plasma on Metal Erosion and Redeposition in the DIII-D Divertor

The Influence of Carbon in the Plasma on Metal Erosion and Redeposition in the DIII-D Divertor PDF Author:
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ISBN:
Category :
Languages : en
Pages : 1

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Plasma Material Interactions in Current Tokamaks and Their Implications for Next Step Fusion Reactors

Plasma Material Interactions in Current Tokamaks and Their Implications for Next Step Fusion Reactors PDF Author: Gianfranco Federici
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ISBN:
Category : Fusion reactors
Languages : en
Pages : 342

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Divertor Heat and Particle Control Experiments on the DIII-D Tokamak

Divertor Heat and Particle Control Experiments on the DIII-D Tokamak PDF Author:
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Category :
Languages : en
Pages : 39

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In this paper we present a summary of recent DIII-D divertor physics activity and plans for future divertor upgrades. During the past year, DIII-D experimental effort was focused on areas of active heat and particle control and divertor target erosion studies. Using the DIII-D Advanced Divertor system we have succeeded for the first time to control the plasma density and demonstrate helium exhaust in H-mode plasmas. Divertor heat flux control by means of D2 gas puffing and impurity injection were studied separately and in, both cases up to a factor of five reduction of the divertor peak heat flux was observed. Using the DiMES sample transfer system we have obtained erosion data on various material samples in well diagnosed plasmas and compared the results with predictions of numerical models.

Simulation of Gross and Net Erosion of High-Z Materials in the DIII-D Divertor

Simulation of Gross and Net Erosion of High-Z Materials in the DIII-D Divertor PDF Author:
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ISBN:
Category :
Languages : en
Pages : 31

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The three-dimensional Monte Carlo code ERO has been used to simulate dedicated DIII-D experiments in which Mo and W samples with different sizes were exposed to controlled and well-diagnosed divertor plasma conditions to measure the gross and net erosion rates. Experimentally, the net erosion rate is significantly reduced due to the high local redeposition probability of eroded high-Z materials, which according to the modelling is mainly controlled by the electric field and plasma density within the Chodura sheath. Similar redeposition ratios were obtained from ERO modelling with three different sheath models for small angles between the magnetic field and the material surface, mainly because of their similar mean ionization lengths. The modelled redeposition ratios are close to the measured value. Decreasing the potential drop across the sheath can suppress both gross and net erosion because sputtering yield is decreased due to lower incident energy while the redeposition ratio is not reduced owing to the higher electron density in the Chodura sheath. Taking into account material mixing in the ERO surface model, the net erosion rate of high-Z materials is shown to be strongly dependent on the carbon impurity concentration in the background plasma; higher carbon concentration can suppress net erosion. As a result, the principal experimental results such as net erosion rate and profile and redeposition ratio are well reproduced by the ERO simulations.

Erosion and Deposition of Metals and Carbon in the DIII-D Divertor

Erosion and Deposition of Metals and Carbon in the DIII-D Divertor PDF Author:
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ISBN:
Category :
Languages : en
Pages : 18

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Net erosion rates at the outer strike point of the DIII-D divertor plasma were measured for several materials during quiescent H-mode operation with deuterium plasmas. Materials examined include graphite, beryllium, tungsten, vanadium and molybdenum. For graphite, net erosion rates up to 4 nm/sec were found. Erosion rates for the metals were much smaller than for carbon. Ion fluxes from Langmuir probe measurements were used to predict gross erosion by sputtering. Measured net erosion was much smaller than predicted gross erosion. Transport of metal atoms by the plasma across the divertor surface was also examined. Light atoms were transported farther than heavy atoms as predicted by impurity transport models.

Reconstruction of Detached Divertor Plasma Conditions in DIII-D Using Spectroscopic and Probe Data

Reconstruction of Detached Divertor Plasma Conditions in DIII-D Using Spectroscopic and Probe Data PDF Author: P. Stangeby
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ISBN:
Category :
Languages : en
Pages : 8

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Book Description
For some divertor aspects, such as detached plasmas or the private flux zone, it is not clear that the controlling physics has been fully identified. This is a particular concern when the details of the plasma are likely to be important in modeling the problem--for example, modeling co-deposition in detached inner divertors. An empirical method of ''reconstructing'' the plasma based on direct experimental measurements may be useful in such situations. It is shown that a detached plasma in the outer divertor leg of DIII-D can be reconstructed reasonably well using spectroscopic and probe data as input to a simple onion-skin model and the Monte Carlo hydrogenic code, EIRENE. The calculated 2D distributions of n{sub e} and T{sub e} in the detached divertor were compared with direct measurements from the divertor Thomson scattering system, a diagnostic capability unique to DIII-D.

ספר פרקי הדורות

ספר פרקי הדורות PDF Author:
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Category : Jewish wit and humor
Languages : en
Pages :

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DiMES Divertor Erosion Experiments on DIII-D.

DiMES Divertor Erosion Experiments on DIII-D. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 18

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Book Description
The DiMES (Divertor Material Evaluation Studies) mechanism allows insertion of material samples to the lower divertor floor of the DIII-D tokamak. The main purpose of these studies is to measure erosion rates and redeposition mechanisms under tokamak divertor plasma conditions in order to obtain a physical understanding of the erosion/redeposition processes and to determine its implications for fusion power plant plasma facing components. Thin metal films of Be, W, V, and Mo, were deposited on a Si depth-marked graphite sample and exposed to the steady-state outer strike point on DIII-D.A variety of surface analysis techniques are used to determine the erosion/redeposition of the metals and the carbon after 5--15 seconds of exposure. These short exposure times ensure controlled exposure conditions and the extensive array of DIII-D divertor diagnostics provide a well characterized plasma for modeling efforts. Erosion rates and redeposition lengths are found to decrease with the atomic number of the metallic species, as expected. Under these conditions, the peak net erosion rate for carbon is (approximately) 4 nm/s, with the erosion following the ion flux profile. Comparisons of the measured carbon erosion with REDEP code calculations show good agreement for both the absolute net erosion rate and its spatial variation. Measured erosion rates of the metals are smaller than predicted for sputtering from a bare metal surface, apparently due to effects of carbon deposition on the metal surface. Visible spectroscopic measurements of singly ionized Be have determined that the erosion process reaches steady-state during the exposure.