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Statements

Subject Item
n2:RIV%2F61389021%3A_____%2F12%3A00383249%21RIV13-AV0-61389021
rdf:type
n6:Vysledek skos:Concept
dcterms:description
In ITER, magnetic fusion will explore the burning plasma regime. Because such burning plasma is sustained by its own fusion reactions, alpha particles need to be confined (Hazeltine 2010 Fusion Eng. Des. 7-9 85). New experiments using d(He-3,p)alpha and d(d,p)t fusion reaction products were performed in JET. Fusion product loss was measured from MHD-quiescent plasmas with a charged particle activation probe installed at a position opposite to the magnetic field ion gradient drift (see figure 1)-1.77m above mid-plane-in the ceiling of JET tokamak. This new kind of escaping ion detector (Bonheure et al 2008 Fusion Sci. Technol. 53 806) provides for absolutely calibrated measurements. Both the mechanism and the magnitude of the loss are dealt with by this research. Careful analysis shows measured loss is in quantitative agreement with predictions from the classical orbit loss model. However, the comparison with simulated loss radial profile, although improved compared with previous In ITER, magnetic fusion will explore the burning plasma regime. Because such burning plasma is sustained by its own fusion reactions, alpha particles need to be confined (Hazeltine 2010 Fusion Eng. Des. 7-9 85). New experiments using d(He-3,p)alpha and d(d,p)t fusion reaction products were performed in JET. Fusion product loss was measured from MHD-quiescent plasmas with a charged particle activation probe installed at a position opposite to the magnetic field ion gradient drift (see figure 1)-1.77m above mid-plane-in the ceiling of JET tokamak. This new kind of escaping ion detector (Bonheure et al 2008 Fusion Sci. Technol. 53 806) provides for absolutely calibrated measurements. Both the mechanism and the magnitude of the loss are dealt with by this research. Careful analysis shows measured loss is in quantitative agreement with predictions from the classical orbit loss model. However, the comparison with simulated loss radial profile, although improved compared with previous
dcterms:title
Experimental investigation of the confinement of d(He-3,p)alpha and d(d,p)t fusion reaction products in JET Experimental investigation of the confinement of d(He-3,p)alpha and d(d,p)t fusion reaction products in JET
skos:prefLabel
Experimental investigation of the confinement of d(He-3,p)alpha and d(d,p)t fusion reaction products in JET Experimental investigation of the confinement of d(He-3,p)alpha and d(d,p)t fusion reaction products in JET
skos:notation
RIV/61389021:_____/12:00383249!RIV13-AV0-61389021
n6:predkladatel
n17:ico%3A61389021
n3:aktivita
n16:Z
n3:aktivity
Z(AV0Z20430508)
n3:cisloPeriodika
8
n3:dodaniDat
n19:2013
n3:domaciTvurceVysledku
n8:9079831
n3:druhVysledku
n12:J
n3:duvernostUdaju
n15:S
n3:entitaPredkladatele
n18:predkladatel
n3:idSjednocenehoVysledku
135582
n3:idVysledku
RIV/61389021:_____/12:00383249
n3:jazykVysledku
n4:eng
n3:klicovaSlova
Tokamak; activation; diagnostics; fusion; confinement
n3:klicoveSlovo
n10:fusion n10:confinement n10:activation n10:diagnostics n10:Tokamak
n3:kodStatuVydavatele
AT - Rakouská republika
n3:kontrolniKodProRIV
[D717B8313BC7]
n3:nazevZdroje
Nuclear Fusion
n3:obor
n11:BL
n3:pocetDomacichTvurcuVysledku
1
n3:pocetTvurcuVysledku
22
n3:rokUplatneniVysledku
n19:2012
n3:svazekPeriodika
52
n3:tvurceVysledku
Koslowski, R. Hult, M. Salmi, A. Von Thun, C. P. Vermaercke, P. Nielsen, S. K. Asunta, O. Pinches, S. Popovichev, S. Arnold, D. Vidmar, T. Bonheure, G. Murari, A. Mlynář, Jan Reich, M. Wieslander, E. Laubenstein, M. González de Orduña, R. Jachmich, S. Garcia-Munoz, M. Dombrowski, H.
n3:wos
000307099500007
n3:zamer
n9:AV0Z20430508
s:issn
0029-5515
s:numberOfPages
10
n5:doi
10.1088/0029-5515/52/8/083004