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Measurements with divertor probes on COMPASS

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6 Euratom/CCFE, Culham Science Centre, Abingdon, OX14 3DB, UK. 7 Max-PLanck-Institut für Plasmaphysik, Teilinstitut Greifswald, EURATOM Assoziation, ...
ITPA SOL & Divertor

Multi­tokamak scaling for prediction of ITER  SOL width in HFS­limited startup plasma (Following and concluding from ITPA meeting Oct. 2012)

J. Horacek1, R.A. Pitts2, J. Gunn3, C. Silva4, D. Rudakov5, G. Arnoux6, S. Marsen7, P. Vondracek1,8, G. Maddaluno9, V. Pericoli9, B. Viola9, G. S. Xu10, H. Wang10, M. Shimada2, J. Adamek1, Tsv. Popov11, M. Dimitrova1, R. Goldston12, P.C. Stangeby13, F. Janky1, J. Havlicek1, J. Seidl1, R. Dejarnac1, R. Panek1, P. Dobias14 and the JET-EFDA contributors6 1 Association EURATOM-IPP.CR, Institute of Plasma Physics AS CR, Za Slovankou 3, 18221 Praha 8, Czech Republic 2 ITER Organization, Route de Vinon sur Verdon, 13115 Saint Paul Lez Durance, France 3 CEA, IRFM, F-13108 Saint-Paul-lez-Durance, France 4 Associação EURATOM/IST, Instituto de PLasmas e Fusão Nuclear, IST, Av Rovisco Pais, 1049-001 Lisbon, Portugal 5 General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA 6 Euratom/CCFE, Culham Science Centre, Abingdon, OX14 3DB, UK 7 Max-PLanck-Institut für Plasmaphysik, Teilinstitut Greifswald, EURATOM Assoziation, 17491 Greifswald, Germany 8 Faculty of Math and Physics, Charles University, Czech Republic 9 ENEA-UT Fusione, Centro Ricerche Frascati, Italy 10 Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, China 11 Faculty of Physics, St. Kliment Ohridski University of Sofia, J. Bourchier Blvd., 1164 Sofia, Bulgaria 12 Princeton, Plasma Physics Laboratory, Princeton NJ 08543, USA 13 University of Toronto, Institute for Aerospace Studies, Toronto, M3H 5T6, Canada

th J. This Horacek for ITPA-Div/SOL group by1/13 18P205/12/2327 ITPA/DSOL, and Hefei, ChinaProject 20.3.2013 research was partly supported GA CR MSMT # LM2011021

ITPA SOL & Divertor

Motivation Toroi d

Goal: To predict heat flux spatial distribution on the ITER HFS wall during its startup limiter phase.

al x

λq determines optimal shape of the HFS Beryllium tiles. toroidal

Note: there is no theory-based model with credible predictive capability!

ITER ITER physics basis, Nuclear Fusion 39 2391 (1999)

Derived for diverted plasma at divertor. Is this scaling correct for limiter? No: [Saoutic Nucl.Fus. 2011], [J. Gunn, PSI 2012]

TS : Valid for others than Tore Supra? J. Horacek for ITPA-Div/SOL group

2/13

18th ITPA/DSOL, Hefei, China

20.3.2013

Database overview 264 radial profiles (q)

ITPA SOL & Divertor

ITER

JET

Tore Supra

DIII-D

EAST

FTU

R [m]

6.0

2.8

2.2

1.7

1.85

a [m]

2.0

0.98

0.65

0.6

0.46

Ip [kA]

35007500

1500 | 2500

4001200

6001200

B [T]

5.3

2.8

2.64.1

1.9

1.96

Instrument for Te

-

Swept Langmuir

Tunnel probe

Harmonic

Triple probe

Isotope

H, D, He, T

D

D

D

D

J. Horacek for ITPA-Div/SOL group

3/13

TCV

COMPASS

CASTOR

0.935

0.85

0.55

0.4

0.28

0.3

0.2

0.065

300 250-500

260

80-180

9

2.7-7.5

1.2

1.1

1.3

Swept Langmuir or ball-pen

Swept Langmuir

H/D

H

Limiter double-null

Swept Swept Langmuir Langmuir

D

D

18th ITPA/DSOL, Hefei, China

20.3.2013

(Bottom contact)

ITPA SOL & Divertor

Analysis procedure (1/2) COMPASS 59

TCV

1. Perform plasma limited at HFS 2. Measure q, mapped to

EAST 2

outboard midplane, using reciprocating probe (IR

14

2

camera)

3. q~f(R0,B0,Ip,P,...)

33 DIII-D

4. predict qITER

23

1 representative profile

FTU: 9

13

JET

121

Tore Supra

3cm gap

CASTOR

J. Horacek for ITPA-Div/SOL group

4/13

18th ITPA/DSOL, Hefei, China

20.3.2013

ITPA SOL & Divertor

Reciprocating probes 1. Obtain Te & Jsat by ● Single probe: ● Classical fit IV-characteristics ● Harmonic technique ● Tunnel probe ● Three probes: ● Isat, Te=(BPP -LP )/2.2 fl fl Triple probe 2. Te±Te & Jsat±Jsat =>q||=JsatTe ●

3. plot & fit q||=q0exp(-romp/q) mapped to outer midplane => get one qomp value per reciprocation Note that q-1=Isat-1+Te-1 ≈ Isat-1 ≈ ne-1 => the Te-technique not too important

CASTOR & FTU is different: q reason for q FTU always shorter than COMPASS? J. Horacek for ITPA-Div/SOL group

5/13

18th ITPA/DSOL, Hefei, China

20.3.2013

ITPA SOL & Divertor

Analysis procedure (2/2)

4. Searching for most credible scaling of q with 18 parameters: –

LCFS or Dimensionless (understandable scaling but uncertain for ITER):

• TeLCFS, neLCFS,  LCFS, *LCFS,  • Example: we expect [Garcia, PPCF (2007) B47]  s ~ Lc*vrblobs (*,

LCFS) / cs|| (Ti).

– Engineering (well known for ITER => lower error): • P [W/m3] , Ip[MA/m2], new PSOL/ALCFS, B0, R0, a/R0 omp • less acurate: Lc, n, n/nGW, new Bpol ( no predictive capability. Therefore, parameters used in the credible scalings must satisfy – low mutual correlations, let's say |Exponent| > 1/4, otherwise not credible => usually removing n, n/nGW This still yields dozens of reasonable scalings … however ...

J. Horacek for ITPA-Div/SOL group

12/13

18th ITPA/DSOL, Hefei, China

20.3.2013

ITPA SOL & Divertor

5 most credible scalings ...  yield similar qITER ☺ 

High exponents in anticorrelated parameters =>overfit

J. Horacek for ITPA-Div/SOL group

13/13

18th ITPA/DSOL, Hefei, China

20.3.2013

ITPA SOL & Divertor

Conclusion on ITER scenario

 

λqomp 

2.5MA

5.0MA

73

49

44

83±18

60±11

52±7

Most credible λq[mm]=

7.5MA

overfit

=5100(Ptot/V)-0.37(a/R)0.77κ-1.1 Mean of 12 most credible scalings λq[mm]

λqomp is the SOL decay length mapped to outer midplane. Identified dozens of more-or-less reasonable scalings, yielding similar ITER values. Let ITER staff decide which scaling (= parameter combination) to believe most The actual ITER design assumes HFS IMP q=50mm for 7.5MA … which is pretty close :-)

Warnings: – Based only on probes. – On JET: qIR not well correlated (because small plasma variation) with qRCP, however, power balance OK.

– Valid only in the far SOL! – Both JET & COMPASS IR camera shows qperp>q||sin() in the near SOL (r Theodor

EFIT EFIT mapping angle

Surface temperature

Assuming qlim(r,)=q0exp(-rmid/qcos()+qfunneling(rmid) J. Horacek for ITPA-Div/SOL group

16/13

18th ITPA/DSOL, Hefei, China

G. Arnoux et al. IAEA FEC 2012, EX/P5-37 20.3.2013

ITPA SOL & Divertor

Correlations with q: DIII­D no dependence (all C forget ASDEX Upgrade for the SOL scaling? J. Horacek for ITPA-Div/SOL group

29/13

18th ITPA/DSOL, Hefei, China

20.3.2013

ITPA SOL & Divertor

Inner wall x outer  wall limited  plasmas

C. Silva, …, J. Horacek, et al. PSI conference 2012, J. Nucl. Mat. J. Horacek for ITPA-Div/SOL group

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18th ITPA/DSOL, Hefei, China

20.3.2013

ITPA SOL & Divertor

LFS

J. Horacek for ITPA-Div/SOL group

31/13

18th ITPA/DSOL, Hefei, China

20.3.2013

ITPA SOL & Divertor

 Tokamak CASTOR

R=0.4m, a=0.085m, B=1.3 T, ne