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Overview of MAST results

Chapman, I.T.; Adamek, J.; Akers, R.J.; Allan, S.; Appel, L.; Asunta, O.; Barnes, M.; Ben Ayed, N.; Bigelow, T.; Boeglin, W.; Bradley, J.; Brünner, J.; Cahyna, P.; Carr, M.; Caughman, J.; Cecconello, M.; Challis, C.; Chapman, S.; Chorley, J.; Colyer, G.; Conway, N.; Cooper, W.A.; Cox, M.; Crocker, N.; Crowley, B.; Cunningham, G.; Danilov, A.; Darrow, D.; Dendy, R.; Diallo, A.; Dickinson, D.; Diem, S.; Dorland, W.; Dudson, B.; Dunai, D.; Easy, L.; Elmore, S.; Field, A.; Fishpool, G.; Fox, M.; Fredrickson, E.; Freethy, S.; Garzotti, L.; Ghim, Y.C.; Gibson, K.; Graves, J.; Gurl, C.; Guttenfelder, W.; Ham, C.; Harrison, J.; Harting, D.; Havlickova, E.; Hawke, J.; Hawkes, N.; Hender, T.; Henderson, S.; Highcock, E.; Hillesheim, J.; Hnat, B.; Holgate, J.; Horacek, J.; Howard, J.; Huang, B.; Imada, K.; Jones, O.; Kaye, S.; Keeling, D.; Kirk, A.; Klimek, I.; Kocan, M.; Leggate, H.; Lilley, M.; Lipschultz, B.; Lisgo, S.; Liu, Y.Q.; Lloyd, B.; Lomanowski, B.; Lupelli, I.; Maddison, G.; Mailloux,...

Authors

I.T. Chapman

J. Adamek

R.J. Akers

S. Allan

L. Appel

O. Asunta

M. Barnes

N. Ben Ayed

T. Bigelow

W. Boeglin

J. Bradley

J. Brünner

P. Cahyna

M. Carr

J. Caughman

M. Cecconello

C. Challis

S. Chapman

J. Chorley

G. Colyer

N. Conway

W.A. Cooper

M. Cox

N. Crocker

B. Crowley

G. Cunningham

A. Danilov

D. Darrow

R. Dendy

A. Diallo

D. Dickinson

S. Diem

W. Dorland

B. Dudson

D. Dunai

L. Easy

S. Elmore

A. Field

G. Fishpool

M. Fox

E. Fredrickson

S. Freethy

L. Garzotti

Y.C. Ghim

K. Gibson

J. Graves

C. Gurl

W. Guttenfelder

C. Ham

J. Harrison

D. Harting

E. Havlickova

J. Hawke

N. Hawkes

T. Hender

S. Henderson

E. Highcock

J. Hillesheim

B. Hnat

J. Holgate

J. Horacek

J. Howard

B. Huang

K. Imada

O. Jones

S. Kaye

D. Keeling

A. Kirk

I. Klimek

M. Kocan

H. Leggate

M. Lilley

B. Lipschultz

S. Lisgo

Y.Q. Liu

B. Lloyd

B. Lomanowski

I. Lupelli

G. Maddison

J. Mailloux

R. Martin

G. McArdle

K. McClements

B. McMillan

A. Meakins

H. Meyer

C. Michael

F. Militello

J. Milnes

A.W. Morris

G. Motojima

D. Muir

E. Nardon

V. Naulin

G. Naylor

A. Nielsen

M. O'Brien

T. O'Gorman

Y. Ono

H. Oliver

S. Pamela

L. Pangione

F. Parra

A. Patel

W. Peebles

M. Peng

R. Perez

S. Pinches

L. Piron

M. Podesta

M. Price

M. Reinke

Y. Ren

C. Roach

J. Robinson

M. Romanelli

V. Rozhansky

S. Saarelma

S. Sangaroon

A. Saveliev

R. Scannell

A. Schekochihin

S. Sharapov

V. Shevchenko

S. Silburn

J. Simpson

J. Storrs

Y. Takase

H. Tanabe

H. Tanaka

D. Taylor

G. Taylor

D. Thomas

N. Thomas-Davies

A. Thornton

M. Turnyanskiy

M. Valovic

R. Vann

N. Walkden

H. Wilson

L.V. Wyk

T. Yamada

S. Zoletnik

MAST

MAST Upgrade Teams



Abstract

The Mega Ampère Spherical Tokamak (MAST) programme is strongly focused on addressing key physics issues in preparation for operation of ITER as well as providing solutions for DEMO design choices. In this regard, MAST has provided key results in understanding and optimizing H-mode confinement, operating with smaller edge localized modes (ELMs), predicting and handling plasma exhaust and tailoring auxiliary current drive. In all cases, the high-resolution diagnostic capability on MAST is complemented by sophisticated numerical modelling to facilitate a deeper understanding. Mitigation of ELMs with resonant magnetic perturbations (RMPs) with toroidal mode number nRMP = 2, 3, 4, 6 has been demonstrated: at high and low collisionality; for the first ELM following the transition to high confinement operation; during the current ramp-up; and with rotating nRMP = 3 RMPs. nRMP = 4, 6 fields cause less rotation braking whilst the power to access H-mode is less with nRMP = 4 than nRMP = 3, 6. Refuelling with gas or pellets gives plasmas with mitigated ELMs and reduced peak heat flux at the same time as achieving good confinement. A synergy exists between pellet fuelling and RMPs, since mitigated ELMs remove fewer particles. Inter-ELM instabilities observed with Doppler backscattering are consistent with gyrokinetic simulations of micro-tearing modes in the pedestal. Meanwhile, ELM precursors have been strikingly observed with beam emission spectroscopy (BES) measurements. A scan in beta at the L–H transition shows that pedestal height scales strongly with core pressure. Gyro-Bohm normalized turbulent ion heat flux (as estimated from the BES data) is observed to decrease with increasing tilt of the turbulent eddies. Fast ion redistribution by energetic particle modes depends on density, and access to a quiescent domain with 'classical' fast ion transport is found above a critical density. Highly efficient electron Bernstein wave current drive (1 A W−1) has been achieved in solenoid-free start-up. A new proton detector has characterized escaping fusion products. Langmuir probes and a high-speed camera suggest filaments play a role in particle transport in the private flux region whilst coherence imaging has measured scrape-off layer (SOL) flows. BOUT++ simulations show that fluxes due to filaments are strongly dependent on resistivity and magnetic geometry of the SOL, with higher radial fluxes at higher resistivity. Finally, MAST Upgrade is due to begin operation in 2016 to support ITER preparation and importantly to operate with a Super-X divertor to test extended leg concepts for particle and power exhaust.

Citation

Chapman, I., Adamek, J., Akers, R., Allan, S., Appel, L., Asunta, O., …Upgrade Teams, M. (2015). Overview of MAST results. Nuclear Fusion, 55(10), https://doi.org/10.1088/0029-5515/55/10/104008

Journal Article Type Article
Acceptance Date Mar 4, 2015
Publication Date 2015-10
Deposit Date Aug 25, 2015
Journal Nuclear Fusion
Print ISSN 0029-5515
Electronic ISSN 1741-4326
Publisher IOP Publishing
Peer Reviewed Peer Reviewed
Volume 55
Issue 10
DOI https://doi.org/10.1088/0029-5515/55/10/104008