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Introduction to Spherical Tokamak SUNIST or 4th Workshop on Nonlinear Plasma Sciences International School on Plasma Turbulence and Tran Hangzhou 2005 GAO, Zhe Department of Engineering Physics Tsinghua University, Beijing 100084 [email protected]

Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

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Page 1: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Introduction to Spherical Tokamak

SUNISTSUNIST

for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport

Hangzhou 2005

GAO, ZheDepartment of Engineering PhysicsTsinghua University, Beijing [email protected]

Page 2: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

OUTLINE

• What is the spherical tokamak?

• ST advantage

• ST worldwide

• New physics of toroidal plasmas

• Potential contribution

Page 3: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• What is the Spherical Tokamak?

Spherical tokamak

Spherical torus tokamak

Page 4: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Spherical tokamak=low aspect ratio tokamak

Aspect ratio, A=R/a

Page 5: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

ST in Fusion configuration family

Page 6: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

UNISTUNISTSUNISTSUNIST

The first ST: START

Page 7: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• AdvantageCompact configuration

Natural elongation

Large qa n r si c ea e t n y o toro l l (he efficie c f ida fie d

ypyyrod yy>

large plasma current

lower toroidal field (paramagnetism)

High β

High density limit

Less major disruption (instead of IREs)

Good energy confinement

Improved confinement mode achieved

Page 8: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• ST worldwide

SUNIST

SUNIST

Page 9: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Parameters achieved

MAST NSTX

major radius R (m) 0.7 0.85

minor radius a (m) 0.5 0.68

elonggation κ 2.45 2.2

aspect ratio A (R/a) 1.3 1.27

plasma current IP (MA) 1.35 1.5

toroidal field BT(R0) (T) 0.52 0.6

neutral beam power PNBI (MW) 3.3 7

RF power P (MW) 1.5 ECRH HHFW 6

pulse length (s) 0.7 1.1

Page 10: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• Extended toroidal plasmas & New Physics(1) elongation>3, Bp/Bt~1, β~40%, Vrotation/Valfven~0.3

High βy l r r rot t ony stron s p qu la ge a i g ha ed e i

r umib i

(2) High β, low Valfven,, strong shear γE*B~106/s

yl trom n t tur ul n n ec ag e ic b e ce a dtr nporta t low ya

(3) a/ρi~30-50, a/ρfast ion~3-10, near omnigeneity, strongly mag well

Neoclassical transport at low A

(4) Valfven ~ Vs, Vfast ion>>Valfven ,less damping on TAE

st on p ys sFa i h ic

(5) High dielectric constant (ωpe2/ ωce

2~50-100)

y v yp rt l nt r t on (R t n a e a ic e i e ac i F hea i gyy yD

(6) Narrow inner regions and Low li yol no y r st rtupe idfe e a

Page 11: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Topical Research Plan of ST ( NSTX Five Year Plan)• MHD: RWM active and passive stabilzation

Fast-ion MHD (Alfven like)

NTM (stabilization by RF)

High beta equilibrium

• Transport and turbulence: high k and low k turbulence

H mode

Electron thermal barriers

Aspect ratio scaling

• Wave-plasma interaction: HHFW, EBW

• Solenoid-free startup: Transient CHI, PF induction, RF(ECH/EBW)

• Boundary Physics: Li conditioning, SOL transport

• Integration

UNISTUNISTSUNISTSUNIST

Page 12: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• What might ST bring to fusion application ?

Page 13: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Contribute to AT & burning plasma (ITER) physics

• Advanced Tokamak concept

High plasma kinetic pressure

Good confinement

High self-sustained current

(Quasi-) Stationary state

Advance fuel recycle

• Burning plasma

Page 14: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Other application:

VNSCTFContribution to AT and burning plasma researchSpace propulsion

Page 15: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Future Steps

Tokamak

* T-3, T-4, ST etc. 1970’s

** PLT, ASDEX etc.later 70’s

***TFTR,JET, JT-60U, 80—90‘s

**** ITER

2100’s

Page 16: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

SUNIST: Sino United Spherical Tokamak

major radius R 0.3m

minor radius a 0.23m

Aspect ratio A ~1.3

elongation κ ~1.6

toroidal field ( R0) BT 0.15T

plasma current IP 50kA

central rod current IROD 0.225MA

flux (double swing) ΔΦ 0.06Vs

Page 17: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• AcknowledgementCollecting material from the following references:

Peng Y-K, STW2004, Kyoto.

Gryaznevich M, STW2004, Kyoto.

Peng Y-K, STW2003, Culham.

Peng Y-K, Phys. Plasmas 2000, 7(5): 1681.

Sykes A, Nucl. Fusion 1999, 39(9Y):1271.

NSTX team, NSTX five year research plan

Peng Y-K and Strikler DJ, Nucl. Fusion 1986, 26:576

and many ST Websites.

Page 18: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

TOKAMAK

Page 19: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Spheromak

Page 20: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

UNISTUNISTSUNISTSUNIST

ST: more compact

Page 21: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

ST: natural elongation

Page 22: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

ST: High qa

Page 23: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

ST: high beta

Page 24: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

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ST: high density

Page 25: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

ST: more stable for VDI Internal Reconnection Event (IRE)

Page 26: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• ST: good confinement

Page 27: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

High beta equilibrium with larger rotation

Page 28: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

turbulence and transport

Page 29: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Single particle motion in ST

Page 30: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

HHFW CD

Page 31: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

EBW CD

Page 32: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Diffusion near the T-P boundary

Page 33: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

CHI startup

Page 34: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

Outer Poloidal Field startup

Page 35: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• ECH startup

Page 36: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• Bootstrap current MAST (real discharge) NSTX (Theo prediction)

Page 37: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou

• Divertor configuration

Divertor configurations in MAST:

Double-Null Divertor (DND)

Limited, or Natural Divertor (ND)

Single-Null Divertor(SND)

H-mode in DND and Natural Divertor plasmas

Page 38: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou
Page 39: Introduction to Spherical Tokamak SUNIST for 4th Workshop on Nonlinear Plasma Sciences & International School on Plasma Turbulence and Transport Hangzhou