results from initial snowflake divertor physics studies on ... · 2 s.l. allen/iaea fec/november,...

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1 S.L. Allen/IAEA FEC/November, 2012 S. L. Allen, V. A. Soukhanovskii, T.H. Osborne, E. Kolemen, J. Boedo, N. Brooks, M. Fenstermacher, R. Groebner, D. N. Hill, A. Hyatt, C. Lasnier, A. Leonard, M. Makowski, W.H. Meyer, A. McLean, T. Petrie, D. Ryutov, J. Watkins IAEA Fusion Energy Conference, San Diego, CA October 8-12, 2012 Results From Initial Snowflake Divertor Physics Studies on DIII-D

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Page 1: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

S. L. Allen, V. A. Soukhanovskii, T.H. Osborne, E. Kolemen, J. Boedo, N. Brooks, M. Fenstermacher, R. Groebner, D. N. Hill, A. Hyatt, C. Lasnier, A. Leonard, M. Makowski, W.H. Meyer, A. McLean, T. Petrie, D. Ryutov, J. Watkins IAEA Fusion Energy Conference, San Diego, CA October 8-12, 2012

Results From Initial Snowflake Divertor Physics Studies on DIII-D

Page 2: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

•  Theory1 predicts second order null of SF Divertor (∇BP~0) –  Multiple strike points, increased volume and connection lengths –  Increased edge shear, influencing pedestal stability

•  Experiments2 have made progress on comparisons

•  DIII-D adds new data: Focus on SF(-) configuration

DIII-D Experiments focus on SF(-) configuration

1D. D. Ryutov, PoP 14, 064502 2007, TH/P4-18 2Vijvers EX/P5-22, 3Soukhanovskii EX/P5-21

2nd X-Point in Private Flux

2nd X-Point in SOL

Page 3: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

•  Theory1 predicts with second order null of SF Divertor (∇BP~0) –  Multiple strike points, increased volume and connection lengths –  Increased edge shear, influencing pedestal stability

•  Experiments2 have made progress on comparisons

•  DIII-D adds new data: Focus on SF(-) configuration –  Experience on NSTX

•  Possible heat flux control for future compact machines

DIII-D Experiments focus on SF(-) configuration

1D. D. Ryutov, PoP 14, 064502 2007, TH/P4-18 2Vijvers EX/P5-22, 3Soukhanovskii EX/P5-21

2nd X-Point in SOL

Page 4: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

•  Recent DIII-D long pulse (3s) results at high τ- H(89P) ≥ 2 in SF(-) configuration: –  Divertor “attached” during SF (C III images) –  2 – 3 X Heat flux reduction due to SF geometry (IR camera) –  Constant: Pedestal Profiles, Divertor Radiated Power (Bolometer) –  Reduced ΔW(ELM) and ELM heat flux on divertor

in SF(-) with Gas Puffing: –  Divertor detaches, large radiating volume –  Further heat flux reduction –  Heat flux during ELM reduced

DIII-D data adds new insight into Snowflake divertor

Divertor Heat Flux

Snowflake

Page 5: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

Compare DIII-D Normal Divertor with SF(-)

•  Use NSTX control algorithm •  2- External coils control strike points

(F4B and F8B) •  1- External coil moves 2nd null point

(F5B) •  DIII-D and NSTX use similar

Plasma Control Systems (PCS)

√√ Standard DIII-D Divertor

√√ Snowflake (-)

3mm Flux Line at Midplane

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S.L. Allen/IAEA FEC/November, 2012

•  Ip=1.2 MA, Bt=2 T •  PNBI= 3-5 MW

•  SF(-) maintained for è 3s

•  Flux expansion é 2.5X

•  Radiated Power è similar

•  Confinement è similar

•  Heat Flux reduced ê 2.5X

2.5X Divertor Heat Flux Reduction due to geometry

Page 7: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

New LLNL Periscope: IR image shows 3-D features of SF(-) operation on DIII-D

Pellet Pellet triggered ELM

Strike Point Splitting During SF

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S.L. Allen/IAEA FEC/November, 2012

Lower Divertor C III Shows Attached SF Divertor

Shot 150673, 3056-3654ms, CIII (465nm)

SF(-): Between ELMs, Additional Strike Point

Before SF(-): CIII extends to outer strike point (attached divertor)

Post-Snowflake

SF(-): During ELM, profile broadens

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S.L. Allen/IAEA FEC/November, 2012

•  No significant change in divertor bolometer radiation •  Small recombination (Balmer n= 7-2 line ) •  Tangential divertor Dα and C III cameras show no detachment •  In contrast with NSTX where SF(-) detaches

SF(-) divertor conditions similar to “attached” divertor

Inverted Rad. Power Standard Divertor

Inverted Rad. Power During SF(-)

Page 10: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

Divertor Peak Heat Flux Reduced 2.5X in SF due to changes in divertor geometry

Standard Divertor

Snowflake Snowflake

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S.L. Allen/IAEA FEC/November, 2012

Pedestal profiles between ELMs very similar with and without SF(-)

•  Slightly steeper and higher ne, lower and flatter Te with SF-

Electron Density ne Electron Temperature Te

Note: BLUE is

SF

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S.L. Allen/IAEA FEC/November, 2012

Detailed ELM analysis before/during SF shows:

•  Pedestal Energy (WPEDESTAL)

Constant

•  Confinement Constant

•  Change in stored energy lost

per ELM (ΔWELM) is reduced

•  Consistent with Loarte

connection length scaling

Detailed ELM Analysis: ΔW(ELM) decreased, W pedestal constant in SF

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S.L. Allen/IAEA FEC/November, 2012

New opportunity to study details of SOL transport in attached SF divertor; study ELMs

Standard Divertor

Snowflake

Divertor Heat Flux – Expanded Scale

Major Radius Divertor Plate

Page 14: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

New opportunity to study details of SOL transport in attached SF divertor; study ELMs

ELMs are Variable, Show Additional Strike points

Standard Divertor

Snowflake

Ryutov

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S.L. Allen/IAEA FEC/November, 2012

•  Shot with gas puffing only (black lines)

•  Compared with: –  SF –  SF + Gas puff

•  Reduced ELM peak heat load with SF + Gas Puff

SF + gas puffing reduces divertor ELM peak heat load

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S.L. Allen/IAEA FEC/November, 2012

SF + Gas Puff Reduced ELM divertor heat flux over GP alone

Gas Puff

SF + Gas Puff

SF D2

D2

Major Radius

Gas Puff

Gas Puff & SF

Expanded Divertor Radiation Zone in Both Cases

Divertor Heat Flux

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S.L. Allen/IAEA FEC/November, 2012

SF + Gas Puff (expanded scale)

Gas Puff

SF + Gas Puff

Gas Puff

Gas Puff & SF

Major Radius

Expanded Divertor Radiation Zone in Both Cases

D2

SF D2

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S.L. Allen/IAEA FEC/November, 2012

•  Recent DIII-D long pulse (3s) results at high τ- H(89P) ≥ 2 in SF(-) configuration: –  Divertor “attached” during SF (C III images) –  2 – 3 X Heat flux reduction due to SF geometry (IR camera) –  Constant: Pedestal Profiles, Divertor Radiated Power (Bolometer) –  Reduced ΔW(ELM) and ELM heat flux on divertor

in SF(-) with Gas Puffing: –  Divertor detaches, large radiating volume –  Further heat flux reduction –  Heat flux during ELM reduced

DIII-D data adds new insight into Snowflake divertor

Divertor Heat Flux

Snowflake

Page 19: Results From Initial Snowflake Divertor Physics Studies on ... · 2 S.L. Allen/IAEA FEC/November, 2012 • Theory1 predicts second order null of SF Divertor (∇B P~0) – Multiple

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S.L. Allen/IAEA FEC/November, 2012

•  Recent DIII-D long pulse (3s) results at high τ- H(89P) ≥ 2 in SF(-) configuration: –  Divertor “attached” during SF (C III images) –  2 – 3 X Heat flux reduction due to SF geometry (IR camera) –  Constant: Pedestal Profiles, Divertor Radiated Power (Bolometer) –  Reduced ΔW(ELM) and ELM heat flux on divertor

in SF(-) with Gas Puffing: –  Divertor detaches, large radiating volume –  Further heat flux reduction –  Heat flux during ELM reduced

•  Future snowflake studies: •  Integration with high-δ Advanced Tokamak Scenarios •  Clarification of detachment threshold w.r.t. standard divertor •  Study of parallel versus perpendicular SOL transport – SOL Physics •  Heat flux control in compact machines, new regimes

DIII-D data adds new insight into Snowflake divertor

Divertor Heat Flux

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S.L. Allen/IAEA FEC/November, 2012

Snowflake Divertor Results at the IAEA Conference: DIII-D adds recent new data

Ryutov – Original Theory TH/P4-18

TCV Heat Flux Reduction –

Vijvers EX/P5-22

NSTX Heat Flux Reduction –

Soukhanovskii EX/P5-21

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S.L. Allen/IAEA FEC/November, 2012

Backup Slides

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S.L. Allen/IAEA FEC/November, 2012

Initial DIII-D snowflake divertor results very encouraging and motivate further studies

ü  Demonstrated steady-state (2 s) snowflake-minus and plus configurations at σ = dX-X/aminor=0.15-0.20 §  Optimized divertor geometry and plasma shape for pedestal profile

measurements, analysis commencing

ü  Demonstrated beneficial magnetic geometry properties ü  Demonstrated between-ELM peak divertor heat flux reduction

via geometry ü  Favorable comparison with standard divertor geometry ü  Snowflake divertor attached at PNBI=3-5 MW , 0.5 x n/nG

ü  High confinement maintained (HL89~2.1, H98(y,2)~1.2-1.3)

ü  Demonstrated radiative detachment at 0.55-0.75 x n/nG ü  Density scan using D2 puffing ü  Significant reduction of peak divertor heat flux, Pdiv-rad ≤0.75 Ptot ü  Formation of MARFE-like X-point region outside of separatrix (?) ü  Up to 20 % confinement degradation at higher densities

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S.L. Allen/IAEA FEC/November, 2012

•  SF configuration reduces heat flux 2-3X by flux expansion

•  Divertor heat flux reduced

•  ∆W(ELM) reduced •  Core confinement (H98 > 2)

and pedestal constant

Snowflake divertor configuration reduces ELM and steady state heat flux

Snowflake

Standard Divertor Snowflake

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S.L. Allen/IAEA FEC/November, 2012

•  SF configuration reduces heat flux 2-3X by flux expansion

•  Divertor heat flux reduced

•  ∆W(ELM) reduced •  Core confinement (H98 > 2)

and pedestal constant •  ELM heat flux reduced

dramatically with gas puffing

Recent DIII-D Snowflake divertor experiments show heat flux reduction by flux expansion, ELM reduction

Snowflake

Snowflake

Snowflake Snowflake Major Radius

3.

4.

6.

ReducedDivertor Heat Flux

Increased Divertor Radiation

SF 5.

Time(s)