Coil Concept and Design for NCSX

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Coil Concept and Design for NCSX. S. P. Hirshman, June 3, 1999 on behalf of the NCSX coil team. NCSX Coil Team Members. Art Brooks, Don Monticello and Neil Pomphrey Princeton Plasma Physics Laboratory Coil cutting, plasma reconstruction (VMEC, PIES), Flexibility (Curopt) - PowerPoint PPT Presentation

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Coil Concept and Design for NCSX

S. P. Hirshman, June 3, 1999

on behalf of the NCSX coil team

NCSX Coil Team Members

• Art Brooks, Don Monticello and Neil Pomphrey– Princeton Plasma Physics Laboratory– Coil cutting, plasma reconstruction (VMEC, PIES), Flexibility (Curopt)

• William (“Buff”) Miner, Jr. and Prashant Valanju– Fusion Research Center– The University of Texas at Austin– SVD current optimization, GA coil cutting

• Steve Hirshman– Oak Ridge National Laboratory– Logistical support

Coil Design Activity for NCSX

• Identification of critical design goals– Physics, engineering constraints

• Development of computation tools– Advanced algorithms (Gen.Alg., CurOpt)

• Application to c82 preliminary design– status of target criteria and coil topology

• Flexibility and start-up considerations

C82 Coil Reference Design: Critical Goals

• Physics– Maintain QA-ness (NC transport) and kink

stability at < = 4% for reconstructed surfaces

• Engineering (maintain reconstructability)– limit jmax < 15 kA/cm2 at |B| = 1.2T (RBT = 1.65)

– reduce number of coils (cost)– maximize coil-to-coil separation (machining)

c82 Coil Design Process

PlasmaBoundary

NESCOIL

SVD Scan: Min (jmax)

Plasma-Coil Sep.(18 cm.)

Choose Candidate Coil Contours

Genetic Algorithm: Select Optimum Subset of Coils

Engineering Constraints jmax, coil-coil separtion

Reconstruction

“Fine Tuning”

Coil Designers MUST Serve Two Masters

PHYSICS ENGINEERING

Progress Toward Candidate NCSX Coils

• At Previous PAC– current sheet solutions - looked promising– discrete coils reconstructed for an impractically

large number (> 30) per period– current density acceptable for c10– plasma-coil minimum separation was NOT

uniformly maintained by winding surface

NCSX Candidate Coils (cont’d)

• Present Status:– finite coil designs (< 30 per period) for c82

• Designs exist with 16 - 20 coils (per period)

• “Good” reconstruction of flux surfaces

• jmax < 15 kA/cm2 (< 12 in some cases -> improved flat top, high |B|)

– winding surface - plasma distance (18 cm) – improved kink-stability in reconstructions

Emergence of c82 Candidate Coil Designs

(all designs: <a> = 42 cm, 18 cm. plasma-coil separation, B = 1.2 T)

C82 Case Description Coils Per Jmax Berr -% Surface Deviation Kink Eigenvalue QA-ness measureID Period (kA/cm**2) (ave., max) cm (av., max) (/Target value) (chi-sq/chi-sqTarget)

RECONSTRUCTION INFO --> 121 Equal Current 26 14.7 .95, 7.0 .47, 2.1 9 1.5 (s=.5), 1.0 (s=.8)

A. Brooks: Hand Tuning

4064 Lo-Jmax 20 11.9 1.2, 6.3 3.3, 8.9 (--------)EF-10% adjusted VF 1.0, 3.8 5 2.0 (s=.5), 1.3 (s=.8)

4321 Target Jmax 20 15.8 .95, 5.0 .73, 2.6 6 1.5 (s=.5), 1.1 (s=.8)

Latest GA Lo-# coils 16 14.4 1.1, 4.8"Miner" Miracle (further reduction anticipated)

C82 26-coil/period Design

Coil Cutting Developments

• Rapid Singular Value Decomposition– (SVD) scanning for Valanju minima of jmax

• eliminate small eigenvalues resulting from Least Squares fit of B-field

• NESCOIL current sheet: basis for discrete coils

• Reconstruction recovery of kink stability– the Pomphrey tweak

• Genetic Algorithm– application to cutting discrete coils

Jmax reduction comparison c82 vs. c93

c82.f88 svd scan (Berr target)Best at 121: Berr=0.6%, Jmax=.83

0.8316

0.2

0.4

0.6

0.8

1

1.2

100 110 120 130 140

number of svd weights kept out of 144

0.8

0.85

0.9

0.95

1

1.05

1.1

1.15

1.2<Berr>

jMax

c93.f1010 svd scan (Berr target)Best at 196: Berr=0.22%, Jmax=.81

0.2

0.25

0.3

0.35

180 190 200 210 220

number of svd weights kept out of 220

0.8

0.85

0.9

0.95

1

1.05

1.1

1.15

1.2<Berr>

jMax

Reconstruction with c82 Coils

• Geometric reconstruction– NESCOIL -> coils -> VMEC (free-bdy) ->

surfaces: assess displacement from target

• Physics reconstruction– Calculate of kink stability, QA-ness

• PIES reconstruction (in progress)– Existence of 3D flux surfaces

• basis for stability/transport calculations

Geometric Reconstruction

• c82 case 121 (26 coils/period)– started from lowest Valanju minimum

• SVD weights retained = 121

– very low displacement error– reconstruction: looks “good” to the eye

– jmax (14.7 kA/cm2) even lower than target requirement

Physics Reconstruction for c82 (121/26 coils)

• Quasi-Axisymmetry is well-maintained

• Kink is initially unstable

• Restoration of Kink Stability– An example of synergy between the physics

and the coil groups– the Pomphrey tweak

Restoration of Kink Stability (cont’d)

• Physics identified significance of matching indentation and “wings” at v=– Outboard pusher/puller coils were modestly re-

energized (by 10%) to recover kink stability– Application suggests a viable experimental

knob for “tweaking” the plasma configuration

Genetic Algorithm: Cutting Discrete Coils for c82

• GA: an efficient way to find an optimized subset of coils– pick Ncoil coils out of Ncontour contours (obtained

from NESCOIL, where Ncoil << Ncontour)

– contour selection based on minimizing physics and engineering criteria:

• Berror, Jmax, minimum coil-to-coil separation

– rapid 2D analysis tool (cf. 3D ONSET)

C82 Coil Cutting: A Slide Show

• The following slide show demonstrates the GA application for coil-cutting– first, locate Berror minimum (may be global)

– vary weights on Jmax

– obtain optimized low and moderate current states

• This “chromosome quartet” is composed in B. Miner...

Genetic Algorithm for Coil SelectionDiscrete Potential Contour Evolution

Initial conditions:

Current sheet Berror = .2%

98 coils generated from 60 contour levels.

GA selects the “optimal” 20 coils per period which yield a joint minimum in Berror and Jmax.

Toroidal angle / (2)

Poloidal angle / (2)

Genetic Algorithm for Coil Selection (initial zero weighting on Jmax)

Generation = 0001

Berror = .0090

Jmax = (coils too close to estimate…)

Genetic Algorithm for Coil Selection (lowest Berror state with coils)

Generation = 0236

Berror = .0041

Jmax =

Genetic Algorithm for Coil Selection (weight on Jmax turned on)

Generation = 1003

Berror = .0120

Jmax = est.

Genetic Algorithm for Coil Selection

Generation = 1025

Berror = .0079

Jmax = est.

Genetic Algorithm for Coil Selection

Generation = 1127

Berror = .0122

Jmax = 18.69

Genetic Algorithm for Coil Selection

Generation = 1105

Berror = .0119

Jmax = 18.37

Genetic Algorithm for Coil Selection

Generation = 1318

Berror = .0095

Jmax = 20.68

Genetic Algorithm for Coil Selection

Generation = 2795

Berror = .0090

Jmax = 20.47

Genetic Algorithm for Coil Selection (first big decrease in Jmax)

Generation = 3043

Berror = .0120

Jmax = 11.78

Genetic Algorithm for Coil Selection

Generation = 4001

Berror = .0123

Jmax = 11.86

Genetic Algorithm for Coil Selection

Generation = 4064

Berror = .0123

Jmax = 11.85

Genetic Algorithm for Coil Selection(decreased weighting of Jmax)

Generation = 4074

Berror = .0095

Jmax = 15.78

Genetic Algorithm for Coil Selection (final moderate jmax state)

Generation = 4321

Berror = .0094

Jmax = 15.75

Reconstruction for Low jmax c82(EF-10, VF correction):

kink restabilization likely

NCSX Start-up:Coil Issues

• Three “distinct” plasma states that coils must be capable of supporting– Vacuum start-up

• zero current, zero beta

– Start of flattop • full current, low beta

– End of flattop• full current, full beta: reference design point

NCSX Flexibility:Coil Issues

• Coils must have flexibility to produce– good vacuum surfaces

• in spite of low iota, resonances => stochasticity

– good surfaces at reference state• kink, QA-ness assessed assuming good surfaces

– kink stability and confinement for a range of profiles (pressure, current) around the reference state

Tools for Start-up Assessment• In Vacuum

– Cary-Hanson code (resonance suppression)

– AVAC

• In Vacuum or Finite Beta– Couple Curopt code (Brooks and Pomphrey) to output

from PIES - get internal (plasma) |B|mn spectrum, not just on surface - and target specific resonances for suppression

• Determine whether c82 coils have the re-quired flexibility to restore plasma volume

Vacuum Field Line Plots from fixed boundary

Vacuum Field Line Plots from d18.3.121.16 coil set with re-optimized currents

Tools for Robustness (flexibility) Assessment of c82

• Curopt code– couple with physics group to analyze stability,

QA-ness of neighboring states as pressure, current profiles vary

– compute currents in fixed c82 coils that most nearly generate these desired states

– repeat standard reconstruction analysis• Free boundary VMEC analysis (Mike Z.)

Future Tasks for Coil Group

• Finish c82 low J, low coil number calculations

• Look at c93: even lower J possible => greater experimental flexibility

• Work with physics, experimental teams to formulate flexibility, start-up implications for coils

Coil Designers SUCCESSFULLY Serve Two

Masters

PHYSICS ENGINEERING