Overview P EGASUS : ultra-low A ST designed to study stability - - PowerPoint PPT Presentation

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Overview P EGASUS : ultra-low A ST designed to study stability - - PowerPoint PPT Presentation

I NITIAL O PERATION OF THE U PGRADED P EGASUS ST E XPERIMENT Raymond.J. Fonck University of Wisconsin-Madison for the P EGASUS team: D. Battaglia M. Bongard S. Burke N. Eideitis B. Ford G. Garstka M. Kozar B. Lewicki E. Unterberg G. Winz


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SLIDE 1

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

INITIAL OPERATION

OF THE UPGRADED

PEGASUS ST EXPERIMENT

Raymond.J. Fonck University of Wisconsin-Madison for the PEGASUS team:

  • D. Battaglia
  • M. Bongard
  • S. Burke
  • N. Eideitis
  • B. Ford
  • G. Garstka
  • M. Kozar
  • B. Lewicki
  • E. Unterberg
  • G. Winz

presented to the 10th International ST Workshop Kyoto, Japan

  • Sept. 29- Oct. 1, 2004
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SLIDE 2

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Overview

  • PEGASUS: ultra-low A ST designed to study stability limits as A→1

and Ip/ITF >1

  • High βt and Ip=ITF achieved ohmically
  • Low-order tearing modes and ideal kinks limited access to higher Ip/ITF
  • Path to high Ip/ITF and β via suppression of instabilities
  • After fire: Lab rebuilt with significant upgrades
  • Advancing the experiment mission by improving plasma control
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SLIDE 3

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

NSTX, MAST START

MEDUSA CDX-U, HIT, TST-M, Globus-M, ETE

PEGASUS

TS-3,4 Spheromaks

1.0 1.2 1.4 1.6 1.8 2.0

Ip/ITF

}

qψ=6 Aspect Ratio

“tokamak-spheromak

  • verlap region”

100 10 1 0.1

Ip/Itf = figure of merit for access to low-A physics Pegasus is an extremely low-aspect ratio facility exploring quasi-spherical high-pressure plasmas with the goal of minimizing the central column while maintaining good confinement and stability

Mission: Explore plasma limits as A→1

Original Pegasus Goals:

  • Stability and confinement at high Ip/ITF
  • Extension of tokamak studies
  • Limits on βt and Ip/ITF (kink) as A→1
  • Overlap between the tokamak and the spheromak

Planned Future Emphases:

  • Support ST program movement to next

stages

  • EBW tests for heating & CD (w/PPPL)
  • Noninductive startup tests
  • Novel divertor design tests (w/UT)
  • CT fueling tests (w/UCD)
  • Diagnostics
  • High-pressure gas puff for deep fueling
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SLIDE 4

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Ohmic Trim Coils RF Heating Antenna Vacuum Vessel Centerstack:

Exposing Ohmic Heating Solenoid (NHMFL)

Equilibrium Field Coils Plasma Limiters Toroidal Field Coils

PEGASUS is University-Scale, Mid-Sized ST

Experimental Parameters Parameter Achieved Phase II Goals A 1.15-1.3 1.12-1.3 R (m) 0.2-0.38 0.2-0.45 Ip (MA) 0.16 0.30 IN (MA/m-T) 6-8 15-20 RBt (T-m) 0.03 0.1 κ 1.4−3.7 1.4−3.7 τshot (s) 0.02 0.05 ne (1019 m-3) 1-5

10

βt (%) 20 > 40 PHHFW (MW) 0.2 1.0

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SLIDE 5

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

A < 1.3 → Ready Ohmic Access to High βt

30 25 20 15 10 5

β

t (%)

10 8 6 4 2

Conventional Tokamaks START βN = 6 β

N

= 3 . 5 = Pegasus data

IN = Ip/(aBt )

  • βt up to 25% and IN up to 6.5 achieved ohmically
  • Low field → high IN and βt
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SLIDE 6

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Toroidal field utilization exhibits a “soft limit” around unity

  • Maximum Ip ITF
  • Soft limit due to two factors:
  • Large, internal 2/1, 3/2 tearing modes degrade plasma
  • Low shear over most of plasma, high resistivity
  • Reduced Volt-sec as TF decreases

0.16 0.12 0.08 0.04 0.00

Plasma Current (MA)

0.12 0.08 0.04 0.00

TF Rod Current (MA) Ip=Itf

0.16

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SLIDE 7

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Two factors contributed to the Ip/ITF 1 soft limit

Large resistive MHD instabilities degrade plasma as TF ↓

  • low Bt and fast dIp/dt → early appearance of low-order q=m/n
  • fixed sine-wave loop voltage
  • high resistivity early
  • ultra-low A → low central shear

⇒ Result: rapid growth of tearing modes and large saturated island widths

  • Most common modes: m/n=2/1, 3/2
  • Leads to decreased CE, Ip
  • Ip/ITF 1 ⇒ q0 1.5 - 2

Reduced effective Volt-seconds as TF ↓

  • reduced toroidal field → delayed startup
  • delayed startup + fixed sine Vloop waveform → reduced effective V-s
  • kA
  • Gauss

Ip δB

  • Frequency (Hz)
  • 2/1

3/2 2/1 Time (s)

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SLIDE 8

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Tangential PHC SXR image Image Contours: Measured Reconstructed

⇒ ⇒

Center column

12 8 4 q 1.0 0.8 0.6 0.4 0.2 0.0 ψ

N

q ψ

N

  • Measured q-profile indicates low central shear
  • 2D soft x-ray camera gives q-profile
  • Images soft x-rays
  • Constant-intensity surfaces determined
  • Mapped into flux space
  • G-S equation with SXR constraints
  • Iterate solution until convergence
  • Measured q-profile ⇒ low central shear
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SLIDE 9

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

  • Pegasus Data

δB/B (x10-3)

Mode Amplitude

  • q-profile tailoring increases plasma performance
  • Discharge tailoring → plasmas with reduced MHD activity, increase W and Ip
  • Increased shear, increased q0 ⇒ delay tearing onset
  • MHD amplitude decreases with increasing shear
  • Increased toroidal field strength also reduces MHD activity
  • Along Ip=Itf contour: δB ↑ as TF ↓
  • At high TF effect of MHD minimal
  • CE = 0.4
  • At lower TF MHD amplitude increases
  • CE increases
  • Stored energy decreases

⇒ Access higher Ip/ITF, βt via increased q0, Te, shear

MHD affected by q-profile tailoring and TF strength

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SLIDE 10

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

  • High Ip plasmas often disrupt
  • q95 = 5 observed

preceding disruption

  • i=0.5 at this time
  • DCON analysis ⇒ unstable

to n=1 external kink

  • m=5 most unstable mode
  • Consistent with theory expectation

ψN

0.0 0.2 0.4 0.6 0.8 1.0

Real u1

1.0 0.8 0.6 0.4 0.2 0.0

m=5 m=4 m=3 m=2 m=1

Poloidal mode eigenfunctions via DCON 0.16 0.12 0.08 0.04 0.00

MA

0.024 0.020 0.016 0.012 8 7 6 5 4 8 6 4 2

AU

0.023 0.022 0.021 0.02

Time (s)

10 100

T/s

Plasma Current q95 Free- Boundary Energy (DCON) MHD Amplitude

High q95 external kink limit observed

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SLIDE 11

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Planned path to access to high Ip/Itf, βt operation

  • Suppression of large internal MHD modes
  • Vary q(ψ)
  • Lower η before q(ψ) approaches low-order rational mode surfaces
  • Expand access to external kink modes studies
  • Plasma time evolution, shape
  • Edge conditions and edge currents
  • Access to very high βt regime for stability analysis
  • OH access and HHFW heating availability
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SLIDE 12

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

New tools to access Ip > Itf

  • Suppress tearing modes early in discharge evolution

= Transiently manipulate q during discharge:

  • Increased TF at startup

=> high Itf, low inductance TF bundle

  • Variable Ip and R0 control

=> coil-current-waveform control = Reduce resistivity before low-order rationals appear

  • Maximize J

=> Vloop control, position & shape control

  • Increase ohmic flux

=> new ohmic power supply

  • Use HHFW system

=> position control, Vloop control

  • Explore edge kink boundary at high field utilization
  • Manipulate edge shear

=> divertor coils for separatrix & PF shape control

  • Decrease edge currents

=> loop voltage control

  • Manipulate plasma shape

=> shape control

  • Manipulate current profile

=> Vloop control, position control

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SLIDE 13

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Overview of PEGASUS Phase II Rebuild

  • Power Systems Entirely Replaced
  • PWM controlled H-Bridges allow for complete waveform control
  • Coil currents increased significantly
  • 6 MJ of electrolytic capacitors installed outside of experimental building
  • New power buses installed
  • Low-inductance Toroidal Field Centerstack Installed
  • Provides increased, time-variable TF
  • Lab Infrastructure Improved or Replaced
  • Shielded conduits and cable trays installed
  • New grounding system installed
  • Control and Safety systems upgraded
  • Bakeable gas system
  • Upgraded AC, air, and water services installed
  • Passive Stray field “flux catcher” installed for public safety
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SLIDE 14

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Phase I laboratory layout (2002)

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SLIDE 15

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Laboratory before rebuild (October 2002)

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SLIDE 16

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Rebuilt laboratory (June 2004)

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SLIDE 17

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Power Systems consist of IGBT/IGCT Solid State H-Bridges

ABB IGCT 2.8kV@4kA Steady-State ~ 50 cm long

System Toroidal Field Ohmic Heating Equilibrium Field Phase I

  • 60 turns
  • Quasi-DC
  • 150 kA-t max
  • Half-sine

Waveform

  • 40 KA at 10kV
  • Monolithic coil set
  • 2 Resonant banks
  • Waveform constrained

by startup concerns

  • No divertor

Phase II

  • 12 turns
  • Time-variable
  • up to 450 kA-t
  • 8 IGBT Bridges
  • Programmable
  • 48 KA at 2.7kV
  • 12 IGCT Bridges
  • Independent coils
  • 20 IGBT Bridges
  • Evolution free from

startup constraints

  • Divertor installed
  • Many thanks to the HIT Group for their assistance!

Example

ITF (KA)

0.08

Time (s)

  • Vloop

8

Phase I Phase II

Time (s)

.035

  • Ief (KA)
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SLIDE 18

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

  • Benefits
  • Tailor the current waveform to match the

needs of the desired plasma evolution

  • PWM controlled modern IGCT/IGBT

semiconductors

  • More reliability and control with less overall

stored energy

  • H-Bridge regeneration mode minimizes heating
  • f critical coil sets
  • Fault detection and interruption capability
  • HIT group: CAMAC based, optically isolated

PWM controller

Pulse Width Modulated (PWM) H-Bridges

IGBT H-Bridge (2 of up to 28) 900V, 4kA at up to 5kHz Insulated Gate Bipolar Transistor

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SLIDE 19

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

PEGASUS Centerstack Assembly and TF Waveform

  • 60 Turn Bundle

12 Turn Bundle

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SLIDE 20

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Toroidal Field Joint Area is Critical

Cross-Sectional Drawing (Top)

Contact Finger Wedge Reactor Bottom Wedge Driver Wedge Top Coil Leg G-10 Support Plates 12-Turn Bundle Plastigage™ Pressure Paper

Fit-Check Diagnostics

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SLIDE 21

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Toroidal Field Upper Joint Assembly

Bare TF Assembly Fully Assembled TF Joint

Copper Finger Wedge Reactor Wedge Set Screws Coolant Channel

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SLIDE 22

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

  • Initially using PF power supplies for OH ⇒ limited Volt-s and Vloop
  • 1st plasma in late May
  • 2 month campaign in Summer 2004
  • Transient suppression and PS stabilization
  • New facility tests and systems shakedown
  • Effects of wall currents with new waveforms
  • Low power startup studies
  • Stabilizing operations
  • New power systems stabilized and working as desired
  • Robust to major failures
  • Recent upgrades to enhance operations
  • Major grounding change to stabilize PS
  • New diagnostics installed
  • Single plasma gun installed for tests of CD and fueling
  • Late Sep - Early Oct: Installation of first High-V OH power supplies
  • Upcoming campaign in Fall-Winter 2004-2005: Use New Tools
  • Commission new OH system for high-power ops
  • Tearing mode suppression
  • Access to Ip/Itf > 1, low-q, high IN, high βt regime
  • Characterize ext kink limits
  • Introduce separatrix
  • Use gun for startup assist
  • Install more guns

Present Status - Coming into full power ops

Recent Plasma

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SLIDE 23

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

  • 20
  • 15
  • 10
  • 5

5 10 15 20 Coil Current (kA) 0.04 0.03 0.0 2 0.0 1 0.00 Shot 24239 OH EF123 EF678 EF45 (Bias) TF 30x1

  • 3

20 10 Poloidal Field (R=0.25 m) 40 30 20 10 ms 1.2 1.0 0.8 0.6 0.4 0.2 0.0 A.U. 40 30 20 10 x10-3 4 2

  • 2
  • 4

Vloop (V) 0.04 0.03 0.02 0.01 0.00 s 100 80 60 40 20 Ip (KA)

Vloop Coil Currents Poloidal Flux

Typical waveforms for ohmic operations

Gas Puffs EC PI Ip

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SLIDE 24

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Ip/Itf space expanded

0.28 0.24 0.20 0.16 0.12 0.08 0.04 0.00

Plasma Current (MA)

0.28 0.24 0.20 0.16 0.12 0.08 0.04 0.00

TF Rod Current (MA) Ip = ITF Pegasus Phase I Aug-Sep 2004

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SLIDE 25

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Plasma guns being tested for startup and fueling

Gun installed in lower divertor region Time-integrated plasma image Gun orifice

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SLIDE 26

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Low Gun Current/Power --> Linear Current Scaling

  • Current channel follows field line
  • Maintains helical nature
  • Current (A)
  • Time (s)
  • Current Amplification

Vbias = 50 V sn 24433 I_tor Igun_x5 Ratio

  • Total toroidal current ~ 5 x gun current
  • Ip/Ig constant
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SLIDE 27

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Low Gun Current/Power --> Linear Current Scaling

  • Current channel follows field line
  • Maintains helical nature
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SLIDE 28

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

HIgh Gun Current/Power --> Nonlinear Current Scaling

  • Total toroidal current > 5 x gun current
  • Ip/Ig increases
  • Current channels merge/reconnect
  • Generates extended plasma
  • Current (A)
  • Time (s)
  • Current Amplification

Vbias = 400 V sn 24437 I_tor Igun_x5 Ratio

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SLIDE 29

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

HIgh Gun Current/Power --> Nonlinear Current Scaling

  • Current channels merge/reconnect
  • Generates extended plasma
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SLIDE 30

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

  • Early indications: gun startup compatible with OH
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SLIDE 31

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

Mercier Criterion

  • 2.5
  • 2.0
  • 1.5
  • 1.0

ArcSinh DI (A.U.) x10-1 x10-1 ArcSinh DR (A.U)

1.5 0.0 0.5 1.0 0.0 0.2 0.4 0.6 0.8 1.0

ρ

GGJ Resistive Criterion

0.0 0.2 0.4 0.6 0.8 1.0

ψN

5 10 15 20 25 30

Newcomb Criterion, n=1 (A.U.)

q Profile

1 2 3 4

DI,DR > 0 => Unstable

Flux Plot

  • Equilibria Parameters
  • High-Ip/Itf, “zero”-β Equilibria

Plasma Limits Modeled at Ip/Itf ~ 3

  • DCON Output
  • Approaches Phase II Goals of PEGASUS

βN = 6 βN = 3.5

Increase Aux. Heating

PEGASUS START Conventional Tokamaks

Increase Ip/ITF

120 100 80 60 40 20 βt 20 15 10 5 IN = Ip/aBto [MA/(m T)]

  • 1.0
  • 0.5

0.0 0.5 1.0 1.0 0.5 0.0

R (m) Z (m)

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SLIDE 32

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

EBW heating and current drive of interest for ST regime

  • Plasma startup, sustainment
  • Applicable to low-field, overdense plasmas
  • Of interest to future NSTX development

Basic principles tested on W-7S and CDX

  • Need to be tested at significant power levels

Pegasus good candidate for EBW development

  • Low-cost 2.45 GHz technology
  • Klystrons and waveguide available from PLT
  • Need to demonstrate good target plasma control

Working with PPPL to develop best approach

  • Modeling
  • Hardware
  • Experiments

Economical Tests of EBW Possible on PEGASUS

(a) EBW ray tracing calculations for a 250 kA PEGASUS equilibrium, central density of ne(0) = 1013 cm-3. (b) n|| along the ray path, showing the up- shift depends upon launch position. (c) Power deposition profiles corresponding to the rays in (a) and (b).

deposition profile n|| upshift

0.0 0.0 0.2 0.2 0.4 0.4 0.6 0.6 0.8 0.8 1.0 1.0 1.2 rho rho 20 40 60

  • 4

80

  • 2

10 12 2 4 6 8 10

1 1 2 2 3 3 4 4 5 5 6 6 6 5 4 2 3 2

(a) (b) (c) n|| MWm-3

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SLIDE 33

PEGASUS Toroidal Experiment University of Wisconsin-Madison

10th STW Sept.29, 2004 - rjf

  • Phase I ops finished Spring 2002
  • Ip/Itf = 1.1
  • βt = 25%
  • Factors found limiting plasma current:

+ internal resistive modes + V-s limitations + external kinks

  • Staged upgrades were proposed to suppress limiting mechanisms
  • Fire initiated a “front-loading” of upgrades
  • Upgrades are mostly completed
  • New switching power supplies (final installation now)
  • New capacitor banks
  • New TF centerstack
  • New control code
  • New signal runs and screen room
  • Phase II ops have begun
  • Low power OH
  • Plasma gun tests
  • New diagnostic installations

PEGASUS now poised to exploit its unique niche