design and operation of a novel divertor …labombard/aps07...design and operation of a novel...
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Design and operation of a novel divertor cryopumping system in Alcator C-Mod1
B. LaBombard, B. Beck, J. Bosco, R. Childs, D. Gwinn, J. Irby, R. Leccacorvi, S. Marazita,N. Mucic, S. Pierson, Y. Rokhman, P. Titus, R. Vieira, J. Zaks, A. Zhukovsky
Plasma Science and Fusion Center, M.I.T, Cambridge, MA 02139, USA
Download electronic copyof this poster: http://www.psfc.mit.edu/~labombard/APS07_Cryopump_Poster.pdf
1Supported by USDoE Coop. Agreement DE-FC02-99ER54512
Testing of Full-Scale Prototype Cryopump
Cryopump installation into Test Chamber
"Toroidal Loop" is assembled from three sections...
8 LHe and 4 LN2temperature sensors
... and "hung" from undersideof Test Chamber cover
Stainless steel baffles simulateupper divertor tiles and structures in C-Mod
'Dip-stick' measuresLHe level
Prototype Cryopump Test Results
Liquid Helium Tube Temperature (degrees K)
Liquid Nitrogen Shield Temperature (degrees K)
LiquidHeliumLevel (%)
ChamberPressure (mtorr)
2 mtorr readingduring H2 gas input
pressure riseduring regeneration
Cool-downto LHe
H2 Input Rate(torr-liters/s)
Total H2 Injected (torr-liters)
System PumpingSpeed, H2 (liters/s)
Time (minutes)300 2010
115120125130
5000
1000015000
0
0
100
2000
10
20300
20
40
0
80
40
50100150200
PlasmaShot
Warm-up andRegeneration
12,000 l/s
manually resetto zero priorto “shot”
Simulation of Multiple C-Mod Shot CyclesPrototype Test Chamber
- minimal LHe usage (2-3 liters/shot)
- 10,000 liters/s D2 High pumping speeds
- 12,000 liters/s H2
Excellent interface toC-Mod shot cycle
Efficient
Robust- survived up-to-air vacuum breach test with no damage to pump
- Cool-down/regen. ~8 min.cycle
4. Full-scale prototype tests3. Design
1031211027 EFIT: 1.000 Normalized Surface Heat Flux to Upper Cryo Tiles
0.45 0.50 0.55 0.60 0.65 0.70Major Radius (meters)
-0.2
0.0
0.2
0.4
0.6
0.8
1.0
1.2
SecondarySeparatrix
-1
0
1
2
3
4
5
degr
ees
Field Line Angle
Non-beveled tiles Beveled tiles
Normalized Surface Heat Flux to Lower Divertor Tiles
0.00 0.05 0.10 0.15 0.20Arc Length (meters)
-0.2
0.0
0.2
0.4
0.6
0.8
1.0
1.2
Nor
mal
ized
Hea
t Flu
xN
orm
aliz
ed H
eat F
lux Normalized
Heat Flux
NormalizedHeat Flux
midplane λq = 3.0 mm
PrimarySeparatrix
-1
0
1
2
3
4
5
degr
ees
Field Line Angle
All beveled tiles
Reference: "AT-target plasma" - 1.0MA, 5.4 tesla DN discharge with 4.7 MW RF, steady H-mode, 3.5 mtorr upper div. pressure
Cryopump slots positionedclose to upper x-point
- Exploits flux expansion- Peak heat fluxes similar to lower divertor
Cryopump scheme will handlehigh-power USN discharges
- Allows maximal pumping speed to be utilized for physics experiments
0.50 0.55 0.60 0.65 0.70 0.75
0.30
0.35
0.40
0.45
0.50
0.55
0.60
B. LaBombard19-JUN-2006
C-Mod Cryopump Simulation - Case CH1
0.50 0.55 0.60 0.65 0.70 0.75Major Radius (m)
0.30
0.35
0.40
0.45
0.50
0.55
0.60
Verti
cal H
eigh
t (m
)
B. LaBombard19-JUN-2006
-0.05 0.0 0.05Toroidal Direction (m)
Atoms Launched=10000Trajectories Shown=300Atoms Leaked=883Atoms Pumped=431Atoms Ionized=8686Charge Exchange Events=8314CX Reflected into Slot=2626Pumped/Launched=0.043
Hits on Inner/Outer Connector=449Source= 2.64E+22 D atoms/s 373.1 torr-l/s D2
Baffle Width (meters)=0.063Profile Shot#1021002017:800 1MA:2MW:nebar= 2.5:H-modeEFIT: 1031211007:0.660 SSEP = -1.3 mm
Pumping= 1.14E+21 D atoms/s 16.08 torr-l/s D2Gas inventory = 8.5 torr-l D2
Performance estimate:
Input:Measured SOL profiles,Pump/tile geometry,EFIT equilibrium
Output:Atoms pumped perion incident on divertortile surface
Baffle
LSN H-mode withSSEP ~ -1.3 mm
Initial density e-foldingtime ~ 0.5 seconds
Heat Flux Handling of Upper ‘Flat-Plate’ Divertor Surface is Comparable to Lower ‘Shaped’ Divertor
3D Monte Carlo Modeling provided design guidance and rough estimate of pumping performance
5. Cryopump Installation
C-Mod Cryopump Data 25-may-2007 - 26-may-2007
-40 -20 00
20
40
60 Liquid Nitrogen Inlet Pressure (psi)
-40 -20 0-150-100-50050 Nitrogen Exhaust Temperature (degrees C)
-40 -20 000.20.40.60.811.2 Liquid Helium Inlet Valve Setting (turns)
-40 -20 00
500
1000 Helium Exhaust Flow
-40 -20 0-200
-100
0Helium Exhaust Temperature (degrees C)
-40 -20 00
50
100 Liquid Helium Dipstick Level (%)
-40 -20 0-1e-701e-72e-73e-7 Linear IGT Pressure (Torr)
First cool-down of pump to LN2 and LHe temperatures
Liquid heliumon ‘dip-stick’
C-Mod base pressure drops an order of magnitudeTime (minutes)
LN2 cool-down
LHe cool-down
C-Mod Cryopump Data 25-may-2007 - 26-may-2007
440 450 460 470 48000.20.40.60.811.2 Liquid Helium Inlet Valve Setting (turns)
440 450 460 470 4800
500
1000 Helium Exhaust Flow
440 450 460 470 4800
50
100Liquid Helium Dipstick Level (%)
440 450 460 470 4800
1e-6
2e-6
3e-6 Linear IGT Pressure (Torr)
440 450 460 470 4800
10
20
30
40 TC3 Pressure (mTorr)
Seamless integration of cryopump operation with shot cycle (operated in a ‘manual’ mode for these shots)
RegenerationCooldownPlasma
Time (minutes)
6. First Operation in C-Mod
In-vessel orbital welding andleak testing of cryogenic tubing
LHe inlet
LHe exhaust
CryopumpLN2 shield
Halo currentRogowski coils
Cryopump
Hanger
10 instrumented ‘shim plates’30 sectors: shelf, plates, posts, baffles720 Moly tiles, fasteners, keepers, ...Probes, rogowskis & gauge instrumentation, ...
Gas Baffle
Gas Cuffs(for laser access)
Pumping Slots
Periscope
LHe transfer line fabrication
Cryogenic System on Top of C-Mod
LHe Dewar500 L
PLCRack
LHe stepper control valve
heatexchanger LHe line
LN2 line
Fabrication & Pre-assembly
External Cryogenics & Control System
Heliumtube
Inner LN2shield
Outer LN2shield
~1/30 Sector of Cryopump & Tile Structure
Installation of cryogenic loopin upper chamber
Finished installation of molybdenumtiles, support plates & baffles
Close-up of slot, gas baffle and in-vessel Penning gauge
Penninggauges
Gas BafflePumping Slot
Remote PLC Control Interface
C
G
D
C
G
D
C
G
D
C
G
D
C
G
D
- Guided by a series of passive pumping experiments, design evolved into a novel system of 30 'pumping slots'
- Pumping throughput insensitive to radial location of upper separatrix
Axisymmetric Concept “Pumping Slot” Concept
- Pumping throughput controlled dynamically via secondary separatrix
- Design accommodates vertical port laser access to Rmin= 0.62 m (Thomson, TCI, PCI,...)
=> Increased pumping
- Exploit SOL transport physics (large particle flux e-folding): Heat exhaust to lower div., pumping in upper div., employing near double-null discharges
1. ConceptC-Mod’s novel cryopump concept is driven by key challenges:
(1) Build an efficient, large-area cryopump in a C-Mod divertor with minimal impact on diagnostics and port usage
(2) Pump hydrogen (4.6 K surface temperatures)
(3) Minimize helium usage and cost/complexity of external cryogenic support systems
Ideas- Employ a full toroidal-loop cryogenic system => but this requires using the upper divertor!
- Use ‘pumping slot’ concept instead of axisymmetric design Improved particle throughput Reduced heat fluxes via poloidal flux expansion Diagnostic access aligned with pumping slots
2. Cryopump Project GoalsFull toroidal cryogenic loop in upper divertor chamber - one vertical port for feed lines
Upper divertor tiles/baffles arrangedfor optimal particle pumping -system of 30 'pumping slots'
All-welded design - in-vessel assembly using robotic 'orbital welder'
'Duplicate' of C-Mod pump fullyinstrumented and tested off-line in adedicated vacuum chamber
Liquid helium 'pot' design (4.2 K), capable of pumping hydrogen (4.6 K design target)
> 8,000 liters/s system pumping speedfor room temperature D2
Minimal interruption of line-of-sight access through C-Mod’s vertical ports
Divertor, tiles and cryogenic support structures designed to with-stand eddy current and halo current loads corresponding to a full-performance 2.0 MA (plasma current), 9 tesla (toroidal field) upward-going plasma disruption with a total halo current of 0.5 MA; detailed analysis to be performed with the aid of an ANSYS model of the elec-tromagnetic transients associated with a C-Mod disruption [1]
Rogowski coils embedded into the tile support structures to monitor halo current levels
Simple Monte Carlo modeling combined with C-Mod operational expe-rience to be used to optimize design
Gas pressure gauges (Penning and baratron type) and an embedded Langmuir probe array to measure divertor neutral pressures and plasma fluxes to the target plates
[1] Titus, P., et. al, "C-MOD cryopump design and analysis," presented at the 21st IEEE/NPSS Symposium on Fusion Engineering, Knoxville, TN, USA, 2005.
Test fit-up of full toroidal loopEnd view of 1/3 loop section
Aggressive puff/pump scenariosdemonstrated
Excellent L-mode density control at moderate densities
SS fueling at ~140 torr-l/s20,000 l/s pumping speed at pump entrance... may be important tool for H/D control during startup
We now can produce steady-statedischarges with continuous,non-recycling impurity injection
Example: Steady Ar injection (MP#502)
Shot# 1070830032Plasma Current (MA)
0.00.20.40.60.81.0
Line Density
05.0•1019
1.0•1020
ICRF Power (MW)
01234
Argon Gas Puff
026
10
Radiated Power (MW)
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.40.00.20.61.0
seconds
10705250260.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds
0.20.40.60.81.0
1020
m-2
NL04
0.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds
100
200
Torr-
l/s
Injection Rate
0.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds
2468
mto
rr
UDIV Pressure
0.0 0.5 1.0 1.5 2.0seconds
0
Effectiveness of cryopump for density control is determinedby plasma transport physics
Particle removal ratedrops dramatically asdivertor changes fromhigh to low-recyclingregime
0.0 0.5 1.0 1.5 2.0seconds0.0
0.5
1.0
MA Plasma Current
0.0 0.5 1.0 1.5 2.0seconds0.00.20.40.60.81.01.2
1020
m-2
Line Density
0.0 0.5 1.0 1.5 2.0seconds
050
100150
Torr-
l/s
Gas Injection Rate
0.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds010
20
mto
rr
Upper Divertor Pressure
0.0 0.5 1.0 1.5 2.0seconds02
46
amps
Divertor Probe Flux
0.0 0.5 1.0 1.5 2.0seconds
Pump on
Pump off
C-Mod’s intrinsicwall-pumping takesover role of ‘density control’at the lowest densities
Prompt L-H density riseset by pedestal formation
Cryopump does not alter thisphysics (nor does strong puffing!)
=> evidence of ‘stiff profiles’ and controlling ‘critical gradients’
Cryopump impacts pedestal densities over long time-scales (~0.5 s)
1070601030 & 290.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds0.00.51.01.52.0
1020
m-2
Line Density
0.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds
0
10
mm
Upper Null
0.0 0.5 1.0 1.5 2.0seconds
L-mode reference plasma
L-H density rise
Lower Null X-point Balance
Cryopump is found to affect the toroidal distribution of neutrals
“G-Side” pressure is LOWER“CB-Side” pressure is HIGHER
Puffing with cryopump ON...
This effect has been found to aid operationof J-port ICRF antenna
...because gas injection isat “B-Side”
A
B
C
D
E F
G
H
J
KB
G
CB
0.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds0.00.4
0.81.2
1020
m-2
Line Density
0.0 0.5 1.0 1.5 2.0seconds
050
100150
Torr
-l/s Gas Injection Rate
0.0 0.5 1.0 1.5 2.0seconds
0.0 0.5 1.0 1.5 2.0seconds0.00.2
0.40.6
mto
rr
‘G-Side’ Neutral Pressure
0.0 0.5 1.0 1.5 2.0seconds
0.00.5
1.01.5
mto
rr
‘CB-Side’ Neutral Pressure
Pump on
Pump off
“G-Side”
“CB-Side”
“B-Side” Gas Injection
Cryopump has also aided operations inreducing base pressure (’fixing leaks’)
1070525018 & 21
0.0 0.5 1.0 1.5 2.0seconds0.0
0.5
1.0
MA
Plasma Current 18
0.0
0.5
1.0Plasma Current 21
0.0 0.5 1.0 1.5 2.0seconds0.00.20.40.60.81.01.2
1020
m-2
NL04 18
0.00.20.40.60.81.01.2NL04 21
0.0 0.5 1.0 1.5 2.0seconds-500
50100150
Torr-
l/s
Injection Rate 18
-50050100150Injection Rate 21
0.0 0.5 1.0 1.5 2.0seconds12
14
16
mm
SSEP 18
12
14
16SSEP 21
0.0 0.5 1.0 1.5 2.0seconds010
2030
mto
rr
UDIV Pressure 18
010
2030UDIV Pressure 21
0.0 0.5 1.0 1.5 2.0seconds02
46
amps
UDIV P8 18
02
46UDIV P8 21
0.0 0.5 1.0 1.5 2.0seconds0
1
2
amps
UDIV P10 18
0
1
2UDIV P10 21
0.0 0.5 1.0 1.5 2.0seconds
0.0
0.5
1.0
amps
UDIV P11 18
0.0
0.5
1.0UDIV P11 21
C
G
D
Upper DivertorProbe Array
1 5 9 14
Cryopump Operation Does NOT Change Relationship Between Upper Divertor Plasma Conditions and Machine Parameters (Ip, ne,...)
Black Traces = Pump ONColor Traces = Pump Off
At same line density with pump OFF/ON: - Upper divertor Ion saturation currents are identical
Ion Saturation Currents
7. Performance Tests
20
40
60
Torr
-l/s D2 Injection Rate
0
2mto
rr
Torus Pressure
0 1 2 3 4seconds
0
5.0•103
1.0•1041.5•104
liter
s/s
System Pumping Speed
Pumping speed = 9.62E+03 liters/s
- Chamber ~ 3.5 mtorr
- Pumping speed ~ 9,600 liters/s
Cryopump Easily Exceeds D2 System Pumping Speed Target (> 8,000 l/s)
- D2 injection at ~35 torr-l/s
Pumping slot/baffles work as plannedUSN upper divertor pressures ~ LSN lower divertor pressures
- However, divertor pressures and pumping throughputs are sensitive to magnetic field direction
H-mode Response=> Upper pumping slots are just as effective in ‘compressing’ neutrals as C-Mod’s closed lower divertor structure
Lower Divertor Pressure
Plasma Current
NL04
Upper Divertor Pressure
Reversed Field Direction
0.0
0.5
1.0
MA
0.00.40.8
1020 m-2
NL04 21
05
10
mto
rr
05
10
mto
rr
0.0 0.5 1.0 1.5 2.0seconds
Upper Null - RedLower Null - Blue
Similar neutral pressures
Forward Field Direction
0.0
0.5
1.0
MA Plasma Current
0.00.40.8
1020 m-2
NL04
01020
mto
rr Upper Divertor Pressure
1020
mto
rr Lower Divertor Pressure
0.0 0.5 1.0 1.5 2.0seconds
Similar neutral pressures
1070720021 & 7200021070525013 & 525006
Embedded Langmuir Probe Array
Full toroidal loop in upper divertor, maximizing pumping speed
Gravity-feed liquid helium 'pot' design, capable of pumping hydrogen (4.6 K surfaces)
Minimal LHe usageNo LHe recirculation system
9,600 liters/s pumping speed demonstrated for D2
Optimized tile surface geometry for high-power USN dischargesUnique toroidal array of ‘pumping slots’ and gas baffles
=> In-vessel inspection: no significant melt damage occurred during 2007 run campaign, which had many USN discharges, ICRF > 3 MW
Embedded halo-current rogowski instrumentationTiles and structure designed for 2.0 MA, 9 tesla disruption
Embedded Langmuir probes for particle flux optimization
60-90 liters of LHe consumedduring full C-Mod run day
8. SummaryA novel upper divertor cryopumping system has been successfullycommissioned in Alcator C-Mod
Excellent density control in moderate density plasmasSteady-state puff & pump throughputs of ~140 torr-l/s demonstrated
Toroidal slot geometry ‘compresses’ neutrals effectivelyStatic neutral pressures similar to those attained in closed lower divertor
Dynamic control of pumping throughput via secondary separatrix
=> Additional experiments revealed effect to be caused by in/out divertor asymmetries
‘jog’ in x-point balanceinitiates pumping