LCLS-II 1.3 GHz CM Demagnetization & Active Cancellation - - PowerPoint PPT Presentation
LCLS-II 1.3 GHz CM Demagnetization & Active Cancellation - - PowerPoint PPT Presentation
LCLS-II 1.3 GHz CM Demagnetization & Active Cancellation Saravan K. Chandrasekaran Technical Review Meeting for BCR May 25, 2016 Outline Introduction Previous work Residual magnetic fields and Q 0 pCM test plan for
Outline
- Introduction
– Previous work – Residual magnetic fields and Q0
- pCM test plan for demagnetization & active cancellation
– Understanding till now, & what remains to be understood
- Production demagnetization & active cancellation coil
– Proposed design of coils and connectorization – Cost summaries for different options – Need-by schedule
- Operational modes
– Information for SLAC controls
5/25/2016 S.K. Chandrasekaran | LCLS-II CM Demag & Active Cancellation Tech. Review 2
Outline
- Introduction
– Previous work – Residual magnetic fields and Q0
- pCM test plan for demagnetization & active cancellation
– Understanding till now, & what remains to be understood
- Production demagnetization & active cancellation coil
– Proposed design of coils and connectorization – Cost summaries for different options – Need-by schedule
- Operational modes
– Information for SLAC controls
5/25/2016 S.K. Chandrasekaran | LCLS-II CM Demag & Active Cancellation Tech. Review 3
Magnetic scope, specifications & sources
- First large CW project where magnetic shielding being analyzed
stringently, especially longitudinal component of magnetic field
– Bavg ↓ → Rs ↓ → Q0 ↑ → Pdiss↓ → $oper ↓
- LCLS-II specification [1]:
– Bavg<5 mG to reach Q >2.7E10 at 2 K, 16 MV/m
- Major magnetic field sources: vacuum vessel, components, earth
– Bvessel< 3 G [2] – Bcomponents~ 1 G – Bearth≈ 483 mG at SLAC [3] – B//,beamline≈ 150 mG
- Most analyses done assuming SLAC tunnel magnetic fields
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[1] “1.3 GHz Superconducting RF Cryomodule,” Functional Requirements Document, LCLSII-4.5-FR-0053. [2] A. Crawford, arXiv:1507.06582v1. [3] National Oceanic and Atmospheric Administration, 2014--2019 World Magnetic Model.
Trapped Magnetic Flux & Q0
- Smaller ambient magnetic fields beneficial
– For high Q & for low flux expelling material
- Q0>3 x 1010 may be realized for trapped B<3 mG
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↓B ↑ ↑Q0
- M. Martinello et al., IPAC 2016
- S. Posen et al., arXiv 2016
Benefits of degaussing vessel [4,5]
- Vessel must be degaussed
after final handling
– Fields in steel could be ~200 G when exposed to ~500 mG
- Edge ~factor of 3 reduction
- Central ~factor of 2 reduction
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[4] A. Crawford, arXiv:1409.0828v1. [5] A. Crawford, arXiv:1503.04736v1.
- Expt. With B// ≈50 mG
- 400
- 300
- 200
- 100
100 200 300 400 1 2 3 4 5 6 7 8 9 10 11 B [milligauss] Z [meters] Bz Pipe Before DeMag Bz Pipe After 600 A-Turns/m
What Q to expect with & without demagnetization & compensation coils?
- At 2 K, 16 MV/m
- RBCS = 4.5 nΩ, R0 = 1.5 nΩ
- Rs = RBCS + R0 + (Flux trap. sens. x Bavg)
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Scenario Flux trapping sensitivity (nΩ/mG) Demag. & Comp. coil? Bavg (mG) Rs (nΩ) Q (x1010)
- Oper. cost
(M$) ($100/MW-h) [13] Realistic 0.5 [10,11] No 15 13.5 2 4.6 Yes 3 7.5 3.5 <3.4 Conservative (100% trapping) 1.2 [12] No 15 24 1.1 >>5.7 Yes 3 9.6 2.8 3.5
[10] D. Gonnella et al., J. Appl. Phys. 117, 023908, 2015. [11] A. Grassellino et al., SRF proceedings, MOP028, 2015. [12] M. Martinello et al., SRF proceedings, MOPB015, 2015. [13] J. Theilacker, personal communication with A. Grassellino, 2015.
- Q=3.5x1010 higher gradient operation possible
- Q=1.1x1010 current cryoplant capacity insufficient
Outline
- Introduction
– Previous work – Residual magnetic fields and Q0
- pCM test plan for demagnetization & active cancellation
– Understanding till now, & what remains to be understood
- Production demagnetization & active cancellation coil
– Proposed design of coils and connectorization – Cost summaries for different options – Need-by schedule
- Operational modes
– Information for SLAC controls
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Overview
- Overall goal:
– Prove the importance of demagnetization & active cancellation systems to the performance of the cryomodules
- Testing in three phases
– Phase I: Vacuum vessel only
- pCM assembly schedule must be unaffected
– Phase II: Coldmass as it transitions into cryomodule
- pCM assembly schedule must be unaffected
– Phase III: Cryomodule at CMTS
- Data for production readiness review is priority
- Cooldowns for understanding other systems/overall pCM beyond the
scope of this topic
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Phase I: Vacuum vessel (VV) only
- Goal: Obtain data for the effects of physical
movement & transport on the residual magnetic field of the VV 1. Measure the remnant field inside VV
a. Beamline, top & bottom equator locations
2. Wind coils to VV 3. Demagnetize VV 4. Measure the remnant field inside VV 5. Pick up VV, move inside building using crane, rotate 360°, set down where it was before 6. (If time permits) Transport VV on an air-ride equipped flatbed truck for ~10 miles inside FNAL 7. Measure the remnant field inside VV 8. (If time permits) Test tune active cancellation coils
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pCM Vacuum Vessel Demagnetization
- Wires wound onto the outer surface of vessel
- Used Powerpole connectors to test them for use in the ‘belt’
type system
- FNAL electrical standards determined size of wire
– NFPA-70 = AWG 6; FNAL = AWG 4 – Strand count not taken into consideration due to low duty factor – HI-POT testing of insulation required at FNAL after each move
- f vessel with coils, or installation of coils if removed
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Results: VV demagnetization (B magnitude)
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Bavgat cavities >500 mG ↓ <50 mG & uniform
Results: VV demagnetization (B longitudinal)
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Bz at cavities >300 mG ↓ <50 mG & uniform
Effect of crane handling
- Handling
– Lifted demagnetized VV using crane, moved within building while slung from crane, rotated 360°, set back down
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Effect of transport
- Transport
– Set demagnetized VV on air-ride equipped, lowboy, flatbed truck – Drove within Fermilab for 10 miles, max. speed 30 mph
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Results: Effect of crane handling & transport
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- No change in magnetic field distribution within VV after
handling and transport experiments
- Demagnetization may not be required after each move for
each CM
Phase II: Coldmass as it transitions into CM
- Goal: Obtain data with and without vessel
1. Measure magnetic field at cavities when coldmass attached to Big Bertha, before VV is slid on
a. Fluxgates in longitudinal direction outside cavities’ helium vessel, & azimuthal direction inside cavities’ helium vessels
2. Re-measure magnetic field at cavities after VV slid on, and CM is formed
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Phase III: Cryomodule at CMTS
- Goal: Prove effectiveness & need for demagnetized VV (dVV) & active
cancellation (AC) 1. Install CM at CMTS 2. Before cooldown, tune AC coils to obtain minimal longitudinal mag. field
a. Compare fields without & with AC – prove effective
3. Demagnetize VV/CM if deemed necessary 4. Cooldown (#1) with dVV, AC ON, fast cooldown (FCD)
a. Determine Q0 of cavities at nominal gradient b. Provide data for production readiness review, best case scenario
5. Cooldown (#2) with dVV, AC ON, slow cooldown (SCD)
a. Determine Q0 of cavities at nominal gradient b. Baseline for SCD, with best case magnetic fields
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Phase III: Cryomodule at CMTS
6. Warm-up, cooldown (#3) with dVV, AC OFF, FCD
a. Determine Q0 of cavities at nominal gradient b. Isolate contribution of un-cancelled longitudinal magnetic fields
7. Simulate non-ideal VV (non-dVV) 8. Warm-up, cooldown (#4) with non-dVV, AC OFF, FCD
a. Determine Q0 of cavities at nominal gradient b. Isolate contribution of VV demagnetization
9. Warm-up, cooldown (#5) with non-dVV, AC OFF, SCD
a. Determine Q0 of cavities at nominal gradient b. SCD with worst-case magnetic fields (at CMTS)
- 10. Warm-up, non-dVV, AC ON
a. Determine if non-dVV longitudinal field can be cancelled b. Transverse field still remains
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pCM understanding
- Proven:
– LCLS-II 1.3 GHz VV has varying magnetic fields (>500 mG) in as-received state – VV can be successfully demagnetized – Demagnetization after each move may not be needed
- Yet to be proven:
– Beneficial effects of demagnetization on Q0 pCM tests – Beneficial effects of active cancellation on Q0 pCM tests – No detrimental effects on other components within CM
- First measurements by A. Crawford in 2014 indicate no effects
- Tuner motor, piezo, instrumentation being checked again
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Outline
- Introduction
– Previous work – Residual magnetic fields and Q0
- pCM test plan for demagnetization & active cancellation
– Understanding till now, & what remains to be understood
- Production demagnetization & active cancellation coil
– Proposed design of coils and connectorization – Cost summaries for different options – Need-by schedule
- Operational modes
– Information for SLAC controls
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Production demagnetization & active cancellation coils
- Due to the need for demagnetization after each move not
being present, proposal is to separate the two systems
- Demagnetization to use AWG 4 cables
– Connectorized belt-type system – 1-set per Lab, 1-spare for both – Install at QC, remove – Install at CMTS, remove – Installation at SLAC not accounted for in estimates
- Active cancellation to use AWG 22 or larger cables
– Connectorized belt-type system or wound around the vessel – To be left on CM permanently
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Demagnetization coils
- Main body (5-turn) coils
– Powerpole connectors mounted to backing plate – Backing plate doubles as fastening & locking mechanism – All connectors along a line on vessel outside (bottom or side)
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Powerpole Backing plate
Demagnetization coils
- End (100-turn) coils – same concept as main coils
– Each layer is a separate ‘belt’ – 10 layers X 10 turns coils: 10 ‘belts’ of 10 turns (inc. lengths) – 20 layers X 5 turns coils: 20 ‘belts’ of 5 turns (inc. lengths) – Connector locations to be offset by 60°
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Upstream end 10 X 10 Downstream end 20 X 5
Active cancellation coils
- AWG 22 or 18 (FNAL electrical safety and stranding)
- Ribbon cable a possibility
– FNAL safety not big on using ribbon cable for constant current conduction
- Can be connectorized using similar hardware as
demagnetization system
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Cost summaries
System Includes Cost ($) Demagnetization 1-set FNAL, 1-set JLAB, 1-set spare, labor for 2 install & removal 357,296 Active cancellation Only CM internal components purchased now; external wires etc. in operations (use demag wires in CMTS) 358,113 Active cancellation Full system installed during production 746,167
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$715,409 $1,103,463 Option #1 Option #2
Need by dates
- Fluxgates:
– Lead time ~12 weeks – CM2 at WS2 to be started ~October 21 – Fluxgates for CM2 to be ordered by mid-June
- Cables:
– 90 C insulation wire lead time ~2 weeks – 105 C insulation wire lead time ~8 weeks – VV to be arriving soon…
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Outline
- Introduction
– Previous work – Residual magnetic fields and Q0
- pCM test plan for demagnetization & active cancellation
– Understanding till now, & what remains to be understood
- Production demagnetization & active cancellation coil
– Proposed design of coils and connectorization – Cost summaries for different options – Need-by schedule
- Operational modes
– Information for SLAC controls
5/25/2016 S.K. Chandrasekaran | LCLS-II CM Demag & Active Cancellation Tech. Review 28
Signal list (active cancellation)
- Active cancellation
– 5 Fluxgates per CM (4-wires per fluxgate)
- Extension wires must be low resistance
– 3-active cancellation circuits per CM (2-wires per circuit)
- Extension wires must be low resistance
- Demagnetization
– Power supply controlled through 1-USB – 3-phase, 208 V, 30 A; L21-30R receptacle
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Operational modes
- Commissioning:
– FGs read & coils tuned during commissioning – FGs read during cool downs – Tuning temperature to be determined from pCM tests
- Algorithm to use FG data to tune coils
– Demagnetize if unable to cancel magnetic fields
- Normal Operations:
– After current tuned, coils ALWAYS ON
- To prevent flux trapping in the event of cavity quench
– FGs monitored all the time (multiplexing OK) – Data reviewed and coils adjusted during shutdowns – Demagnetize if unable to cancel magnetic fields
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Thank you!!!
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