Cryogenic Refrigeration Systems as an Enabling Technology ...
Cryogenic refrigeration For The LHC - Www.cea.fr
Transcript of Cryogenic refrigeration For The LHC - Www.cea.fr
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CryogenicCryogenic refrigerationrefrigeration for the LHCfor the LHC
Philippe Lebrun
CERN, Geneva, Switzerland
MaTeFu Spring Training School
Cadarache, 5-9 April 2009
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The The largestlargest scientificscientific instrument in the worldinstrument in the world……
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……basedbased on on advancedadvanced technologytechnology
23 km of 23 km of highhigh--fieldfield superconductingsuperconducting magnetsmagnets
operating in operating in superfluidsuperfluid heliumhelium atat 1.9 K1.9 K
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SuperconductorsSuperconductors for for highhigh--fieldfield magnetsmagnets
0
500
1000
1500
2000
2500
3000
6 7 8 9 10 11 12
B [T]
Jc [A
/mm
2]
NbTi @ 4.5 KNbTi @ 1.8 KNb3Sn @ 4.5 KLHC Spec Cable 1LHC Spec Cable 2
+ 3 tesla
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Cryogenic system layoutCryogenic system layout
• 5 cryogenic islands
• 8 cryogenic plants, each serving adjacent sector, interconnected when possible
• Cryogenic distribution line feeding each sector
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Configuration of Configuration of cryogenicscryogenics atat LHC LHC eveneven pointpoint
UpperCold Box
Interconnection Box
Cold Box
WarmCompressor
Station
LowerCold Box
Distribution Line Distribution Line
Magnet Cryostats, DFB, ACS Magnet Cryostats, DFB, ACS
ColdCompressor
box
Sha
ftS
urfa
ceC
aver
nT
unne
l
LHC Sector (3.3 km) LHC Sector (3.3 km)
1.8 KRefrigeration
Unit
New4.5 K
Refrigerator
Existing4.5 K
Refrigerator
1.8 KRefrigeration
Unit
WarmCompressor
Station
WarmCompressor
Station
WarmCompressor
Station
ColdCompressor
box
Even pointOdd point Odd point
MP StorageMP Storage MP Storage
UpperCold Box
Interconnection Box
Cold Box
WarmCompressor
Station
LowerCold Box
Distribution Line Distribution Line
Magnet Cryostats, DFB, ACS Magnet Cryostats, DFB, ACS
ColdCompressor
box
UpperCold Box
Interconnection Box
Cold Box
WarmCompressor
Station
LowerCold Box
Distribution Line Distribution Line
Magnet Cryostats, DFB, ACS Magnet Cryostats, DFB, ACS
ColdCompressor
box
Sha
ftS
urfa
ceC
aver
nT
unne
l
LHC Sector (3.3 km) LHC Sector (3.3 km)
1.8 KRefrigeration
Unit
New4.5 K
Refrigerator
Existing4.5 K
Refrigerator
1.8 KRefrigeration
Unit
WarmCompressor
Station
WarmCompressor
Station
WarmCompressor
Station
ColdCompressor
box
Even pointOdd point Odd point
MP StorageMP Storage MP Storage
UpperCold Box
Interconnection Box
Cold Box
WarmCompressor
Station
LowerCold Box
Distribution Line Distribution Line
Magnet Cryostats, DFB, ACS Magnet Cryostats, DFB, ACS
ColdCompressor
box
UpperCold Box
Cold Box
WarmCompressor
Station
LowerCold Box
Magnet Cryostats, DFB, ACS Magnet Cryostats, DFB, ACS
ColdCompressor
box
Sha
ftS
urfa
ceC
aver
nT
unne
l
LHC Sector (3.3 km) LHC Sector (3.3 km)
1.8 KRefrigeration
Unit
New4.5 K
Refrigerator
Existing4.5 K
Refrigerator
1.8 KRefrigeration
Unit
WarmCompressor
Station
WarmCompressor
Station
WarmCompressor
Station
ColdCompressor
box
Even pointOdd point Odd point
MP StorageMP Storage MP Storage
UpperCold Box
Interconnection Box
Cold Box
WarmCompressor
Station
LowerCold Box
Distribution Line Distribution Line
Magnet Cryostats, DFB, ACS Magnet Cryostats, DFB, ACS
ColdCompressor
box
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Cryogenic plants Cryogenic plants
1.8 K refrigeration units(2.4 kW @ 1.8 K)
4.5 K refrigerators(18 kW @ 4.5 K)
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Cryogenic storage and distributionCryogenic storage and distribution
GHe storage LIN storage
Cryo-magnet string Distribution line Interconnection box
Vertical transfer line
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Analysis & management of heat loadsAnalysis & management of heat loads
• Heat inleaks
– Radiation 70 K shield, MLI
– Residual gas conduction Vacuum < 10-4 Pa
– Solid conduction Non-metallic supports Heat intercepts
• Joule heating
– Superconductor splices Resistance < a few nΩ• Beam-induced heating
– Synchrotron radiation
– Beam image currents 5-20 K beam screens
– Acceleration of photoelectrons
– Beam halo absorbed in cold mass
Analysis Management
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SteadySteady--state heat loads [W/m]state heat loads [W/m]((CryomagnetsCryomagnets and distribution line in LHC arcs)and distribution line in LHC arcs)
* no contingency
0.110.424.607.7Total ultimate
0.110.401.827.7Total nominal
00.114.360Beam-induced ultimate**
00.091.580Beam-induced nominal**
00.100.0050.02Resistive heating
0.110.210.237.7Heat inleaks*
4 K VLP1.9 K LHe4.6-20 K50-75 KTemperature
3.070.89Photoelectron
0.050.05Beam-gas Scattering
0.820.36Image current
0.500.33Synchrotron radiation
ultimatenominal** Breakdown
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ScalingScaling lawslaws for LHC for LHC dynamicdynamic loadsloads
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UncertaintyUncertainty & & overcapacityovercapacity factorsfactors
• Uncertainty factor Fin– Lack of reproducibility in construction (e.g. MLI wraps)
– Variance of thermal processes at work (e.g. insulation vacuum)
– Evolution in time (ageing, contamination of reflective surfaces)
⇒ applied to static loads only, dynamic loads and their scaling known
from first principles
• Overcapacity factor Foc– Cooldown in finite time
– Refrigerator loading < 100 %
– Variability of machine performance
⇒ applied to sum of static load with uncertainty and dynamic load
⇒ no overcapacity applied to ultimate conditions
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OverallOverall factor on factor on installedinstalled refrigerationrefrigeration
• Installed refrigeration power
Qinstalled = Max [Foc (Fin Qstat + Qdyn nom); (Fin Qstat + Qdyn ult)]
• Values of uncertainty & overcapacity factors
– Fin = 1,5 at beginning of project
– Foc= 1,5
– Fin gradually lowered following refinement of project configuration and improved knowledge of component thermal performance
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Evolution of estimated heat loads & installed Evolution of estimated heat loads & installed
refrigeration capacity per LHC sectorrefrigeration capacity per LHC sector
0
10
20
30
40
50
YR 1987
PB 1991
WB 1993
YB 1995
Specif. 1997
Rev. 2000
As built
Hea
t loa
d @
50-
75 K
[kW
] Static Total Installed
0
2000
4000
6000
8000
10000
YR 1987
PB 1991
WB 1993
YB 1995
Specif. 1997
Rev. 2000
As built
Hea
t loa
d @
5-2
0 K
[W] Static Total Installed
0
1000
2000
3000
YR 1987
PB 1991
WB 1993
YB 1995
Specif. 1997
Rev. 2000
As built
Hea
t loa
d @
1.9
K [W
] Static Total Installed
0
10
20
30
40
50
60
YR 1987
PB 1991
WB 1993
YB 1995
Specif. 1997
Rev. 2000
As built
CL c
oolin
g [g
/s]
Static Total Installed
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Installed cooling duties in the LHC sectorsInstalled cooling duties in the LHC sectors
[g/s]274120-280 K
[W]3804303-4 K
[W]210024001.8 K
[W]1503004.5 K
[W]760077004.6-20 K
[W]310003300050-75 K
Low-load sectorHigh-load sectorTemperature
level
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Evolution of installed power to heat load ratioEvolution of installed power to heat load ratio
1
1.5
2
2.5
3
YR1987
PB1991
WB1993
YB1995
Specif.1997
Rev.2000
Asbuilt
Capa
city
rat
io [
-]
50-75 K 5-20 K 1.9 K CL cooling
Overcapacity target
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Procurement from industryProcurement from industry
• European industry (Air Liquide & Linde Kryotechnik) had demonstrated their competency and know-how in manufacturing turnkey helium refrigerators of medium or large capacity
– HERA (10 kW)
– LEP2 (6 kW, 12 kW)
• Most efficient approach was therefore to procure via a functional and interface specification
– Transform sector cooling requirements into refrigeration duties which can be reception-tested at cryoplant interface
– Clearly define interfaces to cryogenic and other systems
– Promote energy-efficient solutions
• Oligopolistic nature of market & desire to balance industrial returns among Member States led to split procurement under constraints
– Align prices to satisfy CERN lowest-bidder purchasing rule
– Impose convergence of non- or less-proprietary part of supply, i.e. compressor station and control system
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Conversion of Conversion of coolingcooling dutiesduties
fromfrom LHC LHC sectorsector to 4.5 K to 4.5 K refrigeratorrefrigerator
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Specified refrigeration capacitySpecified refrigeration capacity
for the LHC 4.5 K refrigeratorsfor the LHC 4.5 K refrigerators
41
4400
20700
33000
Newrefrigerator
27
4150
19500
31000
Upgradedrefrigerator
[g/s]20-280 K
[W]4.5 K
[W]4.5-20 K
[W]50-75 K
UnitTemperature level
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ScalingScaling lawslaws for for costcost of of cryogeniccryogenic He He refrigeratorsrefrigerators
(single cold box, no LIN (single cold box, no LIN precoolingprecooling, , controlscontrols excludedexcluded))
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How to specify an efficient He refrigeratorHow to specify an efficient He refrigerator
• Include capital & operating costs over amortization period (10 years)in adjudication formula
• Operating costs dominated by electricity
• Include externalities in electricity costs => 60 CHF/MWh– distribution & transformation on CERN site
– heat rejection in aero-refrigerants
• Establish shared incentive in the form of bonus/malus on measured vs. quoted electrical consumption
• Break “high efficiency = high investment” pseudo-rule: for given (specified) output, a more efficient plant is smaller, resulting in lower investment (direct & indirect) as well as cheaper operation
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How to How to makemake an efficient an efficient refrigeratorrefrigerator(exemplified on (exemplified on Carnot cycle Carnot cycle schematicschematic))
Tw
Tc
T
S
T
S
Tw
Tc
isentropicadiabatic
Cooling power
Widen the low-temperature end of the cycle as shown in the T-S diagram
Work Work
Ideal Real
∆S1 ∆S2
AB
C D
AB
C D
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T54.5 K - 20 K loads
(magnets + leads + cavities)
T7
T1
T2
T3
T4
T8
T6
E1
E7
E3
E4
E6
E8
E9a
E9b
E10
E11
E12
E13
LN2Precooler
20 K - 280 K loads
(LHC current leads)
50 K - 75 K loads
(LHC shields)
Adsorber
T1
T3
T7
T4
T8
T5
T6
201 K
75 K
49 K
32 K
20 K
13 K10 K
9 K
4.4 K
0.1 M
Pa
0.4 M
Pa
1.9 M
Pa
0.3 M
Pa
T2
LHC shields
To LHC loads
from LHC loads
from LHC loads
ProcessProcess cycle & Tcycle & T--S S diagramdiagram
of 18 kW @ 4.5 K of 18 kW @ 4.5 K cryoplantcryoplant
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Compressor station of 4.5 K refrigeratorCompressor station of 4.5 K refrigerator
ORSHP supply
MP return
LP return
LP compressors
HP compressors
Oil removal system
Gas coolers
800 g/s @ 1.05 bar
880 g/s @ 3.9 bar
1680 g/s @ 20 bar
Electrical power consumption: 4 MW
Identical installation for both suppliers
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Compressor station of 4.5 K refrigeratorCompressor station of 4.5 K refrigerator
(Power input ~ 4 MW)(Power input ~ 4 MW)
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Cold box of Air Cold box of Air LiquideLiquide 4.5 K refrigerator4.5 K refrigerator
HP
MP
LP
300 K 75 K 50 K 20 K
4.5 K supply
20 K return
75 K return
50 K supply
4.5 K
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Cold box of Air Cold box of Air LiquideLiquide 4.5 K refrigerator4.5 K refrigerator
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Cold box of Cold box of LindeLinde 4.5 K refrigerator4.5 K refrigerator
4.5 K supply
20 K return
50 K supply
75 K return
HP
MP
LP
300 K 90 K 75 K 50 K 20 K 4.5 K
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Cold box of Cold box of LindeLinde 4.5 K refrigerator4.5 K refrigerator
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Guaranteed Guaranteed vsvs measured performancemeasured performance
of the new LHC 4.5 K refrigerators of the new LHC 4.5 K refrigerators
231222247248COP [W/W]
99.3100.1101.597.3Measured cryogenic capacity[% of specified]
4095396444744297Measured energy consumption [kW]
4275427542044204Guaranteed energy consumption [kW]
LindeLindeAir LiquideAir LiquideSupplier
PA8PA6PA4PA18LHC location
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C.O.P. of large C.O.P. of large cryogeniccryogenic heliumhelium refrigeratorsrefrigerators
0
100
200
300
400
500
TORESUPRA
RHIC TRISTAN CEBAF HERA LEP LHC
C.O
.P. [
W/W
@ 4
.5K
]
Carnot Limit
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Liquid nitrogen Liquid nitrogen precoolingprecooling
• Each 3.3 km sector has a mass of 4625 t to be cooled in few weeks
• Corresponding power 600 kW, must be generated by vaporization of 1250 t LIN at rates of up to 5 t/h
• LIN precooling not foreseen for steady-state operation, but may alsobe used to boost helium liquefaction
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First First cooldowncooldown of LHC of LHC sectorssectors
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Challenges of power Challenges of power refrigerationrefrigeration < 2 K< 2 K
1
10
100
1000
10000
0 1 2 3 4 5 6
Temperature [K]
Pre
ssur
e [k
Pa]
SOLID
VAPOUR
He IHe IICRITICAL
POINT
PRESSURIZED He II(Subcooled liquid)
SATURATED He II
SUPER-CRITICAL
SATURATED He I
Compression > 80
• Compress large mass-flow rate of gaseous helium across high pressure ratio
⇒ maximum density at suction, i.e. cold
• Non-lubricated, contact-less machinery ⇒ hydrodynamic compressor, multistage
• Heat of compression rejected at low temperature ⇒ high thermodynamic efficiency
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Main Features of LHC Cold CompressorsMain Features of LHC Cold Compressors
Axial-centrifugalimpeller (3D)
Fixed-vanediffuser
3-phase inductionelectrical motor(rotational speed 200 to 700 Hz)
Activemagneticbearings
300 K under
atmosphere
Cold under
vacuum
Inlet
Outlet
Pressure ratio2 to 3.5
Spiral volute
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Cold Cold hydrodynamichydrodynamic compressorscompressors for the LHCfor the LHC
IHI-Linde Air Liquide
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Specification of LHC 1.8 K refrigeration unitsSpecification of LHC 1.8 K refrigeration units
Steady state operation modes:– Installed pumping capacity 125 g/s at 15 mbar(i.e. ~2.4 kW @ 1.8 K)
– Turndown capability: 1 to 3 without extra liquid burning
– Cold return temperature to the 4.5 K refrigerator below 30 K (reduced capacity) to 20 K (installed capacity).
– Capacity check in standalone mode (Interface B closed)
0.3 MPa4.6 K
0.13 MPa,20 -30 K
WC
S
1.8
K R
efri
gera
tion
Un
it
LHe 1.8 K Q1.8K
CC
B
4.5 KRefrigerator
B
D
C
Col
d co
mpr
esso
rs
Tur
blne
Adsor-bers
LHC SectorLoad
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1.8 K 1.8 K refrigerationrefrigeration cycles for the LHCcycles for the LHC
1.8 K Refrigeration Unit Cycles
CC
Hea
tIn
terc
epts
Air Liquide Cycle IHI-Linde Cycle
4 K, 15 mbar124 g/s
20 K, 1.3 bar124 g/s
0.35 bar
4.75 bar
4 K, 15 mbar124 g/s
20 K, 1.3 bar124 g/s
0.59 bar
9.4 bar
4.6 bar
CC
CC
CC
CC
CC
CC
CC
T
T
T
Adsorber
Adsorber
WC
WC
WC WC
HX
HX
HX
HX
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Isentropic efficiency of cold compressorsIsentropic efficiency of cold compressors
0
10
20
30
40
50
60
70
80
1985 1993 2000Year of construction
Isen
trop
ic e
ffici
ency
[%]
Tore Supra
CEBAF
LHC
12
12'is HH
HHη
−−=
Temper
atur
e (T
)
Entropy (s)
P1
P2
1
2
2'
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C.O.P. of LHC 1.8 K refrigeration unitsC.O.P. of LHC 1.8 K refrigeration units
0
200
400
600
800
1000
Air Liquide IHI-Linde
CO
P [W
@R
T /
W@
1.8K
]4.5 K refrigerator part 1.8 K refrigeration unit part
Carnot Limit
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Controls for LHC cryogenicsControls for LHC cryogenicsChallenges & solutionsChallenges & solutions
UNICOS framework providing1. Programmable logic controllers (PLC) and associated hardware2. Programming rules and code library for common objects3. Automated tools for writing control code4. Gateways based in industrial PC for WorldFIP-based signal conditioners5. Communication via Ethernet gateways <-> PLC and PLC <-> PLC6. Event-driven communication protocol between PLC <-> SCADA7. SCADA based in PVSS with generic widgets, look-and-feel and shared data
server
4704481003285483680Closed Loop Controllers
421227223211849561568Digital Outputs
183565921144398481004536Digital Inputs
700811229260811404856Analog Outputs
2133621611282640521612136Analog Inputs
TOTALCommonQUI1.8 K units4.5 K
refrigeratorsTunnel
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Control system architectureControl system architecture
• Field layer- Interface to process direct
I/O Boards, Fieldbuses
• Process control layer- PLC : the control logic is
performed at that level- Programmers act on that
Level
• Supervision layer- Interface for operation team - All operators action are
taken from this level
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OperatorOperator--friendlyfriendly SCADASCADA
Animatedsynoptics
Alarm & event lists
PID controllers
Trend charts
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SomeSome referencesreferences
• Ph. Lebrun, Cryogenics for the Large Hadron Collider, IEEE Trans. Appl. Superconductivity 10 (March 2000) 1500-1506
• S. Claudet, P. Gayet & U. Wagner, Specification of four new large 4.5 K helium refrigeration systems for the LHC, Adv. Cryo. Eng. 45B (2000) 1269-1276
• S. Claudet, P. Gayet, B. Jager, F. Millet, P. Roussel, L. Tavian & U. Wagner, Specification of eight 2400 W @ 1.8 K refrigeration units for the LHC, Proc. ICEC18 Mumbai, Narosa (2000) 207-210
• Ph. Lebrun, Large cryogenic refrigeration system for the LHC, Proc. ICCR’2003 Hangzhou, IIR (2003)
• H. Gruehagen & U. Wagner, Measured performance of four new 18 kW @ 4.5 K helium refrigerators for the LHC, Proc. ICEC20 Beijing, Elsevier (2005) 991-994
• L. Serio et al., Validation and performance of the LHC cryogenic system through commissioning of the first sector, Adv. Cryo. Eng. 53B (2008) 1411-1418
• S. Claudet, Ph. Lebrun, L. Serio, L.Tavian, R. van Weelderen & U. Wagner, Cryogenic heat load and refrigeration capacity management at the Large Hadron Collider, presented at ICEC22 Seoul (2008)