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Summary of thermal manage ment meeting Summary of thermal management Summary of thermal management working group meeting, working group meeting, December 6 December 6 Presentations Presentations Introduction (G. Viehhauser, Oxford) Reutilisation of present tubing plant (G.V.) Status reports for different coolants: Light fluorocarbons (G. Hallewell, CPP Marseille) CO 2 (A. Colijn, NIKHEF) Flow control with thermostatic expansion valves (N. Hessey, FOM/NIKHEF) Recent experience from cooling system commissioning (R. Bates, Glasgow) From current cooling installation to future CS upgrade for ATLAS ID (V. Vacek, CTU, Prague) Thermal Management Issues for Stave Structures (C. Haber, LBNL)
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Page 1: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Summary of thermal managementSummary of thermal management working group meeting, December 6 working group meeting, December 6

PresentationsPresentations• Introduction (G. Viehhauser, Oxford)

• Reutilisation of present tubing plant (G.V.)

• Status reports for different coolants:– Light fluorocarbons (G. Hallewell, CPP Marseille)

– CO2 (A. Colijn, NIKHEF)

• Flow control with thermostatic expansion valves (N. Hessey, FOM/NIKHEF)

• Recent experience from cooling system commissioning (R. Bates, Glasgow)

• From current cooling installation to future CS upgrade for ATLAS ID (V. Vacek, CTU, Prague)

• Thermal Management Issues for Stave Structures (C. Haber, LBNL)

Page 2: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

MEANS COOLANTS

Page 3: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Issues: Try to use as much of the existing pipework as possible (mainly the tubing through the magnet to the ID volume) External components on access platforms and in USA15

can be considered less static:

Much hinges on delivery and evaporation pressure of final coolant, impedance to evacuate vapour,

critical temperature of chosen fluid

Page 4: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Operating temperature of silicon detectors

Can we estimate a Si operation temperature for sufficient safety margin @ L>>1034?

From Nobu Unno’s September 6th talk: -30°C on SCT Sensors, requiring (my guess) ~-45C evaporation

in on-detector cooling channels

15°C (Si – coolant) T Reasonable? Conservative?...

Page 5: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Power dissipation of silicon detectorelectronics

No estimate given (anywhere in this conference)of dissipation of electronics

(Given the much higher activity within the electronics+ reduced radius (1/r2) of new B layer, extra track /

background activity at luminosities ~ 1035

Page 6: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

The fluids…Two (maybe 3) candidate fluids: C2F6, CO2 & (maybe still) C3F8

A few pros and cons:C2F6: Enthalpy ~ 100J/g, Pevap~ 4 bara @ -45°C, Tcrit ~ 20°C

Liquid delivery pressure in warm zones ≥ 30 bar

CO2: Enthalpy ~ 280J/g Pevap ~ 7 bara @ -45°C, Tcrit ~ 30°CHigher evaporation pressure higher HTCTriple point temperature ~ -56°C (dry ice formation) Liquid delivery pressure in warm zones ≥ 70 bar

C3F8: Enthalpy~100J/g, Pevap < 1 bara*@ -45°C, Tcrit ~ 60°C * low evaporation pressure needs special treatment

Page 7: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

ATLAS SCT & Pixels: Principle of present C3F8 system

Vapour h.p.

Vapourl.p.

Liquidh.p.

Liquidl.p.

Déverseur/Back-pressureregulator for

groups of circuits(Individual Pevap)

Performancesqueezed here!

Page 8: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Possible cycle with CPossible cycle with C22FF66

Surface condenser

Evaporation @ -45°C:

CompressorPin~4.5bara, Pout~15bar

Detent

gh liquid return to pit

Atten

Attention: Tcrit ~20°C

ΔH ~ 110 J/g

Page 9: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

ΔH(-35C) = 280 kJ/kg

Enthalpy [kJ/kg]

Pre

ssur

e [b

ar]

P = 12 bar

liquid

2-phase gas

CO2 properties: p-H diagram

Attention: Tcrit ~30°CP = 60barAttention: Pdeliv ~ 60bar

Page 10: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Problems with the present CProblems with the present C33FF8 8 systemsystem(Which might require ‘external’ intervention)(Which might require ‘external’ intervention)

(1) Back-pressure regulators contribute substantial (& variable) insertion loss (CV variability) being mastered…;

(2) Significant insertion loss in deeply embedded hex’s, heaters;

(1) & (2) low compressor aspiration pressure (~1barabs)

(3) Very high compression ratio xacross compressors due to the very high choice of condenser pressure;

(1), (2) & (3) conspire to put the compressor in a regime of reduced throughput (pumping speed) and hotter operation

Cooling circuits have little margin for reducing Si temperature. Cooling circuits have little margin for reducing Si temperature. Also compressor cooling less efficient: Also compressor cooling less efficient:

(reduced flow of cooling gas) (reduced flow of cooling gas) expect a reduced MTBF? expect a reduced MTBF?

Page 11: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

HEX DCSDetector DCSDet. environmental DCS

Heaters DCS

Off-detector layout, inc DCS

Page 12: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

ATLAS pit(d ~ 92m)

ATLAS Surface Buildings

USA15

Remote Control Pressure regulatorsPin ~ 14bar

(flow proportional to heat load)

Compressors

Condensers operatingWith lower input pressure

than in USA15 location

Tracker

Examplegh(liquid)bar(C3F)

Example:gh(vapour)m

bar(C3F)

Toward a simplified circulator with reduced compressor stress(and enhanced compressor M.T.B.F.)

Tubing to be sizedfor dynamic P

Page 13: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

There is yet space!

Page 14: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

A ‘graded external fix’ approach to A ‘graded external fix’ approach to problems with the present Cproblems with the present C33FF8 8 systemsystem

(Integrable steps in the cooling system for the tracker upgrade)(Integrable steps in the cooling system for the tracker upgrade)

APPROACH (1)APPROACH (1)Eliminate back-pressure regulators +

use compressor aspiration tank pressures (by varying compressor speed using motor speed controller) to control evaporation pressure in pixel and SCT circuits

Moduarity issues?Moduarity issues?

Page 15: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

A ‘graded external fix’ approach to A ‘graded external fix’ approach to problems with the present Cproblems with the present C33FF8 8 systemsystem

IF APPROACH (1) DOES NOT SUFFICIENTLY INCREASEIF APPROACH (1) DOES NOT SUFFICIENTLY INCREASESi DETECTOR OPERATING TEMPERATURE MARGIN…Si DETECTOR OPERATING TEMPERATURE MARGIN…

APPROACH (2) Install ‘local’ (COLD C) condensers (service platforms) Condenser cooled either using LN2 /Gfrom liquid argon calorimeter cooling loops or a compressor system (R404A?)

How to circulate CHow to circulate C33FF88 primary coolant back to capillaries?: primary coolant back to capillaries?:

(2-i) Using liquid pumps (hydraulic or pneumatic drive for B field)(2-i) Using liquid pumps (hydraulic or pneumatic drive for B field)

(2-ii) Using 2(2-ii) Using 2ndnd (external) evaporator (external) evaporator & existing Haug Compressors in USA15& existing Haug Compressors in USA15

Page 16: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

A ‘graded external fix’ approach to A ‘graded external fix’ approach to problems with the present Cproblems with the present C33FF8 8 systemsystem

IF APPROACH (1) DOES NOT SUFFICIENTLY INCREASEIF APPROACH (1) DOES NOT SUFFICIENTLY INCREASESi DETECTOR OPERATING TEMPERATURE MARGIN…Si DETECTOR OPERATING TEMPERATURE MARGIN…

APPROACH (2) Install ‘local’ (COLD C) condensers (service platforms) Condenser cooled either using LN2 /Gfrom liquid argon calorimeter cooling loops or a compressor system (R404A?)

How to circulate CHow to circulate C33FF88 primary coolant back to capillaries?: primary coolant back to capillaries?:

(2-i) Using liquid pumps (hydraulic or pneumatic drive for B field)(2-i) Using liquid pumps (hydraulic or pneumatic drive for B field)

(2-ii) Using 2(2-ii) Using 2ndnd (external) evaporator (external) evaporator & existing Haug Compressors in USA15& existing Haug Compressors in USA15

Page 17: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

USA15

Remote controlpressure regulators

Pin ~ 14-17bar

Haug compressors in USA15

Low temperature condenser operating on GN2 (LN2 boiloff) or else R404a, ex

C3F8 compressor system(Condenser at highest point on ATLAS platforms)

Tracker

Liquid pump (possibly 2-stage):Hydraulic/pneumatic drive for high B-field operation

Must generate ~14-17 bar C3F8 capillary input pressure

2.i Enhancing Si operating temperature margin of the present C3F8 evaporative cooling system

Priming height(maximum possible)

h(liquid)m bar(C3F)

(boosts pump output)

Use Haug compressors tocool local condensers in UX

(no longer in primary cooling loop)

Page 18: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Principle of modified P-H cycle : recovery of present C3F8 system

P (T) between Evaporation & Condensation determined by sizing

of exisiting internal services

Condensation

Evaporation @-45°C

P liquid via(2-stage?)

pump

Pressure regulators & present choiceof capillary (Ø,L)

Page 19: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Fluorocarbons can be mixed (blended ) to arrive at compromise thermodynamic properties

(many modern refrigerants are blends) This was tested with C3F8/C4F10

(2 papers in Fluid Phase Equilibria 2000-2001)

Mixture thermodynamic, transfer properties calculated & set up as ‘temporary’ folders in NIST database verified

by measurement (sound velocity in superheated phase)

Page 20: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

CO2 Status report A. Colijn, NIKHEF

• CO2: Why?

• CO2: Cooling system for LHCb vertex detector

• CO2: Research plans at NIKHEF

Page 21: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

ΔH(-35C) = 280 kJ/kg

Enthalpy [kJ/kg]

Pre

ssur

e [b

ar]

P = 12 bar

liquid

2-phase gas

CO2 properties: p-H diagram

Attention: Tcrit ~30°C

Page 22: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

LHC-b ‘VELO’ vertex tracker CO2 cooling system: (NIKHEF)

2-phase

gas

R404a chiller

22

33

6677

11

88

44

2-phase2-phase

liquid liquid liquid

2-phase

Con

den

ser Evaporators

Concentric tubePump

Rest

rict

ion

AccumulatorCooling plant area

Transfer lines(~50m) VELO area

55

liquid

Fully assembled under testingInstalled nowUnder

construction

VELO areaCooling plant area

detectors

Page 23: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

VTCS cooling cycle

CO2 Cooling at NIKHEF 8 May 2006 Bart Verlaat 13

VTCS CO2 cycle in the Pressure – Enthalpy diagram

-450 -400 -350 -300 -250 -200 -1505x102

103

104

2x104

h [kJ/kg]

P [k

Pa]

-40°C

-30°C

-20°C

-10°C

0°C

10°C

0.2 0.4 0.6

Tertiary VTCS in P-H diagram

1

23

4

5

67

Accumulator pressure = detector temperature

Transf er tube heat exchange brings evaporator pre expansion per defi nition right above saturation

Saturation line

Capillary expansion brings evaporator blocks in saturation

Detector load

Page 24: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

LHCb: Mechanical constructionAccumulator

CO2 pumps

Heat exchanger

Automatic valves

FRONT

BACK

Page 25: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

NIKHEF & CO2: Cooling plant

Test setupCompact CO2 cooling plant

Primary CO2 cooler

Acc

umul

ator

Con

dens

orPump

Heat exchanger

Secondary CO2 circulation circuit

Compressor (with oil)

cond

enso

r

Detector

Page 26: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Page 27: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Page 28: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

USA15:USA15: C C33FF8 8 compressorscompressors

Back-pressure regulator rack: setting of Back-pressure regulator rack: setting of evaporation pressure (temperature) evaporation pressure (temperature) (64 / 324 circuits)(64 / 324 circuits)

Page 29: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Page 30: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Infrastructure at CPPM

Page 31: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

Page 32: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

GUI in PVSS II

Finite state machine in PVSS to send fluid through pixel ladder by sequencing pneumatic valves

Page 33: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

GUI in PVSS II

Machine a état finie pour envoyer fluide vers l’échelleséquencing des vannes pneumatiques

Part of a run of 1000 heat/cool cycles (Accelerated Thermal Stress Test

of thermal interfaces in a pixel stave)

Page 34: Summary of thermal management meeting Summary of thermal management working group meeting, December 6 Presentations Introduction (G. Viehhauser, Oxford)

Summary of thermal management meeting

New compressor at CPPM : capacity = 4kW

PID controllers

Condensor

Aspirationbuffer


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