CO2 Cooling
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Transcript of CO2 Cooling
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CO2 Cooling
For the CMS Pixel detector
11 November 2008 1Hans Postema & Antti Onnela
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Advantages
LHCB has chosen CO2, with the following arguments: • Radiation hard• Has excellent thermodynamic properties for micro-
channels. • Low dT/dP• Low mass • Low liquid/vapour density ratio• Low viscosity• High latent heat• High heat transfer coefficient
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Pressure advantage
• Intuitively, higher pressures seem a disadvantage but:
• Gas flow at higher pressures needs smaller pipe diameters
• Pressure drops due to flow become less significant, allowing smaller pipes
• Small pipes can easily support the required pressures
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Pressure values
• At 20 degrees C – two phase at 57 bar
• At -12 degrees C – two phase at 25 bar– Corresponds to detector operation
• At +5 degrees C – two phase at 40 bar– Corresponds to detector storage using the
standard chilled water to cool the reservoir.
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Existing Supply pipes
• It is virtually impossible to replace the existing tracker supply lines
• The installed pipes reach the elastic limit at approximately 150 bar (measured at CERN)
• Operation at 40 bar seems feasible
• Safety aspects need to be studied
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Modified Mechanics for CO2 Cooling
Cooling pipes stainless steel. Diameter d = 1.50 mm and wall thickness t = 50 icrons
Layer 1 r=4.4cm
Diamond filled Araldite
pmax = 275 bar safety factor 3 pop = 90bar
d
tp yield2max
Old
New
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• Biphase CO2 cooling allows long cooling loops ( ~2-3m) with very small diameter pipes ( ~ 1mm ) for thermal loads of ~ 100 W
• Present C6F14 monophase has parallel cooling pipes with manifold and large crosssection silicon hoses for feed and drain in front of FPIX tracking region.
• New CO2 allows serialized pipes without pressure drop problems and therefore reduces resident cooling liquid by large factor.
• Density of liquid CO2 is ~ 1.03 g/cm3 compared to 1.76 g/cm3 of C6F14
Modified Mechanics for CO2 Cooling (2)
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New cooling pipe
• Estimates by Bart Verlaat from NIKHEF allow for a 5.5 m long cooling pipe with a diameter of 1.5 mm
• This avoids all the manifolding in the detector• The calculated pressure drop along the 5.5 m
is 2 bar giving a dT of 3 degrees C• But calculating 2-phase flow in small tubes is
known to be very difficult
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R & D
• At present everything indicates that this cooling method is feasible
• A simple test setup can increase the confidence level and can show that the concept is correct
• More sophisticated research is important to assure a full understanding of the system and optimize the design details as well as the operating parameters
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Next steps
• Aachen as well as Lyon seem very interested in starting conceptual design verification test (see next slide)
• CERN Cryolab has already started to work on a test setup for high precision measurements and a full characterization of CO2 flow in small tubes
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Design verification
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Year Pixel upgrade CO2 cooling R&D Pixel upgrade project2008 Oct-Dec: Definition of the CO2 study project, write
requirements, collect existing documentations into project database.
2009 Jan: Project start
Sep: Provisional results of the CO2 studies available
2010April: CO2 study results ready, decision on pipe dimensions and routing
Jan onwards: Detail design of Phase 1 pixel upgrade
July: Start of component procurements
2011
Dec: All components ready
2012 Jan: Final integration work start
Nov: Pixel detector ready for installation
2013 Jan: Pixel installation
Planning proposal
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Acknowledgements
• Several slides in this presentation are borrowed from:– CO2 cooling for HEP experiments – Bart Verlaat –
TWEPP-2008– Pixel detector CO2 cooling – Roland Horisberger
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