azu-yone-tirashi-omote03 · Title: azu-yone-tirashi-omote03 Created Date: 5/23/2016 5:20:46 PM
Limits of CO 2 Cooling A clear explanation that an yone can understand (the goal )
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Transcript of Limits of CO 2 Cooling A clear explanation that an yone can understand (the goal )
Hans Postema & Joao Noite PH-CMX-DS 1
Limits of CO2 CoolingA clear explanation that anyone can understand (the goal)
Hans Postema & Joao Noite PH-CMX-DS 2
Introduction
• The Production Readiness Review for the CO2 cooling for the Pixel Phase 1 upgrade is foreseen for the 9th of May.
• This presentation is aimed at the referees who do not necessarily have extensive experience in 2-phase cooling.
• Please let me know if you see anything in this presentation that could be explained clearer or simpler.
3
Limits of CO2 Cooling• Evaporative CO2 cooling is complex.
• Tube is fixed as 1.4mm ID due to space limitation inside the detector.
• Dry-out phenomena limits the maximum power that can successfully be extracted.
• Dry-out can lead to high temperatures at the detector.
Hans Postema & Joao Noite PH-CMX-DS
4
Limits of CO2 Cooling
Hans Postema & Joao Noite PH-CMX-DS
BUBBLY
INTERMITTENT
ANNULAR
DRYOUT
MIST
• Cooling capacity disappears before all the liquid is evaporated.
• Mist flow: the wall is dry, mist around the center of tube
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Limits of CO2 Cooling
Hans Postema & Joao Noite PH-CMX-DS
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10
500
1000
1500
2000
2500
Vapor Quality
Mass V
elo
city [
kg/m
2 .s]
G = 1948kg/m2.s | q = 23.94kW/m2 | Psat = 23.25Bar | xout = 0.33 | xdryout = 0.38
B
I
A
M
1.7g/s
3.0g/s
D
BUBBLY
INTERMITTENT
ANNULAR
DRYOUT
MIST
Dryout line
The dryout line represents the points of maximum heat transfer coefficient.
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Limits of CO2 Cooling
Hans Postema & Joao Noite PH-CMX-DS
•At -20°C the heat transfer
coefficient decreases
extremely rapidly at powers
above the dryout line.
• At 15°C dryout starts at a
much lower power but the
heat transfer coefficient
decreases more gradually
above the dryout line.
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10
5
10
15
20
25
30
35
Vapor Quality
HT
C [
kW/m
2 .K]
-Z Layer #1 m=2.6g/s
-20°C Old Max Power
15°C Old Standby
Hans Postema & Joao Noite PH-CMX-DS 7
0 2 4 6 8 10 12-20
-18
-16
-14
-12
-10
-8
Length [m]
Tem
pera
ture
[°C
]
L2D2PN & L2D1PF OHL | m = 1.98g/s | Qtotal
= 262.35W | dP = 7.17Bar | dT = 8.51°C
0 2 4 6 8 10 1218
20
22
24
26
28
30
Pre
ssur
e [B
ar]
Theory Wall TemperatureTheory CO
2 Temperature
Theory CO2 Pressure
BPix Critical Layers @ -20°C Max Power “Old”
Safety margin OKQexit = 46%
Qdryout = 55%
0 1 2 3 4 5 6 7 8 9 10-20
-18
-16
-14
-12
-10
Length [m]
Tem
pera
ture
[°C
]
L1D2MN & L1D1MF OHL | m = 2.60g/s | Qtotal
= 289.12W | dP = 8.64Bar | dT = 7.51°C
0 1 2 3 4 5 6 7 8 9 1018
20
22
24
26
28
Pre
ssur
e [B
ar]
Theory Wall TemperatureTheory CO
2 Temperature
Theory CO2 Pressure
Very low safety marginQexit = 38%
Qdryout = 41%
+Z Layer #2 -Z Layer #1
Hans Postema & Joao Noite PH-CMX-DS 8
0 1 2 3 4 5 6 7 8 9 1014
16
18
20
22
24
Length [m]
Tem
pera
ture
[°C
]
L1D2MN & L1D1MF OHL | m = 2.60g/s | Qtotal
= 289.12W | dP = 9.39Bar | dT = 6.50°C
0 1 2 3 4 5 6 7 8 9 1050
52
54
56
58
60
Pre
ssur
e [B
ar]
Theory Wall TemperatureTheory CO
2 Temperature
Theory CO2 Pressure
0 2 4 6 8 10 1214
16
18
20
22
24
Length [m]
Tem
pera
ture
[°C
]
L2D2PN & L2D1PF OHL | m = 1.98g/s | Qtotal
= 262.35W | dP = 7.22Bar | dT = 4.54°C
0 2 4 6 8 10 1250
52
54
56
58
60
Pre
ssur
e [B
ar]
Theory Wall TemperatureTheory CO
2 Temperature
Theory CO2 Pressure
BPix Critical Layers @ 15°C Max Power “Old”(for comparison, not part of the requirements)
NO safety marginQexit = 75%
Qdryout = 40%Deep inside dry-out region
+Z Layer #2 -Z Layer #1
NO safety marginQexit = 63%
Qdryout = 26%Deep inside dry-out region
Hans Postema & Joao Noite PH-CMX-DS 9
0 1 2 3 4 5 6 7 8 9 1015
16
17
18
19
20
Length [m]
Tem
pera
ture
[°C
]
L1D2MN & L1D1MF OSB | m = 2.60g/s | Qtotal
= 175.15W | dP = 8.05Bar | dT = 2.63°C
0 1 2 3 4 5 6 7 8 9 1050
52
54
56
58
60
Pre
ssur
e [B
ar]
Theory Wall TemperatureTheory CO
2 Temperature
Theory CO2 Pressure
0 2 4 6 8 10 1215
16
17
18
19
20
Length [m]
Tem
pera
ture
[°C
]
L2D2PN & L2D1PF OSB | m = 1.98g/s | Qtotal
= 194.68W | dP = 6.10Bar | dT = 3.49°C
0 2 4 6 8 10 1250
52
54
56
58
60
Pre
ssur
e [B
ar]
Theory Wall TemperatureTheory CO
2 Temperature
Theory CO2 Pressure
BPix Critical Layers @ 15°C Standby “Old”
NO safety marginQexit = 55%
Qdryout = 44%11% inside dry-out region
+Z Layer #2 -Z Layer #1
NO safety marginQexit = 37%
Qdryout = 33%4% inside dry-out region
Hans Postema & Joao Noite PH-CMX-DS 10
BPix Critical Layers @ 15°C Standby “Old”
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10
500
1000
1500
2000
2500
Vapor Quality
Mass V
elo
city [
kg/m
2 .s]
-Z Layer #1 OSB | Tset
= 15°C | q = 13.67 kW/m2
B
I
A
D M
1.6g/s
1.8g/s
2g/s
2.2g/s
2.4g/s
2.6g/s
2.8g/s
3g/s
3.2g/s
3.4g/s
3.6g/s
Counter intuitive: More flow does not always solve the problem.
Hans Postema & Joao Noite PH-CMX-DS 11
BPix Numbers
Hans Postema & Joao Noite PH-CMX-DS 12
Conclusions
• Assumption:– Values for power include sufficient safety margin, a
safety margin in the cooling system is therefore not needed
• At -20°C, max power operation is close to the dry-out line, is this safe enough?
• At +15°C, standby power operation is deep inside the dry-out region, is this safe enough?
• Increasing the flow might not provide a solution
Hans Postema & Joao Noite PH-CMX-DS 13
Afterword
• Building the lightest pixel detector in the history of high energy physics is an admirable quest that I am happy to participate in.
• Extreme performance is generally achieved using the absolute minimum safety factors.
• Extremely low safety factors can only be used safely when experience is at a high level and unforeseen issues are unlikely to occur.
• In how far does the above apply to our project?