r.valbuena nbi 14-19 march 2002 cngs decay pipe entrance window structural and thermal analysis...
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R.Valbuena NBI 14-19 March 2002
CNGS Decay Pipe Entrance Window
Structural and Thermal Analysis
A.Benechet, P.Cupial, R.Valbuena
CERN-EST-ME
R.Valbuena NBI 14-19 March 2002
Summary1. Structure analysis
• Geometry• Material properties• Boundary conditions• Loading cases• Results
2. Thermal analysis• Assumptions• Material properties• Boundary conditions• Loading cases• Results
3. Thermal and Mechanical Stresses4. Thermal shock5. Conclusions
R.Valbuena NBI 14-19 March 2002
1. Structure Analysis
1.1 Geometry• external diameter : 1665 mm• internal diameter : 1400 mm• spherical radius : 1891 mm• thickness: 2 mm
1.2 Ti 40 properties• Young Modulus 105 GPa• Yield Strength 280 MPa• Ultimate Tensile Strength Rm 460 MPa
1.3 Boundary Conditions• Fixed in-between flanges
Concrete
Decay Steel Pipe
Titanium window
Steel Flanges
R.Valbuena NBI 14-19 March 2002
1.4 Loading cases Case 1: 0.3 MPa test pressure Case 2 : 0.1 MPa service pressure
1.5 Results for Case 11.5.1 Analytical :
Allowable stress according to French Pressure Vessel Code (CODAP) :
For Titanium : under resistance test condition:
-under normal service condition :
MPa142e2
PR
f5.1
f
total
membrane
3.2
Rf
tm
3
Rf
tm MPa460R C50T20
m
P
with =>The condition is fullfilled
R.Valbuena NBI 14-19 March 2002
1.5.1 FEM Analysis
deformations:
Von Mises stress:
=1.8 mm
18.4 36.7 55.1 73.4 91.8 110 128 147 165
The membrane stress is equal to those computed analytically. The red zone is typical of such spherical shell under pressure (edge bending stress).
R.Valbuena NBI 14-19 March 2002
The stress in the red zone attains 240 MPa. It is due to the fixed nodes close to the curvature change.
Location Measured FEM Computed [MPa] [MPa] [MPa]
Gauge 5-6 125 143 143Gauge 7-8 65 144 too close to the filletGauge 3-4 102 142 143
Fillet / 240 /deflection 2.2 mm 1.8 mm /
Deformation and stress values are comparable with those measured on a prototype with strain gauges:
R.Valbuena NBI 14-19 March 2002
0
5 0
1 0 0
1 5 0
2 0 0
0 . 2 0 . 4 0 . 6 0 . 8
0
5 0
1 0 0
1 5 0
2 0 0
2 5 0
0 . 2 0 . 4 0 . 6 0 . 8
R
Z
R ( m ) [ m ] ( m )
R ( m )
[ M P a ]
[ M P a ]
Equivalent von Mises Stress in MPa on external and internal window faces
R.Valbuena NBI 14-19 March 2002
1.6 Result for Load Case 2 : P=0.1 MPa
Location of equivalent von Mises Stresses
Stress values in
MPa
Safety Factor wrt UltimateTensile
Strength
Safety Factor wrt Yield Strength
R=715 mm 80 5.7 3.5
R= 654 mm 54 8.0 5.2
0<R<194 47 8.5 5.9
Conclusions : Good agreement between analytical and FEM results except for fillet zone which has been modeled in a conservative way. The window is safe according to CERN safety rules.
R.Valbuena NBI 14-19 March 2002
2. Thermal Analysis
2.1 Assumptions
Transient analysis Run duration 200 days Initial temperature (materials and air) 15°C
2.2 Material properties :
Unit Titanium steel Concrete
Thermal Conductivity Wm-1C-1 7 51.9 1.8
Expansion coefficient C-1 8.70E-06 1.15E-05 2.10E-06
Density kg m-3 4700 7850 2300Young Modulus GPa 105 200 3.00E+09Poisson ratio --- 0.34 0.3 0.1
Thermal Capacity J Kg-1C-1 525 472 1000
Diffusivity m2/s 2.84E-06 1.40073E-05 7.83E-07
R.Valbuena NBI 14-19 March 2002
2.3 Boundary Conditions:• Case 3 : Natural convection :
• temperatures : Air 15 °CWindow 22 °C
Free convection coefficient:
• Case 4 : Natural and forced convections : Pipe diameter 12 mm Water temperature 15 °C Flow rate 10 l/mn
Forced convection coefficient:
12n KWm 3h
123f KWm 1013h
R.Valbuena NBI 14-19 March 2002
2.4 Loading Constant heat Generation:~30 W in the window~430 W in the flanges
0 10 20 30 40 50 60 70 80 90 100 110 120 10
-7
10 -6
10 -5
10 -4
Energy deposition in the Ti-window and in the flange
Ti-window
Fe-flange
GeV
cm
-3/p
r in cm
Power distribution per unit volume
0
5000
10000
15000
20000
25000
30000
35000
0 100 200 300 400 500 600 700 800 900 1000 1100
Radius [mm]h
eat
dep
osi
tio
n in
W/m
3
Proton Flux Density :
1 GeV = Joule
s/p108 1210106.1
R.Valbuena NBI 14-19 March 2002
2.5 Results2.5.1 Case 3 (free convection)
tem
péra
ture
[°C]
1 765432 temps [jours]
1
C
A
B
47
2
5
6
8
D
A : windowB : mating flangeC : cooling pipeD : flangeE : ConcreteNumbers show measuring points location 9
E
R.Valbuena NBI 14-19 March 2002
temps [j]0 3 6t = 0, arrêt du faisceau
tem
péra
ture
[°C
]
Temperature evolution during 10 days of cooling time
R.Valbuena NBI 14-19 March 2002
0.1 0.90.70.50.3rayon [m]
tem
péra
ture
[°C
]
20
30
40
50
Static Stress [MPa]
Thermal Stress [MPa]
Global Stress [MPa]
Safety Coefficientwrt Yield
Strength limit
Safety Coefficient
wrt Ultimate Tensile strength
90 40 130 2.15 3.5
Stresses close to the fillet
R.Valbuena NBI 14-19 March 2002
2.5.2 Case 4 (free and forced convections)
1 2 3 4te
mp é
r atu
re [
°C]
temps [h]
Temperature rising time : 4 hours
Maximum temperature on window apex : 32°C
Good efficiency of the water cooling for the flanges and weak impact on window temperature
R.Valbuena NBI 14-19 March 2002
0.1 0.3 0.5 0.7 0.9
tempé
ratu
re [°
C]
rayon [m]
0 0.5 1 1.5 temps [h]
tem
pératu
re [
°C
]
Temperature evolution during 2 hours cooling time
Window and Flange Temperature profiles
R.Valbuena NBI 14-19 March 2002
3.Thermal and Mechanical Stresses
Static Stress [MPa]
Thermal Stress [MPa]
Global Stress [MPa]
Safety Coefficientwrt Yield Strength
Safety Coefficient
wrt UltimateTensile
Strength
90 8 100 2.8 4.6
R.Valbuena NBI 14-19 March 2002
3.1 CODAP Verification
point R Top Middle BottomA 0 142 137 142B 194 142 138 142C 654 181 142 103D 703 76 142 201E 715 5 142 272
181 142 272300 200 300
1.66 1.41 1.10
Maximum Stress
Allowable Stress
Shell Stress [MPa] :
Safety Factor
Test Pressure : P=0.3 MPa
Service Pressure : P=0.1 MPa
point R Top Middle BottomA 0 47 46 47B 194 47 46 47C 654 60 47 34D 703 25 47 67E 715 2 47 91 SF
60 47 91 2.54
100 88 132
1.74
68 55 100
2.30
230 153 230Allowable Stress
Shell Stress[MPa]
Maximum structural Maximum Stress Thermal Natural
ConvectionMaximum Stress Thermal Forced
Convection
R.Valbuena NBI 14-19 March 2002
4. Thermal Shock
Full beam on the window : 3.5x1013 p/pulse
=> 3.34x1018 p/s
R.Valbuena NBI 14-19 March 2002
0.00E+00
5.00E+11
1.00E+12
1.50E+12
2.00E+12
2.50E+12
3.00E+12
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16
zone par tranche de 1 mm [0;1], [1;2], ...
géné
ratio
n de
cha
leur
[W/m
3 ]
After 2 pulses with q=2.6x1012 W/m3
T = 22 °C
R.Valbuena NBI 14-19 March 2002
After 1 pulse 10.5 s with q=2.6x1012 W/m3
T = 11 °C
Dynamic stress negligible
0
2
4
6
8
10
12
0 5 10 15 20
Rayon [mm]
tem
péra
ture
[°C]
R.Valbuena NBI 14-19 March 2002
5. Conclusions:
Free Convection inefficient in a CONFINED SPACE => Thermal stresses : 40 MPa on the window 230 MPa on decay tube / concrete interface
With the cooling system : Temperature stabilised at 32 °C, very low thermal stresses
In the event of the beam missing the target, the interlock shall react in less than 1’.
The window is safe according to CODAPSee Technical Note EST-ME/2001-007 EDMS n°323691