PAX DETECTOR THERMAL SIMULATION FzJuelich 27102008 Vittore Carassiti

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PAX DETECTOR THERMAL SIMULATION Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 1

PAX DETECTOR THERMAL SIMULATION Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 1

PAX DETECTOR FEM* ASSEMBLY LAYOUT ELECTRONIC SUPPORT TARGET CELL HEAT FLUX COOLING PLATE COOLING

PAX DETECTOR FEM* ASSEMBLY LAYOUT ELECTRONIC SUPPORT TARGET CELL HEAT FLUX COOLING PLATE COOLING TUBE SILICON SUPPORT SILICON DETECTOR VACUUM CHAMBER * FEM = Finite Element Modeler Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 2

MATERIALS PARTS MATERIALS PART MATERIAL SILICON DETECTOR SILICON TARGET CELL ALUMINUM SILICON SUPPORT ALUMINUM

MATERIALS PARTS MATERIALS PART MATERIAL SILICON DETECTOR SILICON TARGET CELL ALUMINUM SILICON SUPPORT ALUMINUM ELECTRONIC SUPPORT ALUMINUM VACUUM CHAMBER STAINLESS STEEL MATERIAL PROPERTIES MATERIAL DENSITY (Kg/m^3) THERMAL CONDUCTIVITY (W/m. K) EMISSIVITY (*) SPECIFIC HEAT (J/Kg. K) ALUMINUM 2700 237 0. 09 900 STAINLESS STEEL 7960 16, 3 0, 16 502 SILICON 2340 115 0, 9 703 (*) From the Engineering Toolbox (www. engineeringtoolbox. com) Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 3

THE ANALISYS THE FOLLOWING ANALISYS HAVE BEEN PERFORMED : RADIATION ANALISYS SIMULATION EVALUATING THE

THE ANALISYS THE FOLLOWING ANALISYS HAVE BEEN PERFORMED : RADIATION ANALISYS SIMULATION EVALUATING THE AMOUNT OF HEAT LOAD COMING FROM RADIATION TEMPERATURE ANALISYS SIMULATION EVALUATING THE DETECTOR’S TEMPERATURE DISTRIBUTION COMING FROM ELECTRONIC POWER AND RADIATION Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 4

RADIATION ANALISYS q SILICON SUPPORT SET AT CONSTANT TEMPERATURE q ELCTRONIC POWER SWITCHED OFF

RADIATION ANALISYS q SILICON SUPPORT SET AT CONSTANT TEMPERATURE q ELCTRONIC POWER SWITCHED OFF q VACUUM CHAMBER SET AT CONSTANT TEMPERATURE SILICON SUPPORT VACUUM CHAMBER Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 5

RADIATION ANALYSIS BOUNDARY CONDITIONS FEM RADIATION ANALYSIS BCs SILICON DETECTOR SILICON SUPPORT RADIATIVE THERMAL

RADIATION ANALYSIS BOUNDARY CONDITIONS FEM RADIATION ANALYSIS BCs SILICON DETECTOR SILICON SUPPORT RADIATIVE THERMAL COUPLINGS TO ALL PARTS CONDUCTIVE THERMAL COUPLINGS TO SILICON SUPPORT CONSTANT TEMPERATURES (C°) COOLING TUBE TARGET CELL ELECTRONIC & SUPPORT TO ALL PARTS VACUUM CHAMBER TO ALL PARTS -20 20 ; 40 ; 60 HEAT LOAD (W) SWITCHED OFF ADDITIONAL INFORMATIONS § - SHADOWING CHECKS BETWEEN PARTS PERMORMED Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 6

RADIATION ANALYSIS RESULTS 2° ANALISYS - SHARED POWER % 76. 01 80. 00 70.

RADIATION ANALYSIS RESULTS 2° ANALISYS - SHARED POWER % 76. 01 80. 00 70. 00 BOUNDARY CONDITIONS SILICON SUPPORT SURFACES CONSTANT TEMP (C°) VACUUM CHAMBER WALLS CONSTANT TEMP (C°) 60. 00 1° Analysis -20 20 40. 00 2° Analysis -20 40 30. 00 3° Analysis -20 60 VACUUM CHAMBER 50. 00 SILICON DETECTOR TARGET CELL 23. 90 20. 00 0. 11 10. 00 RADIATION ANALYSIS RESULTS PART SILICON DETECTOR 1° ANALYSIS VACUUM CHAMBER Fz-Juelich , 27/10/2008 3° ANALYSIS AVERAGE TEMP (C°) POWER (W) -18, 3 -22, 47 -17, 6 -21, 81 -16, 7 -21, 00 63, 68 SILICON SUPPORT TARGET CELL 2° ANALYSIS -17 -0, 104 91, 27 -15, 5 -41, 10 Vittore Carassiti - INFN FE -0. 096 -69, 37 124, 7 -13, 5 -0. 085 -103, 6 7

TEMPERATURE ANALISYS q COOLING TUBE WALL SET AT CONSTANT TEMPERATURE q ELCTRONIC POWER SWITCHED

TEMPERATURE ANALISYS q COOLING TUBE WALL SET AT CONSTANT TEMPERATURE q ELCTRONIC POWER SWITCHED ON COOLING TUBE Fz-Juelich , 27/10/2008 ELECTRONIC POWER Vittore Carassiti - INFN FE 8

TEMPERATURE ANALYSIS BOUNDARY CONDITIONS FEM TEMPERATURE ANALYSIS BCs SILICON DETECTOR SILICON SUPPORT RADIATIVE THERMAL

TEMPERATURE ANALYSIS BOUNDARY CONDITIONS FEM TEMPERATURE ANALYSIS BCs SILICON DETECTOR SILICON SUPPORT RADIATIVE THERMAL COUPLINGS TO ALL PARTS CONDUCTIVE THERMAL COUPLINGS TO SILICON SUPPORT CONSTANT TEMPERATURES (C°) COOLING TUBE TARGET CELL ELECTRONIC & SUPPORT VACUUM CHAMBER TO ALL PARTS VACUUM CHAMBER & SILICON SUPPORT TO ALL PARTS TO SILICON SUPPORT -20 HEAT LOAD (W) 85 ADDITIONAL INFORMATIONS § - SHADOWING CHECKS BETWEEN PARTS PERMORMED § - ENVIRONMENT TEMPERATURE = 25 C° Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 9

TEMPERATURE ANALYSIS RESULTS 69. 20 SHARED POWER % 70. 00 BOUNDARY CONDITIONS 60. 00

TEMPERATURE ANALYSIS RESULTS 69. 20 SHARED POWER % 70. 00 BOUNDARY CONDITIONS 60. 00 ENVIRONMENT TEMPERATURE = 25 C° COOLING TUBE WALL TEMP (C°) 50. 00 40. 00 ELECTRONIC HEAT LOAD (W) ELECTRONIC SILICON DETECTOR 26. 40 SILICON SUPPORT 30. 00 -20 TARGET CELL 20. 00 85 3. 30 10. 00 1. 20 0. 00 ANALYSIS RESULTS PART TEMPERATURE (C°) POWER (W) Tmin Tmax SILICON DETECTOR -19, 5 -12, 8 -32, 4 SILICON SUPPORT -20 -16, 6 -4 -11, 9 -11, 7 -1, 5 -20 117, 2 TARGET CELL COOLING TUBE WALL -85, 00 ELECTRONIC VACUUM CHAMBER Fz-Juelich , 27/10/2008 28 Vittore Carassiti - INFN FE 31 5, 7 10

SILICON SUPPORT – TEMPERATURE DISTRIBUTION Tmin = -20 C° ; Tmax = -16, 6

SILICON SUPPORT – TEMPERATURE DISTRIBUTION Tmin = -20 C° ; Tmax = -16, 6 C° Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 11

SILICON DETECTOR – TEMPERATURE DISTRIBUTION Tmin = -19, 5 C° ; Tmax = -12,

SILICON DETECTOR – TEMPERATURE DISTRIBUTION Tmin = -19, 5 C° ; Tmax = -12, 8 C° Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 12

TARGET CELL – TEMPERATURE DISTRIBUTION Tmin = -11, 9 C° ; Tmax = -11,

TARGET CELL – TEMPERATURE DISTRIBUTION Tmin = -11, 9 C° ; Tmax = -11, 7 C° Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 13

DETECTOR ASSEMBLY – TEMPERATURE DISTRIBUTION Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 14

DETECTOR ASSEMBLY – TEMPERATURE DISTRIBUTION Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 14

COOLING DESIGN TOTAL COOLING POWER (4/4) Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE

COOLING DESIGN TOTAL COOLING POWER (4/4) Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 15

COOLING DESIGN COOLING FLUID TEMPERATURE VS CONVECTION COEFFICIENT T (C°) fuid temperature @ Twall

COOLING DESIGN COOLING FLUID TEMPERATURE VS CONVECTION COEFFICIENT T (C°) fuid temperature @ Twall = -20 C° & Dtube = 8 mm 0. 00 E+00 -2. 00 E+01 -4. 00 E+01 -6. 00 E+01 Tfluid -8. 00 E+01 Tdelivery -1. 00 E+02 -1. 20 E+02 -1. 40 E+02 -1. 60 E+02 25 50 75 100 125 150 175 200 225 250 275 300 COOLING FLUID & CONVECTION COEFFICIENT SELECTION α (W/m^2 COOLING FLUID : ETHANOL ALCOHOOL °C Boiling point 78, 5 Density (Kg/m^3) ρ 832 Freezing point -114 Specific heat (J/Kg. K) Cp 2215 Thermal conductivity (W/m. K) λ 0, 13 Kinematic viscosity (m^2/s) ν 3, 23 E-06 Kinematic viscosity @ Tw (m^2/s) νw 2, 88 E-06 Convection coefficient α Delivery temperature Td -41 Wall temperature Tw -20 Fluid temperature Tf = (Td + Tw)/2 -30, 5 Fz-Juelich , 27/10/2008 W/m^2 C° 170 ETHANOL PROPERTIES @ Tf and atmospheric pressure Vittore Carassiti - INFN FE 16

COOLING DESIGN FLOW SPEED, FLOW RATE AND PRESSURE LOSS 40. 00 20. 00 25

COOLING DESIGN FLOW SPEED, FLOW RATE AND PRESSURE LOSS 40. 00 20. 00 25 50 75 100 125 150 175 200 225 250 275 300 α (W/m^2 C°) -20. 00 -40. 00 -60. 00 -80. 00 -100. 00 -120. 00 flow rate (Kg/h) flow speed (m/min) -140. 00 Tfluid (C°) d=8 Tdelivery (C°) d=8 -160. 00 Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 17

CONCLUSIONS A THERMAL ANALISYS INVESTIGATING THE RADIATION EFFECTS ON THE SILICON DETECTOR HAS BEEN

CONCLUSIONS A THERMAL ANALISYS INVESTIGATING THE RADIATION EFFECTS ON THE SILICON DETECTOR HAS BEEN DONE. A SUPPLEMENTARY ANALISYS CONSIDERING BOTH THE ELECTRONIC POWER AND THE RADIATION HAS BEEN ALSO SIMULATED. AN IMPROVEMENT OF THE ANALISYS RESULTS CAN BE ACHIEVED , GIVEN THE FOLLOWING INFORMATIONS : Ø AVERAGE WORKING TEMPERATURE OF THE SILICON DETECTOR Ø VALUE OF THE ELECTRONIC POWER Fz-Juelich , 27/10/2008 Vittore Carassiti - INFN FE 18