August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis1 Analysis cases Approach: Start simple to get information— with speed with confidence that.

Slides:



Advertisements
Similar presentations
FEA Course Lecture V – Outline
Advertisements

Conduction Conceptests
Thermal Elements Jake Blanchard Spring Thermal Elements These elements calculate temperatures in solids There are 1-D, 2-D, and 3-D elements All.
Chapter 3c : One-dimensional, Steady state conduction (with thermal energy generation) (Section 3.5 – Textbook) 3.1 Implications of energy generation Involve.
MECHANISM OF HEAT TRANSFER Mode of Heat transfer Conduction Convection
Mike Fitton Engineering Analysis Group Design and Computational Fluid Dynamic analysis of the T2K Target Neutrino Beams and Instrumentation 6th September.
Energy in Thermal Processes
Thermal Analysis of short bake out jacket version 1 12-Nov-2013.
Example 1:- An annular alloyed aluminum (k = 180 W/m . K ) fin of rectangular profile is attached to the outer surface of a circular tube having an outside.
AAE450 Spring 2009 Slide 1 of 7 Orbital Transfer Vehicle (OTV) Thermal Control Ian Meginnis February 26, 2009 Group Leader - Power Systems Phase Leader.
Jed Goodell Jesse Williams. Introduction Problem How much heat does a particular heat sink dissipate How many fins are needed to dissipate a specific.
Heat Transfer  How is heat transferred from one place to another?  What is moving?  In mechanics energy can be transferred through a particle (e.g.
CHE/ME 109 Heat Transfer in Electronics LECTURE 12 – MULTI- DIMENSIONAL NUMERICAL MODELS.
CHE/ME 109 Heat Transfer in Electronics LECTURE 10 – SPECIFIC TRANSIENT CONDUCTION MODELS.
Identified Company (CompositeX) to manufacture Custom Composite Pressure Vessel ● Working pressure 1000psi ● Holds 8 kg Nitrous Oxide ● 700 cubic inch.
Al 2 O 3 Post Combustion Chamber Post Combustion Chamber ANSYS Thermal Model (Embedded Fuel Grain Concept) Outer radius: 1.25” ( m) Inner radius:
Aluminum/Titanium Comparison Aluminum alloy Titanium Alloy Property7075-T6 (ww-T-700) drawn tubing7075-T6; 7075-T651Grade 5 Ti6Al4V% Different SourceCasing.xlsMatweb.
Unsteady Heat Transfer in Semi-infinite Solids Solidification process of the coating layer during a thermal spray operation is an unsteady heat transfer.
Feasibility Analysis h T1 T2 T3 T4 T5 One Dimensional Transient Analysis One Dimensional Finite Difference Steady State Analysis T1 and T5 will be known.
Heat Transfer Rates Conduction: Fourier’s Law
Observations use one or more of the _______. A measurement is an________. An observation cannot be an __________. An inference is based on _________. _________s.
Chapter 18. Heat Transfer A PowerPoint Presentation by
I T i womiller VG1 Meeting UCSC November 10, 2005 ATLAS Upgrade Workshop Silicon Tracker Stave Mechanical Issues.
Heat Transfer in Structures
Ernie Ihloff 21 May 08 Preliminary Heat Shield Design for nEDM.
Calorimeter Analysis Tasks, July 2014 Revision B January 22, 2015.
2D Transient Conduction Calculator Using Matlab
ATLAS Calorimeter Argon Gap Convection Test Bed Brian Cuerden 24 Apr
Micro-Resistor Beam.
LHC Phase II Collimator Compact jaw simulations New FLUKA => ANSYS mapping scheme New 136mm x 950mm jaw –60cm primary collimator –Helical cooling channel.
Thermo-mechanics J. Cugnoni, LMAF / EPFL Three kind of « thermo-mechanics » 1. Un-coupled: Known temperature field => mechanical model (linear statics.
Application of QuickField Software to Heat Transfer Problems i j k By Dr. Evgeni Volpov.
ATLAS Calorimeter Argon Gap Convection Test Bed April 25,
JCOV, 25 OCT 2001Thermal screens in ATLAS Inner Detector J.Godlewski EP/ATI  ATLAS Inner Detector layout  Specifications for thermal screens  ANSYS.
Tutorial 6-1: 3D Modeling.
Calculation of Beam loss on foil septa C. Pai Brookhaven National Laboratory Collider-Accelerator Department
Study Plan of Clearing Electrode at KEKB Y. Suetsugu, H. Fukuma (KEK), M. Pivi, W. Lanfa (SLAC) 2007/12/191 ILC DR Mini Work Shop (KEK) Dec.
Similar Lengths (2) Geometry In each example, two similar models of the same shape are shown. Find the length of the unknown side. 135cm 115cm 86cm h.
J-PARC neutrino experiment Target Specification Graphite or Carbon-Carbon composite cylindrical bar : length 900mm, diameter 25~30mm The bar may be divided.
Chapter 2 Conduction Chapter 2.
Thermal Model of Pixel Blade Conceptual Design C. M. Lei 11/20/08.
Spacing of Cu clamp = 10” Clamp plate width = 2.5”, thickness = 0.375” Thickness of conductor insulation = 0.03” Thickness of coil ground wrap = 0.03”
GRAN SASSO’S HADRON STOP Temperature’s behaviour under specified beam conditions Barbara Calcagno.
Double Pipe HEAT EXCHANGERS with Low Thermal Resistance P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Ideas for Creation of Isotropically.
Bubble Chamber Radiator Thermal Analysis 5.0 MeV, 9.5 MeV Beam Energy Fredrik Fors Mechanical Engineering 8/20/2015.
Finite-Difference Solutions Part 2
Thermal Analysis Assumptions: Body Temperature (Environment) is 37˚C Heat distribution on outside of device will be modeled via FEA Heat transfer method.
Cooling of GEM detector CFD _GEM 2012/03/06 E. Da RivaCFD _GEM1.
Simulation of heat load at JHF decay pipe and beam dump KEK Yoshinari Hayato.
Exercises for Q1. Insulated copper tube A thin walled 10 mm copper tube is used to transport a low-temperature refrigerant with a temperature that is.
Itacil C. Gomes I.C.Gomes Consulting & Investment inc. Project X Forum on Spallation Sources for Particle Physics March 19-20, 2012 Fermi National Accelerator.
TUTORIAL 1 7/3/2016.
1 Calorimeter 4-May-2009 Added Slides Data from MAS GCALOR with phojet min-bias events in ATLAS detector.
Chapter 12 Temperature and Heat Chapter 13 The Transfer of Heat.
11. Stresses in Soil Mass (Das, Chapter 10)
Chapter 18. Heat Transfer A PowerPoint Presentation by
Unsteady Heat Transfer in Semi-infinite Solids
Calorimeter Transient Analysis for Steady State with ID Heat Leak and mini-FCal Analysis with 88.5°K Coolant in the Cooling Coil July 25, 2014 Brian Cuerden.
Maxwell and Ansys simulations for the CAPP detector
TBM thermal modelling status
Power Magnetic Devices: A Multi-Objective Design Approach
Starter Calculate the area of the following shapes 6m 120mm 110mm 4m
Thermo-mechanics J. Cugnoni, LMAF / EPFL 2009.
Heat Transfer in Extended Surface
Eurocode 1: Actions on structures –
Chapter 18. Heat Transfer A PowerPoint Presentation by
Data from MAS GCALOR with phojet min-bias events in ATLAS detector
Thermal behavior of the LHCb PS VFE Board
What are Fins ? Fins are extended surfaces used to increase the rate of heat transfer. It is made of highly conductive materials such as aluminum.
THERMODYNAMIC IN ELECTRONICS
Presentation transcript:

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis1 Analysis cases Approach: Start simple to get information— with speed with confidence that is useful

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis2 Case 1: hand calc comparison model 4.55 cm 18.1 cm -Uniform heating of block using equiv volume heat generation (36.3W) -Same surface area (982 cm^2) -Radiation to “space” node at 298K (view factor=1) -Larger mass than hand calc -Emissivity = 0.1

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis3 Case 1: comparison results Steady state temperature same as hand calc –520 K Transient results same as hand calc if we set hand calc mass equal to FEA model mass 520K

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis4 Case 2: SS block with circular heating Steady state temps -Power deposition = W/mm -Absorbed thickness = 45.5 mm -Absorbed power = 36.3 W -Xsec area of heated volume = 491 mm^2 -SS conductivity = 16.3 W/m-K -SS density = 8.0 g/cc -SS C = 0.5 J/g-degC -Emissivity = 0.1 -Mass = 11.9 kg

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis5 Truncated gaussian beam profile

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis6 Case 2: SS block with circular heating Transient results

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis7 Case 3: Copper block by itself 87 mm 79 mm 15.3 mm -Power deposition = W/mm -Absorbed thickness = 15 mm -Absorbed power = W -Xsec area of heated volume = 484 mm^2 -Cu conductivity = 391 W/m-K -Cu density = 8.9 g/cc -Cu C = J/g-degC -Emissivity = 0.4 -Mass = 0.94 kg

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis8 Case 3: Copper block results Steady state temps Transient temp at corner 443K

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis9 Case 4: Copper block in Macor -Cu emissivity = 0.5 Macor features: -Power deposition = 0.46 W/mm -Absorbed thickness = 12 mm -Absorbed power = 5.52 W -Xsec area of heated volume = 484 mm^2 -Macor conductivity = 1.46 W/m-K -Macor density = 2.52 g/cc -Macor C = 0.79 J/g-degC -Emissivity = 0.5 -Mass = 0.32 kg 97.2 mm 86.2 mm 33 mm Macor Cu View with half of Macor not shown Isometric view

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis10 Case 4 Steady state temps

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis11 Case 4: Transient results 402K 477K 513K

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis12 Case 5: Simplified geometry Cu+Macor+SS SS features: -Power deposition = W/mm -Absorbed thickness = mm -Absorbed power = 51.1 W -Xsec area of heated volume = 484 mm^2 -SS conductivity = 16.3 W/m-K -SS density = 8 g/cc -SS C = 0.5 J/g-degC -Emissivity = 0.5 -Mass = 11.5 kg Front sectional view (plane normal to beam) Side sectional view Overall width=95 mm Cavity width=88 mm Overall height=234 mm Cavity height=183 mm Overall depth=98 mm Cavity depth=45 mm SS Macor Cu 3D view

August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis13 Case 5: Simplified geometry Cu+Macor+SS Tin melts 322 degC 272 degC 222 degC 172 degC 122 degC 72 degC 22 degC SS center SS corner Macor corner Macor center Cu corner and center 565K 555K 482K 438K 409K

August 15, 2003K. Chow, LHC Luminosity Detector Thermal Analysis14 Case 6: Simplified geometry Cu+Macor+SS Emissivities: Cu = 0.7 Macor = 0.25 SS = K 641K 567K 492K 463K

August 15, 2003K. Chow, LHC Luminosity Detector Thermal Analysis15 Case 7: Simplified geometry Cu+Macor+SS Emissivities: Cu = 0.7 Macor = 0.75 SS = K 510K 442K 415K 387K

August 15, 2003K. Chow, LHC Luminosity Detector Thermal Analysis16 Case 8: Simplified geometry Cu+Macor+SS, 4 foot aluminum bar attached Emissivities: Cu = 0.7 Macor = 0.75 SS = 0.7 Alum = K 415K 377K 323K 310K

August 15, 2003K. Chow, LHC Luminosity Detector Thermal Analysis17 Case 11: Simplified geometry Cu+Macor+SS, 4 foot aluminum bar attached, with free convection Emissivities: Cu = 0.7 Macor = 0.75 SS = 0.7 Alum = K 407K 359K 312K 303K

August 15, 2003K. Chow, LHC Luminosity Detector Thermal Analysis18 Case 12: Simplified geometry Cu+Macor+SS, 4 foot aluminum bar attached, with free convection Emissivities: Cu = 0.7 Macor = 0.25 SS = 0.25 Alum = K 517K 367K 315K 304K

August 15, 2003K. Chow, LHC Luminosity Detector Thermal Analysis19 Case 13: Same as 12, but with new beam loading values Emissivities: Cu = 0.7 Macor = 0.25 SS = 0.25 Alum = K 520K 372K 316K 304K

August 21, 2003K. Chow, LHC Luminosity Detector Thermal Analysis20 Comparison 1 Power deposition (W/mm): Cu = Macor = SS = 0.798

August 21, 2003K. Chow, LHC Luminosity Detector Thermal Analysis21 Comparison 2 Emissivities Cu = 0.7 Macor = 0.75 SS = 0.7 Al = 0.7 Power deposition (W/mm): Cu = Macor = SS = 0.798

August 21, Comparison 3: Steady State Temps for Different Conditions Power deposition (W/mm): Cu = Macor = SS = Power deposition (W/mm): Cu = Macor = SS = 0.894