Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation.

Slides:



Advertisements
Similar presentations
Finite Elements Principles and Practices - Fall 03 FE Course Lecture II – Outline UCSD - 10/09/03 1.Review of Last Lecture (I) Formal Definition of FE:
Advertisements

Redesign of Die Internal Structure Dr. Henry Tan School of Mechanical, Aerospace and Civil Engineering The University of Manchester.
Thermal Elements Jake Blanchard Spring Thermal Elements These elements calculate temperatures in solids There are 1-D, 2-D, and 3-D elements All.
Thermal Properties Part III Asst. Prof. Dr. Muanmai Apintanapong.
Plasticity Jake Blanchard Spring Analysis of Plastic Behavior Plastic deformation in metals is an inherently nonlinear process Studying it in ANSYS.
Project 2: Torque-Arm Modeling, Simulation and Optimization
Extended Surface Heat Transfer
Chapter 2: Overall Heat Transfer Coefficient
Analysis of Simple Cases in Heat Transfer P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Gaining Experience !!!
One Dimensional Steady State Heat Conduction
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.
First Wall Thermal Hydraulics Analysis El-Sayed Mogahed Fusion Technology Institute The University of Wisconsin With input from S. Malang, M. Sawan, I.
CHE/ME 109 Heat Transfer in Electronics LECTURE 10 – SPECIFIC TRANSIENT CONDUCTION MODELS.
Al 2 O 3 Post Combustion Chamber Post Combustion Chamber ANSYS Thermal Model (Embedded Fuel Grain Concept) Outer radius: 1.25” ( m) Inner radius:
CHE/ME 109 Heat Transfer in Electronics LECTURE 8 – SPECIFIC CONDUCTION MODELS.
Liquid Argon in a Large Tank --- Some Thermodynamic Calculations Zhijing Tang November 4, 2004.
MSE ISSUES TO ADDRESS... How do materials respond to the application of heat ? How do we define and measure heat capacity? -- thermal expansion?
An Investigation into the use of FEA methods for the prediction of Thermal Stress Ratcheting Huse, Stephen.
Thermal Analysis Module 6. Training Manual January 30, 2001 Inventory # Thermal Analysis In this chapter, we will briefly describe the procedure.
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.
Fins-2 If the pot from previous lecture is made of other materials other than the aluminum, what will be the temperature distribution? Try stainless steel.
RF-Accelerating Structure: Cooling Circuit Modeling Riku Raatikainen
Steam Condenser II Prof. Osama El Masry
1 Calorimeter Thermal Analysis with Increased Heat Loads September 28, 2009.
9.0 New Features Large Deformation Analysis of thin plate assembly spotwelded together Workshop 2 Spotwelds.
Non stationary heat transfer at ceramic pots firing Janna Mateeva, MP 0053 Department Of Material Science And Engineering Finite Element Method.
Calorimeter Analysis Tasks, July 2014 Revision B January 22, 2015.
2D Transient Conduction Calculator Using Matlab
Transient Thermal Problems Jake Blanchard Spring 2008.
ATLAS Calorimeter Argon Gap Convection Test Bed Brian Cuerden 24 Apr
2-d Insulation Analysis of Clamp / Vacuum Vessel Insulation crushing
In UCTM Example 3 Веселин Илиев Thermal Stresses in АNSYS Workbench 10.0 This material is designed for reminding of the subject, studied in the course.
Design of Recuperative Heat Exchanger Presented by -- Jinying Zhu.
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.
Consideration of Baffle cooling scheme
Silesian University of Technology in Gliwice Inverse approach for identification of the shrinkage gap thermal resistance in continuous casting of metals.
Summary of Winding Pack Thermal Results K. Freudenberg
Tutorial 6-1: 3D Modeling.
Residual Stress in a Thin Film Resonator
Heat Transfer Equations. Fouling Layers of dirt, particles, biological growth, etc. effect resistance to heat transfer We cannot predict fouling factors.
GIGATRACKER SUPPORTING PLATE COOLING SYSTEM SIMULATION 1Vittore Carassiti - INFN FECERN, 11/12/2007.
Phase Change Analysis Chapter 9. Training Manual Inventory # March 15, Chapter Overview Phase Change –Terminology –Theory –Material Properties.
COMPASS All-Hands Meeting, FNAL, Sept , 2007 Accelerator Prototyping Through Multi-physics Analysis Volkan Akcelik, Lie-Quan Lee, Ernesto Prudencio,
Investigation of the Thermal Stresses in a Steel Plate.
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”
Bubble Chamber Radiator Thermal Analysis 5.0 MeV, 9.5 MeV Beam Energy Fredrik Fors Mechanical Engineering 8/20/2015.
P14 DESIGN STANDARDS FOR CRCP FOR EACH TEXAS ENVIRONMENTAL REGION Center for Transportation Research The University of Texas at Austin.
Evan Selin & Terrance Hess.  Find temperature at points throughout a square plate subject to several types of boundary conditions  Boundary Conditions:
Thermal Analysis Assumptions: Body Temperature (Environment) is 37˚C Heat distribution on outside of device will be modeled via FEA Heat transfer method.
COUPLED ANALYSES Chapter 7. Training Manual May 15, 2001 Inventory # Fluid-Structure Analysis “One Way” Analysis –Structural deformation effect.
Cooling of GEM detector CFD _GEM 2012/03/06 E. Da RivaCFD _GEM1.
Friedrich-Schiller-University Jena Institute of Solid State Physics – Low Temperature Physics Christian Schwarz 15 th September Genoa 1 Investigation.
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.
TEM3P Simulation of Be Wall Cavity Tianhuan Luo. Cavity Model Pillbox cavity with Be wall R=0.36 m, f0~319 MHz, L=0.25m (not exactly 325 MHz, but not.
HL-LHC-UK Thermal Shield Update Niklas Templeton 07/03/2016.
TUTORIAL 1 7/3/2016.
Coupled Field Analysis Chapter 12. Training Manual October 30, 2001 Inventory # In this chapter, we will briefly describe how to do a thermal-stress.
Workshop Workshop Download & Excute “Diamond_win32.msi”(Windows XP,Windows Vista 32bit, Windows 7 32bit users) Download & Excute.
THERMO-STRUCTURAL ANALYSIS
Maxwell and Ansys simulations for the CAPP detector
Modified Design of Aries T-Tube Divertor Concept
Joule Heating of MEMS Beam Ansys Simulation October 2011
CE 808: Structural Fire Engineering SAFIR - Computer Program
Structural analysis of the CBM magnet coil
What is Fin? Fin is an extended surface, added onto a surface of a structure to enhance the rate of heat transfer from the structure. Example: The fins.
Steady-State Heat Transfer (Initial notes are designed by Dr
Solve the differential equation using the method of undetermined coefficients. y " + 4y = e 3x 1. {image}
Solve the differential equation using the method of undetermined coefficients. y " + 9y = e 2x {image}
Thermo-mechanics J. Cugnoni, LMAF / EPFL 2012.
Presentation transcript:

Thermal Stresses Jake Blanchard Spring 2008

Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation nonlinear ANSYS can handle this with little input from us Examples: ◦ Copper: k= *T (W/m-K; T in K) ◦ Stainless Steel: k= *T ◦ Plot these vs. Temperature from 300 K to 1000 K ◦ Try: ◦ MP,KXX,1,420.75,

Incorporating into ANSYS Input polynomial coefficients into Material Table Set nonlinearity parameters Everything else is the same

In-Class Problems Material 1 is Cu Material 2 is SS cm 1 cm q=10 4 W/m 2 h=1000 W/m 2 -K T b =50 C

Thermal Stresses Thermal stresses occur when there is differential expansion in a structure ◦ Two materials connected, uniform temperature change (different thermal expansion coefficients lead to differential expansion) ◦ Temperature gradient in single material (differential expansion is from temperature variation)

Treating Thermal Stress in ANSYS Two options 1.Treat temperature distributions as inputs (useful for uniform temperature changes) – must input thermal expansion coefficient 2.Let ANSYS calculate temperatures, then read them into an elastic/structural analysis

Prescribing temperatures Use: Preprocessor/Loads/Define Loads/Apply/Structural/Temperature/On Areas (for example)

Sample  1 =2*10 -6 /K E 1 =200 GPa  1 =0.3  2 =5*10 -6 /K E 2 =100 GPa  2 =0.28 Increase T by 200 C Inner radius=10 cm Coating thickness=1 cm 2 1

Calculating both temp and stress Set jobname to ThermTest (File/Change Jobname…) Main Menu/Preferences/Structural&Thermal&h- method Input structural and thermal properties Create geometry and mesh Input thermal loads and BCs Solve and save.db file Delete all load data and switch element type to struct. Edit element options if necessary Apply BCs Loads/Define Loads/Apply/Temperature/from thermal anal./ThermTest.rth Solve

Sample  1 =2*10 -6 /K E 1 =200 Gpa k 1 =10 W/m-K  1 =0.3  2 =5*10 -6 /K E 2 =100 Gpa k 2 =20 W/m-K  2 =0.28 Set outside T to 0 C Set heating in 2 to 10 6 W/m 3 Inner radius=10 cm Coating thickness=1 cm 2 1

In-Class Problems Channels are 3 cm in diameter k=20 W/m-K E=200 Gpa  =0.3  = /K 10 cm q=10 4 W/m 2 15 cm 2 cm h=1000 W/m 2 -K T b =50 C