1 Convection Boundary Condition –Happens when a structure is surrounded by fluid –Does not exist in structural problems –BC includes unknown temperature.

Slides:



Advertisements
Similar presentations
FEA Course Lecture V – Outline
Advertisements

FEM FOR HEAT TRANSFER PROBLEMS
Quiz – An organic liquid enters a in. ID horizontal steel tube, 3.5 ft long, at a rate of 5000 lb/hr. You are given that the specific.
Parabolic Partial Differential Equations
Heat Transfer Chapter 2.
Chapter 2: Overall Heat Transfer Coefficient
Finite Element Method (FEM) Different from the finite difference method (FDM) described earlier, the FEM introduces approximated solutions of the variables.
Chapter 2: Steady-State One-Dimensional Heat Conduction
By S Ziaei-Rad Mechanical Engineering Department, IUT.
Analysis of Simple Cases in Heat Transfer P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Gaining Experience !!!
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.
MECh300H Introduction to Finite Element Methods
Thermal analysis There is a resemblance between the thermal problem and the stress analysis. The same element types, even the same FE mesh, can be used.
MECH300H Introduction to Finite Element Methods
One Dimensional Steady Heat Conduction problems P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Simple ideas for complex.
2005 February, 2 Page 1 Finite Element Analysis Basics – Part 2/2 Johannes Steinschaden.
CHAPTER 8 APPROXIMATE SOLUTIONS THE INTEGRAL METHOD
CHAP 5 FINITE ELEMENTS FOR HEAT TRANSFER PROBLEMS
Internal Flow Convection -constant surface temperature case Another commonly encountered internal convection condition is when the surface temperature.
Heat Conduction Analysis and the Finite Element Method
Flow Inside Heat Exchangers
1 CHAPTER 5 POROUS MEDIA Examples of Conduction in Porous Media component electronic micro channels coolant (d) coolant porous material (e) Fig.
Overall Heat Transfer Coefficient
Lecture Objectives: Analyze the unsteady-state heat transfer Conduction Introduce numerical calculation methods Explicit – Implicit methods.
CHAPTER 5 MESB 374 System Modeling and Analysis Thermal Systems
Two-Dimensional Conduction: Finite-Difference Equations and Solutions
Module 4 Multi-Dimensional Steady State Heat Conduction.
Transient Conduction: Finite-Difference Equations and Solutions Chapter 5 Section 5.9  
Silesian University of Technology in Gliwice Inverse approach for identification of the shrinkage gap thermal resistance in continuous casting of metals.
HEAT TRANSFER FINITE ELEMENT FORMULATION
Convection: Internal Flow ( )
Finite Deference Method
Heat Transfer Equations. Fouling Layers of dirt, particles, biological growth, etc. effect resistance to heat transfer We cannot predict fouling factors.
CHAP 3 WEIGHTED RESIDUAL AND ENERGY METHOD FOR 1D PROBLEMS
1 CHAP 5 FINITE ELEMENTS FOR HEAT TRANSFER PROBLEMS FINITE ELEMENT ANALYSIS AND DESIGN Nam-Ho Kim Audio by Raphael Haftka.
Discretization Methods Chapter 2. Training Manual May 15, 2001 Inventory # Discretization Methods Topics Equations and The Goal Brief overview.
Variational and Weighted Residual Methods
Lecture Objectives: -Define the midterm project -Lean about eQUEST -Review exam problems.
MECH4450 Introduction to Finite Element Methods
Lecture Objectives: Finish with system of equation for
Lecture Objectives: Continue with linearization of radiation and convection Example problem Modeling steps.
Chapter 2: Heat Conduction Equation
Chapter 3 Part 2 One-Dimensional, Steady-State Conduction.
ERT 216 HEAT & MASS TRANSFER Sem 2/ Dr Akmal Hadi Ma’ Radzi School of Bioprocess Engineering University Malaysia Perlis.
Implicit approximation can be solved using: Point iteration (G/S, SOR) Direct (matrix) solution Combination of matrix soln and iteration (used in MODFLOW)
Lecture Objectives: - Numerics. Finite Volume Method - Conservation of  for the finite volume w e w e l h n s P E W xx xx xx - Finite volume.
X1X1 X2X2  Basic Kinematics Real Applications Simple Shear Trivial geometry Proscribed homogenous deformations Linear constitutive.
Model Anything. Quantity Conserved c  advect  diffuse S ConservationConstitutiveGoverning Mass, M  q -- M Momentum fluid, Mv -- F Momentum fluid.
TUTORIAL 1 7/3/2016.
1 Variational and Weighted Residual Methods. 2 Introduction The Finite Element method can be used to solve various problems, including: Steady-state field.
FINITE DIFFERENCE In numerical analysis, two different approaches are commonly used: The finite difference and the finite element methods. In heat transfer.
HEAT TRANSFER Problems with FEM solution
The Finite Element Approach to Thermal Analysis Appendix A.
Li Xuemei Invitation to Heat Transfer Li xuemei
1 CHAP 3 WEIGHTED RESIDUAL AND ENERGY METHOD FOR 1D PROBLEMS FINITE ELEMENT ANALYSIS AND DESIGN Nam-Ho Kim.
Our task is to estimate the axial displacement u at any section x
INTRODUCTION : Convection: Heat transfer between a solid surface and a moving fluid is governed by the Newton’s cooling law: q = hA(Ts-Tɷ), where Ts is.
Chapter 3: One-Dimensional Steady-State Conduction
Extended Surface Heat Transfer
HW2 Example MatLab Code is posted on the course website
Numerical Method (Special Cases)
Lecture Objectives: Analysis of unsteady state heat transfer HW3.
Numerical Method (Special Cases)
HEAT TRANSFER Transient Conduction.
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.
Procedures in deriving element equations (General field problems)
Lecture Objectives: Discuss HW3
Steady-State Heat Transfer (Initial notes are designed by Dr
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.
Presentation transcript:

1 Convection Boundary Condition –Happens when a structure is surrounded by fluid –Does not exist in structural problems –BC includes unknown temperature (mixed BC) –Heat flow is not prescribed. Rather, it is a function of temperature on the boundary, which is unknown 1D Finite Element –When both Nodes 1 and 2 are convection boundary CONVECTION BC Wall TT T qhqh T1T1 T2T2 Fluid Temperature Convection Coefficient

2 EXAMPLE (CONVECTION ON THE BOUNDARY) Element equation Balance of heat flow –Node 1: –Node 2: –Node 3: Global matrix equation T1T1 T2T2 T3T3 12 h3h3 h1h1

3 EXAMPLE cont. Move unknown nodal temperatures to LHS The above matrix is P.D. because of additional positive terms in diagonal How much heat flow through convection boundary? –After solving for nodal temperature, use This is convection at the end of an element

4 EXAMPLE 5.5: FURNACE WALL Firebrick k 1 =1.2W/m/ o C h i =12W/m 2 / o C Insulating brick k 2 =0.2W/m/ o C h o =2.0W/m 2 / o C Firebrick T f = 1,500  C 0.25 m x Insulating brick T a = 20  C 0.12 m hoho hihi No heat flow 1,500  C x T1T1 T2T2 T3T3 TfTf TaTa 12 hoho hihi 20  C Convection boundary

5 CONVECTION ALONG A ROD Long rod is submerged into a fluid Convection occurs across the entire surface Governing differential equation Convection h b Fluid T  i j xixi xjxj

6 CONVECTION ALONG A ROD cont. DE with approximate temperature Minimize the residual with interpolation function N i (x) Integration by parts

7 CONVECTION ALONG A ROD cont. Substitute interpolation scheme and rearrange Perform integration and simplify Repeat the same procedure with interpolation function N j (x)

8 CONVECTION ALONG A ROD cont. Finite element equation with convection along the rod Equivalent conductance matrix due to convection Thermal load vector

9 EXAMPLE: HEAT FLOW IN A COOLING FIN k = 0.2 W/mm/  C, h = 2  10  4 W/mm 2 /  C Element conductance matrix Thermal load vector Element 1 Convection 330  C T  = 30  C 120 mm 160 mm 1.25 mm T1T1 T2T2 T3T3 T4T4 xInsulated 1 2 3

10 EXAMPLE: HEAT FLOW IN A COOLING FIN cont. Element conduction equation –Element 1 –Element 2 –Element 3 Balance of heat flow –Node 1 –Node 2 –Node 3 –Node 4

11 EXAMPLE: HEAT FLOW IN A COOLING FIN cont. Assembly Move T 4 to LHS and apply known T 1 = 330 Move the first column to RHS after multiplying with T 1 =330

12 EXAMPLE: HEAT FLOW IN A COOLING FIN cont. Solve for temperature