The Meaning and Significance of Heat Transfer Coefficient. Alan Mueller, Chief Technology Officer

Similar documents
Tutorial for the heated pipe with constant fluid properties in STAR-CCM+

ME 331 Homework Assignment #6

Lectures on Applied Reactor Technology and Nuclear Power Safety. Lecture No 6

Convection Heat Transfer. Introduction

Lecture 30 Review of Fluid Flow and Heat Transfer

The Dominant Thermal Resistance Approach for Heat Transfer to Supercritical-Pressure Fluids

Introduction to Heat and Mass Transfer. Week 14

Internal Forced Convection. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

Learning Objectives. Lesson 6: Mathematical Models of Fluid Flow Components. ET 438a Automatic Control Systems Technology 8/27/2015

1. Nusselt number and Biot number are computed in a similar manner (=hd/k). What are the differences between them? When and why are each of them used?

PROBLEM 8.3 ( ) p = kg m 1m s m 1000 m = kg s m = bar < P = N m 0.25 m 4 1m s = 1418 N m s = 1.

CHME 302 CHEMICAL ENGINEERING LABOATORY-I EXPERIMENT 302-V FREE AND FORCED CONVECTION

طراحی مبدل های حرارتی مهدي کریمی ترم بهار HEAT TRANSFER CALCULATIONS

Multi-Fidelity Computational Flow Assurance for Design and Development of Subsea Systems and Equipment Simon Lo

Tutorial for the supercritical pressure pipe with STAR-CCM+

Analysis of fluid induced vibration of cryogenic pipes in consideration of the cooling effect

COMPUTATIONAL FLUID DYNAMICS ANALYSIS OF A V-RIB WITH GAP ROUGHENED SOLAR AIR HEATER

Heat Transfer Predictions for Carbon Dioxide in Boiling Through Fundamental Modelling Implementing a Combination of Nusselt Number Correlations

OUTCOME 2 - TUTORIAL 1

Heat Transfer Convection

Principles of Food and Bioprocess Engineering (FS 231) Problems on Heat Transfer

MAE 598 Project #1 Jeremiah Dwight

Lectures on Applied Reactor Technology and Nuclear Power Safety. Lecture No 7

Heat Transfer Modeling using ANSYS FLUENT

8.1 Technically Feasible Design of a Heat Exchanger

TABLE OF CONTENTS CHAPTER TITLE PAGE

Empirical Co - Relations approach for solving problems of convection 10:06:43

Laminar flow heat transfer studies in a twisted square duct for constant wall heat flux boundary condition

Piping Systems and Flow Analysis (Chapter 3)

Principles of Convection

HEAT TRANSFER ENHANCEMENT WITH ELLIPTICAL TUBE UNDER TURBULENT FLOW TiO 2 -WATER NANOFLUID

If there is convective heat transfer from outer surface to fluid maintained at T W.

Lesson 7: Thermal and Mechanical Element Math Models in Control Systems. 1 lesson7et438a.pptx. After this presentation you will be able to:

CONVECTIVE HEAT TRANSFER

Convection. forced convection when the flow is caused by external means, such as by a fan, a pump, or atmospheric winds.

NUMERICAL HEAT TRANSFER ENHANCEMENT IN SQUARE DUCT WITH INTERNAL RIB

BAE 820 Physical Principles of Environmental Systems

Heat Transfer Properties of Hydrogen Peroxide

PROBLEM h fg ρ v ρ l σ 10 3 T sat (kj/kg) (kg/m 3 ) (N/m) (K)

Chapter (4) Motion of Fluid Particles and Streams

Exergy Optimisation for Cascaded Thermal Storage

ELEC9712 High Voltage Systems. 1.2 Heat transfer from electrical equipment

Convection. U y. U u(y) T s. T y

Principles of Food and Bioprocess Engineering (FS 231) Exam 2 Part A -- Closed Book (50 points)

Introduction to Heat and Mass Transfer. Week 14

A New Method for Calculating Oil-Water Relative Permeabilities with Consideration of Capillary Pressure

SHELL-AND-TUBE TEST PROBLEMS

ME 431A/538A/538B Homework 22 October 2018 Advanced Fluid Mechanics

A Comprehensive Method for the Characterization of Engine Heat Rejection

Internal Flow: Heat Transfer in Pipes

External Flows. Dye streak. turbulent. laminar transition

Outlines. simple relations of fluid dynamics Boundary layer analysis. Important for basic understanding of convection heat transfer

PROBLEM ρ v (kg/m 3 ) ANALYSIS: The critical heat flux can be estimated by Eq with C = 0.

Computational Fluid Dynamics Based Analysis of Angled Rib Roughened Solar Air Heater Duct

TankExampleNov2016. Table of contents. Layout

PREDICTION OF MASS FLOW RATE AND PRESSURE DROP IN THE COOLANT CHANNEL OF THE TRIGA 2000 REACTOR CORE

Steam Generator Tubing Inspection

Chapter 5 MATHEMATICAL MODELING OF THE EVACATED SOLAR COLLECTOR. 5.1 Thermal Model of Solar Collector System

Chapter 3 NATURAL CONVECTION

Initial and Boundary Conditions

Tutorial 11. Use of User-Defined Scalars and User-Defined Memories for Modeling Ohmic Heating

Fall 2014 Qualifying Exam Thermodynamics Closed Book

Heat processes. Heat exchange

MYcsvtu Notes HEAT TRANSFER BY CONVECTION

Analysis of the Cooling Design in Electrical Transformer

Natural Convection from a Long Horizontal Cylinder

Convection Workshop. Academic Resource Center

Pressure Losses for Fluid Flow Through Abrupt Area. Contraction in Compact Heat Exchangers

INTERNATIONAL JOURNAL OF SCIENTIFIC & TECHNOLOGY RESEARCH VOLUME 5, ISSUE 09, SEPTEMBER 2016 ISSN

IJSRD - International Journal for Scientific Research & Development Vol. 3, Issue 06, 2015 ISSN (online):

ESRL Module 8. Heat Transfer - Heat Recovery Steam Generator Numerical Analysis

UNIT II CONVECTION HEAT TRANSFER

Introduction to Heat and Mass Transfer. Week 12

HEAT EXCHANGER. Objectives

EXPERIMENTAL AND CFD ANALYSIS OF TURBULENT FLOW HEAT TRANSFER IN TUBULAR HEAT EXCHANGER

Chapter 6 Fundamental Concepts of Convection

EXPERIMENTAL AND CFD ANALYSIS OF TURBULENT FLOW HEAT TRANSFER IN TUBULAR EXCHANGER

EXPERIMENTAL AND THEORETICAL ANALYSIS OF TRIPLE CONCENTRIC TUBE HEAT EXCHANGER

HEAT TRANSFER. Mechanisms of Heat Transfer: (1) Conduction

Introduction to Heat and Mass Transfer. Week 9

cen29305_ch08.qxd 11/30/05 3:05 PM Page 451 INTERNAL FORCED CONVECTION CHAPTER 8 Liquid or gas flow through pipes or ducts is commonly used in heating

CFD Analysis on Flow Through Plate Fin Heat Exchangers with Perforations

Minimizing and maximizing compressor and turbine work respectively

Liquid or gas flow through pipes or ducts is commonly used in heating and

CHAPTER 7 NUMERICAL MODELLING OF A SPIRAL HEAT EXCHANGER USING CFD TECHNIQUE

Chapter 7: External Forced Convection. Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University

Lecture 22. Mechanical Energy Balance

Overview of Convection Heat Transfer

Design of Heat Transfer Equipment

Overview of Convection Heat Transfer

Thermo-Fluid Dynamics of Flue Gas in Heat Accumulation Stoves: Study Cases

Numerical Analysis of Fe 3 O 4 Nanofluid Flow in a Double Pipe U-Bend Heat Exchanger

Performance evaluation of heat transfer enhancement for internal flow based on exergy analysis. S.A. Abdel-Moneim and R.K. Ali*

Water Circuit Lab. The pressure drop along a straight pipe segment can be calculated using the following set of equations:

Application of Solution Mapping to Reduce Computational Time in Actively Cooled Power Electronics

Prepared by: Simanto. Date: Sunday, August 17, 2014

CONCENTRIC EXCHANGER TEST PROBLEMS

COMBINED EFFECTS OF RADIATION AND JOULE HEATING WITH VISCOUS DISSIPATION ON MAGNETOHYDRODYNAMIC FREE CONVECTION FLOW AROUND A SPHERE

Transient Thermal Flow and Thermal Stress Analysis Coupled NASTRAN and SC/Tetra

Chapter 2 Mass Transfer Coefficient

Transcription:

The Meaning and Significance of Heat Transfer Coefficient Alan Mueller, Chief Technology Officer

The Meaning of Heat Transfer Coefficient I kno the meaning of HTC! Why should I aste my time listening to your presentation? What is the difference beteen the STAR-CCM+ Field Functions? Heat Transfer Coefficient Local Heat Transfer Coefficient Virtual Heat Transfer Coefficient Specified Y+ Heat Transfer Coefficient 2

HTC is not the hole picture HTC expresses a linear relation beteen the heat flux at the all and the difference in a reference temperature and the all temperature ( ) q = ht T ref The heat flux is, in general, some very complicated function The linear relation is only an approximation Often referred to as Neton s la of cooling 3

The meaning of Reference Temperature OK, I kno the meaning of heat flux and all temperature, hat is reference temperature? Well duh!, its simply the temperature that satisfies T ref = T + q h h = In textbooks often it is some far-field temperature, or some inlet temperature For boiling heat often it is the boiling saturation temperature Heat transfer coefficient and reference temperature come in pairs Can not define one ithout the other Only all heat flux and all temperature are unambiguous T ref q T

Tref is it important Some of the confusion is that literature focuses on HTC but little on its relationship to the Tref Physical and Computational Aspects of Heat Transfer, Cebeci & Bradsha, Springer-Verlag, 1991 Developing Laminar Duct Flo N u ( x) hxd ( ) q( xd ) = = k T x T x k ( ( ) m( )) T m ( x) = A ( ) ρuxrt (, ) xr, da A ρu( x, r) da????

Conduction Heat Flux in a Boundary Layer Heat flux in Boundary Layer ρ c u ( Tf T) ρ c u q = τ + h= T T T T + = f p, f τ f p, f,, ref f ( + y ) All the physics is in T + and u τ T ( y ) + + ( + ( + u y ) P( )) + + + y > y, Pr Pr / Pr, T T T trans = + + + Pr y, y yt, trans 6

HTC Field Functions in STAR-CCM+ heat transfer coefficient user specifies T ref h = ( T T ) ref q local heat transfer coefficient & local heat transfer reference temperature local la of all near all cell temperature h T ref 7

HTC Field Functions in STAR-CCM+ virtual local heat transfer coefficient local la of all h evaluated at near all cell need not solve energy transport mute about the reference temperature 8

HTC Field Functions in STAR-CCM+ specified y+ heat transfer coefficient & specified y+ heat transfer reference temperature user specifies y+ but uses properties at the cell adjacent to the all h = ρ c T c + pc, u τ ( + y ) y + h T T ref T ref = T + q h 9

Pipe flo example specified q =1e6 W/m 2 Description Value Pipe diameter (cm) 1 Pipe length (cm) 25 Reynolds number 50,000 Inlet temperature 300 K Uniform heat flux at the alls 1E6 W/m2 Density 1000 kg/m3 Specific heat 4200 J/kg-C Dynamic viscosity 0.001 Pa-s Thermal conductivity 0.6 W/m-K Laminar Pr number 7.0 Turbulent Pr number 0.9 10

High y + mesh (near-all cell y + = 150) Wall Treatment All Y+ All Y+ % Error High Y+ High Y+ % Error Turbulence Model RKE 2-layer RKE Wall Temperature 359.39 359.22 Friction velocity u_tau 0.246 0.2465 Local HTC 19150 19202 Local HT Ref Temp 307.17 307.13 Heat Flux 1000013 0.0 1000232 0.0 HTC 16838 16888 Reference Temp for HTC 300 300 Heat Flux 1000009 0.0 1000107 0.0 Specified Y+ HTC 19154 19207 Specified Y+ HT Ref Temp 307.18 307.15 Specified Y+ 150 150 Heat Flux 99963 0.0 1000108 0.0 Virtual Local HTC 19150 19201 Reference Temp for Virtual Local HTC 300 300 Heat Flux 1137318 13.7 1137083 13.7 Dittus Boelter 18000 18000 11

lo y + mesh (near-all cell y + = 2) Wall Treatment All Y+ All Y+ % Error High Y+ High Y+ % Error Lo Y+ Lo Y+ % Error Turbulence Model RKE SKE Lo RKE 2-layer Re Wall Temperature 357.17 327.95 353.37 Friction velocity u_tau 0.239 0.314 0.258 Local HTC 89693 83570 85825 Local HT Ref Temp 346.0 316.0 341.7 Heat Flux 1001870 0.2 998662-0.2 100415-0.4 HTC 17492 35760 18739 Reference Temp for HTC 300 300 300 Heat Flux 1000018 0.0 999492 0.0 100098-0.1 Specified Y+ HTC 18612 24460 NA Specified Y+ HT Ref Temp 303.44 287.1 NA Specified Y+ 150 150 NA Heat Flux 1000023 0.0 999191 0.1 NA Virtual Local HTC 89693 83570 NA Reference Temp for Virtual Local HTC 300 300 NA Heat Flux 5127749-412.77 2335781-133.6 NA Dittus Boelter 18000 18000 18000

Lessons Learned Virtual heat transfer coefficient can be misleading Not paired to any Reference Temperature May not be near textbook HTC Best Practice: Specified y+ heat transfer coefficient For a good guess of y+ then all is consistent ith textbook Not as sensitive to choice of reference temperature 13

Lessons Learned Heat transfer coefficient is not safe Poor choice of reference temperature can lead to negative HTC Difficult to apply hen temperature changes as the fluid cools don or heats up don the axis of the pipe. 14

Lessons learned Local heat transfer coefficient Dangerous if not used ith the local heat transfer reference temperature For lo Re meshes ill give values not anyhere near textbook values. Specified Y+ HTC is good compromise Likely the best option for cycle averaging T ref = T + q h 15

Lessons Learned At least for this constant property example Wall treatment models give reasonable surface temperatures hen used properly The default all y+ is the best for all prism layer meshes size range 16

Heat Transfer in Explicit Coupled Problems Couple to Abaqus T Abaqus => STAR-CCM+ Option 1: (Best Practice) HTC, Tref STAR-CCM+ => Abaqus, or Option 2: Heat flux STAR-CCM+ => Abaqus Option 3: Heat flux Abaqus => STAR-CCM+ T STAR-CCM+ => Abaqus Best Unstable Practice because :Initial T heat is resistance same in both in fluid codes is higher than in solid 17

Heat Transfer in a Exhaust Manifold 18

HTC= Local Heat Transfer Coefficient HTC,Tref Steady Heat flux Steady Heat Unstable!!! Flux, t=100s Heat HTC,Tref Flux, t=10s HTC,Tref t=100s 19

HTC Specified Y+ Heat transfer Coefficient HTC,Tref, y+=200 t=100s HTC,Tref, y+=1e6 t=100s 20

Y+=1e6, and still very accurate!?? HTC,Tref, y+=1e6 t=10s 21

Steady-state Solution in about 2 iterations HTC,Tref, y+=2000

Heat Applied in Abaqus Linear form ( n+ 1 T ) ref q = h T n+ 1 n n ( ) ( ) q = h T T + h T T n+ 1 n n n n n+ 1 n ref What must be accurate is the heat flux! q = q + h T ( + T ) n+ 1 n n n 1 n dq dt Heat flux is linear expansion about all temp Reference Heat Transfer Temperature Coefficient does is more not appear! numerical Exchanging heat flux only is same as n in nature it stabilizes the solution h = 0

Specified Y+ HTC in Coupled Simulations Can be used to give best estimate of the heat at the end of the time step ( ) q = q + h T T n+ 1 n n n+ 1 n The actual physics of the choice of HTC using boundary layer theory is not as important as getting the heat flux correct HTC is not important at all if time step is small 24

Conclusions HTC and Reference Temp come in pairs HTC choices may not be satisfactory if not paired to the proper Reference Temperature Specified Y+ HTC recommended Coupling to other codes Solid passes all temperature Fluid passes HTC and Reference Temperature such that T ref = T + Initial Wall temperatures same in both codes q h