Fundamentals of Heat Transfer Muhammad Rashid Usman

Similar documents
Fundamentals of Heat Transfer Muhammad Rashid Usman

Fundamentals of Heat Transfer Muhammad Rashid Usman

University School of Chemical Technology

Fundamentals of Heat Transfer Muhammad Rashid Usman

Chapters 19 & 20 Heat and the First Law of Thermodynamics

Heat Transfer/Heat Exchanger

De-Coupler Design for an Interacting Tanks System

Experimental Analysis of Heat Transfer Augmentation in Double Pipe Heat Exchanger using Tangential Entry of Fluid

Effects of Radiation on Unsteady Couette Flow between Two Vertical Parallel Plates with Ramped Wall Temperature

Use of fin analysis for determination of thermal conductivity of material

Chapter 1 INTRODUCTION AND BASIC CONCEPTS

Compressor 1. Evaporator. Condenser. Expansion valve. CHE 323, October 8, Chemical Engineering Thermodynamics. Tutorial problem 5.

4.2 - Richardson Extrapolation

University School of Chemical Technology

(4.2) -Richardson Extrapolation

Numerical Differentiation

Department of Chemical Engineering. Year 2 Module Synopses

Section A 01. (12 M) (s 2 s 3 ) = 313 s 2 = s 1, h 3 = h 4 (s 1 s 3 ) = kj/kgk. = kj/kgk. 313 (s 3 s 4f ) = ln

Carnot Factor of a Vapour Power Cycle with Regenerative Extraction

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

CFD Analysis and Optimization of Heat Transfer in Double Pipe Heat Exchanger with Helical-Tap Inserts at Annulus of Inner Pipe

S.E. (Chemical) (Second Semester) EXAMINATION, 2012 HEAT TRANSFER (2008 PATTERN) Time : Three Hours Maximum Marks : 100

Desalination by vacuum membrane distillation: sensitivity analysis

Elmahdy, A.H.; Haddad, K. NRCC-43378

Determination of heat transfer intensity between free streaming water film and rigid surface using thermography

Lecture 10: Carnot theorem

HEAT TRANSFER. PHI Learning PfcO too1. Principles and Applications BINAY K. DUTTA. Delhi Kolkata. West Bengal Pollution Control Board

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

Solution for the Homework 4

C ONTENTS CHAPTER TWO HEAT CONDUCTION EQUATION 61 CHAPTER ONE BASICS OF HEAT TRANSFER 1 CHAPTER THREE STEADY HEAT CONDUCTION 127

INTRODUCTION DEFINITION OF FLUID. U p F FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION

DEVELOPMENT AND PERFORMANCE EVALUATION OF THERMAL CONDUCTIVITY EQUIPMENT FOR LABORATORY USES

A = h w (1) Error Analysis Physics 141

Some Review Problems for First Midterm Mathematics 1300, Calculus 1

Study of Convective Heat Transfer through Micro Channels with Different Configurations

Simulation and verification of a plate heat exchanger with a built-in tap water accumulator

Heat and Mass Transfer Unit-1 Conduction

(a) At what number x = a does f have a removable discontinuity? What value f(a) should be assigned to f at x = a in order to make f continuous at a?

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

Heat Transfer with Phase Change

The entransy dissipation minimization principle under given heat duty and heat transfer area conditions

LOSSES DUE TO PIPE FITTINGS

Fluids and Buoyancy. 1. What will happen to the scale reading as the mass is lowered?

MAT 145. Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points

Chapter: Heat and States

LAMINAR FORCED CONVECTION TO FLUIDS IN COILED PIPE SUBMERGED IN AGITATED VESSEL

Phase space in classical physics

Consider the element shown in Figure 2.1. The statement of energy conservation applied to this element in a time period t is that:

Exam 1 Review Solutions

Chapter 3 Thermoelectric Coolers

Logarithmic functions

Unit B-4: List of Subjects

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY

Law of Heat Transfer

Analysis: The speed of the proton is much less than light speed, so we can use the

Test 2 Review. 1. Find the determinant of the matrix below using (a) cofactor expansion and (b) row reduction. A = 3 2 =

Department of Mechanical Engineering ME 96. Free and Forced Convection Experiment. Revised: 25 April Introduction

Grade: 11 International Physics Olympiad Qualifier Set: 2

INSTRUCTOR: PM DR MAZLAN ABDUL WAHID

Optimization of flat tubular molten salt receivers

Chapter 2 HEAT CONDUCTION EQUATION

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

Taylor Series and the Mean Value Theorem of Derivatives

Physics 207 Lecture 23

Click here to see an animation of the derivative

Exam in Fluid Mechanics SG2214

Combining functions: algebraic methods

Thermodynamics Lecture Series

Large eddy simulation of turbulent flow downstream of a backward-facing step

Recall from our discussion of continuity in lecture a function is continuous at a point x = a if and only if

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is

Order of Accuracy. ũ h u Ch p, (1)

ME-662 CONVECTIVE HEAT AND MASS TRANSFER

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow Neale, A.; Derome, D.; Blocken, B.; Carmeliet, J.E.

HEAT TRANSFER 1 INTRODUCTION AND BASIC CONCEPTS 5 2 CONDUCTION

The Basics of Vacuum Technology

The Laplace equation, cylindrically or spherically symmetric case

INSTRUCTOR: PM DR MAZLAN ABDUL WAHID

Problem Solving. Problem Solving Process

Temperature control of two interacting rooms with decoupled PI Control

3.1 Extreme Values of a Function

Performance Prediction of Commercial Thermoelectric Cooler. Modules using the Effective Material Properties

Hall Effcts Eon Unsteady MHD Free Convection Flow Over A Stretching Sheet With Variable Viscosity And Viscous Dissipation

Mathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative

Math 1241 Calculus Test 1

Chapter 4 Optimal Design

Practice Problem Solutions: Exam 1

Derivatives and Rates of Change

8-4 P 2. = 12 kw. AIR T = const. Therefore, Q &

Continuity and Differentiability Worksheet

CFD calculation of convective heat transfer coefficients and validation Part I: Laminar flow. Annex 41 Kyoto, April 3 rd to 5 th, 2006

Prediction of Oil-Water Two Phase Flow Pressure Drop by Using Homogeneous Model

Exam 1 Solutions. x(x 2) (x + 1)(x 2) = x

PREFACE. Julian C. Smith Peter Harriott. xvii

Handling Missing Data on Asymmetric Distribution

y = 3 2 x 3. The slope of this line is 3 and its y-intercept is (0, 3). For every two units to the right, the line rises three units vertically.

10 Derivatives ( )

Journal of Chemical and Pharmaceutical Research, 2013, 5(12): Research Article

3 Minority carrier profiles (the hyperbolic functions) Consider a

Transcription:

Fundamentals of Heat Transfer Muammad Rasid Usman Institute of Cemical Engineering and Tecnology University of te Punjab, Laore. Figure taken from: ttp://eatexcanger-design.com/20/0/06/eat-excangers-6/ Dated: 7-Jan-202

Course contents final term Convection eat transfer: Free and forced convection. Rate equation for convective eat transfer coefficient. Brief description of ydrodynamic boundary layer and eat transfer coefficient. Units of eat transfer coefficient. Individual and overall eat transfer coefficients: plane wall and ollow cylinder. Numerical problems regarding overall eat transfer coefficient. Determination of eat transfer coefficient. Description of various eat transfer correlations. Log mean temperature difference. Numerical problems involving log mean temperature difference. Heat transfer in coiled and jacketed agitated vessels. Introduction to boiling and condensation. Types of boiling: Pool boiling and film boiling. Critical tickness of insulation. Brief description of eat transfer equipment: Heat excangers, furnaces, and evaporators. Radiation eat transfer: Basics of radiation eat transfer. Stefan-Boltzmann Law. Kircoff s law. Radiation eat transfer coefficient. Radiation to a small object from surroundings. View factors in radiation. Radiation in absorbing gases. 2

Te text book Please read and consult to know and learn. Geankoplis, C.J. (2003). Transport processes and separation process principles: includes unit operations. 4 t ed. Prentice- Hall International, Inc. 3

Convection eat transfer 4

Types of convective eat transfer Free or natural convection eat transfer Forced convection eat transfer 5

Free or natural convection eat transfer If te fluid motion is caused by itself due to difference in densities at two different points suc a process is natural or free convection eat transfer. Te density differences may be caused by temperature differences or concentration differences at two locations. In natural convection, no mecanical means are used to produce convective currents and convective mixing is a solely due to natural motion of te fluid. Boiling of milk and water and eating distant parts of a room in te presence of a room eater are common daily examples. 6

Forced convection eat transfer If te fluid motion is caused by some external or mecanical means te eat transfer is due to forced convection. Pumps, blowers, fans, agitation devices suc as impellers are employed for forced convection eat transfer. gitation using impellers in reaction vessels and pumping of fluids, at ig velocity, in eat excangers devices are te examples of forced convection. 7

Free and forced convection eat transfer In wic of te following cases do you expect greater rate of eat transfer?. Free convection 2. Forced convection 8

Newton s rate equation Rate of eat transfer per unit area is equal to te product of eat transfer coefficient and temperature difference between te eated surface and fluid far from te surface. q ( T s Tf ) q ( T s Tf ) q T f T s 642-727 9

Heat conduction troug a multilayer (composite) ollow cylinder-4: Problem (modified)-7 [p. 7, 2] ir at 20 C blows over a ot plate 50 by 75 cm wile maintained at 250 C. Te convection eat transfer coefficient is 25 W/m 2 K. Calculate te rate of eat transfer. Wat if eat transfer coefficient for te system is very ig or very low suc as 200 W/m 2 K and 0. W/m 2 K respectively. Wat is te direction of eat flow. T air = 20 C ir 75 cm 50 cm T s = 250 C 0

Heat transfer coefficient From te Newton s rate equation, it may be said tat eat transfer coefficient is te ability of te system, for wic it is defined, to transfer eat. Wat are te units of eat transfer coefficient?

Units of eat transfer coefficient SI units: J/s m 2 K or W/m 2 K W/m 2 K is equal to W/m 2 C Englis system: Btu/ ft 2 F Compare units of termal conductivity and eat transfer coefficient. 2

Heat transfer coefficient based on film model: Hydrodynamic boundary layer [p.58, 6] Fully developed boundary layer 3

Heat transfer coefficient based on film model Consider tickness of te film as Δx and k as te termal conductivity of te fluid (material of te film), ten it may be written tat k x Te main resistance to eat transfer is in tis film. Te eat transfer coefficient is sometimes called film coefficient. Note: Liquids and gases ave low termal conductivity. 4

Heat transfer coefficient based on film model Excerpt (p. 3.2) from Heat transfer by K.. Gavana, 8 t ed., Nirali Prakasan, Pune (2008). 5

Heat transfer coefficient based on film model For convective eat transfer, te film model suggests tat were ever a fluid flows past a solid surface tere is a film formed adjacent to te wall and tat tere is no turbulence in tis film and tis film offers te only resistance to eat transfer. It is important to mention ere tat for te film model, in te turbulent region (beyond te film) of a fluid tere is no problem for eat transfer, i.e. due to intense mixing, eat transfer is greatly enanced and tere is no temperature differential. 6

pproximate magnitudes of some eat transfer coefficients [] 7

Heat transfer coefficient based on film model Condensing steam (saturated steam) as ig eat transfer coefficient in contrast to supereated steam tat is wy a process engineer would like to eat a system using condensing steam and not by supereated steam. supereated steam beaves like a gas and you know gases ave low eat transfer coefficients. 8

Individual and overall eat transfer coefficients: plane wall [p. 249, ] Outside film resistance Inside film resistance Wall resistance 9

Individual and overall eat transfer coefficients: plane wall [p. 249, ] For inside film resistance: q i ( T T2) For wall resistance: q k ( T2 T 3) x For outside film: q ( T 3 T4) Wat if we ave two walls? o 20

2 Individual and overall eat transfer coefficients: plane wall [p. 249, ] i o k x T T q 4 k x T T q o i 4 te resistancein series all Sumof Overall temperature difference rate Heat

22 Individual and overall eat transfer coefficients: plane wall Reciprocal of overall resistance is overall conductance and frequently written in terms of overall eat transfer coefficient. i o k x U i o k x U ( 4) T T U q, k x U o i

Individual and overall eat transfer coefficients: plane wall Case : Wat if tickness of te wall wit ig termal conductivity is very small? Case 2: If one of te two film coefficients is a small value compared to te oter, ten major resistance is offered by te one wit small value and te coefficient is called as controlling film coefficient. Wat will be te form of te eat rate equation if i >>> o? Case 3: Wat if tere are a number of plane walls in series? Tink oter cases! 23

Individual and overall eat transfer coefficients: ollow cylinder Pipe wall resistance Outside fluid film resistance r 2 r Inside fluid film resistance 24

Individual and overall eat transfer coefficients: ollow cylinder q i i T T4 ln( r2 / r ) 2 k L o o Overall temperature difference Heat rate Sumof all te resistancein series 25

Individual and overall eat transfer coefficients: ollow cylinder U i i ln( r2 / r 2 k ) L o o Wic? Unlike plane wall, te inside and outside surface areas are different for cylindrical geometry. Te overall eat transfer coefficient is terefore as to be defined eiter on outside or inside surface of te ollow cylinder. 26

27 Individual and overall eat transfer coefficients: ollow cylinder o o i i i i L k r r U 2 ) / ln( 2 o o i i o o L k r r U 2 ) / ln( 2

References. Geankoplis, C.J. (2003). Transport processes and separation process principles: includes unit operations. 4 t ed. Prentice-Hall International, Inc. 2. Holman, J.P. (200). Heat transfer. 0 t ed. McGraw-Hill Higer Education, Singapore. 3. Cengel, Y.. (2003). Heat transfer: practical approac. 2 nd ed. McGraw-Hill. 4. Incropera, F.P.; DeWitt, D.P.; Bergman, T.L.; Lavine..S. (2007) Fundamentals of eat and mass transfer. 6 t ed. Jon Wiley & Sons, Inc. 5. Kern, D.Q. (965). Process eat transfer. McGraw-Hill International Book Co., Singapore. 6. McCabe, W.L.; Smit, J.C.; Harriott, P. (993). Unit operations of cemical engineering. 5 t ed. McGraw-Hill, Inc., Singapore. 7. Coulson, J.M.; Ricardson, J.F.; Backurst, J.R.; Harker, J.H. (999). Coulson and Ricardson s Cemical engineering: Fluid flow, eat transfer and mass transfer. vol.. 6 t ed. Butterwot-Heinemann, Oxford. 8. Staff of Researc and Education ssociation. (984). Te eat transfer problem solver. Researc and Education ssociation, New Jersey. 9. Kreit, F.; Manglik, R.M.; Bon, M.S. (20). Principles of eat transfer, 7 t ed., Cengage learning. 0. Mills.F. (995). Heat and mass transfer. Ricard D. Irwin, Inc. 28