Boiling and Condensation (ME742)

Size: px
Start display at page:

Download "Boiling and Condensation (ME742)"

Transcription

1 Indian Institute of Technology Kanpur Department of Mechanical Engineering Boiling and Condensation (ME742) PG/Open Elective Credits: Updated Syllabus: Introduction: Applications of boiling and condensation. Difference between evaporation and boiling. Comparison of Nucleate and Convective (or Flow) boiling. Pool boiling: Nukiyama Experiment. Theory of vapour bubble formation: Homogeneous and Heterogeneous Nucleation. Bubble Growth Models. Mechanism of Critical Heat Flux (CHF). Various models and correlations. Pool Boiling of Binary Mixture. Flow Boiling: homogeneous and heterogeneous models. Flow Boiling in Microchannels. Flow Boiling of Binary Mixtures. Boiling enhancement techniques. Film and dropwise condensation. Nusselt s analysis of laminar film condensation on vertical plate, single horizontal tube and vertical array of tubes. Laminar-wavy and turbulent film condensation. Film condensation inside horizontal tubes. Condensation enhancement techniques. Special topics (Suggested): Boiling in Microgravity Environment. Boiling of Nanofluids. Liquid Metals Boiling. Boiling on Structured Surfaces. Effect of Non-condensable Gases in Vapour on Condensation. Numerical Modelling of Boiling and Condensation Heat Transfer. Special topics: Boiling of Nanofluids. Computer Simulation of Pool Boiling by the Coupled Map Lattice Method. Lecture-by-Lecture Break-up (Three 50 min lectures per week) Lecture # 1: Introduction: Applications of Boiling and Condensation: Thermal Power Plant Cycle. Ideal Vapour-Compression Refrigeration Cycle. Immersion Cooling of Computers. Heat Pipe. Lecture # 2: Difference between Evaporation and Boiling. Evaporation: Benard Convection. The typical temperature profile in the evaporating liquid. Definition of h. Why Tsat is used in the definition of h? Nucleate Boiling: Bubble Nucleation. Temperature Profile in Water. Comparison of h vs.q // plots for evaporation and nucleate boiling of water at 1 atm. Lecture # 3: Convective Boiling: Various flow regimes in a vertical heated tube. Comparison of nucleate boiling and convective boiling. Lecture # 4: Review of Thermodynamics of Phase Change of Pure Substances: subcooled liquid, saturated liquid, saturated liquid-vapour mixture, saturated vapour, superheated vapour, critical point. Psat vs. Tsat plot: Clapeyron Equation and Clausius- 1

2 Clapeyron Equation. Triple Point. Superheated liquid: Definition. Application in boiling. Concept of metastable equilibrium of vapour bubble and superheated liquid. Lecture # 5: Interfacial Tension: Explanation from Molecular Point of View. Formation of Vapour Bubbles: Derivation of the expression for the diameter of a spherical vapour bubble in thermal and mechanical equilibrium with its superheated liquid. Theory of heterogeneous nucleation (to be continued). Lecture # 6: Heterogeneous Nucleation. Expression of Mikic and Rohsenow (1969) for Activation Superheat of a Cavity. Homogeneous Nucleation. Spinodal lines and metastable states on a p-v diagram. Bubble Growth near a Heated Surface: Liquid Inertia Controlled Growth and Heat Transfer Controlled Growth. Lecture # 7: Mathematical Modelling of heat-transfer controlled bubble growth in the non-uniform temperature field near a superheated wall: Model of Mikic and Rohsenow (1969): Basic assumptions. Expression for the waiting time. Expression for the rate of growth of bubble (to be continued). Lecture # 8: Expression for the rate of bubble growth (completed). Example Problem. Bubble Departure Diameter and the Frequency of Bubble Release: Definition of the frequency of bubble release. Various mechanisms of bubble release. Sample Correlations for Departure Diameter: Fritz (1935), Zuber (1959) and Cole (1967). Lecture # 9: Frequency of Bubble Release: Influencing factors. Correlations for frequency of bubble release (valid in the intermediate regime between inertia and heattransfer controlled growth): Jacob and Fritz (1931), Peebles and Garber (1953), Zuber (1963). Basic forms of correlations given by Ivey (1967) for inertia controlled growth and heat-transfer controlled growth. Favourable conditions for inertia controlled growth and heat-transfer controlled growth. Example Problem. Lecture # 10: Pool Boiling: Definition. Applications. Temperature Controlled Saturated Pool Boiling Curve for a Large Horizontal Surface: Various regimes. Maximum or Critical heat flux (CHF). Minimum heat flux. Points of difference between heating and cooling curves: (a) Contact angle hysteresis in transition regime; (b) near onset of nucleation condition. Heat Flux Controlled Curve: Various regimes. Points of difference between heating and cooling curves: hysteresis effect (Missing transition regime). Lecture # 11: Single Composite Pool Boiling Curve showing heating and cooling for both temperature and heat flux controlled modes. Definition of CHF for temperature controlled and heat flux controlled modes. Definition of Minimum Heat Flux. Experiment of Nukiyama (1934): Saturated Pool Boiling of Water at Atmospheric Pressure (to be continued). Lecture # 12: Details of Nukiyama Experiment: Equipments used. Experimental Procedure. Sources of Experimental Error. Results. Maximum and Minimum heat 2

3 fluxes. High speed video camera pictures of heat flux controlled saturated pool boiling showing regimes till CHF. Lecture # 13: h vs. Tw plot in Pool Boling: Explanation. Heat Transfer Mechanism during Nucleate Boiling: Rohsenow s Model and its basis. Rohsenow (1952) Correlation. Lecture # 14: Stephan and Abdelsalam Correlation (1980): Basis. Correlations for water, hydrocarbons, cryogenic fluids, and refrigerants. Unified correlation valid for all fluids (lower accuracy). Simpler and easy-to-use correlations. Surface roughness // correction. Comparison of q vs. Tw graphs on log-log plot for boiling of water at 1 bar using Rohsenow (1952) and, Stephan and Abdelsalam (1980) correlations. Lecture # 15: Basic approaches used in the making of pool boiling correlations. Applicability of pool boiling correlations for horizontal tubes/surfaces to other geometries/orientations. Example Problems. Liquid Metals Pool Boiling: Physics. Basic differences with respect to boiling of normal fluids. Subbotin et al. (1970) Correlation. Lecture # 16: Transition Boiling and Taylor Instability. Helmholtz Instability. Mechanism of CHF: Derivation of Zuber (1959) Correlation using Taylor instability and Helmholtz instability theories. Lecture # 17: Summary of Zuber s Hypothesis. Drawbacks of Zuber s Model. Effect of geometry on CHF: Correlations given by Lienhard and co-workers for square and round heated surfaces of finite size. Example Problem. Lecture # 18: Accuracy of CHF Correlations given by Lienhard and co-workers. CHF Correlation for Liquid Metals. CHF as a Function of Pressure: Explanation for the nature of the curve. Stephan (1992) Correlation for organic fluids and water. Example Problem. Lecture # 19: Criticisms on Zuber s Model of CHF. Effect of Surface Wetting Characteristics: Pool boiling on a completely non-wetted surface. Alternative Model of Kandlikar (2001) for predicting CHF: Postulate. Basic Mechanism. Model Description. Derivation of CHF. Kandlikar s expression of CHF for saturated pool boiling of pure liquids. Validation with earlier experiments. Lecture # 20: Kandlikar s Model of CHF (Contd.): Effect of bubble contact angle and plate inclination on CHF. Difficulties in the use of Kandlikar s correlation. Lecture # 21: Minimum Heat Flux: Zuber(1959) theory and correlation, and modification by Berenson (1961) for Infinite Plate. Lienhard and Wong (1963) Correlation for Horizontal Cylinder. Film Boiling: Bromley (1950) Correlations for horizontal cylinder and sphere. Berenson (1961) Correlation for Infinite Horizontal Surface. Effect of Radiation on Film Boiling: Correction by Bromley (1950). Film Boiling on Finite Horizontal Surface. 3

4 Lecture # 22: Example Problem on Film Boiling. Summary of Saturated Pool Boiling. Lecture # 23: Parametric Effects on Pool Boiling: Effect of Subcooling. Kutateladze(1952) correlation for CHF in Subcooled Boiling. Effect of Gravity (to be continued). Lecture # 24: Effect of Gravity (Completed). Effect of Size and Wettability. Effect of Surface Roughness. Flow Boiling: Introduction. Lecture # 25: Basic Terms and Definitions in Two-Phase Flows. Basic Model and Governing Equations (Conservation of Mass and Momentum) for One-dimensional Two- Phase Flow: Assumptions and derivations. Expression of total axial pressure gradient in terms of frictional effect at the wall, gravitational head effect and acceleration (or deceleration) of the flow. Lecture # 26: Calculation of Frictional Pressure Gradient: Definition of Two-Phase Multipliers, φ l, φlo, φv. Homogeneous Flow: Basic definition and idealizations. 2 Derivation of the expression for φ lo. Heterogeneous Flow: Basic definition. Method of Lockhart and Martinelli (1949): Basic philosophy. Concept of Correction factor or Martinelli parameter, X. To be continued. Lecture # 27: Heterogeneous Flow (Completed): Details of the method and its accuracy and limitations. Profile of ( dp / dz) fr vs. z: Physical Explanation. Example Problem. (Homogeneous Flow). Lecture # 28: Variation of φ l and φ v as well as α with X: Physical Explanation. Basic Procedure for obtaining Pressure Drop in a Two-Phase Flow. Example Problem. (Heterogeneous Flow). To be continued. Lecture # 29: Example Problem (Completed). Lecture # 30: Regimes of Convective Boiling in Round Tubes. Method of Calculating Heat Transfer Coefficient in Two-Phase Flows: Chen (1966) Correlation for vertical tube. Example Problem (to be continued). Lecture # 31: Example Problem (Completed). Modification to Chen s Correlation: Bennett and Chen (1980) Correlation. Condition of applicability of Chen s Correlation to flow boiling in horizontal tubes. Correlation for stratified flow boiling in horizontal tubes. Gungor and Winterton (1986) Correlation for vertical tube flow boiling. Boiling Regime Map for Constant Wall Flux Condition: Departure from nucleate boiling and dryout. Why is thermodynamic quality negative in subcooled boiling and greater than 1 in drop flow regime? To be continued. 4

5 Lecture # 32: Real Quality vs. Thermodynamic Quality (Completed). Critical Boiling States: Definition of CHF in flow boiling. Boiling Crisis at low quality and at high quality. Plot of CHF vs. Quality. Condensation: Definition. Dropwise and Film Condensation. Nusselt s Analysis of Laminar Film Condensation on a Vertical Flat Plate: Basic Assumptions. To be continued. Lecture # 33: Nusselt s Analysis (Completed): Derivation of expression of average heat transfer coefficient and average Nusselt number. Lecture # 34: Expression for mass rate of condensation. Effect of Subcooling: Derivation of the expression for modified latent heat of condensation h / fg. Turbulent Film Condensation over a Vertical Plate: Definition of film condensation Reynolds number. Various regimes of film condensation flow such as laminar, laminar-wavy and turbulent and transition criteria. Experimental correlations for average heat transfer coefficient for laminar-wavy and turbulent regimes. Basic method of solution of film condensation problems: Why are iterations required? Example Problem (to be continued). Lecture # 35: Example Problem (Completed). Laminar Film Condensation over a Single Horizontal Tube (Nusselt s Approach): Derivation of the expression for Lecture # 36: Laminar Film Condensation on a Vertical Tier of n tubes: Nusselt s Analysis. Chen (1961) Correlation: Modification of Nusselt s correlation. Calculation of total condensation rate on a square array of tubes. Staggered Tube Arrangement. Effect of vapour velocity and non-condensable gases in the vapour. Lectures # 37-40: Special Topics: Boiling of Nanofluids. Computer Simulation of Pool Boiling by the Coupled Map Lattice Method h D. Reference Books 1. Stephan K, 1992, Heat Transfer in Condensation and Boiling, Springer-Verlag, Berlin. 2. Carey, V.P., 2008, Liquid-Vapor Phase-Change Phenomena, 2nd edn, Taylor & Francis, New York. 5

Chapter 10: Boiling and Condensation 1. Based on lecture by Yoav Peles, Mech. Aero. Nuc. Eng., RPI.

Chapter 10: Boiling and Condensation 1. Based on lecture by Yoav Peles, Mech. Aero. Nuc. Eng., RPI. Chapter 10: Boiling and Condensation 1 1 Based on lecture by Yoav Peles, Mech. Aero. Nuc. Eng., RPI. Objectives When you finish studying this chapter, you should be able to: Differentiate between evaporation

More information

heat transfer process where a liquid undergoes a phase change into a vapor (gas)

heat transfer process where a liquid undergoes a phase change into a vapor (gas) Two-Phase: Overview Two-Phase two-phase heat transfer describes phenomena where a change of phase (liquid/gas) occurs during and/or due to the heat transfer process two-phase heat transfer generally considers

More information

Module 8: BoiIing Lecture 29: Boiling Heat Transfer. The Lecture Contains: Introduction. Boiling modes. Pool Boiling. Correlations in Pool Boiling

Module 8: BoiIing Lecture 29: Boiling Heat Transfer. The Lecture Contains: Introduction. Boiling modes. Pool Boiling. Correlations in Pool Boiling The Lecture Contains: Introduction Boiling modes Pool Boiling Correlations in Pool Boiling file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_1.html[12/24/2014

More information

We know from thermodynamics that when the temperature of a liquid

We know from thermodynamics that when the temperature of a liquid cen58933_ch10.qxd 9/4/2002 12:37 PM Page 515 BOILING AND CONDENSATION CHAPTER 10 We know from thermodynamics that when the temperature of a liquid at a specified pressure is raised to the saturation temperature

More information

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

C ONTENTS CHAPTER TWO HEAT CONDUCTION EQUATION 61 CHAPTER ONE BASICS OF HEAT TRANSFER 1 CHAPTER THREE STEADY HEAT CONDUCTION 127 C ONTENTS Preface xviii Nomenclature xxvi CHAPTER ONE BASICS OF HEAT TRANSFER 1 1-1 Thermodynamics and Heat Transfer 2 Application Areas of Heat Transfer 3 Historical Background 3 1-2 Engineering Heat

More information

Fluid Flow, Heat Transfer and Boiling in Micro-Channels

Fluid Flow, Heat Transfer and Boiling in Micro-Channels L.P. Yarin A. Mosyak G. Hetsroni Fluid Flow, Heat Transfer and Boiling in Micro-Channels 4Q Springer 1 Introduction 1 1.1 General Overview 1 1.2 Scope and Contents of Part 1 2 1.3 Scope and Contents of

More information

Module 8: BoiIing Lecture 34: Analysis of Bubble Formation on a Heated Wall. The Lecture Contains: Bubble Growth with Heat and Mass Transfer

Module 8: BoiIing Lecture 34: Analysis of Bubble Formation on a Heated Wall. The Lecture Contains: Bubble Growth with Heat and Mass Transfer The Lecture Contains: Bubble Growth with Heat and Mass Transfer Simple Analysis of Bubble Growth in a Uniform Temperature Field file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture34/34_1.html[12/24/2014

More information

: HEAT TRANSFER & EVAPORATION COURSE CODE : 4072 COURSE CATEGORY : B PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 70 CREDIT : 5 TIME SCHEDULE

: HEAT TRANSFER & EVAPORATION COURSE CODE : 4072 COURSE CATEGORY : B PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 70 CREDIT : 5 TIME SCHEDULE COURSE TITLE : HEAT TRANSFER & EVAPORATION COURSE CODE : 4072 COURSE CATEGORY : B PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 70 CREDIT : 5 TIME SCHEDULE MODULE TOPIC PERIODS 1 Conduction,Fourier law,variation

More information

Chapter 3 PROPERTIES OF PURE SUBSTANCES. Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008

Chapter 3 PROPERTIES OF PURE SUBSTANCES. Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008 Chapter 3 PROPERTIES OF PURE SUBSTANCES Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008 Objectives Introduce the concept of a pure substance. Discuss

More information

CONVECTION HEAT TRANSFER

CONVECTION HEAT TRANSFER CONVECTION HEAT TRANSFER THIRD EDITION Adrian Bejan J. A. Jones Professor of Mechanical Engineering Duke University Durham, North Carolina WILEY JOHN WILEY & SONS, INC. CONTENTS Preface Preface to the

More information

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

PROBLEM h fg ρ v ρ l σ 10 3 T sat (kj/kg) (kg/m 3 ) (N/m) (K) PROBLEM 10.9 KNOWN: Fluids at 1 atm: mercury, ethanol, R-1. FIND: Critical heat flux; compare with value for water also at 1 atm. ASSUMPTIONS: (1) Steady-state conditions, () Nucleate pool boiling. PROPERTIES:

More information

CONVECTION HEAT TRANSFER

CONVECTION HEAT TRANSFER CONVECTION HEAT TRANSFER SECOND EDITION Adrian Bejan J. A. Jones Professor of Mechanical Engineering Duke University Durham, North Carolina A WILEY-INTERSCIENCE PUBUCATION JOHN WILEY & SONS, INC. New York

More information

HEAT AND MASS TRANSFER. List of Experiments:

HEAT AND MASS TRANSFER. List of Experiments: HEAT AND MASS TRANSFER List of Experiments: Conduction Heat Transfer Unit 1. Investigation of Fourier Law for linear conduction of heat along a simple bar. 2. Study the conduction of heat along a composite

More information

Heat Transfer with Phase Change

Heat Transfer with Phase Change CM3110 Transport I Part II: Heat Transfer Heat Transfer with Phase Change Evaporators and Condensers Professor Faith Morrison Department of Chemical Engineering Michigan Technological University 1 Heat

More information

Introduction to Heat and Mass Transfer. Week 12

Introduction to Heat and Mass Transfer. Week 12 Introduction to Heat and Mass Transfer Week 12 Next Topic Convective Heat Transfer» Heat and Mass Transfer Analogy» Evaporative Cooling» Types of Flows Heat and Mass Transfer Analogy Equations governing

More information

Uncertainty Analysis on Prediction of Heat Transfer Coefficient and Pressure Drop in Heat Exchangers Due to Refrigerant Property Prediction Error

Uncertainty Analysis on Prediction of Heat Transfer Coefficient and Pressure Drop in Heat Exchangers Due to Refrigerant Property Prediction Error Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2014 Uncertainty Analysis on Prediction of Heat Transfer Coefficient and Pressure

More information

Thermodynamics I. Properties of Pure Substances

Thermodynamics I. Properties of Pure Substances Thermodynamics I Properties of Pure Substances Dr.-Eng. Zayed Al-Hamamre 1 Content Pure substance Phases of a pure substance Phase-change processes of pure substances o Compressed liquid, Saturated liquid,

More information

Evaporation (Chapter 14) Zan Wu Room: 5123

Evaporation (Chapter 14) Zan Wu Room: 5123 Evaporation (Chapter 14) Zan Wu zan.wu@enery.lth.se Room: 5123 Evaporation, Boilin vätska, liquid 1) Local boilin or subcooled boilin 2) Boilin with net evaporation q Pool boilin Forced convective boilin

More information

Multiphase Flow and Heat Transfer

Multiphase Flow and Heat Transfer Multiphase Flow and Heat Transfer ME546 -Sudheer Siddapureddy sudheer@iitp.ac.in Two Phase Flow Reference: S. Mostafa Ghiaasiaan, Two-Phase Flow, Boiling and Condensation, Cambridge University Press. http://dx.doi.org/10.1017/cbo9780511619410

More information

Introduction to Heat and Mass Transfer. Week 14

Introduction to Heat and Mass Transfer. Week 14 Introduction to Heat and Mass Transfer Week 14 HW # 7 prob. 2 Hot water at 50C flows through a steel pipe (thermal conductivity 14 W/m-K) of 100 mm outside diameter and 8 mm wall thickness. During winter,

More information

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

PROBLEM ρ v (kg/m 3 ) ANALYSIS: The critical heat flux can be estimated by Eq with C = 0. PROBLEM 10.10 KNOWN: Fluids at 1 atm: mercury, ethanol, R-14a. FIND: Critical heat flux; compare with value for water also at 1 atm. ASSUMPTIONS: (1) Steady-state conditions, () Nucleate pool boiling.

More information

A SHORT INTRODUCTION TO TWO-PHASE FLOWS Condensation and boiling heat transfer

A SHORT INTRODUCTION TO TWO-PHASE FLOWS Condensation and boiling heat transfer A SHORT INTRODUCTION TO TWO-PHASE FLOWS Condensation and boiling heat transfer Hervé Lemonnier DM2S/STMF/LIEFT, CEA/Grenoble, 38054 Grenoble Cedex 9 Ph. +33(0)4 38 78 45 40, herve.lemonnier@cea.fr herve.lemonnier.sci.free.fr/tpf/tpf.htm

More information

PROPERTIES OF PURE SUBSTANCES. Chapter 3. Mehmet Kanoglu. Thermodynamics: An Engineering Approach, 6 th Edition. Yunus A. Cengel, Michael A.

PROPERTIES OF PURE SUBSTANCES. Chapter 3. Mehmet Kanoglu. Thermodynamics: An Engineering Approach, 6 th Edition. Yunus A. Cengel, Michael A. Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008 Chapter 3 PROPERTIES OF PURE SUBSTANCES Mehmet Kanoglu Copyright The McGraw-Hill Companies, Inc.

More information

Properties of Vapors

Properties of Vapors Properties of Vapors Topics for Discussion The Pressure/Temperature Relationship Vaporization Condensation Enthalpy Properties of Vapors Topics for Discussion Entropy Properties of Substances Saturated

More information

Level 7 Post Graduate Diploma in Engineering Heat and mass transfer

Level 7 Post Graduate Diploma in Engineering Heat and mass transfer 9210-221 Level 7 Post Graduate Diploma in Engineering Heat and mass transfer 0 You should have the following for this examination one answer book non programmable calculator pen, pencil, drawing instruments

More information

On Contact Line Region Heat Transfer, Bubble Dynamics and Substrate Effects during Boiling

On Contact Line Region Heat Transfer, Bubble Dynamics and Substrate Effects during Boiling Rochester Institute of Technology RIT Scholar Works Theses Thesis/Dissertation Collections 4-2018 On Contact Line Region Heat Transfer, Bubble Dynamics and Substrate Effects during Boiling Pruthvik A.

More information

Chapter 3 PROPERTIES OF PURE SUBSTANCES SUMMARY

Chapter 3 PROPERTIES OF PURE SUBSTANCES SUMMARY Chapter 3 PROPERTIES OF PURE SUBSTANCES SUMMARY PURE SUBSTANCE Pure substance: A substance that has a fixed chemical composition throughout. Compressed liquid (sub-cooled liquid): A substance that it is

More information

C g g s. A Theoretical Model to Predict Pool Boiling CHF Incorporating Effects of Contact Angle and Orientation

C g g s. A Theoretical Model to Predict Pool Boiling CHF Incorporating Effects of Contact Angle and Orientation Satish G. Kandlikar Fellow ASME Mechanical Engineering Department, Rochester Institute of Technology, Rochester, NY 14623 e-mail: sgkeme@rit.edu A Theoretical Model to Predict Pool Boiling CHF Incorporating

More information

Chapter 3 PROPERTIES OF PURE SUBSTANCES

Chapter 3 PROPERTIES OF PURE SUBSTANCES Thermodynamics: An Engineering Approach Seventh Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2011 Chapter 3 PROPERTIES OF PURE SUBSTANCES Copyright The McGraw-Hill Companies, Inc. Permission

More information

Chapter 3 PROPERTIES OF PURE SUBSTANCES

Chapter 3 PROPERTIES OF PURE SUBSTANCES Chapter 3 PROPERTIES OF PURE SUBSTANCES PURE SUBSTANCE Pure substance: A substance that has a fixed chemical composition throughout. Air is a mixture of several gases, but it is considered to be a pure

More information

An experimental investigation on condensation of R134a refrigerant in microchannel heat exchanger

An experimental investigation on condensation of R134a refrigerant in microchannel heat exchanger Journal of Physics: Conference Series PAPER OPEN ACCESS An eperimental investigation on condensation of R134a refrigerant in microchannel heat echanger To cite this article: A S Shamirzaev 218 J. Phys.:

More information

Advanced Heat Sink Material for Fusion Energy Devices

Advanced Heat Sink Material for Fusion Energy Devices University of California, San Diego UCSD-ENG-107 Advanced Heat Sink Material for Fusion Energy Devices A. R. Raffray, J. E. Pulsifer and M. S. Tillack August 31, 2002 Fusion Division Center for Energy

More information

Effect of flow velocity on the process of air-steam condensation in a vertical tube condenser

Effect of flow velocity on the process of air-steam condensation in a vertical tube condenser Effect of flow velocity on the process of air-steam condensation in a vertical tube condenser Jan Havlík 1,*, Tomáš Dlouhý 1 1 Czech Technical University in Prague, Faculty of Mechanical Engineering, Department

More information

FORCED CONVECTION FILM CONDENSATION OF DOWNWARD-FLOWING VAPOR ON HORIZONTAL TUBE WITH WALL SUCTION EFFECT

FORCED CONVECTION FILM CONDENSATION OF DOWNWARD-FLOWING VAPOR ON HORIZONTAL TUBE WITH WALL SUCTION EFFECT Journal of Marine Science and Technology, Vol., No. 5, pp. 5-57 () 5 DOI:.69/JMST--5- FORCED CONVECTION FILM CONDENSATION OF DOWNWARD-FLOWING VAPOR ON HORIZONTAL TUBE WITH WALL SUCTION EFFECT Tong-Bou

More information

Heat and Mass Transfer Unit-1 Conduction

Heat and Mass Transfer Unit-1 Conduction 1. State Fourier s Law of conduction. Heat and Mass Transfer Unit-1 Conduction Part-A The rate of heat conduction is proportional to the area measured normal to the direction of heat flow and to the temperature

More information

Chapter 3 PROPERTIES OF PURE SUBSTANCES

Chapter 3 PROPERTIES OF PURE SUBSTANCES Thermodynamics: An Engineering Approach Seventh Edition in SI Units Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2011 Chapter 3 PROPERTIES OF PURE SUBSTANCES Copyright The McGraw-Hill Companies, Inc.

More information

Convective Mass Transfer

Convective Mass Transfer Convective Mass Transfer Definition of convective mass transfer: The transport of material between a boundary surface and a moving fluid or between two immiscible moving fluids separated by a mobile interface

More information

PHYSICAL MECHANISM OF CONVECTION

PHYSICAL MECHANISM OF CONVECTION Tue 8:54:24 AM Slide Nr. 0 of 33 Slides PHYSICAL MECHANISM OF CONVECTION Heat transfer through a fluid is by convection in the presence of bulk fluid motion and by conduction in the absence of it. Chapter

More information

Evaluating properties of pure substances

Evaluating properties of pure substances Evaluating properties of pure substances Pure substance A pure substance has the same chemical composition throughout. Are the following confined in a fixed volume pure substances: Ice (single component,

More information

DEVELOPMENT OF COMPUTATIONAL MULTIFLUID DYNAMICS MODELS FOR NUCLEAR REACTOR APPLICATIONS

DEVELOPMENT OF COMPUTATIONAL MULTIFLUID DYNAMICS MODELS FOR NUCLEAR REACTOR APPLICATIONS DEVELOPMENT OF COMPUTATIONAL MULTIFLUID DYNAMICS MODELS FOR NUCLEAR REACTOR APPLICATIONS Henry Anglart Royal Institute of Technology, Department of Physics Division of Nuclear Reactor Technology Stocholm,

More information

HEAT TRANSFER THERMAL MANAGEMENT OF ELECTRONICS YOUNES SHABANY. C\ CRC Press W / Taylor Si Francis Group Boca Raton London New York

HEAT TRANSFER THERMAL MANAGEMENT OF ELECTRONICS YOUNES SHABANY. C\ CRC Press W / Taylor Si Francis Group Boca Raton London New York HEAT TRANSFER THERMAL MANAGEMENT OF ELECTRONICS YOUNES SHABANY C\ CRC Press W / Taylor Si Francis Group Boca Raton London New York CRC Press is an imprint of the Taylor & Francis Group, an informa business

More information

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

Heat Transfer Predictions for Carbon Dioxide in Boiling Through Fundamental Modelling Implementing a Combination of Nusselt Number Correlations Heat Transfer Predictions for Carbon Dioxide in Boiling Through Fundamental Modelling Implementing a Combination of Nusselt Number Correlations L. Makaum, P.v.Z. Venter and M. van Eldik Abstract Refrigerants

More information

Evaporation of Liquid Chlorides in Closed Tanks using the PHOENICS Code. Presentation of a Rigid Interface Model (RIModel)

Evaporation of Liquid Chlorides in Closed Tanks using the PHOENICS Code. Presentation of a Rigid Interface Model (RIModel) Evaporation of Liquid Chlorides in Closed Tanks using the PHOENICS Code Presentation of a Rigid Interface Model (RIModel) Olivier PRAT 1,3 - Jalil OUAZZANI 2 - Olivier BRIOT 3 1 QUALIFLOW S.A. MONTPELLIER

More information

Forced Convection: Inside Pipe HANNA ILYANI ZULHAIMI

Forced Convection: Inside Pipe HANNA ILYANI ZULHAIMI + Forced Convection: Inside Pipe HANNA ILYANI ZULHAIMI + OUTLINE u Introduction and Dimensionless Numbers u Heat Transfer Coefficient for Laminar Flow inside a Pipe u Heat Transfer Coefficient for Turbulent

More information

Performance Analyses of a Multiple Horizontal Tubes for Steam Condensation

Performance Analyses of a Multiple Horizontal Tubes for Steam Condensation IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 78-1684 Volume 5, Issue 4 (Jan. - Feb. 013), PP 1-18 Performance Analyses of a Multiple Horizontal Tubes for Steam Condensation Dharmendra

More information

A New Numerical Approach for Predicting the Two- Phase Flow of Refrigerants during Evaporation and Condensation

A New Numerical Approach for Predicting the Two- Phase Flow of Refrigerants during Evaporation and Condensation Numerical Heat Transfer, Part B: Fundamentals An International Journal of Computation and Methodology ISSN: 1040-7790 (Print) 1521-0626 (Online) Journal homepage: http://www.tandfonline.com/loi/unhb20

More information

Technological design and off-design behavior of heat exchangers 26

Technological design and off-design behavior of heat exchangers 26 Technological design and off-design behavior of heat exchangers 26 2.2 MODELING OF HEAT TRANSFER The overall heat transfer coefficient U depends on the distribution of thermal resistances in the exchanger.

More information

GAS. Outline. Experiments. Device for in-class thought experiments to prove 1 st law. First law of thermodynamics Closed systems (no mass flow)

GAS. Outline. Experiments. Device for in-class thought experiments to prove 1 st law. First law of thermodynamics Closed systems (no mass flow) Outline First law of thermodynamics Closed systems (no mass flow) Device for in-class thought experiments to prove 1 st law Rubber stops GAS Features: Quasi-equlibrium expansion/compression Constant volume

More information

UNIT II CONVECTION HEAT TRANSFER

UNIT II CONVECTION HEAT TRANSFER UNIT II CONVECTION HEAT TRANSFER Convection is the mode of heat transfer between a surface and a fluid moving over it. The energy transfer in convection is predominately due to the bulk motion of the fluid

More information

Flow Boiling Heat Transfer of Refrigerant R-134a in Copper Microchannel Heat Sink

Flow Boiling Heat Transfer of Refrigerant R-134a in Copper Microchannel Heat Sink UCL, London, UK, 7-10 September 014 Flow Boiling Heat Transfer of Refrigerant R-134a in Copper Microchannel Heat Sink Vladimir V. KUZNETSOV *, Alisher S. SHAMIRZAEV * Corresponding author: Tel.: ++7(383)

More information

A Pool Boiling Map: Water on a Horizontal Surface at Atmospheric Pressure

A Pool Boiling Map: Water on a Horizontal Surface at Atmospheric Pressure University of Central Florida Retrospective Theses and Dissertations Masters Thesis (Open Access) A Pool Boiling Map: Water on a Horizontal Surface at Atmospheric Pressure 1986 O. Burr. Osborn University

More information

Fundamental issues, mechanisms and models of flow boiling heat transfer in microscale channels

Fundamental issues, mechanisms and models of flow boiling heat transfer in microscale channels Fundamental issues, mechanisms and models of flow boiling heat transfer in microscale channels CHENG, Lixin and XIA, Guodong Available from Sheffield Hallam University Research Archive (SHURA) at: http://shura.shu.ac.uk/14546/

More information

Basic Thermodynamics Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur. Lecture No 16

Basic Thermodynamics Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur. Lecture No 16 Basic Thermodynamics Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture No 16 Properties of Pure Substances-I Good afternoon. In the last class, we were

More information

Steven W. Van Sciver. Helium Cryogenics. Second Edition. 4) Springer

Steven W. Van Sciver. Helium Cryogenics. Second Edition. 4) Springer Steven W. Van Sciver Helium Cryogenics Second Edition 4) Springer Contents 1 Cryogenic Principles and Applications 1 1.1 Temperature Scale 2 1.2 Historical Background 4 1.3 Applications for Cryogenics

More information

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

If there is convective heat transfer from outer surface to fluid maintained at T W. Heat Transfer 1. What are the different modes of heat transfer? Explain with examples. 2. State Fourier s Law of heat conduction? Write some of their applications. 3. State the effect of variation of temperature

More information

AN EXPERIMENTAL INVESTIGATION OF POOL BOILING AT ATMOSPHERIC PRESSURE

AN EXPERIMENTAL INVESTIGATION OF POOL BOILING AT ATMOSPHERIC PRESSURE 8 DAFFODIL INTERNATIONAL UNIVERSITY JOURNAL OF SCIENCE AND TECHNOLOGY, VOLUME 6, ISSUE 1, JULY 11 AN EXPERIMENTAL INVESTIGATION OF POOL BOILING AT ATMOSPHERIC PRESSURE Md. Saimon Islam, Khadija Taslima

More information

Module 3: "Thin Film Hydrodynamics" Lecture 12: "" The Lecture Contains: Linear Stability Analysis. Some well known instabilities. Objectives_template

Module 3: Thin Film Hydrodynamics Lecture 12:  The Lecture Contains: Linear Stability Analysis. Some well known instabilities. Objectives_template The Lecture Contains: Linear Stability Analysis Some well known instabilities file:///e /courses/colloid_interface_science/lecture12/12_1.htm[6/16/2012 1:39:16 PM] Linear Stability Analysis This analysis

More information

UCLA UCLA Electronic Theses and Dissertations

UCLA UCLA Electronic Theses and Dissertations UCLA UCLA Electronic Theses and Dissertations Title A Unified Numerical Model for Pool Boiling Curve with Parallel Computing Permalink https://escholarship.org/uc/item/5q61h0pq Author Garg, Deepak Publication

More information

THERMODYNAMICS SSC-JE STAFF SELECTION COMMISSION MECHANICAL ENGINEERING STUDY MATERIAL THERMODYNAMICS THERMODYNAMICS THERMODYNAMICS

THERMODYNAMICS SSC-JE STAFF SELECTION COMMISSION MECHANICAL ENGINEERING STUDY MATERIAL THERMODYNAMICS THERMODYNAMICS THERMODYNAMICS 1 SSC-JE STAFF SELECTION COMMISSION MECHANICAL ENGINEERING STUDY MATERIAL 2 Syllabus: Thermal Engineering (Thermodynamics) Properties of Pure Substances : p-v & P-T diagrams of pure substance like H 2

More information

NUMERICAL PREDICTION OF NUCLEATE POOL BOILING HEAT TRANSFER COEFFICIENT UNDER HIGH HEAT FLUXES. P.O. Box 522, Belgrade, Serbia

NUMERICAL PREDICTION OF NUCLEATE POOL BOILING HEAT TRANSFER COEFFICIENT UNDER HIGH HEAT FLUXES. P.O. Box 522, Belgrade, Serbia NUMERICAL PREDICTION OF NUCLEATE POOL BOILING HEAT TRANSFER COEFFICIENT UNDER HIGH HEAT FLUXES Milada L. PEZO a*, Vladimir D. STEVANOVIĆ b a Department of Thermal Engineering and Energy, Institute of Nuclear

More information

Heat Transfer of Condensation in Smooth Round Tube from Superheated Vapor

Heat Transfer of Condensation in Smooth Round Tube from Superheated Vapor Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2016 Heat Transfer of Condensation in Smooth Round Tube from Superheated Vapor

More information

(Refer Slide Time: 00:00:59 min)

(Refer Slide Time: 00:00:59 min) Refrigeration & Air Conditioning Prof. M. Ramgopal Department Of Mechanical Engineering Indian Institute Of Technology, Kharagpur Lecture No. # 27 Refrigeration Systems Component: Condensers Welcome back

More information

Integration of Boiling Experiments in the Undergraduate Heat Transfer Laboratory

Integration of Boiling Experiments in the Undergraduate Heat Transfer Laboratory Integration of Boiling Experiments in the Undergraduate Heat Transfer Laboratory Hosni I. Abu-Mulaweh, Josué Njock Libii Engineering Department Indiana University-Purdue University at Fort Wayne Fort Wayne,

More information

Mass flow determination in flashing openings

Mass flow determination in flashing openings Int. Jnl. of Multiphysics Volume 3 Number 4 009 40 Mass flow determination in flashing openings Geanette Polanco Universidad Simón Bolívar Arne Holdø Narvik University College George Munday Coventry University

More information

Stratified Flow Condensation of CO 2 in a Tube at Low Temperatures Pei-hua Li 1, a, Joe Deans 2,b and Stuart Norris 3,c

Stratified Flow Condensation of CO 2 in a Tube at Low Temperatures Pei-hua Li 1, a, Joe Deans 2,b and Stuart Norris 3,c Applied Mechanics and Materials Submitted: 2015-05-13 ISSN: 1662-7482, Vols. 789-790, pp 184-192 Accepted: 2015-05-22 doi:10.4028/www.scientific.net/amm.789-790.184 Online: 2015-09-02 2015 Trans Tech Publications,

More information

Latif M. Jiji. Heat Convection. With 206 Figures and 16 Tables

Latif M. Jiji. Heat Convection. With 206 Figures and 16 Tables Heat Convection Latif M. Jiji Heat Convection With 206 Figures and 16 Tables Prof. Latif M. Jiji City University of New York School of Engineering Dept. of Mechanical Engineering Convent Avenue at 138th

More information

Available online at

Available online at Available online at www.sciencedirect.com International Journal of Heat and Mass Transfer 51 (2008) 4327 4341 www.elsevier.com/locate/ijhmt Fluid flow and heat transfer characteristics of low temperature

More information

ME-662 CONVECTIVE HEAT AND MASS TRANSFER

ME-662 CONVECTIVE HEAT AND MASS TRANSFER ME-66 CONVECTIVE HEAT AND MASS TRANSFER A. W. Date Mechanical Engineering Department Indian Institute of Technology, Bombay Mumbai - 400076 India LECTURE- INTRODUCTION () March 7, 00 / 7 LECTURE- INTRODUCTION

More information

High Resolution Measurements of Boiling Heat Transfer

High Resolution Measurements of Boiling Heat Transfer High Resolution Measurements of Boiling Heat Transfer Martin Freystein Institute of Technical Thermodynamics, TU armstadt Personal Skills and Boiling Experience Single Bubble Pool Boiling Bubble Coalescence

More information

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

HEAT TRANSFER. PHI Learning PfcO too1. Principles and Applications BINAY K. DUTTA. Delhi Kolkata. West Bengal Pollution Control Board HEAT TRANSFER Principles and Applications BINAY K. DUTTA West Bengal Pollution Control Board Kolkata PHI Learning PfcO too1 Delhi-110092 2014 Contents Preface Notations ix xiii 1. Introduction 1-8 1.1

More information

Forced Convective Boiling Heat Transfer in Microtubes at Low Mass and Heat Fluxes

Forced Convective Boiling Heat Transfer in Microtubes at Low Mass and Heat Fluxes Symposium on Compact Heat Exchangers, A Festschrift on the th Birthday of Ramesh K. Shah, August, Grenoble, France, pp.1~ 1 Forced Convective Boiling Heat Transfer in Microtubes at Low Mass and Heat Fluxes

More information

THE EFFECT OF LIQUID FILM EVAPORATION ON FLOW BOILING HEAT TRANSFER IN A MICRO TUBE

THE EFFECT OF LIQUID FILM EVAPORATION ON FLOW BOILING HEAT TRANSFER IN A MICRO TUBE Proceedings of the International Heat Transfer Conference IHTC14 August 8-13, 2010, Washington, DC, USA IHTC14-22751 THE EFFECT OF LIQUID FILM EVAPORATION ON FLOW BOILING HEAT TRANSFER IN A MICRO TUBE

More information

PART ONE TWO-PHASE FLOW

PART ONE TWO-PHASE FLOW PART ONE TWO-PHASE FLOW 1 Thermodynamic and Single-Phase Flow Fundamentals 1.1 States of Matter and Phase Diagrams f Pure Substances 1.1.1 Equilibrium States Recall from thermodynamics that f a system

More information

Prediction of Critical Heat Flux (CHF) for Vertical Round Tubes with Uniform Heat Flux in Medium Pressure Regime

Prediction of Critical Heat Flux (CHF) for Vertical Round Tubes with Uniform Heat Flux in Medium Pressure Regime Korean J. Chem. Eng., 21(1), 75-80 (2004) Prediction of Critical Heat Flux (CHF) for Vertical Round Tubes with Uniform Heat Flux in Medium Pressure Regime W. Jaewoo Shim and Joo-Yong Park Department of

More information

Helium two-phase flow in a thermosiphon open loop

Helium two-phase flow in a thermosiphon open loop Presented at the COMSOL Conference 2009 Milan COMSOL Conference 2009 Milan October 14-16 2009 Helium two-phase flow in a thermosiphon open loop Florian Visentin, Bertrand Baudouy CEA Saclay Accelerator,

More information

Modelling of phase change for Two-Phase Refrigerant Flow inside Capillary Tube under Adiabatic Conditions

Modelling of phase change for Two-Phase Refrigerant Flow inside Capillary Tube under Adiabatic Conditions International Journal of Current Engineering and Technology E-ISSN 2277 4106, P-ISSN 2347 5161 2016 INPRESSCO, All Rights Reserved Available at http://inpressco.com/category/ijcet Research Article Modelling

More information

Examination Heat Transfer

Examination Heat Transfer Examination Heat Transfer code: 4B680 date: 17 january 2006 time: 14.00-17.00 hours NOTE: There are 4 questions in total. The first one consists of independent sub-questions. If necessary, guide numbers

More information

Chapter 1 Introduction and Basic Concepts

Chapter 1 Introduction and Basic Concepts Chapter 1 Introduction and Basic Concepts 1-1 Thermodynamics and Energy Application Areas of Thermodynamics 1-2 Importance of Dimensions and Units Some SI and English Units Dimensional Homogeneity Unity

More information

Boiling crisis dynamics: low gravity experiments and modeling

Boiling crisis dynamics: low gravity experiments and modeling Boiling crisis dynamics: low gravity experiments and modeling V. Nikolayev (1), Y. Garrabos (2), C. Lecoutre (2), D. Hitz (3), D. Chatain (3), R. Guillaument (2), V. Janeček (4,5), D. Beysens (3,4) (1)

More information

Mathematical Modelling for Refrigerant Flow in Diabatic Capillary Tube

Mathematical Modelling for Refrigerant Flow in Diabatic Capillary Tube Mathematical Modelling for Refrigerant Flow in Diabatic Capillary Tube Jayant Deshmukh Department of Mechanical Engineering Sagar Institute of Research and Technology, Bhopal, M.P., India D.K. Mudaiya

More information

Flow Boiling Heat Transfer in Microchannels

Flow Boiling Heat Transfer in Microchannels Purdue University Purdue e-pubs CTRC Research Publications Cooling Technologies Research Center 2007 Flow Boiling Heat Transfer in Microchannels D. Liu S V. Garimella Purdue University, sureshg@purdue.edu

More information

Modelling of Multistream LNG Heat Exchangers

Modelling of Multistream LNG Heat Exchangers Modelling of Multistream LNG Heat Exchangers Joan Soler Fossas Natural Gas Technology Submission date: June 2011 Supervisor: Kjell Kolsaker, EPT Norwegian University of Science and Technology Department

More information

Modeling of Wall-boiling Phenomena from Nucleate Subcooled Boiling up to CHF Conditions

Modeling of Wall-boiling Phenomena from Nucleate Subcooled Boiling up to CHF Conditions Modeling of Wall-boiling Phenomena from Nucleate Subcooled Boiling up to CHF Conditions Thomas Frank (1), Amine Ben Hadj Ali (1), Conxita Lifante (1), Florian Kaiser (2), Stephan Gabriel (2), Henning Eickenbusch

More information

Enhanced Boiling Heat Transfer by using micropin-finned surfaces for Electronic Cooling

Enhanced Boiling Heat Transfer by using micropin-finned surfaces for Electronic Cooling Enhanced Boiling Heat Transfer by using micropin-finned surfaces for Electronic Cooling JinJia Wei State Key Laboratory of Multiphase Flow in Power Engineering Xi an Jiaotong University Contents 1. Background

More information

first law of ThermodyNamics

first law of ThermodyNamics first law of ThermodyNamics First law of thermodynamics - Principle of conservation of energy - Energy can be neither created nor destroyed Basic statement When any closed system is taken through a cycle,

More information

Guidelines for simulating cryogenic film boiling using volume of fluid (VOF) method

Guidelines for simulating cryogenic film boiling using volume of fluid (VOF) method Guidelines for simulating cryogenic film boiling using volume of fluid (VOF) method Monir Ahammad 1, Tomasz Olewski 2, Yi Liu 1, Samina Rahmani 1, Sam Mannan 1 and Luc Vechot 2* Mary Kay O Connor Process

More information

Thermodynamics is concerned with the amount of heat transfer as a system undergoes a process from one equilibrium state to another.

Thermodynamics is concerned with the amount of heat transfer as a system undergoes a process from one equilibrium state to another. ecture 1, 2, 3, 4, 5: Heat transfer: Introduction to Heat Transfer Heat transfer is that science which predicts the rate of energy transfer taking place between material bodies as a result of temperature

More information

Appendix A Uncertainty Analysis for Experimental Data

Appendix A Uncertainty Analysis for Experimental Data Appendix A Uncertainty Analysis for Experimental Data To compute the uncertainty in the experimental data of this work, error analyses have been conducted according to the principles proposed by Taylor

More information

Internal Annular Flow-boiling and Flow-condensation: Context, Results and Recommendations

Internal Annular Flow-boiling and Flow-condensation: Context, Results and Recommendations Internal Annular Flow-boiling and Flow-condensation: Context, Results and Recommendations By Amitabh Narain*, Hrishikesh Prasad Ranga Prasad, Aliihsan Koca Michigan Technological University, Houghton,

More information

R13. II B. Tech I Semester Regular Examinations, Jan THERMODYNAMICS (Com. to ME, AE, AME) PART- A

R13. II B. Tech I Semester Regular Examinations, Jan THERMODYNAMICS (Com. to ME, AE, AME) PART- A SET - 1 II B. Tech I Semester Regular Examinations, Jan - 2015 THERMODYNAMICS (Com. to ME, AE, AME) Time: 3 hours Max. Marks: 70 Note 1. Question Paper consists of two parts (Part-A and Part-B) 2. Answer

More information

Contents. I Introduction 1. Preface. xiii

Contents. I Introduction 1. Preface. xiii Contents Preface xiii I Introduction 1 1 Continuous matter 3 1.1 Molecules................................ 4 1.2 The continuum approximation.................... 6 1.3 Newtonian mechanics.........................

More information

Pure substance-1. LIQUIFIED air is also a pure substance for the same reason.

Pure substance-1. LIQUIFIED air is also a pure substance for the same reason. Pure substance-1 A substance that has a fixed chemical composition throughout is called a pure substance. Now there are two important keywords in this: 1. Fixed Chemical Composition 2. Throughout I will

More information

BOILING AND CONDENSATION HEAT TRANSFER COEFFICIENTS FOR A HEAT PIPE HEAT EXCHANGER

BOILING AND CONDENSATION HEAT TRANSFER COEFFICIENTS FOR A HEAT PIPE HEAT EXCHANGER Frontiers in Heat Pipes Available at www.thermalfluidscentral.org BOILING AND CONDENSATION HEAT TRANSFER COEFFICIENTS FOR A HEAT PIPE HEAT EXCHANGER R. Laubscher, R.T. Dobson * Department of Mechanical

More information

A STUDY ON THE CRITICAL HEAT FLUX TEMPERATURE

A STUDY ON THE CRITICAL HEAT FLUX TEMPERATURE A STUDY ON THE CRITICAL HEAT FLUX TEMPERATURE Sabiha Yildiz*, Gerhart Bartsch** *Yildiz Teknik Universitesi, Makine Fakültesi, 80750 Besiktas, Istanbul, Turkey **Institut fuer Energietechnik, TU-Berlin,

More information

Pool Boiling Heat Transfer to Pure Liquids

Pool Boiling Heat Transfer to Pure Liquids Pool Boiling Heat Transfer to Pure Liquids S. A. ALAVI FAZEL, S. ROUMANA Chemical Engineering Department Islamic Azad University, Mahshahr branch Mahshahr, Khuzestan province IRAN alavifazel@gmail.com

More information

Innovative Minichannel Condensers and Evaporators for Air Conditioning Equipment

Innovative Minichannel Condensers and Evaporators for Air Conditioning Equipment Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 14 Innovative Minichannel Condensers and Evaporators for Air Conditioning Equipment

More information

Put sufficient ice cubes into water (1 M) and wait for equilibrium (both exist) (1 M)

Put sufficient ice cubes into water (1 M) and wait for equilibrium (both exist) (1 M) NAME : F.5 ( ) Marks: /70 FORM FOUR PHYSICS REVISION TEST on HEAT Allowed: 70 minutes This paper consists of two sections. Section A (50 marks) consists of the structure-type questions, and Section B (20

More information

5.1. Trufin in Boiling Heat Transfer

5.1. Trufin in Boiling Heat Transfer 5.1. Trufin in Boiling Heat Transfer Boiling is the formation of vapor bubbles at the heating surface. These bubbles form at nucleation sites whose number and location depend upon the surface roughness

More information

WITPRESS WIT Press publishes leading books in Science and Technology. Visit our website for the current list of titles.

WITPRESS WIT Press publishes leading books in Science and Technology. Visit our website for the current list of titles. Introduction to Heat Transfer WITPRESS WIT Press publishes leading books in Science and Technology. Visit our website for the current list of titles. www.witpress.com WITeLibrary Home of the Transactions

More information

Capillary Blocking in Forced Convective Condensation in Horizontal Miniature Channels

Capillary Blocking in Forced Convective Condensation in Horizontal Miniature Channels Yuwen Zhang Mem. ASME A. Faghri Fellow ASME M. B. Shafii Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269 Capillary Blocking in Forced Convective Condensation in Horizontal

More information