WP1.3 Transient fluid dynamics of CO 2 mixtures in pipelines

Size: px
Start display at page:

Download "WP1.3 Transient fluid dynamics of CO 2 mixtures in pipelines"

Transcription

1 WP1.3 Transient fluid dynamics of CO 2 mixtures in pipelines Sintef Energy Research (Norway), TNO (Netherland), CSM (Italia) Workshop EC FP7 Projects: Leading the way in CCS implementation London, April 2014 Alexandre Morin, 1

2 The work package Transient fluid dynamics of CO 2 mixtures in pipelines Assess the influence of impurities in CO 2 in pipeline transport Benchmarking of existing tools available to the consortium Contribute to SP2 by giving results Techno-economic analysis Risk assessment

3 Many natural gas pipelines why start over with CO 2? Stronger cooling with CO 2 Higher pressure during depressurisation Natural gas phase diagram CO 2 phase diagram From wikimedia commons

4 Challenges related to CO 2 transport Behaviour during transients Depressurisation of a pipe Pressure evolution Predict the lowest temperature Crack propagation Not in IMPACTS SINTEF Materials and chemistry 4

5 Challenges in numerical modelling Mixture with "overwhelmingly" CO 2 Close to single component Thin phase envelope in pressure/temperature From wikimedia commons Liquid-gas Single phase 5

6 Challenges in numerical modelling OLGA generally solves the equations in Pressure/Temperature Instabilities with mixtures containing one overwhelming component Solved for pure CO 2 with the single-component module New OLGA model solves the equations in Pressure/Enthalpy Not available yet Expected to work better on CO 2 mixtures with impurities We solve the equations in Density/Energy Natural variables for the fluid-dynamical equations Thermodynamic routines non-standard From wikimedia commons 6

7 Fluid-dynamical model Single-phase compressible flow equations (Euler equations) Mass conservation Momentum conservation + + = 0 ρρ v + p = 0 Total energy conservation ρ e + v2 2 + ρ e + v2 2 v + pp = 0 Multiphase flow model Two sets of the three conservation equations Advection of volume fraction α k Seven equations In the phases gas α g p g, T g, μ g, v g p g, T g, μ g, v g p l, T l, μ l, v l liquid p l, T l, μ l, v l 7

8 Fluid-dynamical model Play on relaxation and instantaneous equilibrium Two-fluid: Two independent phases Drift-flux: Mixture seen as one complex phase TF 4 /DF 3 necessary to use an equilibrium equation of state Are the underlying assumptions reasonable? 8

9 Fluid-dynamic model Slow transients Time scales of flow larger than equilibrium time scale 0 C Faster transients Time scales of equilibrium relevant to the problem dynamics Equilibrium kinetics impacts the speed of sound Not satisfying to force equilibrium? Define how to be outside of equilibrium Not a thermodynamic problem: caused by the averaging T > 0 C Water with ice cube 0 C T > 0 C Averaged 9

10 Implementation of thermodynamic routines Ruhr University Bochum (Prof. Roland Span) Accurate equation of state for combustion gases Thermodynamic interface between fluid-dynamics and thermodynamics Flash routines Density/Energy 10

11 Status of work SINTEF general-purpose thermodynamics library interfaced with RUB's library Use EOSCG with our general equilibrium calculation routines Development of energy/density flash algorithms Strong focus on robustness Efficiency increased by parallelisation The following impurities have been successfully tested so far (as binary mixture with CO 2 ): N 2 CO Ar O 2 11

12 Benchmark study Benchmark study Focus on transient/accidental situation Report describing the benchmark cases Different pipe geometries Compositions based on results of IMPACTS workshop The cases will highlight the strengths of the different codes Pipe geometries CO 2 N 2 O 2 Ar NO x SO x CO H 2 S H 2 CH 4 C 2 + NH 3 Amine Pure CO 2 100% Coal-fired power plant Amine-based absorption Coal-fired power plant Selexol-based absorption Natural gas processing Amine-based absorption 99% 2000ppm 200ppm 100ppm 50ppm 10ppm 10ppm 1ppm 1ppm 98% 6000ppm 1ppm 500ppm 400ppm 100ppm 1% 1000ppm 95% 5000ppm 200ppm 4% 5000ppm

13 Benchmark study Vapour film Type of code OLGA and SINTEF in-house code: 1D Fluent (CSM): 3D Results very dependent on submodels Heat transfer Friction Equilibrium Heat transfer Critical flux Film boiling Onset of nucleate boiling Wall temperature Gas Depressurisation P aaa v ooo < c sssss Liquid P iiii

14 Link to experimental data CO 2 transport rig, CIUDEN, Spain Possibility to depressurise it to atmosphere Impurities in CO 2 CO 2 transport rig, CIUDEN, Spain 14

15 Why is it important for IMPACTS Steel qualities have design minimum temperatures Lowest temperature to be expected Qualify or disqualify a steel quality Pipeline design must take the transient events into account Minimum acceptable pipe thickness Impacts the amount of steel Effect on the cost of pipeline Input model for atmospheric dispersion models

16 Thank you for your attention Nils A Røkke, Chairman of the Executive Board, Nils.A.Rokke@sintef.no Mona J. Mølnvik, Coordinator, Mona.J.Molnvik@sintef.no Astrid Lilliestråle, Project manager, Astrid.Lilliestrale@sintef.no An Hilmo, Project secretary, An.Hilmo@sintef.no Website: Acknowledgement: The research leading to these results has received funding from the European Community's Seventh Framework Programme (FP7-ENERGY STAGE) under grant agreement n (The IMPACTS project). The authors acknowledge the project partners and the following funding partners for their contributions: Statoil Petroleum AS, Lundin Norway AS, Gas Natural Fenosa, MAN Diesel & Turbo SE and Vattenfall AB. 16

TCCS Published by Elsevier Ltd. Selection and/or peer-review under responsibility of [name organizer]

TCCS Published by Elsevier Ltd. Selection and/or peer-review under responsibility of [name organizer] Energy Procedia 00 (2011) 000 000 Energy Procedia www.elsevier.com/locate/procedia TCCS-6 Depressurization of CO 2 a numerical benchmark study Sigmund Clausen a,c* and Svend Tollak Munkejord b a Gassco

More information

Available online at Energy Procedia 00 (2010) GHGT-10

Available online at   Energy Procedia 00 (2010) GHGT-10 Available online at www.sciencedirect.com Energy Procedia 00 (2010) 000 000 Energy Procedia www.elsevier.com/locate/xxx GHGT-10 Depressurization of carbon dioxide in pipelines models and methods Halvor

More information

CHEMICAL ENGINEERING II (MASTERY) Professor K. Li Dr. S. Kalliadasis Professor R. Kandiyoti

CHEMICAL ENGINEERING II (MASTERY) Professor K. Li Dr. S. Kalliadasis Professor R. Kandiyoti 2 ND YEAR COURSE OBJECTIVES CHEMICAL ENGINEERING II (MASTERY) Professor K. Li Dr. S. Kalliadasis Professor R. Kandiyoti ChE.201 The aim of mastery in the 2 nd year is to further develop students ability

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

EFFECT OF LIQUID PHASE COMPRESSIBILITY ON MODELING OF GAS-LIQUID TWO-PHASE FLOWS USING TWO-FLUID MODEL

EFFECT OF LIQUID PHASE COMPRESSIBILITY ON MODELING OF GAS-LIQUID TWO-PHASE FLOWS USING TWO-FLUID MODEL EFFECT OF LIQUID PHASE COMPRESSIBILITY ON MODELING OF GAS-LIQUID TWO-PHASE FLOWS USING TWO-FLUID MODEL Vahid SHOKRI 1*,Kazem ESMAEILI 2 1,2 Department of Mechanical Engineering, Sari Branch, Islamic Azad

More information

Evaluation of the SPUNG Equation of State for use in Carbon Capture and Storage Modelling

Evaluation of the SPUNG Equation of State for use in Carbon Capture and Storage Modelling 6 th Trondheim CCS-conference June 14-16 2011 Evaluation of the SPUNG Equation of State for use in Carbon Capture and Storage Modelling Geir Skaugen a Øivind Wilhelmsen a, Oddvar Jørstad b, Hailong Li

More information

CHEMISTRY WORKSHEET. 1. Anything that occupies space and has weight. 2. The state of matter having maximum compressibility.

CHEMISTRY WORKSHEET. 1. Anything that occupies space and has weight. 2. The state of matter having maximum compressibility. CH.1 Q.1:- Name the Following:- 1. Anything that occupies space and has weight. 2. The state of matter having maximum compressibility. 3. The state which has maximum intermolecular space. 4. The process

More information

Rigorous calculation of LNG flow reliefs using the GERG-2004 equation of state

Rigorous calculation of LNG flow reliefs using the GERG-2004 equation of state Rigorous calculation of LNG reliefs using the GERG-2004 equation of state Luigi Raimondi Process Simulation Services www.xpsimworld.com Via Galvani 105, 20025 Legnano (MI) - Italy The design of process

More information

Preliminary Evaluation of the SPUNG Equation of State for Modelling the Thermodynamic Properties of CO 2 Water Mixtures

Preliminary Evaluation of the SPUNG Equation of State for Modelling the Thermodynamic Properties of CO 2 Water Mixtures Available online at www.sciencedirect.com Energy Procedia 26 (2012 ) 90 97 2 nd Trondheim Gas Technology Conference Preliminary Evaluation of the SPUNG Equation of State for Modelling the Thermodynamic

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

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

Multiphase Flows. Mohammed Azhar Phil Stopford

Multiphase Flows. Mohammed Azhar Phil Stopford Multiphase Flows Mohammed Azhar Phil Stopford 1 Outline VOF Model VOF Coupled Solver Free surface flow applications Eulerian Model DQMOM Boiling Model enhancements Multi-fluid flow applications Coupled

More information

Urea Injection and Preparation in Diesel Applications Multiphase Multicomponent Modeling using Star-CD

Urea Injection and Preparation in Diesel Applications Multiphase Multicomponent Modeling using Star-CD , London Urea Injection and Preparation in Diesel Applications Multiphase Multicomponent Modeling using Star-CD Institute for Powertrains & Automotive Technology Dipl.-Phys. Simon Fischer Dr. Thomas Lauer

More information

Mechanical Engineering. Postal Correspondence Course HEAT TRANSFER. GATE, IES & PSUs

Mechanical Engineering. Postal Correspondence Course HEAT TRANSFER. GATE, IES & PSUs Heat Transfer-ME GATE, IES, PSU 1 SAMPLE STUDY MATERIAL Mechanical Engineering ME Postal Correspondence Course HEAT TRANSFER GATE, IES & PSUs Heat Transfer-ME GATE, IES, PSU 2 C O N T E N T 1. INTRODUCTION

More information

A LARGE TIME STEP ROE SCHEME APPLIED TO TWO-PHASE FLOW

A LARGE TIME STEP ROE SCHEME APPLIED TO TWO-PHASE FLOW ECCOMAS Congress 2016 VII European Congress on Computational Methods in Applied Sciences and Engineering M. Papadrakakis, V. Papadopoulos, G. Stefanou, V. Plevris (eds.) Crete Island, Greece, 5 10 June

More information

Coupling of ChemApp and OpenFOAM

Coupling of ChemApp and OpenFOAM Coupling of ChemApp and OpenFOAM Messig, Danny; Rehm, Markus; Meyer, Bernd 19th May 2009 Contents 1 Introduction 2 Software OpenFOAM ChemApp Cantera 3 Coupling of chemistry packages and OpenFOAM 4 Testcases

More information

Boiling and Condensation (ME742)

Boiling and Condensation (ME742) Indian Institute of Technology Kanpur Department of Mechanical Engineering Boiling and Condensation (ME742) PG/Open Elective Credits: 3-0-0-9 Updated Syllabus: Introduction: Applications of boiling and

More information

Hydraulic Modelling for Drilling Automation

Hydraulic Modelling for Drilling Automation Hydraulic Modelling for Drilling Automation CASA Day Harshit Bansal April 19, 2017 Where innovation starts Team: Supervisors at TU/e : W.H.A. Schilders, N. van de Wouw, B. Koren, L. Iapichino Collaborators:

More information

This Week. 6/2/2015 Physics 214 Summer

This Week. 6/2/2015 Physics 214 Summer This Week Heat and Temperature Water and Ice Our world would be different if water didn t expand Engines We can t use all the energy! Why is a diesel engine more efficient? Geysers: You have to be faithful

More information

Experimental study of CO 2 releases from a saturated liquid reservoir

Experimental study of CO 2 releases from a saturated liquid reservoir Available online at www.sciencedirect.com Energy Procedia 37 (213 ) 4818 4824 GHGT-11 Experimental study of CO 2 releases from a saturated liquid reservoir S. Toesse 1*, K. Vaagsaether 1, J. Lundberg 1,

More information

Dynamic simulation and Control of a CO 2 Compression and Purification Unit for Oxy-Coal-Fired Power Plants

Dynamic simulation and Control of a CO 2 Compression and Purification Unit for Oxy-Coal-Fired Power Plants Dynamic simulation and Control of a CO 2 Compression and Purification Unit for Oxy-Coal-Fired Power Plants Authors A. Chansomwong, K.E. Zanganeh, A. Shafeen, P.L. Douglas,E. Croiset, L.A. Ricardez-Sandoval,

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

Introduction & Basic Concepts of Thermodynamics

Introduction & Basic Concepts of Thermodynamics Introduction & Basic Concepts of Thermodynamics Reading Problems 2-1 2-8 2-53, 2-67, 2-85, 2-96 Introduction to Thermal Sciences Thermodynamics Conservation of mass Conservation of energy Second law of

More information

1. Increasing the pressure above a liquid will cause the boiling point of the liquid to:

1. Increasing the pressure above a liquid will cause the boiling point of the liquid to: JASPERSE CHEM 210 PRACTICE TEST 1 VERSION 2 Ch. 11 Liquids, Solids, and Materials Ch. 10 Gases Ch. 15 The Chemistry of Solutes and Solutions Ch. 13 Chemical Kinetics 1 Constants and/or Formulas Formulas

More information

Adam G. Hawley Darin L. George. Southwest Research Institute 6220 Culebra Road San Antonio, TX 78238

Adam G. Hawley Darin L. George. Southwest Research Institute 6220 Culebra Road San Antonio, TX 78238 USE OF EQUATIONS OF STATE AND EQUATION OF STATE SOFTWARE PACKAGES Adam G. Hawley Darin L. George Southwest Research Institute 6220 Culebra Road San Antonio, TX 78238 Introduction Determination of fluid

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

A WIMF Scheme for the Drift-Flux Two-Phase Flow Model

A WIMF Scheme for the Drift-Flux Two-Phase Flow Model A WIMF Scheme for the Drift-Flux Two-Phase Flow Model Steinar Eve A,B,D, Tore Flåtten B,A and Svend Tollak Munkeord C A Centre of Mathematics for Applications (CMA), 153 Blindern, NO-316 Oslo, Norway B

More information

ScienceDirect. Modelling CO 2 Water Thermodynamics Using SPUNG Equation of State (EoS) concept with Various Reference Fluids

ScienceDirect. Modelling CO 2 Water Thermodynamics Using SPUNG Equation of State (EoS) concept with Various Reference Fluids Available online at www.sciencedirect.com ScienceDirect Energy Procedia 51 (2014 ) 353 362 7th Trondheim CCS Conference, TCCS-7, June 5-6 2013, Trondheim, Norway Modelling CO 2 Water Thermodynamics Using

More information

1. Which of the following would have the highest molar heat of vaporization? c. Cl 2

1. Which of the following would have the highest molar heat of vaporization? c. Cl 2 JASPERSE CHEM 160 PRACTICE TEST 1 VERSION 1 Corrected Ch. 11 Liquids, Solids, and Materials Ch. 15 The Chemistry of Solutes and Solutions Ch. 13 Chemical Kinetics Formulas for First Order Reactions: kt

More information

CST Investigation on High Speed Liquid Jet using Computational Fluid Dynamics Technique

CST Investigation on High Speed Liquid Jet using Computational Fluid Dynamics Technique The 23 rd Conference of the Mechanical Engineering Network of Thailand November 4 7, 2009, Chiang Mai Investigation on High Speed Liquid Jet using Computational Fluid Dynamics Technique Wirapan Seehanam*,

More information

CFD Simulation of Flashing and Boiling Flows Using FLUENT

CFD Simulation of Flashing and Boiling Flows Using FLUENT CFD Simulation of Flashing and Boiling Flows Using FLUENT Hua Bai and Paul Gillis The Dow Chemical Company FLUENT UGM 2004 Liquid/Gas Phase Change found in many industrial chemical processes involves complex

More information

CHEMICAL ENGINEERING

CHEMICAL ENGINEERING CHEMICAL ENGINEERING Subject Code: CH Course Structure Sections/Units Section A Unit 1 Unit 2 Unit 3 Unit 4 Unit 5 Unit 6 Section B Section C Section D Section E Section F Section G Section H Section I

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

Numerical investigation of cavitation-regimes in a converging-diverging nozzle

Numerical investigation of cavitation-regimes in a converging-diverging nozzle Numerical investigation of cavitation-regimes in a converging-diverging nozzle 1 Polina Gorkh, 1 Steffen J. Schmidt, and 1 Nikolaus A. Adams 1 Institute of Aerodynamics and Fluid Mechanics, Department

More information

3D Simulation of the Plunger Cooling during the Hollow Glass Forming Process Model, Validation and Results

3D Simulation of the Plunger Cooling during the Hollow Glass Forming Process Model, Validation and Results Thomas Bewer, Cham, CH 3D Simulation of the Plunger Cooling during the Hollow Glass Forming Process Model, Validation and Results A steady state model to describe the flow and temperature distribution

More information

A SHORT INTRODUCTION TO TWO-PHASE FLOWS 1D-time averaged models

A SHORT INTRODUCTION TO TWO-PHASE FLOWS 1D-time averaged models A SHORT INTRODUCTION TO TWO-PHASE FLOWS 1D-time averaged models Hervé Lemonnier DM2S/STMF/LIEFT, CEA/Grenoble, 38054 Grenoble Cedex 9 Ph. +3304 38 78 45 40 herve.lemonnier@cea.fr, herve.lemonnier.sci.free.fr/tpf/tpf.htm

More information

Severe slugging: modeling, simulation and stability criteria

Severe slugging: modeling, simulation and stability criteria Severe slugging: modeling, simulation and stability criteria Jorge Luis Baliño jlbalino@usp.br Departamento de Engenharia Mecânica Escola Politécnica Outline Introduction Air-water model Simulation results

More information

mechanical integrity of PFHE in LNG liquefaction process

mechanical integrity of PFHE in LNG liquefaction process mechanical integrity of PFHE in LNG liquefaction process Norbert Ligterink, Svetlana Hageraats, Han Velthuis Fluid Dynamics Group, TNO, Delft, The Netherlands temperature, boiling flow, thermal stresses

More information

CHEMISTRY. Chapter 11 Intermolecular Forces Liquids and Solids

CHEMISTRY. Chapter 11 Intermolecular Forces Liquids and Solids CHEMISTRY The Central Science 8 th Edition Chapter 11 Liquids and Solids Kozet YAPSAKLI States of Matter difference between states of matter is the distance between particles. In the solid and liquid states

More information

INDEX. (The index refers to the continuous pagination)

INDEX. (The index refers to the continuous pagination) (The index refers to the continuous pagination) Accuracy in physical models methods for assessing overall assessment acquisition of information acrylonitrile hazards polymerisation toxic effects toxic

More information

Laws of Thermodynamics

Laws of Thermodynamics Laws of Thermodynamics The Three Laws of Thermodynamics - The first lawof thermodynamics, also called conservation of energy. We can use this knowledge to determine the amount of energy in a system, the

More information

T H E R M O D Y N A M I C S M T

T H E R M O D Y N A M I C S M T T H E R M O D Y N A M I C S M T THERMODYNAMICS AND RATE PROCESSES CONTENTS CHAPTER DESCRIPTION PAGE NO 1 Thermodynamics NOTES 1.1. Definitions 1 1.2. Laws of Thermodynamics 3 1.2.1. Zeroth Law of Thermodynamics

More information

Gases and IMFs Unit Exam Review Guide

Gases and IMFs Unit Exam Review Guide Gases and IMFs Unit Exam Review Guide The following review guide does not necessarily contain all topics that will appear on the test. Make sure to review all notes and concepts from this unit. This review

More information

Accurate thermodynamic-property models for CO 2 -rich mixtures

Accurate thermodynamic-property models for CO 2 -rich mixtures Available online at www.sciencedirect.com Energy Procedia 37 (2013 ) 2914 2922 GHGT-11 Accurate thermodynamic-property models for CO 2 -rich mixtures Roland Span*, Johannes Gernert, Andreas Jäger Thermodynamics,

More information

On the Modeling and Simulation of a Laser-Induced Caviation Bubble

On the Modeling and Simulation of a Laser-Induced Caviation Bubble 1 On the Modeling and Simulation of a Laser-Induced Caviation Bubble Ali Zein Supervisor: Prof. Dr. Gerald Warnecke Co-supervisor: Dr. Maren Hantke Institut für Analysis und Numerik Otto-von-Guericke-Universität

More information

Controlled FTIR measurements of acid gas (NO, mixed NO/SO 2 ) capture in water at high pressure

Controlled FTIR measurements of acid gas (NO, mixed NO/SO 2 ) capture in water at high pressure ANLECR&D project 6 0215 0234 Controlled FTIR measurements of acid gas (NO, mixed NO/SO 2 ) capture in water at high pressure Sub contract to Macquarie University Report of ANLECR&D Project 6 0215 0243

More information

Chapter 11. Intermolecular forces. Chapter 11 1

Chapter 11. Intermolecular forces. Chapter 11 1 Chapter 11 Intermolecular Attractions and the Properties of Liquids and Solids 1 2 Intermolecular forces Forces of attraction between molecules Directly dependent on the distance between the molecules

More information

Chapter Intermolecular attractions

Chapter Intermolecular attractions Chapter 11 11.2 Intermolecular attractions Intermolecular Attractions and the Properties of Liquids and Solids Intermolecular forces control the physical properties of the substance. Intramolecular forces

More information

Development of a consistent and conservative Eulerian - Eulerian algorithm for multiphase flows

Development of a consistent and conservative Eulerian - Eulerian algorithm for multiphase flows Development of a consistent and conservative Eulerian - Eulerian algorithm for multiphase flows Ana Cubero Alberto Sanchez-Insa Norberto Fueyo Numerical Fluid Dynamics Group University of Zaragoza Spain

More information

Phase equilibrium studies of impure CO 2 systems to underpin developments of CCS technologies

Phase equilibrium studies of impure CO 2 systems to underpin developments of CCS technologies Phase equilibrium studies of impure CO 2 systems to underpin developments of CCS technologies Jie Ke, Martyn Poliakoff and Michael W. George School of Chemistry The University of Nottingham 1 September,

More information

Name Date Class. Electromagnetic Spectrum. Colors

Name Date Class. Electromagnetic Spectrum. Colors b e n c h m a r k t e s t : p h y s i c a l s c i e n c e Multiple Choice Directions: Use the diagram below to answer question 1. Electromagnetic Spectrum Radio waves A B C D Gamma rays Long Wavelength

More information

3. FORMS OF GOVERNING EQUATIONS IN CFD

3. FORMS OF GOVERNING EQUATIONS IN CFD 3. FORMS OF GOVERNING EQUATIONS IN CFD 3.1. Governing and model equations in CFD Fluid flows are governed by the Navier-Stokes equations (N-S), which simpler, inviscid, form is the Euler equations. For

More information

ScienceDirect. Impact of heat stable salts on equilibrium CO 2 absorption

ScienceDirect. Impact of heat stable salts on equilibrium CO 2 absorption Available online at www.sciencedirect.com ScienceDirect Energy Procedia 63 (2014 ) 1781 1794 GHGT-12 Impact of heat stable salts on equilibrium CO 2 absorption Ugochukwu Edwin Aronu*, Kristin Giske Lauritsen,

More information

Chemistry A: States of Matter Packet Name: Hour: Page 1. Chemistry A States of Matter Packet

Chemistry A: States of Matter Packet Name: Hour: Page 1. Chemistry A States of Matter Packet Chemistry A: States of Matter Packet Name: Hour: Page 1 Chemistry A States of Matter Packet Chemistry A: States of Matter Packet Name: Hour: Page 2 Worksheet #1: States of Matter In this packet we will

More information

Development of a one-dimensional boiling model: Part I A two-phase flow pattern map for a heavy hydrocarbon feedstock

Development of a one-dimensional boiling model: Part I A two-phase flow pattern map for a heavy hydrocarbon feedstock Development of a one-dimensional boiling model: Part I A two-phase flow pattern map for a heavy hydrocarbon feedstock Pieter Verhees, Abdul Akhras Rahman, Kevin M. Van Geem, Geraldine J. Heynderickx Laboratory

More information

Computational fluid dynamics study of flow depth in an open Venturi channel for Newtonian fluid

Computational fluid dynamics study of flow depth in an open Venturi channel for Newtonian fluid Computational fluid dynamics study of flow depth in an open Venturi channel for Newtonian fluid Prasanna Welahettige 1, Bernt Lie 1, Knut Vaagsaether 1 1 Department of Process, Energy and Environmental

More information

Properties of Liquids and Solids

Properties of Liquids and Solids Properties of Liquids and Solids World of Chemistry Chapter 14 14.1 Intermolecular Forces Most substances made of small molecules are gases at normal temperature and pressure. ex: oxygen gas, O 2 ; nitrogen

More information

Dynamic Modeling of the Solvent Regeneration Part of a CO 2 Capture Plant

Dynamic Modeling of the Solvent Regeneration Part of a CO 2 Capture Plant Available online at www.sciencedirect.com Energy Procedia 37 (2013 ) 2058 2065 GHGT-11 Dynamic Modeling of the Solvent Regeneration Part of a CO 2 Capture Plant Nina Enaasen a *, Andrew Tobiesen b, Hanne

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

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

Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines

Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines Zeroeth Law Two systems individually in thermal equilibrium with a third

More information

2. THE STATES OF MATTER

2. THE STATES OF MATTER 2. THE STATES OF MATTER 2.1. THE THREE STATES OF MATTER Every substance can take on several distinct forms called phases or states of aggregation of matter. Four states of matter are observable in everyday

More information

Mass Transfer in a Small Scale Flue Gas Absorber Experimental and Modeling

Mass Transfer in a Small Scale Flue Gas Absorber Experimental and Modeling Mass Transfer in a Small Scale Flue Gas Absorber Experimental and Modeling P.J.G. Huttenhuis, E.P. van Elk, S. Van Loo, G.F. Versteeg Procede Gas Treating B.V., The Netherlands 11 th MEETING of the INTERNATIONAL

More information

Modeling of two-phase flow > Direct steam generation in solar thermal power plants

Modeling of two-phase flow > Direct steam generation in solar thermal power plants Modeling of two-phase flow > Direct steam generation in solar thermal power plants Pascal Richter RWTH Aachen University EGRIN Pirirac-sur-Mer June 3, 2015 Novatec Solar GmbH Direct steam generation Solar

More information

PAPER 2 THEORY QUESTIONS

PAPER 2 THEORY QUESTIONS PAPER 2 THEORY QUESTIONS 1 Fig. 1.1 shows the arrangement of atoms in a solid block. Fig. 1.1 (a) End X of the block is heated. Energy is conducted to end Y, which becomes warm. (i) Explain how heat is

More information

MODEL BASED PIPELINE MONITORING WITH LEAK DETECTION

MODEL BASED PIPELINE MONITORING WITH LEAK DETECTION MODEL BASED PIPELINE MONITORING WITH LEAK DETECTION Espen Hauge Ole Morten Aamo, John-Morten Godhavn Department of Engineering Cybernetics, Norwegian University of Science and Technology, Trondheim, Norway

More information

MASS TRANSFER AND GAS ABSORPTION EQUIPMENT

MASS TRANSFER AND GAS ABSORPTION EQUIPMENT MASS TRANSFER AND GAS ABSORPTION EQUIPMENT Mark J McCready University of Notre Dame Indiana, USA TOPICS Review of heat transfer and heat exchangers Some fundamental aspects of mass transfer Analysis of

More information

glycerine/water solutions from biodiesel production.

glycerine/water solutions from biodiesel production. Study of the ion exchange equilibrium of sodium and chloride ions in glycerine/water solutions from biodiesel production. A. de Lucas, G. García, Jolanta Warchol, J.F. Rodríguez y M. Carmona. Chemical

More information

Energy Procedia. Two-Phase Flow of CO 2 with Phase Transfer. Halvor Lund a,, Peder Aursand b. 6th Trondheim CCS Conference. Abstract. 1.

Energy Procedia. Two-Phase Flow of CO 2 with Phase Transfer. Halvor Lund a,, Peder Aursand b. 6th Trondheim CCS Conference. Abstract. 1. Energy Procedia 00 (2011) 1 10 Energy Procedia www.elsevier.com/locate/procedia 6th Trondheim CCS Conference Two-Phase Flow of CO 2 with Phase Transfer Halvor Lund a,, Peder Aursand b a Dept. of Energy

More information

General Physics I (aka PHYS 2013)

General Physics I (aka PHYS 2013) General Physics I (aka PHYS 2013) PROF. VANCHURIN (AKA VITALY) University of Minnesota, Duluth (aka UMD) OUTLINE CHAPTER 12 CHAPTER 19 REVIEW CHAPTER 12: FLUID MECHANICS Section 12.1: Density Section 12.2:

More information

TAU Extensions for High Enthalpy Flows. Sebastian Karl AS-RF

TAU Extensions for High Enthalpy Flows. Sebastian Karl AS-RF TAU Extensions for High Enthalpy Flows Sebastian Karl AS-RF Contents Motivation Extensions available in the current release: Numerical schemes for super- and hypersonic flow fields Models for gas mixtures,

More information

Unit Five: Intermolecular Forces MC Question Practice April 14, 2017

Unit Five: Intermolecular Forces MC Question Practice April 14, 2017 Unit Five: Intermolecular Forces Name MC Question Practice April 14, 2017 1. Which of the following should have the highest surface tension at a given temperature? 2. The triple point of compound X occurs

More information

HiLumi LHC FP7 High Luminosity Large Hadron Collider Design Study. Milestone Report. Cryogenic Scenarios for the Cold Powering System

HiLumi LHC FP7 High Luminosity Large Hadron Collider Design Study. Milestone Report. Cryogenic Scenarios for the Cold Powering System CERN-ACC-2014-0065 HiLumi LHC FP7 High Luminosity Large Hadron Collider Design Study Milestone Report Cryogenic Scenarios for the Cold Powering System Ballarino, A (CERN) et al 27 May 2014 The HiLumi LHC

More information

COMBUSTION OF FUEL 12:57:42

COMBUSTION OF FUEL 12:57:42 COMBUSTION OF FUEL The burning of fuel in presence of air is known as combustion. It is a chemical reaction taking place between fuel and oxygen at temperature above ignition temperature. Heat is released

More information

Thermodynamics 1. Lecture 7: Heat transfer Open systems. Bendiks Jan Boersma Thijs Vlugt Theo Woudstra. March 1, 2010.

Thermodynamics 1. Lecture 7: Heat transfer Open systems. Bendiks Jan Boersma Thijs Vlugt Theo Woudstra. March 1, 2010. hermodynamics Lecture 7: Heat transfer Open systems Bendiks Jan Boersma hijs Vlugt heo Woudstra March, 00 Energy echnology Summary lecture 6 Poisson relation efficiency of a two-stroke IC engine (Otto

More information

Agenda 1) Homework Questions 2) Review Concepts of Thermal Energy 3) States of Matter / Latent Heat 4) Practice

Agenda 1) Homework Questions 2) Review Concepts of Thermal Energy 3) States of Matter / Latent Heat 4) Practice Agenda 1) Homework Questions 2) Review Concepts of Thermal Energy 3) States of Matter / Latent Heat 4) Practice Important Terms and their Usage Drag each term below into the sentence in which it is properly

More information

Nucleation Quality and Bubble Momentum and Their Effect on Droplet Velocity and Stability

Nucleation Quality and Bubble Momentum and Their Effect on Droplet Velocity and Stability Nucleation Quality and Bubble Momentum and Their Effect on Droplet Velocity and Stability Robert Cornell Lexmark International Inc. Lexington, Kentucky Abstract A recent paper, presented at NIP12 in San

More information

Chemistry B11 Chapter 6 Gases, Liquids, and Solids

Chemistry B11 Chapter 6 Gases, Liquids, and Solids Chapter 6 Gases, Liquids, and Solids States of matter: the physical state of matter depends on a balance between the kinetic energy of particles, which tends to keep them apart, and the attractive forces

More information

The kinetic Molecular Theory of Liquids and solids

The kinetic Molecular Theory of Liquids and solids The kinetic Molecular Theory of Liquids and solids States of Matter The fundamental difference between states of matter is the distance between particles. 2012 Pearson Education, Inc. Intermolecular Forces

More information

2012 AP CHEMISTRY FREE-RESPONSE QUESTIONS

2012 AP CHEMISTRY FREE-RESPONSE QUESTIONS 01 AP CHEMISTRY FREE-RESPONSE QUESTIONS. A sample of a pure, gaseous hydrocarbon is introduced into a previously evacuated rigid 1.00 L vessel. The pressure of the gas is 0.00 atm at a temperature of 17C.

More information

Experimental Investigation of Drag Reduction with polymer of Kerosene flow in a horizontal pipe

Experimental Investigation of Drag Reduction with polymer of Kerosene flow in a horizontal pipe International Journal of Thermal Technologies E-ISSN 2277 4114 2018 INPRESSCO, All Rights Reserved Available at http://inpressco.com/category/ijtt/ Research Article Experimental Investigation of Drag Reduction

More information

Chapter 11. Liquids and Intermolecular Forces

Chapter 11. Liquids and Intermolecular Forces Chapter 11 Liquids and Intermolecular Forces States of Matter The three states of matter are 1) Solid Definite shape Definite volume 2) Liquid Indefinite shape Definite volume 3) Gas Indefinite shape Indefinite

More information

TOPICAL PROBLEMS OF FLUID MECHANICS 97

TOPICAL PROBLEMS OF FLUID MECHANICS 97 TOPICAL PROBLEMS OF FLUID MECHANICS 97 DOI: http://dx.doi.org/10.14311/tpfm.2016.014 DESIGN OF COMBUSTION CHAMBER FOR FLAME FRONT VISUALISATION AND FIRST NUMERICAL SIMULATION J. Kouba, J. Novotný, J. Nožička

More information

Modeling of dispersed phase by Lagrangian approach in Fluent

Modeling of dispersed phase by Lagrangian approach in Fluent Lappeenranta University of Technology From the SelectedWorks of Kari Myöhänen 2008 Modeling of dispersed phase by Lagrangian approach in Fluent Kari Myöhänen Available at: https://works.bepress.com/kari_myohanen/5/

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

JSUNIL TUTORIAL. 6. Gay lussac s Law : At constant V, The pressure of fixed amount of gas varies directly with its absolute temperature.

JSUNIL TUTORIAL. 6. Gay lussac s Law : At constant V, The pressure of fixed amount of gas varies directly with its absolute temperature. CHAER 5 SAES OF MAER. Change in state : It is over all effect of Intermolecular forces, molecular Interactional energy & thermal energy:. Measurable properties of gases :,,, n, iscosity, specific heat

More information

States of matter. Book page , Syllabus /09/2016

States of matter. Book page , Syllabus /09/2016 States of matter Book page 169 171, 173-175 Syllabus 5.7 5.14 05/09/2016 cgrahamphysics.com 2015 What is my state of matter? sand Decaffeinated coffee Glass Supercritical fluids Supercritical fluids Coldest

More information

HiPerCap WP3 Membrane based technologies

HiPerCap WP3 Membrane based technologies HiPerCap WP3 Membrane based technologies May-Britt Hägg - NTNU WP Leader: NTNU Partners: SINTEF MC TIPS CNRS TNO EDF (CSIRO) Joint EU Australien workshop Workshop September 13 14, 2017 Oslo - Norway 22/09/2017

More information

Lecture Presentation. Chapter 11. Liquids and Intermolecular Forces. John D. Bookstaver St. Charles Community College Cottleville, MO

Lecture Presentation. Chapter 11. Liquids and Intermolecular Forces. John D. Bookstaver St. Charles Community College Cottleville, MO Lecture Presentation Chapter 11 Liquids and Intermolecular Forces John D. Bookstaver St. Charles Community College Cottleville, MO Properties of Gases, Liquids, and Solids State Volume Shape of State Density

More information

Best Practice Guidelines for Combustion Modeling. Raphael David A. Bacchi, ESSS

Best Practice Guidelines for Combustion Modeling. Raphael David A. Bacchi, ESSS Best Practice Guidelines for Combustion Modeling Raphael David A. Bacchi, ESSS PRESENTATION TOPICS Introduction; Combustion Phenomenology; Combustion Modeling; Reaction Mechanism; Radiation; Case Studies;

More information

Visit For All NCERT solutions, CBSE sample papers, Question papers, Notes for Class 6 to 12 V T P T. const, T

Visit  For All NCERT solutions, CBSE sample papers, Question papers, Notes for Class 6 to 12 V T P T. const, T isit www.ncerthelp.com For All NCER solutions, CBSE sample papers, Question papers, Notes for Class 6 to CHAER 5 SAES OF MAER. Change in state : It is over all effect of Intermolecular forces, molecular

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

Chapter 1: FUNDAMENTAL CONCEPTS OF THERMODYNAMICS AND VARIOUS THERMODYMIC PROCESSES

Chapter 1: FUNDAMENTAL CONCEPTS OF THERMODYNAMICS AND VARIOUS THERMODYMIC PROCESSES Chapter 1: FUNDAMENTAL CONCEPTS OF THERMODYNAMICS AND VARIOUS THERMODYMIC PROCESSES Thermodynamics is that branch of science which deals with energy transfer A system may be closed, open or isolated system

More information

CHEMISTRY - TRO 4E CH.11 - LIQUIDS, SOLIDS & INTERMOLECULAR FORCES

CHEMISTRY - TRO 4E CH.11 - LIQUIDS, SOLIDS & INTERMOLECULAR FORCES !! www.clutchprep.com CONCEPT: INTERMOLECULAR FORCES When looking at a molecular substance such as H 2 O you will discover two types of electrostatic forces at work: forces exist within a molecule and

More information

S = k log W CHEM Thermodynamics. Change in Entropy, S. Entropy, S. Entropy, S S = S 2 -S 1. Entropy is the measure of dispersal.

S = k log W CHEM Thermodynamics. Change in Entropy, S. Entropy, S. Entropy, S S = S 2 -S 1. Entropy is the measure of dispersal. , S is the measure of dispersal. The natural spontaneous direction of any process is toward greater dispersal of matter and of energy. Dispersal of matter: Thermodynamics We analyze the constraints on

More information

EF 152 Exam 3 - Spring 2017 Page 1 Copy 515

EF 152 Exam 3 - Spring 2017 Page 1 Copy 515 EF 152 Exam 3 - Spring 2017 Page 1 Copy 515 Instructions Do not open the exam until instructed to do so. Do not leave if there is less than 5 minutes to go in the exam. When time is called, immediately

More information

0654 CO-ORDINATED SCIENCES

0654 CO-ORDINATED SCIENCES CAMBRIDGE INTERNATIONAL EXAMINATIONS Cambridge International General Certificate of Secondary Education MARK SCHEME for the May/June 2015 series 0654 CO-ORDINATED SCIENCES 0654/31 Paper 3 (Extended Theory),

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

Classification and Labelling

Classification and Labelling Classification and Labelling Physical Hazards Eugen Anwander, Institute for Environment & Food Safety State of Vorarlberg / Austria Tour through the Topic physico-chemical hazards today (DSD 67/548/EEC)

More information

data Subsonic, helium release H 2 release concentrations Choked, Steady-state, concentrations release Transient, Subsonic, concentrations Subsonic,

data Subsonic, helium release H 2 release concentrations Choked, Steady-state, concentrations release Transient, Subsonic, concentrations Subsonic, GRAD CFD Software Validation The Gas Release And Dispersion (GRAD) CFD modeling tool has been designed as a customized module based on the commercial general-purpose CFD software, PHOENICS [1]. GRAD CFD

More information