11/8/20074th Challenge IFPSC1 Establishing Benchmarks for the Fourth Industrial Fluid Properties Simulation Challenge James D. Olson The Dow Chemical Company.

Slides:



Advertisements
Similar presentations
Properties of a Pure Substance
Advertisements

Cavitation and Bubble Dynamics Ch.1 Cavitation and Boiling.
Non-tabular approaches to calculating properties of real gases
Lecture 15: Capillary motion
Advanced Thermodynamics Note 3 Heat Effects
Advanced Thermodynamics Note 6 Applications of Thermodynamics to Flow Processes Lecturer: 郭修伯.
VOLUMETRIC PROPERTIES OF PURE FLUIDS
Chemical Thermodynamics 2013/ nd Lecture: Zeroth Law, Gases and Equations of State Valentim M B Nunes, UD de Engenharia.
Matter: Properties & Change
Chem. Eng. Thermodynamics (TKK-2137) 14/15 Semester 3 Instructor: Rama Oktavian Office Hr.: M.13-15, Tu , W ,
Advanced Thermodynamics Note 5 Thermodynamic Properties of Fluids
Solid-vapor equilibrium (SVE) and Solid-liquid equilibrium (SLE)
Chapter 14: Phase Equilibria Applications
Lecture 3411/30/05. Vapor pressure vs. boiling point?
Thermodynamic Property Relations
Now we introduce a new concept: fugacity
Liquid Argon in a Large Tank --- Some Thermodynamic Calculations Zhijing Tang November 4, 2004.
Chapter 1 – Fluid Properties
Kern Method of SHELL-AND-TUBE HEAT EXCHANGER Analysis
AME Int. Heat Trans. D. B. Go 1 Work Examples F CM ΔxΔx [1] Sliding Block work done to the control mass so it is energy gained [2] Shear Work on.
Presenter: Ian Richardson (WSU) Co-Authors: Thomas Blackham (WSU), Jacob Leachman (WSU), Eric Lemmon (NIST) 1 Helium-Hydrogen P ρ T-x Measurements and.
Chapter 3 Properties of a Pure Substance
Real Gases Deviation from ideal gas Law: -Gas particles have volume - Attraction exists between gas particles (liquefication) Ideal gas law applies only.
Dicky Dermawan ITK-234 Termodinamika Teknik Kimia II Nonideal Behavior Dicky Dermawan
Phases of Matter.
Real gas 1.molecules not always in motion (condense phase can be formed) 2.molecular size is non-negligible (there is molecular repulsion) 3.Molecules.
PVT Behavior of Fluids and the Theorem of Corresponding States
IFPSC vision statement A robust, accurate, and easy-to-use set of modeling tools will be widely available for the prediction.
Advance Chemical Engineering Thermodynamics
Adventures in Thermochemistry James S. Chickos * Department of Chemistry and Biochemistry University of Missouri-St. Louis Louis MO 63121
I. Molecular Simulations of Water and Steam II. Hazardous Waste Treatment: Supercritical Water Oxidation I. Molecular Simulations of Water and Steam II.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review April , 2004, LBNL Target Simulation Roman Samulyak, in collaboration with.
chapter 2 Properties of Pure Substances
PETE 310 Lecture # 5 Phase Behavior – Pure Substances.
CHROMATOGRAPHY Chromatography basically involves the separation of mixtures due to differences in the distribution coefficient.
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 5 Thermodynamic Properties.
Overview AIChE Annual Meeting Salt Lake City, Utah November 8, 2007
1. (1.3) (1.8) (1.11) (1.14) Fundamental equations for homogeneous closed system consisting of 1 mole:
Reduced-adiabat Isotherms of Metals and Hard Materials at 100 GPa Pressures and Finite Temperatures W. J. Nellis Department of Physics Harvard University.
GASES.
Advance Chemical Engineering Thermodynamics By Dr.Dang Saebea.
Real Gas Relationships
Solution thermodynamics theory—Part I
6. Coping with Non-Ideality SVNA 10.3
Chem. Eng. Thermodynamics (TKK-2137) 14/15 Semester 3 Instructor: Rama Oktavian Office Hr.: M.13-15, Tu , W ,
CHAPTER 2 Properties of Pure Substances. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. A Pure Substance.
A "Reference Series" Method for Prediction of Properties of Long-Chain Substances Inga Paster and Mordechai Shacham Dept. Chem. Eng. Ben-Gurion University.
Properties of Liquids Kinetic-Molecular theory …The phase of any substance is determined by the inter and intramolecular forces present and the KE of the.
Pressure – Volume – Temperature Relationship of Pure Fluids.
Chapter 5 Single Phase Systems
Introduction to phase equilibrium
Solution thermodynamics theory
Thermodynamics I Inter - Bayamon Lecture 3 Thermodynamics I MECN 4201 Professor: Dr. Omar E. Meza Castillo
SOLUTION THERMODYNAMICS:
GASES. Gases  The physical state of gases is defined by several physical properties  Volume  Temperature  Amount (commonly expressed as number of.
Investigation of Thin Film Evaporation Limit in Single Screen Mesh Layers Presented to IMECE 2002 Nov. 19, 2002, New Orleans, LA Yaxiong Wang & G.P. “Bud”
1 Prediction of Phase Equilibrium Related Properties by Correlations Based on Similarity of Molecular Structures N. Brauner a, M. Shacham b, R.P. Stateva.
CHEM 112 Spring 2011 Exam 1 Review.
Sections 11.1 – 11.3 Properties of Liquids. Properties of Liquids In these sections… a.Phases of Matter b.Phase Changes c.Properties of Liquids: 1.Enthalpy.
Chapter 14: Phase Equilibria Applications Part II.
공정 열역학 Chapter 3. Volumetric Properties of Pure Fluids
Process Design Course Using the NIST, DIPPR and DDBSP databases for Finding Physical, Chemical and Thermodynamic Properties Process Design Course.
MODUL KE SATU TEKNIK MESIN FAKULTAS TEKNOLOGI INDUSTRI
Gas Properties & PVT Tests
Thermodynamics of Wet, Saturated & Superheated Vapor
Understanding Hydrocarbon Fluid Properties and Behavior
THERMODYNAMIC PROPERTIES OF FLUIDS
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.
Ch. 8 – phases: gases,liquids,and solids
Theory of Steam Production
Presentation transcript:

11/8/20074th Challenge IFPSC1 Establishing Benchmarks for the Fourth Industrial Fluid Properties Simulation Challenge James D. Olson The Dow Chemical Company November 8, 2007

11/8/20074th Challenge IFPSC2 Overview zThe Fourth Challenge  Three Categories of Benchmarks zBenchmark Data Sources  Literature and estimations from DIPPR and PPDS zThe 17 Benchmarks and Uncertainties  Second virial coefficient Benchmark value was revised

11/8/20074th Challenge IFPSC3 Acknowledgements – Data Reviewed by: zDan Friend – NIST zRob Chirico – NIST (TRC) zMarcia Huber - NIST

11/8/20074th Challenge IFPSC4 Industrial Fluid Properties Simulation Challenge zIndustrial use of molecular simulation:  Qualitative use vs quantitative chemical use: xQualitative - explore structure and mechanisms at the molecular level, pico-sec time scale; e.g., to study formation and structure of surfactant micelles. xQuantitative - produce process design data for state conditions not (easily) accessible to lab measurements.

11/8/20074th Challenge IFPSC5 The Fourth Challenge zThe primary objective of the Fourth Industrial Fluid Properties Simulation Challenge is to test the transferability of methods and force fields to a wide variety of properties for a given small molecule.

11/8/20074th Challenge IFPSC6 Three Categories of Benchmarks zCategory 1 (100 points total)  Saturated liquid phase density at 375 K (11 points max)  Saturated vapor phase density at 375 K (11 points max)  Second virial coefficient at 375 K (11 points max)  Vapor pressure at 375 K (11 points max)  Heat of vaporization at 375 K (11 points max)  Normal boiling temperature at kPa (15 points max)  Critical density (15 points max)  Critical temperature (15 points max)

11/8/20074th Challenge IFPSC7 Three Categories of Benchmarks zCategory 2 (100 points total)  Saturated liquid phase heat capacity at 375 K (15 points max)  Saturated vapor phase heat capacity at 375 K (15 points max)  Saturated liquid phase isothermal compressibility at 375 K (20 points max)  Saturated vapor phase isothermal compressibility at 375 K (20 points max)  Surface tension at 375 K (30 points max)

11/8/20074th Challenge IFPSC8 Three Categories of Benchmarks zCategory 3 (100 points total)  Saturated liquid phase viscosity at 375 K (25 points max)  Saturated vapor phase viscosity at 375 K (25 points max)  Saturated liquid phase thermal conductivity at 375 K (25 points max)  Saturated vapor phase thermal conductivity at 375 K (25 points max)

11/8/20074th Challenge IFPSC9 Benchmark Data Sources zThe previous three Challenges used data measured specifically for the challenge, e.g., liquid viscosity of 2-propanol + nonane mixtures. zNo new experimental data were measured for the Fourth Challenge. Also, for several EO properties no data have ever been measured above 280 K. zAppropriately larger uncertainties were assigned.

11/8/20074th Challenge IFPSC10 Benchmark Data Source Strategy zThree data sources were used (similar strategy to that used in an industrial process design) :  Data published in peer-reviewed scientific literature.  Data from AICHE DIPPR Database – correlations fitted to experimental data where available or estimation methods.  Data from Physical Properties Data Service (PPDS) – associated with UK NPL

11/8/20074th Challenge IFPSC14 Second Virial Coefficient at 375 K zBenchmark = cm 3 /g  Uncertainty = 4.9 %  Maximum allowed Deviation = 25 % zBenchmark taken as mean between the value derived from the Walters and Smith PVT data and the value derived from the Hurly sound speed data. zBenchmark value was revised after discovery of Hurly sound speed data for ethylene oxide

11/8/20074th Challenge IFPSC16 Saturated Liquid-Phase Density at 375 K zBenchmark = g/cm 3  Uncertainty = 0.5 %  Maximum allowed Deviation = 5 % zBenchmark taken from DIPPR density equation fitted to available experimental data.

11/8/20074th Challenge IFPSC18 Saturated Vapor-Phase Density at 375 K zBenchmark = g/cm 3  Uncertainty = 4.1 %  Maximum allowed Deviation = 20 % zBenchmark calculated from second virial equation – agrees within uncertainty with the PPDS value.

11/8/20074th Challenge IFPSC19 Vapor Pressure at 375 K zBenchmark = 1437 kPa  Uncertainty = 1.5 %  Maximum allowed Deviation = 8 % zBenchmark taken from DIPPR vapor pressure equation fitted to available experimental data.

11/8/20074th Challenge IFPSC20 Heat of Vaporization at 375 K zBenchmark = 453 J/g  Uncertainty = 1.8 %  Maximum allowed Deviation = 10 % zBenchmark taken from DIPPR heat of vaporization equation fitted to data derived from the vapor pressure via the Clapeyron equation.

11/8/20074th Challenge IFPSC21 Normal Boiling Point at kPa zBenchmark = K  Uncertainty = 0.2 %  Maximum allowed Deviation = 5 % zBenchmark taken from data of Giauque and co-workers, J. Amer. Chem. Soc. (1949) 71, 2176

11/8/20074th Challenge IFPSC22 Critical Density zBenchmark = g/cm 3  Uncertainty = 5.1 %  Maximum allowed Deviation = 25 % zBenchmark taken from Ambrose & Townsend, "Vapor-Liquid Critical Properties“, National Physical Laboratory, Middlesex, United Kingdom (1977)

11/8/20074th Challenge IFPSC23 Critical Temperature zBenchmark = K  Uncertainty = 0.2 %  Maximum allowed Deviation = 5 % zBenchmark taken from Ambrose & Townsend, “Vapor-Liquid Critical Properties“, National Physical Laboratory, Middlesex, United Kingdom (1977)

11/8/20074th Challenge IFPSC24 Saturated Liquid Heat Capacity at 375 K zBenchmark = 2.30 J/[g-K]  Uncertainty = 8.3 %  Maximum allowed Deviation = 40 % zBenchmark taken from an extrapolation of the measured data of Giauque and coworkers compared to PPDS and DIPPR

11/8/20074th Challenge IFPSC26 Saturated Vapor Heat Capacity at 375 K zBenchmark = 1.67 J/[g-K]  Uncertainty = 15 %  Maximum allowed Deviation = 50 % zBenchmark taken from PPDS real gas correction to ideal gas heat capacity.

11/8/20074th Challenge IFPSC27 Saturated Liquid Isothermal Compressibility at 375 K zBenchmark = 2.60 [10 6 kPa] -1  Uncertainty = 23.1 %  Maximum allowed Deviation = 50 % zBenchmark calculated from Brelvi- O'Connell correlation.

11/8/20074th Challenge IFPSC28 Saturated Vapor Isothermal Compressibility at 375 K zBenchmark = 819 [10 6 kPa] -1  Uncertainty = 9.2 %  Maximum allowed Deviation = 45 % zBenchmark calculated from second virial equation.

11/8/20074th Challenge IFPSC29 Surface Tension at 375 K zBenchmark = N/m  Uncertainty = 12.5 %  Maximum allowed Deviation = 50 % zBenchmark taken from DIPPR surface tension equation fitted to data given by Jasper.

11/8/20074th Challenge IFPSC30 Saturated Liquid Viscosity at 375 K zBenchmark = Pa-s  Uncertainty = 13.2 %  Maximum allowed Deviation = 50 % zBenchmark taken from DIPPR viscosity equation fitted to experimental data of Maass and Boomer.

11/8/20074th Challenge IFPSC32 Saturated Vapor Viscosity at 375 K zBenchmark = Pa-s  Uncertainty = 6.5 %  Maximum allowed Deviation = 30 % zBenchmark taken from PPDS estimation.

11/8/20074th Challenge IFPSC33 Saturated Liquid Thermal Conductivity at 375 K zBenchmark = 0.12 W/[m-K]  Uncertainty = 25 %  Maximum allowed Deviation = 50 % zBenchmark taken from DIPPR thermal conductivity equation fitted to data estimated by Missenard method (there are no experimental data at any temperature).

11/8/20074th Challenge IFPSC34 Saturated Vapor Thermal Conductivity at 375 K zBenchmark = W/[m-K]  Uncertainty = 14.7 %  Maximum allowed Deviation = 50 % zBenchmark taken from DIPPR thermal conductivity equation fitted to data measured by Senftleben.