PETE 310 Lectures # 6 & # 7 Phase Behavior – Pure Substances (Lecture # 5) Two Component Mixtures Three & Multicomponent Mixtures.

Slides:



Advertisements
Similar presentations
Properties of pure substances
Advertisements

APPLICATIONS Applications of Raoult’s law
Instructor’s Visual Aids Heat Work and Energy. A First Course in Thermodynamics © 2002, F. A. Kulacki Chapter 2 Module 2 Slide 1 Additional Aspects for.
VOLUMETRIC PROPERTIES OF PURE FLUIDS
ES 202 Fluid and Thermal Systems Lecture 15: Properties in Two-Phase Region (1/16/2003)
Lecture 18Multicomponent Phase Equilibrium1 Thermodynamics of Solutions Let’s consider forming a solution. Start with X A moles of pure A and X B moles.
Pure Substances Thermodynamics Professor Lee Carkner Lecture 5.
CHE-201: Introduction to Chemical Engineering
Phase Changes Courtesy
Chapter 12 Gas-Liquid Equilibrium
PETE 310 Lectures # 32 to 34 Cubic Equations of State …Last Lectures.
Properties of Solutions
Chapter 141 Solutions and Their Behavior Chapter 14.
Solid-vapor equilibrium (SVE) and Solid-liquid equilibrium (SLE)
Chapter 14-Part VII Applications of VLLE.
Chapter 14: Phase Equilibria Applications
Lec 5: Thermodynamic properties, Pvt behavior
Ideal Gas Law Physics 313 Professor Lee Carkner Lecture 10.
ES 202 Fluid and Thermal Systems Lecture 17: More on properties and phases (1/21/2003)
Solution Thermodynamic:
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 31 Ideal Gas Mixtures.
Chapter 3 PROPERTIES OF PURE SUBSTANCES
Lesson 5 CHANGE OF PHASE DISTINGUISH between intensive and extensive properties. DEFINE the following terms: – Saturation – Subcooled liquid – Superheated.
Chapter 3 Properties of a Pure Substance
Three & Multicomponent Mixtures…
MEL140 Properties of pure substances. Pure substance A pure substance has the same chemical composition throughout. Are the following confined in a fixed.
Chemical Thermodynamics 2013/ th Lecture: Mixtures of Volatile Liquids Valentim M B Nunes, UD de Engenharia.
Vapor pressure and liquids Vapor : A gas that exists below its critical point Gas : gas that exists above its critical point ِNote : A gas can not condense.
Eng. Samra Essalaimeh Philadelphia University 2nd Semester
Ch# 2 Properties of Pure Substances. Objectives Introduce the concept of a pure substance. Introduce the concept of a pure substance. Discuss the physics.
PETE 310 Lecture # 5 Phase Behavior – Pure Substances.
CHAPTER 3 Volumetric Properties of Pure Fluids Miss. Rahimah Bt. Othman ERT 206/4 Thermodynamics.
Chapter 11: Other Types of Phase Equilibria in Fluid Mixtures (selected topics)
Carbon Dioxide Dr. Reid B. Grigg New Mexico Petroleum Recovery Research Center New Mexico Institute of Mining and Technology Socorro, New Mexico.
Ideal Gases.
PHASE EQUILIBRIA. Ternary Systems Types:  (Liquid –Vapor) ternary systems  (Liquid – Solid ) ternary systems.
Lecture # 4 PROPERTIES OF PURE SUBSTANCES PURE SUBSTANCE.
CHAPTER 5 Multi-phase systems
CHAPTER 2 Properties of Pure Substances. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. A Pure Substance.
Chapter 4 PROPERTIES OF PURE SUBSTANCES
WCB/McGraw-Hill © The McGraw-Hill Companies, Inc.,1998 Thermodynamics Çengel Boles Third Edition 2 CHAPTER Properties of Pure Substances.
Objectives Solve thermodynamic problems and use properties in equations (today) Calculate heat transfer by all three modes including phase change (Thursday)
APPLICATIONS Applications of Raoult’s law
PETE 310 Lecture # 26 Chapter 12 Gas-Liquid Equilibrium Non-ideal VLE.
Introduction to phase equilibrium
Thermodynamics I Inter - Bayamon Lecture 3 Thermodynamics I MECN 4201 Professor: Dr. Omar E. Meza Castillo
Ideal and Dilute Solutions 2/21/2016. Master Thermodynamics Equations.
Chapter 3 PROPERTIES OF PURE SUBSTANCES Dr. Kagan ERYURUK Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Clapeyron and Clausius Clapeyron Equations
Noorulnajwa Diyana Yaacob PPK Bioproses Universiti Malaysia Perlis MULTIPHASE SYSTEM.
Chapter 14: Phase Equilibria Applications Part II.
공정 열역학 Chapter 3. Volumetric Properties of Pure Fluids
Section 14.1 Types of Mixtures
Solutions Textbook Chapter 14. Definitions n A solution is a homogeneous mixture n A solute is dissolved in a solvent. –solute is the substance being.
1 Equations of State The relationship among the state variables, temperature, pressure, and specific volume is called the equation of state. We now consider.
RESERVOIR ENGINEERING
Gas Properties & PVT Tests
THERMODYNAMICS OF SOLUTIONS
Classical description of a single component system
What is Petroleum ? l Petroleum is a mixture of naturally ocurring hydrocarbons which may exist in the solid, liquid or gaseous states, depending on the.
Liquid-Liquid Phase Equilibrium
Lecture 49 More on Phase Transition, binary system
Properties of water Solid phase ______ dense than liquid
Gases Ch 12.
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.
Enthalpy vs. Composition – Ponchon-Savarit Plot
Lecture # 26 Chapter 12 Gas-Liquid Equilibrium Non-ideal VLE
Lecture 31 Ideal Gas Mixtures.
Chapter 12 Gas-Liquid Equilibrium
Chapter 3: Evaluating Properties
Presentation transcript:

PETE 310 Lectures # 6 & # 7 Phase Behavior – Pure Substances (Lecture # 5) Two Component Mixtures Three & Multicomponent Mixtures

Learning Objectives After completing this chapter you will be able to:  Understand pure component phase behavior as a function of pressure, temperature, and molecular size.  Understand the behavior of binary and multicomponent mixtures  Behavior understood through proper interpretation of phase diagrams

Phase Diagrams  Types of phase diagrams for a single component (pure substance)  (PT)  (PV) or (P  )  (TV) or (T 

Phase Diagrams Single Component Phase Diagram

Phase Diagrams Vapor Pressure Curve Pressure Temperature Vapor Liquid Critical Point  l  v P c T c

Hydrocarbon Families Physical Properties One point in the Vapor Pressure Curve

Pressure vs Specific Volume Pure Substance TcTc 2-phase T Specific Volume (ft 3 / lbm) Pressure ( psia ) V v V L CP

 Tabulated critical properties (McCain) Pure Component Properties

Heat Effects Accompanying Phase Changes of Pure Substances Heat Effects Accompanying Phase Changes of Pure Substances Lv = T  V dP v dT With  V = V Mg -V Ml Btu/lb-mol Clapeyron equation

Heat Effects Accompanying Phase Changes of Pure Substances Heat Effects Accompanying Phase Changes of Pure Substances Lv = T  V dP v dT = Approximate relation (Clausius - Clapeyron Equation) dP v dT RT 2 P v Lv

Example of Heat Effects Accompanying Phase Changes  Steam flooding Problem: Calculate how many BTU/day (just from the latent heat of steam) are provided to a reservoir by injecting 6000 bbl/day of steam at 80% quality and at a T=462 o F Calculate how many BTU/day (just from the latent heat of steam) are provided to a reservoir by injecting 6000 bbl/day of steam at 80% quality and at a T=462 o F

COX - Vapor Pressure Charts (normal paraffins) Pressure Temperature heavier Non-linear scale Log scale

Determination of Fluid Properties Temperature of Test Constant V t1 V t2 V t3 = V b V t5 V t4 liquid gas Hg P 1 >> P s P 2 > P s P 3 = P s P 4 = P s P 5 =P s Ps =saturation pressure

Vapor Pressure Determination Pressure P S Volume V L T2T2T2T2 T1T1T1T1

Binary Mixtures  Relationships to analyze: P, T, molar or specific volume or (molar or mass density) - as for a pure component – +  COMPOSITION – Molar Composition

Hydrocarbon Composition  The hydrocarbon composition may be expressed on a weight basis or on a molar basis (most common)  Recall

Hydrocarbon Composition  By convention liquid compositions (mole fractions) are indicated with an x and gas compositions with a y.

Our Systems of Concern Gas system Oil system open

A separator z i (T 1,P 1 ) x i (T 1,P 2 ) y i (T 1,P 2 ) P 1 > P 2 T 1,P 2

with In general Mathematical Relationships

Key Concepts  Fraction of vapor (fv)  Mole fractions in vapor (or gas) phase  yi  Mole fractions in liquid (or oil) phase  xi  Overall mole fractions (zi)  combining gas & liquid

Phase Diagrams for Binary Mixtures  Types of phase diagrams for a two- component mixture Most common  (PT) zi at a fixed composition  (Pzi) T at a fixed T  (Tzi  P  at a fixed P  (PV) zi or (P  ) zi

Pressure vs Temperature Diagram (PT) zi CB CT CP Bubble Curve Dew Curve Pressure Temperature Liquid Gas 2 Phases Zi = fixed

Pressure Composition Diagrams - Binary Systems

Temperature vs. Composition Diagrams – Binary Systems Temperature Pressure Bubble Curve Dew Curve 2-phases x 1, y 1 PaPa PaPa CP 1 CP 2 T1sT1s T2sT2s T2sT2s T1sT1s 0 1

Gas-Liquid Relations z 1 =overall mole fraction of [1],y 1 =vapor mole fraction of [1],x 1 =liquid mole fraction of [1]

Supercritical Conditions Binary Mixture

Quantitative Phase Equilibrium Exercise

Ternary Diagrams: Review

Pressure Effect C3C3 C3C3 nC 5 C3C3 C1C1 Gas p=14.7 psia C1C1 nC 5 Gas 2-phase Liquid p=380 psia C3C3 nC 5 C1C1 C3C3 Gas 2-phase Liquid p=500 psia C1C1 Gas 2-phase Liquid nC 5 p=1500 psia 2-phase Liquid C1C1 nC 5 Gas p=2000 psia C1C1 nC 5 C3C3 Liquid p=2350 psia

Dilution Lines Ternary Diagrams: Review

Quantitative Representation of Phase Equilibria - Tie (or equilibrium) lines  Tie lines join equilibrium conditions of the gas and liquid at a given pressure and temperature.  Dew point curve gives the gas composition.  Bubble point curve gives the liquid composition.

Ternary Diagrams: Review Quantitative Representation of Phase Equilibria - Tie (or equilibrium) lines  All mixtures whose overall composition (z i ) is along a tie line have the SAME equilibrium gas (y i ) and liquid composition (x i ), but the relative amounts on a molar basis of gas and liquid (f v and f l ) change linearly (0 – vapor at B.P., 1 – liquid at B.P.).

Illustration of Phase Envelope and Tie Lines

Uses of Ternary Diagrams Representation of Multi-Component Phase Behavior with a Pseudoternary Diagram  Ternary diagrams may approximate phase behavior of multi-component mixtures by grouping them into 3 pseudocomponents  heavy (C 7 + )  intermediate (C 2 -C 6 )  light (C 1, CO 2, N 2 - C 1, CO 2 -C 2,...)

Uses of Ternary Diagrams Miscible Recovery Processes Solvent1 oil Solvent2

Exercise Find overall composition of mixture made with 100 moles oil "O" + 10 moles of mixture "A". __________________________________________________________________________________________________________________________________

Practice Ternary Diagrams Pressure Effect T=180F P=14.7 psia Pressure Effect O T=180F P=200 psia C1-C3-C10 Pressure Effect O T=180F P=400 psia Pressure Effect O T=180F P=600 psia Pressure Effect O

Practice Ternary Diagrams Pressure Effect T=180F P=1000 psia Pressure Effect O T=180F P=1500 psia Pressure Effect O T=180F P=2000 psia O T=180F P=3000 psia O T=180F P=4000 psia O

Practice Ternary Diagrams Temperature Effect T=100F P=2000 psia Temperature Effect O T=150F P=2000 psia Temperature Effect O T=200F P=2000 psia Temperature Effect O T=300F P=2000 psia Temperature Effect O

Practice Ternary Diagrams Temperature Effect T=350F P=2000 psia Temperature Effect O T=400F P=2000 psia Temperature Effect O T=450F P=2000 psia Temperature Effect O

Pressure-Temperature Diagram for Multicomponent Systems

Changes During Production and Injection Temperature t 1 Pressure t 3 t 2 Gas Injection Production t t 3 2 Gas Injection Production

Homework  See Syllabus please