Stat Mech of Non-Ideal Gases: Equations of State

Slides:



Advertisements
Similar presentations
Non-tabular approaches to calculating properties of real gases
Advertisements

GASES Question 1: 1994 B Free Response
VOLUMETRIC PROPERTIES OF PURE FLUIDS
Chemical Thermodynamics 2013/ nd Lecture: Zeroth Law, Gases and Equations of State Valentim M B Nunes, UD de Engenharia.
Properties of Reservoir Fluids Fugacity and Equilibrium Fall 2010 Shahab Gerami 1.
An equation of state is a relation between state variables It is a thermodynamic equation describing the state of matter under a given set of physical.
Chapter 18 Ideal vs. Real Gases. Variables Affecting Gases 4 Variables: 1.Pressure 2.Volume 3.Temperature 4.Number of particles By changing any one of.
PETE 310 Lectures # 32 to 34 Cubic Equations of State …Last Lectures.
5. Equations of State SVNA Chapter 3
Chem. Eng. Thermodynamics (TKK-2137) 14/15 Semester 3 Instructor: Rama Oktavian Office Hr.: M.13-15, Tu , W ,
Speed of Gases. Speed of Gases Root Mean Square Speed of Gases R = J *K / mol J = 1kg * m2 / s2 MM = molar mass.
Atkins’ Physical Chemistry Eighth Edition Chapter 1 The Properties of Gases Copyright © 2006 by Peter Atkins and Julio de Paula Peter Atkins Julio de Paula.
Now we introduce a new concept: fugacity
Real gases 1.4 Molecular interactions 1.5 The van de Waals equation 1.6 The principle of corresponding states Real gases do not obey the perfect gas law.
Real vs. Ideal Gas Under what types of pressure do gases behave ideally? Under what type of temperatures do gases behave ideally? We originally defined.
Real Gases Deviation from ideal gas Law: -Gas particles have volume - Attraction exists between gas particles (liquefication) Ideal gas law applies only.
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
Chapter 8 Real Gases.
Properties of Pure Substances Chapter 3. Why do we need physical properties?  As we analyze thermodynamic systems we describe them using physical properties.
Miscellaneous Contributions by:
GASES.
Advance Chemical Engineering Thermodynamics By Dr.Dang Saebea.
Real Gas Relationships
Chapter 5: The Gaseous State Chemistry 1061: Principles of Chemistry I Andy Aspaas, Instructor.
Physical Property Modeling from Equations of State David Schaich Hope College REU 2003 Evaluation of Series Coefficients for the Peng-Robinson Equation.
5.2 Ideal Gases Densities of gases  Sensitive to T and P P-V-T relation  Equation of State (EOS) Ideal Gas Law for Single Component PV = nRT Ideal Gas.
Pressure – Volume – Temperature Relationship of Pure Fluids.
The Boltzmann Distribution allows Calculation of Molecular Speeds Mathematically the Boltzmann Distribution says that the probability of being in a particular.
Chapter 5 Single Phase Systems
Thermodynamics I Inter - Bayamon Lecture 3 Thermodynamics I MECN 4201 Professor: Dr. Omar E. Meza Castillo
Ideal gases: Gas particles do not attract one another Gas particles do not occupy volume There are no ideal gases in real life.
GASES. Gases  The physical state of gases is defined by several physical properties  Volume  Temperature  Amount (commonly expressed as number of.
CHEM 112 Spring 2011 Exam 1 Review.
REAL GAS RELATIONSHIPS How can we predict behavior of gases at such conditions ? There are FOUR methods: 1) Compressibility Charts 2) Equations of State.
공정 열역학 Chapter 3. Volumetric Properties of Pure Fluids
Equations of State The Ideal Gas
1 Equations of State The relationship among the state variables, temperature, pressure, and specific volume is called the equation of state. We now consider.
Parul Institute of Engineering & Technology
Real Gases Real gases often do not behave like ideal gases at high pressure or low temperature. Ideal gas laws assume 1. no attractions between gas molecules.
Prepared By: Bhadka Ravi H. Guided By: Mr. P. L. Koradiya
The Ideal Gas.
Chapter 5 Continued: More Topics in Classical Thermodynamics
Critical Point Consider what happens when the volume of 1.0 mole of water vapor initially at 10 torr is decreased at a constant temperature of 25 oC. thermostated.
Chapter 1. Properties of Gases
Pressure and KMT mvx−m(−vx)=2mvx
Properties of Gases Kinetic Molecular Model Speed of gas
Lecture 11 Critical point and real gases
Chapter 10 Gases: Their Properties and Behavior
The Ideal Gas Law.
Chapter Three: Part Two
Behaviors of Solids, Liquids, and Gases
Modified by Jed Macosko
Einstein Model for the Vibrational Heat Capacity of Solids
Satish Pradhan Dnyanasadhana college, Thane
Behavior of Gases Byeong-Joo Lee Thermodynamics POSTECH - MSE
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.
Gas Laws For Real Gases.
Chapter Three: Part Two
13.6 NOTES Temperature and Pressure Behavior
Chapter 8 Real Gases.
CHAPTER 3 Volumetric Properties of Pure Fluids: Part 1
Gas Stoichiometry Unit
Chapter10 Gases.
States of Matter Lesson 4.6
Chapter Three_ Part Two
2 CHAPTER Properties of Pure Substances.
Non-Ideal Behavior (Real gases):
Root Mean Square Velocity (urms)
Lecture 11 Critical point and real gases
Presentation transcript:

Stat Mech of Non-Ideal Gases: Equations of State

This state is called a supercritical fluid. Real Gases Many real gases do not come even close to obeying The Ideal Gas Law. At modest temperatures & high pressure, the molecules get close enough together that intermolecular attractive forces become significant. Two Things Can Happen: At low temperatures the gas can turn into a liquid. At higher temperatures the gas stays a gas but behaves a lot like a liquid. This state is called a supercritical fluid.

Critical Temperature (Tc) & Pressure (Pc) For all gases, there is a temperature at which it is impossible to ever form a liquid, regardless of the pressure. That temperature is called The Critical Temperature  Tc. For all gases, there is a pressure at which there is both vapor and liquid. That pressure is called The Critical Pressure  Pc. Tc & Pc. are key parameters for calculating the relationship between P, V, and T for non-ideal gases using empirical Equations of State. Tc & Pc are tabulated for many gases & fluids.

Empirical Equations of State Several empirical “cubic” equations have been invented to relate P to V and T for non-ideal gases: 1. Van der Waals 2. Redlich-Kwong 3. Peng-Robinson 4. Redlich-Kwong-Suave Now, brief discussions of #1 & #3.

Van der Waals Equation of State This one of the earliest & simplest empirical Equation of State. It was briefly discussed earlier in the course. It has the form: Comes from intermolecular attractions & is most important at small molar volumes. Molar Volume (Volume per Mole) Comes from the volume of the molecules themselves & is most important at small molar volumes.

The values of the empirical parameters a & b are different for different gas molecules, but they are related in the same way to the Tc & Pc for each gas. Note again that the critical properties Tc & Pc are tabulated for the common gases. It can be shown that the Van der Waals parameters a & b are related to Tc & Pc in the following way:

Peng-Robinson Equation of State The Van der Waals Equation of State is OK but other empirical Equations of State are more accurate. Of course, that also means that they are more complicated! An empirical Equation of State that tries to achieve a balance of accuracy vs complexity is the Peng-Robinson Equation of State. It has the form:

Peng-Robinson Equation of State The empirical parameters a & b are related to the critical temperature & pressure Tc & Pc in the following way: The empirical parameter a is temperature dependent & also depends on another tabulated, chemical specific, parameter, the so-called “acentric factor” :

Peng-Robinson It is usually a good idea to program the more complex equations into a spreadsheet or Maple. Because of the way the equation is written, finding the volume when T and P are given or finding the temperature when P and V are given requires trial and error calculations (root finding)

Beware Multiple Roots When the object is to find V with T and P known, then it is possible to get 3 answers (roots) that all satisfy the equation. This will only happen for T below the critical temperature. The smallest value is a volume that corresponds to the liquid at that T and P The largest value is a volume that corresponds to the vapor (most accurate). The middle value has no physical meaning (just a mathematical artifact). In trial and error programs like Solver, one must achieve the desired root by an initial guess that is close to desired root.

Cubic EOS roots Pressure P Isotherm above Tc Specific Volume (V)

Below Tc Three roots (3 V’s are predicted by equation) Pressure P Isotherm below Tc T1 Specific Volume (V)

Root Evaluation Below Tc – care must be taken to make sure that the right root is obtained There is one root near the ideal gas law (The large volume) There is one root near b This is the liquid root and is hard to get There is one root near 3b This is a physically meaningless root (the middle one)

Virial Equations For sophisticated calculations fitting equations with more adjustable parameters are used. These are called virial equations. Some equations (like those for water) might have 20 or more adjustable constants…

Summary EOS are more accurate representations of fluid PVT relationships than the simple ideal gas law. Cubic equations of state have a good balance between simplicity and accuracy. The other main type of empirical equation is a “virial” equation that attempts to fit the PVT behavior with a long series of “adjustment” terms: