Chemical Engineering Thermodynamics-II Topic: Excess Gibbs Free Energy, Data Reduction, Thermodynamic Consistency Prepatred by:- Patel Nirav (130110105032)

Slides:



Advertisements
Similar presentations
Thermodynamics l l a system: Some portion of the universe that you wish to study l The surroundings: The adjacent part of the universe outside the system.
Advertisements

Entropy and Free Energy Chapter 19. Laws of Thermodynamics First Law – Energy is conserved in chemical processes neither created nor destroyed converted.
Thermodynamics and P-T
THERMODYNAMICS 2 Dr. Harris Suggested HW: Ch 23: 43, 59, 77, 81.
Chapter 16 Chemical and Phase Equilibrium Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus.
Solution Thermodynamics: Applications
Thermodynamic Property Relations
Gibbs Free Energy Gibbs free energy is a measure of chemical energy All chemical systems tend naturally toward states of minimum Gibbs free energy G =
Q&A_ /17/2005(10) Ji-Sheng Chang
System. surroundings. universe.
Volume Changes (Equation of State) Volume is related to energy changes: Mineral volume changes as a function of T: , coefficient of thermal expansion.
Thermodynamics: Spontaneity, Entropy and Free Energy.
Solution thermodynamics theory—Part IV
Heat Capacity Amount of energy required to raise the temperature of a substance by 1C (extensive property) For 1 mol of substance: molar heat capacity.
Chemical Thermodynamics BLB 12 th Chapter 19. Chemical Reactions 1. Will the reaction occur, i.e. is it spontaneous? Ch. 5, How fast will the reaction.
Spontaneity and Equilibrium in Chemical Systems
 Section 1 – Thermochemistry  Section 2 – Driving Force of Reactions.
Chemical Thermodynamics The chemistry that deals with the energy and entropy changes and the spontaneity of a chemical process.
Energy Changes in Chemical Reactions -- Chapter First Law of Thermodynamics (Conservation of energy)  E = q + w where, q = heat absorbed by system.
Thermochemistry Study of energy transformations and transfers that accompany chemical and physical changes. Terminology System Surroundings Heat (q) transfer.
Chapter 19 Chemical Thermodynamics. First Law of Thermodynamics Energy cannot be created nor destroyed. Therefore, the total energy of the universe is.
Thermodynamics Chapter 18.
Gibbs Free energy and Helmholtz free energy. Learning objectives After reviewing this presentation learner will be able to Explain entropy and enthalpy.
THERMODYNAMICS!!!! Nick Fox Dan Voicu.
The Third Law, Absolute Entropy and Free Energy Lecture 4.
Thermodynamics. Spontaneity What does it mean when we say a process is spontaneous? A spontaneous process is one which occurs naturally with no external.
Thermodynamics Chapter 19. First Law of Thermodynamics You will recall from Chapter 5 that energy cannot be created or destroyed. Therefore, the total.
A.P. Chemistry Spontaneity, Entropy, and Free Energy.
Chapter 19 Chemical Thermodynamics HW:
Chapter 18: Thermodynamics Renee Y. Becker Valencia Community College.
Energy Many ways to describe energy changes in thermodynamics Originally developed to describe changes in heat and ‘work’ (think a steam engine piston)
Review: Expressions of the thermodynamic equilibrium constant K
1 The Second Law of Thermodynamics (II). 2 The Fundamental Equation We have shown that: dU = dq + dw plus dw rev = -pdV and dq rev = TdS We may write:
Thermody-nizzle-amics A (Josh)^2 Production. Heating Shindig Amount of energy needed to change a given substance a given temperature depends on; Amount.
Chapter 19 Chemical Thermodynamics Lecture Presentation John D. Bookstaver St. Charles Community College Cottleville, MO © 2012 Pearson Education, Inc.
Chemical Thermodynamics Chapter 17 Chemical Thermodynamics.
1 Chemical Reaction - Observation Reaction (1) CH 4 + 2O 2  CO 2 + 2H 2 O Reaction (2) CH 4 + CO 2  2CO + 2H 2 When carrying out these reactions we.
Chapter 18 – Rates of Reactions and Equilibrium Every biological and non-biological chemical reaction in nature eventually reaches a state called equilibrium.
Solution thermodynamics theory—Part I
Characteristic functions. Thermodynamics of chemical equilibrium
Chemical Equilibrium By Doba Jackson, Ph.D.. Outline of Chpt 5 Gibbs Energy and Helmholtz Energy Gibbs energy of a reaction mixture (Chemical Potential)
Enthalpy, Entropy, and Spontaneity Explained. Review of Enthalpy Change.
Solution thermodynamics theory—Part IV
Thermodynamics, pt 2 Dr. Harris Lecture 22 (Ch 23) 11/19/12
Chapter 20 Energy and Disorder.
THERMOCHEMISTRY ENERGY CHANGES ASSOCIATED WITH CHEMICAL REACTION.
42C.1 Non-Ideal Solutions This development is patterned after that found in Molecular Themodynamics by D. A. McQuarrie and John D. Simon. Consider a molecular.
Solution thermodynamics theory
Thermodynamics and the Phase Rule
G EOL 2312 I GNEOUS AND M ETAMORPHIC P ETROLOGY Lecture 4 Introduction to Thermodynamics Jan. 27, 2016.
Chapter 7: Equilibrium and Stability in One-Component Systems
Chemical Thermodynamics BLB 11 th Chapter 19. Chemical Reactions 1. How fast will the reaction occur? Ch How far toward completion will the reaction.
Chemical Thermodynamics  2009, Prentice-Hall, Inc. First Law of Thermodynamics You will recall that energy cannot be created nor destroyed. Therefore,
Thermodynamics (the other part) Topic 19 in Red Book Chapter 16 in textbook.
Energy Changes in Chemical Reactions -- Chapter First Law of Thermodynamics (Conservation of energy)  E = q + w where, q = heat absorbed by system.
If I spend more than 45 minutes on it, you have permission to take a nap.
Chapter 19 Spontaneity, entropy and free energy (rev. 11/09/08)
Solution thermodynamics theory—Part III
1 Vanessa N. Prasad-Permaul Valencia College CHM 1046.
 Course number: 527 M1700  Designation: Graduate course  Instructor: Chao-Sung Lin, MSE Dept., (office), (lab)  Office hours: 2 ~
Thermodynamics and the Phase Rule
PHYSICAL CHEMISTRY ERT 108 Semester II 2011/2012
Thermodynamics and the Phase Rule
Solution of Thermodynamics: Theory and applications
Figure 6.2 Comparison among the Debye heat capacity, the Einstein heat capacity, and the actual heat capacity of aluminum.
Entropy and Free Energy
Natural systems tend toward states of minimum energy
BASIC THERMODYNAMIC PRINCIPLES
Natural systems tend toward states of minimum energy
Presentation transcript:

Chemical Engineering Thermodynamics-II Topic: Excess Gibbs Free Energy, Data Reduction, Thermodynamic Consistency Prepatred by:- Patel Nirav ( ) Patel Parth( ) Patel Prajesh ( ) Patel Rishi ( ) Patel Ronak ( ) PREPARED BY : DR. M S BHAKHAR PROF. HARESH K DAVE G H PATEL COLLEGE OF ENGINEERING AND TECHNOLOGY

Gibbs Free Energy  Gibbs free energy is a measure of chemical energy All chemical systems tend naturally toward states of minimum Gibbs free energy The gibbs free energy is defined as G = H - TS Where: G = Gibbs Free Energy H = Enthalpy (heat content) T = Temperature in Kelvins S = Entropy (can think of as randomness)

Products and reactants are in equilibrium when their Gibbs free energies are equal A chemical reaction will proceed in the direction of lower Gibbs free energy (i.e.,  G r < 0) The reaction won’t proceed if the reaction produces an increase in Gibbs free energy Gibbs Free Energy

Cont…  For a phase we can determine V, T, P, etc., but not G or H We can only determine changes in G or H as we change some other parameters of the system Example: measure  H for a reaction by calorimeter - the heat given off or absorbed as a reaction proceeds

Cont…  Arbitrary reference state and assign an equally arbitrary value of H to it: Choose K/25°C and 0.1 MPa/1 atm/1 bar (lab conditions)...and assign H = 0 for pure elements (in their natural state - gas, liquid, solid) at that reference

Cont… In our calorimeter we can then determine  H for the reaction: Si (metal) + O 2 (gas) = SiO 2  H = -910,648 J/mol = molar enthalpy of formation of quartz (at 25°C, 1 atm) It serves quite well for a standard value of H for the phase Entropy has a more universal reference state: entropy of every substance = 0 at 0K, so we use that (and adjust for temperature) Then we can use G = H - TS to determine G for quartz = -856,288 J/mol

Cont… K=equilibrium constant at standard T T in kelvin K R=gas constant=1.987 cal/mol o

Example: What is the  G o R of calcite dissociation? Use data in appendix B for  G o f  G o R = [(-132.3)+( )] - [(-269.9)] = kcal (+) means that the reaction goes from right to left so K must be small What is the value of K? K = 10 (-11.43/1.364) = = x CaCO 3 Ca 2+ + CO 3 2-

What if T  25 o C? Use the Van’t Hoff Equation Enthalpy of reaction R=1.987 cal/mol° T in Kelvin  G° r =  H° r -T  S° r and lnK T - lnK T° = (-  H° r /R)(1/T-1/T°) We can derive:

Example: What is K T of calcite dissociation at T=38°C? = [( )+(-161.8)] - [( )] = When T increases, K decreases (K T° = x )

Cont… G is a measure of relative chemical stability for a phase We can determine G for any phase by measuring H and S for the reaction creating the phase from the elements We can then determine G at any T and P mathematically Most accurate if know how V and S vary with P and T dV/dP is the coefficient of isothermal compressibility dS/dT is the heat capacity (Cp)

Excess properties The most important excess function is the excess Gibbs free energy G E Excess entropy can be calculated from the derivative of G E wrt T Excess volume can be calculated from the derivative of G E wrt P And we also define partial molar excess properties

Excess gibbs free enerrgy 

Activity coefficient  The activity coefficient of component i is found by differentiation of the excess Gibbs energy towards x i. This yields, when applied only to the first term and using the Gibbs–Duhem equation,Gibbs–Duhem equation In here A 12 and A 21 are constants which are equal to the logarithm of the limiting activit coefficients: and respectively. When, which implies molecules of same molecular size but different polarity, the equations reduce to the one-parameter Margules activity model:

Example of data reduction  The following is a set of VLE data for the system methanol(1)/water(2) at K P/kPax1y1P/kPax1y

Find parameter values for the Margules equation that give the best fit of G E /RT to the data, and prepare a P x y diagram that compares the experimental points with Curves determined from the correlation 1) Calculate EXPERIMENTAL values of activity coefficients  1 and  2 and G E

We have shown that:

Now we have our analytical model Lets calculate ln  1, ln  2, G E /x 1 x 2 RT, and:

RMS= SQRT (  (P i -P i calc ) 2 /n = kPa

Thermodynamic consistency  We need to check that the experimentally obtained activity coefficients satisfy the Gibbs-Duhem equation of P-x ₁ -y ₁ data.  If the experimental data are inconsistent with the G-D equation, they are not correct

Consistency test

Solid lines are the result of data reduction adjusting G E /RT

THANK YOU