Co-current cascade of ideal stages Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.

Slides:



Advertisements
Similar presentations
ORDINARY DIFFERENTIAL EQUATIONS (ODE)
Advertisements

Conversion and Reactor Sizing
1111 Chemistry 132 NT I never let my schooling get in the way of my education. Mark Twain.
Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik Schemes for absorbent recovery.
© 2014 Carl Lund, all rights reserved A First Course on Kinetics and Reaction Engineering Class 15.
RATIONAL AND IRRATIONAL NUMBERS
Alloy Solidification Def. Partition coefficient k
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.
Nonisothermal case: adiabatic approach Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Created by Tara L. Moore, MGCCC General Chemistry, 5 th ed. Whitten, Davis & Peck Definitions Left click your mouse to continue.
Ch. 14: Chemical Equilibrium Dr. Namphol Sinkaset Chem 201: General Chemistry II.
15.1b Equilibrium Constant, K c. created in 1864 by Guldberg and Waage (Norweigen) for a reaction: aA + bB ⇄ cC + dD equilibrium constant: K c.
Liquid-Liquid Equilibrium
03 Nov 2011Prof. R. Shanthini1 Course content of Mass transfer section LTA Diffusion Theory of interface mass transfer Mass transfer coefficients, overall.
Cross-current cascade of ideal stages Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
ERT 313 BIOSEPARATION ENGINEERING EXTRACTION
17 Chemical Equilibrium.
Chapter 14-Part VII Applications of VLLE.
Stripping process design Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik Nonisothermal case: temperature profile in the column.
CHEN 4470 – Process Design Practice Dr. Mario Richard Eden Department of Chemical Engineering Auburn University Lecture No. 3 – Overview of Mass Exchange.
Comparison between co-, cross- and counter-current Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Counter-current cascade of ideal stages Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
 For a non-ideal system, where the molar latent heat is no longer constant and where there is a substantial heat of mixing, the calculations become much.
Representation on the x-y plane Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Process design for multisolute absorption Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Absorption process design Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Simulation Approach Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Chemical Equilibrium Introduction to Chemical Equilibrium Equilibrium Constants and Expressions Calculations Involving Equilibrium Constants Using.
Sample Exercise 15.7 Calculating K When All Equilibrium Concentrations Are Known After a mixture of hydrogen and nitrogen gases in a reaction vessel is.
Solution Thermodynamic:
FLASH CALCULATION A flash is a single-equilibrium stage distillation in witch a feed is partially vaporized to give a vapor richer in the most volatile.
ERT 313 BIOSEPARATION ENGINEERING EXTRACTION
24 Nov 2011Prof. R. Shanthini1 Course content of Mass transfer section LTA Diffusion Theory of interface mass transfer Mass transfer coefficients, overall.
Converting Rational Numbers to Fractions
Notation convention Let G' stand for total free energy and in a similar fashion S', V', H', etc. Then we will let = G'/n represent the free energy per.
31.1 Thermodynamics of Mixing of Ideal Solutions For the process where solute and solvent are mixed to form an ideal solution at constant temperature and.
Dr Saad Al-ShahraniChE 334: Separation Processes Absorption of Dilute Mixtures  Graphical Equilibrium Stage Method for Trayed Tower  Consider the countercurrent-flow,
LIAL HORNSBY SCHNEIDER
Section 8.3—Reaction Quotient
Sec. 9-4: Rational Expressions. 1.Rational Expressions: Expressions (NOT equations that involve FRACTIONS). We will be reducing these expressions NOT.
Chapter 11: Other Types of Phase Equilibria in Fluid Mixtures (selected topics)
VAPOR/LIQUID EQUILIBRIUM- Introduction
© 2014 Carl Lund, all rights reserved A First Course on Kinetics and Reaction Engineering Class 13.
31 Polyelectrolyte Chains at Finite Concentrations Counterion Condensation N=187, f=1/3,  LJ =1.5, u=3 c  3 = c  3 =
THERMODYNAMICS OF SEPARATION OPERATIONS
Partial Molar Quantities and the Chemical Potential Lecture 6.
1 Chapter 7. Applications of the Second Law. 2 Consider entropy changes in various reversible (!!!) processes We have: (a) Adiabatic process Hence a reversible.
20 Oct 2011Prof. R. Shanthini1 Course content of Mass transfer section LTA Diffusion Theory of interface mass transfer Mass transfer coefficients, overall.
- Equilibrium Constant - 1.  Please READ pp. 439 – 440  Equilibrium constant (K eq ) is the value obtained from the mathematical combination of equilibrium.
Chapter 13.  Equilibrium is not static. It is a highly dynamic state.  Macro level reaction appears to have stopped  Molecular level frantic activity.
Liquid-Liquid Extraction
Introduction We have seen how to Integrate in C1 In C2 we start to use Integration, to work out areas below curves It is increasingly important in this.
Template by Bill Arcuri, WCSD Click Once to Begin JEOPARDY! Chemistry Final Review Chapter 8: Equilibrium.
ACTIVITY AND ACTIVITY COEFFICIENT
SECONDARY ONE 6.1a Using Substitution to Solve a System.
SOLVING TWO VARIABLE EQUATIONS Brittney. Methods ◦ Graphing ◦ Slope intercept y=mx+b ◦ Standard form Ax+By=C ◦ Substitution ◦ Solve for one variable then.
1 Chemical Equilibrium Chapter 14 Henri L. le Chatlier Adapted thermodynamics to equilibria; formulated the principle known by his name.
Section 8.2—Equilibrium Constant How can we describe a reaction at equilibrium?
Absorption design with nonlinear equilibrium Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Absorption design with real stages Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik.
Identify direct and inverse variation EXAMPLE 1 Tell whether the equation represents direct variation, inverse variation, or neither. a. xy = 4 SOLUTION.
Equilibrium Constant in terms of pressure, Heterogeneous Equilibria, and the Reaction Quotient.
SHROFF S.R. ROTARY INSTITUTE OF CHEMICAL TECHNOLOGY
Students: Amiran Divekar ( ) Ameedhara Hingrajiya ( ) Priyal Parikh ( ) Sal College of engineering Department of Chemical.
CHEM171 – Lecture Series Two : 2012/01 PHASE CHEMISTRY AND COLLIGATIVE PROPERTIES  Phase Diagrams  Solutions  Solution Concentrations  Colligative.
Gibbs-Duhem and the Chemical Potential of Ideal Solutions
Single equilibrium stage
Section 8.2—Equilibrium Constant
The Lever Rule.
Presentation transcript:

Co-current cascade of ideal stages Prof. Dr. Marco Mazzotti - Institut für Verfahrenstechnik

1 G, y 0 L, x 0 y0y0 x0x0 y = m x y x Let’s consider two ideal stages. The solvent is put in contact with the gas phase in the first stage. The solvent can be pure or can have a certain concentration of solute, represented by x o. The equilibrium between phases can be represented in a x-y diagram for a given temperature and pressure. Let’s consider again that it is a straight line, y = m x. The inlet compositions of the two phases can be represented in the diagram 2

The content of solute in the gas is now lower than at the entrance: y 1 < y 0 The solvent is now charged in solute, so that x 1 > x o. Repeating what we saw before in the case of ideal single stage, the change on composition in the two phases can be represented on the diagram... The equation is: The slope of the operating line is then (-L/G) y x y0y0 x0x0 1 G, y 0 L, x 0 y1y1 x1x1 2 Because this is an ideal equilibrium stage, the equilibrium between phases is reached. -L/G y1y1 x1x1

1 G, y 0 L, x 0 y1y1 x1x1 2 y2y2 x2x2 y x y0y0 x0x0 -L/G  y1y1 x1x1 In the single ideal stage we have derived the next equation for y 1 : Where A is the absorption factor. Now we have a second ideal stage, in which the gas composition at the outlet can be expressed by analogy: You find the derivation of these equations in the next slide

Material Balance to the solute: The equilibrium equation: Dividing by G: Using the equilibrium equation, x 1 can be expressed as y 1 /m: Where we find the Absorption factor: Multiplying and dividing by m in the first term: And finally, we obtain the composition at the outlet of the first stage: Derivation of the outlet composition of the gas The next outlet compositions can be calculated by analogy as...

1 G, y 0 L, x 0 y1y1 x1x1 2 y2y2 x2x2 y x y0y0 x0x0 -L/G  y1y1 x1x1 The aim of the second stage is to have y 2 smaller than y 1, so that we improve the operation by decreasing the gas concentration of pollutant. But we already know that the equilibrium line represents a barrier and determines a region of values (x, y) that cannot be reached for any ratio (L/G) and any number of stages... Since in the first stage we have already arrived to the equilibrium, we cannot go further and y 2 must be equal to y 1. y 2 = = x 2

y x y0y0 x0x0 -L/G  y1y1 x1x1 This result can be obtained looking at the equations... Since the equilibrium is reached... Y 2 = = x 2 So in the equation of y 2, we get: Thus, as we have already deduced: 1 G, y 0 L, x 0 y1y1 x1x1 2 y2y2 x2x2

The composition equation for the last stage can be written as follows: And then, the fractional absorption...