Study of Excess Gibbs Energy for a Lattice Solution by Random Number Simulation

Σχετικά έγγραφα
Θερμοδυναμική - Εργαστήριο

VBA Microsoft Excel. J. Comput. Chem. Jpn., Vol. 5, No. 1, pp (2006)

High order interpolation function for surface contact problem

By R.L. Snyder (Revised March 24, 2005)

Θερμοδυναμική - Εργαστήριο

P É Ô Ô² 1,2,.. Ò± 1,.. ±μ 1,. ƒ. ±μ μ 1,.Š. ±μ μ 1, ˆ.. Ê Ò 1,.. Ê Ò 1 Œˆ ˆŸ. ² μ Ê ² μ Ì μ ÉÓ. É μ ±, Ì μé μ Ò É μ Ò ² μ Ö

Vol. 38 No Journal of Jiangxi Normal University Natural Science Nov. 2014

difluoroboranyls derived from amides carrying donor group Supporting Information

DuPont Suva 95 Refrigerant

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee

DuPont Suva. DuPont. Thermodynamic Properties of. Refrigerant (R-410A) Technical Information. refrigerants T-410A ENG

APPENDICES APPENDIX A. STATISTICAL TABLES AND CHARTS 651 APPENDIX B. BIBLIOGRAPHY 677 APPENDIX C. ANSWERS TO SELECTED EXERCISES 679

Θερμοδυναμική - Εργαστήριο

Studies on the Binding Mechanism of Several Antibiotics and Human Serum Albumin

Technical Information T-9100 SI. Suva. refrigerants. Thermodynamic Properties of. Suva Refrigerant [R-410A (50/50)]

An experimental and theoretical study of the gas phase kinetics of atomic chlorine reactions with CH 3 NH 2, (CH 3 ) 2 NH, and (CH 3 ) 3 N

Solubility Modelling and Mixing Thermodynamics of Thiamphenicol in Water and Twelve Neat Organic Solvents from T = ( to 318.

Supporting Information for: electron ligands: Complex formation, oxidation and

5.4 The Poisson Distribution.

Supporting Information To. Microhydration of caesium compounds: Journal of Molecular Modeling

ES440/ES911: CFD. Chapter 5. Solution of Linear Equation Systems

Selecting Critical Properties of Terpenes and Terpenoids through Group-Contribution Methods and Equations of State

DuPont Suva 95 Refrigerant

Prey-Taxis Holling-Tanner

Electronic structure and spectroscopy of HBr and HBr +

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

Web-based supplementary materials for Bayesian Quantile Regression for Ordinal Longitudinal Data

Supporting Information

NonEquilibrium Thermodynamics of Flowing Systems: 2

Design Method of Ball Mill by Discrete Element Method

Major Concepts. Multiphase Equilibrium Stability Applications to Phase Equilibrium. Two-Phase Coexistence

Table of Contents 1 Supplementary Data MCD

8Q5SAC) 8Q5SAC UV2Vis 8500 ( ) ; PHS23C ) ;721 ( ) :1 4. ;8Q5SAC : molπl ;Britton2Robinson Q5SAC BSA Britton2Robinson,

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review

Buried Markov Model Pairwise

Αξιολόγηση Ημιαγώγιμων Υμενίων Σεληνιούχου Καδμίου Σε Υπόστρωμα Νικελίου Για Φωτοβολταϊκές Εφαρμογές

ELECTRONIC SUPPORTING INFORMATION

,,, (, ) , ;,,, ; -

Multifunctinality and Crystal Dynamics of Highly Stable Porous Metal-Organic Framework [Zn 4 O(NTB) 2 ]

ΜΔΛΔΣΖ ΔΝΓΟΣΡΑΥΤΝΖ Δ ΥΑΛΤΒΔ ΘΔΡΜΖ ΔΛΑΖ

Supplementary Appendix

Partial Differential Equations in Biology The boundary element method. March 26, 2013

CE 530 Molecular Simulation

Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. Supplementary to Theoretical Study on the Gas Adsorption Capacity and

LUO, Hong2Qun LIU, Shao2Pu Ξ LI, Nian2Bing

Applying Markov Decision Processes to Role-playing Game

Pyrrolo[2,3-d:5,4-d']bisthiazoles: Alternate Synthetic Routes and a Comparative Study to Analogous Fused-ring Bithiophenes

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

EE512: Error Control Coding

Θερμοδυναμική - Εργαστήριο

Supporting Information. Partial thioamide scan on the lipopeptaibiotic trichogin GA IV. Effects on


Correction of chromatic aberration for human eyes with diffractive-refractive hybrid elements

: Ω F F 0 t T P F 0 t T F 0 P Q. Merton 1974 XT T X T XT. T t. V t t X d T = XT [V t/t ]. τ 0 < τ < X d T = XT I {V τ T } δt XT I {V τ<t } I A

2.1

Supplementary Materials for. Kinetic and Computational Studies on Pd(I) Dimer- Mediated Halogen Exchange of Aryl Iodides

Research on Economics and Management

: Monte Carlo EM 313, Louis (1982) EM, EM Newton-Raphson, /. EM, 2 Monte Carlo EM Newton-Raphson, Monte Carlo EM, Monte Carlo EM, /. 3, Monte Carlo EM

ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΥΠΡΟΥ ΣΧΟΛΗ ΓΕΩΠΟΝΙΚΩΝ ΕΠΙΣΤΗΜΩΝ ΒΙΟΤΕΧΝΟΛΟΓΙΑΣ ΚΑΙ ΕΠΙΣΤΗΜΗΣ ΤΡΟΦΙΜΩΝ. Πτυχιακή εργασία

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

Calculating the propagation delay of coaxial cable

Αρχές Κβαντικής Χημείας και Φασματοσκοπίας

Homework 3 Solutions

Solutions to Exercise Sheet 5

Engineering Tunable Single and Dual Optical. Emission from Ru(II)-Polypyridyl Complexes. Through Excited State Design

Copper-catalyzed formal O-H insertion reaction of α-diazo-1,3-dicarb- onyl compounds to carboxylic acids with the assistance of isocyanide

Mean bond enthalpy Standard enthalpy of formation Bond N H N N N N H O O O

Pseudo-compressibility 방법에서이상유동해석을위한 Level Set 방법의적용 Level Set Method Applied on Pseudo-compressibility Method for the Analysis of Two-phase Flow

Fused Bis-Benzothiadiazoles as Electron Acceptors

Optimizing Microwave-assisted Extraction Process for Paprika Red Pigments Using Response Surface Methodology

Aquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET

Supporting Information

FORMULAS FOR STATISTICS 1

Electronic Supplementary Information DFT Characterization on the Mechanism of Water Splitting Catalyzed by Single-Ru-substituted Polyoxometalates

Higher Derivative Gravity Theories

Supplementary Information

Novel electroluminescent donor-acceptors based on dibenzo[a,c]phenazine as

ST5224: Advanced Statistical Theory II

Αρχές Κβαντικής Χημείας και Φασματοσκοπίας

ADVANCED STRUCTURAL MECHANICS

Matrices and Determinants

Quantum dot sensitized solar cells with efficiency over 12% based on tetraethyl orthosilicate additive in polysulfide electrolyte

Thermodynamics of the motility-induced phase separation

2 ~ 8 Hz Hz. Blondet 1 Trombetti 2-4 Symans 5. = - M p. M p. s 2 x p. s 2 x t x t. + C p. sx p. + K p. x p. C p. s 2. x tp x t.

Study on the Strengthen Method of Masonry Structure by Steel Truss for Collapse Prevention

Supplementary Materials for Evolutionary Multiobjective Optimization Based Multimodal Optimization: Fitness Landscape Approximation and Peak Detection

Numerical Analysis FMN011

Η ΕΠΙΔΡΑΣΗ ΤΗΣ ΑΙΘΑΝΟΛΗΣ,ΤΗΣ ΜΕΘΑΝΟΛΗΣ ΚΑΙ ΤΟΥ ΑΙΘΥΛΟΤΡΙΤΟΤΑΓΗ ΒΟΥΤΥΛΑΙΘΕΡΑ ΣΤΙΣ ΙΔΙΟΤΗΤΕΣ ΤΗΣ ΒΕΝΖΙΝΗΣ

ΖΩΝΟΠΟΙΗΣΗ ΤΗΣ ΚΑΤΟΛΙΣΘΗΤΙΚΗΣ ΕΠΙΚΙΝΔΥΝΟΤΗΤΑΣ ΣΤΟ ΟΡΟΣ ΠΗΛΙΟ ΜΕ ΤΗ ΣΥΜΒΟΛΗ ΔΕΔΟΜΕΝΩΝ ΣΥΜΒΟΛΟΜΕΤΡΙΑΣ ΜΟΝΙΜΩΝ ΣΚΕΔΑΣΤΩΝ

Homomorphism in Intuitionistic Fuzzy Automata

Enhancing σ/π-type Copper(I) thiophene Interactions by Metal Doping (Metal = Li, Na, K, Ca, Sc)

J. of Math. (PRC) 6 n (nt ) + n V = 0, (1.1) n t + div. div(n T ) = n τ (T L(x) T ), (1.2) n)xx (nt ) x + nv x = J 0, (1.4) n. 6 n

1 h, , CaCl 2. pelamis) 58.1%, (Headspace solid -phase microextraction and gas chromatography -mass spectrometry,hs -SPME - Vol. 15 No.

ΑΛΚΑΛΟΕΙΔΩΝ ΘΡΥΠΤΟΦΑΝΗΣ ΑΛΕΞΑΝΔΡΟΣ Λ. ΖΩΓΡΑΦΟΣ

ΠΟΛΥΤΕΧΝΕΙΟ ΚΡΗΤΗΣ ΣΧΟΛΗ ΜΗΧΑΝΙΚΩΝ ΠΕΡΙΒΑΛΛΟΝΤΟΣ

A facile and general route to 3-((trifluoromethyl)thio)benzofurans and 3-((trifluoromethyl)thio)benzothiophenes

Approximation of distance between locations on earth given by latitude and longitude

[2] T.S.G. Peiris and R.O. Thattil, An Alternative Model to Estimate Solar Radiation

J. of Math. (PRC) Banach, , X = N(T ) R(T + ), Y = R(T ) N(T + ). Vol. 37 ( 2017 ) No. 5

Transcript:

Journal of the Korean Chemical Society 007, Vol. 5, o. 4 Printed in the Republic of Korea ù x mw ½ w š w * w yw (007. 5. Study of Excess Gibbs Energy for a Lattice Solution by Random umber Simulation Hae-Young Jung* Department of Chemistry, DukSung Women's University, Seoul 3-74, Korea (Received May, 007. ù x ww w w s y w ³ s w. s l yw ½ G E w w. w -» sx w š» w. : yw, ½, ABSTRACT. Performing random number simulations, we approximated that the distribution of the number of ways for arranging molecules randomly on a lattice is a normal distributon for, the number of interactions between the nearest neighbors of different molecules. From this distribution, an approximate equation of the excess Gibbs energy G E for a lattice solution of nonrandom mixing was derived. Using the equation, liquid-vapor equilibria of several binary solutions were calculated and compared with the calculated result of other equations. Keywords: onrandom Mixing, Excess Gibbs Energy, Lattice w w w» w cell, hole, free volume (lattice. p wƒ w ƒ w x s š. yw w, w yw w w š. ù y w ywz w t wùƒ quasi-chemical. ƒ ywsx ƒ ¾ quasi-chemical š. k w 3, Wilson 4 w -» sx x w š. z Wilson UIQUAC 3 œw w ù ywz yw wš w. ù» w 5ƒ w w x ww. w w 3

s y w ³ s w š, y w ½ G E w w. w 0ƒ -» w sx w š, Redlich- Kister, Van Laar, Wilson 3 w. ù x mw s x ù» mw ù w - - + w. x, s,,, 5ƒ w x. ƒ z, 4, 6, 8,. x w yw wƒ ù w x sw g. x j w yw y w - - y w. 5 ù x mw ½ w š 33 Fig.. Probability distribution of X/ from 0 6 trials when x =0.3, =0648 for a cubic lattice. HX!! ( -------------------------------------------------! ---------------------- ; X = = ------- ( ( X! ( X!X! ( +! ( y s»w s w w X w s³ t r. 6 s³ X = -----------; = + ( Fig.. σ X/, X/ vs x from 0 6 trials when =0648 for a cubic lattice. t r ------------------ ----------- (3 σ X = X ----- x (4 x 0000~80000, - x = / 0., 0., 0.3, 0.4, 0.5 w ww. w wz 0 6 w. Fig. ƒ j, X w y s ³ s w, t ƒ j s w 6 w ³ s w w. š Fig. X s³ r, x ƒ w. σ X ----- x (5 x mw (4, (5 Table,. Table, Linear, Square, Cubic, BCC, FCC ƒƒ x, s,,, ù kü x wš. Table, x w yw (, (3 mw (4, (5 ù 007, Vol. 5, o. 4

34 w Table. Slope of < X/ > vs x for 5 different lattice structures Linear Square Cubic BCC FCC 0000.00008.0000 3.0008 4.0004 6.00057 0000.00004.0000 3.0005 4.0008 6.0003 40000.0000.00005 3.00008 4.0000 6.0004 80000.00000.00003 3.00004 4.00005 6.00008 in the st column are approximate values except for a linear lattice Table. Slope of σx/ vs x for 5 different lattice structures Linear Square Cubic BCC FCC 0000.00003.446.7330.99870.44947 0000.0008.4365.73.0000.44845 40000 0.99954.446.7339.99907.44864 80000.000.437.7370.99986.450 average 0.99997.4406.7385.9994.4490 deviation 0.0009 0.00046 0.0009 0.00063 0.0008 in the st column are approximate values except for a linear lattice w ƒƒ z/, z., f w X y s s³ r ³ s w. z X = ----- x x σ X = z -----x x (6 (7 (6, (7 j w y s ù w z w š. ³ s w ½ G E X w y s ³ s w» w., w Ω. ( Ω(,, X +! ---------------------- --------------- exp!! πσ -- X X --------------- σ X X (8 w m w w Q. 5 Q Ω,, X βe ( e ( X = ; β = ----- kt { X} (9 (9 E(X -i,j y εij w t. (0 ( Q (9 w w. 5 ( X * w X. (8, (0, (3 l (8, (, (4 l EX ( = β εx + βz ----- ( ε + ε ε + ε ε = ε -----------------; ε ij < 0 ( Q Ω(,, X * e βex* ----- [ ln Ω(,, X βex ( ] = 0 X X * = X β εσ X ( (3 (4 ( lnq +! ln---------------------- ln( πσ X β ε X β ε = + σ X!! βz ----- ( ε + ε (5 Journal of the Korean Chemical Society

, ƒ j (5 w. lnq lnx lnx β ε X β ε + σ X (6 (6, (7 w w 007, Vol. 5, o. 4 ù x mw ½ w š 35 (6 (7 yw v y Vmix wš m w œ 3 w (7 l yw½ Gmix G E t. (8, (9 βz ----- ( ε + ε lnq -------- x lnx x lnx zβ εx x ( β εx x zβ ----- ( ε + ε G ------------- mix = x lnx + x lnx + x x ( A Bx x G E ------ = x x ( A Bx x A = zβ ε, B = zβ ε = A z (8 (9 (0 (0 z š j (9 -. B yw ùkù z ùkü w. š (9 3- Redlich-Kister B'=0 w. G E ------ = x x [ A + B ( x x + C ( x x ] ( (9 x =0.5 w e ùkü j», š». x, j» š w ( w» w. r φ = ------------------------- = ---------------- ; r = --- r + r x + rx r ( ( r, r š w Flory- x r Huggins 7 š - ¼ ùkü j», š w x ƒ š. (9, ( l G E ------ = φ φ ( A Bφ φ, B = A z (3 (3 z A, r. A, B yw w z ùkü, r j», w z ùkü w. (3 (8 l A, B ƒƒ x ƒw A, B, r 3- w ww š. CH 3O +CCl 48, EtOH +chloroform 9, MeOH+benzene 0, benzene+methylcyclohexane, cyclohexane +toluene, cyclopentane+benzene, propanol+benzene, EtOH+benzene, methylcyclopentane+benzene, methylcyclopentane+toluene 0ƒ w sx w. (3 sw w Redlich-Kister, Van Laar, Wilson w. Redlich-Kister, Van Laar, Wilson w š x 3. š ƒ ùkù yw» w» w x s³s (4 y j Barker 3 w. P = data i = ( P i P calc ---------------------------------- data (4 (4» Pcalc w w. P calc = γ x P + γ x P (5 γ, γ y ½ G l E. 3 (5

36 w Table 3. relative error % in vapor pressure calculated for 0 binary mixtures RK- RK-3 Eqn.(3 Eqn.(3-B Van Laar Wilson CH 3O +CCl 4 at 45 C.34 0.48.5 0.3.30 0.44 EtOH+chloroform at 35,45,55 C.03..5.7.66.97 MeOH+benzene at 35,55 C 3.7.03.46.89.78.68 benzene+methylcyclohexane at atm 0.5 0.5 0.7 0.6 0.8 0.8 cyclohexane+toluene at atm 0.9 0.8 0.9 0.8 0.9 0.9 cyclopentane+benzene at atm 0.38 0.7 0.39 0.8 0.38 0.38 propanol+benzene at atm.30 0.86.5 0.96.6.08 EtOH+benzene at atm.66.9.4 0.79.55 0.87 methylcyclopentane+benzene at atm 0. 0.09 0.3 0.09 0. 0. methylcyclopentane+toluene at atm 0.40 0.40 0.40 0.40 0.40 0.40 average [%].08 0.69 0.94 0.64.09 0.74 Table 4. y calculated for 0 binary mixtures RK- RK-3 Eqn.(3 Eqn.(3-B Van Laar Wilson CH 3O +CCl 4 at 45 C 0.048 0.0 0.09 0.09 0.045 0.0 EtOH+chloroform at 35,45,55 C 0.0064 0.008 0.03 0.0094 0.03 0.045 MeOH+benzene at 35,55 C 0.055 0.039 0.083 0.06 0.08 0.0 benzene+methylcyclohexane at atm 0.0040 0.0039 0.004 0.0039 0.004 0.004 cyclohexane+toluene at atm 0.0044 0.0043 0.0044 0.0043 0.0044 0.0044 cyclopentane+benzene at atm 0.005 0.008 0.005 0.008 0.005 0.005 propanol+benzene at atm 0.000 0.007 0.0088 0.0076 0.0097 0.008 EtOH+benzene at atm 0.058 0.008 0.0 0.0077 0.03 0.0049 methylcyclopentane+benzene at atm 0.007 0.006 0.008 0.006 0.007 0.007 methylcyclopentane+toluene at atm 0.004 0.004 0.004 0.004 0.004 0.004 average of y 0.0090 0.0067 0.0080 0.0067 0.0090 0.0069 P P P s exp v s ( B ( P calc P P calc δ y = -------------------------------------------------------------------------- P s exp v s ( B ( P calc P P calc δ y = -------------------------------------------------------------------------- δ = B B B (6 (7 (6 v, v v modified Rackett 4 w, P s, P s ƒ s x» š x 4. B, B, B ƒ Hayden O Connell 5 w y v w š x 6. Table 3, 4 ùkü. Table 3» w %, Table 4» w s³s yƒ. Table 3, 4 RK-, RK-3 ƒƒ ƒ, 3 Redlich-Kister ùkü Eqn. (3-B (3 B w 3 w ùkü. Table 3, 4 3 w (3 ƒ š, (3 Redlich-Kister š. w Wilson ƒ š. ù x ww w s w ³ s w. l yw ½ G E w x œ w, ùkù Journal of the Korean Chemical Society

3 ƒƒ, yw, j» z ùkü ƒ š.» Redlich- Kister. w p y w z š w š w ƒ. 006 w ü w. x ù x mw ½ w š 37. Hirschfelder, J.G O.; Curtiss, C.G F.;G Bird, R.G B. The Molecular Theory of Gases and Liquids; John Wiley & Sons, 954.. Guggenheim, E.GA. Mixtures; Clarendon Press, Oxford, 95. 3. Prausnitz, J. M.; Lichtenthaler, R..; de Azevedo, E. G. Molecular Thermodynamics of Fluid-Phase Equilibria, nd Ed.; Prentice-Hall, 986. 4. Wilson, J. M. J. Am. Chem. Soc. 964, 86, 7. 5. Hill, T. L. An Introduction to Statistical Thermodynamics; Dover Publications, 987. 6. Mendenhall, W.; Sincich, T. Statistics for Engineering and the Sciences, 4th Ed.; Prentice-Hall, 995. 7. Flory, P. J. Principles of Polymer Chemistry; Cornell Univ. Press, 953. 8. Brown, I; Smith, F. Aust. J. Chem. 957, 0, 43. 9. Scatchard, G.; Raymond, C. J. Am. Chem. Soc. 938, 60, 79. 0. Scatchard, G.; Wood, S.; Mochel, J. J. Am. Chem. Soc. 946, 68, 957.. Myers, H. S. Ind. Eng. Chem. 956, 48, 04.. Wehe, A.; Coates, J. AICHE J. 955,, 4. 3. Barker, J. A. Aust. J. Chem. 953, 6, 07. 4. Reid, R. C.; Prausnitz, J. M.; Sherwood, T. K. The Properties of Gases and Liquids, 4th Ed.; McGraw- Hill, 988. 5. Hayden, J. G.; O Connell, J. P. Ind. Eng. Chem., Process Des. Dev. 975, 4, 09. 6. Prausnitz, J. M. et al. Computer calculations for multicomponent vapor-liquid and liquid-liquid equilibria; Prentice-Hall, 980. 007, Vol. 5, o. 4