Phase Equilibrium and Solutions
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Physical Model for Vaporization
Physical model for vaporization Jozsef Garai Department of Mechanical and Materials Engineering, Florida International University, University Park, VH 183, Miami, FL 33199 Abstract Based on two assumptions, the surface layer is flexible, and the internal energy of the latent heat of vaporization is completely utilized by the atoms for overcoming on the surface resistance of the liquid, the enthalpy of vaporization was calculated for 45 elements. The theoretical values were tested against experiments with positive result. 1. Introduction The enthalpy of vaporization is an extremely important physical process with many applications to physics, chemistry, and biology. Thermodynamic defines the enthalpy of vaporization ()∆ v H as the energy that has to be supplied to the system in order to complete the liquid-vapor phase transformation. The energy is absorbed at constant pressure and temperature. The absorbed energy not only increases the internal energy of the system (U) but also used for the external work of the expansion (w). The enthalpy of vaporization is then ∆ v H = ∆ v U + ∆ v w (1) The work of the expansion at vaporization is ∆ vw = P ()VV − VL (2) where p is the pressure, VV is the volume of the vapor, and VL is the volume of the liquid. Several empirical and semi-empirical relationships are known for calculating the enthalpy of vaporization [1-16]. Even though there is no consensus on the exact physics, there is a general agreement that the surface energy must be an important part of the enthalpy of vaporization. The vaporization diminishes the surface energy of the liquid; thus this energy must be supplied to the system. -
Using the Vapor Pressure of Pure Volatile Organic Compounds to Predict the Enthalpy of Vaporization and Computing the Entropy of Vaporization
Open Access Library Journal Using the Vapor Pressure of Pure Volatile Organic Compounds to Predict the Enthalpy of Vaporization and Computing the Entropy of Vaporization Shawn M. Abernathy, Kelly R. Brown Department of Chemistry, Howard University, Washington DC, USA Email: [email protected] Received 5 September 2015; accepted 21 September 2015; published 28 September 2015 Copyright © 2015 by authors and OALib. This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/ Abstract The objective of this investigation was to develop a vapor pressure (VP) acquisition system and methodology for performing temperature-dependent VP measurements and predicting the en- thalpy of vaporization (ΔHvap) of volatile organic compounds, i.e. VOCs. High quality VP data were acquired for acetone, ethanol, and toluene. VP data were also obtained for water, which served as the system calibration standard. The empirical VP data were in excellent agreement with its ref- erence data confirming the reliability/performance of the system and methodology. The predicted values of ΔHvap for water (43.3 kJ/mol, 1.0%), acetone (31.4 kJ/mol; 3.4%), ethanol (42.0 kJ/mol; 1.0%) and toluene (35.3 kJ/mol; 5.4%) were in excellent agreement with the literature. The com- puted values of ΔSvap for water (116.0 J/mol∙K), acetone (95.2 J/mol∙K), ethanol (119.5 J/mol∙K) and toluene (92.0.J/mol∙K) compared also favorably to the literature. Keywords Vapor Pressure (VP), Enthalpy of Vaporization, Entropy of Vaporization, Volatile Organic Compounds (VOCs), Predict Subject Areas: Physical Chemistry 1. -
High Temperature Enthalpies of the Lead Halides
HIGH TEMPERATURE ENTHALPIES OF THE LEAD HALIDES: ENTHALPIES AND ENTROPIES OF FUSION APPROVED: Graduate Committee: Major Professor Committee Member Min fessor Committee Member X Committee Member UJ. Committee Member Committee Member Chairman of the Department of Chemistry Dean or the Graduate School HIGH TEMPERATURE ENTHALPIES OF THE LEAD HALIDES: ENTHALPIES AND ENTROPIES OF FUSION DISSERTATION Presented to the Graduate Council of the North Texas State University in Partial Fulfillment of the Requirements For the Degree of DOCTOR OF PHILOSOPHY By Clarence W, Linsey, B. S., M. S, Denton, Texas June, 1970 ACKNOWLEDGEMENT This dissertation is based on research conducted at the Oak Ridge National Laboratory, Oak Ridge, Tennessee, which is operated by the Uniofl Carbide Corporation for the U. S. Atomic Energy Commission. The author is also indebted to the Oak Ridge Associated Universities for the Oak Ridge Graduate Fellowship which he held during the laboratory phase. 11 TABLE OF CONTENTS Page LIST OF TABLES iv LIST OF ILLUSTRATIONS v Chapter I. INTRODUCTION . 1 Lead Fluoride Lead Chloride Lead Bromide Lead Iodide II. EXPERIMENTAL 11 Reagents Fusion-Filtration Method Encapsulation of Samples Equipment and Procedure Bunsen Ice Calorimeter Computer Programs Shomate Method Treatment of Data Near the Melting Point Solution Calorimeter Heat of Solution Calculations III. RESULTS AND DISCUSSION 41 Lead Fluoride Variation in Heat Contents of the Nichrome V Capsules Lead Chloride Lead Bromide Lead Iodide Summary BIBLIOGRAPHY ...... 98 in LIST OF TABLES Table Pa8e I. High-Temperature Enthalpy Data for Cubic PbE2 Encapsulated in Gold 42 II. High-Temperature Enthalpy Data for Cubic PbF2 Encapsulated in Molybdenum 48 III. -
Physics, Chapter 17: the Phases of Matter
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Robert Katz Publications Research Papers in Physics and Astronomy 1-1958 Physics, Chapter 17: The Phases of Matter Henry Semat City College of New York Robert Katz University of Nebraska-Lincoln, [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/physicskatz Part of the Physics Commons Semat, Henry and Katz, Robert, "Physics, Chapter 17: The Phases of Matter" (1958). Robert Katz Publications. 165. https://digitalcommons.unl.edu/physicskatz/165 This Article is brought to you for free and open access by the Research Papers in Physics and Astronomy at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Robert Katz Publications by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. 17 The Phases of Matter 17-1 Phases of a Substance A substance which has a definite chemical composition can exist in one or more phases, such as the vapor phase, the liquid phase, or the solid phase. When two or more such phases are in equilibrium at any given temperature and pressure, there are always surfaces of separation between the two phases. In the solid phase a pure substance generally exhibits a well-defined crystal structure in which the atoms or molecules of the substance are arranged in a repetitive lattice. Many substances are known to exist in several different solid phases at different conditions of temperature and pressure. These solid phases differ in their crystal structure. Thus ice is known to have six different solid phases, while sulphur has four different solid phases. -
THE ENTROPY of VAPORIZATION AS a MBANS of DIS- Tinguismg NORIKAL LIQUIDS
970 JOEL H. HILDEBRAND. iodide solution are shown to give a constant e. m. f. when measured against an unpolarizable electrode. Freshly cast rods of cadmium are shown to attain this value with time. 4. The behavior of cadmium electrodes in concentration cells is ex- plained as due to an allotropic change. 5. Crystalline electrolytic deposits of cadmium on cadmium rods or platinum are shown to give a reproducible e. m. f. when measured against an unpolarizsMe ekctrode. This e. m. f. is, however, slightly higher than that given by the gray cadmium electrodes. Amalgamated electrodes are not reproducible. 6. Photomicrographs indicate a change in crystalline form and con- firm the conclusions drawn from the e. m. f. measurements. 7. Attempts to inoculate the surface of the freshly cast cadmium with the stable rnaatian indicate that the action is extremely slow. 8. Phobmicrogtsphs indicate that in all cases the change is due to a deposit upon the surface htead of to a pitting of the surface. LHEMICALLAJJOUT~BT, BSYN MAWRCOLLBGE, BlYN MAWR. PA [CONTRIBUTION FROM THE CHEMICAL LABOBATORYOF TaS UNIVERSITY OF cALlmRNIA. I THE ENTROPY OF VAPORIZATION AS A MBANS OF DIS- TINGUISmG NORIKAL LIQUIDS. BY JOSL H. HILDSBRAND. Received February 23. 1915. In a series of studies which we are making on the theory of solutions, it has become necessary to distinguish between deviations from Raoult’s Law, whose cause may be considered physical, and those due to chemical changes. As has been pointed out it1 a previous paper,’ the choice be- tween the alternatives in a given case is possible if we know whether or not the pure liquids are associated. -
Chapter 11 Liquids, Solids, and Phase Changes
Lecture Presentation Chapter 11 Liquids, Solids, and Phase Changes 11.1, 11.2, 11.3, 11.4, 11.15, 11.17, 11.26, 11.30, 11.32, 11.40, 11.42, 11.60, 11.82, 11.116 John E. McMurry Robert C. Fay Properties of Liquids Viscosity: The measure of a liquid’s resistance to flow (higher intermolecular force, higher viscosity) Surface Tension: The resistance of a liquid to spread out and increase its surface area (forms beads) (higher intermolecular force, higher surface tension) Properties of Liquids low intermolecular force – low viscosity, low surface tension high intermolecular force – high viscosity, high surface tension HW 11.1 Properties of Liquids high intermolecular force – high viscosity, high surface tension For the following molecules which has the higher intermolecular force, viscosity and surface tension ? (LD structure, VSEPRT, dipole of molecule) (if the molecules are in the liquid state) a. CHCl3 vs CH4 b. H2O vs H2 (changed from handout) c. N Cl3 vs N H Cl2 Phase Changes between Solids, Liquids, and Gases Phase Change (State Change): A change in the physical state but not the chemical identity of a substance Fusion (melting): solid to liquid Freezing: liquid to solid Vaporization: liquid to gas Condensation: gas to liquid Sublimation: solid to gas Deposition: gas to solid Phase Changes between Solids, Liquids, and Gases Enthalpy – add heat to system Entropy – add randomness to system Phase Changes between Solids, Liquids, and Gases Heat (Enthalpy) of Fusion (DHfusion ): The amount of energy required to overcome enough intermolecular forces to convert a solid to a liquid Heat (Enthalpy) of Vaporization (DHvap): The amount of energy required to overcome enough intermolecular forces to convert a liquid to a gas HW 11.2: Phase Changes between Solids, Liquids, & Gases DHfusion solid to a liquid DHvap liquid to a gas At phase change (melting, boiling, etc) : DG = DH – TDS & D G = zero (bc 2 phases in equilibrium) DH = TDS o a. -
Corollary from the Exact Expression for Enthalpy of Vaporization
Hindawi Publishing Corporation Journal of Thermodynamics Volume 2011, Article ID 945047, 7 pages doi:10.1155/2011/945047 Research Article Corollary from the Exact Expression for Enthalpy of Vaporization A. A. Sobko Department of Physics and Chemistry of New Materials, A. M. Prokhorov Academy of Engineering Sciences, 19 Presnensky Val, Moscow 123557, Russia Correspondence should be addressed to A. A. Sobko, [email protected] Received 14 November 2010; Revised 9 March 2011; Accepted 16 March 2011 Academic Editor: K. A. Antonopoulos Copyright © 2011 A. A. Sobko. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. A problem on determining effective volumes for atoms and molecules becomes actual due to rapidly developing nanotechnologies. In the present study an exact expression for enthalpy of vaporization is obtained, from which an exact expression is derived for effective volumes of atoms and molecules, and under certain assumptions on the form of an atom (molecule) it is possible to find their linear dimensions. The accuracy is only determined by the accuracy of measurements of thermodynamic parameters at the critical point. 1. Introduction 1938 [2] with the edition from 1976 [3], we may find them actually similar. we may come to the same conclusion if In the present study, the relationship is obtained that we compare [2] with recent monograph by Prigogine and combines the enthalpy of vaporization with other thermody- Kondepudi “Modern Thermodynamics” [4]. The chapters namic evaporation parameters from the general expression devoted to first-order phase transitions in both monographs for the heat of first-order phase transformations. -
Problem Set #10 Assigned November 8, 2013 – Due Friday, November 15, 2013 Please Show All Work for Credit
Problem Set #10 Assigned November 8, 2013 – Due Friday, November 15, 2013 Please show all work for credit To Hand in 1. 1 2. –1 A least squares fit of ln P versus 1/T gives the result Hvaporization = 25.28 kJ mol . 3. Assuming constant pressure and temperature, and that the surface area of the protein is reduced by 25% due to the hydrophobic interaction: 2 G 0.25 N A 4 r Convert to per mole, ↓determine size per molecule 4 r 3 V M N 0.73mL/ g 60000g / mol (6.02 1023) 3 2 2 A r 2.52 109 m 2 23 9 2 G 0.25 N A 4 r 0.0720N / m 0.25 6.02 10 / mol (4 ) (2.52 10 m) 865kJ / mol We think this is a reasonable approach, but the value seems high 2 4. The vapor pressure of an unknown solid is approximately given by ln(P/Torr) = 22.413 – 2035(K/T), and the vapor pressure of the liquid phase of the same substance is approximately given by ln(P/Torr) = 18.352 – 1736(K/T). a. Calculate Hvaporization and Hsublimation. b. Calculate Hfusion. c. Calculate the triple point temperature and pressure. a) Calculate Hvaporization and Hsublimation. From Equation (8.16) dPln H sublimation dT RT 2 dln P d ln P dT d ln P H T 2 sublimation 11 dT dT R dd TT For this specific case H sublimation 2035 H 16.92 103 J mol –1 R sublimation Following the same proedure as above, H vaporization 1736 H 14.43 103 J mol –1 R vaporization b. -
Phase Diagrams a Phase Diagram Is Used to Show the Relationship Between Temperature, Pressure and State of Matter
Phase Diagrams A phase diagram is used to show the relationship between temperature, pressure and state of matter. Before moving ahead, let us review some vocabulary and particle diagrams. States of Matter Solid: rigid, has definite volume and definite shape Liquid: flows, has definite volume, but takes the shape of the container Gas: flows, no definite volume or shape, shape and volume are determined by container Plasma: atoms are separated into nuclei (neutrons and protons) and electrons, no definite volume or shape Changes of States of Matter Freezing start as a liquid, end as a solid, slowing particle motion, forming more intermolecular bonds Melting start as a solid, end as a liquid, increasing particle motion, break some intermolecular bonds Condensation start as a gas, end as a liquid, decreasing particle motion, form intermolecular bonds Evaporation/Boiling/Vaporization start as a liquid, end as a gas, increasing particle motion, break intermolecular bonds Sublimation Starts as a solid, ends as a gas, increases particle speed, breaks intermolecular bonds Deposition Starts as a gas, ends as a solid, decreases particle speed, forms intermolecular bonds http://phet.colorado.edu/en/simulation/states- of-matter The flat sections on the graph are the points where a phase change is occurring. Both states of matter are present at the same time. In the flat sections, heat is being removed by the formation of intermolecular bonds. The flat points are phase changes. The heat added to the system are being used to break intermolecular bonds. PHASE DIAGRAMS Phase diagrams are used to show when a specific substance will change its state of matter (alignment of particles and distance between particles). -
Jgt3 R:. A) -2ZJ(6 .' .'
2 1. (24) a. In the diagram below to the to the right, helium atoms are represented by unshaded spheres, neon atoms by gray spheres, and argon atoms by black spheres. If the total pressure in the container is 900 mm Hg, wh at is the parti~ressure of helium? A) 90 mm Hg ~ 180 mm HgC) 270 mm Hg D) 450 mm Hg • 0 o b. Which of the following is not a ~ e function? O. A) enthalpy ® heat C) internal energy D) volume .0.o c. Which one of the followin g~ ses will have the high est rate of effusion? A) N02 ~ N20 C) N204 D) N03 SF(" '$ ,..""I"' DI A-r:: Q09/mol d. At what temperature will sulfur hexafluoride molecules have th e same average speed as argon atoms at 20°C? JGt3 r:. A) -2ZJ(6 B) 73.2° C C) 381 °C @ 799°C e. Which substance in each of the following pairs is expected to have the larger dispersion forces? I BrZ o r I Z '" ""o'o....r~SS ~ A) Br2 in set I and n-butane in set" H H H H B) Br2 in set 1 and isobutane in set II I I I I © 12 in set I and n-butane in set" I I E-t-C----,:::-C-C-H o r H I I I I I D) 12 in set I and isobutane in set II H H H H H-C- C---C-H n- bu t ane I I I H H H l.sDbut a na f. -
Entropy and Free Energy
Spontaneous Change: Entropy and Free Energy 2nd and 3rd Laws of Thermodynamics Problem Set: Chapter 20 questions 29, 33, 39, 41, 43, 45, 49, 51, 60, 63, 68, 75 The second law of thermodynamics looks mathematically simple but it has so many subtle and complex implications that it makes most chemistry majors sweat a lot before (and after) they graduate. Fortunately its practical, down-to-earth applications are easy and crystal clear. We can build on those to get to very sophisticated conclusions about the behavior of material substances and objects in our lives. Frank L. Lambert Experimental Observations that Led to the Formulation of the 2nd Law 1) It is impossible by a cycle process to take heat from the hot system and convert it into work without at the same time transferring some heat to cold surroundings. In the other words, the efficiency of an engine cannot be 100%. (Lord Kelvin) 2) It is impossible to transfer heat from a cold system to a hot surroundings without converting a certain amount of work into additional heat of surroundings. In the other words, a refrigerator releases more heat to surroundings than it takes from the system. (Clausius) Note 1: Even though the need to describe an engine and a refrigerator resulted in formulating the 2nd Law of Thermodynamics, this law is universal (similarly to the 1st Law) and applicable to all processes. Note 2: To use the Laws of Thermodynamics we need to understand what the system and surroundings are. Universe = System + Surroundings universe Matter Surroundings (Huge) Work System Matter, Heat, Work Heat 1. -
Cryometric Determination of the Enthalpy of Fusion of Sodium Cryolite
Cryometric determination of the enthalpy of fusion of sodium cryolite M. MALINOVSKÝ Department of Chemical Technology of Inorganic Substances, Slovak Technical University, CS-812 37Bratislava Received 30 July 1982 Accepted for publication 22 August 1983 Using the method of classical thermal analysis a part of the liquidus of sodium cryolite in the system Na3AlF6—Na3FS04 was measured in the compo sition range 0—5 mole % Na3FS04. On the basis of these results the molar enthalpy of fusion of cryolite was calculated. It was found that AHf(Na3AlFft) = = 115.4 kJ mol"1; error in this result was estimated to be ±4.9 %. Методом классического термического анализа измерена часть ликви дуса натриевого криолита в системе Na3AlF6—Na3FS04 в интервале кон центраций 0—5 мол. % Na3FS04. На основании этих результатов рассчи тана мольная энтальпия плавления криолита. Найдено, что 1 AH,(Na3AlF6) = 115,4 кДж моль" ; точность этого результата ±4,9 %. Literature survey and theoretical Knowledge of the enthalpy of fusion of sodium hexafluoroaluminate Na3AlF6 (cryolite) is important both from theoretical and practical points of view. For example, it is needed at calculation of the thermal and energy balance and/or the thermal inertia of aluminium cells (the electrolyte contains about 90 mass % of Na3AlF6). The most precise values of the molar enthalpy of fusion AHf(i) of chemical substances can be generally obtained from calorimetric measurements. However, when we deal with substances having higher melting temperature and which are also unstable and very corrosive the calorimetric determination of the quantity AHf(i) can be less reliable. In the case of cryolite Roth and Bertram [1] found from the calorimetric 1 1 measurements ÄH,(Na3 A1F6) = 16.64 kcal mol" = 69.62 kJ mol" .