Liquid Equilibrium Measurements in Binary Polar Systems
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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. -
International Journal of Engineering Sciences
[Kanse*, 4.(12): December, 2015] ISSN: 2277-9655 (I2OR), Publication Impact Factor: 3.785 IJESRT INTERNATIONAL JOURNAL OF ENGINEERING SCIENCES & RESEARCH TECHNOLOGY A REVIEW OF PERVAPORATION MEMBRANE SYSTEM FOR THE SEPARATION OF ETHANOL/WATER (AZEOTROPIC MIXTURE) Nitin G. Kanse*, Dr. S. D. Dawande * Research Scholar, Department of Chemical Engineering Laxminarayan Institute of Technology, Nagpur. ABSTRACT Membrane separation process has become one of the emerging technologies that undergo a rapid growth for the past few decades. Pervaporation is the one of the membrane separation processes that have gained increasing interest in the chemical and allied industries. Pervaporation has significant advantages in separation of azeotropic systems where traditional distillation can recover pure solvents with the use of entrainers, which then must be removed using an additional separation step. Pervaporation can be used to break the azeotrope, as its mechanism of separation is quite different to that of distillation. This review presents the separation of Azeotropic mixture such as ethanol-water by using Pervaporation. The fundamental aspects of Pervaporation over different types of membrane are revived and compared. The focus of this review is on separation of azeotropic mixture by using different membrane and effect of various parameters on Pervaporation. KEYWORDS: Pervaporation, Azeotropic mixture, Membrane, selectivity. INTRODUCTION Pervaporation is a new membrane technique which is used to separate a liquid mixture by partly vaporizing it through a nonporous permselective membrane. The feed mixture is allowed to flow along one side of the membrane and a fraction of it (the ‘permeate’) is evolved in the vapor state from the opposite side, which is kept under vacuum by continuous pumping Membrane separation processes offer many advantages over existing separation processes such as higher selectivity, lower energy consumption, moderate cost to performance ratio and compact with modular design [12, 19]. -
Equation of State for Benzene for Temperatures from the Melting Line up to 725 K with Pressures up to 500 Mpa†
High Temperatures-High Pressures, Vol. 41, pp. 81–97 ©2012 Old City Publishing, Inc. Reprints available directly from the publisher Published by license under the OCP Science imprint, Photocopying permitted by license only a member of the Old City Publishing Group Equation of state for benzene for temperatures from the melting line up to 725 K with pressures up to 500 MPa† MONIKA THOL ,1,2,* ERIC W. Lemm ON 2 AND ROLAND SPAN 1 1Thermodynamics, Ruhr-University Bochum, Universitaetsstrasse 150, 44801 Bochum, Germany 2National Institute of Standards and Technology, 325 Broadway, Boulder, Colorado 80305, USA Received: December 23, 2010. Accepted: April 17, 2011. An equation of state (EOS) is presented for the thermodynamic properties of benzene that is valid from the triple point temperature (278.674 K) to 725 K with pressures up to 500 MPa. The equation is expressed in terms of the Helmholtz energy as a function of temperature and density. This for- mulation can be used for the calculation of all thermodynamic properties. Comparisons to experimental data are given to establish the accuracy of the EOS. The approximate uncertainties (k = 2) of properties calculated with the new equation are 0.1% below T = 350 K and 0.2% above T = 350 K for vapor pressure and liquid density, 1% for saturated vapor density, 0.1% for density up to T = 350 K and p = 100 MPa, 0.1 – 0.5% in density above T = 350 K, 1% for the isobaric and saturated heat capaci- ties, and 0.5% in speed of sound. Deviations in the critical region are higher for all properties except vapor pressure. -
Determination of the Identity of an Unknown Liquid Group # My Name the Date My Period Partner #1 Name Partner #2 Name
Determination of the Identity of an unknown liquid Group # My Name The date My period Partner #1 name Partner #2 name Purpose: The purpose of this lab is to determine the identity of an unknown liquid by measuring its density, melting point, boiling point, and solubility in both water and alcohol, and then comparing the results to the values for known substances. Procedure: 1) Density determination Obtain a 10mL sample of the unknown liquid using a graduated cylinder Determine the mass of the 10mL sample Save the sample for further use 2) Melting point determination Set up an ice bath using a 600mL beaker Obtain a ~5mL sample of the unknown liquid in a clean dry test tube Place a thermometer in the test tube with the sample Place the test tube in the ice water bath Watch for signs of crystallization, noting the temperature of the sample when it occurs Save the sample for further use 3) Boiling point determination Set up a hot water bath using a 250mL beaker Begin heating the water in the beaker Obtain a ~10mL sample of the unknown in a clean, dry test tube Add a boiling stone to the test tube with the unknown Open the computer interface software, using a graph and digit display Place the temperature sensor in the test tube so it is in the unknown liquid Record the temperature of the sample in the test tube using the computer interface Watch for signs of boiling, noting the temperature of the unknown Dispose of the sample in the assigned waste container 4) Solubility determination Obtain two small (~1mL) samples of the unknown in two small test tubes Add an equal amount of deionized into one of the samples Add an equal amount of ethanol into the other Mix both samples thoroughly Compare the samples for solubility Dispose of the samples in the assigned waste container Observations: The unknown is a clear, colorless liquid. -
Application of Pervaporation and Vapor Permeation in Environmental Protection
Polish Journal of Environmental Studies Vol. 9, No. 1 (2000), 13-26 Application of Pervaporation and Vapor Permeation in Environmental Protection W. Kujawski Faculty of Chemistry, Nicholas Copernicus University, ul. Gagarina 7, 87-100 Toruń, Poland e-mail: [email protected] Abstract A review concerning pervaporation and vapor permeation - membrane separation techniques used to separate liquid mixtures, is presented. Examples of polymers for membrane preparation as well as perform- ance parameters of pervaporation and vapor permeation membranes are described. The second part of the paper presents applications of pervaporation and vapor permeation in environmental protection. At the present, liquid product mixtures must fulfill high purity requirements as well as effluents; there- fore, they have to be concentrated or reconditioned. In the process of product-integrated environmental protection, liquid substances should be separated specifically from the mainstream, either to save raw materials, to prevent or to minimize the disposal of effluents, or to recycle by-products. Such completely or partly soluble fluid mixtures can be separated with membrane methods. Pervaporation and vapor per- meation as the most well-known membrane processes for the separation of liquid and vapor mixtures allow a variety of possible application areas: i) dewatering of organic fluids like alcohols, ketones, ethers etc.; ii) separation of mixtures from narrow boiling temperatures to constant (azeotrop) boiling temperatures; iii) removal of organic pollutants from water and air streams; iv) separation of fermentation products; v) separation of organic-organic liquid mixtures. Keywords: pervaporation, vapor permeation, polymers, membrane methods, environmental protection Introduction ous organics from contaminated water in applications Most industrial scale separation processes are based such as groundwater remediation. -
The Basics of Vapor-Liquid Equilibrium (Or Why the Tripoli L2 Tech Question #30 Is Wrong)
The Basics of Vapor-Liquid Equilibrium (Or why the Tripoli L2 tech question #30 is wrong) A question on the Tripoli L2 exam has the wrong answer? Yes, it does. What is this errant question? 30.Above what temperature does pressurized nitrous oxide change to a gas? a. 97°F b. 75°F c. 37°F The correct answer is: d. all of the above. The answer that is considered correct, however, is: a. 97ºF. This is the critical temperature above which N2O is neither a gas nor a liquid; it is a supercritical fluid. To understand what this means and why the correct answer is “all of the above” you have to know a little about the behavior of liquids and gases. Most people know that water boils at 212ºF. Most people also know that when you’re, for instance, boiling an egg in the mountains, you have to boil it longer to fully cook it. The reason for this has to do with the vapor pressure of water. Every liquid wants to vaporize to some extent. The measure of this tendency is known as the vapor pressure and varies as a function of temperature. When the vapor pressure of a liquid reaches the pressure above it, it boils. Until then, it evaporates until the fraction of vapor in the mixture above it is equal to the ratio of the vapor pressure to the total pressure. At that point it is said to be in equilibrium and no further liquid will evaporate. The vapor pressure of water at 212ºF is 14.696 psi – the atmospheric pressure at sea level. -
Liquid-Vapor Equilibrium in a Binary System
Liquid-Vapor Equilibria in Binary Systems1 Purpose The purpose of this experiment is to study a binary liquid-vapor equilibrium of chloroform and acetone. Measurements of liquid and vapor compositions will be made by refractometry. The data will be treated according to equilibrium thermodynamic considerations, which are developed in the theory section. Theory Consider a liquid-gas equilibrium involving more than one species. By definition, an ideal solution is one in which the vapor pressure of a particular component is proportional to the mole fraction of that component in the liquid phase over the entire range of mole fractions. Note that no distinction is made between solute and solvent. The proportionality constant is the vapor pressure of the pure material. Empirically it has been found that in very dilute solutions the vapor pressure of solvent (major component) is proportional to the mole fraction X of the solvent. The proportionality constant is the vapor pressure, po, of the pure solvent. This rule is called Raoult's law: o (1) psolvent = p solvent Xsolvent for Xsolvent = 1 For a truly ideal solution, this law should apply over the entire range of compositions. However, as Xsolvent decreases, a point will generally be reached where the vapor pressure no longer follows the ideal relationship. Similarly, if we consider the solute in an ideal solution, then Eq.(1) should be valid. Experimentally, it is generally found that for dilute real solutions the following relationship is obeyed: psolute=K Xsolute for Xsolute<< 1 (2) where K is a constant but not equal to the vapor pressure of pure solute. -
Pressure Vs Temperature (Boiling Point)
Boiling Points and Vapor Pressure Background Boiling Points and Vapor Pressure Background: Definitions Vapor Pressure: The equilibrium pressure of a vapor above its liquid; the pressure of the vapor resulting from the evaporation of a liquid above a sample of the liquid in a closed container. Boiling Point: The temperature at which the vapor pressure of a liquid is equal to the atmospheric (or applied) pressure. As the temperature of the liquid increases, the vapor pressure will increase, as seen below: https://www.chem.purdue.edu/gchelp/liquids/vpress.html Vapor pressure is interpreted in terms of molecules of liquid converting to the gaseous phase and escaping into the empty space above the liquid. In order for the molecules to escape, the intermolecular forces (Van der Waals, dipole- dipole, and hydrogen bonding) have to be overcome, which requires energy. This energy can come in the form of heat, aka increase in temperature. Due to this relationship between vapor pressure and temperature, the boiling point of a liquid decreases as the atmospheric pressure decreases since there is more room above the liquid for molecules to escape into at lower pressure. The graph below illustrates this relationship using common solvents and some terpenes: Pressure vs Temperature (boiling point) Ethanol Heptane Isopropyl Alcohol B-myrcene 290.0 B-caryophyllene d-Limonene Linalool Pulegone 270.0 250.0 1,8-cineole (eucalyptol) a-pinene a-terpineol terpineol-4-ol 230.0 p-cymene 210.0 190.0 170.0 150.0 130.0 110.0 90.0 Temperature (˚C) Temperature 70.0 50.0 30.0 10 20 30 40 50 60 70 80 90 100 200 300 400 500 600 760 10.0 -10.0 -30.0 Pressure (torr) 1 Boiling Points and Vapor Pressure Background As a very general rule of thumb, the boiling point of many liquids will drop about 0.5˚C for a 10mmHg decrease in pressure when operating in the region of 760 mmHg (atmospheric pressure). -
Pervatech BV, Will Give a Presentation: up to New Horizons in Ceramic Membrane Pervaporation
PERVATECH selective ceramic membranes process design -NEWS FLASH- UP TO NEW HORIZONS IN CERAMIC MEMBRANE PERVAPORATION PRESENTATION AT THE ICOM Up to new horizons in ceramic membrane pervaporation Pervaporation is a membrane-based separation technique in which the feed stream is fed as a liquid and the permeate is evaporated through the membrane. Polymeric and ceramic membranes can be employed in this technique. In general polymeric pervaporation membranes are most suited for dehydration of organic solvents at low temperatures, whereas ceramic pervaporation membranes are utilized to dehydrate organic solvents at higher temperatures. More recently, pervaporation has earned more interest from the pharmaceutical and chemical markets, since pervaporation for dehydration is an energy-saving technique compared to conventional separation methods, like distillation. Suzhou, July 2014. With Pervatechs’ long-term experience in manufacturing ceramic pervaporation membranes it is now possible to break the azeotrope of water-solvent mixtures, like water-ethanol. The focus of Pervatech is We are happy to announce that Pervatech will be present at the ICOM 2014 Suzhou, to explore new possibilities in the field of pervaporation. With this drive and ongoing membrane the 10th International Congress on Membrane and Membrane Processes. development it has become feasible to dehydrate acetonitrile, acetyl acetate, THF, many other solvent systems and enhances esterification reactions by in situ dehydration. On Wednesday the 23rd of July 8:30uur, Frans Velterop, managing director of Pervatech BV, will give a presentation: Up to new horizons in ceramic membrane pervaporation. The ceramic membranes are produced via a sol-gel technique, a method most suited to tailor the functionality of the top-layer towards the intended application. -
An Instructional Module on Hybrid Separations for Undergraduate
AC 2012-3671: AN INSTRUCTIONAL MODULE ON HYBRID SEPARA- TIONS FOR UNDERGRADUATE CHEMICAL ENGINEERING SEPARA- TIONS COURSES Dr. Rebecca K. Toghiani, Mississippi State University Rebecca K. Toghiani is an Associate Professor of chemical engineering at Mississippi State University. She received her B.S.ChE, M.S.ChE, and Ph.D. in chemical engineering from the University of Missouri, Columbia. She received the 1996 Dow Outstanding New Faculty Award and the 2005 Outstanding Teach- ing Award from the ASEE Southeastern Section. A John Grisham Master Teacher at MSU, she was also an inaugural member of the Bagley College of Engineering Academy of Distinguished Teachers. She has also been recognized at MSU with the 2001 Outstanding Faculty Woman Award, the 2001 Hearin Professor of Engineering Award, and the 1999 College of Engineering Outstanding Engineering Educator Award. Dr. Priscilla J. Hill, Mississippi State University Priscilla Hill is currently an Associate Professor in the Dave C. Swalm School of Chemical Engineering at Mississippi State University. She has research interests in crystallization, particle technology, popu- lation balance modeling, and process synthesis. Her teaching interests include particle technology and thermodynamics. Dr. Carlen Henington, Mississippi State University Carlen Henington is a nationally certified School Psychologist and is an Associate Professor in School Psychology at Mississippi State University. She completed her doctoral work at Texas A&M University and her internship at the Monroe Meyer Institute for Genetics and Rehabilitation at the University of Nebraska Medical Center, Omaha. She received the Texas A&M Educational Psychology Distinguished Dissertation Award in 1997, the Mississippi State University Golden Key National Honor Society Out- standing Faculty Member Award in 2000, the Mississippi State University Phi Delta Kappa Outstanding Teaching Award in 1998, and the College of Education Service Award in 2010. -
Freezing and Boiling Point Changes
Freezing Point and Boiling Point Changes for Solutions and Solids Lesson Plans and Labs By Ranald Bleakley Physics and Chemistry teacher Weedsport Jnr/Snr High School RET 2 Cornell Center for Materials Research Summer 2005 Freezing Point and Boiling Point Changes for Solutions and Solids Lesson Plans and Labs Summary: Major skills taught: • Predicting changes in freezing and boiling points of water, given type and quantity of solute added. • Solving word problems for changes to boiling points and freezing points of solutions based upon data supplied. • Application of theory to real samples in lab to collect and analyze data. Students will describe the importance to industry of the depression of melting points in solids such as metals and glasses. • Students will describe and discuss the evolution of glass making through the ages and its influence on social evolution. Appropriate grade and level: The following lesson plans and labs are intended for instruction of juniors or seniors enrolled in introductory chemistry and/or physics classes. It is most appropriately taught to students who have a basic understanding of the properties of matter and of solutions. Mathematical calculations are intentionally kept to a minimum in this unit and focus is placed on concepts. The overall intent of the unit is to clarify the relationship between changes to the composition of a mixture and the subsequent changes in the eutectic properties of that mixture. Theme: The lesson plans and labs contained in this unit seek to teach and illustrate the concepts associated with the eutectic of both liquid solutions, and glasses The following people have been of great assistance: Professor Louis Hand Professor of Physics. -
Methods for the Determination of the Normal Boiling Point of a High
Metalworking Fluids & VOC, Today and Tomorrow A Joint Symposium by SCAQMD & ILMA South Coast Air Quality Management District Diamond Bar, CA, USA March 8, 2012 Understanding & Determining the Normal Boiling Point of a High Boiling Liquid Presentation Outline • Relationship of Vapor Pressure to Temperature • Examples of VP/T Curves • Calculation of Airborne Vapor Concentration • Binary Systems • Relative Volatility as a function of Temperature • GC Data and Volatility • Everything Needs a Correlation • Conclusions Vapor Pressure Models (pure vapor over pure liquid) Correlative: • Clapeyron: Log(P) = A/T + B • Antoine: Log(P) = A/(T-C) + B • Riedel: LogP = A/T + B + Clog(T) + DTE Predictive: • ACD Group Additive Methods • Riedel: LogP = A/T + B + Clog(T) + DTE Coefficients defined, Reduced T = T/Tc • Variations: Frost-Kalkwarf-Thodos, etc. Two Parameters: Log(P) = A/T + B Vaporization as an CH OH(l) CH OH(g) activated process 3 3 G = -RTln(K) = -RTln(P) K = [CH3OH(g)]/[CH3OH(l)] G = H - TS [CH3OH(g)] = partial P ln(P) = -G/RT [CH3OH(l)] = 1 (pure liquid) ln(P) = -H/RT+ S/R K = P S/R = B ln(P) = ln(K) H/R = -A Vapor pressure Measurement: Direct versus Distillation • Direct vapor pressure measurement (e.g., isoteniscope) requires pure material while distillation based determination can employ a middle cut with a relatively high purity. Distillation allows for extrapolation and/or interpolation of data to approximate VP. • Direct vapor pressure measurement requires multiple freeze-thaw cycles to remove atmospheric gases while distillation (especially atmospheric distillation) purges atmospheric gases as part of the process. • Direct measurement OK for “volatile materials” (normal BP < 100 oC) but involved for “high boilers” (normal BP > 100 oC).