Physical Model for Vaporization
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Surface Structure, Chemisorption and Reactions
Surface Structure, Chemisorption and Reactions Eckhard Pehlke, Institut für Theoretische Physik und Astrophysik, Christian-Albrechts-Universität zu Kiel, 24098 Kiel, Germany. Topics: (i) interplay between the geometric and electronic structure of solid surfaces, (ii) physical properties of surfaces: surface energy, surface stress and their relevance for surface morphology (iii) adsorption and desorption energy barriers, chemical reactivity of surfaces, heterogeneous catalysis (iv) chemisorption dynamics and energy dissipation: electronically non-adiabatic processes Technological Importance of Surfaces Solid surfaces are intriguing objects for basic research, and they are also of high technological utility: substrates for homo- or hetero-epitaxial growth of semiconductor thin films used in device technology surfaces can act as heterogeneous catalysts, used to induce and steer the desired chemical reactions Sect. I: The Geometric and the Electronic Structure of Crystal Surfaces Surface Crystallography 2D 3D number of space groups: 17 230 number of point groups: 10 32 number of Bravais lattices: 5 14 2D- symbol lattice 2D Bravais space point crystal system parameters lattice group groups m mp 1 oblique (mono- γ b 2 a, b, γ 2 clin) a o op b (ortho- a, b a m rectangular rhom- o 7 γ = 90 2mm bic) oc b a t (tetra- a = b 4 o tp a 3 square gonal) γ = 90 a 4mm a h hp 3 o a hexagonal (hexa- a = b 120 6 o gonal) γ = 120 5 3m 6mm Bulk Terminated fcc Crystal Surfaces z z fcc a (010) x y c a=c/ √ 2 x square lattice (tp) z z fcc (110) a c _ [110] y x rectangular lattice (op) z _ (111) fcc [011] _ [110] a y hexagonal lattice (hp) x Surface Atomic Geometry Examples: a reduced inter-layer H/Si(111) separation normal relaxation 2a Si(111) (7x7) (2x1) reconstruction K. -
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. -
Liquid Equilibrium Measurements in Binary Polar Systems
DIPLOMA THESIS VAPOR – LIQUID EQUILIBRIUM MEASUREMENTS IN BINARY POLAR SYSTEMS Supervisors: Univ. Prof. Dipl.-Ing. Dr. Anton Friedl Associate Prof. Epaminondas Voutsas Antonia Ilia Vienna 2016 Acknowledgements First of all I wish to thank Doctor Walter Wukovits for his guidance through the whole project, great assistance and valuable suggestions for my work. I have completed this thesis with his patience, persistence and encouragement. Secondly, I would like to thank Professor Anton Friedl for giving me the opportunity to work in TU Wien and collaborate with him and his group for this project. I am thankful for his trust from the beginning until the end and his support during all this period. Also, I wish to thank for his readiness to help and support Professor Epaminondas Voutsas, who gave me the opportunity to carry out this thesis in TU Wien, and his valuable suggestions and recommendations all along the experimental work and calculations. Additionally, I would like to thank everybody at the office and laboratory at TU Wien for their comprehension and selfless help for everything I needed. Furthermore, I wish to thank Mersiha Gozid and all the students of Chemical Engineering Summer School for their contribution of data, notices, questions and solutions during my experimental work. And finally, I would like to thank my family and friends for their endless support and for the inspiration and encouragement to pursue my goals and dreams. Abstract An experimental study was conducted in order to investigate the vapor – liquid equilibrium of binary mixtures of Ethanol – Butan-2-ol, Methanol – Ethanol, Methanol – Butan-2-ol, Ethanol – Water, Methanol – Water, Acetone – Ethanol and Acetone – Butan-2-ol at ambient pressure using the dynamic apparatus Labodest VLE 602. -
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). -
Vapor Pressures and Vaporization Enthalpies of the N-Alkanes from 2 C21 to C30 at T ) 298.15 K by Correlation Gas Chromatography
BATCH: je1a04 USER: jeh69 DIV: @xyv04/data1/CLS_pj/GRP_je/JOB_i01/DIV_je0301747 DATE: October 17, 2003 1 Vapor Pressures and Vaporization Enthalpies of the n-Alkanes from 2 C21 to C30 at T ) 298.15 K by Correlation Gas Chromatography 3 James S. Chickos* and William Hanshaw 4 Department of Chemistry and Biochemistry, University of MissourisSt. Louis, St. Louis, Missouri 63121 5 6 The temperature dependence of gas chromatographic retention times for n-heptadecane to n-triacontane 7 is reported. These data are used to evaluate the vaporization enthalpies of these compounds at T ) 298.15 8 K, and a protocol is described that provides vapor pressures of these n-alkanes from T ) 298.15 to 575 9 K. The vapor pressure and vaporization enthalpy results obtained are compared with existing literature 10 data where possible and found to be internally consistent. Sublimation enthalpies for n-C17 to n-C30 are 11 calculated by combining vaporization enthalpies with fusion enthalpies and are compared when possible 12 to direct measurements. 13 14 Introduction 15 The n-alkanes serve as excellent standards for the 16 measurement of vaporization enthalpies of hydrocarbons.1,2 17 Recently, the vaporization enthalpies of the n-alkanes 18 reported in the literature were examined and experimental 19 values were selected on the basis of how well their 20 vaporization enthalpies correlated with their enthalpies of 21 transfer from solution to the gas phase as measured by gas 22 chromatography.3 A plot of the vaporization enthalpies of 23 the n-alkanes as a function of the number of carbon atoms 24 is given in Figure 1. -
A Review of Surface Energy Balance Models for Estimating Actual Evapotranspiration with Remote Sensing at High Spatiotemporal Resolution Over Large Extents
Prepared in cooperation with the International Joint Commission A Review of Surface Energy Balance Models for Estimating Actual Evapotranspiration with Remote Sensing at High Spatiotemporal Resolution over Large Extents Scientific Investigations Report 2017–5087 U.S. Department of the Interior U.S. Geological Survey Cover. Aerial imagery of an irrigation district in southern California along the Colorado River with actual evapotranspiration modeled using Landsat data https://earthexplorer.usgs.gov; https://doi.org/10.5066/F7DF6PDR. A Review of Surface Energy Balance Models for Estimating Actual Evapotranspiration with Remote Sensing at High Spatiotemporal Resolution over Large Extents By Ryan R. McShane, Katelyn P. Driscoll, and Roy Sando Prepared in cooperation with the International Joint Commission Scientific Investigations Report 2017–5087 U.S. Department of the Interior U.S. Geological Survey U.S. Department of the Interior RYAN K. ZINKE, Secretary U.S. Geological Survey William H. Werkheiser, Acting Director U.S. Geological Survey, Reston, Virginia: 2017 For more information on the USGS—the Federal source for science about the Earth, its natural and living resources, natural hazards, and the environment—visit https://www.usgs.gov or call 1–888–ASK–USGS. For an overview of USGS information products, including maps, imagery, and publications, visit https://store.usgs.gov. Any use of trade, firm, or product names is for descriptive purposes only and does not imply endorsement by the U.S. Government. Although this information product, for the most part, is in the public domain, it also may contain copyrighted materials as noted in the text. Permission to reproduce copyrighted items must be secured from the copyright owner. -
How Does the Surface Free Energy Influence the Tack of Acrylic
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Springer - Publisher Connector J. Coat. Technol. Res., 10 (6) 879–885, 2013 DOI 10.1007/s11998-013-9522-2 How does the surface free energy influence the tack of acrylic pressure-sensitive adhesives (PSAs)? Arkadiusz Kowalski, Zbigniew Czech, Łukasz Byczyn´ ski Ó The Author(s) 2013. This article is published with open access at Springerlink.com Abstract This article describes a comparative study Introduction of the tack properties of a model acrylic pressure- sensitive adhesive (PSA) crosslinked using aluminum Pressure-sensitive adhesives (PSAs) are unique in that acetylacetonate on several substrates, including stain- they form a strong bond under relatively light pressure less steel, glass, polyethylene, polypropylene, polytet- over short contact times. PSAs immediately grab onto rafluoroethylene, polycarbonate, and poly(methyl a substrate (the material to which the PSA is applied) methacrylate). The tack measurements were con- without the need for activation agents (e.g., heat, ducted using a technique commonly used to measure water, solvent, etc.). Among the various classes of the tack of an adhesive tape in the PSA industries. The adhesives, PSAs are possibly the most common adhe- surface free energy (SFE) values of the materials were sive found in consumer products. Self-adhesive tapes evaluated using the Owens–Wendt and van Oss– and labels of all kinds are ubiquitous in everyday life. Chaudhury–Good methods. The experiments showed Synthetic polymers based on acrylics, silicones, poly- a clear relationship between the SFE of the substrate urethanes, or rubbers are preferred adhesive materials and the tack of the model acrylic PSA. -
Measured and Predicted Vapor Liquid Equilibrium
NREL/CP-5400-71336. Posted with permission. Presented at WCX18: SAE World Congress Experience, 10-12 April 2018, Detroit, Michigan. 2018-01-0361 Published 03 Apr 2018 Measured and Predicted Vapor Liquid Equilibrium of Ethanol-Gasoline Fuels with Insight on the Influence of Azeotrope Interactions on Aromatic Species Enrichment and Particulate Matter Formation in Spark Ignition Engines Stephen Burke Colorado State University Robert Rhoads University of Colorado Matthew Ratcliff and Robert McCormick National Renewable Energy Laboratory Bret Windom Colorado State University Citation: Burke, S., Rhoads, R., Ratcliff, M., McCormick, R. et al., “Measured and Predicted Vapor Liquid Equilibrium of Ethanol-Gasoline Fuels with Insight on the Influence of Azeotrope Interactions on Aromatic Species Enrichment and Particulate Matter Formation in Spark Ignition Engines,” SAE Technical Paper 2018-01-0361, 2018, doi:10.4271/2018-01-0361. Abstract the azeotrope interactions on the vapor/liquid composition relationship has been observed between increasing evolution of the fuel, distillations were performed using the ethanol content in gasoline and increased particulate Advanced Distillation Curve apparatus on carefully selected Amatter (PM) emissions from direct injection spark samples consisting of gasoline blended with ethanol and heavy ignition (DISI) vehicles. The fundamental cause of this obser- aromatic and oxygenated compounds with varying vapor pres- vation is not well understood. One potential explanation is sures, including cumene, p-cymene, 4-tertbutyl toluene, that increased evaporative cooling as a result of ethanol’s high anisole, and 4-methyl anisole. Samples collected during the HOV may slow evaporation and prevent sufficient reactant distillation indicate an enrichment of the heavy aromatic or mixing resulting in the combustion of localized fuel rich oxygenated additive with an increase in initial ethanol concen- regions within the cylinder. -
Surface Energy Storage
NASA SBIR 2017 Phase I Solicitation Z1.02 Surface Energy Storage Lead Center: GRC Participating Center(s): JPL, JSC Technology Area: TA3 Space Power and Energy Storage NASA is seeking innovative energy storage solutions for surface missions on the moon and Mars. The objective is to develop energy storage systems for landers, construction equipment, crew rovers, and science platforms. Energy requirements for mobile assets are expected to range up to 120 kW-hr with potential for clustering of smaller building blocks to meet the total need. Requirements for energy storage systems used in combination with surface solar arrays range from 500 kW-hr (Mars) to over 14 MW-hr (moon). Applicable technologies such as batteries and regenerative fuel cells should be lightweight, long-lived, and low cost. Of particular interest are technologies that are multi-use (e.g., moon and Mars) or cross-platform (e.g., lander use and rover use). Strong consideration should be given to environmental robustness for surface environments that include day/night thermal cycling, natural radiation, partial gravity, vacuum or very low ambient pressure, reduced solar insolation, dust, and wind. Creative ideas that utilize local materials to store energy would also be considered under this subtopic. Advanced secondary batteries that go beyond lithium-ion, can safely provide >300-400 watt-hours per kilogram, and have long calendar and shelf lives are highly desired for cross-cutting applications. Secondary batteries that can operate at -60°C with excellent capacity retention as compared to room temperature operation are also highly desired. Additionally, for the Mars Ascent vehicle, secondary batteries that can operate reliably after a 15 year shelf life are highly desired. -
Thermodynamics Guide Definitions, Guides, and Tips Definitions What Each Thermodynamic Value Means Enthalpy of Formation
Thermodynamics Guide Definitions, guides, and tips Definitions What each thermodynamic value means Enthalpy of Formation Definition The enthalpy required or released during formation of a molecule from its elements. H2(g) + ½O2(g) → H2O(g) ∆Hºf(H2O) Sign: ∆Hºf can be positive or negative. Direction: From elements to product. Phase: The phase of the product being formed can be anything, but the elemental starting materials must be in their elemental standard phase. Notes: • RC&O Appendix 1 collects these values. • Limited by what values are experimentally available. • Knowing the elemental form of each atom is helpful. Ionization Enthalpy (IE) Definition The enthalpy required to remove one electron from an atom or ion. Li(g) → Li+(g) + e– IE(Li) Sign: IE is always positive — removing electrons from proximity of nucleus requires enthalpy input Direction: IE goes from atom to ion/electron pair. Phase: IE is a gas phase property. Reactants and products must be gas phase. Notes: • Phase descriptors are not generally given to an electron. • Ionization energy is taken to be identical to ionization enthalpy. • The first IE of Li(g) is shown above. A second, third, or higher IE can also be determined. Removing each additional electron costs even more enthalpy. Electron Affinity (EA) Definition How much enthalpy is gained when an electron is added to an atom or ion. (How much an atom “wants” an electron). Cl(g) + e– → Cl–(g) EA(Cl) Sign: EA is always positive, but the enthalpy is negative: ∆Hºrxn < 0. This is because of how we describe the property as an “affinity”. -
Chapter 9 Phases of Nuclear Matter
Nuclear Science—A Guide to the Nuclear Science Wall Chart ©2018 Contemporary Physics Education Project (CPEP) Chapter 9 Phases of Nuclear Matter As we know, water (H2O) can exist as ice, liquid, or steam. At atmospheric pressure and at temperatures below the 0˚C freezing point, water takes the form of ice. Between 0˚C and 100˚C at atmospheric pressure, water is a liquid. Above the boiling point of 100˚C at atmospheric pressure, water becomes the gas that we call steam. We also know that we can raise the temperature of water by heating it— that is to say by adding energy. However, when water reaches its melting or boiling points, additional heating does not immediately lead to a temperature increase. Instead, we must overcome water's latent heats of fusion (80 kcal/kg, at the melting point) or vaporization (540 kcal/kg, at the boiling point). During the boiling process, as we add more heat more of the liquid water turns into steam. Even though heat is being added, the temperature stays at 100˚C. As long as some liquid water remains, the gas and liquid phases coexist at 100˚C. The temperature cannot rise until all of the liquid is converted to steam. This type of transition between two phases with latent heat and phase coexistence is called a “first order phase transition.” As we raise the pressure, the boiling temperature of water increases until it reaches a critical point at a pressure 218 times atmospheric pressure (22.1 Mpa) and a temperature of 374˚C is reached. -
Phase Changes Do Now
Phase Changes Do Now: What are the names for the phases that matter goes through when changing from solid to liquid to gas, and then back again? States of Matter - Review By adding energy, usually in the form of heat, the bonds that hold a solid together can slowly break apart. The object goes from one state, or phase, to another. These changes are called PHASE CHANGES. Solids A solid is an ordered arrangement of particles that have very little movement. The particles vibrate back and forth but remain closely attracted to each other. Liquids A liquid is an arrangement of less ordered particles that have gained energy and can move about more freely. Their attraction is less than a solid. Compare the two states: Gases By adding energy, solids can change from an ordered arrangement to a less ordered arrangement (liquid), and finally to a very random arrangement of the particles (the gas phase). Each phase change has a specific name, based on what is happening to the particles of matter. Melting and Freezing The solid, ordered The less ordered liquid molecules gain energy, molecules loose energy, collide more, and slow down, and become become less ordered. more ordered. Condensation and Vaporization The more ordered liquid molecules gain energy, speed The less ordered gas up, and become less ordered. molecules loose energy, Evaporation only occurs at slow down, and become the surface of a liquid. more ordered. Boiling occurs throughout the liquid. The linked image cannot be displayed. The file may have been moved, renamed, or deleted. Verify that the link points to the correct file and location.