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Characteristics of Chemical Equilibrium
Characteristics of Chemical Equilibrium Chapter 14: Chemical Equilibrium © 2008 Brooks/Cole 1 © 2008 Brooks/Cole 2 Equilibrium is Dynamic Equilibrium is Independent of Direction of Approach Reactants convert to products N2(g) + 3 H2(g) 2 NH3(g) a A + b B c C + d D Species do not stop forming OR being destroyed Rate of formation = rate of removal Concentrations are constant. © 2008 Brooks/Cole 3 © 2008 Brooks/Cole 4 Equilibrium and Catalysts The Equilibrium Constant For the 2-butene isomerization: H3C CH3 H3C H C=C C=C H H H CH3 At equilibrium: rate forward = rate in reverse An elementary reaction, so: kforward[cis] = kreverse[trans] © 2008 Brooks/Cole 5 © 2008 Brooks/Cole 6 1 The Equilibrium Constant The Equilibrium Constant At equilibrium the concentrations become constant. We had: kforward[cis] = kreverse[trans] kforward [trans] or = kreverse [cis] kforward [trans] Kc = = = 1.65 (at 500 K) kreverse [cis] “c” for concentration based © 2008 Brooks/Cole 7 © 2008 Brooks/Cole 8 The Equilibrium Constant The Equilibrium Constant For a general reaction: a A + b B c C + d D [NO]2 N2(g) + O2(g) 2 NO(g) Kc = Products raised to [N2] [O2] stoichiometric powers… k [C]c [D]d forward …divided by reactants Kc = = a b kreverse [A] [B] raised to their stoichiometric [SO ] 1 2 powers 8 S8(s) + O2(g) SO2(g) Kc = [O2] © 2008 Brooks/Cole 9 © 2008 Brooks/Cole 10 Equilibria Involving Pure Liquids and Solids Equilibria in Dilute Solutions [Solid] is constant throughout a reaction. density g / L • pure solid concentration = mol. -
Laboratory 1: Chemical Equilibrium 1
1 Laboratory 1: Chemical Equilibrium 1 Reading: Olmstead and Williams, Chemistry , Chapter 14 (all sections) Purpose: The shift in equilibrium position of a chemical reaction with applied stress is determined. Introduction Chemical Equilibrium No chemical reaction goes to completion. When a reaction stops, some amount of reactants remain. For example, although we write → ← 2 CO 2 (g) 2 CO (g) + O 2 (g) (1) as though it goes entirely to products, at 2000K only 2% of the CO 2 decomposes. A chemical reaction reaches equilibrium when the concentrations of the reactants and products no longer change with time. The position of equilibrium describes the relative amounts of reactants and products that remain at the end of a chemical reaction. The position of equilibrium for reaction (1) is said to lie with the reactants, or to the left, because at equilibrium very little of the carbon dioxide has reacted. On the other hand, in the reaction → ← H2 (g) + ½ O2 (g) H2O (g) (2) the equilibrium position lies very far to the right since only very small amounts of H 2 and O 2 remain after the reaction reaches equilibrium. Since chemists often wish to maximize the yield of a reaction, it is vital to determine how to control the position of the equilibrium. The equilibrium position of a reaction may shift if an external stress is applied. The stress may be in the form of a change in temperature, pressure, or the concentration of one of the reactants or products. For example, consider a flask with an equilibrium mixture of CO 2, CO, and O 2, as in reaction (1). -
Oxygen Reduction Reactions in Ionic Liquids and the Formulation of a General ORR Mechanism for Li−Air Batteries † † † † ‡ Chris J
Article pubs.acs.org/JPCC Oxygen Reduction Reactions in Ionic Liquids and the Formulation of a General ORR Mechanism for Li−Air Batteries † † † † ‡ Chris J. Allen, Jaehee Hwang, Roger Kautz, Sanjeev Mukerjee, Edward J. Plichta, ‡ † Mary A. Hendrickson, and K. M. Abraham*, † Department of Chemistry and Chemical Biology, Northeastern University Center for Renewable Energy Technology (NUCRET), Northeastern University, Boston, Massachusetts 02115, United States ‡ Power Division, U.S. Army RDECOM CERDEC CP&I, RDER-CCP, 5100 Magazine Road, Aberdeen Proving Ground, Maryland 21005, United States ABSTRACT: Oxygen reduction and evolution reactions (ORRs and OERs) have been studied in ionic liquids containing singly charged cations having a range of ionic radii, or charge densities. Specifically, ORR and OER mechanisms were studied using cyclic and rotating disk electrode voltammetry in the neat ionic liquids (ILs), 1-ethyl- 3-methylimidazolium bis(trifluoromethylsulfonyl)imide (EMITFSI) and 1-methyl-1-butyl-pyrrolidinium bis- fl (tri ouromethanesulfonyl)imide (PYR14TFSI), and in their solutions containing LiTFSI, NaPF6, KPF6, and tetrabutylam- fl monium hexa uorophosphate (TBAPF6). A strong correlation was found between the ORR products and the ionic charge density, including those of the ionic liquids. The observed trend is explained in terms of the Lewis acidity of the cation present in the electrolyte using an acidity scale created from 13C − 13 NMR chemical shifts and spin lattice relaxation (T1) times of C O in solutions of these charged ions in propylene carbonate (PC). The ionic liquids lie in a continuum of a cascading Lewis acidity scale with respect to the charge density of alkali metal, IL, and TBA cations with the result that the ORR products in ionic liquids and in organic electrolytes containing any conducting cations can be predicted on the basis of a general theory based on the hard soft acid base (HSAB) concept. -
Protein Unfolding (Model Peptide Helix/Helix-Coil Transition/Denaturant Effects) J
Proc. Natl. Acad. Sci. USA Vol. 92, pp. 185-189, January 1995 Biochemistry Urea unfolding of peptide helices as a model for interpreting protein unfolding (model peptide helix/helix-coil transition/denaturant effects) J. MARTIN SCHOLTZ*tt, DOUG BARRICK*§, EUNICE J. YORK0, JOHN M. STEWART$, AND ROBERT L. BALDWIN*: *Department of Biochemistry, Stanford University School of Medicine, Stanford, CA 97305-5307; tDepartment of Medical Biochemistry and Genetics, Center for Macromolecular Design, Texas A&M University, College Station, TX 77843-1114; and 1Department of Biochemistry, University of Colorado Health Sciences Center, Denver, CO 80262 Contributed by Robert L. Baldwin, August 29, 1994 ABSTRACT To provide a model system for understand- The peptides examined here consist primarily of alanine;"1 ing how the unfolding of protein a-helices by urea contributes thus side-chain interactions are minimal, and the primary to protein denaturation, urea unfolding was measured for a structural and thermodynamic changes during helix unfolding homologous series of helical peptides with the repeating should result from the peptide backbone. Because these helical sequence Ala-Glu-Ala-Ala-Lys-Ala and chain lengths varying peptides lack hydrophobic cores and long-range tertiary in- from 14 to 50 residues. The dependence of the helix propa- teractions, the thermodynamics of solvent denaturation of gation parameter of the Zimm-Bragg model for helix-coil secondary structure can be measured directly. Although sec- transition theory (s) on urea molarity ([urea]) was deter- ondary structure formation must be an integral part of the mined at 0°C with data for the entire set of peptides, and a protein folding reaction, these other factors (hydrophobic core linear dependence ofIns on [urea] was found. -
The Strongest Acid Christopher A
Chemistry in New Zealand October 2011 The Strongest Acid Christopher A. Reed Department of Chemistry, University of California, Riverside, California 92521, USA Article (e-mail: [email protected]) About the Author Chris Reed was born a kiwi to English parents in Auckland in 1947. He attended Dilworth School from 1956 to 1964 where his interest in chemistry was un- doubtedly stimulated by being entrusted with a key to the high school chemical stockroom. Nighttime experiments with white phosphorus led to the Headmaster administering six of the best. He obtained his BSc (1967), MSc (1st Class Hons., 1968) and PhD (1971) from The University of Auckland, doing thesis research on iridium organotransition metal chemistry with Professor Warren R. Roper FRS. This was followed by two years of postdoctoral study at Stanford Univer- sity with Professor James P. Collman working on picket fence porphyrin models for haemoglobin. In 1973 he joined the faculty of the University of Southern California, becoming Professor in 1979. After 25 years at USC, he moved to his present position of Distinguished Professor of Chemistry at UC-Riverside to build the Centre for s and p Block Chemistry. His present research interests focus on weakly coordinating anions, weakly coordinated ligands, acids, si- lylium ion chemistry, cationic catalysis and reactive cations across the periodic table. His earlier work included extensive studies in metalloporphyrin chemistry, models for dioxygen-binding copper proteins, spin-spin coupling phenomena including paramagnetic metal to ligand radical coupling, a Magnetochemi- cal alternative to the Spectrochemical Series, fullerene redox chemistry, fullerene-porphyrin supramolecular chemistry and metal-organic framework solids (MOFs). -
Lecture 15: 11.02.05 Phase Changes and Phase Diagrams of Single- Component Materials
3.012 Fundamentals of Materials Science Fall 2005 Lecture 15: 11.02.05 Phase changes and phase diagrams of single- component materials Figure removed for copyright reasons. Source: Abstract of Wang, Xiaofei, Sandro Scandolo, and Roberto Car. "Carbon Phase Diagram from Ab Initio Molecular Dynamics." Physical Review Letters 95 (2005): 185701. Today: LAST TIME .........................................................................................................................................................................................2� BEHAVIOR OF THE CHEMICAL POTENTIAL/MOLAR FREE ENERGY IN SINGLE-COMPONENT MATERIALS........................................4� The free energy at phase transitions...........................................................................................................................................4� PHASES AND PHASE DIAGRAMS SINGLE-COMPONENT MATERIALS .................................................................................................6� Phases of single-component materials .......................................................................................................................................6� Phase diagrams of single-component materials ........................................................................................................................6� The Gibbs Phase Rule..................................................................................................................................................................7� Constraints on the shape of -
Superacid Chemistry
SUPERACID CHEMISTRY SECOND EDITION George A. Olah G. K. Surya Prakash Arpad Molnar Jean Sommer SUPERACID CHEMISTRY SUPERACID CHEMISTRY SECOND EDITION George A. Olah G. K. Surya Prakash Arpad Molnar Jean Sommer Copyright # 2009 by John Wiley & Sons, Inc. All rights reserved Published by John Wiley & Sons, Inc., Hoboken, New Jersey Published simultaneously in Canada No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by any means, electronic, mechanical, photocopying, recording, scanning, or otherwise, except as permitted under Section 107 or 108 of the 1976 United States Copyright Act, without either the prior written permission of the Publisher, or authorization through payment of the appropriate per-copy fee to the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923, (978) 750-8400, fax (978) 750-4470, or on the web at www.copyright.com. Requests to the Publisher for permission should be addressed to the Permissions Department, John Wiley & Sons, Inc., 111 River Street, Hoboken, NJ 07030, (201) 748-6011, fax (201) 748-6008, or online at http://www.wiley.com/go/permission. Limit of Liability/Disclaimer of Warranty: While the publisher and author have used their best efforts in preparing this book, they make no representations or warranties with respect to the accuracy or completeness of the contents of this book and specifically disclaim any implied warranties of merchantability or fitness for a particular purpose. No warranty may be created or extended by sales representatives or written sales materials. The advice and strategies contained herein may not be suitable for your situation. -
Phase Diagrams
Module-07 Phase Diagrams Contents 1) Equilibrium phase diagrams, Particle strengthening by precipitation and precipitation reactions 2) Kinetics of nucleation and growth 3) The iron-carbon system, phase transformations 4) Transformation rate effects and TTT diagrams, Microstructure and property changes in iron- carbon system Mixtures – Solutions – Phases Almost all materials have more than one phase in them. Thus engineering materials attain their special properties. Macroscopic basic unit of a material is called component. It refers to a independent chemical species. The components of a system may be elements, ions or compounds. A phase can be defined as a homogeneous portion of a system that has uniform physical and chemical characteristics i.e. it is a physically distinct from other phases, chemically homogeneous and mechanically separable portion of a system. A component can exist in many phases. E.g.: Water exists as ice, liquid water, and water vapor. Carbon exists as graphite and diamond. Mixtures – Solutions – Phases (contd…) When two phases are present in a system, it is not necessary that there be a difference in both physical and chemical properties; a disparity in one or the other set of properties is sufficient. A solution (liquid or solid) is phase with more than one component; a mixture is a material with more than one phase. Solute (minor component of two in a solution) does not change the structural pattern of the solvent, and the composition of any solution can be varied. In mixtures, there are different phases, each with its own atomic arrangement. It is possible to have a mixture of two different solutions! Gibbs phase rule In a system under a set of conditions, number of phases (P) exist can be related to the number of components (C) and degrees of freedom (F) by Gibbs phase rule. -
The Role of Hydrogen Bonding in Paracetamol–Solvent and Paracetamol–Hydrogel Matrix Interactions
materials Article The Role of Hydrogen Bonding in Paracetamol–Solvent and Paracetamol–Hydrogel Matrix Interactions Marta Miotke-Wasilczyk *, Marek Józefowicz * , Justyna Strankowska and Jerzy Kwela Insitute of Experimental Physics, Faculty of Mathematics, Physics and Informatics, University of Gda´nsk, Wita Stwosza 57, 80-308 Gda´nsk,Poland; [email protected] (J.S.); [email protected] (J.K.) * Correspondence: [email protected] (M.M.-W.); [email protected] (M.J.) Abstract: The photophysical and photochemical properties of antipyretic drug – paracetamol (PAR) and its two analogs with different substituents (acetanilide (ACT) and N-ethylaniline (NEA)) in 14 solvents of different polarity were investigated by the use of steady–state spectroscopic technique and quantum–chemical calculations. As expected, the results show that the spectroscopic behavior of PAR, ACT, and NEA is highly dependent on the nature of the solute–solvent interactions (non- specific (dipole-dipole) and specific (hydrogen bonding)). To characterize these interactions, the multiparameter regression analysis proposed by Catalán was used. In order to obtain a deeper insight into the electronic and optical properties of the studied molecules, the difference of the dipole moments of a molecule in the ground and excited state were determined using the theory proposed by Lippert, Mataga, McRae, Bakhshiev, Bilot, and Kawski. Additionally, the influence of the solute polarizability on the determined dipole moments was discussed. The results of the solvatochromic studies were related to the observations of the release kinetics of PAR, ACT, and NEA from polyurethane hydrogels. The release kinetics was analyzed using the Korsmayer-Peppas and Hopfenberg models. -
2701X0073.Pdf
COORDINATION AND REDOX PROPERTIES IN SOLUTION YIKTOR GUTMANN Inst it Ut für Anorganische Chemie der Technischen Hochschule Wien, Austria ABSTRACT A primitive description of the functional electron cloud is given and is used to account for the mutual influence between coordinating and redox properties. Rules are given for the change in redox properties by coordination and vice versa. It is further shown that the redox potential in a donor solvent is determined by its donor number and an empirical approach is suggested to obtain the electromotive series for any solvent of given donor number. The donor number is also considered important for the ionization of a covalent substrate. Finally a new classification is suggested for charge-transfer complexes. THE PRIMITIVE DESCRIPTION OF THE FUNCTIONAL ELECTRON CLOUD In a primitive way, a characteristic 'electron cloud' may be ascribed to each atom, ion or molecule. Even in the state of highest stability of the entity, the ground state, the electronic arrangement is usually far from 'ideal' as is evidenced by the tendency to undergo chemical reactions. In the primitive description of the 'functional electron cloud', the 'non-ideality' of the cloud is considered responsible for its tendency to change; the actual function will depend also on the properties of the reactant. The functional cloud may deviate from the ideal by being either too 'dilute' or too 'dense' compared with that of the reacting molecule. An entity with a 'dilute' electron cloud will tend to gain electrons or to achieve an appropriate share of them and will thus function as an acceptor of elec- trons. -
Title a Hydronium Solvate Ionic Liquid
A Hydronium Solvate Ionic Liquid: Facile Synthesis of Air- Title Stable Ionic Liquid with Strong Bronsted Acidity Kitada, Atsushi; Takeoka, Shun; Kintsu, Kohei; Fukami, Author(s) Kazuhiro; Saimura, Masayuki; Nagata, Takashi; Katahira, Masato; Murase, Kuniaki Journal of the Electrochemical Society (2018), 165(3): H121- Citation H127 Issue Date 2018-02-22 URL http://hdl.handle.net/2433/240665 © The Author(s) 2018. Published by ECS. This is an open access article distributed under the terms of the Creative Commons Attribution 4.0 License (CC BY, Right http://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse of the work in any medium, provided the original work is properly cited. Type Journal Article Textversion publisher Kyoto University Journal of The Electrochemical Society, 165 (3) H121-H127 (2018) H121 A Hydronium Solvate Ionic Liquid: Facile Synthesis of Air-Stable Ionic Liquid with Strong Brønsted Acidity Atsushi Kitada, 1,z Shun Takeoka,1 Kohei Kintsu,1 Kazuhiro Fukami,1,∗ Masayuki Saimura,2 Takashi Nagata,2 Masato Katahira,2 and Kuniaki Murase1,∗ 1Department of Materials Science and Engineering, Kyoto University, Yoshida-honmachi, Sakyo, Kyoto 606-8501, Japan 2Institute of Advanced Energy, Gokasho, Uji, Kyoto 611-0011, Japan + A new kind of ionic liquid (IL) with strong Brønsted acidity, i.e., a hydronium (H3O ) solvate ionic liquid, is reported. The IL can + + be described as [H3O · 18C6]Tf2N, where water exists as the H3O ion solvated by 18-crown-6-ether (18C6), of which the counter – – + anion is bis(trifluoromethylsulfonyl)amide (Tf2N ;Tf= CF3SO2). The hydrophobic Tf2N anion makes [H3O · 18C6]Tf2N stable + in air. -
140. Sulphuric, Hydrochloric, Nitric and Phosphoric Acids
nr 2009;43(7) The Nordic Expert Group for Criteria Documentation of Health Risks from Chemicals 140. Sulphuric, hydrochloric, nitric and phosphoric acids Marianne van der Hagen Jill Järnberg arbete och hälsa | vetenskaplig skriftserie isbn 978-91-85971-14-5 issn 0346-7821 Arbete och Hälsa Arbete och Hälsa (Work and Health) is a scientific report series published by Occupational and Enviromental Medicine at Sahlgrenska Academy, University of Gothenburg. The series publishes scientific original work, review articles, criteria documents and dissertations. All articles are peer-reviewed. Arbete och Hälsa has a broad target group and welcomes articles in different areas. Instructions and templates for manuscript editing are available at http://www.amm.se/aoh Summaries in Swedish and English as well as the complete original texts from 1997 are also available online. Arbete och Hälsa Editorial Board: Editor-in-chief: Kjell Torén Tor Aasen, Bergen Kristina Alexanderson, Stockholm Co-editors: Maria Albin, Ewa Wigaeus Berit Bakke, Oslo Tornqvist, Marianne Törner, Wijnand Lars Barregård, Göteborg Eduard, Lotta Dellve och Roger Persson Jens Peter Bonde, Köpenhamn Managing editor: Cina Holmer Jörgen Eklund, Linköping Mats Eklöf, Göteborg © University of Gothenburg & authors 2009 Mats Hagberg, Göteborg Kari Heldal, Oslo Arbete och Hälsa, University of Gothenburg Kristina Jakobsson, Lund SE 405 30 Gothenburg, Sweden Malin Josephson, Uppsala Bengt Järvholm, Umeå ISBN 978-91-85971-14-5 Anette Kærgaard, Herning ISSN 0346–7821 Ann Kryger, Köpenhamn http://www.amm.se/aoh