Reaction Kinetics and Mechanisms in Coordination Compounds
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Transition State Theory. I
MIT OpenCourseWare http://ocw.mit.edu 5.62 Physical Chemistry II Spring 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 5.62 Spring 2007 Lecture #33 Page 1 Transition State Theory. I. Transition State Theory = Activated Complex Theory = Absolute Rate Theory ‡ k H2 + F "! [H2F] !!" HF + H Assume equilibrium between reactants H2 + F and the transition state. [H F]‡ K‡ = 2 [H2 ][F] Treat the transition state as a molecule with structure that decays unimolecularly with rate constant k. d[HF] ‡ ‡ = k[H2F] = kK [H2 ][F] dt k has units of sec–1 (unimolecular decay). The motion along the reaction coordinate looks ‡ like an antisymmetric vibration of H2F , one-half cycle of this vibration. Therefore k can be approximated by the frequency of the antisymmetric vibration ν[sec–1] k ≈ ν ≡ frequency of antisymmetric vibration (bond formation and cleavage looks like antisymmetric vibration) d[HF] = νK‡ [H2] [F] dt ! ‡* $ d[HF] (q / N) 'E‡ /kT [ ] = ν # *H F &e [H2 ] F dt "#(q 2 N)(q / N)%& ! ‡ $ ‡ ‡* ‡ (q / N) ' q *' q *' g * ‡ K‡ = # trans &) rot ,) vib ,) 0 ,e-E kT H2 qH2 ) q*H2 , gH2 gF "# (qtrans N) %&( rot +( vib +( 0 0 + ‡ Reaction coordinate is antisymmetric vibrational mode of H2F . This vibration is fully excited (high T limit) because it leads to the cleavage of the H–H bond and the formation of the H–F bond. For a fully excited vibration hν kT The vibrational partition function for the antisymmetric mode is revised 4/24/08 3:50 PM 5.62 Spring 2007 Lecture #33 Page 2 1 kT q*asym = ' since e–hν/kT ≈ 1 – hν/kT vib 1! e!h" kT h! Note that this is an incredibly important simplification. -
Eyring Equation
Search Buy/Sell Used Reactors Glass microreactors Hydrogenation Reactor Buy Or Sell Used Reactors Here. Save Time Microreactors made of glass and lab High performance reactor technology Safe And Money Through IPPE! systems for chemical synthesis scale-up. Worldwide supply www.IPPE.com www.mikroglas.com www.biazzi.com Reactors & Calorimeters Induction Heating Reacting Flow Simulation Steam Calculator For Process R&D Laboratories Check Out Induction Heating Software & Mechanisms for Excel steam table add-in for water Automated & Manual Solutions From A Trusted Source. Chemical, Combustion & Materials and steam properties www.helgroup.com myewoss.biz Processes www.chemgoodies.com www.reactiondesign.com Eyring Equation Peter Keusch, University of Regensburg German version "If the Lord Almighty had consulted me before embarking upon the Creation, I should have recommended something simpler." Alphonso X, the Wise of Spain (1223-1284) "Everything should be made as simple as possible, but not simpler." Albert Einstein Both the Arrhenius and the Eyring equation describe the temperature dependence of reaction rate. Strictly speaking, the Arrhenius equation can be applied only to the kinetics of gas reactions. The Eyring equation is also used in the study of solution reactions and mixed phase reactions - all places where the simple collision model is not very helpful. The Arrhenius equation is founded on the empirical observation that rates of reactions increase with temperature. The Eyring equation is a theoretical construct, based on transition state model. The bimolecular reaction is considered by 'transition state theory'. According to the transition state model, the reactants are getting over into an unsteady intermediate state on the reaction pathway. -
Density Functional and Molecular Orbital Studies
Reports in Theoretical Chemistry Dovepress open access to scientific and medical research Open Access Full Text Article REVIEW Relative stabilities of two difluorodiazene isomers: density functional and molecular orbital studies Jibanananda Jana Abstract: The N–N bond length in the cis isomer of difluorodiazene is shorter than that in the Department of Chemistry, Krishnagar trans isomer, giving the cis isomer higher stability. The energy partitioning approach identifies Government College, Krishnagar, the necessary and dictating parameters responsible for the higher N–N bond energy and higher Nadia, West Bengal, India non-bonded F–F interaction energy in the cis isomer. Using density functional theory, the cis isomer is found to have higher chemical hardness and lower softness, and hence, it has higher stability than the trans isomer on the basis of the principle of maximum hardness. Localized molecular orbital study shows that the cis isomer has a higher strength of delocalization of the lone pairs of electrons on the F atoms than does the trans isomer, leading to higher stability of the cis isomer. For personal use only. Keywords: cis/trans isomers, difluorodiazene, PMH, energy partitioning, localized molecular orbital, chemical hardness, softness Introduction 1 It is well known that difluorodiazine (dinitrogen difluoride), N2F2, is a gas with two isomers – cis and trans – which are shown in Figure 1. It is also known that the cis isomer predominates (∼90%) at 25°C over the trans isomer. It seems to be very obvious that the two fluorine atoms in the cis isomer, due to their greater proximity than in the trans isomer, undergo strong repulsion involving the lone pairs of electrons on the F atoms and that cis isomer is less stable than the trans one. -
A Study of the CIS Effect of Some Phosphorus Donor Ligands
A STUDY OF THE CIS EFFECT OF SOME PHOSPHORUS DONOR LIGANDS Karen L. Chalk B.Sc. (Hons., Chem.), Queen's University, 1979 A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE RFQTJIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE in the Department of Chemistry @ Karen L. Chalk, 1981 SIMON FRASER UNIVERSITY November 1981 All riqhts reserved. This thesis may not be reproduced in whole or in part, by photocopy or other means, without permission of the author APPROVAL Name : Karen L. Chalk Deqree : Master of Science Title of Research Pro3ect: A Study of the -Cis-Effect of Some Phosphorus Liaands Supervisory Committee: - --Senior ~upervid?: R.K. Pomeroy a Assistant Professor D. Sutton Professor - T.N. Bell Professor K. E. Newman Internal Examiner Date Approved : no^* 26: iq81 ii PART l AL COPYR l GHT L l CENSE I hereby grant to Simon Fraser University the right to lend my thesis, project or extended essay (the title of which is shown below) to users of the Simon Fraser University Library, and to make partial or single copies only for such users or in response to a request from the library of any other university, or other educational institution, on its own behalf or for one of its users. I further agree that permission for multiple copying of this work for scholarly purposes may be granted by me or the Dean of Graduate Studies. It is understood that copying or publication of this work for financial gain shall not be allowed without my written permission. Title of Thesis/Project/Extended Essay "A Study of the Cis-Effect of Some Phosphorus Donor Linands" Author: (signature) Karen L. -
Answers to Selected Problems
Answers to Selected Problems Chapter 1 1.2. 0.55 A 1.3. +-y-.z- ++ y+, z+ t-t-y+,~+ -!-!y+.z+ *x+ lx+ t-x+ *s -ls i- s- 1- s+ -l s+ t- s+ BeO triplet CO singlet NO doublet 1.5. "Ionic bonds" using 6p electrons are stronger than those using 6s electrons (Pb2+2Br- p Pb4 +4Br-). "Covalent bonds" with 6s electrons are stronger than those with 6p electrons (PbMe4 > PbMe2)' The energy gap between 6p and 6s orbitals is larger than that for 2p and 2s orbitals. 1.6. SOl = Cda + b + c + d + e + f) S02 = C2(a + b - c - d + e +f) S03 = C3(a - b + c - d + e + f) 541 542 Answers to Selected Problems S04 = C4 (a + b + c + d - e +f) SOs = Cs(a + b - c - d - e +f) SOb = C6 (a - b - c + d - e + f) 1.9. B. c. D d. 0 1.10. There is no vibrational distortion of a homonuclear diatomic that can lower its symmetry. Chapter 2 2.2. Charge density qi = 1; n-bond order Pii = I. 2.3. Il.E = 1l.E,. + IlE,; 1l.E, = 2(1 - i 12) {J. 2.4. Second-order perturbations are not additive. In double union of even AHs, the second order terms are large and cannot be ignored. Chapter 3 3.1. 4 J -jill jm Answers to Selected Problems 543 3.2. a. Ii) I1E n = 2-=( 2 + --3) {J = 0.92{J " ,,/17.7 j17.7 I1Enp = 2 ( --~- + 1 ) {J = 1.28{J j17.7 )17.7 (ii) I1En, = 2 ( -~= + ~-- ) {J = 0.84{J )20.7 fti0 (iii) I1Enp = 2( -- 6- + -~){J = 1.47{J ,,/17.7 v17.7 (iv) I1En, = 2 ( -/ + 2 ) {J = 1.35{J ..;20.7 )20.7 Thus (iii) > (ii) > Ii): (iv) > (ii). -
Bimolecular Reaction Rate Coefficients in the Last Lecture, We Learned Qualitatively the Reaction Mechanisms of Hydrocarbon Combustion
Combustion Chemistry Hai Wang Stanford University 2015 Princeton-CEFRC Summer School On Combustion Course Length: 3 hrs June 22 – 26, 2015 Copyright ©2015 by Hai Wang This material is not to be sold, reproduced or distributed without prior written permission of the owner, Hai Wang. Lecture 4 4. Bimolecular Reaction Rate Coefficients In the last lecture, we learned qualitatively the reaction mechanisms of hydrocarbon combustion. To make this description quantitative, we will need to have a basic knowledge of reaction rate theories. While the rate coefficients of a large number of combustion reactions are experimentally measured, reaction rate theories are often necessary to interpret the experimental data. We shall focus our discussion here to bimolecular reactions of the type A + B → C + D and leave the discussion for unimolecular reactions to a later time. 4.1 Hard Sphere Collision We discussed earlier that an elementary chemical reaction requires molecular collision. The rate coefficient of a bimolecular reaction is essentially the product of reaction probability of two reactants (A and B) upon collision at a given temperature γ(T) and the frequency of collision ZAB, k(T) [A][B] = γ(T) ZAB (4.1) Here we assume that molecules may be described by rigid spheres. Figure 4.1 shows several scenarios of molecular encounter. Starting from the head-on collision, an offset of the two axes of molecular motion leads to off-center collision. Suppose the diameter of A and B are σA and σB, respectively. The limiting off-center collision would have a spacing equal to (σA+σB)/2 between the two axes of molecular motions. -
Download Syllabus
D. Cremer, CHEM 6341, Models and Concepts in Chemistry 1 CHEM 6341 Models and Concepts in Chemistry, Spring term Class location: TBD Lectures, time and location: TBD Lab times and location: TBD Instructor: Dieter Cremer, 325 FOSC, ext 8-1300, [email protected] http://smu.edu/catco/ Office Hours: By appointment Units: 3 Grading: ABC Letter Grade Class number TBD 1. Rationale: In chemistry, every year 2 million new chemical facts are added to what is known since decades and centuries. No chemist can memorize just a fraction of this data. Nevertheless, chemists must be able to adjust their knowledge to all new chemical observations. This is effectively done by a series of models and concepts, which summarizes myriads of data in a simple way. The course focuses on a general understanding of chemistry in terms of models and concepts that describe structure, stability, reactivity and other properties of molecules in a simple, yet very effective way. The concept of electronegativity, the concept of the chemcial bond, molecular orbital theory, orbital symmetry, the Mulliken-Walsh model, the concept of the potential energy surface, the Jahn-Teller effects, conjugation and delocalization models, the Hückel and Möbius (anti)aromaticity concepts, through-space and through-bond interaction models, the concept of the hydrogen bond, the Woodward-Hoffman rules, the Evans-Dewar-Zimmermann rules, and the isolobal concept will be discussed among other topics. Many chemical problems from organic chemistry, inorganic chemistry, transition metal chemistry, and biochemistry will be presented and the applicability of the various models and concepts as well as their limitations will be demonstrated. -
The Photochemical Properties of Arene Metal Carbonyl Complexes of Group 6 and 7 Elements
THE PHOTOCHEMICAL PROPERTIES OF ARENE METAL CARBONYL COMPLEXES OF GROUP 6 AND 7 ELEMENTS DCU THIS THESIS IS PRESENTED FOR THE DEGREE OF DOCTOR OF PHILOSOPHY AT DUBLIN CITY UNIVERSITY BY Peter Brennan B.Sc. UNDER THE SUPERVISION OF DR. MARY PRYCE AND PROF. CONOR LONG SCHOOL OF CHEMICAL SCIENCES FEBRUARY-2003 DECLARATION I hereby certify that this thesis, which I now submit for assessment on the programme of study leading to the award of Doctor of Philosophy is entirely my own work and has not been taken from the work of others save and to the extent that such work has been cited and acknowledged within the text of my work Signed :________________________ Date :_________________________ Peter Brennan Student ID No. 97970646 Table of contents Page Title i Declaration ii Table of contents iii Acknowledgements ix Abstract x Chapter 1 Literature survey 1.1 Introduction to the chemistry of organometallic complexes 2 1.2 UV/vis monitored flash photolysis 8 1.3 Time Resolved InfraRed (TRIR) Spectroscopy 10 1.3.1 Step scan TRIR spectroscopy 10 1.3.2 Point by point TRIR 12 1.4 Matrix isolation 14 1.5 Bonding in M-CO complexes 19 1.6 Metal - Arene bonding 24 1.7 The electronic absorption spectra of (fi6-arene)Cr(CO)3 complexes 26 1.8 Photochemistry of (ri6-arene)M(CO)3 complexes 27 1.9 Photochemistry of (r|S-CsHs)Mn(CO)3 complexes 32 1.10 Arene exchange reactions 35 1.11 Ring slippage reactions 41 1.12 The Indenyl ligand effect 43 1.13 References 46 Chapter 2 The photochemistry of substituted arene metal carbonyls 2.1 Introduction to the photochemistry -
Ligand Substitution Processes
Ligand Substitution Processes COOPER H. LANGFORD, Amherst College HARRY B. GRAY, Columbia University W. A. Benjamin, Inc. NEW YORK AMSTERDAM Ligand Substitution Processes Copyright @ 1966 by W. A. Benjamin, Inc. All rights reserved Library of Congress Catalog Card Number 66-12702 Manufactured in the United States of America The manuscript was put into firoduction on 7 July 1.965; this book was published on 70 March 7966 W. A. Benjamin, Inc. New York, New York 10016 Page 1 of 2 George Porter From: Dana Roth Sent: Tuesday, May 02, 2006 9:51 AM To: George Porter Subject: FW: An online version of Ligand Substitution Processes? From: Harry Gray [mailto:[email protected]] Sent: Monday, May 01, 2006 5:44 PM To: Dana Roth Subject: Re: An online version of Ligand Substitution Processes? Dana! Great! Of course you have my permission. It will be good to have LSP in CODA. Thanks, and all the best, Harry At 03:48 PM 5/1/2006, you wrote: Harry: The library has an on-going project of adding Caltech author's books to Caltech Collection of Open Digital Archives (CODA) I notice that you are the copyright holder of: RE-687-085 (COHM) Ligand substitution processes. By Harry Barkus Gray & Cooper H. Langford. Claimant: acHarry Barkus Gray (A) Effective Registration Date: 30Dec94 Original Registration Date: 10Mar66; With you permission, I can have this scanned and announce its public availability. We have done this for 3 of Jack Roberts' books (for which he is the copyright holder): 5/6/2006 Page 2 of 2 Nuclear Magnetic Resonance: applications to organic chemistry, 1959 http://resolver.caltech.edu/CaltechBOOK:1959.001 Notes on Molecular Orbital Calculations, 1961 http://resolver.caltech.edu/CaltechBOOK:1961.001 An introduction to the analysis of spin-spin splitting in high-resolution nuclear magnetic resonance spectra, 1961 http://resolver.caltech.edu/CaltechBOOK:1961.002 Dana L. -
Fluxionality and Isomerism of the Bis(Dihydrogen) Complex Ruh2(H2)2(Pcy3)2: INS, NMR, and Theoretical Studies
Inorg. Chem. 1998, 37, 3475-3485 3475 Fluxionality and Isomerism of the Bis(dihydrogen) Complex RuH2(H2)2(PCy3)2: INS, NMR, and Theoretical Studies Venancio Rodriguez, Sylviane Sabo-Etienne, and Bruno Chaudret* Laboratoire de Chimie de Coordination du CNRS, 205 Route de Narbonne, 31077 Toulouse Cedex 4, France John Thoburn, Stefan Ulrich, and Hans-Heinrich Limbach Institut fu¨r Organische Chemie, Fachbereich Chemie, Freie Universita¨t Berlin, Takustrasse 3, D-14195 Berlin 33, Germany Juergen Eckert Manuel Lujan, Jr., Neutron Scattering Center (LANSCE), Los Alamos National Laboratory, Los Alamos, New Mexico 87545 Jean-Claude Barthelat, Khansaa Hussein,† and Colin J. Marsden Laboratoire de Physique Quantique, UMR IRSAMC-CNRS UMR 5626, Universite´ Paul Sabatier, 118 Route de Narbonne, 31062 Toulouse Cedex 4, France ReceiVed June 5, 1997 To study the fluxionality of the bis(dihydrogen) complex RuH2(H2)2(PCy3)2 (1), NMR spectra were recorded in Freons (mixture of CDCl3, CDFCl2, and CDF2Cl). 1 was found to remain fluxional at all temperatures, but the presence of CDCl3 necessary for its solubilization induces its transformation into, first, RuHCl(H2)2(PCy3)2 (3) and the new ruthenium(IV) dihydride RuH2Cl2(PCy3)2 (4). 4 is produced selectively in pure CDCl3 but reacts further to give a mixture of chloro complexes. 4 was isolated from the reaction of 1 with aqueous HCl in Et2O and shows a fluxional process attributed to the interconversion between two symmetrical isomers. The activation parameters of this process were obtained by 1H NMR line shape analysis, as well as those corresponding to the exchange between 3 and free dihydrogen. -
Reaction Mechanism of Transition Metal Complexes
CHAPTER 3 Reaction Mechanism of Transition Metal Complexes – I: Inert and Labile Complexes The metal complexes in which the rate of ligand displacement reactions is very fast and hence show high reactivity are called as labile Complexes and this property is termed as lability. On the other hand, the metal complexes in which the rate of ligand displacement reactions is very slow and hence show less reactivity are called as inert complexes and this property is termed as inertness. Thermodynamic stability is the measure of the extent to which the complex will form or will be transformed into another complex when the system has reached equilibrium while kinetic stability refers to the speeds at which these transformations take place. The thermodynamic stability depends upon the energy difference of the reactant and product if the product has less energy than that of the reactant, it will be more stable than the reactant. The thermodynamic stability of metal complexes is calculated by the overall formation constant. If the value of log β is more than 8, the complex is considered as thermodynamically stable. Figure 1. The general reaction coordinates diagram. The kinetic stability of the complex depends upon the activation energy of the reaction. If the activation energy barrier is low, the reaction will take place at a higher speed. These types of complexes are also called as kinetically unstable. If the activation energy barrier is high, the substance will react slowly and will be called as kinetically stabilized or inert. There is no correlation between thermodynamic and kinetic stability. Thermodynamically stable products may labile or inert and the vice versa is also true. -
Dissociative Ligand Substitution
Dissociative Ligand Substitution Associative substitution is unlikely for saturated, 18-electron complexes—coordination of another ligand would produce a 20-electron intermediate. For 18-electron complexes, dissociative substitution mechanisms involving 16- electron intermediates are more likely. In a slow step with positive entropy of activation, the departing ligand leaves, generating a coordinatively unsaturated intermediate. The incoming ligand then enters the coordination sphere of the metal to generate the product. For the remainder of this post, we’ll focus on the kinetics of the reaction and the nature of the unsaturated intermediate (which influences the stereochemistry of the reaction). The reverse of the first step, re-coordination of the departing ligand (rate constant k–1), is often competitive with dissociation. A general scheme for dissociative ligand substitution. There’s more to the intermediate than meets the eye! Reaction Kinetics Let’s begin with the general situation in which k1 and k–1 are similar in magnitude. Since k1 is rate limiting, k2 is assumed to be much larger than k1 and k–1. Most importantly, we need to assume that variation in the concentration of the unsaturated intermediate is essentially zero. This is called the steady state approximation, and it allows us to set up an equation that relates reaction rate to observable concentrations Hold onto that for a second; first, we can use step 2 to establish a preliminary rate expression. (1) rate = k2[LnM–◊][Li] Of course, the unsaturated complex is present in very small concentration and is unmeasurable, so this equation doesn’t help us much. We need to remove the concentration of the unmeasurable intermediate from (1), and the steady state approximation helps us do this.