Exercise 1 Q.2 the Gas Is Cooled Such That It Loses 65 J of Heat
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Chapter 3. Second and Third Law of Thermodynamics
Chapter 3. Second and third law of thermodynamics Important Concepts Review Entropy; Gibbs Free Energy • Entropy (S) – definitions Law of Corresponding States (ch 1 notes) • Entropy changes in reversible and Reduced pressure, temperatures, volumes irreversible processes • Entropy of mixing of ideal gases • 2nd law of thermodynamics • 3rd law of thermodynamics Math • Free energy Numerical integration by computer • Maxwell relations (Trapezoidal integration • Dependence of free energy on P, V, T https://en.wikipedia.org/wiki/Trapezoidal_rule) • Thermodynamic functions of mixtures Properties of partial differential equations • Partial molar quantities and chemical Rules for inequalities potential Major Concept Review • Adiabats vs. isotherms p1V1 p2V2 • Sign convention for work and heat w done on c=C /R vm system, q supplied to system : + p1V1 p2V2 =Cp/CV w done by system, q removed from system : c c V1T1 V2T2 - • Joule-Thomson expansion (DH=0); • State variables depend on final & initial state; not Joule-Thomson coefficient, inversion path. temperature • Reversible change occurs in series of equilibrium V states T TT V P p • Adiabatic q = 0; Isothermal DT = 0 H CP • Equations of state for enthalpy, H and internal • Formation reaction; enthalpies of energy, U reaction, Hess’s Law; other changes D rxn H iD f Hi i T D rxn H Drxn Href DrxnCpdT Tref • Calorimetry Spontaneous and Nonspontaneous Changes First Law: when one form of energy is converted to another, the total energy in universe is conserved. • Does not give any other restriction on a process • But many processes have a natural direction Examples • gas expands into a vacuum; not the reverse • can burn paper; can't unburn paper • heat never flows spontaneously from cold to hot These changes are called nonspontaneous changes. -
UNITS This Appendix Explains Some of the Abbreviations1•2 Used For
APPENDIX: UNITS This appendix explains some of the abbreviations1•2 used for units in this book and gives conversion factors to SI units and atomic units: length 1 a0 = 1 bohr = 0.5291771 X 10-10 m 1 A= 1 Angstrom= lo-10 m = 1.889727 ao mass 1 me = 1 atomic unit of mass = mass of an electron 9.109534 X 10-31 kg = 5.485803 X 10-4 U 1 u 1 universal atomic mass unit = one twelfth the mass of a 12c atom 1.6605655 x lo-27 kg = 1822.887 me time 1 t Eh 1 = 1 atomic unit of time = 2.418884 x l0-17 s 1 s = 1 second = 4.134137 x 1016 t/Eh temperature 1 K = 1 Kelvin amount of substance 1 mol = 1 mole 6.022045 x 1023 atoms, molecules, or formula units energy 1 cm-1 = 1 wavenumber 1 kayser 1.986477 x lo-23 J 4.556335 x 10-6 Eh 857 858 APPENDIX: UNITS 1 kcal/mol = 1 kilocalorie per mole 4.184 kJ/mol = 1.593601 x 10-3 Eh 1 eV 1 electron volt = 1.602189 x lo-19 J 3.674902 X 10-2 Eh 1 Eh 1 hartree = 4.359814 x lo-18 J Since so many different energy units are used in the book, it is helpful to have a conversion table. Such a table was calculated from the recommended values of Cohen and Taylor3 for the physical censtants and is given in Table 1. REFERENCES 1. "Standard for Metric Practice", American Society for Testing and Materials, Philadelphia (1976). -
A Mathematical and Computational Review of Hartree-Fock SCF
February 1, 2008 5:24 Molecular Physics introSCF Molecular Physics, Vol. 00, No. 00, DD Month 200x, 1–64 A mathematical and computational review of Hartree-Fock SCF methods in Quantum Chemistry Pablo Echenique∗ and J. L. Alonso †‡ †‡ Departamento de F´ısica Te´orica, Universidad de Zaragoza, † Pedro Cerbuna 12, 50009, Zaragoza, Spain. Instituto de Biocomputaci´on y F´ısica de los Sistemas Complejos (BIFI), ‡ Edificio Cervantes, Corona de Arag´on 42, 50009, Zaragoza, Spain. (May 2007 ) We present here a review of the fundamental topics of Hartree-Fock theory in Quantum Chemistry. From the molecular Hamiltonian, using and discussing the Born-Oppenheimer ap- proximation, we arrive to the Hartree and Hartree-Fock equations for the electronic problem. Special emphasis is placed in the most relevant mathematical aspects of the theoretical deriva- tion of the final equations, as well as in the results regarding the existence and uniqueness of their solutions. All Hartree-Fock versions with different spin restrictions are systematically extracted from the general case, thus providing a unifying framework. Then, the discretization of the one-electron orbitals space is reviewed and the Roothaan-Hall formalism introduced. This leads to a exposition of the basic underlying concepts related to the construction and selection of Gaussian basis sets, focusing in algorithmic efficiency issues. Finally, we close the review with a section in which the most relevant modern developments (specially those related to the design of linear-scaling methods) are commented and linked to the issues discussed. The whole work is intentionally introductory and rather self-contained, so that it may be useful for non experts that aim to use quantum chemical methods in interdisciplinary applications. -
Estimation of Internal Pressure of Liquids and Liquid Mixtures
Available online at www.ilcpa.pl International Letters of Chemistry, Physics and Astronomy 5 (2012) 1-7 ISSN 2299-3843 Estimation of internal pressure of liquids and liquid mixtures N. Santhi 1, P. Sabarathinam 2, G. Alamelumangai 1, J. Madhumitha 1, M. Emayavaramban 1 1Department of Chemistry, Government Arts College, C.Mutlur, Chidambaram-608102, India 2Retd. Registrar & Head of the Department of Technology, Annamalai University, Annamalainagar-608002, India E-mail address: [email protected] ABSTRACT By combining the van der Waals’ equation of state and the Free Length Theory of Jacobson, a new theoretical model is developed for the prediction of internal pressure of pure liquids and liquid mixtures. It requires only the molar volume data in addition to the ratio of heat capacities and critical temperature. The proposed model is simple, reliably accurate and capable of predicting internal pressure of pure liquids with an average absolute deviation of 4.24% in the predicted internal pressure values compared to those given in literature. The average absolute deviation in the predicted internal pressure values through the proposed model for the five binary liquid mixtures tested varies from 0.29% to 1.9% when compared to those of literature values. Keywords: van der Waals, pressure of liquids, theory of Jacobson, capacity of heat liquids, equation of Srivastava and Berkowitz 1. INTRODUTION The importance of internal pressure in understanding the properties of liquids and the full potential of internal pressure as a structural probe did become apparent with the pioneering work of Hildebrand 1, 2 and the first review of the subject by Richards 3 appeared in 1925. -
The Carnot Cycle, Reversibility and Entropy
entropy Article The Carnot Cycle, Reversibility and Entropy David Sands Department of Physics and Mathematics, University of Hull, Hull HU6 7RX, UK; [email protected] Abstract: The Carnot cycle and the attendant notions of reversibility and entropy are examined. It is shown how the modern view of these concepts still corresponds to the ideas Clausius laid down in the nineteenth century. As such, they reflect the outmoded idea, current at the time, that heat is motion. It is shown how this view of heat led Clausius to develop the entropy of a body based on the work that could be performed in a reversible process rather than the work that is actually performed in an irreversible process. In consequence, Clausius built into entropy a conflict with energy conservation, which is concerned with actual changes in energy. In this paper, reversibility and irreversibility are investigated by means of a macroscopic formulation of internal mechanisms of damping based on rate equations for the distribution of energy within a gas. It is shown that work processes involving a step change in external pressure, however small, are intrinsically irreversible. However, under idealised conditions of zero damping the gas inside a piston expands and traces out a trajectory through the space of equilibrium states. Therefore, the entropy change due to heat flow from the reservoir matches the entropy change of the equilibrium states. This trajectory can be traced out in reverse as the piston reverses direction, but if the external conditions are adjusted appropriately, the gas can be made to trace out a Carnot cycle in P-V space. -
Pressure Vessels
PRESSURE VESSELS David Roylance Department of Materials Science and Engineering Massachusetts Institute of Technology Cambridge, MA 02139 August 23, 2001 Introduction A good deal of the Mechanics of Materials can be introduced entirely within the confines of uniaxially stressed structural elements, and this was the goal of the previous modules. But of course the real world is three-dimensional, and we need to extend these concepts accordingly. We now take the next step, and consider those structures in which the loading is still simple, but where the stresses and strains now require a second dimension for their description. Both for their value in demonstrating two-dimensional effects and also for their practical use in mechanical design, we turn to a slightly more complicated structural type: the thin-walled pressure vessel. Structures such as pipes or bottles capable of holding internal pressure have been very important in the history of science and technology. Although the ancient Romans had developed municipal engineering to a high order in many ways, the very need for their impressive system of large aqueducts for carrying water was due to their not yet having pipes that could maintain internal pressure. Water can flow uphill when driven by the hydraulic pressure of the reservoir at a higher elevation, but without a pressure-containing pipe an aqueduct must be constructed so the water can run downhill all the way from the reservoir to the destination. Airplane cabins are another familiar example of pressure-containing structures. They illus- trate very dramatically the importance of proper design, since the atmosphere in the cabin has enough energy associated with its relative pressurization compared to the thin air outside that catastrophic crack growth is a real possibility. -
CHAPTER 17 Internal Pressure and Internal Energy of Saturated and Compressed Phases Ainstitute of Physics of the Dagestan Scient
CHAPTER 17 Internal Pressure and Internal Energy of Saturated and Compressed Phases ILMUTDIN M. ABDULAGATOV,a,b JOSEPH W. MAGEE,c NIKOLAI G. POLIKHRONIDI,a RABIYAT G. BATYROVAa aInstitute of Physics of the Dagestan Scientific Center of the Russian Academy of Sciences, Makhachkala, Dagestan, Russia. E-mail: [email protected] bDagestan State University, Makhachkala, Dagestan, Russia cNational Institute of Standards and Technology, Boulder, Colorado 80305 USA. E- mail: [email protected] Abstract Following a critical review of the field, a comprehensive analysis is provided of the internal pressure of fluids and fluid mixtures and its determination in a wide range of temperatures and pressures. Further, the physical meaning is discussed of the internal pressure along with its microscopic interpretation by means of calorimetric experiments. A new relation is explored between the internal pressure and the isochoric heat capacity jump along the coexistence curve near the critical point. Various methods (direct and indirect) of internal pressure determination are discussed. Relationships are studied between the internal pressure and key thermodynamic properties, namely expansion coefficient, isothermal compressibility, speed of sound, enthalpy increments, and viscosity. Loci of isothermal, isobaric, and isochoric internal pressure maxima and minima were examined in addition to the locus of zero internal pressure. Details were discussed of the new method of direct internal pressure determination by a calorimetric experiment that involves simultaneous measurement of the thermal pressure coefficient (∂P / ∂T )V , i.e. internal pressure Pint = (∂U / ∂V )T and heat capacity cV = (∂U / ∂T )V . The dependence of internal pressure on external pressure, temperature and density for pure fluids, and on concentration for binary mixtures is considered on the basis of reference (NIST REFPROP) and crossover EOS. -
Ideal Gas Temperature.)
FUNDAMENTALS OF CLASSICAL AND STATISTICAL THERMODYNAMICS SPRING 2005 1 1. Basic Concepts of Thermodynamics The basic concepts of thermodynamics such as system, energy, property, state, process, cycle, pressure, and temperature are explained. Thermodynamics can be defined as the science of energy. Energy can be viewed as the ability to cause changes. Thermodynamics is concerned with the transfer of heat and the appearance or disappearance of work attending various chemical and physical processes. • The natural phenomena that occur about us; • Controlled chemical reactions; • The performance of engines • Hypothetical processes such as chemical reactions that do not occur but can be imagined. HISTORY: Thermodynamics emerged as a science with the construction of the first successful atmospheric steam engines in England by Thomas Savery in 1697 and Thomas Newcomen in 1712. These engines were very slow and inefficient, but they opened the way for the development of a new science. The first and second laws of thermodynamics emerged 2 simultaneously in the 1850s primarily out of the works of William Rankine, Rudolph Clausius, and Lord Kelvin (formerly William Thomson). The term thermodynamics was first used in a publication by Lord Kelvin in 1849. The first thermodynamic textbook was written in 1859 by William Rankine, a professor at the University of Glasgow. 3 Classical vs. Statistical Thermodynamics Substances consist of large number of particles called molecules. The properties of the substance naturally depend on the behavior of these particles. For example, the pressure of a gas in a container is the result of momentum transfer between the molecules and the walls of the container. -
Lecture452 2 12.Pdf
University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2012 Lecture 2. 6/20/12 A. Differentials and State Functions • Thermodynamics allows us to calculate energy transformations occurring in systems composed of large numbers of particles, systems so complex as to make rigorous mechanical calculations impractical. • The limitation is that thermodynamics does not allow us to calculate trajectories. We can only calculate energy changes that occur when a system passes from one equilibrium state to another. • In thermodynamics, we do not calculate the internal energy U. We calculate the change in internal energy ∆U, taken as the difference between the internal energy of the initial equilibrium state and the internal energy of the final equilibrium state: ∆=UUfinal − U initial • The internal energy U belongs to a class of functions called state functions. State function changes ∆F are only dependent on the initial state of the system, described by Pinitial, Vinitial, Tinitial, ninitial, and the final state of the system, described by Pfinal, Vfinal, Tfinal, and nfinal. State function changes do not depend upon the details of the specific path followed (i.e. the trajectory). • Quantities that are path-dependent are not state functions. • Thermodynamic state functions are functions of several state variables including P, V, T, and n. changes in the state variable n is are not considered at present. We will concentrate at first on single component/single phase systems with no loss or gain of material. Of the three remaining state variables P, V, T only two are independent because of the constraint imposed by the equation of state. -
3. the First Law of Thermodynamics and Related Definitions
09/30/08 1 3. THE FIRST LAW OF THERMODYNAMICS AND RELATED DEFINITIONS 3.1 General statement of the law Simply stated, the First Law states that the energy of the universe is constant. This is an empirical conservation principle (conservation of energy) and defines the term "energy." We will also see that "internal energy" is defined by the First Law. [As is always the case in atmospheric science, we will ignore the Einstein mass-energy equivalence relation.] Thus, the First Law states the following: 1. Heat is a form of energy. 2. Energy is conserved. The ways in which energy is transformed is of interest to us. The First Law is the second fundamental principle in (atmospheric) thermodynamics, and is used extensively. (The first was the equation of state.) One form of the First Law defines the relationship among work, internal energy, and heat input. In this chapter (and in subsequent chapters), we will explore many applications derived from the First Law and Equation of State. 3.2 Work of expansion If a system (parcel) is not in mechanical (pressure) equilibrium with its surroundings, it will expand or contract. Consider the example of a piston/cylinder system, in which the cylinder is filled with a gas. The cylinder undergoes an expansion or compression as shown below. Also shown in Fig. 3.1 is a p-V thermodynamic diagram, in which the physical state of the gas is represented by two thermodynamic variables: p,V in this case. [We will consider this and other types of thermodynamic diagrams in more detail later. -
Energy Analysis of Chemistry for Correct Insertion by DNA Polymerase 
Energy analysis of chemistry for correct insertion by DNA polymerase  Ping Lin†, Lars C. Pedersen‡, Vinod K. Batra‡, William A. Beard‡, Samuel H. Wilson‡, and Lee G. Pedersen†‡§ †Department of Chemistry, University of North Carolina, Chapel Hill, NC 27599; and ‡Laboratory of Structural Biology, National Institute of Environmental Health Sciences, National Institutes of Health, P.O. Box 12233, Research Triangle Park, NC 27709-2233 Communicated by Robert G. Parr, University of North Carolina, Chapel Hill, NC, July 19, 2006 (received for review March 8, 2006) X-ray crystallographic structures of human DNA polymerase  with transition-state (TS) theory applied to an enzyme-catalyzed nonhydrolyzable analogs containing all atoms in the active site reaction (27) and an insertion rate constant of 10 sϪ1 measured required for catalysis provide a secure starting point for a theo- for gapped DNA (28), the apparent free energy of activation is retical analysis (quantum mechanics͞molecular mechanics) of the estimated to be 16.1 kcal (1 kcal ϭ 4.18 kJ)͞mol at room mechanism of chemistry without biasing of modeling assumptions temperature. Although there is some debate about the extent to as required in previous studies. These structures provide the basis which a conformational change or the chemical reaction is the for a detailed quantum mechanics͞molecular mechanics study of rate-limiting step (29), we may use this value for comparison with the path for the complete transfer of a monophosphate nucleoside our calculated reaction energy barrier. donor to the sugar acceptor in the active site. The reaction is largely The development of combined quantum mechanics (QM) and associative with the main energetic step preceded by proton molecular mechanics (MM) methods provides tools for investi- transfer from the terminal primer deoxyribose O3 to Asp-256. -
Hydrogen Fluoride and the Thermochemistry of Fluorine
Jmxutm ' *•* ft 9 fi HI I '! fi£ HH 4 • acL I V'.. ^HH 9 HI jamH ; <v IfaflonaJ Bureau of Standard', Library, E-01 Admin. Bldg. KITED STATES URTMENT OF MAR 2 8 1970 MMERCE LICATION NBS TECHNICAL NOTE 513 8E~ -, I <^sk? Hydrogen Fluoride and the Thermochemistry of Fluorine U.S. :partment OF COMMERCE National Bureau of Standards - NATIONAL BUREAU OF STANDARDS The National Bureau of Standards ' was established by an act of Congress March 3, 1901. Today, in addition to serving as the Nation's central measurement laboratory, the Bureau is a principal focal point in the Federal Government for assuring maximum application of the physical and engineering sciences to the advancement of technology in industry and commerce. To this end the Bureau conducts research and provides central national services in four broad program areas. These are: (1) basic measurements and standards, (2) materials measurements and standards, (3) technological measurements and standards, and (4) transfer of technology. The Bureau comprises the Institute for Basic Standards, the Institute for Materials Research, the Institute for Applied Technology, the Center for Radiation Research, the Center for Computer Sciences and Technology, and the Office for Information Programs. THE INSTITUTE FOR BASIC STANDARDS provides the central basis within the United States of a complete and consistent system of physical measurement; coordinates that system with measurement systems of other nations; and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation's scientific community, industry, and com- merce. The Institute consists of an Office of Measurement Services and the following technical divisions: Applied Mathematics—Electricity—Metrology—Mechanics—Heat—Atomic and Molec- ular Physics—Radio Physics -—Radio Engineering -'—Time and Frequency -—Astro- physics -—Cryogenics.