Chapter 4 Solution Theory
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Thermodynamics, Flame Temperature and Equilibrium
Thermodynamics, Flame Temperature and Equilibrium Combustion Summer School 2018 Prof. Dr.-Ing. Heinz Pitsch Course Overview Part I: Fundamentals and Laminar Flames • Introduction • Fundamentals and mass balances of combustion systems • Thermodynamic quantities • Thermodynamics, flame • Flame temperature at complete temperature, and equilibrium conversion • Governing equations • Chemical equilibrium • Laminar premixed flames: Kinematics and burning velocity • Laminar premixed flames: Flame structure • Laminar diffusion flames • FlameMaster flame calculator 2 Thermodynamic Quantities First law of thermodynamics - balance between different forms of energy • Change of specific internal energy: du specific work due to volumetric changes: δw = -pdv , v=1/ρ specific heat transfer from the surroundings: δq • Related quantities specific enthalpy (general definition): specific enthalpy for an ideal gas: • Energy balance for a closed system: 3 Multicomponent system • Specific internal energy and specific enthalpy of mixtures • Relation between internal energy and enthalpy of single species 4 Multicomponent system • Ideal gas u and h only function of temperature • If cpi is specific heat at constant pressure and hi,ref is reference enthalpy at reference temperature Tref , temperature dependence of partial specific enthalpy is given by • Reference temperature may be arbitrarily chosen, most frequently used: Tref = 0 K or Tref = 298.15 K 5 Multicomponent system • Partial molar enthalpy hi,m is and its temperature dependence is where the molar specific -
Homework 5 Solutions
SCI 1410: materials science & solid state chemistry HOMEWORK 5. solutions Textbook Problems: Imperfections in Solids 1. Askeland 4-67. Why is most “gold” or “silver” jewelry made out of gold or silver alloyed with copper, i.e, what advantages does copper offer? We have two major considerations in jewelry alloying: strength and cost. Copper additions obviously lower the cost of gold or silver (Note that 14K gold is actually only about 50% gold). Copper and other alloy additions also strengthen pure gold and pure silver. In both gold and silver, copper will strengthen the material by either solid solution strengthening (substitutional Cu atoms in the Au or Ag crystal), or by formation of second phase in the microstructure. 2. Solid state solubility. Of the elements in the chart below, name those that would form each of the following relationships with copper (non-metals only have atomic radii listed): a. Substitutional solid solution with complete solubility o Ni and possibly Ag, Pd, and Pt b. Substitutional solid solution of incomplete solubility o Ag, Pd, and Pt (if you didn’t include these in part (a); Al, Co, Cr, Fe, Zn c. An interstitial solid solution o C, H, O (small atomic radii) Element Atomic Radius (nm) Crystal Structure Electronegativity Valence Cu 0.1278 FCC 1.9 +2 C 0.071 H 0.046 O 0.060 Ag 0.1445 FCC 1.9 +1 Al 0.1431 FCC 1.5 +3 Co 0.1253 HCP 1.8 +2 Cr 0.1249 BCC 1.6 +3 Fe 0.1241 BCC 1.8 +2 Ni 0.1246 FCC 1.8 +2 Pd 0.1376 FCC 2.2 +2 Pt 0.1387 FCC 2.2 +2 Zn 0.1332 HCP 1.6 +2 3. -
Chapter 15: Solutions
452-487_Ch15-866418 5/10/06 10:51 AM Page 452 CHAPTER 15 Solutions Chemistry 6.b, 6.c, 6.d, 6.e, 7.b I&E 1.a, 1.b, 1.c, 1.d, 1.j, 1.m What You’ll Learn ▲ You will describe and cate- gorize solutions. ▲ You will calculate concen- trations of solutions. ▲ You will analyze the colliga- tive properties of solutions. ▲ You will compare and con- trast heterogeneous mixtures. Why It’s Important The air you breathe, the fluids in your body, and some of the foods you ingest are solu- tions. Because solutions are so common, learning about their behavior is fundamental to understanding chemistry. Visit the Chemistry Web site at chemistrymc.com to find links about solutions. Though it isn’t apparent, there are at least three different solu- tions in this photo; the air, the lake in the foreground, and the steel used in the construction of the buildings are all solutions. 452 Chapter 15 452-487_Ch15-866418 5/10/06 10:52 AM Page 453 DISCOVERY LAB Solution Formation Chemistry 6.b, 7.b I&E 1.d he intermolecular forces among dissolving particles and the Tattractive forces between solute and solvent particles result in an overall energy change. Can this change be observed? Safety Precautions Dispose of solutions by flushing them down a drain with excess water. Procedure 1. Measure 10 g of ammonium chloride (NH4Cl) and place it in a Materials 100-mL beaker. balance 2. Add 30 mL of water to the NH4Cl, stirring with your stirring rod. -
Self-Assembly of a Colloidal Interstitial Solid Solution with Tunable Sublattice Doping: Supplementary Information
Self-assembly of a colloidal interstitial solid solution with tunable sublattice doping: Supplementary information L. Filion,∗ M. Hermes, R. Ni, E. C. M. Vermolen,† A. Kuijk, C. G. Christova,‡ J. C. P. Stiefelhagen, T. Vissers, A. van Blaaderen, and M. Dijkstra Soft Condensed Matter, Debye Institute for NanoMaterials Science, Utrecht University, Princetonplein 1, NL-3584 CC Utrecht, the Netherlands I. CRYSTAL STRUCTURE LS6 In the main paper we use full free-energy calculations to determine the phase diagram for binary mixtures of hard spheres with size ratio σS/σL = 0.3 where σS(L) is the diameter of the small (large) particles. The phases we considered included a structure with LS6 stoichiometry for which we could not identify an atomic analogue. Snapshots of this structure from various perspectives are shown in Fig. S1. FIG. S1: Unit cell of the binary LS6 superlattice structure described in this paper. Note that both species exhibit long-range crystalline order. The unit cell is based on a body-centered-cubic cell of the large particles in contrast to the face-centered-cubic cell associated with the interstitial solid solution covering most of the phase diagram (Fig. 1). II. PHASE DIAGRAM AT CONSTANT VOLUME 3 In the main paper, we present the xS − p representation of the phase diagram where p = βPσL is the reduced pressure, xS = NS/(NS + NL), NS(L) is the number of small (large) hard spheres, β = 1/kBT , kB is the Boltzmann constant, and T is the absolute temperature. This is the natural representation arising from common tangent construc- tions at constant pressure and the representation required for further simulation studies such as nucleation studies. -
Solid Solution Softening and Enhanced Ductility in Concentrated FCC Silver Solid Solution Alloys
UC Irvine UC Irvine Previously Published Works Title Solid solution softening and enhanced ductility in concentrated FCC silver solid solution alloys Permalink https://escholarship.org/uc/item/7d05p55k Authors Huo, Yongjun Wu, Jiaqi Lee, Chin C Publication Date 2018-06-27 DOI 10.1016/j.msea.2018.05.057 Peer reviewed eScholarship.org Powered by the California Digital Library University of California Materials Science & Engineering A 729 (2018) 208–218 Contents lists available at ScienceDirect Materials Science & Engineering A journal homepage: www.elsevier.com/locate/msea Solid solution softening and enhanced ductility in concentrated FCC silver T solid solution alloys ⁎ Yongjun Huoa,b, , Jiaqi Wua,b, Chin C. Leea,b a Electrical Engineering and Computer Science University of California, Irvine, CA 92697-2660, United States b Materials and Manufacturing Technology University of California, Irvine, CA 92697-2660, United States ARTICLE INFO ABSTRACT Keywords: The major adoptions of silver-based bonding wires and silver-sintering methods in the electronic packaging Concentrated solid solutions industry have incited the fundamental material properties research on the silver-based alloys. Recently, an Solid solution softening abnormal phenomenon, namely, solid solution softening, was observed in stress vs. strain characterization of Ag- Twinning-induced plasticity In solid solution. In this paper, the mechanical properties of additional concentrated silver solid solution phases Localized homologous temperature with other solute elements, Al, Ga and Sn, have been experimentally determined, with their work hardening Advanced joining materials behaviors and the corresponding fractography further analyzed. Particularly, the concentrated Ag-Ga solid so- lution has been discovered to possess the best combination of mechanical properties, namely, lowest yield strength, highest ductility and highest strength, among the concentrated solid solutions of the current study. -
Chapter 18 Solutions and Their Behavior
Chapter 18 Solutions and Their Behavior 18.1 Properties of Solutions Lesson Objectives The student will: • define a solution. • describe the composition of solutions. • define the terms solute and solvent. • identify the solute and solvent in a solution. • describe the different types of solutions and give examples of each type. • define colloids and suspensions. • explain the differences among solutions, colloids, and suspensions. • list some common examples of colloids. Vocabulary • colloid • solute • solution • solvent • suspension • Tyndall effect Introduction In this chapter, we begin our study of solution chemistry. We all might think that we know what a solution is, listing a drink like tea or soda as an example of a solution. What you might not have realized, however, is that the air or alloys such as brass are all classified as solutions. Why are these classified as solutions? Why wouldn’t milk be classified as a true solution? To answer these questions, we have to learn some specific properties of solutions. Let’s begin with the definition of a solution and look at some of the different types of solutions. www.ck12.org 394 E-Book Page 402 Homogeneous Mixtures A solution is a homogeneous mixture of substances (the prefix “homo-” means “same”), meaning that the properties are the same throughout the solution. Take, for example, the vinegar that is used in cooking. Vinegar is approximately 5% acetic acid in water. This means that every teaspoon of vinegar contains 5% acetic acid and 95% water. When a solution is said to have uniform properties, the definition is referring to properties at the particle level. -
Calculation of Chemical Potential and Activity Coefficient of Two Layers of Co2 Adsorbed on a Graphite Surface
Physical Chemistry Chemical Physics CALCULATION OF CHEMICAL POTENTIAL AND ACTIVITY COEFFICIENT OF TWO LAYERS OF CO2 ADSORBED ON A GRAPHITE SURFACE Journal: Physical Chemistry Chemical Physics Manuscript ID: CP-ART-08-2014-003782.R1 Article Type: Paper Date Submitted by the Author: 07-Nov-2014 Complete List of Authors: Trinh, Thuat; NTNU, Department of Chemistry Bedeaux, Dick; NTNU, Chemistry Simon, Jean-Marc; Universit� de Bourgogne, Chemistry Kjelstrup, Signe; Norwegian University of Science and Technology, Natural Sciences Page 1 of 8 Physical Chemistry Chemical Physics PCCP RSC Publishing ARTICLE CALCULATION OF CHEMICAL POTENTIAL AND ACTIVITY COEFFICIENT OF TWO LAYERS Cite this: DOI: 10.1039/x0xx00000x OF CO2 ADSORBED ON A GRAPHITE SURFACE T.T. Trinh,a D. Bedeaux a , J.-M Simon b and S. Kjelstrup a,c,* Received 00th January 2014, Accepted 00th January 2014 We study the adsorption of carbon dioxide at a graphite surface using the new Small System DOI: 10.1039/x0xx00000x Method, and find that for the temperature range between 300K and 550K most relevant for CO separation; adsorption takes place in two distinct thermodynamic layers defined according www.rsc.org/ 2 to Gibbs. We calculate the chemical potential, activity coefficient in both layers directly from the simulations. Based on thermodynamic relations, the entropy and enthalpy of the CO 2 adsorbed layers are also obtained. Their values indicate that there is a trade-off between entropy and enthalpy when a molecule chooses for one of the two layers. The first layer is a densely packed monolayer of relatively constant excess density with relatively large repulsive interactions and negative enthalpy. -
Solid-Liquid Partition Coefficients, Rcjs: What's the Value and When Does It Matter?
Radioprotection - Colloques, volume 37, Cl (2002) Cl-225 Solid-liquid partition coefficients, rCjs: What's the value and when does it matter? M.I. Sheppard and S.C. Sheppard ECOMatters, 24 Aberdeen Avenue, P.O. Box 430, Pinawa, Manitoba ROE 1L0, Canada Abstract. Environmental risk assessments binge on our ability to predict the fete and mobility of radionuclides and metals in terrestrial soils and aquatic sediments. Solid-solution partitioning (the Kd approach), despite its shortcomings, has been used extensively. Much attention has been devoted to grooming the existing key compendia for values applicable for each nuclear risk assessment carried out worldwide. This appears to be an important task. For example, soil Kd values for a single nuclide can vary over several orders of magnitude, yet the soil Kd value is the most important parameter in the soil leaching model. Similarly, plant uptake depends primarily on the nuclide present in solution phase. Despite this apparent sensitivity, our experience has shown that risk assessors dwell too much on the precision of the Kd value for all nuclides. This paper discusses the effect of the Kd value on the resulting soil concentration during leaching and identifies those radionuclides and assessment conditions where a precise value is required. Only those radionuclides that typically have a soil Kd value of 10 LAg or less (Tc, CL I, As) need be accurately described for timeframes of up to 10,000 years for desired soil model prediction outcomes (soil concentrations within two-fold). 1. INTRODUCTION Environmental risk assessments of radionuclides and metals are key to acceptance and sustainability of industrial progress and the disposal of industry's wastes, particularly in the nuclear and imriing and metal smelting industry. -
Chemical Equilibrium and Reaction Modeling of Arsenic and Selenium in Soils
3 Chemical Equilibrium and Reaction Modeling of Arsenic and Selenium in Soils Sabine Goldberg CONTENTS Inorganic Chemistry of As and Se in Soil Solution .......................................... 66 Methylation and Volatilization Reactions ......................................................... 66 Precipitation-Dissolution Reactions .................................................................. 68 Oxidation-Reduction Reactions .......................................................................... 68 Adsorption-Desorption Reactions ..................................................................... 69 Modeling of Adsorption by Soils: Empirical Models ...................................... 70 Modeling of Adsorption by Soils: Constant Capacitance ModeL................ 72 Summary................................................................................................................ 86 References ............................................................................................................... 87 High concentrations of the trace elements arsenic (As) and selenium (Se) in soils pose a threat to agricultural production and the health of humans and animals. As is toxic to both plants and animals. Se, despite being an essential micronutrient for animal nutrition, is potentially toxic because the concentra tion range between deficiency and toxicity in animals is narrow. Seleniferous soils release enough Se to produce vegetation toxic to grazing animals. Such soils occur in the semiarid states of the western United -
Chapter 2: Equation of State
Chapter 2: Equation of State Introduction The Local Thermodynamic Equilibrium The Distribution Function Black Body Radiation Fermi-Dirac EoS The Complete Degenerate Gas Application to White Dwarfs Temperature Effects Ideal Gas The Saha Equation “Almost Perfect” EoS Adiabatic Exponents and Other Derivatives Outline Introduction The Local Thermodynamic Equilibrium The Distribution Function Black Body Radiation Fermi-Dirac EoS The Complete Degenerate Gas Application to White Dwarfs Temperature Effects Ideal Gas The Saha Equation “Almost Perfect” EoS Adiabatic Exponents and Other Derivatives The EoS, together with the thermodynamic equation, allows to study how the stellar material properties react to the heat, changing density, etc. Introduction Goal of the Chapter: derive the equation of state (or the mutual dependencies among local thermodynamic quantities such as P; T ; ρ, and Ni ), not only for the classic ideal gas, but also for photons and fermions. Introduction Goal of the Chapter: derive the equation of state (or the mutual dependencies among local thermodynamic quantities such as P; T ; ρ, and Ni ), not only for the classic ideal gas, but also for photons and fermions. The EoS, together with the thermodynamic equation, allows to study how the stellar material properties react to the heat, changing density, etc. Thermodynamics Thermodynamics is defined as the branch of science that deals with the relationship between heat and other forms of energy, such as work. The Laws of Thermodynamics: I First law: Energy can be neither created nor destroyed. This is a version of the law of conservation of energy, adapted for (isolated) thermodynamic systems. I Second law: In an isolated system, natural processes are spontaneous when they lead to an increase in disorder, or entropy, finally reaching an equilibrium. -
Substitutional Solid Solution Interstitial Solid Solution for Substitutional Solid Solution to Form: Atoms Enters Intersitital Positions in the Host Structure
Substitutional solid solution Interstitial solid solution For substitutional solid solution to form: Atoms enters intersitital positions in the host structure. The ions must be of same charge The ions must be similar in size. The host structure may be expanded but not altered. (For metal atoms < 15% difference) (a bit higher for non-metals) High temperature helps – increase in entropy H2 in Pt (0 > ∆H vs. 0 < ∆H) The crystal structures of the end members must be isostructural for complete solid solubility Partial solid solubility is possible for non-isostructural end members Mg2SiO4 (Mg in octahedras) - Zn2SiO4 (Zn in tetrahedras) Preference for the same type of sites Cr3+ only in octahedral sites, Al3+ in both octahedra and tetraheda sites LiCrO2 -LiCr1-xAlxO2 - LiAlO2 Consider metallic alloys Mg2NH4 LaNi5H6 H2 (liquid) H2 (200 bar) Interstitial solid solution fcc (F) Z=4 bcc (I)Z=2 Fe-C system δ-Fe (bcc) -> 0.1 % C Tm = 1534 °C γ-Fe (fcc) -> 2.06 % C < 1400 °C α-Fe (bcc) -> 0.02 % C < 910 °C Disordered Cu0.75Au0.25 Disordered Cu0.50Au0.50 High temp High temp fcc (F) Z=4 bcc (I)Z=2 Low temp Low temp 2 x 1.433 Å Ordered Cu3Au Ordered CuAu 4 x 2.03 Å 6 x 1.796 Å 3.592 Å 2.866 Å Aliovalent substitution Aliovalent substitution Substitution with ions of different charge 1 Cation vacancies, Substitution by higher valence Need charge compensation mechanism Preserve charge neutrality by leaving out more cations than those that are replaced. Substitution by higher valence cations NaCl dissolves CaCl2 by: Na1-2xCaxVxCl 1 2 Ca2+ vil have a net excess charge of +1 in the structure and attract Na+ vacancies which have net charge -1 Cation vacancies Interstitial anions 2+ 3+ Mg may be replaced by Al : Mg1-3xAl2+2xVxO4 Substitution by lower valence cations 3 4 Anion vacancies Interstitial cations Aliovalent substitution Aliovalent substitution 2 Interstitial anions, Substitution by higher valence 3 Anion vacancies, Substitution by lower valence Preserve charge neutrality by inserting more anions interstitially. -
Modelling the Dissolution/Precipitation of Ideal Solid Solutions
Oil & Gas Science and Technology – Rev. IFP, Vol. 60 (2005), No. 2, pp. 401–415 Copyright © 2005, Institut français du pétrole IFP International Workshop Rencontres scientifiques de l’IFP Gas-Water-Rock Interactions ... / Interactions gaz-eau-roche ... Modelling the Dissolution/Precipitation of Ideal Solid Solutions 1 2 3 4 2 3 E. Nourtier-Mazauric ∗, B. Guy , B. Fritz , E. Brosse , D. Garcia and A. Clément 1 École nationale supérieure des mines de Saint-Etienne – 152 cours Fauriel, 42023 Saint-Etienne Cedex – France 2 idem – affiliated to U.R.A. C.N.R.S. no.6524 3 Centre de géochimie de la surface, C.N.R.S. – 1 rue Blessig, 67084 Strasbourg Cedex – France 4 Institut français du pétrole – 1 et 4 avenue de Bois-Préau, 92852 Rueil-Malmaison Cedex – France e-mail: [email protected] - [email protected] - [email protected] - [email protected] - [email protected] - [email protected] ∗ Corresponding author Résumé — Modélisation de la dissolution/précipitation des solutions solides idéales — Le com- portement cinétique d'une solution solide idéale est modélisé en mettant en compétition deux réactions : la dissolution stoechiométrique du solide existant et la précipitation du composé le moins soluble, c'est- à-dire celui par rapport auquel la sursaturation du fluide est maximum ; les vitesses de ces deux réactions sont exprimées en fonction des écarts à l'équilibre correspondants, les constantes cinétiques dépendant du pH. Dans ce modèle idéal, les courbes de saturation et l'évolution du fluide au sein d'un système réactif simple peuvent être représentées commodément dans des diagrammes en potentiels chimiques.