Carrying out thermodynamic calculations and definition of the main reactions of decomposition of vapours of ethyl alcohol

Size: px
Start display at page:

Download "Carrying out thermodynamic calculations and definition of the main reactions of decomposition of vapours of ethyl alcohol"

Transcription

1 Carrying out thermodynamic calculations and definition of the main reactions of decomosition of vaours of ethyl alcohol A I Sechin, O S Kyrmakova, T A Ivanova National Research Tomsk olytechnic university, 645, Tomsk, Lenin Avenue,, Russia olia_917@mail.ru Abstract. Thermodynamic oortunities of course of chemical reactions of decomosition of the vaors of ethyl alcohol necessary at develoment of devices where these reactions will take lace are considered. The entaliyny method of calculation of constants of balance of robable chemical reactions is given in the Excel editor. Indeendent reactions of rocess of oxidation are defined. By result of thermodynamic calculation of each reaction schedules of deendence of a constant of balance on environment temerature from which follows are constructed that one reactions roceed until the end of aside formation of the final roducts, and others are imrobable or imossible. The analysis of the received results shows that reactions of oxidation will successfully roceed in the established directions, and for an intensification of rocess of decomosition it is necessary to rovide a suly of some energy which quantity will be sufficient for oxidation of vaors of ethyl alcohol. Results of calculations showed good convergence with rograms of thermodynamic calculations like "Aster 4" and "TERRA". 1.Introduction Problem of ollution of atmosheric air one of the most serious global roblems which the mankind faced. Danger of ollution of the atmoshere that harmful substances get to clean air, ernicious for live organisms. Gravity of the environmental roblems connected with ollution of the atmoshere is illustrated by the following statistical data: only 15% of urban oulation of Russia breathe rather clean air. In 15 cities of the Russian Federation the exceeding maximum concentration limits of concentration of ollution of the atmoshere are annually fixed at 5-1 times [1]. Hit in it uncharacteristic hysical, chemical and biological substances in the course of activity of the erson is the main reason for air ollution. In the course of roduction of medicinal substances, there is a need of cleaning of organized emissions in environment of vaors of various organic substances which are emitted as in synthesis rocesses, and rocessings of a number of chemicals. The main share of ollution of the atmoshere belongs to drying rocesses. The dividing systems reresenting two-level cleaning of dust fractions most often dont rovide cleaning of a steam hase. There is a need of the solution of a question of cleaning of organized atmosheric emissions of vaors of organic chemistry. For successful fight against similar ollution it is necessary to know as hysical and chemical roerties of the substances deleted from roduction volume, and the thermodynamic oortunities of course of chemical reactions necessary at develoment of devices where these reactions will take lace. This work is also devoted to the thermodynamic analysis of chemical catalytic reactions of decomosition of vaors of ethyl alcohol and definition of the main reactions..calculated art The chemical thermodynamics considers interrelations between work and energy in relation to chemical transformations. As chemical transformation usually is followed by release or absortion of a certain amount of heat, it submits to the fundamental rinciles (beginnings) of thermodynamics. The chemical thermodynamics defines, first of all, conditions (such as temerature and ressure) courses Content from this work may be used under the terms of the Creative Commons Attribution. licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. Published under licence by Ltd 1

2 of chemical reactions and equilibrium states which they reach []. For carrying out thermodynamic calculations it is necessary from ossible reactions to define indeendent reactions of rocess of oxidation of ethyl alcohol. For calculation of thermodynamic arameters of rocess of oxidation of ethyl alcohol balance reactions were made: 1) С Н 5 ОН + О = СО + Н О; ) С Н 5 ОН С Н + Н ; ) С Н 5 ОН СН 4 + Н О + С; 4) С Н 5 ОН СН 4 + СО + Н ; 5) С Н 5 ОН С Н 4 + Н О; 6) С Н 5 ОН С Н + Н О + Н. Number of indeendent reactions equally to number of substances (С Н 5 ОН, О, СО, H O, С Н, Н, СН 4, С Н 4, С) in system minus number of diverse atoms (to Н, О, С) of which reagents are formed, i.e. the number of indeendent reactions is equal to six (9-=6) []. Therefore, all resented reactions are indeendent. Thermodynamic calculations were imlemented on a method of calculation of the balance [] considering deendence ΔН = f (Т), by means of which lgкр = f (Т), and ΔН, lgk in the range of temeratures 1 C are counted. Influence of temerature on a constant of balance is described by Vant Hoffs equation [4]. d ln K H dt RT () where, ΔН standard thermal effect of reaction; R universal gas constant; T temerature is К; Кр a balance constant. In case of exact calculation and at big temerature intervals the equation () considers deendence of thermal effect of reaction on temerature. For this urose we will substitute the equation C a b T c T () in the equation of the law of Kirchhoff [5]. Integrating, we will receive: in a final formula: d( H) dt C b T c T c H H a T (5) T T Combining the equation () with the equation (4) and integrating, we will receive the equation in technical system of coordinates: lg H a lg b T c T c K T T J. RT R. R.6 R. R According to the equation of an isobar of chemical reaction G RT ln K. RT lg K (6) T J G T. R J. H b T a T ln T c T 6 c T J T where, In the equations 6 unknown sizes are Δа, Δв, Δс, Δс, ΔН 98, Δ G 98, ΔН, J, which are in comliance of the equations: (4) (7)

3 H 98 H 98( прод) H 98( (8) c ( G98 G98( прод) G98( a a( прод ) a( b b( прод ) b( c c( прод ) c( прод) ( c c Coefficients а, в, с, с and ΔН 98, ΔG 98 undertake taking into account the stekhiometricheskikh of coefficients of the equation of the counted reactions. For stay ΔН, which are an extraolation constant we will substitute in the equation () values Δа, Δв, Δс, Δс at Т=98 К and ΔН 98 we will receive in case of high temeratures: b c c H H 98 a (14) 98 For finding of J we will substitute values ΔН (the equation 14), ΔG 98 and Т = 98 К in the equation (7), we will receive ( G98 H ) bt c T c T ( G98 H ) J a lnt T 6 98 (15) 6 a 5.69 b149 c 1481 c 5.61 We will substitute values 8 15 in 5 and we will receive: H T a.lgt.5b T.5c T J lg K (16). R It is known that thermodynamic arameters share on extensive and intensive. The sizes roortional to weight (or to amount of substance) the considered thermodynamic system, carry to extensive, it is volume, internal energy, an enthaly, etc., intensive sizes dont deend on the mass of thermodynamic system. It, for examle, temerature and ressure. Results By result of thermodynamic calculation of each reaction schedules of deendence of a constant of balance of lgk on environment temerature which are reresented in figure 1 were constructed. Reactions of decomosition can go in several directions. Everything deends on energy which is alied to these rocesses. From figure 1 it is visible that reactions: С Н 5 ОН С Н + Н и С Н 5 ОН С Н + Н О + Н arent feasible as have negative value of a constant of balance of lgk and course of reaction towards formation of roducts it is imossible. Following reactions: С Н 5 ОН СН 4 + Н О + С; С Н 5 ОН СН 4 + СО + Н ; С Н 5 ОН С Н 4 + Н О have low robability of course towards formation of roducts. Reaction with high robability of course until the end of aside formation of the final roducts the following: С Н 5 ОН + О = СО + Н О. (9) (1) (11) (1) (1)

4 After the analysis of schedules of deendence of a constant of balance on temerature of the environment the directions of decomosition of reactions were defined. From schedules it is visible that one reactions roceed until the end of aside formation of the final roducts, and others are imrobable or imossible. Figure 1. Deendence of a constant of balance of reaction of oxidation of ethyl lgk alcohol on environment temerature. The analysis of the received results allows to draw a conclusion that reactions of oxidation will successfully roceed in the established directions, and for an intensification of rocess of decomosition it is necessary to rovide a suly of some energy which quantity will be sufficient for oxidation of vaors of alcohol, thereby minimizing technological emission on a steam comonent in environment. 4. Conclusion As a result of the conducted research thermodynamic calculation of ossible reactions of oxidation of alcohol was considered. Indeendent reactions of rocess of oxidation are defined. Thermodynamic calculations of rocess of oxidation of ethyl alcohol are carried out (balance constants, Gibbss energy). The entaliyny method of calculation of constants of balance of chemical reactions is given in the Excel editor. Results of calculations showed good convergence with rograms of thermodynamic 4

5 calculations like "Aster 4" and "TERRA" [6, 7]. References: [1] Smurov A., Snakin V., Komarova N. Current state of atmosheric air. Ecology of Russia, Educational edition. 1. P.1 [] Kosintsev V., Kulikova M., Sechin A., Bordunov S., Prokudin I. Physical and chemical bases of chemical rocesses of receiving inorganic salts: manual. Tomsk, Tomsk University Publ., [] Bezdenezhnyh A. Engineering methods of drawing u equations of seeds of reactions and calculation of kinetic constants. Chemistry, 197 [4] Shilyaev M, Dorokhov A Criteria of a choice and comarison of devices of gas urification. Izv. higher education institutions. Construction, 1998, 6. P [5] Vladimirov L. The accelerated methods of thermodynamic calculations of chemical reactions. LSU Publ., 1956 [6] Dyachenko A., Ftorammoniynaya technology of rocessing of mineral raw materials: the abstract of the thesis on cometition of an academic degree the Dr.Sci.Tech. Tomsk, 8 [7] Pushkarev A. The gaseous lasmochemical rocesses initiated by a ulse electron beam: the abstract of the thesis on cometition of an academic degree of doctor of hysical and mathematical sciences. The automated system of thermodynamic calculations of "TERRA" in the range of temeratures -1 K and ressure of initial mix of,1-,1 MPas. Tomsk,7 5

dn i where we have used the Gibbs equation for the Gibbs energy and the definition of chemical potential

dn i where we have used the Gibbs equation for the Gibbs energy and the definition of chemical potential Chem 467 Sulement to Lectures 33 Phase Equilibrium Chemical Potential Revisited We introduced the chemical otential as the conjugate variable to amount. Briefly reviewing, the total Gibbs energy of a system

More information

Chapter 1 Fundamentals

Chapter 1 Fundamentals Chater Fundamentals. Overview of Thermodynamics Industrial Revolution brought in large scale automation of many tedious tasks which were earlier being erformed through manual or animal labour. Inventors

More information

Phase transition. Asaf Pe er Background

Phase transition. Asaf Pe er Background Phase transition Asaf Pe er 1 November 18, 2013 1. Background A hase is a region of sace, throughout which all hysical roerties (density, magnetization, etc.) of a material (or thermodynamic system) are

More information

ANALYTICAL MODEL FOR THE BYPASS VALVE IN A LOOP HEAT PIPE

ANALYTICAL MODEL FOR THE BYPASS VALVE IN A LOOP HEAT PIPE ANALYTICAL MODEL FOR THE BYPASS ALE IN A LOOP HEAT PIPE Michel Seetjens & Camilo Rindt Laboratory for Energy Technology Mechanical Engineering Deartment Eindhoven University of Technology The Netherlands

More information

Chapter-6: Entropy. 1 Clausius Inequality. 2 Entropy - A Property

Chapter-6: Entropy. 1 Clausius Inequality. 2 Entropy - A Property hater-6: Entroy When the first law of thermodynamics was stated, the existence of roerty, the internal energy, was found. imilarly, econd law also leads to definition of another roerty, known as entroy.

More information

A Model for Randomly Correlated Deposition

A Model for Randomly Correlated Deposition A Model for Randomly Correlated Deosition B. Karadjov and A. Proykova Faculty of Physics, University of Sofia, 5 J. Bourchier Blvd. Sofia-116, Bulgaria ana@hys.uni-sofia.bg Abstract: A simle, discrete,

More information

Homework #11. (Due December 5 at the beginning of the class.) Numerical Method Series #6: Engineering applications of Newton-Raphson Method to

Homework #11. (Due December 5 at the beginning of the class.) Numerical Method Series #6: Engineering applications of Newton-Raphson Method to Homework #11 (Due December 5 at the beginning of the class.) Numerical Method Series #6: Engineering alications of Newton-Rahson Method to solving systems of nonlinear equations Goals: 1. Understanding

More information

Prediction of Vapour Pressures of Dioxin Congeners. R & D Center, Baoshan Iron & Steel Co., Ltd., Fujin Rd., Baoshan District, Shanghai , China

Prediction of Vapour Pressures of Dioxin Congeners. R & D Center, Baoshan Iron & Steel Co., Ltd., Fujin Rd., Baoshan District, Shanghai , China Prediction of Vaour Pressures of Dioxin Congeners Xian-Wei Li, 1 Etsuro Shibata, 2 Eiki Kasai, 2 Takashi Nakamura 2 1 R & D Center, Baoshan Iron & Steel Co., Ltd., Fujin Rd., Baoshan District, Shanghai

More information

ONE. The Earth-atmosphere system CHAPTER

ONE. The Earth-atmosphere system CHAPTER CHAPTER ONE The Earth-atmoshere system 1.1 INTRODUCTION The Earth s atmoshere is the gaseous enveloe surrounding the lanet. Like other lanetary atmosheres, it figures centrally in transfers of energy between

More information

Statics and dynamics: some elementary concepts

Statics and dynamics: some elementary concepts 1 Statics and dynamics: some elementary concets Dynamics is the study of the movement through time of variables such as heartbeat, temerature, secies oulation, voltage, roduction, emloyment, rices and

More information

SIMULATION OF DIFFUSION PROCESSES IN LABYRINTHIC DOMAINS BY USING CELLULAR AUTOMATA

SIMULATION OF DIFFUSION PROCESSES IN LABYRINTHIC DOMAINS BY USING CELLULAR AUTOMATA SIMULATION OF DIFFUSION PROCESSES IN LABYRINTHIC DOMAINS BY USING CELLULAR AUTOMATA Udo Buschmann and Thorsten Rankel and Wolfgang Wiechert Deartment of Simulation University of Siegen Paul-Bonatz-Str.

More information

Speed of sound measurements in liquid Methane at cryogenic temperature and for pressure up to 10 MPa

Speed of sound measurements in liquid Methane at cryogenic temperature and for pressure up to 10 MPa LNGII - raining Day Delft, August 07 Seed of sound measurements in liquid Methane at cryogenic temerature and for ressure u to 0 MPa Simona Lago*, P. Alberto Giuliano Albo INRiM Istituto Nazionale di Ricerca

More information

Chapter 7 Sampling and Sampling Distributions. Introduction. Selecting a Sample. Introduction. Sampling from a Finite Population

Chapter 7 Sampling and Sampling Distributions. Introduction. Selecting a Sample. Introduction. Sampling from a Finite Population Chater 7 and s Selecting a Samle Point Estimation Introduction to s of Proerties of Point Estimators Other Methods Introduction An element is the entity on which data are collected. A oulation is a collection

More information

Chapter 9 Practical cycles

Chapter 9 Practical cycles Prof.. undararajan Chater 9 Practical cycles 9. Introduction In Chaters 7 and 8, it was shown that a reversible engine based on the Carnot cycle (two reversible isothermal heat transfers and two reversible

More information

4. A Brief Review of Thermodynamics, Part 2

4. A Brief Review of Thermodynamics, Part 2 ATMOSPHERE OCEAN INTERACTIONS :: LECTURE NOTES 4. A Brief Review of Thermodynamics, Part 2 J. S. Wright jswright@tsinghua.edu.cn 4.1 OVERVIEW This chater continues our review of the key thermodynamics

More information

FUGACITY. It is simply a measure of molar Gibbs energy of a real gas.

FUGACITY. It is simply a measure of molar Gibbs energy of a real gas. FUGACITY It is simly a measure of molar Gibbs energy of a real gas. Modifying the simle equation for the chemical otential of an ideal gas by introducing the concet of a fugacity (f). The fugacity is an

More information

About determining the wettability of coal surface

About determining the wettability of coal surface IOP Conference Series: Earth and Environmental Science PAPER OPEN ACCESS About determining the wettability of coal surface To cite this article: V A Arkhiov et al 16 IOP Conf. Ser.: Earth Environ. Sci.

More information

The Role of Water Vapor. atmosphere (we will ignore the solid phase here) Refer to the phase diagram in the web notes.

The Role of Water Vapor. atmosphere (we will ignore the solid phase here) Refer to the phase diagram in the web notes. The Role of Water Vaor Water can exist as either a vaor or liquid in the atmoshere (we will ignore the solid hase here) under a variety of Temerature and ressure conditions. Refer to the hase diagram in

More information

Explosion Protection of Buildings

Explosion Protection of Buildings 1 Exlosion Protection of Buildings Author: Miroslav Mynarz 2 Exlosion Protection of Buildings Exlosion of a Condensed Exlosive and Calculation of Blast Wave Parameters Theory of exlosion of condensed exlosive

More information

δq T = nr ln(v B/V A )

δq T = nr ln(v B/V A ) hysical Chemistry 007 Homework assignment, solutions roblem 1: An ideal gas undergoes the following reversible, cyclic rocess It first exands isothermally from state A to state B It is then comressed adiabatically

More information

Churilova Maria Saint-Petersburg State Polytechnical University Department of Applied Mathematics

Churilova Maria Saint-Petersburg State Polytechnical University Department of Applied Mathematics Churilova Maria Saint-Petersburg State Polytechnical University Deartment of Alied Mathematics Technology of EHIS (staming) alied to roduction of automotive arts The roblem described in this reort originated

More information

The Second Law: The Machinery

The Second Law: The Machinery The Second Law: The Machinery Chater 5 of Atkins: The Second Law: The Concets Sections 3.7-3.9 8th Ed, 3.3 9th Ed; 3.4 10 Ed.; 3E 11th Ed. Combining First and Second Laws Proerties of the Internal Energy

More information

Physics 2A (Fall 2012) Chapters 11:Using Energy and 12: Thermal Properties of Matter

Physics 2A (Fall 2012) Chapters 11:Using Energy and 12: Thermal Properties of Matter Physics 2A (Fall 2012) Chaters 11:Using Energy and 12: Thermal Proerties of Matter "Kee in mind that neither success nor failure is ever final." Roger Ward Babson Our greatest glory is not in never failing,

More information

Feedback-error control

Feedback-error control Chater 4 Feedback-error control 4.1 Introduction This chater exlains the feedback-error (FBE) control scheme originally described by Kawato [, 87, 8]. FBE is a widely used neural network based controller

More information

High speed wind tunnels 2.0 Definition of high speed. 2.1 Types of high speed wind tunnels

High speed wind tunnels 2.0 Definition of high speed. 2.1 Types of high speed wind tunnels Module Lectures 6 to 1 High Seed Wind Tunnels Keywords: Blow down wind tunnels, Indraft wind tunnels, suersonic wind tunnels, c-d nozzles, second throat diffuser, shocks, condensation in wind tunnels,

More information

Efficiencies. Damian Vogt Course MJ2429. Nomenclature. Symbol Denotation Unit c Flow speed m/s c p. pressure c v. Specific heat at constant J/kgK

Efficiencies. Damian Vogt Course MJ2429. Nomenclature. Symbol Denotation Unit c Flow speed m/s c p. pressure c v. Specific heat at constant J/kgK Turbomachinery Lecture Notes 1 7-9-1 Efficiencies Damian Vogt Course MJ49 Nomenclature Subscrits Symbol Denotation Unit c Flow seed m/s c Secific heat at constant J/kgK ressure c v Secific heat at constant

More information

Determination of Pressure Losses in Hydraulic Pipeline Systems by Considering Temperature and Pressure

Determination of Pressure Losses in Hydraulic Pipeline Systems by Considering Temperature and Pressure Paer received: 7.10.008 UDC 61.64 Paer acceted: 0.04.009 Determination of Pressure Losses in Hydraulic Pieline Systems by Considering Temerature and Pressure Vladimir Savi 1,* - Darko Kneževi - Darko Lovrec

More information

arxiv: v1 [physics.data-an] 26 Oct 2012

arxiv: v1 [physics.data-an] 26 Oct 2012 Constraints on Yield Parameters in Extended Maximum Likelihood Fits Till Moritz Karbach a, Maximilian Schlu b a TU Dortmund, Germany, moritz.karbach@cern.ch b TU Dortmund, Germany, maximilian.schlu@cern.ch

More information

Where: Where: f Wave s frequency (Hz) c Speed of light ( ms -1 ) Wavelength (m)

Where: Where: f Wave s frequency (Hz) c Speed of light ( ms -1 ) Wavelength (m) in a direction to both of the fields as shown in Figure 1. In wave model, the electromagnetic radiation is commonly associated with wavelength and frequency, exressed mathematically as: c f...(1) f Wave

More information

Main Menu. Summary (1)

Main Menu. Summary (1) Elastic roerty changes of bitumen reservoir during steam injection Ayato Kato*, University of Houston, higenobu Onozuka, JOGMEC, and Toru Nakayama, JAPEX ummary Elastic roerty changes of bitumen reservoir

More information

Paper C Exact Volume Balance Versus Exact Mass Balance in Compositional Reservoir Simulation

Paper C Exact Volume Balance Versus Exact Mass Balance in Compositional Reservoir Simulation Paer C Exact Volume Balance Versus Exact Mass Balance in Comositional Reservoir Simulation Submitted to Comutational Geosciences, December 2005. Exact Volume Balance Versus Exact Mass Balance in Comositional

More information

ATMOS Lecture 7. The First Law and Its Consequences Pressure-Volume Work Internal Energy Heat Capacity Special Cases of the First Law

ATMOS Lecture 7. The First Law and Its Consequences Pressure-Volume Work Internal Energy Heat Capacity Special Cases of the First Law TMOS 5130 Lecture 7 The First Law and Its Consequences Pressure-Volume Work Internal Energy Heat Caacity Secial Cases of the First Law Pressure-Volume Work Exanding Volume Pressure δw = f & dx δw = F ds

More information

PHYS1001 PHYSICS 1 REGULAR Module 2 Thermal Physics Chapter 17 First Law of Thermodynamics

PHYS1001 PHYSICS 1 REGULAR Module 2 Thermal Physics Chapter 17 First Law of Thermodynamics PHYS1001 PHYSICS 1 REGULAR Module Thermal Physics Chater 17 First Law of Thermodynamics References: 17.1 to 17.9 Examles: 17.1 to 17.7 Checklist Thermodynamic system collection of objects and fields. If

More information

The extreme case of the anisothermal calorimeter when there is no heat exchange is the adiabatic calorimeter.

The extreme case of the anisothermal calorimeter when there is no heat exchange is the adiabatic calorimeter. .4. Determination of the enthaly of solution of anhydrous and hydrous sodium acetate by anisothermal calorimeter, and the enthaly of melting of ice by isothermal heat flow calorimeter Theoretical background

More information

A Quadratic Cumulative Production Model for the Material Balance of Abnormally-Pressured Gas Reservoirs

A Quadratic Cumulative Production Model for the Material Balance of Abnormally-Pressured Gas Reservoirs A Quadratic Cumulative Production Model for the Material Balance of Abnormally-Pressured as Reservoirs F.E. onale, M.S. Thesis Defense 7 October 2003 Deartment of Petroleum Engineering Texas A&M University

More information

PV/T = k or PV = kt Describe the difference between an ideal gas and a real gas.

PV/T = k or PV = kt Describe the difference between an ideal gas and a real gas. 10.1 Thermodynamics 10.2 Processes 10 10.3 The second law of thermodynamics and entroy 10.1 Thermodynamics From the combined gas laws, we determined that: P/T = k or P = kt 10.1.1 State the equation of

More information

MODELING OF CONSTANT VOLUME COMBUSTION OF PROPELLANTS FOR ARTILLERY WEAPONS

MODELING OF CONSTANT VOLUME COMBUSTION OF PROPELLANTS FOR ARTILLERY WEAPONS MODELING OF CONSTANT VOLUME COMBUSTION OF PROPELLANTS FOR ARTILLERY WEAPONS Lt.col. lect. dr.ing. Daniel ANTONIE, Col.(r). rof.as. dr.ing. Sorin GHEORGHIAN, Col.(r). C.S.II dr.ing. Nicolae MĂRUNȚELU MILITARY

More information

Modeling and Simulation a Catalytic Fixed Bed Reactor to Produce Ethyl Benzene from Ethanol

Modeling and Simulation a Catalytic Fixed Bed Reactor to Produce Ethyl Benzene from Ethanol Journal of Physical Chemistry and Electrochemistry Vol. No.3 (20) 55-6 Journal of Physical Chemistry and Electrochemistry Islamic Azad University Marvdasht ranch Journal homeage: htt://journals.miau.ac.ir/je

More information

Homogeneous and Inhomogeneous Model for Flow and Heat Transfer in Porous Materials as High Temperature Solar Air Receivers

Homogeneous and Inhomogeneous Model for Flow and Heat Transfer in Porous Materials as High Temperature Solar Air Receivers Excert from the roceedings of the COMSOL Conference 1 aris Homogeneous and Inhomogeneous Model for Flow and Heat ransfer in orous Materials as High emerature Solar Air Receivers Olena Smirnova 1 *, homas

More information

Ideal Gas Law. September 2, 2014

Ideal Gas Law. September 2, 2014 Ideal Gas Law Setember 2, 2014 Thermodynamics deals with internal transformations of the energy of a system and exchanges of energy between that system and its environment. A thermodynamic system refers

More information

A New GP-evolved Formulation for the Relative Permittivity of Water and Steam

A New GP-evolved Formulation for the Relative Permittivity of Water and Steam ew GP-evolved Formulation for the Relative Permittivity of Water and Steam S. V. Fogelson and W. D. Potter rtificial Intelligence Center he University of Georgia, US Contact Email ddress: sergeyf1@uga.edu

More information

Liquid water static energy page 1/8

Liquid water static energy page 1/8 Liquid water static energy age 1/8 1) Thermodynamics It s a good idea to work with thermodynamic variables that are conserved under a known set of conditions, since they can act as assive tracers and rovide

More information

High Temperature Catalysis

High Temperature Catalysis Fritz-Haber Haber-Institute, Max-Planc Planc-Society, Inorganic Chemistry Deartment High Temerature Catalysis Raimund Horn Lecture Series Modern Methods in Heterogeneous Catalysis 3..9 Outline. What is

More information

On Using FASTEM2 for the Special Sensor Microwave Imager (SSM/I) March 15, Godelieve Deblonde Meteorological Service of Canada

On Using FASTEM2 for the Special Sensor Microwave Imager (SSM/I) March 15, Godelieve Deblonde Meteorological Service of Canada On Using FASTEM2 for the Secial Sensor Microwave Imager (SSM/I) March 15, 2001 Godelieve Deblonde Meteorological Service of Canada 1 1. Introduction Fastem2 is a fast model (multile-linear regression model)

More information

The International Association for the Properties of Water and Steam

The International Association for the Properties of Water and Steam IAPWS SR5-05(2016) he International Association for the Proerties of Water and Steam Moscow, Russia June 2014 Revised Sulementary Release on Backward Equations for Secific Volume as a Function of Pressure

More information

We now turn to considerations of mixtures. To keep our discussion reasonably simple,

We now turn to considerations of mixtures. To keep our discussion reasonably simple, 143 Lecture 23 We now turn to considerations of mixtures. To kee our discussion reasonably simle, we will limit our discussion to non-reacting systems, and to non-ionic systems. In other words, we will

More information

Thermodynamics in combustion

Thermodynamics in combustion Thermodynamics in combustion 2nd ste in toolbox Thermodynamics deals with a equilibrium state and how chemical comosition can be calculated for a system with known atomic or molecular comosition if 2 indeendent

More information

The thermal wind 1. v g

The thermal wind 1. v g The thermal win The thermal win Introuction The geostrohic win is etermine by the graient of the isobars (on a horizontal surface) or isohyses (on a ressure surface). On a ressure surface the graient of

More information

Spin as Dynamic Variable or Why Parity is Broken

Spin as Dynamic Variable or Why Parity is Broken Sin as Dynamic Variable or Why Parity is Broken G. N. Golub golubgn@meta.ua There suggested a modification of the Dirac electron theory, eliminating its mathematical incomleteness. The modified Dirac electron,

More information

AT 25 C! CH10090 Thermodynamics (part 2) Enthalpy changes during reactions. Let s remember what we did in CH10089

AT 25 C! CH10090 Thermodynamics (part 2) Enthalpy changes during reactions. Let s remember what we did in CH10089 CH10090 hermodynamics (art ) Let s remember what we did in CH10089 Enthaly changes during reactions o o o H98 ( reaction) = νi Hf, 98( roducts) νi Hf, 98( reactants) ν i reresents the stoichiometric coefficient.

More information

Lecture 7: Thermodynamic Potentials

Lecture 7: Thermodynamic Potentials Lecture 7: Thermodynamic Potentials Chater II. Thermodynamic Quantities A.G. Petukhov, PHY 743 etember 27, 2017 Chater II. Thermodynamic Quantities Lecture 7: Thermodynamic Potentials A.G. Petukhov, etember

More information

Modeling Volume Changes in Porous Electrodes

Modeling Volume Changes in Porous Electrodes Journal of The Electrochemical Society, 53 A79-A86 2006 003-465/2005/53/A79/8/$20.00 The Electrochemical Society, Inc. Modeling olume Changes in Porous Electrodes Parthasarathy M. Gomadam*,a,z John W.

More information

Internal Energy in terms of Properties

Internal Energy in terms of Properties Lecture #3 Internal Energy in terms of roerties Internal energy is a state function. A change in the state of the system causes a change in its roerties. So, we exress the change in internal energy in

More information

Lecture 13. Heat Engines. Thermodynamic processes and entropy Thermodynamic cycles Extracting work from heat

Lecture 13. Heat Engines. Thermodynamic processes and entropy Thermodynamic cycles Extracting work from heat Lecture 3 Heat Engines hermodynamic rocesses and entroy hermodynamic cycles Extracting work from heat - How do we define engine efficiency? - Carnot cycle: the best ossible efficiency Reading for this

More information

Session 12 : Monopropellant Thrusters

Session 12 : Monopropellant Thrusters Session 12 : Monoroellant Thrusters Electrothermal augmentation of chemical rockets was the first form of electric roulsion alied in sace vehicles. In its original imlementation, resistojets were used

More information

Actual exergy intake to perform the same task

Actual exergy intake to perform the same task CHAPER : PRINCIPLES OF ENERGY CONSERVAION INRODUCION Energy conservation rinciles are based on thermodynamics If we look into the simle and most direct statement of the first law of thermodynamics, we

More information

PHYSICAL REVIEW LETTERS

PHYSICAL REVIEW LETTERS PHYSICAL REVIEW LETTERS VOLUME 81 20 JULY 1998 NUMBER 3 Searated-Path Ramsey Atom Interferometer P. D. Featonby, G. S. Summy, C. L. Webb, R. M. Godun, M. K. Oberthaler, A. C. Wilson, C. J. Foot, and K.

More information

Lecture 28: Kinetics of Oxidation of Metals: Part 1: rusting, corrosion, and

Lecture 28: Kinetics of Oxidation of Metals: Part 1: rusting, corrosion, and Lecture 8: Kinetics of xidation of etals: Part 1: rusting, corrosion, and the surface rotection, all about chemistry Today s toics hemical rocesses of oxidation of metals: the role layed by oxygen. How

More information

Use of Transformations and the Repeated Statement in PROC GLM in SAS Ed Stanek

Use of Transformations and the Repeated Statement in PROC GLM in SAS Ed Stanek Use of Transformations and the Reeated Statement in PROC GLM in SAS Ed Stanek Introduction We describe how the Reeated Statement in PROC GLM in SAS transforms the data to rovide tests of hyotheses of interest.

More information

Lecture 13 Heat Engines

Lecture 13 Heat Engines Lecture 3 Heat Engines hermodynamic rocesses and entroy hermodynamic cycles Extracting work from heat - How do we define engine efficiency? - Carnot cycle: the best ossible efficiency Reading for this

More information

Formation and transformation of volatile nanoparticles from a diesel engine during exhaust dilution

Formation and transformation of volatile nanoparticles from a diesel engine during exhaust dilution Article Mechanical Engineering March 2012 Vol.57 No.8: 948954 doi: 10.1007/s11434-011-4927-8 Formation and transformation of volatile nanoarticles from a diesel engine during exhaust dilution LI XinLing

More information

Thermodynamic equations of state of polymers and conversion processing

Thermodynamic equations of state of polymers and conversion processing Polimery, No.,,. 66 hermodynamic equations of state of olymers and conversion rocessing B. Kowalska Selected from International Polymer Science and echnology, 9, No.,, reference P //66; transl. serial

More information

/ p) TA,. Returning to the

/ p) TA,. Returning to the Toic2610 Proerties; Equilibrium and Frozen A given closed system having Gibbs energy G at temerature T, ressure, molecular comosition (organisation ) and affinity for sontaneous change A is described by

More information

Chemical Kinetics and Equilibrium - An Overview - Key

Chemical Kinetics and Equilibrium - An Overview - Key Chemical Kinetics and Equilibrium - An Overview - Key The following questions are designed to give you an overview of the toics of chemical kinetics and chemical equilibrium. Although not comrehensive,

More information

GEF2200 vår 2017 Løsningsforslag sett 1

GEF2200 vår 2017 Løsningsforslag sett 1 GEF2200 vår 2017 Løsningsforslag sett 1 A.1.T R is the universal gas constant, with value 8.3143JK 1 mol 1. R is the gas constant for a secic gas, given by R R M (1) where M is the molecular weight of

More information

MODELING AND SIMULATION OF REFORMER AUTO- THERMAL REACTOR IN AMMONIA UNIT

MODELING AND SIMULATION OF REFORMER AUTO- THERMAL REACTOR IN AMMONIA UNIT Peet trool lleeuum & Cooaal ll IISSN 337-77 Available online at www.vuru.sk/c Petroleum & Coal 9 (), 6-7, 7 MODELING AND SIMULATION OF REFORMER AUTO- THERMAL REACTOR IN AMMONIA UNIT Kayvan Khorsand *,

More information

whether a process will be spontaneous, it is necessary to know the entropy change in both the

whether a process will be spontaneous, it is necessary to know the entropy change in both the 93 Lecture 16 he entroy is a lovely function because it is all we need to know in order to redict whether a rocess will be sontaneous. However, it is often inconvenient to use, because to redict whether

More information

Ultrasonic Peeling. The Bauman Moscow State Technical University, Russia,

Ultrasonic Peeling. The Bauman Moscow State Technical University, Russia, V. M. Gorshkova Ultrasonic Peeling The Bauman Moscow State Technical University, ussia, v_gorshkova@mail.ru ABSTACT The article suggests a mathematical descrition o eeling by ultrasound technologies. INTODUCTION

More information

Lecture 8, the outline

Lecture 8, the outline Lecture, the outline loose end: Debye theory of solids more remarks on the first order hase transition. Bose Einstein condensation as a first order hase transition 4He as Bose Einstein liquid Lecturer:

More information

Optical properties of semiconductors. Dr. Katarzyna Skorupska

Optical properties of semiconductors. Dr. Katarzyna Skorupska Otical roerties of semiconductors Dr. Katarzyna Skoruska band structure of crystalline solids by solution of Schroedinger equation (one e - aroximation) Solution leads to energy bands searated by an energy

More information

Mixture Homogeneous Mixtures (air, sea water ) same composition, no chemical bond components are NOT distinguishable

Mixture Homogeneous Mixtures (air, sea water ) same composition, no chemical bond components are NOT distinguishable BASIC CONCEPTAND DEFINITIONS1 2 THERMODYNAMICS CHAPTER 2 Thermodynamic Concets Lecturer Axel GRONIEWSKY, PhD 11 th of February2019 Thermodynamics study of energy and its transformation describes macroscoic

More information

Dynamics and Heat and Mass Transfer of Liquid-Droplet Cloud in the Emergency Discharge of Aviation Fuel into the Atmosphere

Dynamics and Heat and Mass Transfer of Liquid-Droplet Cloud in the Emergency Discharge of Aviation Fuel into the Atmosphere Dynamics and Heat and Mass Transer o Liquid-Drolet Cloud in the Emergency Discharge o Aviation Fuel into the Atmoshere Evgeny Maslov 1,,*, Amgalan Badmaev, and Irina Zharova 1 1 National Research Tomsk

More information

Chapter 2 Solutions. 2.1 (D) Pressure and temperature are dependent during phase change and independent when in a single phase.

Chapter 2 Solutions. 2.1 (D) Pressure and temperature are dependent during phase change and independent when in a single phase. Chater Solutions.1 (D) Pressure and temerature are deendent during hase change and indeendent when in a single hase.. (B) Sublimation is the direct conversion of a solid to a gas. To observe this rocess,

More information

Shadow Computing: An Energy-Aware Fault Tolerant Computing Model

Shadow Computing: An Energy-Aware Fault Tolerant Computing Model Shadow Comuting: An Energy-Aware Fault Tolerant Comuting Model Bryan Mills, Taieb Znati, Rami Melhem Deartment of Comuter Science University of Pittsburgh (bmills, znati, melhem)@cs.itt.edu Index Terms

More information

MATHEMATICAL MODELLING OF THE WIRELESS COMMUNICATION NETWORK

MATHEMATICAL MODELLING OF THE WIRELESS COMMUNICATION NETWORK Comuter Modelling and ew Technologies, 5, Vol.9, o., 3-39 Transort and Telecommunication Institute, Lomonosov, LV-9, Riga, Latvia MATHEMATICAL MODELLIG OF THE WIRELESS COMMUICATIO ETWORK M. KOPEETSK Deartment

More information

A High Precision Double Tubed Hydrostatic Leveling System for Accelerator Alignment Applications

A High Precision Double Tubed Hydrostatic Leveling System for Accelerator Alignment Applications 9th International Worksho on Accelerator Alignment, Setember 6-9, 6 A High Precision Double Tubed Hydrostatic Leveling System for Accelerator Alignment Alications S. Singatulin, J. olk,. Shiltsev Fermilab,

More information

VISCOELASTIC PROPERTIES OF INHOMOGENEOUS NANOCOMPOSITES

VISCOELASTIC PROPERTIES OF INHOMOGENEOUS NANOCOMPOSITES VISCOELASTIC PROPERTIES OF INHOMOGENEOUS NANOCOMPOSITES V. V. Novikov ), K.W. Wojciechowski ) ) Odessa National Polytechnical University, Shevchenko Prosekt, 6544 Odessa, Ukraine; e-mail: novikov@te.net.ua

More information

An Improved Calibration Method for a Chopped Pyrgeometer

An Improved Calibration Method for a Chopped Pyrgeometer 96 JOURNAL OF ATMOSPHERIC AND OCEANIC TECHNOLOGY VOLUME 17 An Imroved Calibration Method for a Choed Pyrgeometer FRIEDRICH FERGG OtoLab, Ingenieurbüro, Munich, Germany PETER WENDLING Deutsches Forschungszentrum

More information

On Gravity Waves on the Surface of Tangential Discontinuity

On Gravity Waves on the Surface of Tangential Discontinuity Alied Physics Research; Vol. 6, No. ; 4 ISSN 96-9639 E-ISSN 96-9647 Published by anadian enter of Science and Education On Gravity Waves on the Surface of Tangential Discontinuity V. G. Kirtskhalia I.

More information

The analysis of combustion heat of the metallized solid fuel compositions

The analysis of combustion heat of the metallized solid fuel compositions The analysis of combustion heat of the metallized solid fuel comositions Yana Dubkova 1,*, and Alexander Zhukov 1 1 National Research Tomsk State University, 634050 Tomsk, Russia Abstract. The technique

More information

8 STOCHASTIC PROCESSES

8 STOCHASTIC PROCESSES 8 STOCHASTIC PROCESSES The word stochastic is derived from the Greek στoχαστικoς, meaning to aim at a target. Stochastic rocesses involve state which changes in a random way. A Markov rocess is a articular

More information

Week 8 lectures. ρ t +u ρ+ρ u = 0. where µ and λ are viscosity and second viscosity coefficients, respectively and S is the strain tensor:

Week 8 lectures. ρ t +u ρ+ρ u = 0. where µ and λ are viscosity and second viscosity coefficients, respectively and S is the strain tensor: Week 8 lectures. Equations for motion of fluid without incomressible assumtions Recall from week notes, the equations for conservation of mass and momentum, derived generally without any incomressibility

More information

Proof: We follow thearoach develoed in [4]. We adot a useful but non-intuitive notion of time; a bin with z balls at time t receives its next ball at

Proof: We follow thearoach develoed in [4]. We adot a useful but non-intuitive notion of time; a bin with z balls at time t receives its next ball at A Scaling Result for Exlosive Processes M. Mitzenmacher Λ J. Sencer We consider the following balls and bins model, as described in [, 4]. Balls are sequentially thrown into bins so that the robability

More information

SIMULATED ANNEALING AND JOINT MANUFACTURING BATCH-SIZING. Ruhul SARKER. Xin YAO

SIMULATED ANNEALING AND JOINT MANUFACTURING BATCH-SIZING. Ruhul SARKER. Xin YAO Yugoslav Journal of Oerations Research 13 (003), Number, 45-59 SIMULATED ANNEALING AND JOINT MANUFACTURING BATCH-SIZING Ruhul SARKER School of Comuter Science, The University of New South Wales, ADFA,

More information

Compressible Flow Introduction. Afshin J. Ghajar

Compressible Flow Introduction. Afshin J. Ghajar 36 Comressible Flow Afshin J. Ghajar Oklahoma State University 36. Introduction...36-36. he Mach Number and Flow Regimes...36-36.3 Ideal Gas Relations...36-36.4 Isentroic Flow Relations...36-4 36.5 Stagnation

More information

Participation Factors. However, it does not give the influence of each state on the mode.

Participation Factors. However, it does not give the influence of each state on the mode. Particiation Factors he mode shae, as indicated by the right eigenvector, gives the relative hase of each state in a articular mode. However, it does not give the influence of each state on the mode. We

More information

International Journal of Mathematics Trends and Technology- Volume3 Issue4-2012

International Journal of Mathematics Trends and Technology- Volume3 Issue4-2012 Effect of Hall current on Unsteady Flow of a Dusty Conducting Fluid through orous medium between Parallel Porous Plates with Temerature Deendent Viscosity and Thermal Radiation Harshbardhan Singh and Dr.

More information

THE FIRST LAW OF THERMODYNAMICS

THE FIRST LAW OF THERMODYNAMICS THE FIRST LA OF THERMODYNAMIS 9 9 (a) IDENTIFY and SET UP: The ressure is constant and the volume increases (b) = d Figure 9 Since is constant, = d = ( ) The -diagram is sketched in Figure 9 The roblem

More information

A Computer Model of the Evaporator for the Development of an Automatic Control System

A Computer Model of the Evaporator for the Development of an Automatic Control System IOP Conference Series: Materials Science and Engineering PAPER OPEN ACCESS A Computer Model of the Evaporator for the Development of an Automatic Control System To cite this article: K A Kozin et al 2016

More information

NEW DIFFERENTIAL DATA ANALYSIS METHOD IN THE ACTIVE THERMOGRAPHY.

NEW DIFFERENTIAL DATA ANALYSIS METHOD IN THE ACTIVE THERMOGRAPHY. Proceedings 3rd Annual Conference IEEE/EMBS Oct.5-8, 001, Istanbul, TURKEY 1 of 4 NEW DIFFERENTIAL DATA ANALYSIS METHOD IN THE ACTIVE THERMOGRAPHY. J. Rumiński, M. Kaczmarek, A. Nowakowski Deartment of

More information

Effect of Hall current and rotation on heat transfer in MHD flow of oscillating dusty fluid in a porous channel

Effect of Hall current and rotation on heat transfer in MHD flow of oscillating dusty fluid in a porous channel Indian Journal of Pure & Alied Physics Vol. 5 October 03. 669-68 Effect of Hall current and rotation on heat transfer in MHD flow of oscillating dusty fluid in a orous channel Khem Chand K D Singh & Shavnam

More information

PERFORMANCE BASED DESIGN SYSTEM FOR CONCRETE MIXTURE WITH MULTI-OPTIMIZING GENETIC ALGORITHM

PERFORMANCE BASED DESIGN SYSTEM FOR CONCRETE MIXTURE WITH MULTI-OPTIMIZING GENETIC ALGORITHM PERFORMANCE BASED DESIGN SYSTEM FOR CONCRETE MIXTURE WITH MULTI-OPTIMIZING GENETIC ALGORITHM Takafumi Noguchi 1, Iei Maruyama 1 and Manabu Kanematsu 1 1 Deartment of Architecture, University of Tokyo,

More information

A flexible inversion algorithm for retrieval of aerosol optical properties from sun and sky radiance measurements

A flexible inversion algorithm for retrieval of aerosol optical properties from sun and sky radiance measurements A flexible inversion algorithm for retrieval of aerosol otical roerties from sun and sky radiance measurements Oleg Dubovik (1,2), and Michael D. King (3) 1. Laboratory for Terrestrial Physics, NASA Goddard

More information

What did we learn in Ch. 1? Energy Transfers Link Ch What did we learn in Ch. 3? What did we learn in Ch. 4? Key Combined 1 st +2 nd Law Results

What did we learn in Ch. 1? Energy Transfers Link Ch What did we learn in Ch. 3? What did we learn in Ch. 4? Key Combined 1 st +2 nd Law Results Energy ransfers Link Ch. - Ch. Atmosheric Comosition dry air (N, O, Ar, CO ), Water, (articles) Ch. First and Second Laws Energy Balance (System/Environment) Ch. 3 Stefan-Boltzmann Equation Kirchoff s

More information

3. High Temperature Gases FPK1 2009/MZ 1/23

3. High Temperature Gases FPK1 2009/MZ 1/23 3. High Temerature Gases FP 9/MZ /3 Terms and Concets Dissociation Diatomic element gases Bond energy, dissociation energy (enthali) Flood s dissociation diagram Vaorization, eaoration, boiling, sublimation

More information

Optimizing the Polynomial to Represent the Extended True Boiling Point Curve from High Vacuum Distillation Data Using Genetic Algorithms

Optimizing the Polynomial to Represent the Extended True Boiling Point Curve from High Vacuum Distillation Data Using Genetic Algorithms 1561 A ublication of CHEMICAL ENGINEERING TRANSACTIONS VOL. 43, 015 Chief Editors: Sauro Pierucci, Jiří J. Klemeš Coyright 015, AIDIC Servizi S.r.l., ISBN 978-88-95608-34-1; ISSN 83-916 The Italian Association

More information

Equilibrium Thermodynamics

Equilibrium Thermodynamics Part I Equilibrium hermodynamics 1 Molecular hermodynamics Perhas the most basic equation in atmosheric thermodynamics is the ideal gas law = rr where is ressure, r is the air density, is temerature, and

More information

International Association of Scientific Innovation and Research (IASIR) (An Association Unifying the Sciences, Engineering, and Applied Research)

International Association of Scientific Innovation and Research (IASIR) (An Association Unifying the Sciences, Engineering, and Applied Research) International Association of ientific Innovation and Research (IASIR) (An Association Unifying the iences, Engineering, and Alied Research) International Journal of Emerging Technologies in Comutational

More information

Setting up the Mathematical Model Review of Heat & Material Balances

Setting up the Mathematical Model Review of Heat & Material Balances Setting u the Mathematical Model Review of Heat & Material Balances Toic Summary... Introduction... Conservation Equations... 3 Use of Intrinsic Variables... 4 Well-Mixed Systems... 4 Conservation of Total

More information