Analytical calculation of adiabatic processes in real gases

Size: px
Start display at page:

Download "Analytical calculation of adiabatic processes in real gases"

Transcription

1 Journal of Physs: Conferene Seres PAPER OPEN ACCESS Analytal alulaton of adabat roesses n real gases o te ths artle: I B Amarskaja et al 016 J. Phys.: Conf. Ser Related ontent - Shortuts to quantum adabat roesses J G Muga, X Chen, E orrontegu et al. - Letters and Comments Joaqum Analeto and Máro G Perera - Rely to 'Comment on "Dssatve work n thermodynams"' Joaqum Analeto, Máro G Perera and J M Ferrera Vew the artle onlne for udates and enhanements. hs ontent was downloaded from IP address on 04/0/018 at 08:57

2 Journal of Physs: Conferene Seres 754 (016) IOP Publshng do: / /754/11/11003 Analytal alulaton of adabat roesses n real gases I B Amarskaja, V S Belousov, P S Flov Ural Federal Unversty, 19 Mra street, Ekaternburg, Russa E-mal: tot@urfu.ru Abstrat. he mat of gases nondealty n the omresson and exanson roesses on the sef heat rato and the heat aaty s analyzed. he sef heat rato varaton leads to temerature varaton durng omresson n the omressor and exanson n the turbne and, onsequently, the gas turbne yle effeny fator varaton. It s also essental to onsder the gases nondealty n the omresson and exanson roesses n the omresson roesses n omressor. Generally t s assumed durng alulatons that the heat aates deend only on temerature, n ths ase the referene data resented by varous authors dffers markedly. In the real roesses the heat aaty and the sef heat rato deend on temerature and wthn the artular temeratures and ressures range deend on ressure. Consequently, the oeratng flud nondealty n the gas turbne yle should be onsdered. 1. Introduton he roesses of gases omresson n the nonooled omressor and exanson n the turbne an be assumed as adabat to a good aroxmaton. Usually durng the thermodynam analyss of the roesses mentoned above t s assumed that the oeratng flud s an deal gas wth the thermohysal roertes deendng only on temerature. In real roesses the heat aaty and, onsequently, the sef heat rato deend heavly on temerature and wthn the artular temeratures and ressures range deend on ressure, t means that the oeratng flud nondealty n the gas turbne yle should be onsdered. he thermodynam effeny mrovement n the modern gas turbne unts s aheved by means of the nrease n the omresson ressure rato n the omressor and the ombuston roduts temerature rse before the turbne, whh an result n the neessty of the gas nondealty onsderaton. For nstane, the hange of % n the sef heat rato as omared to the k value beng equal to 1.4 at the omresson ressure rato 5,at the temerature before the turbne of 1600 K, at the relatve effeny of the omressor and the turbne 0, 85 results n the r r hange of 35 K and 30 K n temerature at the end of the omresson roess n the omressor and at the end of the exanson roess n the turbne resetvely, n ths ase the gas turbne yle effeny fator hanges n %. herefore the aurate determnaton of the sef heat rato values s of hgh mortane.. he ressure deendene of the sef heat rato for the nondeal gas Usually durng the alulatons the heat aaty s taken to be not deendng on ressure and the temerature deendenes at the ressure of 0.1 MPa, resented n the gudelnes [1-3] are used. It should be mentoned that sometmes the referene data resented by varous authors dffer markedly, as t s seen n Fg.1, where the deendenes mentoned above are gven for ar. t Content from ths work may be used under the terms of the Creatve Commons Attrbuton 3.0 lene. Any further dstrbuton of ths work must mantan attrbuton to the author(s) and the ttle of the work, journal taton and DOI. Publshed under lene by IOP Publshng Ltd 1

3 Journal of Physs: Conferene Seres 754 (016) IOP Publshng do: / /754/11/11003 Fgure 1. emerature deendene of the molar heat aaty at onstant ressure of 0.1 MPa he ressure deendene of the ar heat aaty was aroxmated n [4] by the olynomals, obtaned by the table data roessng, but the heat aaty at onstant volume, whh s nluded n the sef heat rato exresson was alulated by the Meyer relaton v R beng true only for the deal gas. he resent exresson s not arorate for the real gas and the relaton between the heat aates s wrtten as v v v v v v he dervatves n the sef heat exresson an be alulated only f the real gas state equaton s known. he ressure deendene at dfferent temeratures was onsdered wth a orreton, 0, 0,, the temerature deendene of the heat aaty at ressure of 0.1 MP, to. (1) he orreton to the ressure deendene was aroxmated by data [3] as follows 4, A ехр 0,1 a 0, () 50 where, A, b b a. (3) 0 1 j0 j 100 j

4 Journal of Physs: Conferene Seres 754 (016) IOP Publshng do: / /754/11/11003 he analytal temerature deendene at ressure of 0.1 MPa was aeted n aordane wth [3]: In ths ase the Redlh-Kwong and Dterh equatons [] are the most adequate equatons []. he devaton from dealty an be also taken nto onsderaton by the omressblty fator v z, the analytal exresson of whh an be obtaned by the referene data roessng [3]. R he roessng results for ar are resented n Fg.. Fgure. emerature deendene of the ar omressblty at dfferent ressures a In Dterh state equaton v b ex R the orretons for the nteratons Rv between moleules and ther volume, defned from the ondton that the frst and the seond order r r dervatves are equal to zero v v 0 n the rtal ont, are as follows v r a R v, b r r. he results of the sef heat rato alulaton by the Dterh equaton are resented n Fg.3. he nondealty onsderaton at the ressure of 4MPa results n the sef heat rato hange from k=1.4 to k=1.5 value, whh results n the temerature nrease from 83 to 93 K at the end of omresson at the omresson ressure rato 5 and at the relatve effeny of the omressor t 0, 85. r r 3

5 Journal of Physs: Conferene Seres 754 (016) IOP Publshng do: / /754/11/11003 Fgure 3. emerature deendene of the ar sef heat rato at dfferent ressures he ressure deendene of the heat aaty s suffent for temeratures less than ~ 700 K, whh are tyal for the end of omresson roesses n the omressor. 3. Conluson hus, the aurate determnaton of the sef heat rato values wth onsderaton of both temerature and ressure deendenes of the heat aaty s of hgh mortane. It s artularly true for the omresson roesses n the omressor as far as at the temeratures tyal for the exanson roesses n the turbne the ressure deendene s not so essental and the gas an be assumed to be deal, and n ths ase only the temerature deendene of the heat aates an be onsdered. hs work was arred out at UrFU and fnanally suorted by the Russan Sene Foundaton (rojet number ). Referenes [1] Rd R, Prausnots J and Shervud 198 he gases and lquds roertes (L.:Chemstry) 59 [] Vargaft N B 1963 he gudelnes for thermal and hysal roertes of gases and lquds (M. Physmathgz) 708 [3] Ravdel A 1983 Quk referene of the hysal and hemal values edted by A.A. Ravdel and A.M. Ponomareva (L. Chemstry) 3 [4] Hasanov N G and Shgaov A B 014 he real ar roertes mat on the statonary gas turbne unts erformane (he ower ndustry roblems N 9-10)

The calculation of ternary vapor-liquid system equilibrium by using P-R equation of state

The calculation of ternary vapor-liquid system equilibrium by using P-R equation of state The alulaton of ternary vapor-lqud syste equlbru by usng P-R equaton of state Y Lu, Janzhong Yn *, Rune Lu, Wenhua Sh and We We Shool of Cheal Engneerng, Dalan Unversty of Tehnology, Dalan 11601, P.R.Chna

More information

Non-Ideality Through Fugacity and Activity

Non-Ideality Through Fugacity and Activity Non-Idealty Through Fugacty and Actvty S. Patel Deartment of Chemstry and Bochemstry, Unversty of Delaware, Newark, Delaware 19716, USA Corresondng author. E-mal: saatel@udel.edu 1 I. FUGACITY In ths dscusson,

More information

Scientific Research of the Institute of Mathematics and Computer Science 1(11) 2012, 23-30

Scientific Research of the Institute of Mathematics and Computer Science 1(11) 2012, 23-30 Please te ts artle as: Grażyna Kałuża, Te numeral soluton of te transent eat onduton roblem usng te latte Boltzmann metod, Sentf Resear of te Insttute of Matemats and Comuter Sene,, Volume, Issue, ages

More information

Energy and metric gauging in the covariant theory of gravitation

Energy and metric gauging in the covariant theory of gravitation Aksaray Unversty Journal of Sene and Engneerng, Vol., Issue,. - (18). htt://dx.do.org/1.9/asujse.4947 Energy and metr gaugng n the ovarant theory of gravtaton Sergey G. Fedosn PO box 61488, Svazeva str.

More information

An identification algorithm of model kinetic parameters of the interfacial layer growth in fiber composites

An identification algorithm of model kinetic parameters of the interfacial layer growth in fiber composites IOP Conference Seres: Materals Scence and Engneerng PAPER OPE ACCESS An dentfcaton algorthm of model knetc parameters of the nterfacal layer growth n fber compostes o cte ths artcle: V Zubov et al 216

More information

Development of the Schrodinger equation for attosecond laser pulse interaction with Planck gas

Development of the Schrodinger equation for attosecond laser pulse interaction with Planck gas Develoment of the Shrodnger equaton for attoseond laser ulse nteraton wth Plank gas M. Kozlowsk 1 * J. Marak Kozlowska 1 Josef Plsudsk Warsaw Unversty, Insttute of Eletron Tehnology Abstrat The reaton

More information

Positivity-preserving and symmetry-preserving Lagrangian schemes for. compressible Euler equations in cylindrical coordinates.

Positivity-preserving and symmetry-preserving Lagrangian schemes for. compressible Euler equations in cylindrical coordinates. Postvty-reservng and symmetry-reservng Lagrangan shemes for omressble Euler equatons n ylndral oordnates Dan Lng, Juan Cheng and Ch-Wang Shu 3 Abstrat For a Lagrangan sheme solvng the omressble Euler equatons

More information

Modeling of Determination of Effective Stress of Soil

Modeling of Determination of Effective Stress of Soil Internatonal Journal of Aled Engneerng Researh ISSN 973-56 olume 3, Number (). 75-755 Researh Inda Publatons. h://www.rublaton.om Modelng of Determnaton of Effetve Stress of Sol Huong Th Thanh Ngo; Bnh

More information

425. Calculation of stresses in the coating of a vibrating beam

425. Calculation of stresses in the coating of a vibrating beam 45. CALCULAION OF SRESSES IN HE COAING OF A VIBRAING BEAM. 45. Calulaton of stresses n the oatng of a vbratng beam M. Ragulsks,a, V. Kravčenken,b, K. Plkauskas,, R. Maskelunas,a, L. Zubavčus,b, P. Paškevčus,d

More information

ME 440 Aerospace Engineering Fundamentals

ME 440 Aerospace Engineering Fundamentals Fall 006 ME 440 Aerosace Engneerng Fundamentals roulson hrust Jet Engne F m( & Rocket Engne F m & F ρ A - n ) ρ A he basc rncle nsde the engne s to convert the ressure and thermal energy of the workng

More information

CANKAYA UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE MECHANICAL ENGINEERING DEPARTMENT ME 212 THERMODYNAMICS II CHAPTER 11 EXAMPLES SOLUTION

CANKAYA UNIVERSITY FACULTY OF ENGINEERING AND ARCHITECTURE MECHANICAL ENGINEERING DEPARTMENT ME 212 THERMODYNAMICS II CHAPTER 11 EXAMPLES SOLUTION CANKAYA UNIVESIY FACULY OF ENGINEEING AND ACHIECUE MECHANICAL ENGINEEING DEPAMEN ME HEMODYNAMICS II CHAPE EXAMPLES SOLUION ) he reure wthn a. m tank hould not exeed 0 ar. Chek the reure wthn the tank f

More information

Uncertainty in measurements of power and energy on power networks

Uncertainty in measurements of power and energy on power networks Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:

More information

Statistical Evaluation of WATFLOOD

Statistical Evaluation of WATFLOOD tatstcal Evaluaton of WATFLD By: Angela MacLean, Dept. of Cvl & Envronmental Engneerng, Unversty of Waterloo, n. ctober, 005 The statstcs program assocated wth WATFLD uses spl.csv fle that s produced wth

More information

Lecture 3 Examples and Problems

Lecture 3 Examples and Problems Lecture 3 Examles and Problems Mechancs & thermodynamcs Equartton Frst Law of Thermodynamcs Ideal gases Isothermal and adabatc rocesses Readng: Elements Ch. 1-3 Lecture 3, 1 Wllam Thomson (1824 1907) a.k.a.

More information

COMPLEX COEFFICIENT OF COMPLEXITY FOR GAME-TREE STRUCTURES IN DISCRETE OPTIMIZATION OF A GEAR PUMP HAVING TEETH UNDERCUTTING

COMPLEX COEFFICIENT OF COMPLEXITY FOR GAME-TREE STRUCTURES IN DISCRETE OPTIMIZATION OF A GEAR PUMP HAVING TEETH UNDERCUTTING COMPLEX COEFFICIENT OF COMPLEXITY FOR GAME-TREE STRUCTURES IN DISCRETE OPTIMIZATION OF A GEAR PUMP HAVING TEETH UNDERCUTTING Adam DEPTUŁA, Maran A. PARTYA Abstrat: A gear um otmzaton requres alulatng olumetr,

More information

Journal of Engineering and Applied Sciences. Ultraspherical Integration Method for Solving Beam Bending Boundary Value Problem

Journal of Engineering and Applied Sciences. Ultraspherical Integration Method for Solving Beam Bending Boundary Value Problem Journal of Engneerng and Appled Senes Volue: Edton: Year: 4 Pages: 7 4 Ultraspheral Integraton Method for Solvng Bea Bendng Boundary Value Proble M El-Kady Matheats Departent Faulty of Sene Helwan UnverstyEgypt

More information

On resolving the optical spectra of the edge plasma radiation against a strong background of the divertor stray light

On resolving the optical spectra of the edge plasma radiation against a strong background of the divertor stray light Journal of Physcs: Conference Seres PAPER OPEN ACCESS On resolvng the optcal spectra of the edge plasma radaton aganst a strong background of the dvertor stray lght To cte ths artcle: L Ognev and V S Lstsa

More information

Implementation of α-qss Stiff Integration Methods for Solving the Detailed Combustion Chemistry

Implementation of α-qss Stiff Integration Methods for Solving the Detailed Combustion Chemistry Proeedngs of the World Congress on Engneerng 2007 Vol II Implementaton of α-qss Stff Integraton Methods for Solvng the Detaled Combuston Chemstry Shafq R. Quresh and Robert Prosser Abstrat Implt methods

More information

Controller Design for Networked Control Systems in Multiple-packet Transmission with Random Delays

Controller Design for Networked Control Systems in Multiple-packet Transmission with Random Delays Appled Mehans and Materals Onlne: 03-0- ISSN: 66-748, Vols. 78-80, pp 60-604 do:0.408/www.sentf.net/amm.78-80.60 03 rans eh Publatons, Swtzerland H Controller Desgn for Networed Control Systems n Multple-paet

More information

Phase Transition in Collective Motion

Phase Transition in Collective Motion Phase Transton n Colletve Moton Hefe Hu May 4, 2008 Abstrat There has been a hgh nterest n studyng the olletve behavor of organsms n reent years. When the densty of lvng systems s nreased, a phase transton

More information

Voltammetry. Bulk electrolysis: relatively large electrodes (on the order of cm 2 ) Voltammetry:

Voltammetry. Bulk electrolysis: relatively large electrodes (on the order of cm 2 ) Voltammetry: Voltammetry varety of eletroanalytal methods rely on the applaton of a potental funton to an eletrode wth the measurement of the resultng urrent n the ell. In ontrast wth bul eletrolyss methods, the objetve

More information

Prediction of Solid Paraffin Precipitation Using Solid Phase Equation of State

Prediction of Solid Paraffin Precipitation Using Solid Phase Equation of State Predton of old Paraffn Preptaton Usng old Phase Equaton of tate Proeedngs of European Congress of Chemal Engneerng (ECCE-6) Copenhagen, 16- eptember 7 Predton of old Paraffn Preptaton Usng old Phase Equaton

More information

Dr. Shalabh Department of Mathematics and Statistics Indian Institute of Technology Kanpur

Dr. Shalabh Department of Mathematics and Statistics Indian Institute of Technology Kanpur Analyss of Varance and Desgn of Exerments-I MODULE III LECTURE - 2 EXPERIMENTAL DESIGN MODELS Dr. Shalabh Deartment of Mathematcs and Statstcs Indan Insttute of Technology Kanur 2 We consder the models

More information

Module 3: The Whole-Process Perspective for Thermochemical Hydrogen

Module 3: The Whole-Process Perspective for Thermochemical Hydrogen "Thermodynamc Analyss of Processes for Hydrogen Generaton by Decomposton of Water" by John P. O'Connell Department of Chemcal Engneerng Unversty of Vrgna Charlottesvlle, VA 2294-4741 A Set of Energy Educaton

More information

Hans-Joachim Kretzschmar and Katja Knobloch

Hans-Joachim Kretzschmar and Katja Knobloch Sulementary Backward Equatons for the Industral Formulaton IAPWS-IF of Water and Steam for Fast Calculatons of Heat Cycles, Bolers, and Steam Turbnes Hans-Joachm Kretzschmar and Katja Knobloch Deartment

More information

Water and ice transfer in porous media near the phase transition point

Water and ice transfer in porous media near the phase transition point Permafrost, Phlls, Srngman & Arenson (eds) 3 Sets & Zetlnger, Lsse, ISBN 9 589 58 7 Water and e transfer n orous meda near the hase transton ont V.S. Kolunn Earth s ryoshere Insttute, SB AS, Tyumen, ussa

More information

Solving the Temperature Problem under Relativistic Conditions within the Frame of the First Principle of Thermodynamics

Solving the Temperature Problem under Relativistic Conditions within the Frame of the First Principle of Thermodynamics Physs & Astronomy Internatonal Journal Solvng the Temperature Problem under Relatvst Condtons wthn the Frame of the Frst Prnple of Thermodynams Abstrat The frst prnples of thermodynams under relatvst ondtons

More information

Managing Capacity Through Reward Programs. on-line companion page. Byung-Do Kim Seoul National University College of Business Administration

Managing Capacity Through Reward Programs. on-line companion page. Byung-Do Kim Seoul National University College of Business Administration Managng Caacty Through eward Programs on-lne comanon age Byung-Do Km Seoul Natonal Unversty College of Busness Admnstraton Mengze Sh Unversty of Toronto otman School of Management Toronto ON M5S E6 Canada

More information

ON DUALITY FOR NONSMOOTH LIPSCHITZ OPTIMIZATION PROBLEMS

ON DUALITY FOR NONSMOOTH LIPSCHITZ OPTIMIZATION PROBLEMS Yugoslav Journal of Oeratons Researh Vol 9 (2009), Nuber, 4-47 DOI: 0.2298/YUJOR09004P ON DUALITY FOR NONSMOOTH LIPSCHITZ OPTIMIZATION PROBLEMS Vasle PREDA Unversty of Buharest, Buharest reda@f.unbu.ro

More information

A New Approach for Assigning Costs and Fuels to Cogeneration Products

A New Approach for Assigning Costs and Fuels to Cogeneration Products Int.J. Appled Thermodynams, ISSN 30-9724 Vol.4, (No.3), pp.45-56, September200 A New Approah for Assgnng Costs and Fuels to Cogeneraton Produts Bert RLACH, George TSATSARONIS, Fran CZISLA Insttute for

More information

ESCI 341 Atmospheric Thermodynamics Lesson 6 Thermodynamic Processes

ESCI 341 Atmospheric Thermodynamics Lesson 6 Thermodynamic Processes ESCI 341 Atmosherc Thermodynamcs Lesson 6 Thermodynamc Processes Reerences: An Introducton to Atmosherc Thermodynamcs, Tsons Introducton to Theoretcal Meteorology, Hess Physcal Chemstry (4 th edton), Lene

More information

Opportunities in Analytical Approaches to Spray Drying of Solid Dosage Forms

Opportunities in Analytical Approaches to Spray Drying of Solid Dosage Forms Opportuntes n Analytal Approahes to Spray Dryng of Sold Dosage Forms Dr. Renhard Vehrng Assoate Professor and George Ford Char n Materals Engneerng Unversty of Alberta, Department of Mehanal Engneerng

More information

Exercise 10: Theory of mass transfer coefficient at boundary

Exercise 10: Theory of mass transfer coefficient at boundary Partle Tehnology Laboratory Prof. Sotrs E. Pratsns Sonneggstrasse, ML F, ETH Zentrum Tel.: +--6 5 http://www.ptl.ethz.h 5-97- U Stoffaustaush HS 7 Exerse : Theory of mass transfer oeffent at boundary Chapter,

More information

PHYSICS 212 MIDTERM II 19 February 2003

PHYSICS 212 MIDTERM II 19 February 2003 PHYSICS 1 MIDERM II 19 Feruary 003 Exam s losed ook, losed notes. Use only your formula sheet. Wrte all work and answers n exam ooklets. he aks of pages wll not e graded unless you so request on the front

More information

Evaluating Thermodynamic Properties in LAMMPS

Evaluating Thermodynamic Properties in LAMMPS D. Keffer ME 64 Det. of Materals cence & Engneerng Unversty of ennessee Knoxvlle Evaluatng hermodynamc Proertes n LAMMP Davd Keffer Deartment of Materals cence & Engneerng Unversty of ennessee Knoxvlle

More information

Estimation of the composition of the liquid and vapor streams exiting a flash unit with a supercritical component

Estimation of the composition of the liquid and vapor streams exiting a flash unit with a supercritical component Department of Energ oltecnco d Mlano Va Lambruschn - 05 MILANO Eercses of Fundamentals of Chemcal rocesses rof. Ganpero Gropp Eercse 8 Estmaton of the composton of the lqud and vapor streams etng a unt

More information

EC3075 Mathematical Approaches to Economics

EC3075 Mathematical Approaches to Economics EC3075 Mathematal Aroahes to Eonoms etures 7-8: Dualt and Constraned Otmsaton Pemberton & Rau haters 7-8 Dr Gaa Garno [Astle Clarke Room 4 emal: gg44] Dualt n onsumer theor We wll exose the rmal otmsaton

More information

Effect of the r-value change on the forming limit analysis for a ultra-low carbon steel sheet

Effect of the r-value change on the forming limit analysis for a ultra-low carbon steel sheet Journal of Physcs: Conference Seres PAPER OPEN ACCESS Effect of the r-value change on the formng lmt analyss for a ultra-low carbon steel sheet Related content - Effect of deformaton twnnng on formng lmt

More information

Tom BLASINGAME Texas A&M U. Slide 1

Tom BLASINGAME Texas A&M U. Slide 1 Fundamental Flow Lecture 3 Materal Balance Concets Slde 1 Fundamental Flow Lecture 3 Materal Balance Concets Slde 2 Fundamental Flow Lecture 3 Materal Balance Concets Materal Balance Notes from Deartment

More information

Research on dynamic adjustment of cooperation in price duopoly game

Research on dynamic adjustment of cooperation in price duopoly game 3rd Internatonal Conferene on Mehatrons and Informaton Tehnology (ICMIT 06 Researh on dynam adjustment of ooeraton n re duooly game Gung ShaDehang XabYujng gao3bentu L4dDehua Wang5e 345 Shandong Voatonal

More information

A Solution of the Harry-Dym Equation Using Lattice-Boltzmannn and a Solitary Wave Methods

A Solution of the Harry-Dym Equation Using Lattice-Boltzmannn and a Solitary Wave Methods Appled Mathematcal Scences, Vol. 11, 2017, no. 52, 2579-2586 HIKARI Ltd, www.m-hkar.com https://do.org/10.12988/ams.2017.79280 A Soluton of the Harry-Dym Equaton Usng Lattce-Boltzmannn and a Soltary Wave

More information

technische universiteit eindhoven Analysis of one product /one location inventory control models prof.dr. A.G. de Kok 1

technische universiteit eindhoven Analysis of one product /one location inventory control models prof.dr. A.G. de Kok 1 TU/e tehnshe unverstet endhoven Analyss of one produt /one loaton nventory ontrol models prof.dr. A.G. de Kok Aknowledgements: I would lke to thank Leonard Fortun for translatng ths ourse materal nto Englsh

More information

FAULT DETECTION AND IDENTIFICATION BASED ON FULLY-DECOUPLED PARITY EQUATION

FAULT DETECTION AND IDENTIFICATION BASED ON FULLY-DECOUPLED PARITY EQUATION Control 4, Unversty of Bath, UK, September 4 FAUL DEECION AND IDENIFICAION BASED ON FULLY-DECOUPLED PARIY EQUAION C. W. Chan, Hua Song, and Hong-Yue Zhang he Unversty of Hong Kong, Hong Kong, Chna, Emal:

More information

GEL 446: Applied Environmental Geology

GEL 446: Applied Environmental Geology GE 446: ppled Envronmental Geology Watershed Delneaton and Geomorphology Watershed Geomorphology Watersheds are fundamental geospatal unts that provde a physal and oneptual framewor wdely used by sentsts,

More information

This column is a continuation of our previous column

This column is a continuation of our previous column Comparson of Goodness of Ft Statstcs for Lnear Regresson, Part II The authors contnue ther dscusson of the correlaton coeffcent n developng a calbraton for quanttatve analyss. Jerome Workman Jr. and Howard

More information

Confidence intervals for weighted polynomial calibrations

Confidence intervals for weighted polynomial calibrations Confdence ntervals for weghted olynomal calbratons Sergey Maltsev, Amersand Ltd., Moscow, Russa; ur Kalambet, Amersand Internatonal, Inc., Beachwood, OH e-mal: kalambet@amersand-ntl.com htt://www.chromandsec.com

More information

Active Structural Acoustic Control of Sound Radiation from Flat Plates

Active Structural Acoustic Control of Sound Radiation from Flat Plates Proeedngs of th Internatonal Congress on Aousts, ICA 10 23-27 August 10, Sydney, Australa Atve Strutural Aoust Control of Sound Radaton from Flat Plates Xa Pan and James A. Forrest Martme Platforms Dvson,

More information

Variance of Estimates in Dynamic Data Reconciliation

Variance of Estimates in Dynamic Data Reconciliation 9 th Eropean Sypos on Copter Aded Proess Engneerng ESCAPE9 J. Jeżowsk and J. hlle (Edtors) 2009 Elsever B.V./Ltd. All rghts reserved. Varane of Estates n Dyna Data Reonlaton Chrstophe Ullrh, Georges Heyen

More information

Adsorption: A gas or gases from a mixture of gases or a liquid (or liquids) from a mixture of liquids is bound physically to the surface of a solid.

Adsorption: A gas or gases from a mixture of gases or a liquid (or liquids) from a mixture of liquids is bound physically to the surface of a solid. Searatons n Chemcal Engneerng Searatons (gas from a mxture of gases, lquds from a mxture of lquds, solds from a soluton of solds n lquds, dssolved gases from lquds, solvents from gases artally/comletely

More information

SUPPORTING INFORMATION

SUPPORTING INFORMATION A mult-sale study o MOFs as adsorbents n H PSA uraton Ana-Mara Banu, Danel Fredrh, Steano Brandan, na Düren* Insttute or Materals and Proesses, Shool o Engneerng, he Unversty o Ednburgh, Sanderson Buldng,

More information

Simulated Power of the Discrete Cramér-von Mises Goodness-of-Fit Tests

Simulated Power of the Discrete Cramér-von Mises Goodness-of-Fit Tests Smulated of the Cramér-von Mses Goodness-of-Ft Tests Steele, M., Chaselng, J. and 3 Hurst, C. School of Mathematcal and Physcal Scences, James Cook Unversty, Australan School of Envronmental Studes, Grffth

More information

STEADY-STATE CAVITATING NOZZLE FLOWS WITH NUCLEATION

STEADY-STATE CAVITATING NOZZLE FLOWS WITH NUCLEATION Ca-GS-- Ffth Internatonal Symosum on Cataton (a) Osaka, Jaan, Noember -, STEADY-STATE CAVITATING NOZZE FOWS WITH NUCEATION Can F. Delale Deartment of Aeronauts Astronauts, Istanbul Tehnal Unersty, 866

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle

More information

Performance Modeling of Hierarchical Memories

Performance Modeling of Hierarchical Memories Performane Modelng of Herarhal Memores Marwan Sleman, Lester Lpsky, Kshor Konwar Department of omputer Sene and Engneerng Unversty of onnetut Storrs, T 0669-55 Emal: {marwan, lester, kshor}@engr.uonn.edu

More information

Gravity Drainage Prior to Cake Filtration

Gravity Drainage Prior to Cake Filtration 1 Gravty Dranage Pror to ake Fltraton Sott A. Wells and Gregory K. Savage Department of vl Engneerng Portland State Unversty Portland, Oregon 97207-0751 Voe (503) 725-4276 Fax (503) 725-4298 ttp://www.e.pdx.edu/~wellss

More information

The Exact Formulation of the Inverse of the Tridiagonal Matrix for Solving the 1D Poisson Equation with the Finite Difference Method

The Exact Formulation of the Inverse of the Tridiagonal Matrix for Solving the 1D Poisson Equation with the Finite Difference Method Journal of Electromagnetc Analyss and Applcatons, 04, 6, 0-08 Publshed Onlne September 04 n ScRes. http://www.scrp.org/journal/jemaa http://dx.do.org/0.46/jemaa.04.6000 The Exact Formulaton of the Inverse

More information

APPENDIX 2 FITTING A STRAIGHT LINE TO OBSERVATIONS

APPENDIX 2 FITTING A STRAIGHT LINE TO OBSERVATIONS Unversty of Oulu Student Laboratory n Physcs Laboratory Exercses n Physcs 1 1 APPEDIX FITTIG A STRAIGHT LIE TO OBSERVATIOS In the physcal measurements we often make a seres of measurements of the dependent

More information

Convection Heat Transfer. Textbook: Convection Heat Transfer. Reference: Convective Heat and Mass Transfer. Convection Heat Transfer

Convection Heat Transfer. Textbook: Convection Heat Transfer. Reference: Convective Heat and Mass Transfer. Convection Heat Transfer Convecton Heat Transfer Tetbook: Convecton Heat Transfer Adran Bean, John Wley & Sons Reference: Convectve Heat and Mass Transfer Kays, Crawford, and Wegand, McGraw-Hll Convecton Heat Transfer Vedat S.

More information

2-Adic Complexity of a Sequence Obtained from a Periodic Binary Sequence by Either Inserting or Deleting k Symbols within One Period

2-Adic Complexity of a Sequence Obtained from a Periodic Binary Sequence by Either Inserting or Deleting k Symbols within One Period -Adc Comlexty of a Seuence Obtaned from a Perodc Bnary Seuence by Ether Insertng or Deletng Symbols wthn One Perod ZHAO Lu, WEN Qao-yan (State Key Laboratory of Networng and Swtchng echnology, Bejng Unversty

More information

HEAT PERFORMANCE ANALYSIS OF MULTI-FLUID HEAT EXCHANGERS

HEAT PERFORMANCE ANALYSIS OF MULTI-FLUID HEAT EXCHANGERS HEA PERFORANCE ANALYSIS OF ULI-FLUID HEA EXCHANGERS A hess Submtted to the Faulty Of Purdue Unversty By Sang Bae Par Advsor: Dr. S. S. Krshnan /3/2003 HEA EXCHANGERS Deves that provde flow of thermal energy

More information

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH Turbulence classfcaton of load data by the frequency and severty of wnd gusts Introducton Oscar Moñux, DEWI GmbH Kevn Blebler, DEWI GmbH Durng the wnd turbne developng process, one of the most mportant

More information

Physics 41 Chapter 22 HW Serway 7 th Edition

Physics 41 Chapter 22 HW Serway 7 th Edition yss 41 apter H Serway 7 t Edton oneptual uestons: 1,, 8, 1 roblems: 9, 1, 0,, 7, 9, 48, 54, 55 oneptual uestons: 1,, 8, 1 1 Frst, te effeny of te automoble engne annot exeed te arnot effeny: t s lmted

More information

Logistic regression with one predictor. STK4900/ Lecture 7. Program

Logistic regression with one predictor. STK4900/ Lecture 7. Program Logstc regresson wth one redctor STK49/99 - Lecture 7 Program. Logstc regresson wth one redctor 2. Maxmum lkelhood estmaton 3. Logstc regresson wth several redctors 4. Devance and lkelhood rato tests 5.

More information

BLEVE: Theory and Importance in Oil Recovery

BLEVE: Theory and Importance in Oil Recovery The Open Thermodynams Journal, 2008, 2, 89-94 89 BLEVE: Theory and Importane n Ol Reovery Open Aess Anthony A. Clfford* Department of Chemstry, Unversty of Leeds, Leeds LS2 9JT, UK Abstrat: BLEVEs as phenomena

More information

x = , so that calculated

x = , so that calculated Stat 4, secton Sngle Factor ANOVA notes by Tm Plachowsk n chapter 8 we conducted hypothess tests n whch we compared a sngle sample s mean or proporton to some hypotheszed value Chapter 9 expanded ths to

More information

Physics 4C. Chapter 19: Conceptual Questions: 6, 8, 10 Problems: 3, 13, 24, 31, 35, 48, 53, 63, 65, 78, 87

Physics 4C. Chapter 19: Conceptual Questions: 6, 8, 10 Problems: 3, 13, 24, 31, 35, 48, 53, 63, 65, 78, 87 Physcs 4C Solutons to Chater 9 HW Chater 9: Concetual Questons: 6, 8, 0 Problems:,, 4,,, 48,, 6, 6, 78, 87 Queston 9-6 (a) 0 (b) 0 (c) negate (d) oste Queston 9-8 (a) 0 (b) 0 (c) negate (d) oste Queston

More information

EXCESS FUNCTIONS MATHEMATICAL EXPLANATION

EXCESS FUNCTIONS MATHEMATICAL EXPLANATION EXCESS FUNCTIONS Excess functons... 1 Mathematcal exlanaton... 1 Physcal examle: Molar volume of a ure substance... 2 Chemcal otental for a ure substance... 3 Actvty, actvty coeffcent and fugacty (ure

More information

Taylor series coefficients of the HP-polynomial as an invariant for links in the solid torus

Taylor series coefficients of the HP-polynomial as an invariant for links in the solid torus Al. Math. Inf. c. 7, No. 1, 23-28 (213) 23 Aled Mathematcs & Informaton cences An Internatonal Journal c 213 NP Natural cences Publshng Cor. aylor seres coeffcents of the HP-olynomal as an nvarant for

More information

Temperature. Chapter Heat Engine

Temperature. Chapter Heat Engine Chapter 3 Temperature In prevous chapters of these notes we ntroduced the Prncple of Maxmum ntropy as a technque for estmatng probablty dstrbutons consstent wth constrants. In Chapter 9 we dscussed the

More information

Diffusion Mass Transfer

Diffusion Mass Transfer Dffuson Mass Transfer General onsderatons Mass transfer refers to mass n transt due to a speces concentraton gradent n a mture. Must have a mture of two or more speces for mass transfer to occur. The speces

More information

One-sided finite-difference approximations suitable for use with Richardson extrapolation

One-sided finite-difference approximations suitable for use with Richardson extrapolation Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,

More information

Chapter 3 The Kinetic Theory of Gases 3.1. Ideal Gases Experimental Laws and the Equation of State

Chapter 3 The Kinetic Theory of Gases 3.1. Ideal Gases Experimental Laws and the Equation of State Chater 3 The Knetc Theory of Gases 3.1. Ideal Gases 3.1.1. Exermental Laws and the Equaton of State 3.1.2. Molecular Model of an Ideal Gas 3.3. Mean Free Path 3.4. The Boltzmann Dstrbuton Law and The Dstrbuton

More information

A computer-aided optimization method of bending beams

A computer-aided optimization method of bending beams WSES Internatonal Conferene on ENGINEERING MECHNICS, STRUCTURES, ENGINEERING GEOLOGY (EMESEG '8), Heraklon, Crete Island, Greee, July 22-24, 28 omputer-aded optmzaton method of bendng beams CRMEN E. SINGER-ORCI

More information

Determination of the response distributions of cantilever beam under sinusoidal base excitation

Determination of the response distributions of cantilever beam under sinusoidal base excitation Journal of Physcs: Conference Seres OPEN ACCESS Determnaton of the response dstrbutons of cantlever beam under snusodal base exctaton To cte ths artcle: We Sun et al 13 J. Phys.: Conf. Ser. 448 11 Vew

More information

Horizontal mergers for buyer power. Abstract

Horizontal mergers for buyer power. Abstract Horzontal mergers for buyer power Ramon Faul-Oller Unverstat d'alaant Llus Bru Unverstat de les Illes Balears Abstrat Salant et al. (1983) showed n a Cournot settng that horzontal mergers are unproftable

More information

NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS

NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS IJRRAS 8 (3 September 011 www.arpapress.com/volumes/vol8issue3/ijrras_8_3_08.pdf NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS H.O. Bakodah Dept. of Mathematc

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

Testing for seasonal unit roots in heterogeneous panels

Testing for seasonal unit roots in heterogeneous panels Testng for seasonal unt roots n heterogeneous panels Jesus Otero * Facultad de Economía Unversdad del Rosaro, Colomba Jeremy Smth Department of Economcs Unversty of arwck Monca Gulett Aston Busness School

More information

The Tangential Force Distribution on Inner Cylinder of Power Law Fluid Flowing in Eccentric Annuli with the Inner Cylinder Reciprocating Axially

The Tangential Force Distribution on Inner Cylinder of Power Law Fluid Flowing in Eccentric Annuli with the Inner Cylinder Reciprocating Axially Open Journal of Flud Dynamcs, 2015, 5, 183-187 Publshed Onlne June 2015 n ScRes. http://www.scrp.org/journal/ojfd http://dx.do.org/10.4236/ojfd.2015.52020 The Tangental Force Dstrbuton on Inner Cylnder

More information

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS

More information

Water Hammer in Pipes

Water Hammer in Pipes Waer Haer Hydraulcs and Hydraulc Machnes Waer Haer n Pes H Pressure wave A B If waer s flowng along a long e and s suddenly brough o res by he closng of a valve, or by any slar cause, here wll be a sudden

More information

11/19/2013. PHY 113 C General Physics I 11 AM 12:15 PM MWF Olin 101

11/19/2013. PHY 113 C General Physics I 11 AM 12:15 PM MWF Olin 101 PHY 113 C General Pyss I 11 AM 12:15 PM MWF Oln 101 Plan or Leture 23: Capter 22: Heat engnes 1. ermodynam yles; work and eat eeny 2. Carnot yle 3. Otto yle; desel yle 4. Bre omments on entropy 11/19/2013

More information

Chapter 13: Multiple Regression

Chapter 13: Multiple Regression Chapter 13: Multple Regresson 13.1 Developng the multple-regresson Model The general model can be descrbed as: It smplfes for two ndependent varables: The sample ft parameter b 0, b 1, and b are used to

More information

A Hybrid Variational Iteration Method for Blasius Equation

A Hybrid Variational Iteration Method for Blasius Equation Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method

More information

Chapter 12 Lyes KADEM [Thermodynamics II] 2007

Chapter 12 Lyes KADEM [Thermodynamics II] 2007 Chapter 2 Lyes KDEM [Therodynacs II] 2007 Gas Mxtures In ths chapter we wll develop ethods for deternng therodynac propertes of a xture n order to apply the frst law to systes nvolvng xtures. Ths wll be

More information

ENV05: METROLOGY FOR OCEAN SALINITY AND ACIDITY

ENV05: METROLOGY FOR OCEAN SALINITY AND ACIDITY Kck-off meetng EMRP ENV5 Ocean Metrology - Setember, PB Berln ENV5: MEROLOGY FOR OCEAN SALINIY AND ACIDIY WP: Extenson of measurement range for thermohyscal arameters (INRM, PB) ISIUO MEROLOGICA Smona

More information

Color Rendering Uncertainty

Color Rendering Uncertainty Australan Journal of Basc and Appled Scences 4(10): 4601-4608 010 ISSN 1991-8178 Color Renderng Uncertanty 1 A.el Bally M.M. El-Ganany 3 A. Al-amel 1 Physcs Department Photometry department- NIS Abstract:

More information

AGC Introduction

AGC Introduction . Introducton AGC 3 The prmary controller response to a load/generaton mbalance results n generaton adjustment so as to mantan load/generaton balance. However, due to droop, t also results n a non-zero

More information

Conceptual design of independently configurable Mach 6.8 hydrogen fuelled dual mode scramjet propulsion system

Conceptual design of independently configurable Mach 6.8 hydrogen fuelled dual mode scramjet propulsion system Student Researh Paper Conferene Vol-1, No-4, Aug 214 Coneptual desgn of ndependently onfgurable Mah 6.8 hydrogen fuelled dual mode sramjet propulson system Qasm Manzoor Dept. of Aerospae, CAE Natonal Unversty

More information

If two volatile and miscible liquids are combined to form a solution, Raoult s law is not obeyed. Use the experimental data in Table 9.

If two volatile and miscible liquids are combined to form a solution, Raoult s law is not obeyed. Use the experimental data in Table 9. 9.9 Real Solutons Exhbt Devatons from Raoult s Law If two volatle and mscble lquds are combned to form a soluton, Raoult s law s not obeyed. Use the expermental data n Table 9.3: Physcal Chemstry 00 Pearson

More information

Module 3: Element Properties Lecture 1: Natural Coordinates

Module 3: Element Properties Lecture 1: Natural Coordinates Module 3: Element Propertes Lecture : Natural Coordnates Natural coordnate system s bascally a local coordnate system whch allows the specfcaton of a pont wthn the element by a set of dmensonless numbers

More information

Compressor map prediction tool

Compressor map prediction tool IOP Conference Seres: Materals Scence and Engneerng PAPER OPEN ACCESS Compressor map predcton tool To cte ths artcle: Arjun Rav et al 015 IOP Conf. Ser.: Mater. Sc. Eng. 90 0104 Vew the artcle onlne for

More information

The finite element method explicit scheme for a solution of one problem of surface and ground water combined movement

The finite element method explicit scheme for a solution of one problem of surface and ground water combined movement IOP Conference Seres: Materals Scence and Engneerng PAPER OPEN ACCESS e fnte element metod explct sceme for a soluton of one problem of surface and ground water combned movement o cte ts artcle: L L Glazyrna

More information

A General Class of Selection Procedures and Modified Murthy Estimator

A General Class of Selection Procedures and Modified Murthy Estimator ISS 684-8403 Journal of Statstcs Volume 4, 007,. 3-9 A General Class of Selecton Procedures and Modfed Murthy Estmator Abdul Bast and Muhammad Qasar Shahbaz Abstract A new selecton rocedure for unequal

More information

Modeling the Phase Composition of Gas Condensate in Pipelines

Modeling the Phase Composition of Gas Condensate in Pipelines IOP Conferene Seres: Materals Sene and Enneern PAPER OPE ACCESS Modeln the Phase Composton of Gas Condensate n Ppelnes To te ths artle: S M Dudn et al 016 IOP Conf. Ser.: Mater. S. En. 154 01010 Vew the

More information

Departure Process from a M/M/m/ Queue

Departure Process from a M/M/m/ Queue Dearture rocess fro a M/M// Queue Q - (-) Q Q3 Q4 (-) Knowledge of the nature of the dearture rocess fro a queue would be useful as we can then use t to analyze sle cases of queueng networs as shown. The

More information

Cite This: J. Chem. Theory Comput. XXXX, XXX, XXX XXX

Cite This: J. Chem. Theory Comput. XXXX, XXX, XXX XXX Cte Ths: ubs.as.org/jctc Comarson between the Bethe aleter Equaton and Confguraton nteraton Aroahes for olvng a Quantum Chemstry Problem: Calulatng the Extaton Energy for Fnte D ubbard Chans Q Ou and Joseh

More information

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850) hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In

More information

Quantum Particle Motion in Physical Space

Quantum Particle Motion in Physical Space Adv. Studes Theor. Phys., Vol. 8, 014, no. 1, 7-34 HIKARI Ltd, www.-hkar.co http://dx.do.org/10.1988/astp.014.311136 Quantu Partcle Moton n Physcal Space A. Yu. Saarn Dept. of Physcs, Saara State Techncal

More information

Concrete strength evaluation using fracture mechanics technology

Concrete strength evaluation using fracture mechanics technology (016) DOI: 10.1051/ matecconf/0168601014 IPICSE-016 Concrete strength evaluaton usng fracture mechancs technology Valery Poov 1, Dmtry Poov 1, and Anna Davdenko 1. 1 Samara State Techncal Unversty, Insttute

More information