Nernst-Planck equation

Size: px
Start display at page:

Download "Nernst-Planck equation"

Transcription

1 NenstPlan equaton The man poblem o the peous appoahes s that t s ey dult to estmate the ouplng between on luxes. n the NenstPlan appoxmaton t s assumed that l, ; Ths seems to mean that the luxes ae deoupled but due to the eletoneutalty ondton and the denton o elet uent densty,.4 thee s stong ouplng. Hene, wtng the on phenomenologal equaton and expandng the eletohemal potental, l m~ ln 3., l, 3. and ntodung the phenomenologal oeent, l we eah the NenstPlan equaton: ; / Aboe equaton apples n the Htto eeene ame o, n the absene o oneton, n the xed laboatoy oodnates.

2 thee s oneton n the system e.g. soluton low aoss a membane, we add the oespondng tem: 3.5 duson mgaton oneton on lux thus depends on thee atos: duson due to the onentaton gadent s law, mgaton eletophoess due to the potental gadent and oneton due to the solent low pumpng, stng. t has to be ealed that the oneton tem does not ognate om the gadent o the eletohemal potental but due to mehanal oes. t meely maes the onneton between the eeene ames. Solent low due to the gadent o the hemal potental o the solent.e. osmoss s possble but that eques an osmot membane that does not n pnple allow any solute low. Let s multply Eq. 3.5 by and sum oe all the spees: 3.6 The st obseaton s that the last tem s eo due to eletoneutalty,.e. oneton has no ontbuton to elet uent. Solng om aboe, t s obtaned m t t ln ln / 3.7

3 n Eq. 3.7 we hae used the ondutane o the soluton and the tanspot numbe o an on : t Eq. 3.7 has a ey poound message. Potental dop n the system has an eesble ontbuton, ohm loss,, and a eesble pat, duson potental. n the absene o onentaton gadents, we an wte the Ohm s law E and the dsspaton unton qohm E E that s nown as Joule heat. Although elet uent wee eo on luxes exst due to duson potental but the luxes o aton and anon spees must balane eah othe so that eletoneutalty s ept. Ohm potental dop always omes om an extenal soue and duson potental s an ntenal popety, asng om the deenes between the on mobltes see eq..88 n the textboo. Theeoe, duson potental usually s athe low, unless a system nludes ons wth sgnantly hgh moblty, suh as H o OH, o ey lage ons wth low moblty. As explaned n detal on p. 54 o the textboo, the deene between on mgaton and onduton s that the ome taes plae due to the total potental gadent, nludng both the ohm and duson potental, whle the latte omes only om the extenal soue uent. When we ay out an eletohemal expement we wsh to hae ontol oe the eletode potental but, n pate, the oltage we apply between the eletodes s patly onsumed n the ohm loss and duson potental. n the lght o Eq. 3.7 and 3.9 t s obous that neasng the soluton ondutty, we an edue these losses. These leads us to the onept o a suppotng eletolyte and a taeon to whh we etun late on

4 The analyss o a bnay system s useul n eealng some mpotant aspets o on tanspot. Let s onsde agan an eletolyte A u B u dssoatng ompletely to ons A and B. Hene, u and u whee s the eletolyte onentaton. Eletoneutalty eads u u. Let s wte the NenstPlan equatons o the both spees: u u u 3. u u u Summng aboe equatons ges u u u u Realng that / t s obtaned ate some algeba that u u u u u u u u u dentyng the ollowng goups o aables, u u ; u u u u u u u 3.3

5 u t ; t t u u we an wte the tanspot equaton as eale pesented: t u u ;, Eq. 3.3 s nown as the NenstHatley equaton, and s the duson oeent o the eletolyte. t shows that an on annot duse by tsel but t s oupled to a ounteon. Ths s tue also n a multomponent system although the equatons beome ey omplated. That s also the eason why sngle on mobltes annot be measued om the ondutane data o eletolytes home exese. nstead, loong at and the tanspot numbe t, that ae both measuable quanttes, t u u Example: The duson oeent o H s m /s, that o Cl.3 5 m /s and that o SO m /s. om the NenstHatley equaton, the duson oeent o HCl s m /s and that o H SO m /s. Ths shows that these anons slow down the tanse o H, whle H s aeleatng the tanse o the slowe anons. Ths s exatly the eet o duson potental, eleted n the alues o the eletolyte duson oeents. ue to nheent ouplng o on luxes a longange eletostat nteatons NenstPlan equaton wos ey nely, apat om ey onentated solutons. n ey onentated solutons onon nteatons beome moe mpotant, whh eques anothe appoah. 3.6

6 SteanMaxwell ton oeent appoah n onentated solutons the most natual appoah s to onsde the nteatons between all spees n the soluton. When a solute s tanseng though a soluton t olldes wth solent moleules and othe solutes, ausng ton to ts tanse. The tonal oe depends on the stength o the nteaton, haateed wth a ton oeent ', the numbe o ollsons, the numbe o patles le n the net gas theoy, expessed n mole atons, and the elate speed o the olldng patles. At steadystate, the dng oe o tanse s equal but opposte to the ton oes: dng oe tonal oe we onsde duson, the dng oe ould be the onentaton gadent, leadng to ' x 3.7 We an deelop uthe the let hand sde: ln m ' x m ' x 3.8 n ode to poeed, let s onsde st the smplest ase, a bnay soluton. om eq. 3.8, m 3.9 whee the mole aton and ae nluded n.

7 n the Htto eeene ame the solute lux s expessed as H m m x 3.9 The aboe equaton ntodues the SteanMaxwell duson oeent x ' 3. At modeately dlute solutons x and m ln /. Hene, H 3. At modeately dlute solutons the an and SteanMaxwell duson oeents thus ae equal, but de at hgh onentatons sgnantly. o a spheal patle the Stoes law ges the ton oeent as 6pR hn A, leadng to» BT 6pR hn 6pR h A 3. whee R s the patle adus and N A the Aogado s numbe. Although Stoes law was deed o maosop patles t wos supsngly well also to moleules and ons but not o ons n wate, see next page.

8 Valdty o Stoes law o and Cs n aous solents. l

9 Consdeng a bnay eletolyte soluton whee a salt dssoates nto u atons wth the hage numbe and u anons wth the hage numbe u u, the tanspot equatons beome ~ ~ m m 3.3 Also hee Onsage s epoal theoem apples,. Elet uent densty n Htto eeene s [ ] [ ] H H 3.4 Eq. 3.4 one agan shows that elet uent s ndependent o the eeene eloty hee and n the absene o uent n that ase the lux beomes staght om eq. 3.9, eplang. [ ] œ ß ø Œ º Ø g g m x x x ln ln ln H 3.5 The aboe equaton esembles the NenstPlan equaton wth the exepton o the atty oeent oeton. As the plot n the ollowng page shows, ths oeton tem an eah up to a. % sgnane n the ase o NaCl n wate. n pnple, ths oeton ould be mposed also n the NenstPlan equaton. ln / ln g ~ : m wth m

10 n the ase o pue onduton, n the absene o onentaton gadents, the equatons ae 3.6 Ths pa o equatons an be teated as ollows: 3.7 Subtatng eqs. 3.7 om eah othe ges note Onsage s theoem œ ß ø Œ º Ø 3.8 Solng n the om o Ohm s law, the ondutty s eahed as textboo eq..47, / / 3.9

11 n the pesene o both onentaton gadents and elet uent the textboo pesents the appopate equatons,.5.58, pp An nteestng example s on lquds,.e. solents that ae omed om atons and anons. n that ase the solent s also a hage ae and dssolng any eletolyte n an on lqud maes the system at least tenay, moe oten quatenay. The tanspot o an eletolyte n an on lqud s hadly desbed wth the NenstPlan equaton o s laws. Only when the onentaton o an eletolyte s ey low ompaed wth the on lqud these appoahes an be appled wth ae. n the ase o an on lqud alone, no onentaton gadents an exst, and the only possble tanspot poess s elet onduton: 3.3 Note that these equatons ae atually dental beause and. om ethe o these equatons t s obtaned: Hene, the only deene to the NenstPlan equaton s the SteanMaxwell duson oeent. Measung the ondutty o an on lqud the ton oeent and an be detemned.

12 we hae an on lqud A B and an eletolyte A Cl 3, the ollowng expesson an be deed ate lengthy algeba* t 3 3 M Ø m m ø t3 3 Œ 3 3 œ 3 3 M 3 M ß º whee M and ae the mola mass and mola olume o the eletolyte, espetely. Only at the lmt 3 «the tanspot equaton o Cl edue to the om o s law o NenstPlan wth elet uent, and 3 taes the om 3» The poblem o the SteanMaxwell omalsm s obous: the alues o the ton oeents ae meely unnown. Yet, t s the most appopate appoah as t onsdes all the nteatons n the soluton. t s lea that the teatment o multon systems beomes extemely dult. Theeoe, the NenstPlan equaton has eeed the mao ole n the study o on tanspot. SteanMaxwell appoah s used n modellng the tanspot o, e.g. mxtues o hydoabons n petohemal ndusty. * T. Vana et al. Eletohma Ata

The virial theorem and the kinetic energy of particles of a macroscopic system in the general field concept

The virial theorem and the kinetic energy of particles of a macroscopic system in the general field concept Contnuum Mehans and Themodynams, Vol. 9, Issue, pp. 61-71 (16). https://dx.do.og/1.17/s161-16-56-8. The al theoem and the knet enegy of patles of a maosop system n the geneal feld onept Segey G. Fedosn

More information

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Physics 2A Chapter 11 - Universal Gravitation Fall 2017 Physcs A Chapte - Unvesal Gavtaton Fall 07 hese notes ae ve pages. A quck summay: he text boxes n the notes contan the esults that wll compse the toolbox o Chapte. hee ae thee sectons: the law o gavtaton,

More information

Introduction to Thermodynamics

Introduction to Thermodynamics Unestà d sa Intoduton to hemodynams.. Intoduton. Hstoy of of hemodynams.. he he Fst Fst Law. Mosop ew. Joule 3. 3. he he eond Law. Mosop ew. Canot 4. 4. hemodynam opetes of of Fluds 5. 5. Multomponent

More information

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model 6. ntoucton to anssto mples: oncepts an Small-Sgnal Moel Lectue notes: Sec. 5 Sea & Smth 6 th E: Sec. 5.4, 5.6 & 6.3-6.4 Sea & Smth 5 th E: Sec. 4.4, 4.6 & 5.3-5.4 EE 65, Wnte203, F. Najmaba Founaton o

More information

Computational Vision. Camera Calibration

Computational Vision. Camera Calibration Comutatonal Vson Camea Calbaton uo hate 6 Camea Calbaton Poblem: Estmate amea s etns & ntns aametes MthdU Method: Use mage(s) () o knon sene ools: Geomet amea models SVD and onstaned least-squaes Lne etaton

More information

Remember: When an object falls due to gravity its potential energy decreases.

Remember: When an object falls due to gravity its potential energy decreases. Chapte 5: lectc Potental As mentoned seveal tmes dung the uate Newton s law o gavty and Coulomb s law ae dentcal n the mathematcal om. So, most thngs that ae tue o gavty ae also tue o electostatcs! Hee

More information

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o? Test 1 phy 0 1. a) What s the pupose of measuement? b) Wte all fou condtons, whch must be satsfed by a scala poduct. (Use dffeent symbols to dstngush opeatons on ectos fom opeatons on numbes.) c) What

More information

LINEAR MOMENTUM. product of the mass m and the velocity v r of an object r r

LINEAR MOMENTUM. product of the mass m and the velocity v r of an object r r LINEAR MOMENTUM Imagne beng on a skateboad, at est that can move wthout cton on a smooth suace You catch a heavy, slow-movng ball that has been thown to you you begn to move Altenatvely you catch a lght,

More information

4.4 Continuum Thermomechanics

4.4 Continuum Thermomechanics 4.4 Contnuum Themomechancs The classcal themodynamcs s now extended to the themomechancs of a contnuum. The state aables ae allowed to ay thoughout a mateal and pocesses ae allowed to be eesble and moe

More information

Lecture 8. Light and Electromagnetic Spectrum

Lecture 8. Light and Electromagnetic Spectrum Letue 8 Optal oesses 7. henomenologal Theoy 7. Optal popetes of Cystals 7.. Maxwell s quatons 7.. Delet Funtons 7..3 Kames Kong Relatons 7.3 Optal oesses n semondutos - Det and Indet Tanstons Refeenes:

More information

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the

More information

Substances that are liquids or solids under ordinary conditions may also exist as gases. These are often referred to as vapors.

Substances that are liquids or solids under ordinary conditions may also exist as gases. These are often referred to as vapors. Chapte 0. Gases Chaacteistics of Gases All substances have thee phases: solid, liquid, and gas. Substances that ae liquids o solids unde odinay conditions may also exist as gases. These ae often efeed

More information

CENTRAL INDEX BASED SOME COMPARATIVE GROWTH ANALYSIS OF COMPOSITE ENTIRE FUNCTIONS FROM THE VIEW POINT OF L -ORDER. Tanmay Biswas

CENTRAL INDEX BASED SOME COMPARATIVE GROWTH ANALYSIS OF COMPOSITE ENTIRE FUNCTIONS FROM THE VIEW POINT OF L -ORDER. Tanmay Biswas J Koean Soc Math Educ Se B: Pue Appl Math ISSNPint 16-0657 https://doiog/107468/jksmeb01853193 ISSNOnline 87-6081 Volume 5, Numbe 3 August 018, Pages 193 01 CENTRAL INDEX BASED SOME COMPARATIVE GROWTH

More information

UNIT10 PLANE OF REGRESSION

UNIT10 PLANE OF REGRESSION UIT0 PLAE OF REGRESSIO Plane of Regesson Stuctue 0. Intoducton Ojectves 0. Yule s otaton 0. Plane of Regesson fo thee Vaales 0.4 Popetes of Resduals 0.5 Vaance of the Resduals 0.6 Summay 0.7 Solutons /

More information

Pulse Neutron Neutron (PNN) tool logging for porosity

Pulse Neutron Neutron (PNN) tool logging for porosity Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Hotwell Handelsges.m.b.H Oedenbuge Stasse 6 7013 Klingenbach, AUSTRIA Tel.: +43 (0) 687-48058 Fax: +43 (0) 687 48059 office@hotwell.at

More information

SYSTEMS OF NON-LINEAR EQUATIONS. Introduction Graphical Methods Close Methods Open Methods Polynomial Roots System of Multivariable Equations

SYSTEMS OF NON-LINEAR EQUATIONS. Introduction Graphical Methods Close Methods Open Methods Polynomial Roots System of Multivariable Equations SYSTEMS OF NON-LINEAR EQUATIONS Itoduto Gaphal Method Cloe Method Ope Method Polomal Root Stem o Multvaale Equato Chapte Stem o No-Lea Equato /. Itoduto Polem volvg o-lea equato egeeg lude optmato olvg

More information

Red Shift and Blue Shift: A realistic approach

Red Shift and Blue Shift: A realistic approach Red Shift and Blue Shift: A ealisti appoah Benhad Rothenstein Politehnia Uniesity of Timisoaa, Physis Dept., Timisoaa, Romania E-mail: benhad_othenstein@yahoo.om Coina Nafonita Politehnia Uniesity of Timisoaa,

More information

Lesson 8: Work, Energy, Power (Sections ) Chapter 6 Conservation of Energy

Lesson 8: Work, Energy, Power (Sections ) Chapter 6 Conservation of Energy Lesson 8: Wok, negy, Powe (Sectons 6.-6.8) Chapte 6 Conseaton o negy Today we begn wth a ey useul concept negy. We wll encounte many amla tems that now hae ey specc dentons n physcs. Conseaton o enegy

More information

Physical & Interfacial Electrochemistry 2013

Physical & Interfacial Electrochemistry 2013 Physcal & Intefacal Electochemsty 013 Lectue 3. Ion-on nteactons n electolyte solutons. Module JS CH3304 MoleculaThemodynamcs and Knetcs Ion-Ion Inteactons The themodynamc popetes of electolyte solutons

More information

Extra Examples for Chapter 1

Extra Examples for Chapter 1 Exta Examples fo Chapte 1 Example 1: Conenti ylinde visomete is a devie used to measue the visosity of liquids. A liquid of unknown visosity is filling the small gap between two onenti ylindes, one is

More information

( ) α is determined to be a solution of the one-dimensional minimization problem: = 2. min = 2

( ) α is determined to be a solution of the one-dimensional minimization problem: = 2. min = 2 Homewo (Patal Solton) Posted on Mach, 999 MEAM 5 Deental Eqaton Methods n Mechancs. Sole the ollowng mat eqaton A b by () Steepest Descent Method and/o Pecondtoned SD Method Snce the coecent mat A s symmetc,

More information

Energy in Closed Systems

Energy in Closed Systems Enegy n Closed Systems Anamta Palt palt.anamta@gmal.com Abstact The wtng ndcates a beakdown of the classcal laws. We consde consevaton of enegy wth a many body system n elaton to the nvese squae law and

More information

Set of square-integrable function 2 L : function space F

Set of square-integrable function 2 L : function space F Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,

More information

8 Baire Category Theorem and Uniform Boundedness

8 Baire Category Theorem and Uniform Boundedness 8 Bae Categoy Theoem and Unfom Boundedness Pncple 8.1 Bae s Categoy Theoem Valdty of many esults n analyss depends on the completeness popety. Ths popety addesses the nadequacy of the system of atonal

More information

Physics 201 Lecture 4

Physics 201 Lecture 4 Phscs 1 Lectue 4 ltoda: hapte 3 Lectue 4 v Intoduce scalas and vectos v Peom basc vecto aleba (addton and subtacton) v Inteconvet between atesan & Pola coodnates Stat n nteestn 1D moton poblem: ace 9.8

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

Tian Zheng Department of Statistics Columbia University

Tian Zheng Department of Statistics Columbia University Haplotype Tansmsson Assocaton (HTA) An "Impotance" Measue fo Selectng Genetc Makes Tan Zheng Depatment of Statstcs Columba Unvesty Ths s a jont wok wth Pofesso Shaw-Hwa Lo n the Depatment of Statstcs at

More information

P 365. r r r )...(1 365

P 365. r r r )...(1 365 SCIENCE WORLD JOURNAL VOL (NO4) 008 www.scecncewoldounal.og ISSN 597-64 SHORT COMMUNICATION ANALYSING THE APPROXIMATION MODEL TO BIRTHDAY PROBLEM *CHOJI, D.N. & DEME, A.C. Depatment of Mathematcs Unvesty

More information

Experiment 1 Electric field and electric potential

Experiment 1 Electric field and electric potential Expeiment 1 Eleti field and eleti potential Pupose Map eleti equipotential lines and eleti field lines fo two-dimensional hage onfiguations. Equipment Thee sheets of ondutive papes with ondutive-ink eletodes,

More information

2 dependence in the electrostatic force means that it is also

2 dependence in the electrostatic force means that it is also lectc Potental negy an lectc Potental A scala el, nvolvng magntues only, s oten ease to wo wth when compae to a vecto el. Fo electc els not havng to begn wth vecto ssues woul be nce. To aange ths a scala

More information

Sound Radiation of Circularly Oscillating Spherical and Cylindrical Shells. John Wang and Hongan Xu Volvo Group 4/30/2013

Sound Radiation of Circularly Oscillating Spherical and Cylindrical Shells. John Wang and Hongan Xu Volvo Group 4/30/2013 Sound Radaton of Culaly Osllatng Spheal and Cylndal Shells John Wang and Hongan Xu Volvo Goup /0/0 Abstat Closed-fom expesson fo sound adaton of ulaly osllatng spheal shells s deved. Sound adaton of ulaly

More information

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. Flux: = da i. Force: = -Â g a ik k = X i. Â J i X i (7. Themodynamcs and Knetcs of Solds 71 V. Pncples of Ievesble Themodynamcs 5. Onsage s Teatment s = S - S 0 = s( a 1, a 2,...) a n = A g - A n (7.6) Equlbum themodynamcs detemnes the paametes of an equlbum

More information

Human being is a living random number generator. Abstract: General wisdom is, mathematical operation is needed to generate number by numbers.

Human being is a living random number generator. Abstract: General wisdom is, mathematical operation is needed to generate number by numbers. Huan beng s a lvng o nube geneato Anda Mta Anushat Abasan, Utta halgun -7, /AF, alt Lae, olata, West Bengal, 764, Inda Abstat: Geneal wsdo s, atheatal oeaton s needed to geneate nube by nubes It s onted

More information

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions A Bef Gude to Recognzng and Copng Wth Falues of the Classcal Regesson Assumptons Model: Y 1 k X 1 X fxed n epeated samples IID 0, I. Specfcaton Poblems A. Unnecessay explanatoy vaables 1. OLS s no longe

More information

Review. Physics 231 fall 2007

Review. Physics 231 fall 2007 Reew Physcs 3 all 7 Man ssues Knematcs - moton wth constant acceleaton D moton, D pojectle moton, otatonal moton Dynamcs (oces) Enegy (knetc and potental) (tanslatonal o otatonal moton when detals ae not

More information

(8) Gain Stage and Simple Output Stage

(8) Gain Stage and Simple Output Stage EEEB23 Electoncs Analyss & Desgn (8) Gan Stage and Smple Output Stage Leanng Outcome Able to: Analyze an example of a gan stage and output stage of a multstage amplfe. efeence: Neamen, Chapte 11 8.0) ntoducton

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same

More information

A. Thicknesses and Densities

A. Thicknesses and Densities 10 Lab0 The Eath s Shells A. Thcknesses and Denstes Any theoy of the nteo of the Eath must be consstent wth the fact that ts aggegate densty s 5.5 g/cm (ecall we calculated ths densty last tme). In othe

More information

2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8

2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8 5 CHAPTER Fundamentals When solving equations that involve absolute values, we usually take cases. EXAMPLE An Absolute Value Equation Solve the equation 0 x 5 0 3. SOLUTION By the definition of absolute

More information

The pair-model of monopolar and dipolar moments of elemental electric scalar and magnetic vector charges

The pair-model of monopolar and dipolar moments of elemental electric scalar and magnetic vector charges The pa-model of opola dpola moments of elemental elet sala magnet veto hages Max Chwa hyss Depatment, Faulty of Sene, Engneeng Tehnology, Walte Ssulu Unvesty, Mthatha 57, Easten Cape, South Afa E-mal:

More information

Chapter 6 Balanced Incomplete Block Design (BIBD)

Chapter 6 Balanced Incomplete Block Design (BIBD) Chapte 6 Balanced Incomplete Bloc Design (BIBD) The designs lie CRD and RBD ae the complete bloc designs We now discuss the balanced incomplete bloc design (BIBD) and the patially balanced incomplete bloc

More information

Dynamics of Rigid Bodies

Dynamics of Rigid Bodies Dynamcs of Rgd Bodes A gd body s one n whch the dstances between consttuent patcles s constant thoughout the moton of the body,.e. t keeps ts shape. Thee ae two knds of gd body moton: 1. Tanslatonal Rectlnea

More information

E For K > 0. s s s s Fall Physical Chemistry (II) by M. Lim. singlet. triplet

E For K > 0. s s s s Fall Physical Chemistry (II) by M. Lim. singlet. triplet Eneges of He electonc ψ E Fo K > 0 ψ = snglet ( )( ) s s+ ss αβ E βα snglet = ε + ε + J s + Ks Etplet = ε + ε + J s Ks αα ψ tplet = ( s s ss ) ββ ( αβ + βα ) s s s s s s s s ψ G = ss( αβ βα ) E = ε + ε

More information

19 The Born-Oppenheimer Approximation

19 The Born-Oppenheimer Approximation 9 The Bon-Oppenheme Appoxmaton The full nonelatvstc Hamltonan fo a molecule s gven by (n a.u.) Ĥ = A M A A A, Z A + A + >j j (883) Lets ewte the Hamltonan to emphasze the goal as Ĥ = + A A A, >j j M A

More information

E(r,t) = e 3. r 3. (b) Show that the transverse current, J t,is 3n(n e 3 ) e 3

E(r,t) = e 3. r 3. (b) Show that the transverse current, J t,is 3n(n e 3 ) e 3 Polem Set 3 (Jakson 6.20).. An example of the pesevation of ausality and finite speed of popagation in spite of the use of the Coulomg gauge is affoded y a unit stength dipole soue that is flashed on and

More information

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems Engneeng echancs oce esultants, Toques, Scala oducts, Equvalent oce sstems Tata cgaw-hll Companes, 008 Resultant of Two oces foce: acton of one bod on anothe; chaacteed b ts pont of applcaton, magntude,

More information

On the integration of the equations of hydrodynamics

On the integration of the equations of hydrodynamics Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious

More information

Chapter 13 - Universal Gravitation

Chapter 13 - Universal Gravitation Chapte 3 - Unesal Gataton In Chapte 5 we studed Newton s thee laws of moton. In addton to these laws, Newton fomulated the law of unesal gataton. Ths law states that two masses ae attacted by a foce gen

More information

( m is the length of columns of A ) spanned by the columns of A : . Select those columns of B that contain a pivot; say those are Bi

( m is the length of columns of A ) spanned by the columns of A : . Select those columns of B that contain a pivot; say those are Bi Assgmet /MATH 47/Wte Due: Thusday Jauay The poblems to solve ae umbeed [] to [] below Fst some explaatoy otes Fdg a bass of the colum-space of a max ad povg that the colum ak (dmeso of the colum space)

More information

Generalized Vapor Pressure Prediction Consistent with Cubic Equations of State

Generalized Vapor Pressure Prediction Consistent with Cubic Equations of State Genealized Vapo Pessue Pedition Consistent with Cubi Equations of State Laua L. Petasky and Mihael J. Misovih, Hope College, Holland, MI Intodution Equations of state may be used to alulate pue omponent

More information

The Hooke-Newton transmutation system of magnetic force

The Hooke-Newton transmutation system of magnetic force Jounal of Physs Communatons PAPER OPEN ACCESS The HookeNewton tansmutaton system of magnet foe To te ths atle: DeHone Ln 08 J. Phys. Commun. 06507 Related ontent Quantum Mehans: Spheally symmet potentals

More information

Rotating Disk Electrode -a hydrodynamic method

Rotating Disk Electrode -a hydrodynamic method Rotatng Dsk Electode -a hdodnamc method Fe Lu Ma 3, 0 ente fo Electochemcal Engneeng Reseach Depatment of hemcal and Bomolecula Engneeng Rotatng Dsk Electode A otatng dsk electode RDE s a hdodnamc wokng

More information

Rigid Bodies: Equivalent Systems of Forces

Rigid Bodies: Equivalent Systems of Forces Engneeng Statcs, ENGR 2301 Chapte 3 Rgd Bodes: Equvalent Sstems of oces Intoducton Teatment of a bod as a sngle patcle s not alwas possble. In geneal, the se of the bod and the specfc ponts of applcaton

More information

Chem 453/544 Fall /08/03. Exam #1 Solutions

Chem 453/544 Fall /08/03. Exam #1 Solutions Chem 453/544 Fall 3 /8/3 Exam # Solutions. ( points) Use the genealized compessibility diagam povided on the last page to estimate ove what ange of pessues A at oom tempeatue confoms to the ideal gas law

More information

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid: hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of

More information

G = G 1 + G 2 + G 3 G 2 +G 3 G1 G2 G3. Network (a) Network (b) Network (c) Network (d)

G = G 1 + G 2 + G 3 G 2 +G 3 G1 G2 G3. Network (a) Network (b) Network (c) Network (d) Massachusetts Insttute of Technology Department of Electrcal Engneerng and Computer Scence 6.002 í Electronc Crcuts Homework 2 Soluton Handout F98023 Exercse 21: Determne the conductance of each network

More information

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables). II PARTIAL DIFFERENTIATION FUNCTIONS OF SEVERAL VARIABLES In man engineeing and othe applications, the behaviou o a cetain quantit dependent vaiable will oten depend on seveal othe quantities independent

More information

4. Some Applications of first order linear differential

4. Some Applications of first order linear differential August 30, 2011 4-1 4. Some Applications of fist ode linea diffeential Equations The modeling poblem Thee ae seveal steps equied fo modeling scientific phenomena 1. Data collection (expeimentation) Given

More information

Chapter 23: Electric Potential

Chapter 23: Electric Potential Chapte 23: Electc Potental Electc Potental Enegy It tuns out (won t show ths) that the tostatc foce, qq 1 2 F ˆ = k, s consevatve. 2 Recall, fo any consevatve foce, t s always possble to wte the wok done

More information

Electric Field, Potential Energy, & Voltage

Electric Field, Potential Energy, & Voltage Slide 1 / 66 lectic Field, Potential negy, & oltage Wok Slide 2 / 66 Q+ Q+ The foce changes as chages move towads each othe since the foce depends on the distance between the chages. s these two chages

More information

Lecture 28: Convergence of Random Variables and Related Theorems

Lecture 28: Convergence of Random Variables and Related Theorems EE50: Pobability Foundations fo Electical Enginees July-Novembe 205 Lectue 28: Convegence of Random Vaiables and Related Theoems Lectue:. Kishna Jagannathan Scibe: Gopal, Sudhasan, Ajay, Swamy, Kolla An

More information

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints. Mathematcal Foundatons -1- Constaned Optmzaton Constaned Optmzaton Ma{ f ( ) X} whee X {, h ( ), 1,, m} Necessay condtons fo to be a soluton to ths mamzaton poblem Mathematcally, f ag Ma{ f ( ) X}, then

More information

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation:

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation: HPT 3 xercses 3. The emtter current s gen by the Shockley equaton: S exp VT For operaton wth, we hae exp >> S >>, and we can wrte VT S exp VT Solng for, we hae 3. 0 6ln 78.4 mv 0 0.784 5 4.86 V VT ln 4

More information

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M Dola Bagayoko (0) Integal Vecto Opeatons and elated Theoems Applcatons n Mechancs and E&M Ι Basc Defnton Please efe to you calculus evewed below. Ι, ΙΙ, andιιι notes and textbooks fo detals on the concepts

More information

= e2. = 2e2. = 3e2. V = Ze2. where Z is the atomic numnber. Thus, we take as the Hamiltonian for a hydrogenic. H = p2 r. (19.4)

= e2. = 2e2. = 3e2. V = Ze2. where Z is the atomic numnber. Thus, we take as the Hamiltonian for a hydrogenic. H = p2 r. (19.4) Chapte 9 Hydogen Atom I What is H int? That depends on the physical system and the accuacy with which it is descibed. A natual stating point is the fom H int = p + V, (9.) µ which descibes a two-paticle

More information

QUANTILE ESTIMATION: A MINIMALIST APPROACH

QUANTILE ESTIMATION: A MINIMALIST APPROACH Poeedngs o the 2006 Wnte Smulaton Coneene L. F. Peone F. P. Weland J. Lu B. G. Lawson D.. Nol and R.. Fujmoto eds QUANTILE ESTIATION: A INIALIST APPROACH Yuy Baksh AT&T Laboatoes 200 S Lauel Ave ddletown

More information

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering Themodynamcs of solds 4. Statstcal themodynamcs and the 3 d law Kwangheon Pak Kyung Hee Unvesty Depatment of Nuclea Engneeng 4.1. Intoducton to statstcal themodynamcs Classcal themodynamcs Statstcal themodynamcs

More information

Confidence Intervals for the Squared Multiple Semipartial Correlation Coefficient. James Algina. University of Florida. H. J.

Confidence Intervals for the Squared Multiple Semipartial Correlation Coefficient. James Algina. University of Florida. H. J. Eet Size Conidene Inteval 1 Conidene Intevals o the Squaed Multiple Semipatial Coelation Coeiient by James Algina Univesity o Floida H. J. Keselman Univesity o Manitoba all D. Penield Univesity o Miami

More information

24-2: Electric Potential Energy. 24-1: What is physics

24-2: Electric Potential Energy. 24-1: What is physics D. Iyad SAADEDDIN Chapte 4: Electc Potental Electc potental Enegy and Electc potental Calculatng the E-potental fom E-feld fo dffeent chage dstbutons Calculatng the E-feld fom E-potental Potental of a

More information

Introduction to Algorithms 6.046J/18.401J

Introduction to Algorithms 6.046J/18.401J 3/4/28 Intoduton to Algothms 6.46J/8.4J Letue 8 - Hashng Pof. Manols Kells Hashng letue outlne Into and defnton Hashng n pate Unvesal hashng Pefet hashng Open Addessng (optonal) 3/4/28 L8.2 Data Stutues

More information

33. 12, or its reciprocal. or its negative.

33. 12, or its reciprocal. or its negative. Page 6 The Point is Measuement In spite of most of what has been said up to this point, we did not undetake this poject with the intent of building bette themometes. The point is to measue the peson. Because

More information

MATHEMATICS II PUC VECTOR ALGEBRA QUESTIONS & ANSWER

MATHEMATICS II PUC VECTOR ALGEBRA QUESTIONS & ANSWER MATHEMATICS II PUC VECTOR ALGEBRA QUESTIONS & ANSWER I One M Queston Fnd the unt veto n the deton of Let ˆ ˆ 9 Let & If Ae the vetos & equl? But vetos e not equl sne the oespondng omponents e dstnt e detons

More information

Unit_III Complex Numbers: Some Basic Results: 1. If z = x +iy is a complex number, then the complex number z = x iy is

Unit_III Complex Numbers: Some Basic Results: 1. If z = x +iy is a complex number, then the complex number z = x iy is Unt_III Comple Nmbes: In the sstem o eal nmbes R we can sole all qadatc eqatons o the om a b c, a, and the dscmnant b 4ac. When the dscmnant b 4ac

More information

Linear Algebra Math 221

Linear Algebra Math 221 Linea Algeba Math Open Book Eam Open Notes Sept Calculatos Pemitted Sho all ok (ecept #). ( pts) Gien the sstem of equations a) ( pts) Epess this sstem as an augmented mati. b) ( pts) Bing this mati to

More information

PHYS Week 5. Reading Journals today from tables. WebAssign due Wed nite

PHYS Week 5. Reading Journals today from tables. WebAssign due Wed nite PHYS 015 -- Week 5 Readng Jounals today fom tables WebAssgn due Wed nte Fo exclusve use n PHYS 015. Not fo e-dstbuton. Some mateals Copyght Unvesty of Coloado, Cengage,, Peason J. Maps. Fundamental Tools

More information

Contact, information, consultations

Contact, information, consultations ontact, nfomaton, consultatons hemsty A Bldg; oom 07 phone: 058-347-769 cellula: 664 66 97 E-mal: wojtek_c@pg.gda.pl Offce hous: Fday, 9-0 a.m. A quote of the week (o camel of the week): hee s no expedence

More information

Physics 218, Spring March 2004

Physics 218, Spring March 2004 Today in Physis 8: eleti dipole adiation II The fa field Veto potential fo an osillating eleti dipole Radiated fields and intensity fo an osillating eleti dipole Total satteing oss setion of a dieleti

More information

Correspondence Analysis & Related Methods

Correspondence Analysis & Related Methods Coespondene Analysis & Related Methods Oveview of CA and basi geometi onepts espondents, all eades of a etain newspape, osstabulated aoding to thei eduation goup and level of eading of the newspape Mihael

More information

The second law of thermodynamics - II.

The second law of thermodynamics - II. Januay 21, 2013 The second law of themodynamics - II. Asaf Pe e 1 1. The Schottky defect At absolute zeo tempeatue, the atoms of a solid ae odeed completely egulaly on a cystal lattice. As the tempeatue

More information

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system

More information

Viscoelectroelastic behavior of heterogeneous piezoelectric solids

Viscoelectroelastic behavior of heterogeneous piezoelectric solids JOURNAL OF APPLIED PHYSICS VOLUME 89 NUMBER 5 1 MARCH 2001 Vsoeletoelast behavo of heteogeneous pezoelet solds JangYu L a) Dvson of Engneeng and Appled Sene Calfona Insttute of Tehnology Pasadena Calfona

More information

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1 Rotatonal Knematcs Rgd Object about a Fxed Axs Westen HS AP Physcs 1 Leanng Objectes What we know Unfom Ccula Moton q s Centpetal Acceleaton : Centpetal Foce: Non-unfom a F c c m F F F t m ma t What we

More information

If there are multiple rxns, use concentrations not conversions. These might occur in combination or by themselves.

If there are multiple rxns, use concentrations not conversions. These might occur in combination or by themselves. hapte 6 MLTIPLE RETIONS If thee ae multiple xns, use concentations not convesions. intemediate. Seies Reactions onsecutive xns. Paallel Reactions. omplex Reactions: Seies and Paallel 4. Independent None

More information

On Generalized Fractional Hankel Transform

On Generalized Fractional Hankel Transform Int. ournal o Math. nalss Vol. 6 no. 8 883-896 On Generaled Fratonal ankel Transorm R. D. Tawade Pro.Ram Meghe Insttute o Tehnolog & Researh Badnera Inda rajendratawade@redmal.om. S. Gudadhe Dept.o Mathemats

More information

From E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018

From E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018 Fom E.G. Haug Esape eloity To the Golden Ratio at the Blak Hole Banko Zivlak, bzivlak@gmail.om Novi Sad, May 018 Abstat Esape veloity fom the E.G. Haug has been heked. It is ompaed with obital veloity

More information

Large scale magnetic field generation by accelerated particles in galactic medium

Large scale magnetic field generation by accelerated particles in galactic medium Lage scale magnetc feld geneaton by acceleated patcles n galactc medum I.N.Toptygn Sant Petesbug State Polytechncal Unvesty, depatment of Theoetcal Physcs, Sant Petesbug, Russa 2.Reason explonatons The

More information

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

More information

Khintchine-Type Inequalities and Their Applications in Optimization

Khintchine-Type Inequalities and Their Applications in Optimization Khntchne-Type Inequaltes and The Applcatons n Optmzaton Anthony Man-Cho So Depatment of Systems Engneeng & Engneeng Management The Chnese Unvesty of Hong Kong ISDS-Kolloquum Unvestaet Wen 29 June 2009

More information

Physics Exam II Chapters 25-29

Physics Exam II Chapters 25-29 Physcs 114 1 Exam II Chaptes 5-9 Answe 8 of the followng 9 questons o poblems. Each one s weghted equally. Clealy mak on you blue book whch numbe you do not want gaded. If you ae not sue whch one you do

More information

Analytical solutions to the Navier Stokes equations

Analytical solutions to the Navier Stokes equations JOURAL OF MATHEMATICAL PHYSICS 49, 113102 2008 Analytical solutions to the avie Stokes equations Yuen Manwai a Depatment of Applied Mathematics, The Hong Kong Polytechnic Univesity, Hung Hom, Kowloon,

More information

HRW 7e Chapter 13 Page 1 of 5

HRW 7e Chapter 13 Page 1 of 5 HW 7e Chapte Pae o 5 Halliday/enick/Walke 7e Chapte Gaitation The manitude o the oce o one paticle on the othe i ien by F = Gm m /, whee m and m ae the mae, i thei epaation, and G i the unieal aitational

More information

Suppose the medium is not homogeneous (gravity waves impinging on a beach,

Suppose the medium is not homogeneous (gravity waves impinging on a beach, Slowly vaying media: Ray theoy Suppose the medium is not homogeneous (gavity waves impinging on a beach, i.e. a vaying depth). Then a pue plane wave whose popeties ae constant in space and time is not

More information

Chapter 3: Vectors and Two-Dimensional Motion

Chapter 3: Vectors and Two-Dimensional Motion Chape 3: Vecos and Two-Dmensonal Moon Vecos: magnude and decon Negae o a eco: eese s decon Mulplng o ddng a eco b a scala Vecos n he same decon (eaed lke numbes) Geneal Veco Addon: Tangle mehod o addon

More information

15 Solving the Laplace equation by Fourier method

15 Solving the Laplace equation by Fourier method 5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the

More information

Evaluation of Various Types of Wall Boundary Conditions for the Boltzmann Equation

Evaluation of Various Types of Wall Boundary Conditions for the Boltzmann Equation Ealuaton o Vaous Types o Wall Bounday Condtons o the Boltzmann Equaton Chstophe D. Wlson a, Ramesh K. Agawal a, and Felx G. Tcheemssne b a Depatment o Mechancal Engneeng and Mateals Scence Washngton Unesty

More information

III. Electromechanical Energy Conversion

III. Electromechanical Energy Conversion . Electoancal Enegy Coneson Schematc epesentaton o an toancal enegy coneson ece coppe losses coe losses (el losses) ancal losses Deental enegy nput om tcal souce: W V t Rt e t t W net ancal enegy output

More information

C/CS/Phys C191 Shor s order (period) finding algorithm and factoring 11/12/14 Fall 2014 Lecture 22

C/CS/Phys C191 Shor s order (period) finding algorithm and factoring 11/12/14 Fall 2014 Lecture 22 C/CS/Phys C9 Sho s ode (peiod) finding algoithm and factoing /2/4 Fall 204 Lectue 22 With a fast algoithm fo the uantum Fouie Tansfom in hand, it is clea that many useful applications should be possible.

More information

On a quantity that is analogous to potential and a theorem that relates to it

On a quantity that is analogous to potential and a theorem that relates to it Su une quantité analogue au potential et su un théoème y elatif C R Acad Sci 7 (87) 34-39 On a quantity that is analogous to potential and a theoem that elates to it By R CLAUSIUS Tanslated by D H Delphenich

More information

Physics 231 Ch 9 Day

Physics 231 Ch 9 Day Physs Ch 9 Day 0 0 Wed., /6 ab F, /8 n., / Tues. / 9. Rtatnal Enegy Quz 8 8 Enegy Quantzatn Reew Exam (Ch 5-8) Exam (Ch 5-8) RE 9.b bng laptp, smatphne, pad, Pate Exam (due begnnng lass) 9.-.5 (.9) The

More information

1 Similarity Analysis

1 Similarity Analysis ME43A/538A/538B Axisymmetic Tubulent Jet 9 Novembe 28 Similaity Analysis. Intoduction Conside the sketch of an axisymmetic, tubulent jet in Figue. Assume that measuements of the downsteam aveage axial

More information