Phase Velocities of Three-Dimensional and Axis-Symmetrical Elastic Waves in Isotropic Cylindrical Shell

Size: px
Start display at page:

Download "Phase Velocities of Three-Dimensional and Axis-Symmetrical Elastic Waves in Isotropic Cylindrical Shell"

Transcription

1 Intentionl ounl of Teoeticl nd Mteticl Pysics, (6): 96- DOI:.593/j.ijtp.6.4 Pse Velocities of Tee-Diensionl nd Axis-Syeticl Elstic Wves in Isotopic Cylindicl Sell S. L. Ile nov *, A. A. Klescev Sint-Petesug Stte vy Tecnicl nivesity, Sint-Petesug, Lotsnsy st., 3, 98, Russi Astct Bsed on use of Deye s potentils one cn find te diect solution of te pole of definition of te ccteistic equtions fo wve nues of tee-diensionl nd xis-syeticl (flexul nd longitudinl) elstic wves in steel nd luiniu cylindicl sells of vious ticness. Keywods Pse Velocity, Deye s Potentil, Flexul Wve, Longitudinl Wve, Tee-Diensionl Pole, Axis-Sy et icl Pole. Intoduction Te Deye s potentils e used fo te fist tie fo study of te tee-diensionl flexul wves. Te ppe sows te existing of te tee-diensionl nd xis-syet icl flexul wves in cylindicl sell (conty to te cylindicl ). Te ppe deonsttes te clculted vlues of te pse velocities of xis-syeticl nd tee-diensionl flexul wves, wile te pse velocities of te non-eo fos of tee syeticl flexul wves e clculted fo te fist tie. Figue. Te defotion of cylindicl sell fo flexul () nd longitudinl () xis- syeticl wves * Coesponding uto: ils@le.u (S. L. Ilenov) Pulised online t ttp://jounl.spu.og/ijtp Copyigt Scientific & Acdeic Pulising. All Rigts Reseved. Te Tee-Diensionl Flexul Wves in Cylindicl Sell Te fist pt of te ticle sustntites te effectiveness of usge of Deye s potentils[ 3] fo studying of tee-diensionl flexul wves in cylindicl sell. In contst to te te flexul wve in cylindicl sell cn e tee-diensionl nd two-diensionl(xis-sye ticl). Te defotion of cylindicl sell in te popgtion of xis-syeticl flexul (а) nd longitudinl () wves in it is sceticlly sown in fig.. Let s stt wit exintion of tee-diensionl fle xu l wve in isotopic cylindicl sell. In tis cse te se teticl pptus is used s in te study of flexu l wves in [4], ut te nue of unnown quntities nd te nue of oundy conditions incese wit te ccount of te second (intenl) oundy sufce. ow te expnsions of te potentils Ф, V, [5 5] te te fo: i Φ e cos φ A ( ) B( ) i V e cos φ C( ) D( ) () i e sin φ E( ) F( ), wee ( ) ( ) ( ) - e te n s cylindicl function A, B, C, D, E, F - e te unnown coefficients of expnding, wic e clculted sing on te following pysicl

2 97 Intentionl ounl of Teoeticl nd Mteticl Pysics, (6): 96- oundy conditions on te extenl ( ) nd inside ( ) sufces of te sell: tee e no nol nd tngent tensions on te ot oundies of te sell. We desie te nlyticl fo of oundy conditions s following: ( ) (), (3), (4) If we sustitute () in te oundy conditions () - (4), we ll get te deteinnt of six ode[5 5]:, (5) wee [ [ [ ] { [ ]} ( )( ) { ( )( ) } 3 [ ] { [ ]} { ( ) } 4 ( ) 5 ( ) 6 [ [

3 S. L. Ilenov et l.: Pse Velocities of Tee-Diensionl nd Axis-Syeticl 98 Elstic Wves in Isotopic Cylindicl Sell 3 ( ){ [ ( ) ( ) ] ( ) [ ( ) ( ) ]} { ( )( ) ( )( ) ( ) ( )} 4 ( ){ [ ( ) ( ) ] ( ) [ ( ) ( ) ]} { ( )( ) ( ) ( ) ( ) ( )} 5 ( )( ) ( ) 6 ( )( ) ( ) 3 [ ( ) ( ) 3 [ ( ) ( ) 33 { ( ) [ ( ) ] ( ) ( )} 34 { ( ) [ ( ) ] ( ) ( )} 35 ( ) 36 ( ) 4 [ ( ) ( ) 4 [ ( ) ( ) 43 { ( ) [ ( ) ] ( ) ( )} 44 { ( ) [ ( ) ] ( ) ( )} 45 ( ) 46 ( ) 5 i ( ) 5 i ( ) 53 { ( )( ) 5 ( ) ( )} 54 { ( )( ) 5 ( ) ( )} 55 [ ( ) ( ) 56 [ ( ) ( ) 6 i ( ) 6 i ( ) 63 { ( )( ) 5 ( ) ( )} 64 { ( )( ) 5 ( ) ( )} 65 [ ( ) ( ) [ ( ) ( ) 66 Equting te deteinnt (5) eo nd opening i, we eceive te ccteistic eqution fo wve nues of fo of tee-diensionl flexu l wves in isotopic cylindicl sell of ny (ut constnt) ticness. Te decision of te ccteistic eqution fo steel nd lu in iu sells of vious ticness is suitted in fig. nd 3, tus extenl dius ws ccepted equl,, nd dius ccepted two enings:,99 (continuous cuve) nd,8 (dotted cuve). Te enings of velocities longitudinl (С ), ltel (С ) nd Rely s wve (С R ) e sown on te digs. Te ening coesponds to eo fo of flexul wve,

4 99 Intentionl ounl of Teoeticl nd Mteticl Pysics, (6): 96- wic velocity spies siptoticly to velocity of Rely s wve С R, Λ - lengt of longitudinl wve in te sell s teil Λ c f, wee f - fequency of wve in H. In fig. te pse velocities of tee-diensionl flexul wves in steel sells, in fig. 3 - in lu in iu sells e sown. 6 C,/s ,99,8 C C C R /Λ Figue. Pse velocities of tee-diensionl flexul wves in steel sells 7 C,/s ,99,8 C C C R /Λ Figue 3. Pse velocities of tee-diensionl flexul wves in luinu sells Let s tun to xis-syeticl longitudinl nd fle xu l wves. In ccodnce wit[5 5] in xis-syeticl cse te oundy conditions () - (4) ecoe siple: te condition (3) disppes nd te condition () tes te following fo (in tis cse te index o ): ( ) (6), Te deteinnt of te fout ode deived fo oundy conditions tes te fo[5]* : wee (7) ( ) ( ) [ ( ) ( ) ( ) ( ) [ ( ) ( ) 3 i ( ) 4 i ( ) ( ) ( ) [ ( ) ( ) ( ) ( ) [ ( ) ( ) 3 i ( ) 4 i ( ) i ( ) * In te pesent wo te deivtives of cylindicl functions t dil coodinte e ed te following wy: ( ) ( ) ( ) ( ) in te wo[5] diffeently: ( ) ( ) ( ) ( ) ( ) ( ). Bot ppoces e copetent. ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 4 i ( ) 4 i ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) Equting te deteinnt (7) eo nd opening it, we get te ccteistic eqution fo wve nues of flexul nd longitudinl xis-syeticl wves. Te deteinnt fo xis-syeticl tosion wves e epesented in[5]: ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ), (8)

5 S. L. Ilenov et l.: Pse Velocities of Tee-Diensionl nd Axis-Syeticl Elstic Wves in Isotopic Cylindicl Sell wee ( ), - is te desied wve nue of xis-syeticl tosion wve in te sell. Equting te deteinnt (8) eo nd opening it, we get te ccteistic eqution fo wve nues of xis-syeticl tosion wves. 3. Te Results of ueicl Expeient fo Deteintion of Pse Velocities of Elstic Wves Te second pt of te ticle investigtes te esults of nueicl expeient fo deteintion of pse velocities of elstic wves (xis-syeticl nd tee-diensionl) in cylindicl sell nd nlyses te clculted dependences. Te esults of clcultions of pse velocities e epesented in te fig.4. 6 C,/s C C C R /Λ Figue 4. Pse velocities of xis-syeticl flexul, longitudinl nd tosion wves in steel cylindicl sell One cn find te following designtions in te pictue: te cuve - is te pse velocity of eo ode of fle xu l wve te cuve - is te pse velocity of eo ode of longitudinl wve te cuves 3, 4, 5 - e te pse velocities of noneo odes of longitudinl o of flexul wves te stigt line 6 - is te pse velocity of eo ode of tosion wve te cuve 7 - is te pse velocity of te fist ode of tosion wve: Λ c f. In ode to define te influence of extenl nd intenl liquid ediu s on dispesion cuves of pse velocities of sell to te deteinnt of te sixt ode (5) e dded two coluns nd two lines nd it convets into te deteinnt of te eigt ode, nd deteinnt of te fout ode into te deteinnt of te sixt ode. Te potentils of sound wves (in extenl envionent) nd in te filling of te sell expnd y te cylindicl functions te following wy: ( ) Φ G H ( γ ) cos e i Φ K ( γ ) cos e, wee: ( ω c3 ) γ ( ω c4 ) 3 () γ c nd c4 - sound velocities in extenl nd intenl envionents coespondingly. Te coponent of wve vecto lengtwise of xis, s in te sell in te foce of Snellius lw. In tis cse te oundy conditions () fo nol tensions on te ot sufces of te sell tnsfos: (9) ( )( ) ( ) i, wee: ρ - te solidity of te extenl envionent. () ( )( ) ( ) i, () wee: ρ - te solidity of te intenl envionent. Two oe oundy conditions e dded: te nol coponents of displceent vecto e continuous in te ot odes of te sell: Φ A A Φ (3)

6 Intentionl ounl of Teoeticl nd Mteticl Pysics, (6): 96- Φ A A In xis-syeticl cse te condition (6) tnsfos: Φ ( ) i ( ) i (5) (6) (4) Te dded oundy conditions in xis-syeticl cse: Φ A Φ Φ A In xis-syeticl cse: Φ (7) (8) ( ) Φ G H ( γ ) e (9) Φ K ( ) e. () γ Te oundy conditions (), () nd (7), (8) will dd two lines to deteinnt, nd te u ltip lies of unnown coefficients G, K o G, K (xis-syeticl pole) will dd two coluns. In tis cse only two lines in ec of tese two coluns will e diffeent fo eo. If te sell odes te liquid only fo one side (nd fo te ote is still te vcuu) te deteinnt fo deteintion of wve nues will ve te sevent ode in tee-diensionl pole nd te fift ode (in xis-syeticl cse), tt is to deteinnts (5) и (7) one line nd one colun e dded coespondingly. Te esults pesented in te ticle e eceived in te conducting of scientific esec in te fewo of Stte contct P 4 fo 3 Apil FPP (Scientific nd scientific - pedgogicl pesonnel of innovtive Russi fo te yes 9-3). 4. Conclusions Bsed on use of Deye s potentils one cn find te diect solution of te pole of definition of te ccteistic eqution fo pse velocities of tee diensionl flexul wves. Te nueicl solution of tis eqution destintes to otin te dispesive cuves of pse velocities. Te dispesive dependencies of pse velocities of xis syeticl flexul, longitudinl nd tosion wves e epesented. REFERECES [] Deye P. Ann. Pys. 3, 755 (99). [] Foc V. A. Eletognetic Diffction nd Popgtion Poles (Sov. Rdio, Moscow, 97 Pegon Oxfod, 965). [3] Klescev A. A. Te Deye s potentils nd «te potentils of Deye s type» in te poles of diffction, dition nd speding of elstic wves.// Acousticl jounl.. V , P [4] Klescev A. A., Kluin I.I. Aout of te flexul wves in elstic cylindicl. // Poceedings of Sint-Petesug Stte vy Tecnicl nivesity. v P [5] Ilenov S. L., Klescev A. A. Pse velocities of flexul wves in isotopic cylindicl sell of ny ticness (stict decision) // Poceedings of te X Session of te Russin Acousticl Society. -, v., Moscow. GEOS. P [6] Klescev A. A. Diffction nd popgtion of wves in te elstic edius nd odies.// Sint-Petesug: Vls,. P. 56. [7] Klescev A. A. Te dispesive equtions of displceent vectos of diffeent odes of elstic wves in isotopic nd nisotopic cylindicl sells. // Poceedings of te XIII Session of te Russin Acousticl Society.- 3. М.: GEOS. P [8] Klescev A. A. Te sound diffction fo point sound souce in elstic cylindicl sells.// Acousticl jounl.. 4. V. 5.. P [9] Ilenov S. L., Klescev A. A. Sugilo K.A. Te pse velocities of elstic wves in s nd sells.// // Poceedings of te Regionl scientific confeence «Te sipuilding eduction nd science» 3». Pul.ouse of te Sint-Petesug Stte vy Tecnicl nivesity, 3. V.. P [] Ilenov S. L., Klescev A. A. Pysicl odel of sound dition unde ction of te tuulent pulstions. // Poceedings of te Scientific confeence «Bunov s lectues». Pul. ouse of te Kylov sipuilding esec institute. Sint-Petesug. 4. P. 3. [] Klescev A. A. Diffction, dition nd popgtion of elstic wves.// Sint-Petesug.:Pofpint, 6. P.6. [] Klescev A. A. Expeientl sctteing ccteistics of low fequency non-fixed sound signl fo elstic cylindicl sells in Fenel s one. // Poceedings of te XXI

7 S. L. Ilenov et l.: Pse Velocities of Tee-Diensionl nd Axis-Syeticl Elstic Wves in Isotopic Cylindicl Sell Session of te Russin Acousticl Society.-9. М.: GEOS.. P [3] Klescev A. A., Legus F.F., Mslov V. L. Wve pocess in te solids.//sint-petesug. Pul. ouse of te Sint-Petesug Stte vy Tecnicl nivesity,. P.6. [4] Klescev A. A. Sctteing of Low Fequency Pulsed Sound Signls fo Elstic Cylindicl Sells. // Acousticl Pysics.. V P [5] Klescev A. A. Acoustic Scttees.//Te second puliction. Sint-Petesug. Pi,. P. 67.

Available online at ScienceDirect. Procedia Engineering 91 (2014 ) 32 36

Available online at   ScienceDirect. Procedia Engineering 91 (2014 ) 32 36 Aville online t wwwsciencediectcom ScienceDiect Pocedi Engineeing 91 (014 ) 3 36 XXIII R-S-P semin Theoeticl Foundtion of Civil Engineeing (3RSP) (TFoCE 014) Stess Stte of Rdil Inhomogeneous Semi Sphee

More information

Discrete Model Parametrization

Discrete Model Parametrization Poceedings of Intentionl cientific Confeence of FME ession 4: Automtion Contol nd Applied Infomtics Ppe 9 Discete Model Pmetition NOKIEVIČ, Pet Doc,Ing,Cc Deptment of Contol ystems nd Instumenttion, Fculty

More information

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm 3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess 3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess Motition Gien elocit field o ppoimted elocit field, we wnt to be ble to estimte

More information

Fourier-Bessel Expansions with Arbitrary Radial Boundaries

Fourier-Bessel Expansions with Arbitrary Radial Boundaries Applied Mthemtics,,, - doi:./m.. Pulished Online My (http://www.scirp.og/jounl/m) Astct Fouie-Bessel Expnsions with Aity Rdil Boundies Muhmmd A. Mushef P. O. Box, Jeddh, Sudi Ai E-mil: mmushef@yhoo.co.uk

More information

GEOMETRY Properties of lines

GEOMETRY Properties of lines www.sscexmtuto.com GEOMETRY Popeties of lines Intesecting Lines nd ngles If two lines intesect t point, ten opposite ngles e clled veticl ngles nd tey ve te sme mesue. Pependicul Lines n ngle tt mesues

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt

More information

4.2 Boussinesq s Theory. Contents

4.2 Boussinesq s Theory. Contents 00477 Pvement Stuctue 4. Stesses in Flexible vement Contents 4. Intoductions to concet of stess nd stin in continuum mechnics 4. Boussinesq s Theoy 4. Bumiste s Theoy 4.4 Thee Lye System Weekset Sung Chte

More information

A 2 ab bc ca. Surface areas of basic solids Cube of side a. Sphere of radius r. Cuboid. Torus, with a circular cross section of radius r

A 2 ab bc ca. Surface areas of basic solids Cube of side a. Sphere of radius r. Cuboid. Torus, with a circular cross section of radius r Sufce e f ic lid Cue f ide R See f diu 6 Cuid c c Elliticl cectin c Cylinde, wit diu nd eigt Tu, wit cicul c ectin f diu R R Futum, ( tuncted ymid) f e eimete, t e eimete nd lnt eigt. nd e te eective e

More information

Effect of Heat Generation on Quasi- Static Thermal Stresses in a Solid Sphere

Effect of Heat Generation on Quasi- Static Thermal Stresses in a Solid Sphere IOS Jounl of Mthetics (IOS-JM) e-issn: 78-578,p-ISSN: 39-765X, Volue 7, Issue 5 (Jul. - Aug. 3), PP -9 www.iosjounls.og Effect of Het Genetion on Qusi- Sttic Thel Stesses in Solid Sphee S.P. Pw, K.C. Deshukh,

More information

On the Eötvös effect

On the Eötvös effect On the Eötvös effect Mugu B. Răuţ The im of this ppe is to popose new theoy bout the Eötvös effect. We develop mthemticl model which loud us bette undestnding of this effect. Fom the eqution of motion

More information

10.3 The Quadratic Formula

10.3 The Quadratic Formula . Te Qudti Fomul We mentioned in te lst setion tt ompleting te sque n e used to solve ny qudti eqution. So we n use it to solve 0. We poeed s follows 0 0 Te lst line of tis we ll te qudti fomul. Te Qudti

More information

Electric Potential. and Equipotentials

Electric Potential. and Equipotentials Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil

More information

Supplementary material for " Coherent and Tunable Terahertz Radiation from Graphene Surface Plasmon Polarirons Excited by Cyclotron Electron Beam "

Supplementary material for  Coherent and Tunable Terahertz Radiation from Graphene Surface Plasmon Polarirons Excited by Cyclotron Electron Beam Suppleenty teil fo " Coheent nd Tunble Tehet Rdition fo Gphene Sufce Plson Polions Excited by Cycloton Electon Be " To Zho,, Sen Gong,, Min Hu,, Renbin Zhong,,Diwei Liu,,Xioxing Chen,, Ping hng,, Xinn

More information

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 9. CHEM 793, 2008 Fall

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 9. CHEM 793, 2008 Fall Cpte 3 Bsic Cystopy nd Eecton Diffction fom Cysts Lectue 9 Top of tin foi Cyst pne () Bottom of tin foi B Lw d sinθ n Equtions connectin te Cyst metes (,, ) nd d-spcin wit bem pmetes () ( ) ne B Lw d (nm)

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 20

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 20 .615, MHD Theoy of Fusion Systes Pof. Feideg Lectue Resistive Wll Mode 1. We hve seen tht pefectly conducting wll, plced in close poxiity to the pls cn hve stong stilizing effect on extenl kink odes..

More information

Physics 505 Fall 2005 Midterm Solutions. This midterm is a two hour open book, open notes exam. Do all three problems.

Physics 505 Fall 2005 Midterm Solutions. This midterm is a two hour open book, open notes exam. Do all three problems. Physics 55 Fll 5 Midtem Solutions This midtem is two hou open ook, open notes exm. Do ll thee polems. [35 pts] 1. A ectngul ox hs sides of lengths, nd c z x c [1] ) Fo the Diichlet polem in the inteio

More information

Picking Coordinate Axes

Picking Coordinate Axes Picing Coodinte Axes If the object you e inteested in Is cceleting Choose one xis long the cceletion Su of Foce coponents long tht xis equls Su of Foce coponents long ny othe xis equls 0 Clcultions e esie

More information

Chapter 6 Thermoelasticity

Chapter 6 Thermoelasticity Chpte 6 Themoelsticity Intoduction When theml enegy is dded to n elstic mteil it expnds. Fo the simple unidimensionl cse of b of length L, initilly t unifom tempetue T 0 which is then heted to nonunifom

More information

Physics 1502: Lecture 2 Today s Agenda

Physics 1502: Lecture 2 Today s Agenda 1 Lectue 1 Phsics 1502: Lectue 2 Tod s Agend Announcements: Lectues posted on: www.phs.uconn.edu/~cote/ HW ssignments, solutions etc. Homewok #1: On Mstephsics this Fid Homewoks posted on Msteingphsics

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 4 Due on Sep. 1, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt

More information

Radial geodesics in Schwarzschild spacetime

Radial geodesics in Schwarzschild spacetime Rdil geodesics in Schwzschild spcetime Spheiclly symmetic solutions to the Einstein eqution tke the fom ds dt d dθ sin θdϕ whee is constnt. We lso hve the connection components, which now tke the fom using

More information

FI 2201 Electromagnetism

FI 2201 Electromagnetism FI 1 Electomgnetism Alexnde A. Isknd, Ph.D. Physics of Mgnetism nd Photonics Resech Goup Electosttics ELECTRIC PTENTIALS 1 Recll tht we e inteested to clculte the electic field of some chge distiution.

More information

PLEASE DO NOT TURN THIS PAGE UNTIL INSTRUCTED TO DO SO THEN ENSURE THAT YOU HAVE THE CORRECT EXAM PAPER

PLEASE DO NOT TURN THIS PAGE UNTIL INSTRUCTED TO DO SO THEN ENSURE THAT YOU HAVE THE CORRECT EXAM PAPER OLLSCOIL NA ÉIREANN, CORCAIGH THE NATIONAL UNIVERSITY OF IRELAND, CORK COLÁISTE NA OLLSCOILE, CORCAIGH UNIVERSITY COLLEGE, CORK 4/5 Autumn Suppement 5 MS Integ Ccuus nd Diffeenti Equtions Pof. P.J. Rippon

More information

Forging Analysis - 2. ver. 1. Prof. Ramesh Singh, Notes by Dr. Singh/ Dr. Colton

Forging Analysis - 2. ver. 1. Prof. Ramesh Singh, Notes by Dr. Singh/ Dr. Colton Foging Analysis - ve. 1 Pof. ames Sing, Notes by D. Sing/ D. Colton 1 Slab analysis fictionless wit fiction ectangula Cylindical Oveview Stain adening and ate effects Flas edundant wo Pof. ames Sing, Notes

More information

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is: . Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo

More information

Physics Courseware Electromagnetism

Physics Courseware Electromagnetism Pysics Cousewae lectomagnetism lectic field Poblem.- a) Find te electic field at point P poduced by te wie sown in te figue. Conside tat te wie as a unifom linea cage distibution of λ.5µ C / m b) Find

More information

Optimization. x = 22 corresponds to local maximum by second derivative test

Optimization. x = 22 corresponds to local maximum by second derivative test Optimiztion Lectue 17 discussed the exteme vlues of functions. This lectue will pply the lesson fom Lectue 17 to wod poblems. In this section, it is impotnt to emembe we e in Clculus I nd e deling one-vible

More information

MATHEMATICS IV 2 MARKS. 5 2 = e 3, 4

MATHEMATICS IV 2 MARKS. 5 2 = e 3, 4 MATHEMATICS IV MARKS. If + + 6 + c epesents cicle with dius 6, find the vlue of c. R 9 f c ; g, f 6 9 c 6 c c. Find the eccenticit of the hpeol Eqution of the hpeol Hee, nd + e + e 5 e 5 e. Find the distnce

More information

Lecture 11: Potential Gradient and Capacitor Review:

Lecture 11: Potential Gradient and Capacitor Review: Lectue 11: Potentil Gdient nd Cpcito Review: Two wys to find t ny point in spce: Sum o Integte ove chges: q 1 1 q 2 2 3 P i 1 q i i dq q 3 P 1 dq xmple of integting ove distiution: line of chge ing of

More information

Physics 11b Lecture #11

Physics 11b Lecture #11 Physics 11b Lectue #11 Mgnetic Fields Souces of the Mgnetic Field S&J Chpte 9, 3 Wht We Did Lst Time Mgnetic fields e simil to electic fields Only diffeence: no single mgnetic pole Loentz foce Moving chge

More information

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018. SPA7U/SPA7P: THE GALAXY Solutions fo Cousewok Questions distibuted on: 25 Jnuy 28. Solution. Assessed question] We e told tht this is fint glxy, so essentilly we hve to ty to clssify it bsed on its spectl

More information

9.4 The response of equilibrium to temperature (continued)

9.4 The response of equilibrium to temperature (continued) 9.4 The esponse of equilibium to tempetue (continued) In the lst lectue, we studied how the chemicl equilibium esponds to the vition of pessue nd tempetue. At the end, we deived the vn t off eqution: d

More information

SOLUTIONS TO CONCEPTS CHAPTER 11

SOLUTIONS TO CONCEPTS CHAPTER 11 SLUTINS T NEPTS HPTE. Gvittionl fce of ttction, F.7 0 0 0.7 0 7 N (0.). To clculte the gvittionl fce on t unline due to othe ouse. F D G 4 ( / ) 8G E F I F G ( / ) G ( / ) G 4G 4 D F F G ( / ) G esultnt

More information

PDE Notes. Paul Carnig. January ODE s vs PDE s 1

PDE Notes. Paul Carnig. January ODE s vs PDE s 1 PDE Notes Pul Crnig Jnury 2014 Contents 1 ODE s vs PDE s 1 2 Section 1.2 Het diffusion Eqution 1 2.1 Fourier s w of Het Conduction............................. 2 2.2 Energy Conservtion.....................................

More information

Electricity & Magnetism Lecture 6: Electric Potential

Electricity & Magnetism Lecture 6: Electric Potential Electicity & Mgnetism Lectue 6: Electic Potentil Tody s Concept: Electic Potenl (Defined in tems of Pth Integl of Electic Field) Electicity & Mgnesm Lectue 6, Slide Stuff you sked bout:! Explin moe why

More information

3.1 Magnetic Fields. Oersted and Ampere

3.1 Magnetic Fields. Oersted and Ampere 3.1 Mgnetic Fields Oested nd Ampee The definition of mgnetic induction, B Fields of smll loop (dipole) Mgnetic fields in mtte: ) feomgnetism ) mgnetiztion, (M ) c) mgnetic susceptiility, m d) mgnetic field,

More information

Chapter 2. Numerical Integration also called quadrature. 2.2 Trapezoidal Rule. 2.1 A basic principle Extending the Trapezoidal Rule DRAWINGS

Chapter 2. Numerical Integration also called quadrature. 2.2 Trapezoidal Rule. 2.1 A basic principle Extending the Trapezoidal Rule DRAWINGS S Cpter Numericl Integrtion lso clled qudrture Te gol of numericl integrtion is to pproximte numericlly. f(x)dx Tis is useful for difficult integrls like sin(x) ; sin(x ); x + x 4 Or worse still for multiple-dimensionl

More information

PHYS 601 HW3 Solution

PHYS 601 HW3 Solution 3.1 Norl force using Lgrnge ultiplier Using the center of the hoop s origin, we will describe the position of the prticle with conventionl polr coordintes. The Lgrngin is therefore L = 1 2 ṙ2 + 1 2 r2

More information

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = = Chpte 1 nivesl Gvittion 11 *P1. () The un-th distnce is 1.4 nd the th-moon 8 distnce is.84, so the distnce fom the un to the Moon duing sol eclipse is 11 8 11 1.4.84 = 1.4 The mss of the un, th, nd Moon

More information

Answers to test yourself questions

Answers to test yourself questions Answes to test youself questions opic Descibing fields Gm Gm Gm Gm he net field t is: g ( d / ) ( 4d / ) d d Gm Gm Gm Gm Gm Gm b he net potentil t is: V d / 4d / d 4d d d V e 4 7 9 49 J kg 7 7 Gm d b E

More information

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept

More information

U>, and is negative. Electric Potential Energy

U>, and is negative. Electric Potential Energy Electic Potentil Enegy Think of gvittionl potentil enegy. When the lock is moved veticlly up ginst gvity, the gvittionl foce does negtive wok (you do positive wok), nd the potentil enegy (U) inceses. When

More information

1. Motivation. Fig.1. Spherical rotor - view

1. Motivation. Fig.1. Spherical rotor - view Diusz Spłek Silesin Univesity o Tecnology Electicl Engineeing Fculty ul. Akdemick, 44- Gliwice, Polnd e-mil: Diusz.Splek@polsl.pl Speicl induction moto wit nisotopic oto - nlyticl solutions o electomgnetic

More information

Chapter 25: Current, Resistance and Electromotive Force. ~10-4 m/s Typical speeds ~ 10 6 m/s

Chapter 25: Current, Resistance and Electromotive Force. ~10-4 m/s Typical speeds ~ 10 6 m/s Chpte 5: Cuent, esistnce nd lectomotive Foce Chge cie motion in conducto in two pts Constnt Acceletion F m q ndomizing Collisions (momentum, enegy) >esulting Motion http://phys3p.sl.psu.edu/phys_nim/m/ndom_wlk.vi

More information

Previously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system

Previously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system 436-459 Advnced contol nd utomtion Extensions to bckstepping contolle designs Tcking Obseves (nonline dmping) Peviously Lst lectue we looked t designing nonline contolles using the bckstepping technique

More information

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016 Newton's Lw of Univesl Gvittion Gvittionl Foce lick on the topic to go to tht section Gvittionl Field lgeb sed Physics Newton's Lw of Univesl Gvittion Sufce Gvity Gvittionl Field in Spce Keple's Thid Lw

More information

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information m m m00 kg dult, m0 kg bby. he seesw stts fom est. Which diection will it ottes? ( Counte-Clockwise (b Clockwise ( (c o ottion ti (d ot enough infomtion Effect of Constnt et oque.3 A constnt non-zeo toque

More information

Lecture 10. Solution of Nonlinear Equations - II

Lecture 10. Solution of Nonlinear Equations - II Fied point Poblems Lectue Solution o Nonline Equtions - II Given unction g : R R, vlue such tht gis clled ied point o the unction g, since is unchnged when g is pplied to it. Whees with nonline eqution

More information

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 11. Chapter 3, CHEM 793, 2011 Fall, L. Ma

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 11. Chapter 3, CHEM 793, 2011 Fall, L. Ma Cpte 3 Bsic Cystopy nd Eecton Diffction fom Cysts Lectue Pof. Sectmn: Nobe impossibe witout micoscope Isei ecipient of 0 cemisty Nobe Pize sys oundbein discoey of 'qusicysts' woud e been deyed fo yes witout

More information

STUDY OF THE UNIFORM MAGNETIC FIELD DOMAINS (3D) IN THE CASE OF THE HELMHOLTZ COILS

STUDY OF THE UNIFORM MAGNETIC FIELD DOMAINS (3D) IN THE CASE OF THE HELMHOLTZ COILS STUDY OF THE UNIFORM MAGNETIC FIED DOMAINS (3D) IN THE CASE OF THE HEMHOTZ COIS FORIN ENACHE, GHEORGHE GAVRIĂ, EMI CAZACU, Key wods: Unifom mgnetic field, Helmholt coils. Helmholt coils e used to estblish

More information

ME 236 Engineering Mechanics I Test #4 Solution

ME 236 Engineering Mechanics I Test #4 Solution ME 36 Enineein Mechnics I est #4 Slutin Dte: id, M 14, 4 ie: 8:-1: inutes Instuctins: vein hptes 1-13 f the tetbk, clsed-bk test, clcults llwed. 1 (4% blck ves utwd ln the slt in the pltf with speed f

More information

Prof. Anchordoqui Problems set # 12 Physics 169 May 12, 2015

Prof. Anchordoqui Problems set # 12 Physics 169 May 12, 2015 Pof. Anchodoqui Poblems set # 12 Physics 169 My 12, 2015 1. Two concentic conducting sphees of inne nd oute dii nd b, espectively, cy chges ±Q. The empty spce between the sphees is hlf-filled by hemispheicl

More information

A Permanent Magnet Device for Measuring the Coercive Force

A Permanent Magnet Device for Measuring the Coercive Force 7th Wold Confeence on Nondestuctive Testing, 5-8 Oct 008, Shnghi, Chin A Penent Mgnet Device fo Mesuing the Coecive Foce Edud S. GORKUNOV, Ve P. TABACHNIK Institute of Engineeing Science, RAS (Ul Bnch)

More information

Study of Electromagnetic Wave Propagation in Periodic Dielectric Structure; MathCAD Analysis

Study of Electromagnetic Wave Propagation in Periodic Dielectric Structure; MathCAD Analysis Communictions in Applied Sciences ISSN -737 Volume Nume 3-9 Stud of lectomgnetic Wve Popgtion in Peiodic Dielectic Stuctue; MthCAD Anlsis Ugwu mmnuel.i Ieogu C. nd chi M.I Deptment of Industil phsics oni

More information

Stress State for Pipes Made of a Concrete and Fiber Glass when Change the Angle of the Reinforcing

Stress State for Pipes Made of a Concrete and Fiber Glass when Change the Angle of the Reinforcing Intentionl Jounl of Science nd ngineeing Investigtions vol. issue 5 Apil 0 ISSN: 5-884 Stess Stte fo Pipes de of Concete nd Fie lss when Chnge the Angle of the Reinfocing ymo Aed Alstt Sediq echnicl duction

More information

Chapter 2. Review of Newton's Laws, Units and Dimensions, and Basic Physics

Chapter 2. Review of Newton's Laws, Units and Dimensions, and Basic Physics Chpte. Review of Newton's Lws, Units nd Diensions, nd Bsic Physics You e ll fili with these ipotnt lws. But which e bsed on expeients nd which e ttes of definition? FIRST LAW n object oves unifoly (o eins

More information

Solution of fuzzy multi-objective nonlinear programming problem using interval arithmetic based alpha-cut

Solution of fuzzy multi-objective nonlinear programming problem using interval arithmetic based alpha-cut Intentionl Jounl of Sttistics nd Applied Mthemtics 016; 1(3): 1-5 ISSN: 456-145 Mths 016; 1(3): 1-5 016 Stts & Mths www.mthsounl.com Received: 05-07-016 Accepted: 06-08-016 C Lognthn Dept of Mthemtics

More information

Physics 604 Problem Set 1 Due Sept 16, 2010

Physics 604 Problem Set 1 Due Sept 16, 2010 Physics 64 Polem et 1 Due ept 16 1 1) ) Inside good conducto the electic field is eo (electons in the conducto ecuse they e fee to move move in wy to cncel ny electic field impessed on the conducto inside

More information

Mathematical Reflections, Issue 5, INEQUALITIES ON RATIOS OF RADII OF TANGENT CIRCLES. Y.N. Aliyev

Mathematical Reflections, Issue 5, INEQUALITIES ON RATIOS OF RADII OF TANGENT CIRCLES. Y.N. Aliyev themtil efletions, Issue 5, 015 INEQULITIES ON TIOS OF DII OF TNGENT ILES YN liev stt Some inequlities involving tios of dii of intenll tngent iles whih inteset the given line in fied points e studied

More information

π,π is the angle FROM a! TO b

π,π is the angle FROM a! TO b Mth 151: 1.2 The Dot Poduct We hve scled vectos (o, multiplied vectos y el nume clled scl) nd dded vectos (in ectngul component fom). Cn we multiply vectos togethe? The nswe is YES! In fct, thee e two

More information

A P P E N D I X POWERS OF TEN AND SCIENTIFIC NOTATION A P P E N D I X SIGNIFICANT FIGURES

A P P E N D I X POWERS OF TEN AND SCIENTIFIC NOTATION A P P E N D I X SIGNIFICANT FIGURES A POWERS OF TEN AND SCIENTIFIC NOTATION In science, very lrge nd very smll deciml numbers re conveniently expressed in terms of powers of ten, some of wic re listed below: 0 3 0 0 0 000 0 3 0 0 0 0.00

More information

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin 1 1 Electic Field + + q F Q R oigin E 0 0 F E ˆ E 4 4 R q Q R Q - - Electic field intensity depends on the medium! Electic Flux Density We intoduce new vecto field D independent of medium. D E So, electic

More information

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by Clss Summy.5 Eponentil Functions.6 Invese Functions nd Logithms A function f is ule tht ssigns to ech element D ectly one element, clled f( ), in. Fo emple : function not function Given functions f, g:

More information

DYNAMICS. Kinetics of Particles: Newton s Second Law VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

DYNAMICS. Kinetics of Particles: Newton s Second Law VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr. Ninth E CHPTER VECTOR MECHNICS OR ENGINEERS: DYNMICS edinnd P. ee E. Russell Johnston, J. Lectue Notes: J. Wlt Ole Texs Tech Univesity Kinetics of Pticles: Newton s Second Lw The McGw-Hill Copnies, Inc.

More information

13.5. Torsion of a curve Tangential and Normal Components of Acceleration

13.5. Torsion of a curve Tangential and Normal Components of Acceleration 13.5 osion of cuve ngentil nd oml Components of Acceletion Recll: Length of cuve '( t) Ac length function s( t) b t u du '( t) Ac length pmetiztion ( s) with '( s) 1 '( t) Unit tngent vecto '( t) Cuvtue:

More information

Multi-Electron Atoms-Helium

Multi-Electron Atoms-Helium Multi-lecto Atos-Heliu He - se s H but with Z He - electos. No exct solutio of.. but c use H wve fuctios d eegy levels s sttig poit ucleus sceeed d so Zeffective is < sceeig is ~se s e-e epulsio fo He,

More information

Topics for Review for Final Exam in Calculus 16A

Topics for Review for Final Exam in Calculus 16A Topics fo Review fo Finl Em in Clculus 16A Instucto: Zvezdelin Stnkov Contents 1. Definitions 1. Theoems nd Poblem Solving Techniques 1 3. Eecises to Review 5 4. Chet Sheet 5 1. Definitions Undestnd the

More information

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3 DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl

More information

International Journal of Pure and Applied Sciences and Technology

International Journal of Pure and Applied Sciences and Technology Int. J. Pue l. Sci. Technol. () (0). -6 Intentionl Jounl of Pue nd lied Sciences nd Technology ISSN 9-607 vilble online t www.ijost.in Resech Pe Rdil Vibtions in Mico-Isotoic Mico-Elstic Hollow Shee R.

More information

A COMPARISON OF MEMBRANE SHELL THEORIES OF HYBRID ANISOTROPIC MATERIALS ABSTRACT

A COMPARISON OF MEMBRANE SHELL THEORIES OF HYBRID ANISOTROPIC MATERIALS ABSTRACT A COMPARISON OF MEMBRANE SHELL THEORIES OF HYBRID ANISOTROPIC MATERIALS S. W. Chung* School of Achitectue Univesity of Uth Slt Lke City, Uth, USA S.G. Hong Deptment of Achitectue Seoul Ntionl Univesity

More information

1. The sphere P travels in a straight line with speed

1. The sphere P travels in a straight line with speed 1. The sphee P tels in stight line with speed = 10 m/s. Fo the instnt depicted, detemine the coesponding lues of,,,,, s mesued eltie to the fixed Oxy coodinte system. (/134) + 38.66 1.34 51.34 10sin 3.639

More information

Friedmannien equations

Friedmannien equations ..6 Fiedmnnien equtions FLRW metic is : ds c The metic intevl is: dt ( t) d ( ) hee f ( ) is function which detemines globl geometic l popety of D spce. f d sin d One cn put it in the Einstein equtions

More information

Part 2: CM3110 Transport Processes and Unit Operations I. Professor Faith Morrison. CM2110/CM Review. Concerned now with rates of heat transfer

Part 2: CM3110 Transport Processes and Unit Operations I. Professor Faith Morrison. CM2110/CM Review. Concerned now with rates of heat transfer CM30 anspot Pocesses and Unit Opeations I Pat : Pofesso Fait Moison Depatment of Cemical Engineeing Micigan ecnological Uniesity CM30 - Momentum and Heat anspot CM30 Heat and Mass anspot www.cem.mtu.edu/~fmoiso/cm30/cm30.tml

More information

Physics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468

Physics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468 ics Announcements dy, embe 28, 2004 Ch 6: Cicul Motion - centipetl cceletion Fiction Tension - the mssless sting Help this week: Wednesdy, 8-9 pm in NSC 128/119 Sundy, 6:30-8 pm in CCLIR 468 Announcements

More information

Collection of Formulas

Collection of Formulas Collection of Fomuls Electomgnetic Fields EITF8 Deptment of Electicl nd Infomtion Technology Lund Univesity, Sweden August 8 / ELECTOSTATICS field point '' ' Oigin ' Souce point Coulomb s Lw The foce F

More information

Chapter 25: Current, Resistance and Electromotive Force. Charge carrier motion in a conductor in two parts

Chapter 25: Current, Resistance and Electromotive Force. Charge carrier motion in a conductor in two parts Chpte 5: Cuent, esistnce nd Electomotive Foce Chge cie motion in conducto in two pts Constnt Acceletion F m qe ndomizing Collisions (momentum, enegy) =>esulting Motion Avege motion = Dift elocity = v d

More information

Quantum transport (Read Kittel, 8th ed., pp )

Quantum transport (Read Kittel, 8th ed., pp ) Quntum trnsport (Red Kittel, 8t ed., pp. 533-554) Wen we ve structure in wic mny collisions tke plce s crriers trnsport cross it, te quntum mecnicl pse of te electron wvefunctions is essentilly rndomized,

More information

dx was area under f ( x ) if ( ) 0

dx was area under f ( x ) if ( ) 0 13. Line Integls Line integls e simil to single integl, f ( x) dx ws e unde f ( x ) if ( ) 0 Insted of integting ove n intevl [, ] (, ) f xy ds f x., we integte ove cuve, (in the xy-plne). **Figue - get

More information

Influence of field dependent form of collision integral on kinetic coefficients

Influence of field dependent form of collision integral on kinetic coefficients Semiconducto Psics Quntum Electonics & Optoelectonics 6 V 9 N P 7-8 doi: 57/speo97 PCS 7-d 7i nluence o ield dependent om o collision integl on inetic coeicients oio V sov nstitute o Semiconducto Psics

More information

Qualitative Analysis for Solutions of a Class of. Nonlinear Ordinary Differential Equations

Qualitative Analysis for Solutions of a Class of. Nonlinear Ordinary Differential Equations Adv. Theo. Appl. Mech., Vol. 7, 2014, no. 1, 1-7 HIKARI Ltd, www.m-hiki.com http://dx.doi.og/10.12988/tm.2014.458 Qulittive Anlysis fo Solutions of Clss of Nonline Odiny Diffeentil Equtions Juxin Li *,

More information

Problem Set 5: Universal Law of Gravitation; Circular Planetary Orbits

Problem Set 5: Universal Law of Gravitation; Circular Planetary Orbits Poblem Set 5: Univesal Law of Gavitation; Cicula Planetay Obits Design Engineeing Callenge: Te Big Dig.007 Contest Evaluation of Scoing Concepts: Spinne vs. Plowe PROMBLEM 1: Daw a fee-body-diagam of a

More information

RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1

RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1 RELAIVE KINEMAICS he equtions of motion fo point P will be nlyzed in two diffeent efeence systems. One efeence system is inetil, fixed to the gound, the second system is moving in the physicl spce nd the

More information

A Two-Dimensional Analytical Modeling of the Current-Voltage Characteristics for Submicron Gate-Length Ga As MESFET s

A Two-Dimensional Analytical Modeling of the Current-Voltage Characteristics for Submicron Gate-Length Ga As MESFET s Intentionl Jounl of ngineeing & Tecnolog IJT-IJN Vol: No:4 7 Two-imensionl nlticl Modeling of te Cuent-Voltge Ccteistics fo ubmicon Gte-Lengt G s MFT s deddine Kemissi, nd Ceif zizi bstct two-dimensionl

More information

6. Numbers. The line of numbers: Important subsets of IR:

6. Numbers. The line of numbers: Important subsets of IR: 6. Nubes We do not give n xiotic definition of the el nubes hee. Intuitive ening: Ech point on the (infinite) line of nubes coesponds to el nube, i.e., n eleent of IR. The line of nubes: Ipotnt subsets

More information

cos kd kd 2 cosθ = π 2 ± nπ d λ cosθ = 1 2 ± n N db

cos kd kd 2 cosθ = π 2 ± nπ d λ cosθ = 1 2 ± n N db . (Balanis 6.43) You can confim tat AF = e j kd cosθ + e j kd cosθ N = cos kd cosθ gives te same esult as (6-59) and (6-6), fo a binomial aay wit te coefficients cosen as in section 6.8.. Tis single expession

More information

MATHEMATICAL STUDY OF LAPLACE AND YOUNG EQUATIONS IN THE CASE OF THE CONTACT BETWEEN A DROP AND FIBRE

MATHEMATICAL STUDY OF LAPLACE AND YOUNG EQUATIONS IN THE CASE OF THE CONTACT BETWEEN A DROP AND FIBRE MATHEMATICA STUDY O APACE AND YOUNG EQUATIONS IN THE CASE O THE CONTACT BETWEEN A DROP AND IBRE T. Hmie nd A. Bid Institut de Cimie des Sufces et Intefces I.C.S.I.-C.N.R.S.-UPR 969 5, Rue Jen Stcky - B.P.488-6857-

More information

Michael Rotkowitz 1,2

Michael Rotkowitz 1,2 Novembe 23, 2006 edited Line Contolles e Unifomly Optiml fo the Witsenhusen Counteexmple Michel Rotkowitz 1,2 IEEE Confeence on Decision nd Contol, 2006 Abstct In 1968, Witsenhusen intoduced his celebted

More information

A Discussion on Formulas of Seismic Hydrodynamic Pressure

A Discussion on Formulas of Seismic Hydrodynamic Pressure Interntionl Forum on Energy Environment Science nd Mterils (IFEESM 2017) A Discussion on Formuls of Seismic Hydrodynmic Pressure Liu Himing1 To Xixin2 1 Cin Mercnts Congqing Communiction Reserc & Design

More information

Pythagorean Theorem and Trigonometry

Pythagorean Theorem and Trigonometry Ptgoren Teorem nd Trigonometr Te Ptgoren Teorem is nient, well-known, nd importnt. It s lrge numer of different proofs, inluding one disovered merin President Jmes. Grfield. Te we site ttp://www.ut-te-knot.org/ptgors/inde.stml

More information

Math Week 5 concepts and homework, due Friday February 10

Math Week 5 concepts and homework, due Friday February 10 Mt 2280-00 Week 5 concepts nd omework, due Fridy Februry 0 Recll tt ll problems re good for seeing if you cn work wit te underlying concepts; tt te underlined problems re to be nded in; nd tt te Fridy

More information

Micro-scale adhesive contact of a spherical rigid punch on a. piezoelectric half-space

Micro-scale adhesive contact of a spherical rigid punch on a. piezoelectric half-space http://www.ppe.edu.cn Mico-scle dhesive contct of spheicl igid punch on piezoelectic hlf-spce Z.R. Chen, S.W. Yu * Deptment of Engineeing Mechnics, Tsinghu Univesity, Beijing 84, P.R. Chin Abstct The mico-scle

More information

Two dimensional polar coordinate system in airy stress functions

Two dimensional polar coordinate system in airy stress functions I J C T A, 9(9), 6, pp. 433-44 Intentionl Science Pess Two dimensionl pol coodinte system in iy stess functions S. Senthil nd P. Sek ABSTRACT Stisfy the given equtions, boundy conditions nd bihmonic eqution.in

More information

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97 Univesity of Bhin Physics 10 Finl Exm Key Fll 004 Deptment of Physics 13/1/005 8:30 10:30 e =1.610 19 C, m e =9.1110 31 Kg, m p =1.6710 7 Kg k=910 9 Nm /C, ε 0 =8.8410 1 C /Nm, µ 0 =4π10 7 T.m/A Pt : 10

More information

Tutorial on Strehl ratio, wavefront power series expansion, Zernike polynomials expansion in small aberrated optical systems By Sheng Yuan

Tutorial on Strehl ratio, wavefront power series expansion, Zernike polynomials expansion in small aberrated optical systems By Sheng Yuan Tutoial on Stel atio, wavefont powe seies expansion, Zenike polynomials expansion in small abeated optical systems By Seng Yuan. Stel Ratio Te wave abeation function, (x,y, is defined as te distance, in

More information

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s: Chpte 7 Kleene s Theoem 7.1 Kleene s Theoem The following theoem is the most impotnt nd fundmentl esult in the theoy of FA s: Theoem 6 Any lnguge tht cn e defined y eithe egul expession, o finite utomt,

More information

Equations from the Millennium Theory of Inertia and Gravity. Copyright 2004 Joseph A. Rybczyk

Equations from the Millennium Theory of Inertia and Gravity. Copyright 2004 Joseph A. Rybczyk Equtions fo the illenniu heoy of Ineti nd vity Copyight 004 Joseph A. Rybzyk ollowing is oplete list of ll of the equtions used o deived in the illenniu heoy of Ineti nd vity. o ese of efeene the equtions

More information

Solutions to Midterm Physics 201

Solutions to Midterm Physics 201 Solutions to Midtem Physics. We cn conside this sitution s supeposition of unifomly chged sphee of chge density ρ nd dius R, nd second unifomly chged sphee of chge density ρ nd dius R t the position of

More information

Elastic limit angular speed of solid and annular disks under thermomechanical

Elastic limit angular speed of solid and annular disks under thermomechanical MultiCft Intentionl Jounl of Engineeing, Science nd Technology Vol. 8, No., 016, pp. 30-45 INTERNATIONAL JOURNAL OF ENGINEERING, SCIENCE AND TECHNOLOGY www.ijest-ng.com www.jol.info/index.php/ijest 016

More information

Continuous Charge Distributions

Continuous Charge Distributions Continuous Chge Distibutions Review Wht if we hve distibution of chge? ˆ Q chge of distibution. Q dq element of chge. d contibution to due to dq. Cn wite dq = ρ dv; ρ is the chge density. = 1 4πε 0 qi

More information

This immediately suggests an inverse-square law for a "piece" of current along the line.

This immediately suggests an inverse-square law for a piece of current along the line. Electomgnetic Theoy (EMT) Pof Rui, UNC Asheville, doctophys on YouTube Chpte T Notes The iot-svt Lw T nvese-sque Lw fo Mgnetism Compe the mgnitude of the electic field t distnce wy fom n infinite line

More information