NETWORK ANALYSIS OF ANTENNA BASED ON SCATTERING PARAMETERS

Size: px
Start display at page:

Download "NETWORK ANALYSIS OF ANTENNA BASED ON SCATTERING PARAMETERS"

Transcription

1 Intentionl Jounl of Industil Electonics nd Electicl Engineeing, IN: Volume-3, Issue-, Fe.-5 NETWORK ANALYI OF ANTENNA BAED ON CATTERING ARAMETER RENU INGH, KUMARI MAMTA Resech chol Associte ofesso Jhkhnd Ri Univesity, Rnchi, Indi E-mil:- Astct: Antenn design involves mny electicl nd mechnicl metes. The most imotnt electicl metes include dition ens, gin, diectivity, inut imednce, ndwidth, nd efficiency. This e develos new fom of two ot netwok nlysis of n ntenn system sed on sceing metes (-metes) of n ntenn element nd its dition en. In this fomultion, ntenn dition is consideed in tems of electomgnetic couling etween the test ntenn nd oe ntenn. Keywods: Antenn metes, ceing mete Test ntenn, oe ntenn. I. INTRODUCTION In the field of ntenn thee e some of the oul ntenn nlysis methods ely on numeicl techniques, such s the method of moments (MoM), the finite element method (FEM), nd the finitediffeence time-domin method (FDTD) [-3], to diectly solve Mxwell's equtions. The vilility of numeous commecil softwe ckges, llow electicl enginees to vey esily nd idly nlyze ntenns of vious geometies. At the sme time, these comlex simultions codes e often used imoely nd code oututs e not inteeted oely. This e esents new sceing mete sed netwok model fo the nlysis of ntenn. The model includes desciion fo the mutul couling etween y elements nd the couling though the souce netwok. This model llows comct desciion of the imednce chcteistics nd the dition chcteistics of ntenn fom the sme set of -metes. ceing metes e imotnt in micowve design ecuse they e esie to mesue nd wok with t high fequencies thn those of othe kinds of metes. These models llow comuion of dited field nd dited owe in tems of wve incident on the ntenn element o the y elements. The incident wves nd the dited owe cn e used to comute ntenn design metes such s diectivity, gin nd efficiencies. Thee is need fo technique tht integtes the tetment of ll the ntenn metes in systemtic wy duing the design ocess. Netwok desciions of ntenn systems llow the integtion of some of the ntenn electicl metes [4-7]. Then mete in mtix fom cn e wien s, ( ceingmtix ) The incident wves, eflected wves nd metes cn e elted s follows Whee, mtix elements,, nd e efeed to s the sceing metes o the - metes (figue ). The metes, hve the mening of eflection coefficients, nd, the mening of tnsmission coefficients. The tveling wve viles, t ot nd, t ot e defined in tems of V, I nd V, I nd el-vlued ositive efeence imednce Z s follows: V Z I z V Z I z V Z I z V Z I z tvelingwves The ctul mesuements of the -metes e mde y connecting to mtched lod, Z L = Z. Then, thee will e no eflected wves fom the lod, = nd the -mtix equtions will give: Netwok Anlysis Of Antenn Bsed On ceing metes

2 Intentionl Jounl of Industil Electonics nd Electicl Engineeing, IN: = + = = + = Z L Z Z L Z eflection coefficient tnsmission coefficient In two ot netwok, nd e descied in db s follows = log () = log (τ) Volume-3, Issue-, Fe.-5 dition en hving ek elized gin of G R. The oe ntenn is locted t constnt distnce in the diection θ nd zimuth ngles with esect to given efeence lne nd oigin. The test ntenn ot nd the oe ntenn ot fom two ot netwok whose teminl chcteistics cn e descied y mtix. The incident wves, eflected wves nd -mete cn e elted s follows (,)=(,)(,) (3) Whee tnsmission coefficient equls incident voltge divided y tnsmied voltge = V Tnsmied / V Incident And Reflection coefficient equls incident voltge divided y eflected voltge τ = V Reflected / V Incident is genelly etween nd -, exce some ctive cicuits such s oscillto with lge thn db. ceing mtix [] stisfies [] + [] = [I] () Whee [ ] + = ([*]) T = ([ ] T ) *. Hee suesci * eesents conjugtion, [ ] T denotes mtix tnsose nd [I] is unity mtix. Eqution () is efeed to the lossless unitity. Fo two-ot lossless netwok, the unity condition () cn e exessed s thee indeendent equtions * * () Which, in tems of tvelling wve viles, is equivlent to II. MODEL: -ARAMETER NETWORK MODEL Conside n ity test ntenn with n inut ot nd distnt oe ntenn with outut ot (figue 3). The oe ntenn is used to detect the fields dited y the test ntenn. We ssume tht the oe ntenn is line ssive device with Fig. 3: ignl flow digm fo n ity test ntenn nd oe ntenn with two othogonl oliztion ots (,, ), ), ) t t t, ), ), ), ), ) (4) is the sceing mtix, is column vecto whose element is the incident wve t ech ot, nd is column vecto in which the element is the eflected wve t ech ot [8]. The dition en is defined y the owe eceived y the oe ntenn moved ound constnt distnce fom the ntenn unde test oeting in the tnsmit mode.,, t, e the couling coefficient etween the test ntenn nd the oe ntenn. Now if the fowd coulings (the fist column of the -mtix) nd the coesonding evese coulings (the fist ow of the -mtix) e identicl, o (,)= t (,) (5) The viles nd in eqution (4) eesent the outut wves tht come out of the oe ntenn ots nd the wves tht e eflected fom the eceives ck to the oe ntenn ot. Assuming tht nd e exessed in oot men sque fom, the owes deliveed y the test ntenn to the oe ntenn ots will e del, ), ), ) (6) The deliveed owes s function of ngul osition of the oe ntenn e ootionl to the ntenn owe ens of the test ntenn. The deliveed owe is detemined y lying Mson's ule [8] on the -metes. Using the outut wves, the wves eflected fom the eceives to the oe ots e detemined y Netwok Anlysis Of Antenn Bsed On ceing metes

3 Intentionl Jounl of Industil Electonics nd Electicl Engineeing, IN: (,)= (,) (7) When the eceive lod imednces e set to the efeence imednce Z = Z o, the eflection coefficients of the eceives ecome zeo, =. Then, the oe incident wves ecome (,)= (,)= (8) Thus, the owes deliveed t the oe ots simlify to del (,, ) (,, ) (9) The outut wves fom the oes couled fom the test ntenn, Volume-3, Issue-, Fe.-5 Whee the symols hve the following menings: v = owe ville fom souce [W], in = inut owe cceed y the ntenn [W], d = owe dited y the ntenn [W], U = dition intensity [W/s], U n = til dition intensity [W/s], e = dition efficiency, q = imednce mismtch, G R = elized gin, G = gin, D = diectivity, G Rn = til elized gin, G n = til gin, D n = til diectivity, = oliztion efficiency. 3. Diectivity Diectivity quntifies how the dited owe is concentted in given diection comed to the totl dited owe. The diectivity, D (,), is defined s 4 times the tio of the dition intensity in given diection to the totl owe dited,, ), ), ), ) t s s () Theefoe the owe deliveed to the oe ntenn ots e detemined to e del, ) (, ) t, ) (, ) s s () del, ) (, ), ) t () III. RELATIONHI BETWEEN ANTENNA NETWORK MODEL AND ANTENNA ARAMETER Equtions () o () eesent the sic ntenn netwok model fo n ntenn. They include the ntenn dition en, oliztion, inut imednce, nd efficiency in comct fom. Conside the gin nd diectivity flow cht, shown in figue 4, modified fom the cht in IEEE tndd [9]. Fig. 4: Gin nd diectivity flow cht. Modified fom the cht in IEEE td. [9]. 4, ) (, ) (3), ) d D The nomlized dition en is detemined in tems of the -metes will e, ) 3. Gin mx,, (4) Gin is used to quntify how efficiently n ntenn tnsfoms the ville owe t its inut teminl to the owe dited in given diection. This mens, gin is equl to diectivity educed y losses on the ntenn, o dition efficiency (4) G(, ), ) G ( s ) R (5) deceses s inceses. When these - metes vlue e detemined with esect to efeence imednce Z o, tht is comlex conjugte of the ntenn inut imednce, the esulting will e equl to zeo, i.e when the ntenn is mtched. Then, the gin ecomes uely function of the tnsmission coefficient. This esult is consistent with the definition of gin. It is useful to define -metes tht e indeendent of distnce nd oe elized gin G R. Let us define nomlized -metes s ' (, ) 4 G R (,, ) (6) Netwok Anlysis Of Antenn Bsed On ceing metes 3

4 Intentionl Jounl of Industil Electonics nd Electicl Engineeing, IN: The nomlized -mete eesents the couling fom the test ntenn to the oe ntenn e unit din. Using the nomlized -mete the gin y (5) simlifies to Volume-3, Issue-, Fe.-5 4 G(, ) ( s ) (, ) (7) Which is vlid when the oe ntenn is sufficiently f wy fom the test ntenn ( ) such tht vey lile intection occu etween them. 3.3 Rdition Efficiency The dition efficiency of n ntenn is detemined y the tio etween the gin nd diectivity, Tle : A summy of electicl efomnce of the sti diole inted ntenn on n infinite dielectic sustte ove n infinite gound lne detemined y oosed model. e = G(,) / D (,) e G R 4 ( ), ) d e (, ) d IV. MEAUREMENT REULT Let us ly this model to the geomety of single sti diole element inted on n infinite sustte. The sti diole hs length of L = 38 mm, width W = mm nd dielectic constnt =.33. The sustte is susended ove n infinite gound lne t height of h = mm. We will designte the dition en nd the inut imednce of the single sti diole inted on this sustte s the isolted element en nd the isolted element imednce. It must e noted tht the tem isolted does not eesent the sti diole in fee sce. The dielectic sustte nd the gound lne e included in the nlysis. A single sti diole element inted on sustte ws simulted using IE3D fom Zelnd [] to detemine the -mete nd the dition en. All of the sceing metes esented in this exmle e efeenced to Z = 5Ω. The zeo cossing of the imginy t of the -mete ne 3 GHz, nd nely zeo vlue fo the el t of the -mete t the sme fequency indictes tht the ntenn is esonnt ne 3 GHz, with the inut imednce of oximtely 5Ω. Tle : A summy of electicl efomnce of the sti diole inted ntenn on n infinite dielectic sustte ove n infinite gound lne simulted using IE3D. The simulted esults (Tle ) hve good geement with ll stndd metes detemined y oosed model (Tle ), exce fo the mgin of exeimentl eo e it fo odside diectivity, odside gin, odside elized gin, dition efficiency, imednce mismtch fcto o inut imednce t 3GHz. Aove ll, ticully thee is n excellent mtch fo -mete t 3 GHz which hs een t the centl theme nd focus of the e. CONCLUION The ojective, in this e ws to esent the deivtion of single ntenn desciion using two-ot, -mete netwok model nd do its vlidtion using IE3D. The -metes in the netwok wee extended to include the stil deendency to model the couling fom the test ntenn to the oe ntenn locted t (,). The deliveed owe to the oe ntenn ots when the test ntenn is excited with souce ws deived. Fom the deliveed owes, the ntenn metes wee deived in tems of ntenn netwok - metes. The simultion esults otined e found to e in good geement with ll the stndd mete vlues detemined y the oosed model within the limit of exeimentl eo. Netwok Anlysis Of Antenn Bsed On ceing metes 4

5 Intentionl Jounl of Industil Electonics nd Electicl Engineeing, IN: REFERENCE [] Gyen, Rintu K nd Ds, ushut, A high-gin od-nd wveguide longitudinl slot y ntenn, ogess In Electomgnetics Resech C, 3; 44: []Li, J Y, Li, L W nd Gn, Y B, Method of Moments Anlysis of wveguide slot ntenns using he EFIE, J. of Electomgnetics. Wves nd l., 5; 9 n3: [3] Ellio, R, An imoved design ocedue fo smll ys of shunt slots, IEEE Tns. Antenns ogtion, 983; 3 n: [4] Hington R F, Antenn exciion fo mximum gin, IEEE Tns. Antenns ogt., 965; A-3 n6: Volume-3, Issue-, Fe.-5 [5] Khn, W K nd Wsylkiwskyj W, Couling, dition nd scing y ntenns in Genelized Netwoks, J. Fox, Ed., vol. XVI. New Yok: olytechnic ess, New Yok, 966; [6] Gtely, A C J tock, D J R nd Cheo, B R, A netwok desciion fo ntenn olems, oc. IEEE, 968; 56 n7: [7] Wieseck, W nd Heidich, E Wide-Bnd multiot ntenn chcteiztion y olimetic RC mesuements, IEEE Tns. Antenns ogt., 998; 46 n3: [8] Kuokw, K, owe wves nd the sceing mtix, IEEE Tns. Micowve Theoy Tech., 965; 3: 94-. [9] IEEE tndd Definition of Tems fo Antenns, IEEE td , IEEE, 993. [] IE3D Use's Mnul, Relese 7, Zelnd oftwe, Inc., Femont, Clifoni, 999. Netwok Anlysis Of Antenn Bsed On ceing metes 5

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

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

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

10 Statistical Distributions Solutions

10 Statistical Distributions Solutions Communictions Engineeing MSc - Peliminy Reding 1 Sttisticl Distiutions Solutions 1) Pove tht the vince of unifom distiution with minimum vlue nd mximum vlue ( is ) 1. The vince is the men of the sques

More information

( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x

( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x SIO 22B, Rudnick dpted fom Dvis III. Single vile sttistics The next few lectues e intended s eview of fundmentl sttistics. The gol is to hve us ll speking the sme lnguge s we move to moe dvnced topics.

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

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

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

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

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

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

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

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

Multiple-input multiple-output (MIMO) communication systems. Advanced Modulation and Coding : MIMO Communication Systems 1

Multiple-input multiple-output (MIMO) communication systems. Advanced Modulation and Coding : MIMO Communication Systems 1 Multiple-input multiple-output (MIMO) communiction systems Advnced Modultion nd Coding : MIMO Communiction Systems System model # # #n #m eceive tnsmitte infobits infobits #N #N N tnsmit ntenns N (k) M

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

Ch 26 - Capacitance! What s Next! Review! Lab this week!

Ch 26 - Capacitance! What s Next! Review! Lab this week! Ch 26 - Cpcitnce! Wht s Next! Cpcitnce" One week unit tht hs oth theoeticl n pcticl pplictions! Cuent & Resistnce" Moving chges, finlly!! Diect Cuent Cicuits! Pcticl pplictions of ll the stuff tht we ve

More information

mslumped-parameter (zero-dimensions!) groundwater model of Bangladesh

mslumped-parameter (zero-dimensions!) groundwater model of Bangladesh mslumed-pmete (zeo-dimensions!) goundwte model of Bngldesh You gol in this oblem set is to develo bucket model fo the hydology of ou study site in Bngldesh. Using this model, you will investigte how the

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

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy: LCTROSTATICS. Quntiztion of Chge: Any chged body, big o smll, hs totl chge which is n integl multile of e, i.e. = ± ne, whee n is n intege hving vlues,, etc, e is the chge of electon which is eul to.6

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

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

Week 8. Topic 2 Properties of Logarithms

Week 8. Topic 2 Properties of Logarithms Week 8 Topic 2 Popeties of Logithms 1 Week 8 Topic 2 Popeties of Logithms Intoduction Since the esult of ithm is n eponent, we hve mny popeties of ithms tht e elted to the popeties of eponents. They e

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

EECE 260 Electrical Circuits Prof. Mark Fowler

EECE 260 Electrical Circuits Prof. Mark Fowler EECE 60 Electicl Cicuits Pof. Mk Fowle Complex Numbe Review /6 Complex Numbes Complex numbes ise s oots of polynomils. Definition of imginy # nd some esulting popeties: ( ( )( ) )( ) Recll tht the solution

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

11.1 Balanced Three Phase Voltage Sources

11.1 Balanced Three Phase Voltage Sources BAANCED THREE- PHASE CIRCUITS C.T. Pn 1 CONTENT 11.1 Blnced Thee-Phse Voltge Souces 11.2 Blnced Thee-Phse ods 11.3 Anlysis of the Wye-WyeCicuits 11.4 Anlysis of the Wye-Delt Cicuits 11.5 Powe Clcultions

More information

ELECTRO - MAGNETIC INDUCTION

ELECTRO - MAGNETIC INDUCTION NTRODUCTON LCTRO - MAGNTC NDUCTON Whenee mgnetic flu linked with cicuit chnges, n e.m.f. is induced in the cicuit. f the cicuit is closed, cuent is lso induced in it. The e.m.f. nd cuent poduced lsts s

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

Quality control. Final exam: 2012/1/12 (Thur), 9:00-12:00 Q1 Q2 Q3 Q4 Q5 YOUR NAME

Quality control. Final exam: 2012/1/12 (Thur), 9:00-12:00 Q1 Q2 Q3 Q4 Q5 YOUR NAME Qulity contol Finl exm: // (Thu), 9:-: Q Q Q3 Q4 Q5 YOUR NAME NOTE: Plese wite down the deivtion of you nswe vey clely fo ll questions. The scoe will be educed when you only wite nswe. Also, the scoe will

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

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

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

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

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

Important design issues and engineering applications of SDOF system Frequency response Functions

Important design issues and engineering applications of SDOF system Frequency response Functions Impotnt design issues nd engineeing pplictions of SDOF system Fequency esponse Functions The following desciptions show typicl questions elted to the design nd dynmic pefomnce of second-ode mechnicl system

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 CYLINDRICAL CONTACT MODEL FOR TWO DIMENSIONAL MULTIASPERITY PROFILES

A CYLINDRICAL CONTACT MODEL FOR TWO DIMENSIONAL MULTIASPERITY PROFILES Poceedings of 003 STLE/ASME Intentionl Joint Tibology Confeence Ponte Ved Bech, loid USA, Octobe 6 9, 003 003TIB-69 A CYLINDICAL CONTACT MODEL O TWO DIMENSIONAL MULTIASPEITY POILES John J. Jgodnik nd Sinn

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

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

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

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

Review of Mathematical Concepts

Review of Mathematical Concepts ENEE 322: Signls nd Systems view of Mthemticl Concepts This hndout contins ief eview of mthemticl concepts which e vitlly impotnt to ENEE 322: Signls nd Systems. Since this mteil is coveed in vious couses

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

Introductions to ArithmeticGeometricMean

Introductions to ArithmeticGeometricMean Intoductions to AitheticGeoeticMen Intoduction to the Aithetic-Geoetic Men Genel The ithetic-geoetic en eed in the woks of J Lnden (77, 775) nd J-L Lgnge (784-785) who defined it though the following quite-ntul

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

Section 35 SHM and Circular Motion

Section 35 SHM and Circular Motion Section 35 SHM nd Cicul Motion Phsics 204A Clss Notes Wht do objects do? nd Wh do the do it? Objects sometimes oscillte in simple hmonic motion. In the lst section we looed t mss ibting t the end of sping.

More information

I1 = I2 I1 = I2 + I3 I1 + I2 = I3 + I4 I 3

I1 = I2 I1 = I2 + I3 I1 + I2 = I3 + I4 I 3 2 The Prllel Circuit Electric Circuits: Figure 2- elow show ttery nd multiple resistors rrnged in prllel. Ech resistor receives portion of the current from the ttery sed on its resistnce. The split is

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

Mark Scheme (Results) January 2008

Mark Scheme (Results) January 2008 Mk Scheme (Results) Jnuy 00 GCE GCE Mthemtics (6679/0) Edecel Limited. Registeed in Englnd nd Wles No. 4496750 Registeed Office: One90 High Holbon, London WCV 7BH Jnuy 00 6679 Mechnics M Mk Scheme Question

More information

Chapter 6 Frequency Response & System Concepts

Chapter 6 Frequency Response & System Concepts hpte 6 Fequency esponse & ystem oncepts Jesung Jng stedy stte (fequency) esponse Phso nottion Filte v v Foced esponse by inusoidl Excittion ( t) dv v v dv v cos t dt dt ince the focing fuction is sinusoid,

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

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD ollege Physics Student s Mnul hpte 8 HAPTR 8: LTRI HARG AD LTRI ILD 8. STATI LTRIITY AD HARG: OSRVATIO O HARG. ommon sttic electicity involves chges nging fom nnocoulombs to micocoulombs. () How mny electons

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

The Area of a Triangle

The Area of a Triangle The e of Tingle tkhlid June 1, 015 1 Intodution In this tile we will e disussing the vious methods used fo detemining the e of tingle. Let [X] denote the e of X. Using se nd Height To stt off, the simplest

More information

Design optimization of a damped hybrid vibration absorber

Design optimization of a damped hybrid vibration absorber This is the Pe-Published Vesion. Design otimiztion of dmed hybid vibtion bsobe Y. L. CHEUNG, W. O. WONG, L. CHENG Detment of Mechnicl Engineeing, The Hong Kong Polytechnic Univesity, Hung Hom, Hong Kong

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

APPROXIMATION OF STRONG ELECTRIC FIELD

APPROXIMATION OF STRONG ELECTRIC FIELD APPROXIMATION OF STRONG ELECTRIC FIELD PROF. RNDR. ING. MILOSLAV KOŠEK, CSC. ING. JIŘÍ PRIMAS ING. MICHAL MALÍK PROF. ING. ALEŠ RICHTER, CSC. Abstct: Since stong electic field is used now in mny es, simle

More information

Lectures # He-like systems. October 31 November 4,6

Lectures # He-like systems. October 31 November 4,6 Lectue #5-7 7 Octoe 3 oveme 4,6 Self-conitent field Htee-Foc eqution: He-lie ytem Htee-Foc eqution: cloed-hell hell ytem Chpte 3, pge 6-77, Lectue on Atomic Phyic He-lie ytem H (, h ( + h ( + h ( Z Z:

More information

On Some Hadamard-Type Inequalıtıes for Convex Functıons

On Some Hadamard-Type Inequalıtıes for Convex Functıons Aville t htt://vuedu/ Al Al Mth ISSN: 93-9466 Vol 9, Issue June 4, 388-4 Alictions nd Alied Mthetics: An Intentionl Jounl AAM On Soe Hdd-Tye Inequlıtıes o, Convex Functıons M Ein Özdei Detent o Mthetics

More information

5.4 The Quarter-Wave Transformer

5.4 The Quarter-Wave Transformer 3/4/7 _4 The Qurter Wve Trnsformer /.4 The Qurter-Wve Trnsformer Redg Assignment: pp. 73-76, 4-43 By now you ve noticed tht qurter-wve length of trnsmission le ( = λ 4, β = π ) ppers often microwve engeerg

More information

Dynamically Equivalent Systems. Dynamically Equivalent Systems. Dynamically Equivalent Systems. ME 201 Mechanics of Machines

Dynamically Equivalent Systems. Dynamically Equivalent Systems. Dynamically Equivalent Systems. ME 201 Mechanics of Machines ME 0 Mechnics of Mchines 8//006 Dynmicy Equivent Systems Ex: Connecting od G Dynmicy Equivent Systems. If the mss of the connecting od m G m m B m m m. Moment out cente of gvity shoud e zeo m G m B Theefoe;

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

NS-IBTS indices calculation procedure

NS-IBTS indices calculation procedure ICES Dt Cente DATRAS 1.1 NS-IBTS indices 2013 DATRAS Pocedue Document NS-IBTS indices clcultion pocedue Contents Genel... 2 I Rw ge dt CA -> Age-length key by RFA fo defined ge nge ALK... 4 II Rw length

More information

STD: XI MATHEMATICS Total Marks: 90. I Choose the correct answer: ( 20 x 1 = 20 ) a) x = 1 b) x =2 c) x = 3 d) x = 0

STD: XI MATHEMATICS Total Marks: 90. I Choose the correct answer: ( 20 x 1 = 20 ) a) x = 1 b) x =2 c) x = 3 d) x = 0 STD: XI MATHEMATICS Totl Mks: 90 Time: ½ Hs I Choose the coect nswe: ( 0 = 0 ). The solution of is ) = b) = c) = d) = 0. Given tht the vlue of thid ode deteminnt is then the vlue of the deteminnt fomed

More information

Chapter 28 Sources of Magnetic Field

Chapter 28 Sources of Magnetic Field Chpte 8 Souces of Mgnetic Field - Mgnetic Field of Moving Chge - Mgnetic Field of Cuent Element - Mgnetic Field of Stight Cuent-Cying Conducto - Foce Between Pllel Conductos - Mgnetic Field of Cicul Cuent

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

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

Linear Inequalities. Work Sheet 1

Linear Inequalities. Work Sheet 1 Work Sheet 1 Liner Inequlities Rent--Hep, cr rentl compny,chrges $ 15 per week plus $ 0.0 per mile to rent one of their crs. Suppose you re limited y how much money you cn spend for the week : You cn spend

More information

Fluids & Bernoulli s Equation. Group Problems 9

Fluids & Bernoulli s Equation. Group Problems 9 Goup Poblems 9 Fluids & Benoulli s Eqution Nme This is moe tutoil-like thn poblem nd leds you though conceptul development of Benoulli s eqution using the ides of Newton s 2 nd lw nd enegy. You e going

More information

Plane Wave Expansion Method (PWEM)

Plane Wave Expansion Method (PWEM) /15/18 Instucto D. Rymond Rumpf (915) 747 6958 cumpf@utep.edu EE 5337 Computtionl Electomgnetics Lectue #19 Plne Wve Expnsion Method (PWEM) Lectue 19 These notes my contin copyighted mteil obtined unde

More information

7.5-Determinants in Two Variables

7.5-Determinants in Two Variables 7.-eteminnts in Two Vibles efinition of eteminnt The deteminnt of sque mti is el numbe ssocited with the mti. Eve sque mti hs deteminnt. The deteminnt of mti is the single ent of the mti. The deteminnt

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

(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

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

Analysis of Arithmetic. Analysis of Arithmetic. Analysis of Arithmetic Round-Off Errors. Analysis of Arithmetic. Analysis of Arithmetic

Analysis of Arithmetic. Analysis of Arithmetic. Analysis of Arithmetic Round-Off Errors. Analysis of Arithmetic. Analysis of Arithmetic In the fixed-oint imlementation of a digital filte only the esult of the multilication oeation is quantied The eesentation of a actical multilie with the quantie at its outut is shown below u v Q ^v The

More information

Homework: Study 6.2 #1, 3, 5, 7, 11, 15, 55, 57

Homework: Study 6.2 #1, 3, 5, 7, 11, 15, 55, 57 Gols: 1. Undestnd volume s the sum of the es of n infinite nume of sufces. 2. Be le to identify: the ounded egion the efeence ectngle the sufce tht esults fom evolution of the ectngle ound n xis o foms

More information

General Physics (PHY 2140)

General Physics (PHY 2140) Genel Physics (PHY 40) Lightning Review Lectue 3 Electosttics Lst lectue:. Flux. Guss s s lw. simplifies computtion of electic fields Q Φ net Ecosθ ε o Electicl enegy potentil diffeence nd electic potentil

More information

Unit 6. Magnetic forces

Unit 6. Magnetic forces Unit 6 Mgnetic foces 6.1 ntoduction. Mgnetic field 6. Mgnetic foces on moving electic chges 6. oce on conducto with cuent. 6.4 Action of unifom mgnetic field on flt cuent-cying loop. Mgnetic moment. Electic

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

1 Using Integration to Find Arc Lengths and Surface Areas

1 Using Integration to Find Arc Lengths and Surface Areas Novembe 9, 8 MAT86 Week Justin Ko Using Integtion to Find Ac Lengths nd Sufce Aes. Ac Length Fomul: If f () is continuous on [, b], then the c length of the cuve = f() on the intevl [, b] is given b s

More information

AUTOMATIC WHITE BALANCE FOR DIGITAL STILL CAMERA

AUTOMATIC WHITE BALANCE FOR DIGITAL STILL CAMERA AUTOMATI WHITE ALANE FOR DIGITAL STILL AMERA Tzn-Sheng hiou ( 邱贊生 ), hiou-shnn Fuh ( 傅楸善 ), nd Vsh hikne Detment of omute Science nd Infomtion Engineeing, Ntionl Tiwn Univesity, Tiei, Tiwn. E-mil: fuh@csie.ntu.edu.tw

More information

THEORY OF EQUATIONS OBJECTIVE PROBLEMS. If the eqution x 6x 0 0 ) - ) 4) -. If the sum of two oots of the eqution k is -48 ) 6 ) 48 4) 4. If the poduct of two oots of 4 ) -4 ) 4) - 4. If one oot of is

More information

Language Processors F29LP2, Lecture 5

Language Processors F29LP2, Lecture 5 Lnguge Pocessos F29LP2, Lectue 5 Jmie Gy Feuy 2, 2014 1 / 1 Nondeteministic Finite Automt (NFA) NFA genelise deteministic finite utomt (DFA). They llow sevel (0, 1, o moe thn 1) outgoing tnsitions with

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

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

r = (0.250 m) + (0.250 m) r = m = = ( N m / C )

r = (0.250 m) + (0.250 m) r = m = = ( N m / C ) ELECTIC POTENTIAL IDENTIFY: Apply Eq() to clculte the wok The electic potentil enegy of pi of point chges is given y Eq(9) SET UP: Let the initil position of q e point nd the finl position e point, s shown

More information

332:221 Principles of Electrical Engineering I Fall Hourly Exam 2 November 6, 2006

332:221 Principles of Electrical Engineering I Fall Hourly Exam 2 November 6, 2006 2:221 Principles of Electricl Engineering I Fll 2006 Nme of the student nd ID numer: Hourly Exm 2 Novemer 6, 2006 This is closed-ook closed-notes exm. Do ll your work on these sheets. If more spce is required,

More information

St Andrew s Academy Mathematics Department Higher Mathematics VECTORS

St Andrew s Academy Mathematics Department Higher Mathematics VECTORS St ndew s cdemy Mthemtics etment Highe Mthemtics VETORS St ndew's cdemy Mths et 0117 1 Vectos sics 1. = nd = () Sketch the vectos nd. () Sketch the vectos nd. (c) Given u = +, sketch the vecto u. (d) Given

More information

PX3008 Problem Sheet 1

PX3008 Problem Sheet 1 PX38 Poblem Sheet 1 1) A sphee of dius (m) contins chge of unifom density ρ (Cm -3 ). Using Guss' theoem, obtin expessions fo the mgnitude of the electic field (t distnce fom the cente of the sphee) in

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

Andersen s Algorithm. CS 701 Final Exam (Reminder) Friday, December 12, 4:00 6:00 P.M., 1289 Computer Science.

Andersen s Algorithm. CS 701 Final Exam (Reminder) Friday, December 12, 4:00 6:00 P.M., 1289 Computer Science. CS 701 Finl Exm (Reminde) Fidy, Deeme 12, 4:00 6:00 P.M., 1289 Comute Siene. Andesen s Algoithm An lgoithm to uild oints-to gh fo C ogm is esented in: Pogm Anlysis nd Seiliztion fo the C ogmming Lnguge,

More information

Chapter 21: Electric Charge and Electric Field

Chapter 21: Electric Charge and Electric Field Chpte 1: Electic Chge nd Electic Field Electic Chge Ancient Gees ~ 600 BC Sttic electicit: electic chge vi fiction (see lso fig 1.1) (Attempted) pith bll demonsttion: inds of popeties objects with sme

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

Mathematical formulation of the F 0 motor model

Mathematical formulation of the F 0 motor model negy Tnsduction in TP Synthse: Supplement Mthemticl fomultion of the F 0 moto model. Mkov chin model fo the evolution of the oto stte The fou possible potontion sttes of the two oto sp61 sites t the otostto

More information

Math 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013

Math 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013 Mth 4318 : Rel Anlysis II Mid-Tem Exm 1 14 Febuy 2013 Nme: Definitions: Tue/Flse: Poofs: 1. 2. 3. 4. 5. 6. Totl: Definitions nd Sttements of Theoems 1. (2 points) Fo function f(x) defined on (, b) nd fo

More information

Data Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2.

Data Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2. Element Uniqueness Poblem Dt Stuctues Let x,..., xn < m Detemine whethe thee exist i j such tht x i =x j Sot Algoithm Bucket Sot Dn Shpi Hsh Tbles fo (i=;i

More information

s c s (b) Hence, show that the entropy for rubber-like materials must have the separable form

s c s (b) Hence, show that the entropy for rubber-like materials must have the separable form EN: Continuum Mechnics Homewok 6: Aliction of continuum mechnics to elstic solids Due Decembe th, School of Engineeing Bown Univesity. Exeiments show tht ubbe-like mteils hve secific intenl enegy ( ) nd

More information

Chapter 4: Techniques of Circuit Analysis. Chapter 4: Techniques of Circuit Analysis

Chapter 4: Techniques of Circuit Analysis. Chapter 4: Techniques of Circuit Analysis Chpter 4: Techniques of Circuit Anlysis Terminology Node-Voltge Method Introduction Dependent Sources Specil Cses Mesh-Current Method Introduction Dependent Sources Specil Cses Comprison of Methods Source

More information

c( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model

c( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model Relace 85.8.3.2 with the following: 85.8.3.2 Tansmitted outut wavefom The 40GBASE-CR4 and 100GBASE-CR10 tansmit function includes ogammable equalization to comensate fo the fequency-deendent loss of the

More information