Maxwell Equations. Dr. Ray Kwok sjsu

Size: px
Start display at page:

Download "Maxwell Equations. Dr. Ray Kwok sjsu"

Transcription

1 Maxwell quains. Ray Kwk sjsu eeence: lecmagneic Fields and Waves, Lain & Csn (Feeman) Inducin lecdynamics,.. Giihs (Penice Hall) Fundamenals ngineeing lecmagneics,.k. Cheng (Addisn Wesley)

2 Maxwell quains. Ray Kwk lecdynamics ρ ε µ Gauss s Law Faaday s Law N magneic chage Ampee s Law

3 Maxwell quains. Ray Kwk Incnsisence? ( ) div. cul div. k µ µ ( )??? why?

4 Maxwell quains. Ray Kwk Cninuiy quain d ρ((), ) d dρ ρ ρ d ρ dρ ρ d ρ d d ρ v ( ρv) ρ nain (?) cnsevain mae : dρ/d Hee, cnsevain chages. ee, bund, al.

5 Maxwell quains. Ray Kwk Maxwell s wk Gauss s Law Cninuiy qn ρ ( ε ) ε ρ ε Faaday Maxwell µ µ µ ε such ha ε ames Clek Maxwell ( ) ~displacemen cuen densiy

6 Maxwell quains. Ray Kwk Maxwell quains ρ ε µ ε Tgehe wih Lenz Fce Gauss s Law Faaday s Law N magneic chage Mdiied Ampee s Law (Maxwell) F q( v ) descibe all classical elecdynamics in ee space u, wha ae ρ and?

7 Maxwell quains. Ray Kwk In dielecics εεε ε ε P ρ ρ ρ ρ ρ ρ b b P ρ ε ( ) b ρ cninuiy linea, hmgeneus, ispic P bund chage ρ plaizain cuen densiy b P ρ ρ b b ( P)

8 Maxwell quains. Ray Kwk Plaizain cuen P np p I I d I d I N dc cuen because dp/d N ee chage lw m ne side he he.. S. Ne: is he unim beween he plaes. is dieen. is n necessay // inside dielecic!!! (ε is a ens!!) F ac, scillaing diple lks like he chage is cssing he dielecic!!

9 Maxwell quains. Ray Kwk Plaizain cuen AC ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± I

10 Maxwell quains. Ray Kwk In magneic maeials µ Hµ µ Hµ (H M) µ ( H M) m µ m M MχmH µ (Hχ H) µ (1χ )H µ linea, hmgeneus, ispic 1χ m m is he equivalen cuen densiy magneized mae χ m is he magneic suscepibiliy m µ can be < 1 negaive!!! > paamagneic quanum, spin, bial < diamagneic ee e (sceening) >>1 emagneic magne << 1 aniemagneic ec ne: m exiss even in saic ield, bu equie spaial vaiain M

11 Maxwell quains. Ray Kwk Magneizain Cuen e.g. in a peecly magneized 2 maeial, m unim inside and uside. M nm m i ne cuen n he bunday In ealiy, m dn line up peecly and has a spaial vaiain, which pduce a vlume magneizain cuen bund cuen. Again, n ee elecn ansp m ne place anhe in macscpic sense.

12 Maxwell quains. Ray Kwk Tal cuen densiy M P µ ε ε µ ε µ M P M P ( ) µ M Check wih Maxwell s mah M ρ ρ mah cninuiy OK

13 Maxwell quains. Ray Kwk In ems ee chage and cuen ρ da I d H da da d Q da H l l ( ) M H M µ µ n m

14 Maxwell quains. Ray Kwk & H vs. & H is elaed ee cuen depends n maeial & hisy (hyseesis) H is measued when ne builds elecmagnes is elaed ee chages u we measued vlage which is dl n chages Since & H ae wha we measue diecly, hey ae me cmmnly used han &.

15 Maxwell quains. Ray Kwk unday Cndiins 1 2 1n da 1n 1n A 2n Q 2n A σ σ s s A suace chage densiy 2n dl l l da (aea ) same bunday cndiins as in saic case

16 Maxwell quains. Ray Kwk unday Cndiins H 1 2 1n da 1n 1n A 2n 2n A 2n 1 2 nˆ2 H 1 H 2 H nˆ nˆ H dl l H 2 I l sl ( H ) 1 H2 ( H ) 1 H2 s da s same bunday cndiins as in saic case Ne: s nly exiss n cnducs

17 Maxwell quains. Ray Kwk Summay

18 Maxwell quains. Ray Kwk Phas quains One can wie, H,, in ems ime hamnic ields in m : (Fuie) (, ) Re { ()e j } ω The ampliude () is a Vec Phas. The Maxwell quains ( & H) and he cespnding phas m ae: ε ρ H µ H H ε ρ ε jωµ H H H jωε

19 Maxwell quains. Ray Kwk xecise H(, ) xˆ.1cs(9 Wha is, λ,? βz) A/m in vacuum wih n cuen suce. ω 2π 9, 143 Hz λ c/ (3 x 1 8 )/(143) 294 km ppagae he z diecin H jωε () a y j3.77 sin(9 3(1 6 )z) V/m (z) a y 3.77 cs(9 3(1 6 )z) V/m

20 Maxwell quains. Ray Kwk Hmewk (, ) ŷ.1sin(1πx) cs(6π 1 1. Given ha V/m in ai, ind H(,) and β using he phas equains. xˆ 2. An ininie cuen shee 5 A/m cinciding wih he xyplane sepaaes ai (egin 1, z > ) m he medium wih µ 2 2 (egin 2, z < ). Given ha H A/m, ind 1 3xˆ 4ŷ 2ẑ (a) H 2, (b) 2, (c) angle α 1 ha 1 makes wih he zaxis, and (d) angle α 2 ha 2 makes wih he zaxis. 9 βz) 3. A 6 MHz elecmagneic wave exiss in an aidielecic caxial cable having an inne cnduc wih adius a and an ue cnduc wih inne adius b. Assuming peec cnducs, and he phas m he elecic ield inensiy be (a < < b) V/m, (a) ind k, (b) ind H m he, e (c) ind he suace cuen densiies n he inne and ue cnducs. ˆ jωµ H jkz

Fri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields

Fri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields Fi. 0/23 (C4) 4.4. Linea ielectics (ead est at yu discetin) Mn. (C 7) 2..-..2, 2.3. t B; 5..-..2 Lentz Fce Law: fields Wed. and fces Thus. (C 7) 5..3 Lentz Fce Law: cuents Fi. (C 7) 5.2 Bit-Savat Law HW6

More information

Lecture 22 Electromagnetic Waves

Lecture 22 Electromagnetic Waves Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should

More information

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion

More information

r r r r r EE334 Electromagnetic Theory I Todd Kaiser

r r r r r EE334 Electromagnetic Theory I Todd Kaiser 334 lecoagneic Theoy I Todd Kaise Maxwell s quaions: Maxwell s equaions wee developed on expeienal evidence and have been found o goven all classical elecoagneic phenoena. They can be wien in diffeenial

More information

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson ECE Dept. Notes 13

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson ECE Dept. Notes 13 ECE 338 Applied Electicity and Magnetism ping 07 Pof. David R. Jackson ECE Dept. Notes 3 Divegence The Physical Concept Find the flux going outwad though a sphee of adius. x ρ v0 z a y ψ = D nˆ d = D ˆ

More information

Lecture 3. Electrostatics

Lecture 3. Electrostatics Lecue lecsics In his lecue yu will len: Thee wys slve pblems in elecsics: ) Applicin f he Supepsiin Pinciple (SP) b) Applicin f Guss Lw in Inegl Fm (GLIF) c) Applicin f Guss Lw in Diffeenil Fm (GLDF) C

More information

Faraday s Law (continued)

Faraday s Law (continued) Faaday s Law (continued) What causes cuent to flow in wie? Answe: an field in the wie. A changing magnetic flux not only causes an MF aound a loop but an induced electic field. Can wite Faaday s Law: ε

More information

Note: Please use the actual date you accessed this material in your citation.

Note: Please use the actual date you accessed this material in your citation. MIT OpenCuseWae hp://cw.m.edu 6.03/ESD.03J Elecmagnecs and Applcans, Fall 005 Please use he fllwng can fma: Makus Zahn, Ech Ippen, and Davd Saeln, 6.03/ESD.03J Elecmagnecs and Applcans, Fall 005. (Massachuses

More information

11. HAFAT İş-Enerji Power of a force: Power in the ability of a force to do work

11. HAFAT İş-Enerji Power of a force: Power in the ability of a force to do work MÜHENDİSLİK MEKNİĞİ. HFT İş-Eneji Pwe f a fce: Pwe in he abiliy f a fce d wk F: The fce applied n paicle Q P = F v = Fv cs( θ ) F Q v θ Pah f Q v: The velciy f Q ÖRNEK: İŞ-ENERJİ ω µ k v Calculae he pwe

More information

ELECTROSTATIC FIELDS IN MATERIAL MEDIA

ELECTROSTATIC FIELDS IN MATERIAL MEDIA MF LCTROSTATIC FILDS IN MATRIAL MDIA 3/4/07 LCTURS Materials media may be classified in terms f their cnductivity σ (S/m) as: Cnductrs The cnductivity usually depends n temperature and frequency A material

More information

ECE 107: Electromagnetism

ECE 107: Electromagnetism ECE 107: Electromagnetism Set 7: Dynamic fields Instructor: Prof. Vitaliy Lomakin Department of Electrical and Computer Engineering University of California, San Diego, CA 92093 1 Maxwell s equations Maxwell

More information

The Production of Polarization

The Production of Polarization Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview

More information

MEAN GRAVITY ALONG PLUMBLINE. University of New Brunswick, Department of Geodesy and Geomatics Engineering, Fredericton, N.B.

MEAN GRAVITY ALONG PLUMBLINE. University of New Brunswick, Department of Geodesy and Geomatics Engineering, Fredericton, N.B. MEA GRAVITY ALG PLUMBLIE Beh-Anne Main 1, Chis MacPhee, Rbe Tenze 1, Pe Vaníek 1 and Macel Sans 1 1. Inducin 1 Univesiy f ew Bunswick, Depamen f Gedesy and Gemaics Engineeing, Fedeicn,.B., E3B 5A3, Canada

More information

Review Notes on Maxwell's Equations

Review Notes on Maxwell's Equations ELEC344 Micowave Engineeing, Sping 2002 Handout #1 Kevin Chen Review Notes on Maxwell's Equations Review of Vecto Poducts and the Opeato The del, gad o nabla opeato is a vecto, and can be pat of a scala

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is Mon., 3/23 Wed., 3/25 Thus., 3/26 Fi., 3/27 Mon., 3/30 Tues., 3/31 21.4-6 Using Gauss s & nto to Ampee s 21.7-9 Maxwell s, Gauss s, and Ampee s Quiz Ch 21, Lab 9 Ampee s Law (wite up) 22.1-2,10 nto to

More information

Antennas & Propagation

Antennas & Propagation Antennas & Popagation 1 Oveview of Lectue II -Wave Equation -Example -Antenna Radiation -Retaded potential THE KEY TO ANY OPERATING ANTENNA ot H = J +... Suppose: 1. Thee does exist an electic medium,

More information

TUTORIAL 9. Static magnetic field

TUTORIAL 9. Static magnetic field TUTOIAL 9 Static magnetic field Vecto magnetic potential Null Identity % & %$ A # Fist postulation # " B such that: Vecto magnetic potential Vecto Poisson s equation The solution is: " Substitute it into

More information

Physics 1402: Lecture 22 Today s Agenda

Physics 1402: Lecture 22 Today s Agenda Physics 142: ecure 22 Today s Agenda Announcemens: R - RV - R circuis Homework 6: due nex Wednesday Inducion / A curren Inducion Self-Inducance, R ircuis X X X X X X X X X long solenoid Energy and energy

More information

Electromagnetic Waves

Electromagnetic Waves Chapte 3 lectmagnetic Waves 3.1 Maxwell s quatins and ectmagnetic Waves A. Gauss s Law: # clsed suface aea " da Q enc lectic fields may be geneated by electic chages. lectic field lines stat at psitive

More information

The Law of Biot-Savart & RHR P θ

The Law of Biot-Savart & RHR P θ The Law of iot-savat & RHR P R dx x Jean-aptiste iot élix Savat Phys 122 Lectue 19 G. Rybka Recall: Potential Enegy of Dipole Wok equied to otate a cuentcaying loop in a magnetic field Potential enegy

More information

4. Electric field lines with respect to equipotential surfaces are

4. Electric field lines with respect to equipotential surfaces are Pre-es Quasi-saic elecromagneism. The field produced by primary charge Q and by an uncharged conducing plane disanced from Q by disance d is equal o he field produced wihou conducing plane by wo following

More information

March 15. Induction and Inductance Chapter 31

March 15. Induction and Inductance Chapter 31 Mach 15 Inductin and Inductance Chapte 31 > Fces due t B fields Lentz fce τ On a mving chage F B On a cuent F il B Cuent caying cil feels a tque = µ B Review > Cuents geneate B field Bit-Savat law = qv

More information

Lecture 20. Transmission Lines: The Basics

Lecture 20. Transmission Lines: The Basics Lcu 0 Tansmissin Lins: Th Basics n his lcu u will lan: Tansmissin lins Diffn ps f ansmissin lin sucus Tansmissin lin quains Pw flw in ansmissin lins Appndi C 303 Fall 006 Fahan Rana Cnll Univsi Guidd Wavs

More information

Chapter 21: Gauss s Law

Chapter 21: Gauss s Law Chapte : Gauss s Law Gauss s law : intoduction The total electic flux though a closed suface is equal to the total (net) electic chage inside the suface divided by ε Gauss s law is equivalent to Coulomb

More information

Electromagnetic Waves

Electromagnetic Waves Chapte 32 Electomagnetic Waves PowePoint Lectues fo Univesity Physics, Twelfth Edition Hugh D. Young and Roge A. Feedman Lectues by James Pazun Modified P. Lam 8_11_2008 Topics fo Chapte 32 Maxwell s equations

More information

THE MAGNETIC FIELD. This handout covers: The magnetic force between two moving charges. The magnetic field, B, and magnetic field lines

THE MAGNETIC FIELD. This handout covers: The magnetic force between two moving charges. The magnetic field, B, and magnetic field lines EM 005 Handout 7: The Magnetic ield 1 This handout coes: THE MAGNETIC IELD The magnetic foce between two moing chages The magnetic field,, and magnetic field lines Magnetic flux and Gauss s Law fo Motion

More information

3-Axis Vector Magnet: Construction and Characterisation of Split Coils at RT. Semester Project Petar Jurcevic

3-Axis Vector Magnet: Construction and Characterisation of Split Coils at RT. Semester Project Petar Jurcevic 3-Axis Vecto Magnet: Constuction and Chaacteisation of Split Coils at RT Semeste Poject Peta Jucevic Outline Field Calculation and Simulation Constuction Details Field Calculations Chaacteization at RT

More information

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 17

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 17 ECE 634 Intermediate EM Waves Fall 16 Prof. David R. Jacson Dept. of ECE Notes 17 1 General Plane Waves General form of plane wave: E( xz,, ) = Eψ ( xz,, ) where ψ ( xz,, ) = e j( xx+ + zz) The wavenumber

More information

AIR FORCE RESEARCH LABORATORY

AIR FORCE RESEARCH LABORATORY AIR FORC RSARCH LABORATORY The xtinctin Theem as an xample f Reseach Vistas in Mathematical Optics Mach Richad A. Albanese Infmatin Opeatins and Applied Mathematics Human ffectiveness Diectate Bks City-Base

More information

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) , PART A PHYSICS

Prerna Tower, Road No 2, Contractors Area, Bistupur, Jamshedpur , Tel (0657) ,  PART A PHYSICS Pena Towe, oad No, Conacos Aea, isupu, Jamshedpu 83, Tel (657)89, www.penaclasses.com AIEEE PAT A PHYSICS Physics. Two elecic bulbs maked 5 W V and W V ae conneced in seies o a 44 V supply. () W () 5 W

More information

4. Electrodynamic fields

4. Electrodynamic fields 4. Electodynamic fields D. Rakhesh Singh Kshetimayum 1 4.1 Intoduction Electodynamics Faaday s law Maxwell s equations Wave equations Lenz s law Integal fom Diffeential fom Phaso fom Bounday conditions

More information

Lecture 6: Maxwell s Equations, Boundary Conditions.

Lecture 6: Maxwell s Equations, Boundary Conditions. Whites, EE 382 Lecture 6 Page 1 of 7 Lecture 6: Maxwell s Equations, Boundar Conditions. In the last four lectures, we have been investigating the behavior of dnamic (i.e., time varing) electric and magnetic

More information

Review: Electrostatics and Magnetostatics

Review: Electrostatics and Magnetostatics Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion

More information

Chapter Q1. We need to understand Classical wave first. 3/28/2004 H133 Spring

Chapter Q1. We need to understand Classical wave first. 3/28/2004 H133 Spring Chaper Q1 Inroducion o Quanum Mechanics End of 19 h Cenury only a few loose ends o wrap up. Led o Relaiviy which you learned abou las quarer Led o Quanum Mechanics (1920 s-30 s and beyond) Behavior of

More information

Notes 19 Gradient and Laplacian

Notes 19 Gradient and Laplacian ECE 3318 Applied Electricity and Magnetism Spring 218 Prof. David R. Jackson Dept. of ECE Notes 19 Gradient and Laplacian 1 Gradient Φ ( x, y, z) =scalar function Φ Φ Φ grad Φ xˆ + yˆ + zˆ x y z We can

More information

8.022 (E&M) Lecture 13. What we learned about magnetism so far

8.022 (E&M) Lecture 13. What we learned about magnetism so far 8.0 (E&M) Letue 13 Topis: B s ole in Mawell s equations Veto potential Biot-Savat law and its appliations What we leaned about magnetism so fa Magneti Field B Epeiments: uents in s geneate foes on hages

More information

CHAPTER 24 GAUSS LAW

CHAPTER 24 GAUSS LAW CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and

More information

Magnetostatics. Magnetic Forces. = qu. Biot-Savart Law H = Gauss s Law for Magnetism. Ampere s Law. Magnetic Properties of Materials. Inductance M.

Magnetostatics. Magnetic Forces. = qu. Biot-Savart Law H = Gauss s Law for Magnetism. Ampere s Law. Magnetic Properties of Materials. Inductance M. Magnetic Foces Biot-Savat Law Gauss s Law fo Magnetism Ampee s Law Magnetic Popeties of Mateials nductance F m qu d B d R 4 R B B µ 0 J Magnetostatics M. Magnetic Foces The electic field E at a point in

More information

Lecture 4. Electrons and Holes in Semiconductors

Lecture 4. Electrons and Holes in Semiconductors ecue 4 lec ad Hle i Semicduc I hi lecue yu will lea: eeai-ecmbiai i emicduc i me deail The baic e f euai gveig he behavi f elec ad hle i emicduc Shcley uai Quai-eualiy i cducive maeial C 35 Sig 2005 Faha

More information

Chapter 4 AC Network Analysis

Chapter 4 AC Network Analysis haper 4 A Nework Analysis Jaesung Jang apaciance Inducance and Inducion Time-Varying Signals Sinusoidal Signals Reference: David K. heng, Field and Wave Elecromagneics. Energy Sorage ircui Elemens Energy

More information

ELECTRODYNAMICS: PHYS 30441

ELECTRODYNAMICS: PHYS 30441 ELETRODYNAMIS: PHYS 44. Electomagnetic Field Equations. Maxwell s Equations Analysis in space (vacuum). oulomb Bon June 4, 76 Angoulême, Fance Died August 2, 86 Pais, Fance In 785 oulomb pesented his thee

More information

Welcome to Physics 272

Welcome to Physics 272 Welcome to Physics 7 Bob Mose mose@phys.hawaii.edu http://www.phys.hawaii.edu/~mose/physics7.html To do: Sign into Masteing Physics phys-7 webpage Registe i-clickes (you i-clicke ID to you name on class-list)

More information

Non-sinusoidal Signal Generators

Non-sinusoidal Signal Generators Non-sinusoidal Signal Geneaos ecangle, iangle, saw ooh, pulse, ec. Muliibao cicuis: asable no sable saes (wo quasi-sable saes; i emains in each sae fo pedeemined imes) monosable one sable sae, one unsable

More information

Lecture 4. Electrons and Holes in Semiconductors

Lecture 4. Electrons and Holes in Semiconductors Lecue 4 lec ad Hle i Semicduc I hi lecue yu will lea: Geeai-ecmbiai i emicduc i me deail The baic e f euai gveig he behavi f elec ad hle i emicduc Shckley uai Quai-eualiy i cducive maeial C 35 Sig 2005

More information

Electric Charge. Electric charge is quantized. Electric charge is conserved

Electric Charge. Electric charge is quantized. Electric charge is conserved lectstatics lectic Chage lectic chage is uantized Chage cmes in incements f the elementay chage e = ne, whee n is an intege, and e =.6 x 0-9 C lectic chage is cnseved Chage (electns) can be mved fm ne

More information

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes] ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,

More information

Field due to a collection of N discrete point charges: r is in the direction from

Field due to a collection of N discrete point charges: r is in the direction from Physcs 46 Fomula Shee Exam Coulomb s Law qq Felec = k ˆ (Fo example, f F s he elecc foce ha q exes on q, hen ˆ s a un veco n he decon fom q o q.) Elecc Feld elaed o he elecc foce by: Felec = qe (elecc

More information

Course Updates. 2) This week: Electromagnetic Waves +

Course Updates.  2) This week: Electromagnetic Waves + Course Updates http://www.phys.hawaii.edu/~varner/phys272-spr1/physics272.html Reminders: 1) Assignment #11 due Wednesday 2) This week: Electromagnetic Waves + 3) In the home stretch [review schedule]

More information

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission

More information

Your Comments. Do we still get the 80% back on homework? It doesn't seem to be showing that. Also, this is really starting to make sense to me!

Your Comments. Do we still get the 80% back on homework? It doesn't seem to be showing that. Also, this is really starting to make sense to me! You Comments Do we still get the 8% back on homewok? It doesn't seem to be showing that. Also, this is eally stating to make sense to me! I am a little confused about the diffeences in solid conductos,

More information

F = net force on the system (newton) F,F and F. = different forces working. E = Electric field strength (volt / meter)

F = net force on the system (newton) F,F and F. = different forces working. E = Electric field strength (volt / meter) All the Impotant Fomulae that a student should know fom. XII Physics Unit : CHAPTER - ELECTRIC CHARGES AND FIELD CHAPTER ELECTROSTATIC POTENTIAL AND CAPACITANCE S. Fomula No.. Quantization of chage Q =

More information

Chapter 6. Dielectrics and Capacitance

Chapter 6. Dielectrics and Capacitance Chapter 6. Dielectrics and Capacitance Hayt; //009; 6- Dielectrics are insulating materials with n free charges. All charges are bund at mlecules by Culmb frce. An applied electric field displaces charges

More information

Physics 442. Electro-Magneto-Dynamics. M. Berrondo. Physics BYU

Physics 442. Electro-Magneto-Dynamics. M. Berrondo. Physics BYU Physis 44 Eleo-Magneo-Dynamis M. Beondo Physis BYU Paaveos Φ= V + Α Φ= V Α = = + J = + ρ J J ρ = J S = u + em S S = u em S Physis BYU Poenials Genealize E = V o he ime dependen E & B ase Podu of paaveos:

More information

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant. ANTNNAS Vecto and Scala Potentials Maxwell's quations jωb J + jωd D ρ B (M) (M) (M3) (M4) D ε B Fo a linea, homogeneous, isotopic medium and ε ae contant. Since B, thee exists a vecto A such that B A and

More information

Current, Resistance and

Current, Resistance and Cuent, Resistance and Electomotive Foce Chapte 25 Octobe 2, 2012 Octobe 2, 2012 Physics 208 1 Leaning Goals The meaning of electic cuent, and how chages move in a conducto. What is meant by esistivity

More information

Review. Electrostatic. Dr. Ray Kwok SJSU

Review. Electrostatic. Dr. Ray Kwok SJSU Review Electostatic D. Ray Kwok SJSU Paty Balloons Coulomb s Law F e q q k 1 Coulomb foce o electical foce. (vecto) Be caeful on detemining the sign & diection. k 9 10 9 (N m / C ) k 1 4πε o k is the Coulomb

More information

Gauss s Law: Circuits

Gauss s Law: Circuits Gauss s Law: Cicuits Can we have excess chage inside in steady state? E suface nˆ A q inside E nˆ A E nˆ A left _ suface ight _ suface q inside 1 Gauss s Law: Junction Between two Wies n 2

More information

5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement:

5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement: 5/0/011 Chapte 5 In the last lectue: CapacitanceII we calculated the capacitance C f a system f tw islated cnducts. We als calculated the capacitance f sme simple gemeties. In this chapte we will cve the

More information

Ferromagnetism. So that once magnetized the material will stay that way even in the absence of external current it is a permanent magnet.

Ferromagnetism. So that once magnetized the material will stay that way even in the absence of external current it is a permanent magnet. Ferroagnetis We now turn to the case where is not proportional to. We distinguish two cases: soft and hard ferroagnets. In a soft ferroagnet a graph of vs looks like If is now reduced, will retrace the

More information

TECHNO INDIA BATANAGAR

TECHNO INDIA BATANAGAR TECHNO INDIA BATANAGAR ( DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING) QUESTION BANK- 2018 1.Vector Calculus Assistant Professor 9432183958.mukherjee@tib.edu.in 1. When the operator operates on

More information

β A Constant-G m Biasing

β A Constant-G m Biasing p 2002 EE 532 Anal IC Des II Pae 73 Cnsan-G Bas ecall ha us a PTAT cuen efeence (see p f p. 66 he nes) bas a bpla anss pes cnsan anscnucance e epeaue (an als epenen f supply lae an pcess). Hw h we achee

More information

Maxwell s Equations and Electromagnetic Waves

Maxwell s Equations and Electromagnetic Waves Phsics 36: Waves Lecure 3 /9/8 Maxwell s quaions and lecromagneic Waves Four Laws of lecromagneism. Gauss Law qenc all da ρdv Inegral From From he vecor ideni da dv Therefore, we ma wrie Gauss Law as ρ

More information

σ = neμ = v D = E H, the Hall Field B Z E Y = ee y Determining n and μ: The Hall Effect V x, E x I, J x E y B z F = qe + qv B F y

σ = neμ = v D = E H, the Hall Field B Z E Y = ee y Determining n and μ: The Hall Effect V x, E x I, J x E y B z F = qe + qv B F y Detemining n and μ: The Hall Effect V x, E x + + + + + + + + + + + --------- E y I, J x F = qe + qv B F y = ev D B z F y = ee y B z In steady state, E Y = v D B Z = E H, the Hall Field Since v D =-J x

More information

Consider a Binary antipodal system which produces data of δ (t)

Consider a Binary antipodal system which produces data of δ (t) Modulaion Polem PSK: (inay Phae-hi keying) Conide a inay anipodal yem whih podue daa o δ ( o + δ ( o inay and epeively. Thi daa i paed o pule haping ile and he oupu o he pule haping ile i muliplied y o(

More information

( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II.

( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II. Homewok #8. hapte 7 Magnetic ields. 6 Eplain how ou would modif Gauss s law if scientists discoveed that single, isolated magnetic poles actuall eisted. Detemine the oncept Gauss law fo magnetism now eads

More information

2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields

2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields Magnets and Magnetic ields Magnetism Howee, if you cut a magnet in half, you don t get a noth pole and a south pole you get two smalle magnets. ectue otes Chapte 20 Topics Magnets and Magnetic ields Magnets

More information

Unit 7: Sources of magnetic field

Unit 7: Sources of magnetic field Unit 7: Souces of magnetic field Oested s expeiment. iot and Savat s law. Magnetic field ceated by a cicula loop Ampèe s law (A.L.). Applications of A.L. Magnetic field ceated by a: Staight cuent-caying

More information

Lecture 2 Review of Maxwell s Equations and the EM Constitutive Parameters

Lecture 2 Review of Maxwell s Equations and the EM Constitutive Parameters Lecture 2 Review of Maxwell s Equations and the EM Constitutive Parameters Optional Reading: Steer Appendix D, or Pozar Section 1.2,1.6, or any text on Engineering Electromagnetics (e.g., Hayt/Buck) Time-domain

More information

a. (1) Assume T = 20 ºC = 293 K. Apply Equation 2.22 to find the resistivity of the brass in the disk with

a. (1) Assume T = 20 ºC = 293 K. Apply Equation 2.22 to find the resistivity of the brass in the disk with Aignmen #5 EE7 / Fall 0 / Aignmen Sluin.7 hermal cnducin Cnider bra ally wih an X amic fracin f Zn. Since Zn addiin increae he number f cnducin elecrn, we have cale he final ally reiiviy calculaed frm

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 1

ECE Spring Prof. David R. Jackson ECE Dept. Notes 1 ECE 6341 Spring 16 Prof. David R. Jackson ECE Dept. Notes 1 1 Fields in a Source-Free Region Sources Source-free homogeneous region ( ε, µ ) ( EH, ) Note: For a lossy region, we replace ε ε c ( / ) εc

More information

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can. 1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule

More information

Physics Spring 2012 Announcements: Mar 07, 2012

Physics Spring 2012 Announcements: Mar 07, 2012 Physics 00 - Sping 01 Announcements: Ma 07, 01 HW#6 due date has been extended to the moning of Wed. Ma 1. Test # (i. Ma ) will cove only chaptes 0 and 1 All of chapte will be coveed in Test #4!!! Test

More information

Sources of the Magnetic Field. Moving charges currents Ampere s Law Gauss Law in magnetism Magnetic materials

Sources of the Magnetic Field. Moving charges currents Ampere s Law Gauss Law in magnetism Magnetic materials Souces of the Magnetic Field Moving chages cuents Ampee s Law Gauss Law in magnetism Magnetic mateials Biot-Savat Law ˆ ˆ θ ds P db out I db db db db ds ˆ 1 I P db in db db ds sinθ db μ 4 π 0 Ids ˆ B μ0i

More information

PHYS PRACTICE EXAM 2

PHYS PRACTICE EXAM 2 PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,

More information

ELEG 205 Fall Lecture #10. Mark Mirotznik, Ph.D. Professor The University of Delaware Tel: (302)

ELEG 205 Fall Lecture #10. Mark Mirotznik, Ph.D. Professor The University of Delaware Tel: (302) EEG 05 Fall 07 ecure #0 Mark Mirznik, Ph.D. Prfessr The Universiy f Delaware Tel: (3083-4 Email: mirzni@ece.udel.edu haper 7: apacirs and Inducrs The apacir Symbl Wha hey really lk like The apacir Wha

More information

Orthotropic Materials

Orthotropic Materials Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε

More information

A 1. EN2210: Continuum Mechanics. Homework 7: Fluid Mechanics Solutions

A 1. EN2210: Continuum Mechanics. Homework 7: Fluid Mechanics Solutions EN10: Continuum Mechanics Homewok 7: Fluid Mechanics Solutions School of Engineeing Bown Univesity 1. An ideal fluid with mass density ρ flows with velocity v 0 though a cylindical tube with cosssectional

More information

A moving charged particle creates a magnetic field vector at every point in space except at its position.

A moving charged particle creates a magnetic field vector at every point in space except at its position. 1 Pat 3: Magnetic Foce 3.1: Magnetic Foce & Field A. Chaged Paticles A moving chaged paticle ceates a magnetic field vecto at evey point in space ecept at its position. Symbol fo Magnetic Field mks units

More information

ANGULAR MOMENTUM. We have seen that when the system is rotated through an angle about an axis α the unitary operator producing the change is

ANGULAR MOMENTUM. We have seen that when the system is rotated through an angle about an axis α the unitary operator producing the change is ANGULAR MOMENTUM We have seen that when the system is rotated through an angle about an ais α the unitary operator producing the change is U i J e Where J is a pseudo vector obeying the commutation relations

More information

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson Dept. Of ECE. Notes 20 Dielectrics

ECE 3318 Applied Electricity and Magnetism. Spring Prof. David R. Jackson Dept. Of ECE. Notes 20 Dielectrics ECE 3318 Applied Electicity and Magnetism Sping 218 Pof. David R. Jackson Dept. Of ECE Notes 2 Dielectics 1 Dielectics Single H 2 O molecule: H H Wate ε= εε O 2 Dielectics (cont.) H H Wate ε= εε O Vecto

More information

Preliminary Examination - Day 1 Thursday, May 10, 2018

Preliminary Examination - Day 1 Thursday, May 10, 2018 UNL - Department of Physics and Astronomy Preliminary Examination - Day Thursday, May, 28 This test covers the topics of Classical Mechanics (Topic ) and Electrodynamics (Topic 2). Each topic has 4 A questions

More information

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem) Week 1 Lecure Problems, 5 Wha if somehing oscillaes wih no obvious spring? Wha is ω? (problem se problem) Sar wih Try and ge o SHM form E. Full beer can in lake, oscillaing F = m & = ge rearrange: F =

More information

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion

More information

Reflection/Refraction

Reflection/Refraction Reflection/Refraction Page Reflection/Refraction Boundary Conditions Interfaces between different media imposed special boundary conditions on Maxwell s equations. It is important to understand what restrictions

More information

Electromagnetic Theory (Hecht Ch. 3)

Electromagnetic Theory (Hecht Ch. 3) Phys 531 Lecture 2 30 August 2005 Electromagnetic Theory (Hecht Ch. 3) Last time, talked about waves in general wave equation: 2 ψ(r, t) = 1 v 2 2 ψ t 2 ψ = amplitude of disturbance of medium For light,

More information

1 Spherical multipole moments

1 Spherical multipole moments Jackson notes 9 Spheical multipole moments Suppose we have a chage distibution ρ (x) wheeallofthechageiscontained within a spheical egion of adius R, as shown in the diagam. Then thee is no chage in the

More information

An o5en- confusing point:

An o5en- confusing point: An o5en- confusing point: Recall this example fom last lectue: E due to a unifom spheical suface chage, density = σ. Let s calculate the pessue on the suface. Due to the epulsive foces, thee is an outwad

More information

Refocusing t. Small Tip Angle Example. Small Tip Angle Example. Bioengineering 280A Principles of Biomedical Imaging. Fall Quarter 2010 MRI Lecture 5

Refocusing t. Small Tip Angle Example. Small Tip Angle Example. Bioengineering 280A Principles of Biomedical Imaging. Fall Quarter 2010 MRI Lecture 5 Bioengineering 280A Principles of Biomedical Imaging Fall Quarer 2010 MRI Lecure 5 RF N random seps of lengh d Refocusing ' M xy (,) = jm 0 "B 1 ()exp( jk(,))d %& 100 seps This has he 2D form random of

More information

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b.

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b. Solutions. Plum Pudding Model (a) Find the coesponding electostatic potential inside and outside the atom. Fo R The solution can be found by integating twice, 2 V in = ρ 0 ε 0. V in = ρ 0 6ε 0 2 + a 2

More information

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2! Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,

More information

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 6

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 6 ECE 6340 Intermediate EM Waves Fall 016 Prof. David R. Jackson Dept. of ECE Notes 6 1 Power Dissipated by Current Work given to a collection of electric charges movg an electric field: ( qe ) ( ρ S E )

More information

Course Updates. Reminders: 1) Assignment #8 will be able to do after today. 2) Finish Chapter 28 today. 3) Quiz next Friday

Course Updates. Reminders: 1) Assignment #8 will be able to do after today. 2) Finish Chapter 28 today. 3) Quiz next Friday Couse Updates http://www.phys.hawaii.edu/~vane/phys272-sp10/physics272.html Remindes: 1) Assignment #8 will be able to do afte today 2) Finish Chapte 28 today 3) Quiz next Fiday 4) Review of 3 ight-hand

More information

Spin echo. ½πI x -t -πi y -t

Spin echo. ½πI x -t -πi y -t y Spin echo ½πI - -πi y - : as needed, no correlaed wih 1/J. Funcions: 1. refocusing; 2. decoupling. Chemical shif evoluion is refocused by he spin-echo. Heeronuclear J-couplings evoluion are refocused

More information

ELECTROMAGNETIC FIELDS AT BOUNDARIES

ELECTROMAGNETIC FIELDS AT BOUNDARIES ELECTROMGNETIC FIELDS T BOUNDRIES Differential Form of Maxwell s Equations: E = B t, H = J + D t D = ρ, B = 0 Gauss s Divergene Theorem: ( ) v Ddv = D nda ˆ s Stoke s Theorem: ( G) nda ˆ = î G ds S da

More information

Today s Plan. Electric Dipoles. More on Gauss Law. Comment on PDF copies of Lectures. Final iclicker roll-call

Today s Plan. Electric Dipoles. More on Gauss Law. Comment on PDF copies of Lectures. Final iclicker roll-call Today s Plan lectic Dipoles Moe on Gauss Law Comment on PDF copies of Lectues Final iclicke oll-call lectic Dipoles A positive (q) and negative chage (-q) sepaated by a small distance d. lectic dipole

More information

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 1

ECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 1 EE 6340 Intermediate EM Waves Fall 2016 Prof. David R. Jackson Dept. of EE Notes 1 1 Maxwell s Equations E D rt 2, V/m, rt, Wb/m T ( ) [ ] ( ) ( ) 2 rt, /m, H ( rt, ) [ A/m] B E = t (Faraday's Law) D H

More information

CSE590B Lecture 4 More about P 1

CSE590B Lecture 4 More about P 1 SE590 Lece 4 Moe abo P 1 Tansfoming Tansfomaions James. linn Jimlinn.om h://coses.cs.washingon.ed/coses/cse590b/13a/ Peviosly On SE590b Tansfomaions M M w w w w w The ncion w w w w w w 0 w w 0 w 0 w The

More information

Phy 213: General Physics III

Phy 213: General Physics III Phy 1: Geneal Physics III Chapte : Gauss Law Lectue Ntes E Electic Flux 1. Cnside a electic field passing thugh a flat egin in space w/ aea=a. The aea vect ( A ) with a magnitude f A and is diected nmal

More information

Introduction to AC Power, RMS RMS. ECE 2210 AC Power p1. Use RMS in power calculations. AC Power P =? DC Power P =. V I = R =. I 2 R. V p.

Introduction to AC Power, RMS RMS. ECE 2210 AC Power p1. Use RMS in power calculations. AC Power P =? DC Power P =. V I = R =. I 2 R. V p. ECE MS I DC Power P I = Inroducion o AC Power, MS I AC Power P =? A Solp //9, // // correced p4 '4 v( ) = p cos( ω ) v( ) p( ) Couldn' we define an "effecive" volage ha would allow us o use he same relaionships

More information