4/16/2014. PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107
|
|
- Bruce Carpenter
- 5 years ago
- Views:
Transcription
1 PHY 71 Elctroynmics 1-1:5 AM MWF Olin 17 Pln for ctur 3: Spcil Topics in Elctroynmics: Elctromgntic spcts of suprconuctivity -- continu 4/14/14 PHY 71 Spring ctur 3 1 4/14/14 PHY 71 Spring ctur 3 4/14/14 PHY 71 Spring ctur 3 3 1
2 4/14/14 PHY 71 Spring ctur 3 4 Bhvior of suprconucting mtril clusion of mgntic fil ccoring to th onon mol mc Pntrtion lngth for suprconuctor: 4 n / B (, t) B (, t) z z Vctor potntil for A : A yˆ Ay ( ) Ay ( ) Bz ( ) n / Currnt nsity: J y ( ) B z () mc n n J A or mv A = mc m c / Typiclly, 1 7 m 4/14/14 PHY 71 Spring ctur 3 5 Mgntiztion fil Trting onon currnt in trms of corrsponing mgntiztion fil M: B= H 4 M For, H 4 M Gibbs fr nrgy ssocit with mgntiztion for suprconuctor: H 1 GS ( H ) GS ( H ) HM ( H ) G () S H 8 Gibbs fr nrgy ssocit with mgntiztion for norml conuctor: G ( H ) G ( H ) N N Conition t phs bounry btwn norml n suprconucting stts: 1 GN ( HC ) GN () GS ( HC ) GS () HC 8 1 GS () GN () HC 8 1 H H for H H GS ( H ) GN ( H ) 8 for H H C C C 4/14/14 PHY 71 Spring ctur 3 6
3 Mgntiztion fil (for typ I suprconuctor) B -4M H C H G S -G N H C H C H H 4/14/14 PHY 71 Spring ctur 3 7 Empls of typ I suprconuctors 4/14/14 PHY 71 Spring ctur 3 8 4/14/14 PHY 71 Spring ctur 3 9 3
4 Josphson junction -- tunnling currnt btwn two suprconuctors B z 4/14/14 PHY 71 Spring ctur 3 1 Josphson junction -- continu Suprcon lft Junction Suprcon right B z ( /)/ B / Bz ( ) B / / ( /)/ B / 4/14/14 PHY 71 Spring ctur 3 11 Josphson junction -- continu Suprcon lft Junction Suprcon right A y ( /)/ B / / Ay ( ) B / / ( /)/ B / / 4/14/14 PHY 71 Spring ctur 3 1 4
5 Josphson junction -- continu Quntum mchnicl mol of tunnlling currnt t i t E i i i t t not wvfunction for Coopr pir on lft not wvfunction for Coopr pir on right E 4/14/14 PHY 71 Spring ctur 3 13 Josphson junction -- continu Solving for wvfunctions 1 i i i E t t 1 i i i E t t n n n n ( nn) sin t t E n cos t n E n cos t n 4/14/14 PHY 71 Spring ctur 3 14 Josphson junction -- continu n 4 Tunnling currnt: JT ( nn ) sin t E E If n = n n in bsns of mgntic fil, ( t) () t J J J A m c J A m c ltionship btwn suprconuctor currnts J n J n tunnling currnt. Within th suprconuctor, not th gnrliz currnt oprtor cting on pir wvfunction 1 vˆ i A m c i * * with currnt J vˆ vˆ 4/14/14 PHY 71 Spring ctur
6 Josphson junction -- continu J J J A nv m A nv J m c mv mv A A c c n 4 Tunnling currnt: JT ( nn) sin t N to vlut in prsnc of mgntic fil 4/14/14 PHY 71 Spring ctur 3 16 c Josphson junction -- continu J J m v mv A A c c cll tht for v n A / B yˆ for v n A / B yˆ Intgrting th iffrnc of th phs ngls lon g y : B ( ) y 4 Tunnling currnt: JT ( nn ) sin 4/14/14 PHY 71 Spring ctur 3 17 Josphson junction -- continu J J Intgrting th iffrnc of th phs ngls long y : ( ) 4 Tunnling currnt B nsity: y JT n sin Intgrting currnt nsity throughout with w of suprconuctors w/ sin( T h T y T sin( ) / w/ I J hwj whr B w( ) n / ) c 4/14/14 PHY 71 Spring ctur
Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:
Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin
More informationPHYS ,Fall 05, Term Exam #1, Oct., 12, 2005
PHYS1444-,Fall 5, Trm Exam #1, Oct., 1, 5 Nam: Kys 1. circular ring of charg of raius an a total charg Q lis in th x-y plan with its cntr at th origin. small positiv tst charg q is plac at th origin. What
More informationI. The Connection between Spectroscopy and Quantum Mechanics
I. Th Connction twn Spctroscopy nd Quntum Mchnics On of th postults of quntum mchnics: Th stt of systm is fully dscrid y its wvfunction, Ψ( r1, r,..., t) whr r 1, r, tc. r th coordints of th constitunt
More informationChem 104A, Fall 2016, Midterm 1 Key
hm 104A, ll 2016, Mitrm 1 Ky 1) onstruct microstt tl for p 4 configurtion. Pls numrt th ms n ml for ch lctron in ch microstt in th tl. (Us th formt ml m s. Tht is spin -½ lctron in n s oritl woul writtn
More informationLecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9
Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:
More informationSOLVED EXAMPLES. be the foci of an ellipse with eccentricity e. For any point P on the ellipse, prove that. tan
LOCUS 58 SOLVED EXAMPLES Empl Lt F n F th foci of n llips with ccntricit. For n point P on th llips, prov tht tn PF F tn PF F Assum th llips to, n lt P th point (, sin ). P(, sin ) F F F = (-, 0) F = (,
More information/ / MET Day 000 NC1^ INRTL MNVR I E E PRE SLEEP K PRE SLEEP R E
05//0 5:26:04 09/6/0 (259) 6 7 8 9 20 2 22 2 09/7 0 02 0 000/00 0 02 0 04 05 06 07 08 09 0 2 ay 000 ^ 0 X Y / / / / ( %/ ) 2 /0 2 ( ) ^ 4 / Y/ 2 4 5 6 7 8 9 2 X ^ X % 2 // 09/7/0 (260) ay 000 02 05//0
More informationHowever, many atoms can combine to form particular molecules, e.g. Chlorine (Cl) and Sodium (Na) atoms form NaCl molecules.
Lctur 6 Titl: Fundmntls of th Quntum Thory of molcul formtion Pg- In th lst modul, w hv discussd out th tomic structur nd tomic physics to undrstnd th spctrum of toms. Howvr, mny toms cn comin to form
More information(Semi)Classical thermionic emission
Tunnling - primr Nno oftn pprs in rl tchnology in th form of thin lyrs or brrirs. W r going to look t svrl wys lctrons cn trnsport ovr or through ths brrirs undr vrious conditions. Thrmionic mission clssicl
More informationY 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall
Staning Wav Intrfrnc btwn th incint & rflct wavs Staning wav A string with on n fix on a wall Incint: y, t) Y cos( t ) 1( Y 1 ( ) Y (St th incint wav s phas to b, i.., Y + ral & positiv.) Rflct: y, t)
More informationPHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101. Plan for Lecture 4:
PHY 114 A Gnral Physics II 11 AM-1:15 PM TR Olin 101 Plan for Lctur 4: 1. Introuction to th lctric potntial.rlationship btwn th lctric potntial an th lctric fil 1/31/01 PHY 114 A Spring 01 -- Lctur 4 1
More informationWeek 7: Ch. 11 Semiconductor diodes
Wk 7: Ch. 11 Smiconductor diods Principls o Scintilltion Countrs Smiconductor Diods bsics o smiconductors pur lmnts & dopnts 53 Mtrils ion collction, lkg currnt diod structur, pn, np junctions dpltion
More informationTHE SPINOR FIELD THEORY OF THE PHOTON
Romnin Rports in Physics, Vol. 66, No., P. 9 5, 4 THE SPINOR FIELD THEORY OF THE PHOTON RUO PENG WANG Pking Univrsity, Physics Dprtmnt, Bijing 87, P.R. Chin E-mil: rpwng@pku.du.cn Rcivd Octobr 8, Abstrct.
More informationThis Week. Computer Graphics. Introduction. Introduction. Graphics Maths by Example. Graphics Maths by Example
This Wk Computr Grphics Vctors nd Oprtions Vctor Arithmtic Gomtric Concpts Points, Lins nd Plns Eploiting Dot Products CSC 470 Computr Grphics 1 CSC 470 Computr Grphics 2 Introduction Introduction Wh do
More informationSPH4U Electric Charges and Electric Fields Mr. LoRusso
SPH4U lctric Chargs an lctric Fils Mr. LoRusso lctricity is th flow of lctric charg. Th Grks first obsrv lctrical forcs whn arly scintists rubb ambr with fur. Th notic thy coul attract small bits of straw
More informationSection 3: Antiderivatives of Formulas
Chptr Th Intgrl Appli Clculus 96 Sction : Antirivtivs of Formuls Now w cn put th is of rs n ntirivtivs togthr to gt wy of vluting finit intgrls tht is ct n oftn sy. To vlut finit intgrl f(t) t, w cn fin
More informationME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören
ME 522 PINCIPLES OF OBOTICS FIST MIDTEM EXAMINATION April 9, 202 Nm Lst Nm M. Kml Özgörn 2 4 60 40 40 0 80 250 USEFUL FOMULAS cos( ) cos cos sin sin sin( ) sin cos cos sin sin y/ r, cos x/ r, r 0 tn 2(
More informationWORKSHOP 6 BRIDGE TRUSS
WORKSHOP 6 BRIDGE TRUSS WS6-2 Workshop Ojtivs Lrn to msh lin gomtry to gnrt CBAR lmnts Bom fmilir with stting up th CBAR orinttion vtor n stion proprtis Lrn to st up multipl lo ss Lrn to viw th iffrnt
More informationHandout 28. Ballistic Quantum Transport in Semiconductor Nanostructures
Hanout 8 Ballisti Quantum Transport in Smionutor Nanostruturs In this ltur you will larn: ltron transport without sattring (ballisti transport) Th quantum o onutan an th quantum o rsistan Quanti onutan
More information(A) the function is an eigenfunction with eigenvalue Physical Chemistry (I) First Quiz
96- Physcl Chmstry (I) Frst Quz lctron rst mss m 9.9 - klogrm, Plnck constnt h 6.66-4 oul scon Sp of lght c. 8 m/s, lctron volt V.6-9 oul. Th functon F() C[cos()+sn()] s n gnfuncton of /. Th gnvlu s (A)
More informationLecture 6 Thermionic Engines
Ltur 6 hrmioni ngins Rviw Rihrdson formul hrmioni ngins Shotty brrir nd diod pn juntion nd diod disussion.997 Copyright Gng Chn, MI For.997 Dirt Solr/hrml to ltril nrgy Convrsion WARR M. ROHSOW HA AD MASS
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 8: Effect of a Vertical Field on Tokamak Equilibrium
.65, MHD Thory of usion Systms Prof. ridrg Lctur 8: Effct of Vrticl ild on Tokmk Equilirium Toroidl orc lnc y Mns of Vrticl ild. Lt us riw why th rticl fild is imortnt. 3. or ry short tims, th cuum chmr
More informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 301 Signls & Systms Pf. Mk Fwl Discussin #1 Cmplx Numbs nd Cmplx-Vlud Functins Rding Assignmnt: Appndix A f Kmn nd Hck Cmplx Numbs Cmplx numbs is s ts f plynmils. Dfinitin f imginy # j nd sm sulting
More informationMulti-Section Coupled Line Couplers
/0/009 MultiSction Coupld Lin Couplrs /8 Multi-Sction Coupld Lin Couplrs W cn dd multipl coupld lins in sris to incrs couplr ndwidth. Figur 7.5 (p. 6) An N-sction coupld lin l W typiclly dsign th couplr
More informationIntegration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals
Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion
More informationConsider a potential problem in the half-space dened by z 0, with Dirichlet boundary conditions on the plane z = 0 (and at innity).
Problem.7 Consier otentil roblem in the hlf-sce ene by z 0, with Dirichlet bounry conitions on the lne z 0 (n t innity)..7.. Write own the rorite Green function G(~x; ~x 0 ). G D (~x; ~x 0 ) (x x 0 ) (x
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationMore Foundations. Undirected Graphs. Degree. A Theorem. Graphs, Products, & Relations
Mr Funtins Grphs, Pruts, & Rltins Unirt Grphs An unirt grph is pir f 1. A st f ns 2. A st f gs (whr n g is st f tw ns*) Friy, Sptmr 2, 2011 Ring: Sipsr 0.2 ginning f 0.4; Stughtn 1.1.5 ({,,,,}, {{,}, {,},
More informationDeepak Rajput
Q Prov: (a than an infinit point lattic is only capabl of showing,, 4, or 6-fold typ rotational symmtry; (b th Wiss zon law, i.. if [uvw] is a zon axis and (hkl is a fac in th zon, thn hu + kv + lw ; (c
More informationELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware
LG 43 Lctur #6 Mrk Mirtnik, Ph.D. Prfssr Th Univrsity f Dlwr mil: mirtni@c.udl.du Wv Prpgtin nd Plritin TM: Trnsvrs lctrmgntic Wvs A md is prticulr fild cnfigurtin. Fr givn lctrmgntic bundry vlu prblm,
More informationI i o z t a io n c r u re t f t a l e φ.
E ngrg Pysics:PHY S JB Institut Tcnology D EPARTMENT OF PHYSICS S olutions Qustion Bnk UNIT-I M ODERN PHYSICS J un/july 9. ( 4 Mrks i An lctron n pron r cclrt troug sm potntil. rtio - B rogli wvlngt A
More informationfiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
Solid Stte Physics JEST-0 Q. bem of X-rys is incident on BCC crystl. If the difference between the incident nd scttered wvevectors is K nxˆkyˆlzˆ where xˆ, yˆ, zˆ re the unit vectors of the ssocited cubic
More informationWalk Like a Mathematician Learning Task:
Gori Dprtmnt of Euction Wlk Lik Mthmticin Lrnin Tsk: Mtrics llow us to prform mny usful mthmticl tsks which orinrily rquir lr numbr of computtions. Som typs of problms which cn b on fficintly with mtrics
More informationModule 8 Non equilibrium Thermodynamics
Modul 8 Non quilibrium hrmodynamics ctur 8.1 Basic Postulats NON-EQUIIRIBIUM HERMODYNAMICS Stady Stat procsss. (Stationary) Concpt of ocal thrmodynamic qlbm Extnsiv proprty Hat conducting bar dfin proprtis
More informationFundamentals of Continuum Mechanics. Seoul National University Graphics & Media Lab
Fndmntls of Contnm Mchncs Sol Ntonl Unvrsty Grphcs & Md Lb Th Rodmp of Contnm Mchncs Strss Trnsformton Strn Trnsformton Strss Tnsor Strn T + T ++ T Strss-Strn Rltonshp Strn Enrgy FEM Formlton Lt s Stdy
More informationTheoretical Study on the While Drilling Electromagnetic Signal Transmission of Horizontal Well
7 nd ntrntionl Confrnc on Softwr, Multimdi nd Communiction Enginring (SMCE 7) SBN: 978--6595-458-5 Thorticl Study on th Whil Drilling Elctromgntic Signl Trnsmission of Horizontl Wll Y-huo FAN,,*, Zi-ping
More informationa 1and x is any real number.
Calcls Nots Eponnts an Logarithms Eponntial Fnction: Has th form y a, whr a 0, a an is any ral nmbr. Graph y, Graph y ln y y Th Natral Bas (Elr s nmbr): An irrational nmbr, symboliz by th lttr, appars
More informationSolution to Exercise 2
Department of physics, NTNU TFY Mesoscopic Physics Spring Solution to xercise Question Apart from an adjustable constant, the nearest neighbour nn) tight binding TB) band structure for the D triangular
More informationELECTROMAGNETIC COMPATIBILITY HANDBOOK 1. Chapter 30: Antennas
ELECTROMAGNETIC COMATIBILITY HANDBOOK 1 Chaptr 30: Antnnas 30.1 Can a lump-circuit mol b us to rprsnt an lctrically-larg ipol? If ys, inicat whn. If no, why is it rprsnt by a raiation rsistanc an ractanc?
More informationENTHUSIAST, LEADER & ACHIEVER COURSE TARGET : PRE-MEDICAL 2016 Test Type : MAJOR Test Pattern : AIPMT
LSSROO ONTT PROGRE (cdmic Sssion : 0-06) ENTHUSIST, LEDER & HIEER OURSE TRGET : PRE-EDIL 06 Tst Typ : JOR Tst Pttrn : IPT. omponnt of x on y xcos x y ( b) ( b) y b b b. J E I. x.0 cos(t + ).0 cost locity
More informationHow much air is required by the people in this lecture theatre during this lecture?
3 NTEGRATON tgrtio is us to swr qustios rltig to Ar Volum Totl qutity such s: Wht is th wig r of Boig 747? How much will this yr projct cost? How much wtr os this rsrvoir hol? How much ir is rquir y th
More informationMSC Studentenwettbewerb. Wintersemester 2012/13. Nastran - Patran
MSC Stuntnwttwr Wintrsmstr 2012/13 Nstrn - Ptrn Aufg Wi groß ist i mximl Vrshiung? Softwr Vrsion Ptrn 2011 MSC/MD Nstrn 2011 Fils Rquir strut.xmt 3 TUTORIAL Prolm Dsription A lning gr strut hs n sign for
More informationParameter Estimation for a Jiles-Atherton based Current Transformer core model
Prmtr Etimtion for Jil-Athrton bd Currnt Trformr cor modl Y. Chn, D. S. Oulltt, P. A. Foryth, P.G. clrn, Yi Zhg Abtrct-- Th Jil-Athrton (J-A bd currnt trformr (CT cor modl provid ccurt modlling of hytri
More information(Semi)Classical thermionic emission
unnling - primr Nno oftn pprs in rl tchnology in th form of thin lyrs or brrirs. W r going to look t svrl wys lctrons cn trnsport ovr or through ths brrirs undr vrious conditions. hrmionic mission (clssicl
More information0WAVE PROPAGATION IN MATERIAL SPACE
0WAVE PROPAGATION IN MATERIAL SPACE All forms of EM nrgy shar thr fundamntal charactristics: 1) thy all tral at high locity 2) In traling, thy assum th proprtis of was 3) Thy radiat outward from a sourc
More informationKey Ideas So Far. University of California, Berkeley
EE 105 F 2016 Ky I So Fr Pro. A. M. iknj 1 Univrity o Ciorni, Brky EE 105 F 2016 Sov or tion Lngth Pro. A. M. iknj W hv two qution n two unknown. W r iny in oition to ov or th tion th q 2 n n0 2 q 2 2
More information8/31/2018. PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103
PHY 7 Classical Mechanics and Mathematical Methods 0-0:50 AM MWF Olin 03 Plan for Lecture :. Brief comment on quiz. Particle interactions 3. Notion of center of mass reference fame 4. Introduction to scattering
More informationJosephson current noise above T c in superconducting tunnel junctions
PHYSICAL REVIEW B 78, 104507 008 Josphson currnt nois bov T c in suprconducting tunnl junctions Alx Lvchnko School of Physics nd Astronomy, Univrsity of Minnsot, Minnpolis, Minnsot 55455, USA Rcivd 19
More informationLecture 12 Quantum chromodynamics (QCD) WS2010/11: Introduction to Nuclear and Particle Physics
Lctur Quntum chromodynmics (QCD) WS/: Introduction to Nuclr nd Prticl Physics QCD Quntum chromodynmics (QCD) is thory of th strong intrction - bsd on color forc, fundmntl forc dscribing th intrctions of
More informationJOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (JMET)
JOURNAL OF MECHANICAL ENGINEERING AND ECHNOLOGY (JME) Journl of Mchnicl Enginring nd chnology (JME) ISSN 47-94 (Print) ISSN 47-9 (Onlin) Volum Issu July -Dcmbr () ISSN 47-94 (Print) ISSN 47-9 (Onlin) Volum
More informationChapter 2. Vectors. 2.1 Vectors Scalars and Vectors
Chpter 2 Vectors 2.1 Vectors 2.1.1 Sclrs nd Vectors A vector is quntity hving both mgnitude nd direction. Emples of vector quntities re velocity, force nd position. One cn represent vector in n-dimensionl
More informationQ.28 Q.29 Q.30. Q.31 Evaluate: ( log x ) Q.32 Evaluate: ( ) Q.33. Q.34 Evaluate: Q.35 Q.36 Q.37 Q.38 Q.39 Q.40 Q.41 Q.42. Q.43 Evaluate : ( x 2) Q.
LASS XII Q Evlut : Q sc Evlut c Q Evlut: ( ) Q Evlut: Q5 α Evlut: α Q Evlut: Q7 Evlut: { t (t sc )} / Q8 Evlut : ( )( ) Q9 Evlut: Q0 Evlut: Q Evlut : ( ) ( ) Q Evlut : / ( ) Q Evlut: / ( ) Q Evlut : )
More information2. Background Material
S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds
More informationSPACETIME METRIC DEFORMATIONS C O S I M O S T O R N A I O L O I N F N - S E Z I O N E D I N A P O L I I T A L Y
SPETIME METRI DEFORMTIONS O S I M O S T O R N I O L O I N F N - S E Z I O N E D I N P O L I I T L Y Lvori D. Puglis, Dformzioni i mtrich spziotmporli, tsi i lur qurinnl, rltori S. pozzillo. Storniolo S.
More information1.4 The Compton Effect
1.4 The Compton Effect The Nobel Prize in Physics, 1927: jointly-awarded to Arthur Holly Compton (figure 9), for his discovery of the effect named after him. Figure 9: Arthur Holly Compton (1892 1962):
More informationMath 304 Answers to Selected Problems
Math Answers to Selected Problems Section 6.. Find the general solution to each of the following systems. a y y + y y y + y e y y y y y + y f y y + y y y + 6y y y + y Answer: a This is a system of the
More information1.2 Faraday s law A changing magnetic field induces an electric field. Their relation is given by:
Elctromagntic Induction. Lorntz forc on moving charg Point charg moving at vlocity v, F qv B () For a sction of lctric currnt I in a thin wir dl is Idl, th forc is df Idl B () Elctromotiv forc f s any
More informationCONTINUITY AND DIFFERENTIABILITY
MCD CONTINUITY AND DIFFERENTIABILITY NCERT Solvd mpls upto th sction 5 (Introduction) nd 5 (Continuity) : Empl : Chck th continuity of th function f givn by f() = + t = Empl : Emin whthr th function f
More informationThis chapter covers special properties of planar graphs.
Chptr 21 Plnr Grphs This hptr ovrs spil proprtis of plnr grphs. 21.1 Plnr grphs A plnr grph is grph whih n b rwn in th pln without ny gs rossing. Som piturs of plnr grph might hv rossing gs, but it s possibl
More informationCSE 373: AVL trees. Warmup: Warmup. Interlude: Exploring the balance invariant. AVL Trees: Invariants. AVL tree invariants review
rmup CSE 7: AVL trs rmup: ht is n invrint? Mihl L Friy, Jn 9, 0 ht r th AVL tr invrints, xtly? Disuss with your nighor. AVL Trs: Invrints Intrlu: Exploring th ln invrint Cor i: xtr invrint to BSTs tht
More informationSingle-wall carbon nanotubes
CARBON NANOTUBS Nnotus r idl systms for studying th trnsport of lctrons in on dimnsion, nd hv commrcil potntil s nnoscl wirs, trnsistors nd snsors Singl-wll cron nnotus Pul L Mcun 1 Curling up with nnotu
More informationIntroduction to Group Theory
Introduction to Group Theory Let G be n rbitrry set of elements, typiclly denoted s, b, c,, tht is, let G = {, b, c, }. A binry opertion in G is rule tht ssocites with ech ordered pir (,b) of elements
More informationElectrochemistry L E O
Rmmbr from CHM151 A rdox raction in on in which lctrons ar transfrrd lctrochmistry L O Rduction os lctrons xidation G R ain lctrons duction W can dtrmin which lmnt is oxidizd or rducd by assigning oxidation
More informationMATHEMATICS FOR MANAGEMENT BBMP1103
Objctivs: TOPIC : EXPONENTIAL AND LOGARITHM FUNCTIONS. Idntif pnntils nd lgrithmic functins. Idntif th grph f n pnntil nd lgrithmic functins. Clcult qutins using prprtis f pnntils. Clcult qutins using
More informationMathematics. Mathematics 3. hsn.uk.net. Higher HSN23000
Highr Mthmtics UNIT Mthmtics HSN000 This documnt ws producd spcilly for th HSN.uk.nt wbsit, nd w rquir tht ny copis or drivtiv works ttribut th work to Highr Still Nots. For mor dtils bout th copyright
More informationMechanical Translational Systems
QUESTION 1 For the system in Figure 1.1, the springs are at their free lengths when the mass displacements are zero. Complete the following: Figure 1.1 QUESTION 2 For the system in Figure 2.1, the mass
More information(most) due to long range e m forces i.e. via atomic collisions or due to short range nuclear collisions or through decay ( = weak interactions)
Spring 01, P67, YK Monday January 30, 01 8 Obsrvabl particl dtction ffcts ar : (most) du to long rang m forcs i.. via atomic collisions or du to short rang nuclar collisions or through dcay ( = wak intractions)
More information( ) Geometric Operations and Morphing. Geometric Transformation. Forward v.s. Inverse Mapping. I (x,y ) Image Processing - Lesson 4 IDC-CG 1
Img Procssing - Lsson 4 Gomtric Oprtions nd Morphing Gomtric Trnsformtion Oprtions dpnd on Pil s Coordints. Contt fr. Indpndnt of pil vlus. f f (, ) (, ) ( f (, ), f ( ) ) I(, ) I', (,) (, ) I(,) I (,
More informationMiscellaneous open problems in the Regular Boundary Collocation approach
Miscllnous opn problms in th Rgulr Boundry Colloction pproch A. P. Zilińsi Crcow Univrsity of chnology Institut of Mchin Dsign pz@mch.p.du.pl rfftz / MFS Confrnc ohsiung iwn 5-8 Mrch 0 Bsic formultions
More information2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1
F110 Spktrala transformr för Mdia Solutions to Stiglitz, Chaptr 1 Prfac This documnt contains solutions to slctd problms from Kn Stiglitz s book: A Digital Signal Procssing Primr publishd by Addison-Wsly.
More informationPhysics (CBSE 2007) Time: 3 hours Max. Marks: 70. General Instructions
Physics (CSE 7) Tim: 3 hours Max Marks: 7 Gnral nstructions 1 ll qustions ar compulsory Thr is no ovrall choic Howvr, an intrnal choic has bn provi in on qustion of two marks, on qustion of thr marks an
More informationLecture 26: Quadrature (90º) Hybrid.
Whits, EE 48/58 Lctur 26 Pag f Lctur 26: Quadratur (9º) Hybrid. Back in Lctur 23, w bgan ur discussin f dividrs and cuplrs by cnsidring imprtant gnral prprtis f thrand fur-prt ntwrks. This was fllwd by
More informationλ φ φ = hc λ ev stop φ = λ φ and now ev stop λ ' = Physics 220 Homework #2 Spring 2016 Due Monday 4/11/16
Physics 0 Homework # Spring 06 Due Monday 4//6. Photons with a wavelength λ = 40nm are used to eject electrons from a metallic cathode (the emitter) by the photoelectric effect. The electrons are prevented
More informationMid Term Exam 1. Feb 13, 2009
Name: ID: Mid Term Exam 1 Phys 48 Feb 13, 009 Print your name and ID number clearly above. To receive full credit you must show all your work. If you only provide your final answer (in the boxes) and do
More informationFrom Classical to Quantum mechanics
From Classical to Quantum mcanics Engl & Rid 99-300 vrij Univrsitit amstrdam Classical wav baviour Ligt is a wav Two-slit xprimnt wit potons (81-85) 1 On sourc Intrfrnc sourcs ttp://www.falstad.com/matpysics.tml
More informationElliptical motion, gravity, etc
FW Physics 130 G:\130 lctur\ch 13 Elliticl motion.docx g 1 of 7 11/3/010; 6:40 PM; Lst rintd 11/3/010 6:40:00 PM Fig. 1 Elliticl motion, grvity, tc minor xis mjor xis F 1 =A F =B C - D, mjor nd minor xs
More informationSolutions to Homework 6. (b) (This was not part of Exercise 1, but should have been) Let A and B be groups with A B. Then B A.
MTH 4- Astrct Alger II S7 Solutions to Homework 6 Exercise () Let A, B n C e groups with A B n B C Show tht A C () (This ws not prt of Exercise, ut shoul hve een) Let A n B e groups with A B Then B A ()
More informationELEC 351 Notes Set #18
Assignmnt #8 Poblm 9. Poblm 9.7 Poblm 9. Poblm 9.3 Poblm 9.4 LC 35 Nots St #8 Antnns gin nd fficincy Antnns dipol ntnn Hlf wv dipol Fiis tnsmission qution Fiis tnsmission qution Do this ssignmnt by Novmb
More informationCoupled Pendulums. Two normal modes.
Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron
More informationMASTER CLASS PROGRAM UNIT 4 SPECIALIST MATHEMATICS SEMESTER TWO 2014 WEEK 11 WRITTEN EXAMINATION 1 SOLUTIONS
MASTER CLASS PROGRAM UNIT SPECIALIST MATHEMATICS SEMESTER TWO WEEK WRITTEN EXAMINATION SOLUTIONS FOR ERRORS AND UPDATES, PLEASE VISIT WWW.TSFX.COM.AU/MC-UPDATES QUESTION () Lt p ( z) z z z If z i z ( is
More informationMean-field theory for ferroelectricity in Ca 3 CoMnO 6
Mn-fild thory for frrolctricity in C 3 CoMnO 6 Y. J. Guo, 1 Shui Dong, 1,2,3 K. F. Wng, 1 nd J.-M. Liu 1,4, * 1 Ntionl lbortory of Solid Stt Microstructurs, Nnjing Univrsity, Nnjing 210093, Chin 2 Dprtmnt
More informationEmil Olteanu-The plane rotation operator as a matrix function THE PLANE ROTATION OPERATOR AS A MATRIX FUNCTION. by Emil Olteanu
Emil Oltu-Th pl rottio oprtor s mtri fuctio THE PLNE ROTTON OPERTOR S MTRX UNTON b Emil Oltu bstrct ormlism i mthmtics c offr m simplifictios, but it is istrumt which should b crfull trtd s it c sil crt
More informationlim P(t a,b) = Differentiate (1) and use the definition of the probability current, j = i (
PHYS851 Quntum Mechnics I, Fll 2009 HOMEWORK ASSIGNMENT 7 1. The continuity eqution: The probbility tht prticle of mss m lies on the intervl [,b] t time t is Pt,b b x ψx,t 2 1 Differentite 1 n use the
More informationLecture 4. Conic section
Lctur 4 Conic sction Conic sctions r locus of points whr distncs from fixd point nd fixd lin r in constnt rtio. Conic sctions in D r curvs which r locus of points whor position vctor r stisfis r r. whr
More informationh Summary Chapter 7.
Summry Chptr 7. In Chptr 7 w dscussd byond th fr lctron modl of chptr 6. In prtculrly w focusd on th nflunc of th prodc potntl of th on cors on th nrgy lvl dgrm of th outr lctrons of th toms. It wll hlp
More informationUNIT # 08 (PART - I)
. r. d[h d[h.5 7.5 mol L S d[o d[so UNIT # 8 (PRT - I CHEMICL INETICS EXERCISE # 6. d[ x [ x [ x. r [X[C ' [X [[B r '[ [B [C. r [NO [Cl. d[so d[h.5 5 mol L S d[nh d[nh. 5. 6. r [ [B r [x [y r' [x [y r'
More informationFUNCTION OF A HOLLOW ANODE FOR AN ANODE LAYER TYPE HALL THRUSTER
39th AIAA/ASME/SAE/ASEE Joint Propulsion Confrnc an Exhibit -3 July 3, Huntsvill, Alabama AIAA 3-47 FUNCTION OF A HOLLOW ANODE FO AN ANODE LAYE TYPE HALL THUSTE Shinsuk YASUI*, Kn KUMAKUA**, Naoji YAMAMOTO*,Kimiya
More informationPHYS102 - Electric Energy - Capacitors
PHYS102 - lectric nerg - Cpcitors Dr. Suess Februr 14, 2007 Plcing Chrges on Conuctors................................................. 2 Plcing Chrges on Conuctors II................................................
More informationImpedance Transformation and Parameter Relations
8/1/18 Cours nstructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 4 mpdanc Transformation and Paramtr Rlations mpdanc Ths Transformation
More informationCBSE 2015 FOREIGN EXAMINATION
CBSE 05 FOREIGN EXAMINATION (Sris SSO Cod No 65//F, 65//F, 65//F : Forign Rgion) Not tht ll th sts hv sm qustions Onl thir squnc of pprnc is diffrnt M Mrks : 00 Tim Allowd : Hours SECTION A Q0 Find th
More informationReview & Summary. Field Due to a Point Charge The magnitude of the electric set up by a point charge q at a distance r from the charge is
CHATE 22 ELECTIC FIELDS viw & Summr Elctric Fil To lin th lctrosttic forc btwn two chrgs, w ssum tht ch chrg sts u n lctric fil in th sc roun it. Th forc cting on ch chrg is thn u to th lctric fil st u
More informationSection 11.6: Directional Derivatives and the Gradient Vector
Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th
More informationTOPIC 5: INTEGRATION
TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function
More informationBackground: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.
Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby
More informationABREVIATION BLK(24) BLU(24) BRN(24) GRN(24) GRN/YEL(24) GRY(24) ORG(24) RED(24) YEL(24) BLK
MGNTIC DOO INTLOCK / N/O 4677: INTLOCK 4676: KY STIK GY MGY ST COOLING FNS 85: VDC FN 60MM T: FN OINTTION SHOULD XTCT WM I FOM CS. V VITION (4) LU(4) N(4) (4) /(4) GY(4) OG(4) (4) (4) LU N / GY GY/ GY/
More informationPreliminary Examination - Day 2 May 16, 2014
UNL - Department of Physics and Astronomy Preliminary Examination - Day May 6, 04 This test covers the topics of Thermodynamics and Statistical Mechanics (Topic ) and Mechanics (Topic ) Each topic has
More informationIntroduction to the quantum theory of matter and Schrödinger s equation
Introduction to th quantum thory of mattr and Schrödingr s quation Th quantum thory of mattr assums that mattr has two naturs: a particl natur and a wa natur. Th particl natur is dscribd by classical physics
More informationOn the Hamiltonian of a Multi-Electron Atom
On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making
More informationMath 322. Spring 2015 Review Problems for Midterm 2
Linear Algebra: Topic: Linear Independence of vectors. Question. Math 3. Spring Review Problems for Midterm Explain why if A is not square, then either the row vectors or the column vectors of A are linearly
More informationNARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS
. (D). (A). (D). (D) 5. (B) 6. (A) 7. (A) 8. (A) 9. (B). (A). (D). (B). (B). (C) 5. (D) NARAYANA I I T / P M T A C A D E M Y C o m m o n P r a c t i c T s t 6 XII STD BATCHES [CF] Dat: 8.8.6 ANSWER PHYSIS
More information