ECE 344 Microwave Fundamentals
|
|
- Allison Peters
- 5 years ago
- Views:
Transcription
1 ECE 44 Microwav Fundamntals Lctur 08: Powr Dividrs and Couplrs Part Prpard By Dr. hrif Hkal 4/0/08
2 Microwav Dvics 4/0/08
3 Microwav Dvics 4/0/08
4 Powr Dividrs and Couplrs Powr dividrs, combinrs and dirctional couplrs ar passiv structurs that divid RF input powr among svral outputs or combin powr from svral inputs. Powr Dividrs and Combinrs Usd to split input powr into roughly qual outputs, or vic vrsa. Dirctional Couplrs Usd to sampl a fraction of input powr and/or to sparat forward and rvrs travling wavs. 4/0/08 4
5 Powr Dividrs and Couplrs Ths ar xampls of a thr-port ntwork. A powr dividr is usd to split a signal. P P P P P A couplr/combinr is usd to combin a signal. P P P P P Goal: Distribut powr from on input among svral outputs, or combin powr from svral inputs to on output. Problms for RF and microwav dsigns Impdanc match Isolation Phas rlationships among signals 4/0/08 5
6 Thr Port Ntworks Gnral -port ntwork: 4/0/08 6
7 Thr Port Ntworks (cont.) If all thr ports ar matchd, and th dvic is rciprocal and losslss, w hav: (Th matrix is also unitary.) (Thr ar thr distinct valus.) This is not physically possibl! (s nxt slid) 4/0/08 7
8 Powr Dividrs and Couplrs (cont.) Unitary: not physically possibl Losslss [] is unitary Ths cannot all b satisfid. (If only on is nonzro, w cannot satisfy all thr.) 4/0/ At last of,, must b zro. (If only on is zro (or non is zro), w cannot satisfy all thr.) 8
9 Unitary Matrix It can b don in an asy way: Th dot product of any column of [] with th conjugat of that column givs unity. Th dot product of any column with th conjugat of a diffrnt column givs zro (orthogonal). 4/0/08 9
10 Circulators Now considr a -port ntwork that is non-rciprocal, with all ports matchd, and is losslss: (Thr ar six distinct valus.) Circulator Ths quations will b satisfid if: Losslss 0 4/0/ or Not that ij ji. 0 0
11 Circulators (cont.) Not: W hav assumd hr that th phass of all th paramtrs ar zro. Clockwis (LH) circulator Circulators can b mad using biasd frrit matrials. 4/0/08 Countr-clockwis (RH) circulator
12 Powr Dividrs T-Junction: losslss dividr Y in 0 0 Y in 0 0 To match: Not, howvr, Y in Thus, Yi n Also, Y 0 Y in in 0 0 4/0/08 If w match at port, w cannot match at th othr ports!
13 Powr Dividrs (cont.) Assuming port matchd: P in out in in in P P P K P 0 0 out in in in P P P K P 0 0 4/0/08 W can dsign th splittr to control th powrs into th two output lins.
14 Powr Dividrs (cont.) Examin th rflction at ach port ( ii ): 0 / 0 / 0 a a 0 aa0 0 0 in in a a 0 a a /0/08 zro if port is matchd Not: A match on port rquirs (sinc th two output lins combin in paralll) 0, 0 4
15 Powr Dividrs (cont.) Also, w hav: 0 0 a a ; / / 0 0 imilarly, and /0/08 5
16 Powr Dividrs (cont.) If port is matchd: ; ; Only 0 4/0/08 Th output ports ar not isolatd. 6
17 Output powrs: Powr Dividrs (cont.) P 0 P 0 0 P 0 P 0 0 Not: P is th input powr on port. Hnc P P 0 0 Chck : P P P P P P /0/08 7
18 Powr Dividrs (cont.) ummary P P 0 0 0; ; /0/ Th input port is matchd, but not th output ports. Th output ports ar not isolatd. Wavs rflctd from dvics on ports and with caus intrfrnc with th dvics. 8
19 Powr Dividrs (cont.) Exampl: Microstrip T-junction powr dividr [ ] Incidnt 0 00 [ ] [ ] 0 00 [ ] 4/0/08 9
20 Powr Dividrs (cont.) Th matchd powr dividr also works as a match powr combinr [ ] 0 00 [ ] Incidnt [ ] 0 00 [ ] b a a 0 a Equal wavs ar incidnt from ports and. 4/0/08 0
21 Rsistiv Powr Dividr in (Th sam for in and in.) 0 0 in All ports ar matchd. 0 4/0/08
22 Rsistiv Powr Dividr (cont.) 0 0 a a in By rciprocity and symmtry 0 0 4/0/08
23 Rsistiv Powr Dividr (cont.) Hnc w hav P P a in 0 0 in P P P b a P P 4 in All ports ar matchd, but / P in is dissipatd by rsistors, and th output ports ar not isolatd. 4/0/08
24 Evn-Odd Mod Analysis (This is ndd for analyzing th Wilkinson) Exampl: W want to solv for. W do this using vn/odd mod analysis. (This works bcaus th circuit itslf is symmtric.) Corrct answr : 4/0/08 4
25 Evn-Odd Mod Analysis Lt o Plan of symmtry o o o Evn problm Odd problm o 4/0/08 5
26 Evn-Odd Mod Analysis (cont.) Evn problm PO I /0/08 6
27 Evn-Odd Mod Analysis (cont.) Odd problm o o o o hort circuit (C) plan of symmtry 4 o o 0 4/0/08 7
28 Evn-Odd Mod Analysis (cont.) By suprposition: o 0 Hnc w hav 4/0/08 8
29 Wilkinson Powr Dividr Equal-split ( db) powr dividr (Th Wilkinson can b dsignd to hav an unqual split.) g / All ports matchd ( = = = 0) Output ports ar isolatd ( = = 0) g / Not: No powr is lost in going from port to ports and. 0 j /0/08 Obviously not unitary 9
30 Wilkinson Powr Dividr (cont.) Exampl: Microstrip Wilkinson powr dividr 0 50 [ ] 0 50 [ ] 0T 70.7 [ ] 0T 70.7 [ ] R 00 [ ] 0 50 [ ] 4/0/08 0
31 Wilkinson Powr Dividr (cont.) Evn and odd analysis is usd to analyz th structur whn port is xcitd. To dtrmin, Only vn analysis is ndd to analyz th structur whn port is xcitd. To dtrmin, Th othr componnts can b found by using symmtry and rciprocity. 4/0/08
32 Wilkinson Powr Dividr (cont.) Top viw 0 / 4 g g 0 / Plan of symmtry 0 0 A microstrip ralization is shown. plit structur along plan of symmtry (PO) Evn voltag vn about PO plac OC along PO Odd voltag odd about PO plac C along PO 4/0/08
33 Wilkinson Powr Dividr (cont.) 0 / 4 0 g g 0 / How do you split a transmission lin? (This is ndd for th vn cas.) Top viw I / 0 oltag is th sam for ach half of lin () Currnt is halvd for ach half of lin (I/) I / (magntic wall) I h microstrip lin 4/0/08 For ach half
34 Wilkinson Powr Dividr (cont.) Evn Problm g / 4 0 Not: Th 0 rsistor has bn split into two 0 rsistors in sris OC Ports and ar xcitd in phas. OC 0 0 g / 4 0 4/0/08 Not : 4
35 Wilkinson Powr Dividr (cont.) Odd problm g / 4 0 o 0 0 o Not: Th 0 rsistor has bn split into two 0 rsistors in sris. 0 o o Ports and ar xcitd 80 o out of phas g / 4 o 0 o 4/0/08 Not : 0, o o o 5
36 Wilkinson Powr Dividr (cont.) Evn Problm Port xcitation g / 4, in 0 Port 0 0 OC 0 in 0 0 in 0 in 0 0 Rcall: in T (quartr-wav transformr) L Also, by symmtry, 0 4/0/08 6
37 Wilkinson Powr Dividr (cont.) Odd Problm Port xcitation g / 4 0 o, o o in 0 0 o Port 0 o o 0 hort o in 0 0 o o in 0 o in 0 0 4/0/08 Also, by symmtry, o 0 7
38 Wilkinson Powr Dividr (cont.) W add th rsults from th vn and odd cass togthr: a a 0 o o o (by symmtry) a a 0 o o o (by rciprocity) Not: inc all ports hav th sam 0, w ignor th normalizing factor 0 in th paramtr dfinition. 4/0/08 In summary, for port xcitation, w hav:
39 Wilkinson Powr Dividr (cont.) Port xcitation Port g / g / Whn port is xcitd, th rspons, by symmtry, is vn. (Hnc, th total filds ar th sam as th vn filds.) 4/0/08 9
40 Wilkinson Powr Dividr (cont.) Evn Problm Port 0 g / O.C. symmtry plan 0 g / 4 0 OC 0 g / 4 4/0/08 40
41 Wilkinson Powr Dividr (cont.) Evn Problm Port xcitation Port 0 g / 4 0 OC 0 0 in 0 0 in 0 in 0 0, in Hnc a a 0 a /0/08 4
42 Wilkinson Powr Dividr (cont.) Evn Problm Port xcitation a a 0 Port 0 g / z OC j j 4/0/08 j (rciprocal) Along g /4 wav transformr: jz jz 0 z z 0 0 g /4 j distanc from port 4
43 Wilkinson Powr Dividr (cont.) For th othr componnts: By symmtry: j By rciprocity: j 4/0/08 4
44 Wilkinson Powr Dividr (cont.) 0 j g / g / All thr ports ar matchd, and th output ports ar isolatd. 4/0/08 44
45 Wilkinson Powr Dividr (cont.) 0 j g / j 0 0 g / j Whn a wav is incidnt from port, half of th total incidnt powr gts transmittd to ach output port (no loss of powr). Whn a wav is incidnt from port or port, half of th powr gts transmittd to port and half gts absorbd by th rsistor, but nothing gts through to th othr output port. 4/0/08 45
46 Wilkinson Powr Dividr (cont.) Figur 7.5 of Pozar Photograph of a four-way corporat powr dividr ntwork using thr microstrip Wilkinson powr dividrs. Not th isolation chip rsistors. Courtsy of M.D. Abouzahra, MIT Lincoln Laboratory. 4/0/08 46
47 Wilkinson Powr Dividr (cont.) Figur 7. of Pozar Frquncy rspons of an qual-split Wilkinson powr dividr. Port is th input port; ports and ar th output ports. 4/0/08 47
ECE Microwave Engineering
ECE 537-635 Microwave Engineering Fall 8 Prof. David R. Jackson Dept. of ECE Adapted from notes by Prof. Jeffery T. Williams Notes Power Dividers and Circulators Power Dividers and Couplers A power divider
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 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 informationECE 2210 / 00 Phasor Examples
EE 0 / 00 Phasor Exampls. Add th sinusoidal voltags v ( t ) 4.5. cos( t 30. and v ( t ) 3.. cos( t 5. v ( t) using phasor notation, draw a phasor diagram of th thr phasors, thn convrt back to tim domain
More informationChapter 6: Polarization and Crystal Optics
Chaptr 6: Polarization and Crystal Optics * P6-1. Cascadd Wav Rtardrs. Show that two cascadd quartr-wav rtardrs with paralll fast axs ar quivalnt to a half-wav rtardr. What is th rsult if th fast axs ar
More informationLinear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let
It is impossibl to dsign an IIR transfr function with an xact linar-phas It is always possibl to dsign an FIR transfr function with an xact linar-phas rspons W now dvlop th forms of th linarphas FIR transfr
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 informationLecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e
8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain
More informationVoltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes
Lctur 1. oltag, Currnt, Powr, Sris sistanc, Paralll sistanc, and Diods Whn you start to dal with lctronics thr ar thr main concpts to start with: Nam Symbol Unit oltag volt Currnt ampr Powr W watt oltag
More informationAddition of angular momentum
Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat
More informationSlide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS
Slid DIGITAL SIGAL PROCESSIG UIT I DISCRETE TIME SIGALS AD SYSTEM Slid Rviw of discrt-tim signals & systms Signal:- A signal is dfind as any physical quantity that varis with tim, spac or any othr indpndnt
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 informationDefinition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.
Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind
More informationAddition of angular momentum
Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th
More informationThat is, we start with a general matrix: And end with a simpler matrix:
DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss
More informationECEN 5004, Spring 2018 Active Microwave Circuits Zoya Popovic, University of Colorado, Boulder LECTURE 2 SOME PASSIVE CIRCUITS
ECEN 54, pring 18 Activ Microwav Circuits Zoya Popovic, Univrsity of Colorado, Bouldr LECTURE OME PAIVE CIRCUIT W hav alrady rviwd atching circuits, which ar -port ntworks. Thy ar passiv and can b rciprocal
More informationLecture 27: The 180º Hybrid.
Whits, EE 48/58 Lctur 7 Pag f 0 Lctur 7: Th 80º Hybrid. Th scnd rciprcal dirctinal cuplr w will discuss is th 80º hybrid. As th nam implis, th utputs frm such a dvic can b 80º ut f phas. Thr ar tw primary
More information2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line
//03 Ovrviw -owr Transmission Txt: 4.6-4.0 ECEGR 45 owr ystms Consrvation of Complx owr hort in owr Transmission owr Transmission isualization Radial in Mdium and ong in owr Transmission oltag Collaps
More informationThe van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012
Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor
More informationEven/Odd Mode Analysis of the Wilkinson Divider
//9 Wilkinn Dividr Evn and Odd Md Analyi.dc / Evn/Odd Md Analyi f th Wilkinn Dividr Cnidr a matchd Wilkinn pwr dividr, with a urc at prt : Prt Prt Prt T implify thi chmatic, w rmv th grund plan, which
More informationGeneral Notes About 2007 AP Physics Scoring Guidelines
AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1
More informationLast time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same
Last tim Bgin circuits Rsistors Circuits Today Rsistor circuits Start rsistor-capacitor circuits Physical layout Schmatic layout Tu. Oct. 13, 2009 Physics 208 Lctur 12 1 Tu. Oct. 13, 2009 Physics 208 Lctur
More informationThe Transmission Line Wave Equation
1//5 Th Transmission Lin Wav Equation.doc 1/6 Th Transmission Lin Wav Equation Q: So, what functions I (z) and V (z) do satisfy both tlgraphr s quations?? A: To mak this asir, w will combin th tlgraphr
More informationME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002
3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or
More informationMCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems
MCE503: Modling and Simulation o Mchatronic Systms Discussion on Bond Graph Sign Convntions or Elctrical Systms Hanz ichtr, PhD Clvland Stat Univrsity, Dpt o Mchanical Enginring 1 Basic Assumption In a
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 informationClassical Magnetic Dipole
Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg
More informationPropositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018
Propositional Logic Combinatorial Problm Solving (CPS) Albrt Olivras Enric Rodríguz-Carbonll May 17, 2018 Ovrviw of th sssion Dfinition of Propositional Logic Gnral Concpts in Logic Rduction to SAT CNFs
More informationFunction Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0
unction Spacs Prrquisit: Sction 4.7, Coordinatization n this sction, w apply th tchniqus of Chaptr 4 to vctor spacs whos lmnts ar functions. Th vctor spacs P n and P ar familiar xampls of such spacs. Othr
More informationThe Matrix Exponential
Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!
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 informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More informationEE243 Advanced Electromagnetic Theory Lec # 23 Scattering and Diffraction. Reading: Jackson Chapter , lite
Applid M Fall 6, Nuruthr Lctur #3 Vr /5/6 43 Advancd lctromagntic Thory Lc # 3 cattring and Diffraction calar Diffraction Thory Vctor Diffraction Thory Babint and Othr Principls Optical Thorm ading: Jackson
More informationThe Matrix Exponential
Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!
More informationA Propagating Wave Packet Group Velocity Dispersion
Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to
More informationMassachusetts Institute of Technology Department of Mechanical Engineering
Massachustts Institut of Tchnolog Dpartmnt of Mchanical Enginring. Introduction to Robotics Mid-Trm Eamination Novmbr, 005 :0 pm 4:0 pm Clos-Book. Two shts of nots ar allowd. Show how ou arrivd at our
More informationThe graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the
Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th
More informationorbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the
Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly
More informationSAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS
It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS
More informationThere is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real.
Midtrm #, Physics 37A, Spring 07. Writ your rsponss blow or on xtra pags. Show your work, and tak car to xplain what you ar doing; partial crdit will b givn for incomplt answrs that dmonstrat som concptual
More information6. The Interaction of Light and Matter
6. Th Intraction of Light and Mattr - Th intraction of light and mattr is what maks lif intrsting. - Light causs mattr to vibrat. Mattr in turn mits light, which intrfrs with th original light. - Excitd
More informationEinstein Equations for Tetrad Fields
Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for
More informationThus, because if either [G : H] or [H : K] is infinite, then [G : K] is infinite, then [G : K] = [G : H][H : K] for all infinite cases.
Homwork 5 M 373K Solutions Mark Lindbrg and Travis Schdlr 1. Prov that th ring Z/mZ (for m 0) is a fild if and only if m is prim. ( ) Proof by Contrapositiv: Hr, thr ar thr cass for m not prim. m 0: Whn
More informationLie Groups HW7. Wang Shuai. November 2015
Li roups HW7 Wang Shuai Novmbr 015 1 Lt (π, V b a complx rprsntation of a compact group, show that V has an invariant non-dgnratd Hrmitian form. For any givn Hrmitian form on V, (for xampl (u, v = i u
More informationα I I R α N I F I F i C i E R Cx R Ex C Cx i B R Bx
Bipolar transistor, continud - 1 - Ebrs-Moll modl α I I R α N I F E i E i C C R Ex I F I R R Cx C Cx i B R Bx B E B C Figur 1: Dashd lin indicats th "intrinsic" portion of th dvic, xcluding "parasitic"
More informationTheory and Applications of Transmission Lines
Thory and Applications of Transmission ins 1 Introduction Typs Topics Gnral Transmission-in Equations Wav Charactristics on Finit Transmission ins Wavguids Optical Fibr 2 Transmission ins Usd for guiding
More informationu 3 = u 3 (x 1, x 2, x 3 )
Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.
More informationPH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding
PH Modrn Physics SP11 Final Essay Thr will b an ssay portion on th xam, but you don t nd to answr thos qustions if you submit a final ssay by th day of th final: Sat. 5/7 It dosnʼt mattr how smart you
More informationBifurcation Theory. , a stationary point, depends on the value of α. At certain values
Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local
More informationA 1 A 2. a) Find the wavelength of the radio waves. Since c = f, then = c/f = (3x10 8 m/s) / (30x10 6 Hz) = 10m.
1. Young s doubl-slit xprint undrlis th instrunt landing syst at ost airports and is usd to guid aircraft to saf landings whn th visibility is poor. Suppos that a pilot is trying to align hr plan with
More informationQuasi-Classical States of the Simple Harmonic Oscillator
Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats
More informationImpedance (T) EELE 461/561 Digital System Design. Module #3 Interconnect Modeling with Distributed Elements Topics. Transmission Lines
EEE 46/56 igital Systm sign Modul #3 ntrconnct Modling with istributd Elmnts Topics. mpdanc of Transmission ins Ttbook Rading Assignmnts Transmission ins mpdanc T - Transmission ins ar istributd lmnts
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More informationThe Frequency Response of a Quarter-Wave Matching Network
4/1/29 Th Frquncy Rsons o a Quartr 1/9 Th Frquncy Rsons o a Quartr-Wav Matchg Ntwork Q: You hav onc aga rovidd us with conusg and rhas uslss ormation. Th quartr-wav matchg ntwork has an xact SFG o: a Τ
More information10. The Discrete-Time Fourier Transform (DTFT)
Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w
More informationWhat are those βs anyway? Understanding Design Matrix & Odds ratios
Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.
More informationSinusoidal Response Notes
ECE 30 Sinusoidal Rspons Nots For BIBO Systms AStolp /29/3 Th sinusoidal rspons of a systm is th output whn th input is a sinusoidal (which starts at tim 0) Systm Sinusoidal Rspons stp input H( s) output
More informationEIE 332 Electromagnetics
EIE 332 Elctromagntics cturr: Dr. W.Y.Tam Room no.: DE604 Phon no.: 27666265 -mail: nwytam@polyu.du.hk wb: www.n.polyu.du.hk/~m/mypag.htm Normal Offic hour: 9:00am 5:30pm (Mon-Fri) 9:00am 12:30pm (Sat)
More information4. (5a + b) 7 & x 1 = (3x 1)log 10 4 = log (M1) [4] d = 3 [4] T 2 = 5 + = 16 or or 16.
. 7 7 7... 7 7 (n )0 7 (M) 0(n ) 00 n (A) S ((7) 0(0)) (M) (7 00) 8897 (A). (5a b) 7 7... (5a)... (M) 7 5 5 (a b ) 5 5 a b (M)(A) So th cofficint is 75 (A) (C) [] S (7 7) (M) () 8897 (A) (C) [] 5. x.55
More informationScattering Parameters. Scattering Parameters
Motivatio cattrig Paramtrs Difficult to implmt op ad short circuit coditios i high frqucis masurmts du to parasitic s ad Cs Pottial stability problms for activ dvics wh masurd i oopratig coditios Difficult
More informationVII. Quantum Entanglement
VII. Quantum Entanglmnt Quantum ntanglmnt is a uniqu stat of quantum suprposition. It has bn studid mainly from a scintific intrst as an vidnc of quantum mchanics. Rcntly, it is also bing studid as a basic
More informationBasic Polyhedral theory
Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist
More information5.80 Small-Molecule Spectroscopy and Dynamics
MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts
More informationSynchronous machines
Synchronous gnrator (altrnator): transorms mchanical nrgy into lctric nrgy; dsignd to gnrat sinusoidal oltags and currnts; usd in most powr plants, or car altrnators, tc. Synchronous motor: transorms lctric
More informationChapter 6 Folding. Folding
Chaptr 6 Folding Wintr 1 Mokhtar Abolaz Folding Th folding transformation is usd to systmatically dtrmin th control circuits in DSP architctur whr multipl algorithm oprations ar tim-multiplxd to a singl
More information5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd
1. First you chck th domain of g x. For this function, x cannot qual zro. Thn w find th D domain of f g x D 3; D 3 0; x Q x x 1 3, x 0 2. Any cosin graph is going to b symmtric with th y-axis as long as
More informationLecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields
Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration
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 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 informationcycle that does not cross any edges (including its own), then it has at least
W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th
More informationu x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula
7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting
More informationCOMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.
C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH
More informationDealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems
Daling with quantitati data and problm soling lif is a story problm! A larg portion of scinc inols quantitati data that has both alu and units. Units can sa your butt! Nd handl on mtric prfixs Dimnsional
More informationSystem variables. Basic Modeling Concepts. Basic elements single and. Power = effort x flow. Power = F x v. Power = V x i. Power = T x w.
Basic Modling Concpts Basic lmnts singl and multiport t dvics Systm variabls v m F V i Powr F x v T w Powr T x w Powr V x i P Q Powr P x Q Powr ort x low Eort & low ar powr variabls Eorts t... Flows...
More informationEXST Regression Techniques Page 1
EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy
More informationPrinciples of active remote sensing: Lidars. 1. Optical interactions of relevance to lasers. Lecture 22
Lctur 22 Principls of activ rmot snsing: Lidars Ojctivs: 1. Optical intractions of rlvanc to lasrs. 2. Gnral principls of lidars. 3. Lidar quation. quird rading: G: 8.4.1, 8.4.2 Additional/advancd rading:.m.
More informationSolution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:
APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding
More informationCHAPTER 10. Consider the transmission lines for voltage and current as developed in Chapter 9 from the distributed equivalent circuit shown below.
CHAPTER 1 1. Sinusoidal Stady Stat in Transmission ins 1.1 Phasor Rprsntation of olta and Currnt Wavs Considr th transmission lins for volta and currnt as dvlopd in Chaptr 9 from th distributd quivalnt
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 informationAlpha and beta decay equation practice
Alpha and bta dcay quation practic Introduction Alpha and bta particls may b rprsntd in quations in svral diffrnt ways. Diffrnt xam boards hav thir own prfrnc. For xampl: Alpha Bta α β alpha bta Dspit
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 informationEAcos θ, where θ is the angle between the electric field and
8.4. Modl: Th lctric flux flows out of a closd surfac around a rgion of spac containing a nt positiv charg and into a closd surfac surrounding a nt ngativ charg. Visualiz: Plas rfr to Figur EX8.4. Lt A
More informationHydrogen Atom and One Electron Ions
Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial
More informationElectronic Circuits. BJT Amplifiers. Manar Mohaisen Office: F208 Department of EECE
Elctronic Circuits BJT mplifirs Manar Mohaisn Offic: F208 Email: manar.subhi@kut.ac.kr Dpartmnt of EECE viw of th Prcdnt Lctur Explain th DC Oprating Point Explain th Voltag-dividr Bias Othr Bias Mthods
More information1 Isoparametric Concept
UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric
More informationCh. 24 Molecular Reaction Dynamics 1. Collision Theory
Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic
More informationContemporary, atomic, nuclear, and particle physics
Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is
More informationOptics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007
Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting
More information1 1 1 p q p q. 2ln x x. in simplest form. in simplest form in terms of x and h.
NAME SUMMER ASSIGNMENT DUE SEPTEMBER 5 (FIRST DAY OF SCHOOL) AP CALC AB Dirctions: Answr all of th following qustions on a sparat sht of papr. All work must b shown. You will b tstd on this matrial somtim
More informationFrom Elimination to Belief Propagation
School of omputr Scinc Th lif Propagation (Sum-Product lgorithm Probabilistic Graphical Modls (10-708 Lctur 5, Sp 31, 2007 Rcptor Kinas Rcptor Kinas Kinas X 5 ric Xing Gn G T X 6 X 7 Gn H X 8 Rading: J-hap
More information2. Laser physics - basics
. Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"
More informationSeebeck and Peltier Effects
Sbck and Pltir Effcts Introduction Thrmal nrgy is usually a byproduct of othr forms of nrgy such as chmical nrgy, mchanical nrgy, and lctrical nrgy. Th procss in which lctrical nrgy is transformd into
More informationTRANSISTOR AND DIODE STUDIES. Prof. H. J. Zimmermann Prof. S. J. Mason C. R. Hurtig Prof. R. B. Adler Dr. W. D. Jackson R. E.
XI. TANSISTO AND DIODE STUDIES Prof. H. J. Zimmrmann Prof. S. J. Mason C.. Hurti Prof.. B. Adlr Dr. W. D. Jackson. E. Nlson A. DESIGN OF TANSFOMEESS TANSISTO AUDIO AMPIFIES Considrabl ffort by many oranizations
More informationDerivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian
Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting
More informationHigher order derivatives
Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of
More informationThomas Whitham Sixth Form
Thomas Whitham Sith Form Pur Mathmatics Cor rvision gui Pag Algbra Moulus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv blow th ais in th ais. f () f () f
More informationTitle: Vibrational structure of electronic transition
Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum
More informationMath 34A. Final Review
Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right
More informationGradebook & Midterm & Office Hours
Your commnts So what do w do whn on of th r's is 0 in th quation GmM(1/r-1/r)? Do w nd to driv all of ths potntial nrgy formulas? I don't undrstand springs This was th first lctur I actually larnd somthing
More information