Impedance matching concept given ZL, design a matching network to have in=0 or selected value. matching. Zin (=Z Z o )

Size: px
Start display at page:

Download "Impedance matching concept given ZL, design a matching network to have in=0 or selected value. matching. Zin (=Z Z o )"

Transcription

1 Chapter 5 Ipedance atching and tuning 5. Matching with luped eleents -sectin atching netwrks using Sith chart 5. Single-stub tuning shunt stub, series stub 5.3 Duble-stub tuning frbidden regin 5.4 The quarter-wave transfrer frequency respnse 5.5 The thery f sall reflectins single-sectin transfrer, ulti-sectin transfrer 5.6 Binial ultisectin atching transfrers 5.7 Chebyshev ultisectin atching transfrers 5.8 Taper lines expnential taper, triangular taper 5.9 The Bde-Fan criterin -Bandwidth 5-

2 Ipedance atching cncept given, design a atching netwrk t have in=0 r selected value atching in netwrk in (= ) Discussin. Matching netwrk usually uses lssless cpnents:, C, transissin line and transfrer.. There are pssible slutins fr the atching circuit. 3. Prperly use Sith chart t find the ptial design. 4. Factrs fr selecting atching circuit are cplexity, bandwidth, ipleentatin and adjustability. 5-

3 5. Matching with luped eleents (-eleent -netwrk) Sith chart slutin cnstant G-circle cnstant R-circle C -plane Y-plane CW add series CW add shunt C (reduce series C) (reduce shunt ) CCW add series C CCW add shunt (reduce series ) (reduce shunt C) 5-3

4 j0.5 -j0.5 (explanatin) A C C C j -j B D -j j cnstant R-circle r C in series.5 () CW A B : j0.5 jx j jx j.5 j : add an in series () CCW B A: j jx j0.5 jx j.5 C jc.5 : add a C in series.5 r CCW B A: j jx j0.5 jx j.5 j.5 : reduce extra jx j.5 (r reduce series by ) (3) CCW C D : j0.5 jx j jx j.5 C jc.5 : add a C in series.5 (4) CW D C : j jx j0.5 jx j.5 j : add an in series r CW D C : j jx j0.5 jx j.5 C jc.5 reduce extra jx j.5 (r reduce series C by C ).5 in -plane CW add a series (r reduce series C) CCW add a series C (r reduce series ) 5-4

5 cnstant G-circle r C in shunt -j j A C C -j C j -j0.5 B D j0.5.5y () CW A B : j jb j0.5 jb j.5y jc C : add a C in shunt r CW A B : j jb j0.5 jb j.5y j.5y : reduce shunt jb j.5 Y (r reduce shunt by ).5Y () CCW B A : j0.5 jb j jb j.5 j : add an in shunt (3) CCW C D : j jb j0.5 jb j.5 j : add an in shunt.5y r CCW C D : j jb j0.5 jb j.5y jc C.5Y reduce shunt jb j.5 Y (r reduce shunt C by C ) (4) CW D C : j0.5 jb j jb j.5 jc : add a C in shunt in Y-plane CW add a shunt C (r reduce shunt ) CCW add a shunt (r reduce shunt C) 5-5

6 Discussin. inside +jx circle, tw pssible slutins Sith chart slutin (shunt-series eleents) +jb circle B z +jx circle A: A B: series-shunt eleents? N analytical slutin jx jx jb 5-6 jb R jx B 0 C,B 0 X 0, X 0 C

7 . utside +jx circle, tw pssible slutins Sith chart slutin (series-shunt eleents) +jb circle B A z +jx circle A B shunt-series eleents? Y analytical slutin jb jx R j( X X B 0 C,B 0 jb X 0, X 0 C ) 5-7

8 3. Ex. 5. =00-j00, =00, f=500mhz A: B A 3 C z. z=-j, y=0.4+j0. Slutin A. y=0.4+j0.5 jb=j0.3 jb=jc=jb/ C=b/ =0.9pF z=-j. jx=j. jx=j =jx =x / =38.8nH Slutin B 3. y=0.4-j0.5 jb=-j0.7-jb=/j=-jb/ =- /b=46.nh z=+j. jx=-j. jx=/jc=-jx C=-/x =.6pF frequency respnse (p.33, Fig.5.3(c)) B: C 5-8

9 4. Pssible 3-eleent -netwrk z +jx circle series? Y +jb circle z 5-9

10 5. Pssible 4-eleent -netwrk shrter paths fr a wider peratinal bandwidth z +jx circle +jb circle z 5-0

11 6. uped eleents (size</0) capacitr: chip capacitr, MIM capacitr (<5pF), interdigital gap capacitr (<0.5pF), pen stub(<0.pf) inductr: chip inductr, lp inductr, spiral inductr (<0nH) resistr: chip resistr, planar resistr All these luped eleents inherently have parasitic eleents in the icrwave range. (p.33, pint f interest ) B A C D 5- Size (il) A B C D il=0.00in=5u=/40

12 5. Single-stub tuning equivalent icrstrip eleents a series C --- a series in series with a high ipedance icrstrip line a shunt C in shunt with an pen icrstrip line, r in series with a lw ipedance icrstrip line a shunt in shunt with a shrt icrstrip line an pen-circuited icrstrip line a shrt-circuited icrstrip line in in j tan l jc j tan l j, l a high/lw ipedance icrstrip line l j tan Y3 l j tan sin l j 5- high lw j l βl j

13 (derivatin f high/lw ipedance line), l l j tan Y3 high,y3 0 l j tan sin l j j βl l βl l j βl jω ω c 3 jsin l 3 j csc l Y3 j sin l j (ct l csc l) j l cs l sin l l sin lsin cs 5-3 l j sin cs lw,, 0 slide (4 ) j (ct l csc l) j cscl 3 cs l sin l sin j tan l l l βl βl l j jωc C ω c l βl j

14 Discussin. Shunt stub Sith chart slutin y in jb jc d G y l y in jb cnstant -circle y in jb j d G y l y in jb 5-4

15 . Series stub Sith chart slutin z in jx d G z l z in jx jc z in jx d G z l z in jx j 5-5

16 3. Ex. 5. =60-j80, =50, f=ghz, using a shunt shrt stub G S.C. l 3 4. z=.-j.6, y=0.3+j0.4 Slutin A B. y=+j.47 d=0. 3. y=-j.47 l=0.095, shrt stub 5 l A z Slutin B 4. y=-j.47 d= y=j.47 l=0.405, shrt stub d frequency respnse (p.37, Fig.5.5(c)) Slutin A has a wider bandwidth. l 5-6

17 4. Ex. 5.3 =00+j80, =50, f=ghz, using series pen stub G l B 4 A 3 5 z O.C. l. z=+j.6 Slutin A. z=-j.33 d=0. 3. z=j.33 l=0.397, pen stub Slutin B 4. z=+j.33 d= z=-j.33 l=0.03, pen stub frequency respnse (p.40, Fig.5.6(c)) It can nt be ipleented in icrstrip lines. 5-7

18 5. Analytical slutin fr shunt stub Y in jb d l Y in Y jb j tan d Y Re d j tan d pen stub j tan d tan l B I l j tan d shrt stub tan l 5-8

19 6. Analytical slutin fr series stub in jx d l in jx j tan d Re d j tan d j tan d - pen stub X I tan l l j tan d tan l shrt stub 5-9

20 5.3 Duble-stub tuning 4, 5 ±jb, 3 /8 G 5 z l l frbidden regin 3 4 Discussin. There exists a frbidden regin fr. It can be tuned ut by adding a certain length f line. 5-0

21 G l. Ex. 5.4 =60-j80, =50, f=ghz, using duble-shuntpen-stubs. z=.-j.6, y=0.3+j0.4 l 7 Slutin A 6. y=0.3+j b = l 5 = y=+j b = -.38 l =0.35 O.C. B A 4 Slutin B 3. y=0.3+j b =.34 3 z l = l 5. y=-j b = 3.38 l 8 l =0.04 /8 l l 5- frequency respnse (p.45, Fig.5.9(c))

22 3. Analytical slutin Y = Y - jb Y d l jb l jb Y Re Y Y Y Y I jb, Y Y B Y B l l jb j j tan d tan d 5-

23 5.4 The quarter-wave transfrer frequency respnse l / 0=0 / 0= (real) Γ( θ ) cs, fr near, l - : ax. tlerated Γver the bandwidth f 4 Γ f π cs ( ),, increases f Γ 5-3

24 (derivatin f (θ) cs ) j tan ( ) j tan j tan ( θ) ( ) j tan j tan in j tan j tan in j tan ( ) ( ) j tan j tan j tan sec cs Δf 4 (derivatin f cs ( )) f π Γ / 5-4 Γ j ( θ) ( ) 4 4 / [( ) ( tan ) ] [ tan ] ( ) ( ) 4 [ sec ] ( ) tan /

25 Γθ ( ) 4 [ sec ] ( ) / ( ) cs ( ) cs cs f f vp( f) f f f TEM line: l v ( f ) 4 v ( f ) 4 f f f f f f p p ( f f) f 4 4 cs f f 5-5

26 partial reflectin cefficients 5.5 The thery f sall reflectins single-sectin transfrer, 3 T T 3 (real) in in T e 3 T e j j e j 3 e j, T, T Γ in 5-6 jθ 3 jθ ΓΓ3e Γ Γ Γ e ( )( ) Γ e Γ Γ jθ jθ 3 3 jθ ΓΓ3e Γ e Γ Γ e 3 3 TT Γe jθ jθ Γ Γ e if jθ 3

27 ultisectin transfrer N N (real) Γ( ) Γ Γ e Γ e... Γ e, if Γ Γ, Γ Γ... jθ j4θ j Nθ N N N e [ Γ ( e e ) Γ ( e e )... Γ ( e e )] N dd e Γ e e Γ e e Γ N even jnθ jnθ jnθ j( N ) θ j( N ) θ jθ jθ ( N)/ jnθ jnθ jnθ j( N ) θ j( N ) θ [ ( ) ( )... N/ ] jnθ e [ Γ cs N Γ cs( N )... Γn cs( N n)... Γ( N )/ cs ] N dd jnθ e [ Γ cs N Γ cs( N )... Γn cs( N n)... Γ N / ] N even given Γ( ), design,,... n 5-7

28 5.6 Binial ultisectin atching transfrer axial flatness respnse fr () jθ N N N jnθ jθ j4θ n N jnθ n0 Γ( ) A( e ) A C e Γ Γ e Γ e... Γ e Γ n AC N n Discussin. Maxial flatness respnse,. 3. (p.54, Table 5. fr n values) 5-8 d N d Γ( ) N N N Γ(0) A A Γ x ln (ln ) x n n n n x n n n rl 4 0 n N N N N N ln Γn ACn Cn Cn ln n

29 4. Δf 4 Γ N N N cs [ ( ) ], N, Δ f, Γ A cn θ f π A jθ N N N Γ( ) A( e ) Γ( ) A cs f 4 4 f cs [ ( N ) ] 5. Ex.5.6 =50, =00, N=3, =0.05 Δf N 3, A ln , 70% N N f ln C ln ln C ln 9.7 n N N 3 3 n 0 n ln C ln 70.7, ln C ln (p.56, Fig.5.5 fr frequency respnse f Γ ) 5-9 Γ A

30 5.7 Chebyshev ultisectin atching transfrers Equal ripple respnse fr (): ptial design jnθ Γ( ) e [ Γ cs N Γ cs( N )... Γ cs( N n)...] jnθ Ae T (sec cs ) Γ (p.60, Table 5.) N n T ( x) x, T ( x) x, T ( x) 4x 3 x, T ( x) 8x 8x, cs Tn ( x) xtn- ( x) Tn- ( x), x, x cs Discussin.. (0) AT N (sec θ) A T (sec θ ) AT () A T N 3. Optial design: given, axial f given f, inial. N f 4 (sec ) (5.63) Γ f N 5-30 n - x π-θ θ

31 4. Ex.5.7 =00, =50, N=3, =0.05 N 3, Γ( ) e ( Γ cs 3 Γ cs ) Ae T (sec cs ) Ae j3θ 3 3 j3θ j3θ 3 (4sec cs 3sec cs ) j3θ 3 Ae [sec (cs 3 3cs ) 3sec cs ] f A Γ sec = % T f 3(sec ) 3 Γ Asec Γ Γ3 Γ A(3sec 3sec ) Γ Γ Γ Γ Γ Γ frequency respnse (p.6, Fig.5.7) 5-3

32 5.8 Tapered lines Frequency respnse (z) + 0 z z+z z d d ln d dz dz d dz jz ( ) e (ln ) 0 dz 5-3

33 Discussin. Expnential taper az ( z) e 0 z a ( ) e a ln d sin Γ e e dz e jz az j ( ) (ln ) ln 0 dz, Γ( ) (p. 63, Fig.5.9). Triangular taper (z/) ln e 0 z (z) ( 4z/z / ) ln e z j sin( ) Γ( ) ln e [ ] first null at (p. 64, Fig.5.0) 5-33

34 3. Klpfenstein taper z ( ) (5.74), (5.75), Γ( ) (5.76), ptial taper 4. Ex.5.8 =00, =50, =0.0 az expnential taper: ( z) e, a ln sin Γ( ) ln sin triangular taper: Γ( ) ln [ ] cs ( ) A Klpfenstein taper: Γ( ) Γ, A 3.543, Γ csh A frequency respnse (p. 66, Fig.5.) 5-34

35 5.9 The Bde-Fan criterin lssless () atching C R 0 netwrk ln d ( ) RC Discussin. ln/ ln/ 5-35

36 0 ln ln d ln ( ) RC d : cnstant () given RC () 0, unless =0 i.e., =0 nly at a finite nuber f frequencies (3) R and/r C and/r high Q lad is harder t atch lssless () atching C R netwrk 5-36 parallel resnatr Q= RC

37 Slved prbles: Prb.5.7 find and l.95+j0.98 z 4+j =40Ω, l 00+j00 zin r in 0.8 r ax j00 j tan l j (00 j 00) tan l 40 j8000 tan l 4000 tan l 00 j00 j tanl tan l 00 j8000 tan l j00 j tanl 5tan l j j j l l 0.5 l tan tan kr k, 50 kr R ' in in ' in R' ax ax ' ax r' in r' ax in ax R ' R' k r ' r ' k 4. k.05 () (50)

38 Prb.5.4 find the best R ver perating range f 3.~0.6GHz () UWB netwrk 0.6pF 75Ω 0 ln d Γ( ) ln (0.6 3.) ln , R 6.4dB RC 5-38

39 Prb. Fr a lssless and reciprcal tw-prt atching netwrk, * * if then. s in ut ssless and reciprcal atching circuit S in ut () if S in S S in in in S in in in in in S in in S in in in in in in in S ( ) in in in in in if ut ut ut ut ut ut ut ut ut ut ut ut ut ut ut ut ut ut ( ) ut ut ut ut ut 5-39

40 S S S S 0...( i) lssless S S S S S S 0...( ii) () S S S S...( iii) in ADS exaples: Ch5_prj 5-40 ssless and reciprcal atching circuit S S...( iv) S in () i SS SS S S S S S S S S SS S SS S SS S S S S S S S S S S S S S S S S ( iii) in if ut S in...( v) ( ) () i SSS SS S S S S SS S S S SS SS S SSS S SSS S S S S S S S S ( ) S ( ) ( ),( ) ( ) S iv i ii v SS SS SS SS S( in S) S SS S SSS S SSS S( Sin ) SS S S( S S SS S S S S S S S S S S S S S S S S S S S S S S S S S S S S S S S S S S S S ( ) ) S ut

Impedance Matching and Tuning

Impedance Matching and Tuning C h a p t e r F i v e Impedance Matching and Tuning This chapter marks a turning point, in that we now begin to apply the theory and techniques of previous chapters to practical problems in microwave engineering.

More information

5.7 Chebyshev Multi-section Matching Transformer

5.7 Chebyshev Multi-section Matching Transformer 3/8/6 5_7 Chebyshev Multisection Matching Transforers / 5.7 Chebyshev Multi-section Matching Transforer Reading Assignent: pp. 5-55 We can also build a ultisection atching network such that Γ f is a Chebyshev

More information

ECE 391 supplemental notes - #11. Adding a Lumped Series Element

ECE 391 supplemental notes - #11. Adding a Lumped Series Element ECE 391 supplemental notes - #11 Adding a umped Series Element Consider the following T-line circuit: Z R,1! Z,2! Z z in,1 = r in,1 + jx in,1 Z in,1 = z in,1 Z,1 z = Z Z,2 zin,2 = r in,2 + jx in,2 z,1

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 2100 Circuit Analysis Lessn 25 Chapter 9 & App B: Passive circuit elements in the phasr representatin Daniel M. Litynski, Ph.D. http://hmepages.wmich.edu/~dlitynsk/ ECE 2100 Circuit Analysis Lessn

More information

Dr. Kasra Etemadi February 27, 2007

Dr. Kasra Etemadi February 27, 2007 Dr. Kasra Eteadi February 7, 7 Chapter 4:Transients Chapter 5: Sinusidal Surces Chapter 6: nnsinusidal surces Furier Trasr Transer Functin Filters Lwpass Filters Highpass Filters andpass Filters Surce

More information

Lecture 12 Date:

Lecture 12 Date: Lecture 12 Date: 09.02.2017 Microstrip Matching Networks Series- and Shunt-stub Matching Quarter Wave Impedance Transformer Microstrip Line Matching Networks In the lower RF region, its often a standard

More information

The Chebyshev Matching Transformer

The Chebyshev Matching Transformer /9/ The Chebyshev Matching Transforer /5 The Chebyshev Matching Transforer An alternative to Binoial (Maxially Flat) functions (and there are any such alternatives!) are Chebyshev polynoials. Pafnuty Chebyshev

More information

Simulation of Push-pull Multi-output Quasi-resonant Converter

Simulation of Push-pull Multi-output Quasi-resonant Converter IOSR Jurnal f Electrical and Electrnics Engineering (IOSR-JEEE) e-issn: 78-1676,p-ISSN: 3-3331, Vlue 9, Issue 1 Ver. V (Feb. 14), PP 19-4 Siulatin f Push-pull Multi-utput Quasi-resnant Cnverter T.Anitha

More information

MICROWAVE COMMUNICATIONS AND RADAR

MICROWAVE COMMUNICATIONS AND RADAR MICROWAVE COMMUNICATIONS AND RADAR Generic Architecture: Signal Amplificatin Guide Antenna Prcessing Micrwave r ptical Signal Prcessing Detectin Guide Antenna tuning, resnance waveguides transitins cupling

More information

Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax .7.4: Direct frequency dmain circuit analysis Revisin: August 9, 00 5 E Main Suite D Pullman, WA 9963 (509) 334 6306 ice and Fax Overview n chapter.7., we determined the steadystate respnse f electrical

More information

Fields and Waves I. Lecture 3

Fields and Waves I. Lecture 3 Fields and Waves I ecture 3 Input Impedance n Transmissin ines K. A. Cnnr Electrical, Cmputer, and Systems Engineering Department Rensselaer Plytechnic Institute, Try, NY These Slides Were Prepared by

More information

2. Find i, v, and the power dissipated in the 6-Ω resistor in the following figure.

2. Find i, v, and the power dissipated in the 6-Ω resistor in the following figure. CSC Class exercise DC Circuit analysis. Fr the ladder netwrk in the fllwing figure, find I and R eq. Slutin Req 4 ( 6 ) 5Ω 0 0 I Re q 5 A. Find i, v, and the pwer dissipated in the 6-Ω resistr in the fllwing

More information

ANTENNAS and MICROWAVES ENGINEERING (650427)

ANTENNAS and MICROWAVES ENGINEERING (650427) Philadelphia University Faculty of Engineering Communication and Electronics Engineering ANTENNAS and MICROWAVES ENGINEERING (65427) Part 2 Dr. Omar R Daoud 1 General Considerations It is a two-port network

More information

CHAPTER 5. Solutions for Exercises

CHAPTER 5. Solutions for Exercises HAPTE 5 Slutins fr Exercises E5. (a We are given v ( t 50 cs(00π t 30. The angular frequency is the cefficient f t s we have ω 00π radian/s. Then f ω / π 00 Hz T / f 0 ms m / 50 / 06. Furthermre, v(t attains

More information

Harmonic Motion (HM) Oscillation with Laminar Damping

Harmonic Motion (HM) Oscillation with Laminar Damping Harnic Mtin (HM) Oscillatin with Lainar Daping If yu dn t knw the units f a quantity yu prbably dn t understand its physical significance. Siple HM r r Hke' s Law: F k x definitins: f T / T / Bf x A sin

More information

Impedance Matching with Transmission Lines

Impedance Matching with Transmission Lines Impedance Matching with Transmission Lines /4 W Z L useful functions and identities Units Constants Table of Contents I. Introduction II. Inputs III. Transmission Line Synthesis Function IV. Single Shunt

More information

5.2 Single-Stub Tuning

5.2 Single-Stub Tuning 3/26/29 5_2 Sgle_Stub Tung.doc 1/1 5.2 Sgle-Stub Tung Readg Assignment: pp. 228-235 Q: If we cannot use lumped elements like ductors or capacitors to build lossless matchg networks, what can we use? A:

More information

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string? Term: 111 Thursday, January 05, 2012 Page: 1 Q1. A string f length L is fixed at bth ends. Which ne f the fllwing is NOT a pssible wavelength fr standing waves n this string? Q2. λ n = 2L n = A) 4L B)

More information

Series and Parallel Resonances

Series and Parallel Resonances Series and Parallel esnances Series esnance Cnsider the series circuit shwn in the frequency dmain. The input impedance is Z Vs jl jl I jc C H s esnance ccurs when the imaginary part f the transfer functin

More information

ECE 598 JS Lecture 08 Lossy Transmission Lines

ECE 598 JS Lecture 08 Lossy Transmission Lines ECE 598 JS Lecture 8 Lssy Transmissin Lines Spring 22 Jse E. Schutt-Aine Electrical & Cmputer Engineering University f Illinis jesa@illinis.edu Lss in Transmissin Lines RF SOURCE Signal amplitude decreases

More information

TC 412 Microwave Communications. Lecture 6 Transmission lines problems and microstrip lines

TC 412 Microwave Communications. Lecture 6 Transmission lines problems and microstrip lines TC 412 Microwave Communications Lecture 6 Transmission lines problems and microstrip lines RS 1 Review Input impedance for finite length line Quarter wavelength line Half wavelength line Smith chart A

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 00 Circuit Analysis Lessn 6 Chapter 4 Sec 4., 4.5, 4.7 Series LC Circuit C Lw Pass Filter Daniel M. Litynski, Ph.D. http://hmepages.wmich.edu/~dlitynsk/ ECE 00 Circuit Analysis Lessn 5 Chapter 9 &

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 4 Digital Signal Prcessing Pr. ar Fwler DT Filters te Set #2 Reading Assignment: Sect. 5.4 Prais & anlais /29 Ideal LP Filter Put in the signal we want passed. Suppse that ( ) [, ] X π xn [ ] y[ n]

More information

Copyright Paul Tobin 63

Copyright Paul Tobin 63 DT, Kevin t. lectric Circuit Thery DT87/ Tw-Prt netwrk parameters ummary We have seen previusly that a tw-prt netwrk has a pair f input terminals and a pair f utput terminals figure. These circuits were

More information

6-1 Chapter 6 Transmission Lines

6-1 Chapter 6 Transmission Lines 6-1 Chapter 6 Transmission ines ECE 3317 Dr. Stuart A. ong 6-2 General Definitions p.133 6-3 Voltage V( z) = α E ds ( C z) 1 C t t ( a) Current I( z) = α H ds ( C0 closed) 2 C 0 ( b) http://www.cartoonstock.com

More information

Transmission Line Theory

Transmission Line Theory S. R. Zinka zinka@vit.ac.in School of Electronics Engineering Vellore Institute of Technology April 26, 2013 Outline 1 Free Space as a TX Line 2 TX Line Connected to a Load 3 Some Special Cases 4 Smith

More information

Lecture 20a. Circuit Topologies and Techniques: Opamps

Lecture 20a. Circuit Topologies and Techniques: Opamps Lecture a Circuit Tplgies and Techniques: Opamps In this lecture yu will learn: Sme circuit tplgies and techniques Intrductin t peratinal amplifiers Differential mplifier IBIS1 I BIS M VI1 vi1 Vi vi I

More information

Solutions to Problems in Chapter 6

Solutions to Problems in Chapter 6 Appendix F Solutions to Problems in Chapter 6 F.1 Problem 6.1 Short-circuited transmission lines Section 6.2.1 (book page 193) describes the method to determine the overall length of the transmission line

More information

Module 4: General Formulation of Electric Circuit Theory

Module 4: General Formulation of Electric Circuit Theory Mdule 4: General Frmulatin f Electric Circuit Thery 4. General Frmulatin f Electric Circuit Thery All electrmagnetic phenmena are described at a fundamental level by Maxwell's equatins and the assciated

More information

Pre-Calculus Individual Test 2017 February Regional

Pre-Calculus Individual Test 2017 February Regional The abbreviatin NOTA means Nne f the Abve answers and shuld be chsen if chices A, B, C and D are nt crrect. N calculatr is allwed n this test. Arcfunctins (such as y = Arcsin( ) ) have traditinal restricted

More information

192 Chapter 4: Microwave Network Analysis

192 Chapter 4: Microwave Network Analysis 92 hapter 4: Microwave Network nalysis TLE 4.2 onversions etween Two-Port Network Parameters S Z Y S S (Z Z 0 )(2 + Z 0 ) (Y 0 Y )(Y 0 + Y 22 ) + Y 2 Y 2 + /Z 0 Z 0 + /Z 0 + Z 0 + S S 2Z 2 Z 0 2 2 2Y 2

More information

Physics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018

Physics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018 Michael Faraday lived in the Lndn area frm 1791 t 1867. He was 29 years ld when Hand Oersted, in 1820, accidentally discvered that electric current creates magnetic field. Thrugh empirical bservatin and

More information

ENGIN 211, Engineering Math. Complex Numbers

ENGIN 211, Engineering Math. Complex Numbers ENGIN 211, Engineering Math Complex Numbers 1 Imaginary Number and the Symbol J Consider the solutions for this quadratic equation: x 2 + 1 = 0 x = ± 1 1 is called the imaginary number, and we use the

More information

Lecture 14 Date:

Lecture 14 Date: Lecture 14 Date: 18.09.2014 L Type Matching Network Examples Nodal Quality Factor T- and Pi- Matching Networks Microstrip Matching Networks Series- and Shunt-stub Matching L Type Matching Network (contd.)

More information

Oscillator. Introduction of Oscillator Linear Oscillator. Stability. Wien Bridge Oscillator RC Phase-Shift Oscillator LC Oscillator

Oscillator. Introduction of Oscillator Linear Oscillator. Stability. Wien Bridge Oscillator RC Phase-Shift Oscillator LC Oscillator Oscillatr Intrductin f Oscillatr Linear Oscillatr Wien Bridge Oscillatr Phase-Shift Oscillatr L Oscillatr Stability Oscillatrs Oscillatin: an effect that repeatedly and regularly fluctuates abut the mean

More information

STABILITY ANALYSIS TECHNIQUES

STABILITY ANALYSIS TECHNIQUES ECE4540/5540: Digital Control Systems 4 1 STABILITY ANALYSIS TECHNIQUES 41: Bilinear transformation Three main aspects to control-system design: 1 Stability, 2 Steady-state response, 3 Transient response

More information

Section I5: Feedback in Operational Amplifiers

Section I5: Feedback in Operational Amplifiers Sectin I5: eedback in Operatinal mplifiers s discussed earlier, practical p-amps hae a high gain under dc (zer frequency) cnditins and the gain decreases as frequency increases. This frequency dependence

More information

Cop yri ht 2006, Barr Mabillard.

Cop yri ht 2006, Barr Mabillard. Trignmetry II Cpyright Trignmetry II Standards 006, Test Barry ANSWERS Mabillard. 0 www.math0s.cm . If csα, where sinα > 0, and 5 cs α + β value f sin β, where tan β > 0, determine the exact 9 First determine

More information

Introduction to Smith Charts

Introduction to Smith Charts Intrductin t Smith Charts Dr. Russell P. Jedlicka Klipsch Schl f Electrical and Cmputer Engineering New Mexic State University as Cruces, NM 88003 September 2002 EE521 ecture 3 08/22/02 Smith Chart Summary

More information

Review Problems 3. Four FIR Filter Types

Review Problems 3. Four FIR Filter Types Review Prblems 3 Fur FIR Filter Types Fur types f FIR linear phase digital filters have cefficients h(n fr 0 n M. They are defined as fllws: Type I: h(n = h(m-n and M even. Type II: h(n = h(m-n and M dd.

More information

Microwave Circuit Design I

Microwave Circuit Design I 9 1 Microwave Circuit Design I Lecture 9 Topics: 1. Admittance Smith Chart 2. Impedance Matching 3. Single-Stub Tuning Reading: Pozar pp. 228 235 The Admittance Smith Chart Since the following is also

More information

Precalculus A. Semester Exam Review

Precalculus A. Semester Exam Review Precalculus A 015-016 MCPS 015 016 1 The semester A eaminatin fr Precalculus cnsists f tw parts. Part 1 is selected respnse n which a calculatr will NOT be allwed. Part is shrt answer n which a calculatr

More information

Chapter 10: Sinusoidal Steady-State Analysis

Chapter 10: Sinusoidal Steady-State Analysis Chapter 0: Sinusoidal Steady-State Analysis Sinusoidal Sources If a circuit is driven by a sinusoidal source, after 5 tie constants, the circuit reaches a steady-state (reeber the RC lab with t τ). Consequently,

More information

MODULE 1. e x + c. [You can t separate a demominator, but you can divide a single denominator into each numerator term] a + b a(a + b)+1 = a + b

MODULE 1. e x + c. [You can t separate a demominator, but you can divide a single denominator into each numerator term] a + b a(a + b)+1 = a + b . REVIEW OF SOME BASIC ALGEBRA MODULE () Slving Equatins Yu shuld be able t slve fr x: a + b = c a d + e x + c and get x = e(ba +) b(c a) d(ba +) c Cmmn mistakes and strategies:. a b + c a b + a c, but

More information

ECE 5318/6352 Antenna Engineering. Spring 2006 Dr. Stuart Long. Chapter 6. Part 7 Schelkunoff s Polynomial

ECE 5318/6352 Antenna Engineering. Spring 2006 Dr. Stuart Long. Chapter 6. Part 7 Schelkunoff s Polynomial ECE 538/635 Antenna Engineering Spring 006 Dr. Stuart Lng Chapter 6 Part 7 Schelkunff s Plynmial 7 Schelkunff s Plynmial Representatin (fr discrete arrays) AF( ψ ) N n 0 A n e jnψ N number f elements in

More information

Time varying fields and Maxwell's equations Chapter 9

Time varying fields and Maxwell's equations Chapter 9 Tie varying fields and Maxwell's equatins hapter 9 Dr. Naser Abu-Zaid Page 9/7/202 FARADAY LAW OF ELETROMAGNETI INDUTION A tie varying agnetic field prduces (induces) a current in a clsed lp f wire. The

More information

PHYSICS Unit 3 Trial Examination

PHYSICS Unit 3 Trial Examination STAV Publishing Pty Ltd 005 PHYSICS Unit 3 Trial Examinatin SOLUTIONS BOOK Published by STAV Publishing Pty Ltd. STAV Huse, 5 Munr Street, Cburg VIC 3058 Australia. Phne: 6 + 3 9385 3999 Fax: 6 + 3 9386

More information

A Correlation of. to the. South Carolina Academic Standards for Mathematics Precalculus

A Correlation of. to the. South Carolina Academic Standards for Mathematics Precalculus A Crrelatin f Suth Carlina Academic Standards fr Mathematics Precalculus INTRODUCTION This dcument demnstrates hw Precalculus (Blitzer), 4 th Editin 010, meets the indicatrs f the. Crrelatin page references

More information

LEARNING : At the end of the lesson, students should be able to: OUTCOMES a) state trigonometric ratios of sin,cos, tan, cosec, sec and cot

LEARNING : At the end of the lesson, students should be able to: OUTCOMES a) state trigonometric ratios of sin,cos, tan, cosec, sec and cot Mathematics DM 05 Tpic : Trignmetric Functins LECTURE OF 5 TOPIC :.0 TRIGONOMETRIC FUNCTIONS SUBTOPIC :. Trignmetric Ratis and Identities LEARNING : At the end f the lessn, students shuld be able t: OUTCOMES

More information

Trigonometric Ratios Unit 5 Tentative TEST date

Trigonometric Ratios Unit 5 Tentative TEST date 1 U n i t 5 11U Date: Name: Trignmetric Ratis Unit 5 Tentative TEST date Big idea/learning Gals In this unit yu will extend yur knwledge f SOH CAH TOA t wrk with btuse and reflex angles. This extensin

More information

Preparation work for A2 Mathematics [2017]

Preparation work for A2 Mathematics [2017] Preparatin wrk fr A2 Mathematics [2017] The wrk studied in Y12 after the return frm study leave is frm the Cre 3 mdule f the A2 Mathematics curse. This wrk will nly be reviewed during Year 13, it will

More information

Lecture 13 Date:

Lecture 13 Date: ecture 13 Date: 29.02.2016 Quarter-wave Impedance Transformer The Theory of Small Reflections The Quarter Wave Transformer (contd.) The quarter-wave transformer is simply a transmission line with characteristic

More information

TRANSMISSION LINES AND MATCHING

TRANSMISSION LINES AND MATCHING TRANSMISSION LINES AND MATCHING for High-Frequency Circuit Design Elective by Michael Tse September 2003 Contents Basic models The Telegrapher s equations and solutions Transmission line equations The

More information

CHAPTER 45 COMPLEX NUMBERS

CHAPTER 45 COMPLEX NUMBERS CHAPTER 45 COMPLEX NUMBERS EXERCISE 87 Page 50. Solve the quadratic equation: x + 5 0 Since x + 5 0 then x 5 x 5 ( )(5) 5 j 5 from which, x ± j5. Solve the quadratic equation: x x + 0 Since x x + 0 then

More information

Synchronous Motor V-Curves

Synchronous Motor V-Curves Synchrnus Mtr V-Curves 1 Synchrnus Mtr V-Curves Intrductin Synchrnus mtrs are used in applicatins such as textile mills where cnstant speed peratin is critical. Mst small synchrnus mtrs cntain squirrel

More information

1. Transformer A transformer is used to obtain the approximate output voltage of the power supply. The output of the transformer is still AC.

1. Transformer A transformer is used to obtain the approximate output voltage of the power supply. The output of the transformer is still AC. PHYSIS 536 Experiment 4: D Pwer Supply I. Intrductin The prcess f changing A t D is investigated in this experiment. An integrated circuit regulatr makes it easy t cnstruct a high-perfrmance vltage surce

More information

ZVS Boost Converter. (a) (b) Fig 6.29 (a) Quasi-resonant boost converter with M-type switch. (b) Equivalent circuit.

ZVS Boost Converter. (a) (b) Fig 6.29 (a) Quasi-resonant boost converter with M-type switch. (b) Equivalent circuit. EEL6246 Pwer Electrnics II Chapter 6 Lecture 6 Dr. Sam Abdel-Rahman ZVS Bst Cnverter The quasi-resnant bst cnverter by using the M-type switch as shwn in Fig. 6.29(a) with its simplified circuit shwn in

More information

" W I T H M: A. L I G E T O ' W ^ P L D IST O ISTE -A-IsTD G H! A-I^IT Y IPO PL A.LI-i. :

 W I T H M: A. L I G E T O ' W ^ P L D IST O ISTE -A-IsTD G H! A-I^IT Y IPO PL A.LI-i. : : D D! Y : V Y JY 4 96 J z z Y &! 0 6 4 J 6 4 0 D q & J D J» Y j D J & D & Y = x D D DZ Z # D D D D D D V X D DD X D \ J D V & Q D D Y D V D D? q ; J j j \V ; q» 0 0 j \\ j! ; \?) j: ; : x DD D J J j ;

More information

Microelectronics Circuit Analysis and Design. NMOS Common-Source Circuit. NMOS Common-Source Circuit 10/15/2013. In this chapter, we will:

Microelectronics Circuit Analysis and Design. NMOS Common-Source Circuit. NMOS Common-Source Circuit 10/15/2013. In this chapter, we will: Mcrelectrncs Crcut Analyss and Desn Dnald A. Neaen Chapter 4 Basc FET Aplfers In ths chapter, we wll: Inestate a snle-transstr crcut that can aplfy a sall, te-aryn nput snal Deelp sall-snal dels that are

More information

Applying Kirchoff s law on the primary circuit. V = - e1 V+ e1 = 0 V.D. e.m.f. From the secondary circuit e2 = v2. K e. Equivalent circuit :

Applying Kirchoff s law on the primary circuit. V = - e1 V+ e1 = 0 V.D. e.m.f. From the secondary circuit e2 = v2. K e. Equivalent circuit : TRANSFORMERS Definitin : Transfrmers can be defined as a static electric machine which cnverts electric energy frm ne ptential t anther at the same frequency. It can als be defined as cnsists f tw electric

More information

Introduction. A microwave circuit is an interconnection of components whose size is comparable with the wavelength at the operation frequency

Introduction. A microwave circuit is an interconnection of components whose size is comparable with the wavelength at the operation frequency Introduction A microwave circuit is an interconnection of components whose size is comparable with the wavelength at the operation frequency Type of Components: Interconnection: it is not an ideal connection

More information

Lesson #15. Section BME 373 Electronics II J.Schesser

Lesson #15. Section BME 373 Electronics II J.Schesser Feedack and Ocillatr Len # Tranient and Frequency Repne Sectin 9.6- BME 373 Electrnic II J.Scheer 78 Cled-Lp Gain in the Frequency Dmain ume that th the pen-lp gain, and the eedack, β are unctin requency

More information

Chapter 8: Frequency Domain Analysis

Chapter 8: Frequency Domain Analysis Chapter 8: Frequency Domain Analysis Samantha Ramirez Preview Questions 1. What is the steady-state response of a linear system excited by a cyclic or oscillatory input? 2. How does one characterize the

More information

Chapter 10: Sinusoidal Steady-State Analysis

Chapter 10: Sinusoidal Steady-State Analysis Chapter 0: Sinusoidal Steady-State Analysis Sinusoidal Sources If a circuit is driven by a sinusoidal source, after 5 tie constants, the circuit reaches a steady-state (reeber the RC lab with t = τ). Consequently,

More information

Dr. Vahid Nayyeri. Microwave Circuits Design

Dr. Vahid Nayyeri. Microwave Circuits Design Lect. 8: Microwave Resonators Various applications: including filters, oscillators, frequency meters, and tuned amplifiers, etc. microwave resonators of all types can be modelled in terms of equivalent

More information

X (z) = n= 1. Ã! X (z) x [n] X (z) = Z fx [n]g x [n] = Z 1 fx (z)g. r n x [n] ª e jnω

X (z) = n= 1. Ã! X (z) x [n] X (z) = Z fx [n]g x [n] = Z 1 fx (z)g. r n x [n] ª e jnω 3 The z-transform ² Two advantages with the z-transform:. The z-transform is a generalization of the Fourier transform for discrete-time signals; which encompasses a broader class of sequences. The z-transform

More information

Supplementary Course Notes Adding and Subtracting AC Voltages and Currents

Supplementary Course Notes Adding and Subtracting AC Voltages and Currents Supplementary Curse Ntes Adding and Subtracting AC Vltages and Currents As mentined previusly, when cmbining DC vltages r currents, we nly need t knw the plarity (vltage) and directin (current). In the

More information

ANSWER KEY FOR MATH 10 SAMPLE EXAMINATION. Instructions: If asked to label the axes please use real world (contextual) labels

ANSWER KEY FOR MATH 10 SAMPLE EXAMINATION. Instructions: If asked to label the axes please use real world (contextual) labels ANSWER KEY FOR MATH 10 SAMPLE EXAMINATION Instructins: If asked t label the axes please use real wrld (cntextual) labels Multiple Chice Answers: 0 questins x 1.5 = 30 Pints ttal Questin Answer Number 1

More information

Introduction to Electronic circuits.

Introduction to Electronic circuits. Intrductn t Electrnc crcuts. Passve and Actve crcut elements. Capactrs, esstrs and Inductrs n AC crcuts. Vltage and current dvders. Vltage and current surces. Amplfers, and ther transfer characterstc.

More information

4) What is the magnitude of the net electric field at the center of the square?

4) What is the magnitude of the net electric field at the center of the square? Fur charges are n the fur crners f a square. Q = +5C, Q = -0C, Q 3 = +5C, Q 4 = -0C. The side length f each side f the square is 3 m. Q Q ) What is the directin f the frce n Q due t ONLY Q 4? (a) up (b)

More information

Signals and Systems. Lecture 11 Wednesday 22 nd November 2017 DR TANIA STATHAKI

Signals and Systems. Lecture 11 Wednesday 22 nd November 2017 DR TANIA STATHAKI Signals and Systems Lecture 11 Wednesday 22 nd November 2017 DR TANIA STATHAKI READER (ASSOCIATE PROFFESOR) IN SIGNAL PROCESSING IMPERIAL COLLEGE LONDON Effect on poles and zeros on frequency response

More information

PHYS College Physics II Final Examination Review

PHYS College Physics II Final Examination Review PHYS 1402- Cllege Physics II Final Examinatin Review The final examinatin will be based n the fllwing Chapters/Sectins and will cnsist f tw parts. Part 1, cnsisting f Multiple Chice questins, will accunt

More information

SFDMB3638F. Specifications and Applications Information. orce LED Driver. Mass: 7 grams typ. 10/15/08 Preliminary. Package Configuration

SFDMB3638F. Specifications and Applications Information. orce LED Driver. Mass: 7 grams typ. 10/15/08 Preliminary. Package Configuration Specificatins and Applicatins Infrmatin 1/1/8 Prelimary Smart Fr rce LED Driver The ERG Smart Frce Series f LED Drivers are specifically designed fr applicatins which require high efficiency, small ftprt

More information

STUDENT NAME: STUDENT id #: WORK ONLY 5 QUESTIONS

STUDENT NAME: STUDENT id #: WORK ONLY 5 QUESTIONS GENERAL PHYSICS PH -A (MIROV) Exam 3 (03/31/15) STUDENT NAME: STUDENT i #: ------------------------------------------------------------------------------------------------------------------------------------------

More information

Chapter 30. Inductance

Chapter 30. Inductance Chapter 30 nductance 30. Self-nductance Cnsider a lp f wire at rest. f we establish a current arund the lp, it will prduce a magnetic field. Sme f the magnetic field lines pass thrugh the lp. et! be the

More information

1.1 The main transmission network of Eskom The classical two generator model 11

1.1 The main transmission network of Eskom The classical two generator model 11 LIST OF FIGURS Figure Page 1.1 The main transmissin netwrk f skm 4 2.1 The classical tw generatr mdel 11 2.2 Obtaining the lcatin f the electrical centre. The line cnnecting A with B represents the netwrk

More information

2015 Regional Physics Exam Solution Set

2015 Regional Physics Exam Solution Set 05 Reginal hysics Exa Slutin Set. Crrect answer: D Nte: [quantity] dentes: units f quantity WYSE Acadeic Challenge 05 Reginal hysics Exa SOLUTION SET r F r a lengthass length / tie ass length / tie. Crrect

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

GENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS. J.e. Sprott. Plasma Studies. University of Wisconsin

GENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS. J.e. Sprott. Plasma Studies. University of Wisconsin GENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS J.e. Sprtt PLP 924 September 1984 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated.

More information

6.1 Introduction

6.1 Introduction 6. Introduction A.C Circuits made up of resistors, inductors and capacitors are said to be resonant circuits when the current drawn from the supply is in phase with the impressed sinusoidal voltage. Then.

More information

Characteristics of Passive IC Devices

Characteristics of Passive IC Devices 008/Oct 8 esistors Characteristics of Passive IC Devices Poly esistance Diffusion esistance Well esistance Parasitic esistance Capacitors Poly Capacitors MOS Capacitors MIM Capacitors Parasitic Capacitors

More information

Case Study: Parallel Coupled- Line Combline Filter

Case Study: Parallel Coupled- Line Combline Filter MICROWAVE AND RF DESIGN MICROWAVE AND RF DESIGN Case Study: Parallel Coupled- Line Combline Filter Presented by Michael Steer Reading: 6. 6.4 Index: CS_PCL_Filter Based on material in Microwave and RF

More information

1 PreCalculus AP Unit G Rotational Trig (MCR) Name:

1 PreCalculus AP Unit G Rotational Trig (MCR) Name: 1 PreCalculus AP Unit G Rtatinal Trig (MCR) Name: Big idea In this unit yu will extend yur knwledge f SOH CAH TOA t wrk with btuse and reflex angles. This extensin will invlve the unit circle which will

More information

Figure 1a. A planar mechanism.

Figure 1a. A planar mechanism. ME 5 - Machine Design I Fall Semester 0 Name f Student Lab Sectin Number EXAM. OPEN BOOK AND CLOSED NOTES. Mnday, September rd, 0 Write n ne side nly f the paper prvided fr yur slutins. Where necessary,

More information

Phys102 Second Major-102 Zero Version Coordinator: Al-Shukri Thursday, May 05, 2011 Page: 1

Phys102 Second Major-102 Zero Version Coordinator: Al-Shukri Thursday, May 05, 2011 Page: 1 Crdinatr: Al-Shukri Thursday, May 05, 2011 Page: 1 1. Particles A and B are electrically neutral and are separated by 5.0 μm. If 5.0 x 10 6 electrns are transferred frm particle A t particle B, the magnitude

More information

ECE357H1S ELECTROMAGNETIC FIELDS TERM TEST 1. 8 February 2016, 19:00 20:00. Examiner: Prof. Sean V. Hum

ECE357H1S ELECTROMAGNETIC FIELDS TERM TEST 1. 8 February 2016, 19:00 20:00. Examiner: Prof. Sean V. Hum UNIVERSITY OF TORONTO FACULTY OF APPLIED SCIENCE AND ENGINEERING The Edward S. Rogers Sr. Department of Electrical and Computer Engineering ECE57HS ELECTROMAGNETIC FIELDS TERM TEST 8 February 6, 9:00 :00

More information

Bicycle Generator Dump Load Control Circuit: An Op Amp Comparator with Hysteresis

Bicycle Generator Dump Load Control Circuit: An Op Amp Comparator with Hysteresis Bicycle Generatr Dump Lad Cntrl Circuit: An Op Amp Cmparatr with Hysteresis Sustainable Technlgy Educatin Prject University f Waterl http://www.step.uwaterl.ca December 1, 2009 1 Summary This dcument describes

More information

International Distinguished Lecturer Program

International Distinguished Lecturer Program U 005-006 International Distinguished Lecturer Program Ken-ya Hashimoto Chiba University Sponsored by The Institute of Electrical and Electronics Engineers (IEEE) Ultrasonics, Ferroelectrics and Frequency

More information

Pages with the symbol indicate that a student should be prepared to complete items like these with or without a calculator. tan 2.

Pages with the symbol indicate that a student should be prepared to complete items like these with or without a calculator. tan 2. Semester Eam Review The semester A eaminatin fr Hnrs Precalculus cnsists f tw parts. Part 1 is selected respnse n which a calculatr will NOT be allwed. Part is shrt answer n which a calculatr will be allwed.

More information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electrnc Crcuts Feedback & Stablty Sectns f Chapter 2. Kruger Feedback & Stablty Cnfguratn f Feedback mplfer S S S S fb Negate feedback S S S fb S S S S S β s the feedback transfer functn Implct

More information

Berkeley. The Smith Chart. Prof. Ali M. Niknejad. U.C. Berkeley Copyright c 2017 by Ali M. Niknejad. September 14, 2017

Berkeley. The Smith Chart. Prof. Ali M. Niknejad. U.C. Berkeley Copyright c 2017 by Ali M. Niknejad. September 14, 2017 Berkeley The Smith Chart Prof. Ali M. Niknejad U.C. Berkeley Copyright c 17 by Ali M. Niknejad September 14, 17 1 / 29 The Smith Chart The Smith Chart is simply a graphical calculator for computing impedance

More information

ENGI 4430 Parametric Vector Functions Page 2-01

ENGI 4430 Parametric Vector Functions Page 2-01 ENGI 4430 Parametric Vectr Functins Page -01. Parametric Vectr Functins (cntinued) Any nn-zer vectr r can be decmpsed int its magnitude r and its directin: r rrˆ, where r r 0 Tangent Vectr: dx dy dz dr

More information

CHAPTER 5: LAPLACE TRANSFORMS

CHAPTER 5: LAPLACE TRANSFORMS CHAPTER 5: LAPLACE TRANSFORMS SAMANTHA RAMIREZ PREVIEW QUESTIONS What are some commonly recurring functions in dynamic systems and their Laplace transforms? How can Laplace transforms be used to solve

More information

GATE : , Copyright reserved. Web:www.thegateacademy.com

GATE : , Copyright reserved. Web:www.thegateacademy.com GATE-2016 Index 1. Question Paper Analysis 2. Question Paper & Answer keys : 080-617 66 222, info@thegateacademy.com Copyright reserved. Web:www.thegateacademy.com ANALYSIS OF GATE 2016 Electrical Engineering

More information

Lecture #2 : Impedance matching for narrowband block

Lecture #2 : Impedance matching for narrowband block Lectue # : Ipedance atching f nawband blck ichad Chi-Hsi Li Telephne : 817-788-848 (UA) Cellula phne: 13917441363 (C) Eail : chihsili@yah.c.cn 1. Ipedance atching indiffeent f bandwidth ne pat atching

More information

Cambridge Assessment International Education Cambridge Ordinary Level. Published

Cambridge Assessment International Education Cambridge Ordinary Level. Published Cambridge Assessment Internatinal Educatin Cambridge Ordinary Level ADDITIONAL MATHEMATICS 4037/1 Paper 1 Octber/Nvember 017 MARK SCHEME Maximum Mark: 80 Published This mark scheme is published as an aid

More information

Supplementary Course Notes Adding and Subtracting AC Voltages and Currents

Supplementary Course Notes Adding and Subtracting AC Voltages and Currents Supplementary Curse Ntes Adding and Subtracting AC Vltages and Currents As mentined previusly, when cmbining DC vltages r currents, we nly need t knw the plarity (vltage) and directin (current). In the

More information

) Rotate L by 120 clockwise to obtain in!! anywhere between load and generator: rotation by 2d in clockwise direction. d=distance from the load to the

) Rotate L by 120 clockwise to obtain in!! anywhere between load and generator: rotation by 2d in clockwise direction. d=distance from the load to the 3.1 Smith Chart Construction: Start with polar representation of. L ; in on lossless lines related by simple phase change ) Idea: polar plot going from L to in involves simple rotation. in jj 1 ) circle

More information