Smith Chart Problems

Total Page:16

File Type:pdf, Size:1020Kb

Smith Chart Problems Smith Chart Problems 1. The 0:1 length line shown has acharacteristic imp edance of 50 and is terminated with a load imp edance of Z =5+j 25 . L Z L =0:1+j 0:5on the Smith chart. (a) Lo cate z = L Z 0 See the point plotted on the Smith chart. (b) What is the imp edance at ` =0:1? Since we want to move away from the load (i.e., toward the generator), read read 0:074 on the wavelengths toward generator scale and add ` =0:1 to obtain 0:174 on the wavelengths toward generator scale. A radial line from the center of the chart intersects the constant re ec- tion co ecient magnitude circle at z = 0:38 + j 1:88: Hence Z = zZ =50(0:38 + j 1:88) = 19 + 94 . 0 (c) What is the VSWR on the line? Find VSWR = z =13on the horizontal line to the right max of the chart's center. Or use the SWR scale on the chart. (d) What is ? L From the reflection coefficient scale below the chart, nd j j = 0:855. From the angle of reflection coef- L ficient scale on the p erimeter of the chart, nd the angle of j 126:5 = 126:5 . Hence =0:855e . L L (e) What is at ` =0:1 from the load? Note that jj = j j =0:855. Read the angle of the re ection L co ecient from the angle of reflection coefficient j 55:0 scale as 55:0 . Hence =0:855e . Problem 1 l = 0.1λ 01 Z50=Ω =+ Ω 0 ZL Z525[]L j l = 0.1λ 01 0.174λ .TG . 0.074λ .TG . AngΓ= 55.00 Γ= 0 AngL 126.5 =+ z0.10.5L j z=+ 0.38j 1.88 Γ=0.855 55.00 Γ= 0 L 0.855126.5 == VSWRzmax 13 VSWR= 13 Γ=Γ= L 0.855 2. A transmission line has Z =1:0, Z = z =0:2 j 0:2 : 0 L L (a) What is z at ` = =0:25? 4 From the chart, read 0:467 from the wavelengths to- ward generator scale. Add 0:25 to obtain 0:717 on the wavelengths toward generator scale. This is not on the chart, but since it rep eats every half wavelength, it is the same as 0:717 0:500 = 0:217. Drawing a ra- dial line from the center of the chart, we nd an intersec- tion with the constant re ection co ecient magnitude circle at z = Z =2:5+j 2:5. (b) What is the VSWR on the line? From the intersection of the constant re ection co ecientcir- cle with the right hand side of the horizontal axis, read VSWR = z =5:3: max (c) How far from the load is the rst voltage minimum? The rst current minimum? The voltage minimum o ccurs at z which is at a distance of min 0:500 0:467 =0:033 from the load. Or read this distance directly on the wavelengths toward load scale. The current minimum o ccurs at z which is a quarter of a max wavelength farther down the line or at 0:033 +0:25 =0:283 from the load. Problem 2 l = 0.25λ Z=Ω 1.0 == − ΩΩ 0 ZL ZLL z 0.2j 0.2 [ / ] l = 0.25λ 0.217λ .TG . zZ2.52.5== +j zmin λ == 0.033 VSWRzmax 5.3 =− z0.20.2L j 0.467λ .TG . VSWR= 5.3 3. The air- lled two-wire line has a characteristic imp edance of 50 and is op erated at f =3 GHz. The load is Z = 100 + j 40 . L (a) For the line ab ove, nd z on the chart. L 100 + j 40 Z L = The normalized load is z = = 2:0+ j 0:8. L Z 50 0 See the Smith chart for lo cation of p oint. (b) What is the line imp edance 2:5cm from the load? 10 3 10 cm/sec c = = 10 cm: Since we are Note that = 9 f 3 10 Hz going to move toward the generator (away from the load), at the normalized load p osition, rst read 0:217 on the wave- lengths toward generator scale. Then add 2.5 cm/10 cm = 0:25 to this value to obtain 0:467 on the wave- lengths toward generator scale. A radial line from the center at this p oint intersects the constant re ection co- ecient magnitude circle at z =0:43 j 0:17, so Z = zZ = 0 50(0:43 + j 0:17) = 21:5 j 8:5 . (c) What is the VSWR on the line? From the intersection of the re ection co ecient circle and the horizontal axis on the right hand side of the chart, read VSWR = 2.4. Or use the SWR scale belowthe chart. Problem 3 l = 2.5 [cm] Z=Z z → Z=Ω= 50 ,f 3GHz =+ Ω 0 0 ZL ZL 100j 40 [ ] 0.217λ .TG . =+ z2.00.8L j == VSWRzmax 2.4 z=− 0.43j 0.17 0.467λ .TG . l = 0.25λ 4. The line shown is 3=8 long and its normalized input imp edance is z = j 2:5: (a) What is the normalized receiving or load end imp edance, z ? L Since wemust movetoward the load to nd the load imp edance, lo cate z = j 2:5 on the chart and nd the intersection on the wavelengths toward load scale at 0:189. Add the dis- tance 3=8 = 0:375 to get 0:064 on the wavelengths toward load scale. At the intersection of the line from the center of the chart and the constant re ection co ecient circle, read z = j 0:425. L (b) What is the distance from the load to the rst voltage minimum? The voltage minimum o ccurs at the imp edance minimum on the horizontal line to the left of the chart's center. This dis- tance can be read directly o the wavelengths toward load scale (why?) as 0:064. Note that the line imp edance at the voltage minimum would b e that of a short circuit. (c) What length of op en-circuited line could b e used to replace z ? L From the p osition of z ,wewanttomovetoward the new load L (i.e., toward the end of the op en-circuited line) until wereach the op en circuit condition z = 1. This o ccurs at 0:25 on the wavelengths toward load scale and the total distance moved is hence 0:25 0:064 =0:186, which is the length of op en-circuited line needed to replace z . L Problem 4 λ l = 3 8 z2.5=−j → zL """ """! open circuited line section replacing original load zL λ l = 3 8 Vmin z =∞ 0.064 λ z2.5=−j =− zL j 0.425 0.064λ .T.L. 0.189λ .T.L. 0.186 λ 5. An air- lled 50 coaxial line has a loaded VSWR of 3.3 at a frequency of 3GHz. Replacing the load with a short causes the voltage minimum to move 1.0 cm towards the generator. What is the normalized load imp edance? For an air- lled line, the wavelength is 10 c 3 10 cm/sec = = = 10 cm: 9 f 3 10 Hz With the VSWR lo cated at z =3:3, draw the circle of con- max stant re ection co ecient magnitude. With the load in place, our only information is the lo cation of a voltage minimum (equivalent to an imp edance minimum). But thinking of the Smith chart as a crank diagram, we know that the voltage minimum must be at the intersection of the constant re ection co ecient circle and the horizontal axis on the left hand side of the chart between z =0 and z =1:0, (i.e., at z =0:3). With this information, min we have thus established a corresp ondence between a lo cation on the line and a point on the chart. Now, move from this 1:0cm minimum voltage point on the chart =0:1 toward the 10:0cm generator to the lo cation where the voltage minimum was mea- sured in the shorted line measurement. Since it was obtained from a shorted line measurement, the lo cation of this p ointmust be an integral number of half-wavelengths from the load (and hence must have the same line imp edance as at the load). The normalized imp edance here is therefore z =0:44 + j 0:63. For a L line with a 50 characteristic imp edance, the load imp edance is thus Z = 50(0:44 + j 0:63) = 22 + j 31:5: L Problem 5 0.10 λ =+ zL 0.44j 0.63 Vmin VSWR= 3.3 6. A slotted line measurement on an air- lled TEM line yields a VSWR of 1.6 at a frequency of 1 GHz. When the load is replaced by a short, the voltage minimum moves 3 cm towards the load. Find the normalized load imp edance. Lo cate the re ection co ecient circle by its intersection with z = VSWR = 1:6. The wavelength for an air- lled TEM max line is 10 3 10 cm/s = c=f = =30cm: 9 10 Hz Hence the shift in the voltage minimum is 3cm =0:1: 30 cm= Lo cate the voltage minimum at the imp edance minimum, z = min 0:625 and move 0:1 toward the load to a p osition an integral numb er of half-wavelengths from the load.
Recommended publications
  • Smith Chart Tutorial
    Frank Lynch, W4FAL Smith Charts Frank A. Lynch W 4FA L Page 1 24 April 2008 “SCARS” http://smithchart.org Frank Lynch, W4FAL Smith Chart History • Invented by Phillip H. Smith in 1939 • Used to solve a variety of transmission line and waveguide problems Basic Uses For evaluating the rectangular components, or the magnitude and phase of an input impedance or admittance, voltage, current, and related transmission functions at all points along a transmission line, including: • Complex voltage and current reflections coefficients • Complex voltage and current transmission coefficents • Power reflection and transmission coefficients • Reflection Loss • Return Loss • Standing Wave Loss Factor • Maximum and minimum of voltage and current, and SWR • Shape, position, and phase distribution along voltage and current standing waves Page 2 24 April 2008 Frank Lynch, W4FAL Basic Uses (continued) For evaluating the effects of line attenuation on each of the previously mentioned parameters and on related transmission line functions at all positions along the line. For evaluating input-output transfer functions. Page 3 24 April 2008 Frank Lynch, W4FAL Specific Uses • Evaluating input reactance or susceptance of open and shorted stubs. • Evaluating effects of shunt and series impedances on the impedance of a transmission line. • For displaying and evaluating the input impedance characteristics of resonant and anti-resonant stubs including the bandwidth and Q. • Designing impedance matching networks using single or multiple open or shorted stubs. • Designing impedance matching networks using quarter wave line sections. • Designing impedance matching networks using lumped L-C components. • For displaying complex impedances verses frequency. • For displaying s-parameters of a network verses frequency.
    [Show full text]
  • Smith Chart Calculations
    The following material was extracted from earlier edi- tions. Figure and Equation sequence references are from the 21st edition of The ARRL Antenna Book Smith Chart Calculations The Smith Chart is a sophisticated graphic tool for specialized type of graph. Consider it as having curved, rather solving transmission line problems. One of the simpler ap- than rectangular, coordinate lines. The coordinate system plications is to determine the feed-point impedance of an consists simply of two families of circles—the resistance antenna, based on an impedance measurement at the input family, and the reactance family. The resistance circles, Fig of a random length of transmission line. By using the Smith 1, are centered on the resistance axis (the only straight line Chart, the impedance measurement can be made with the on the chart), and are tangent to the outer circle at the right antenna in place atop a tower or mast, and there is no need of the chart. Each circle is assigned a value of resistance, to cut the line to an exact multiple of half wavelengths. The which is indicated at the point where the circle crosses the Smith Chart may be used for other purposes, too, such as the resistance axis. All points along any one circle have the same design of impedance-matching networks. These matching resistance value. networks can take on any of several forms, such as L and pi The values assigned to these circles vary from zero at the networks, a stub matching system, a series-section match, and left of the chart to infinity at the right, and actually represent more.
    [Show full text]
  • Slotted Line-SWR
    Lab 2: Slotted Line and SWR Meter NAME NAME NAME Introduction: In this lab you will learn how to characterize and use a 50-ohm slotted line, crystal detector, and standing wave ratio (SWR) meter to measure an unknown impedance. The apparatus used is shown below. The slotted line is a (rigid) continuation of the coaxial transmission lines. Its characteristic impedance is 50 ohms. It has a thin slot in its outer conductor, cut along z. A probe rides within (but not touching) the slot to sample the transmission line voltage. The probe can be moved along z to sample the standing wave ratio at different locations. It can also be moved into and out of the slot by means of a micrometer in order to adjust the signal strength. The probe is connected to a crystal (diode) detector that converts the time-varying microwave voltage to a DC value with the help of a low speed modulation envelope (1 kHz) on the microwave signal. The DC voltage is measured using the SWR meter (HP 415D). 1 Using Slotted Line to Measure an Unknown Impedance: The magnitude of the line voltage as a function of position is: + −2 jβ l + j(θ −2β l ) jθ V ()z = V0 1− Γe = V0 1+ Γ e with Γ = Γ e and l the distance from the load towards the generator. Notice that the voltage magnitude has maxima and minima at different locations. + Vmax = V0 (1+ Γ ) when θ − 2β l = π + Vmin = V0 (1− Γ ) when θ − 2β l = 0 V 1+ Γ The SWR is defined as: SWR = max = .
    [Show full text]
  • Smith Chart Examples
    SMITH CHART EXAMPLES Dragica Vasileska ASU Smith Chart for the Impedance Plot It will be easier if we normalize the load impedance to the characteristic impedance of the transmission line attached to the load. Z z = = r + jx Zo 1+ Γ z = 1− Γ Since the impedance is a complex number, the reflection coefficient will be a complex number Γ = u + jv 2 2 2v 1− u − v x = r = 2 2 ()1− u 2 + v2 ()1− u + v Real Circles 1 Im {Γ} 0.5 r=0 r=1/3 r=1 r=2.5 1 0.5 0 0.5 1 Re {Γ} 0.5 1 Imaginary Circles Im 1 {Γ} x=1/3 x=1 x=2.5 0.5 Γ 1 0.5 0 0.5 1 Re { } x=-1/3 x=-1 x=-2.5 0.5 1 Normalized Admittance Y y = = YZ o = g + jb Yo 1− Γ y = 1+ Γ 2 1− u 2 − v2 g 1 u + + v2 = g = 2 ()1+ u 2 + v2 1+ g ()1+ g − 2v 2 b = 2 1 1 2 2 ()u +1 + v + = ()1+ u + v b b2 These are equations for circles on the (u,v) plane Real admittance 1 Im {Γ} 0.5 g=2.5 g=1 g=1/3 1 0.5 0 0.5Re {Γ} 1 0.5 1 Complex Admittance 1 Im {Γ} b=-1 b=-1/3 b=-2.5 0.5 1 0.5 0 0.5Re {Γ 1} b=2.5 b=1/3 0.5 b=1 1 Matching • For a matching network that contains elements connected in series and parallel, we will need two types of Smith charts – impedance Smith chart – admittance Smith Chart • The admittance Smith chart is the impedance Smith chart rotated 180 degrees.
    [Show full text]
  • Department of Electronics and Communication Engineering EC8651 – Transmission Line and Waveguide Unit III - MCQ Bank 1
    ChettinadTech Dept of ECE Department of Electronics and Communication Engineering EC8651 – Transmission Line and Waveguide Unit III - MCQ Bank 1. Slotted line is a transmission line configuration that allows the sampling of a) electric field amplitude of a standing wave on a terminated line b) magnetic field amplitude of a standing wave on a terminated line c) voltage used for excitation d) current that is generated by the source Answer: a Explanation: Slotted line allows the sampling of the electric field amplitude of a standing wave on a terminated line. With this device, SWR and the distance of the first voltage minimum from the load can be measured, from this data, load impedance can be found. 2. A slotted line can be used to measure _____ and the distance of _____________ from the load. a) SWR, first voltage minimum b) SWR, first voltage maximum c) characteristic impedance, first voltage minimum d) characteristic impedance, first voltage maximum Answer: a Explanation: With a slotted line, SWR and the distance of the first voltage minimum from the load can be measured, from this data, load impedance can be found. Page 1 EC8651– Transmission Line and Waveguide ChettinadTech Dept of ECE 3. A modern device that replaces a slotted line is: a) Digital CRO b) generators c) network analyzers d) computers Answer: c Explanation: Although slotted lines used to be the principal way of measuring unknown impedance at microwave frequencies, they have largely been superseded by the modern network analyzer in terms of accuracy, versatility and convenience. 4. If the standing wave ratio for a transmission line is 1.4, then the reflection coefficient for the line is: a) 0.16667 b) 1.6667 c) 0.01667 d) 0.96 Answer: a Explanation: ┌= (SWR-1)/ (SWR+1).
    [Show full text]
  • Smith Chart • Smith Chart Was Developed by P
    Smith Chart • Smith Chart was developed by P. Smith at the Bell Lab in 1939 • Smith Chart provides an very useful way of visualizing the transmission line phenomenon and matching circuits. • In this slide, for convenience, we assume the normalized impedance is 50 Ohm. Smith Chart and Reflection coefficient Smith Chart is a polar plot of the voltage reflection coefficient, overlaid with impedance grid. So, you can covert the load impedance to reflection coefficient and vice versa. Smith Chart and impedance Examples: The upper half of the smith chart is for inductive impedance. The lower half of the is for capacitive impedance. Constant Resistance Circle This produces a circle where And the impedance on this circle r = 1 with different inductance (upper circle) and capacitance (lower circle) More on Constant Impedance Circle The circles for normalized rT = 0.2, 0.5, 1.0, 2.0 and 5.0 with Constant Inductance/Capacitance Circle Similarly, if xT is hold unchanged and vary the rT You will get the constant Inductance/capacitance circles. Constant Conductance and Susceptance Circle Reflection coefficient in term of admittance: And similarly, We can draw the constant conductance circle (red) and constant susceptance circles(blue). Example 1: Find the reflection coefficient from input impedance Example1: Find the reflection coefficient of the load impedance of: Step 1: In the impedance chart, find 1+2j. Step 2: Measure the distance from (1+2j) to the Origin w.r.t. radius = 1, which is read 0.7 Step 3: Find the angle, which is read 45° Now if we use the formula to verify the result.
    [Show full text]
  • Impedance Matching
    Impedance Matching Advanced Energy Industries, Inc. Introduction The plasma industry uses process power over a wide range of frequencies: from DC to several gigahertz. A variety of methods are used to couple the process power into the plasma load, that is, to transform the impedance of the plasma chamber to meet the requirements of the power supply. A plasma can be electrically represented as a diode, a resistor, Table of Contents and a capacitor in parallel, as shown in Figure 1. Transformers 3 Step Up or Step Down? 3 Forward Power, Reflected Power, Load Power 4 Impedance Matching Networks (Tuners) 4 Series Elements 5 Shunt Elements 5 Conversion Between Elements 5 Smith Charts 6 Using Smith Charts 11 Figure 1. Simplified electrical model of plasma ©2020 Advanced Energy Industries, Inc. IMPEDANCE MATCHING Although this is a very simple model, it represents the basic characteristics of a plasma. The diode effects arise from the fact that the electrons can move much faster than the ions (because the electrons are much lighter). The diode effects can cause a lot of harmonics (multiples of the input frequency) to be generated. These effects are dependent on the process and the chamber, and are of secondary concern when designing a matching network. Most AC generators are designed to operate into a 50 Ω load because that is the standard the industry has settled on for measuring and transferring high-frequency electrical power. The function of an impedance matching network, then, is to transform the resistive and capacitive characteristics of the plasma to 50 Ω, thus matching the load impedance to the AC generator’s impedance.
    [Show full text]
  • Beyond the Smith Chart
    IMAGE LICENSED BY GRAPHIC STOCK Beyond the Smith Chart Eli Bloch and Eran Socher he topic of impedance transformation and Since CMOS technology was primarily and ini- matching is one of the well-established tially developed for digital purposes, the lack of and essential aspects of microwave engi- high-quality passive components made it practically neering. A few decades ago, when discrete useless for RF design. The device speed was also radio-frequency (RF) design was domi- far inferior to established III-V technologies such as Tnant, impedance matching was mainly performed us- GaAs heterojunction bipolar transistors (HBTs) and ing transmission-lines techniques that were practical high-electron mobility transistors (HEMTs). The first due to the relatively large design size. As microwave RF CMOS receiver was constructed at 1989 [1], but design became possible using integrated on-chip com- it would take another several years for a fully inte- ponents, area constraints made LC- section match- grated CMOS RF receiver to be presented. The scal- ing (using lumped passive elements) more practical ing trend of CMOS in the past two decades improved than transmission line matching. Both techniques are the transistors’ speed exponentially, which provided conveniently visualized and accomplished using the more gain at RF frequencies and also enabled opera- well-known graphical tool, the Smith chart. tion at millimeter-wave (mm-wave) frequencies. The Eli Bloch ([email protected]) is with the Department of Electrical Engineering, Technion— Israel Institute of Technology, Haifa 32000, Israel. Eran Socher ([email protected]) is with the School of Electrical Engineering, Tel-Aviv University, 69978, Israel.
    [Show full text]
  • Microwave Impedance Measurements and Standards
    NBS MONOGRAPH 82 MICROWAVE IMPEDANCE MEASUREMENTS AND STANDARDS . .5, Y 1 p p R r ' \ Jm*"-^ CCD 'i . y. s. U,BO»WOM t «• U.S. DEPARTMENT OF STANDARDS NATIONAL BUREAU OF STANDARDS THE NATIONAL BUREAU OF STANDARDS The National Bureau of Standards is a principal focal point in the Federal Government for assuring maximum application of the physical and engineering sciences to the advancement of technology in industry and commerce. Its responsibilities include development and main- tenance of the national standards of measurement, and the provisions of means for making measurements consistent with those standards; determination of physical constants and properties of materials; development of methods for testing materials, mechanisms, and struc- tures, and making such tests as may be necessary, particularly for government agencies; cooperation in the establishment of standard practices for incorporation in codes and specifications; advisory service to government agencies on scientific and technical problems; invention and development of devices to serve special needs of the Government; assistance to industry, business, and consumers in the development and acceptance of commercial standards and simplified trade practice recommendations; administration of programs in cooperation with United States business groups and standards organizations for the development of international standards of practice; and maintenance of a clearinghouse for the collection and dissemination of scientific, technical, and engineering information. The scope of the Bureau's activities is suggested in the following listing of its four Institutes and their organizational units. Institute for Basic Standards. Applied Mathematics. Electricity. Metrology. Mechanics. Heat. Atomic Physics. Physical Chem- istry. Laboratory Astrophysics.* Radiation Physics. Radio Stand- ards Laboratory:* Radio Standards Physics; Radio Standards Engineering.
    [Show full text]
  • 36 Smith Chart and VSWR
    36 Smith Chart and VSWR Generator Transmission line I d ( ) Wire 2 + Load Z + g V d Zo • Consider the general phasor expressions - ( ) ZL F = Vg - Wire 1 l d V +ejβd(1 − Γ e−j2βd) 0 + jβd −j2βd L |V (d)|max V (d)=V e (1 + ΓLe ) and I(d)= |V (d)| Zo describing the voltage and current variations on TL’s in sinusoidal |V (d)|min dmax steady-state. dmin – Complex addition displayed Unless ΓL =0,thesephasorscontainreflectedcomponents,which graphically superposed on a means that voltage and current variations on the line “contain” Smith Chart standing waves. SmithChart 1 .5 2 In that case the phasors go through cycles of magnitude variations as a function of d,andinthevoltagemagnitudeinparticular(seemargin) .2 z(dmaxx!5) ( d) Γ(d) varying as 1+Γ =VSWR .2 .5 1 2 r!5 + −j2βd + 0 VSWR |V (d)| = |V ||1+ΓLe | = |V ||1+Γ(d)| 1 Γ(dmax)=|ΓL| takes maximum and minimum values of ".2 x!"5 + + |V (d)|max = |V |(1 + |ΓL|) and |V (d)|min = |V |(1 −|ΓL|) ".5 "2 "1 at locations d = dmax and dmin such that |1+Γ(d)| maximizes for d = dmax −j2βdmax −j2βdmin Γ(dmax)=ΓLe = |ΓL| and Γ(dmin)=ΓLe = −|ΓL|, |1+Γ(d)| minimizes for d = dmin and such that Γ(dmin)=−Γ(dmax) λ d − d is an odd multiple of . max min 4 1 Generator Transmission line I d – These results can be most easily understood and verified graphi- ( ) Wire 2 + Load cally on a SC as shown in the margin. + Zg Z - V (d) o ZL F = Vg - Wire 1 l d • We define a parameter known as voltage standing wave ratio,or 0 |V (d)|max VSWR for short, by |V (d)| |V (d)|min dmax |V (dmax)| 1+|ΓL| VSWR − 1 VSWR ≡ = ⇔|ΓL| = .
    [Show full text]
  • EECS 117A Demonstration 2 Microwave Measurement Instruments
    University of California, Berkeley Spring 2007 EECS 117 Prof. A. Niknejad EECS 117A Demonstration 2 Microwave Measurement Instruments NAME Introduction. Please review the general sinusoidal wave concepts in Secs. 3.1–3.9 of Inan & Inan. Note carefully Section 3.3. In this demonstration you will learn how to use a “50 ohm” slotted line, crystal detector, and standing wave ratio meter to obtain the wavelength λ and voltage standing wave ratio S on a coaxial transmission line. In a later demonstration you will use these techniques to measure and control impedances and reflection coefficients on a microwave transmission system. The apparatus used is shown below. The slotted line is a (rigid) continuation of the coaxial transmission lines “a” connected at each end. It has a thin slot in its outer conductor, cut along z. A probe rides within (but not touching) the slot to sample the transmission line voltage. The probe can be moved along z, and can also be moved into and out of the slot by means of a micrometer. The probe is connected to a crystal (diode) detector that converts the time-varying microwave voltage to dc. The dc voltage is measured using the standing wave ratio (SWR) meter. MICROMETER HP 415D b SWR METER DETECTOR TUNER HP 612 A UHF SIGNAL a TERMINATION GENERATOR a GR SLOTTED LINE POINT (LOAD) Z = 0 Z Suppose a sinusoidal voltage wave j(ωt−βz) v+(t) = Re hV+ e i (1) travels from the RF generator through the slotted line and is incident on a load (resistor, capacitor etc.) at z = 0.
    [Show full text]
  • S-Parameter Simulation and Optimization
    S-parameter Simulation and Optimization ADS 2009 (version 1.0) Copyright Agilent Technologies 2009 Slide 5 - 1 S-parameters are Ratios Usually given in dB as 20 log of the voltage ratios of the waves at the ports: incident, reflected, or transmitted. S-parameter (ratios): out / in • S11 - Forward Reflection (input match - impedance) Best viewed on a • S22 - Reverse Reflection (output match - impedance) Smith chart. • S21 - Forward Transmission (gain or loss) These are easier • S12 - Reverse Transmission (leakage or isolation) to understand and simply plotted. Results of an S-Parameter Simulation in ADS • S-matrix with all complex values at each frequency point • Read the complex reflection coefficient (Gamma) • Change the marker readout for Zo • Smith chart plots for impedance matching • Results are similar to Network Analyzer measurements Next, ADS data ADS 2009 (version 1.0) Copyright Agilent Technologies 2009 Slide 5 - 2 Typical S-parameter data in ADS Transmission: S21 Reflection: S11 magnitude vs frequency Impedance on a Smith Chart Complete S-matrix with port impedance Note: Smith marker impedance readout is changed to Zo = 50 ohms. Smith chart basics... ADS 2009 (version 1.0) Copyright Agilent Technologies 2009 Slide 5 - 3 The Impedance Smith Chart simplified... This is an impedance chart transformed from rectangular Z. Normalized to 50 ohms, the center = R50+J0 or Zo (perfect match). For S11 or S22 (two-port), you get the complex impedance. Circles of constant Resistance 16.7 50 150 SHORT OPEN 25 50 100 Lines of constant Reactance (+jx above and -jx below) Zo (characteristic impedance) = 50 + j0 More Smith chart..
    [Show full text]