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`Transmission LinesSmith ChartThe Smith chart is one of the most useful graphical tools for high frequency circuit applications. The chart provides a clever way to visualize complex functions and it continues to endure popularity, decades after its original conception. From a mathematical point of view, the Smith chart is a 4-D representation of all possible complex impedances with respect to coordinates defined by the complex reflection coefficient.Im( )1Re( )The domain of definition of the reflection coefficient for a loss-less line is a circle of unitary radius in the complex plane. This is also the domain of the Smith chart. In the case of a general lossy line, the reflection coefficient might have magnitude larger than one, due to the complex characteristic impedance, requiring an extended Smith chart.© Amanogawa, 2006 - Digital Maestro Series165Transmission LinesThe goal of the Smith chart is to identify all possible impedances on the domain of existence of the reflection coefficient. To do so, we start from the general definition of line impedance (which is equally applicable to a load impedance when d=0)V(d) 1+ (d) Z( d ) = = Z0 1 - (d) I(d)This provides the complex function Z( d ) = f {Re (  ) , Im (  )} that we want to graph. It is obvious that the result would be applicable only to lines with exactly characteristic impedance Z0. In order to obtain universal curves, we introduce the concept of normalized impedanceZ (d ) 1+ (d ) zn ( d ) = = Z0 1- (d )© Amanogawa, 2006 - Digital Maestro Series 166Transmission LinesThe normalized impedance is represented on the Smith chart by using families of curves that identify the normalized resistance r (real part) and the normalized reactance x (imaginary part)zn ( d ) = Re ( zn ) + j Im ( zn ) = r + jxLet's represent the reflection coefficient in terms of its coordinates ( d ) = Re (  ) + j Im (  )Now we can write1 + Re (  ) + j Im (  ) r + jx = 1 - Re (  ) - j Im (  ) = 1 - Re2 (  ) - Im2 (  ) + j 2 Im (  )(1 - Re (  ) )2+ Im2 (  )167© Amanogawa, 2006 - Digital Maestro SeriesTransmission LinesThe real part givesr=1 - Re2(  ) - Im2 (  )2Add a quantity equal to zero( 1 - Re (  ) )2 + Im 2 (  )=0r ( Re (  ) - 1 ) + Re(2() - 12) + r Im )12(  ) + Im (  ) +21 1+ r-1 1+ r=0 r ( Re (  ) - 1 )2 +  ( Re() - 1 + ( 1 + r ) Im 2 (  ) = 1 +  1 + r 1+ r2  2  r r 1 2 ( 1 + r )  Re (  ) - 2 Re (  ) + + ( 1 + r ) Im (  ) = 2 1 + r (1 + r )  1+ r  Re (  ) -     1 + rr2+ Im2() =( )1 1+ r2Equation of a circle© Amanogawa, 2006 - Digital Maestro Series168Transmission LinesThe imaginary part givesx= x22 Im (  )Multiply by x and add a quantity equal to zero( 1 - Re (  ) )2 + Im2 (  )( 1 - Re (  ) ) 2 + Im2 (  )  - 2 x Im (  ) + 1 - 1 = 0  =0( 1 - Re (  ) ) 2 + Im 2 (  )  - 2 Im (  ) + 1 = 1   x 2 2 x x 2 1  1 2  2 ( 1 - Re (  ) ) +  Im (  ) - Im (  ) + 2  = 2 x  x  x 1  Im (  ) - = ( Re (  ) - 1 ) + 2    x x212Equation of a circle© Amanogawa, 2006 - Digital Maestro Series169Transmission LinesThe result for the real part indicates that on the complex plane with coordinates (Re(), Im()) all the possible impedances with a given normalized resistance r are found on a circle with r  ,0 Center =   1+ r 1 Radius = 1+ rAs the normalized resistance r varies from 0 to  , we obtain a family of circles completely contained inside the domain of the reflection coefficient |  |  1 .Im( )r=1Re( )r=5r=0r = 0.5r 170© Amanogawa, 2006 - Digital Maestro SeriesTransmission LinesThe result for the imaginary part indicates that on the complex plane with coordinates (Re(), Im()) all the possible impedances with a given normalized reactance x are found on a circle with 1 Center =  1 ,   x1 Radius = xAs the normalized reactance x varies from - to  , we obtain a family of arcs contained inside the domain of the reflection coefficient |  |  1 .Im( )x=1 x ±Re( )x = 0.5 x=0 x = - 0.5© Amanogawa, 2006 - Digital Maestro Seriesx = -1171Transmission LinesBasic Smith Chart techniques for loss-less transmission lines Given Z(d) Given (d) Find (d)  Find Z(d)  Find (d) and Z(d)  Find R and ZRGiven R and ZR Given (d) and Z(d)Find dmax and dmin (maximum and minimum locations for the voltage standing wave pattern) Find the Voltage Standing Wave Ratio (VSWR) Given Z(d) Given Y(d) Find Y(d)  Find Z(d)© Amanogawa, 2006 - Digital Maestro Series172Transmission LinesGiven Z(d) Find (d)1.Normalize the impedanceZ (d) R X zn ( d ) = = + j =r+ j x Z0 Z0 Z02. 3. 4. Find the circle of constant normalized resistance r Find the arc of constant normalized reactance x The intersection of the two curves indicates the reflection coefficient in the complex plane. The chart provides directly the magnitude and the phase angle of (d)Example: Find (d), givenZ ( d ) = 25 + j 100 with Z0 = 50 © Amanogawa, 2006 - Digital Maestro Series173Transmission Lines1. Normalizationzn (d) = (25 + j 100)/50 = 0.5 + j 2.02. Find normalized resistance circle053. Find normalized reactance arcx = 2.02 31r = 0.50.2 0 0.2 0.5 1 250.906 °54. This vector represents the reflection coefficient  (d) = 0.52 + j0.64 | (d)| = 0.8246-3 -0 5 -2 -0.2  (d) = 0.8885 rad= 50.906 °-11. 0.8246© Amanogawa, 2006 - Digital Maestro Series174Transmission LinesGiven (d) Find Z(d)1. 2. 3.Determine the complex point representing the given reflection coefficient (d) on the chart. Read the values of the normalized resistance r and of the normalized reactance x that correspond to the reflection coefficient point. The normalized impedance iszn ( d ) = r + j xand the actual impedance isZ (d) = Z 0 zn ( d ) = Z 0 ( r + j x ) = Z 0 r + j Z 0 x© Amanogawa, 2006 - Digital Maestro Series175Transmission LinesGiven R and ZR Find(d) and Z(d)NOTE: the magnitude of the reflection coefficient is constant along a loss-less transmission line terminated by a specified load, since ( d ) =  R exp ( - j 2 d ) =  RTherefore, on the complex plane, a circle with center at the origin and radius | R | represents all possible reflection coefficients found along the transmission line. When the circle of constant magnitude of the reflection coefficient is drawn on the Smith chart, one can determine the values of the line impedance at any location. The graphical step-by-step procedure is:1.Identify the load reflection coefficient R and the normalized load impedance ZR on the Smith chart.176© Amanogawa, 2006 - Digital Maestro SeriesTransmission Lines2. 3.Draw the circle of constant reflection coefficient amplitude |(d)| =|R|. Starting from the point representing the load, travel on the circle in the clockwise direction, by an angle4.The new location on the chart corresponds to location d on the transmission line. Here, the values of (d) and Z(d) can be read from the chart as before.Example: Given2 d = 2d= 2 ZR = 25 + j 100 findwithZ0 = 50 Z( d ) and ( d )© Amanogawa, 2006 - Digital Maestro Seriesford = 0.18177Transmission LinesCircle with constant |  |0.51zR R2 30.2=2d R0 0.2 0.5 1 2 5= 2 (2/) 0.18  = 2.262 rad = 129.6°-0.2(d) = 0.8246 -78.7° = 0.161 ­ j 0.809-0.5 (d)zn(d)-2= 0.236 ­ j1.192 Z(d) = z(d) × Z0 = 11.79 ­ j59.6 -1 -3z(d)© Amanogawa, 2006 - Digital Maestro Series178Transmission LinesGiven R and ZR Find dmax and dmin1. 2.3.Identify on the Smith chart the load reflection coefficient R or the normalized load impedance ZR . Draw the circle of constant reflection coefficient amplitude |(d)| =|R|. The circle intersects the real axis of the reflection coefficient at two points which identify dmax (when (d) = Real positive) and dmin (when (d) = Real negative) A commercial Smith chart provides an outer graduation where the distances normalized to the wavelength can be read directly. The angles, between the vector R and the real axis, also provide a way to compute dmax and dmin .Example:Find dmax and dmin forZR = 25 + j 100  ; ZR = 25 - j100© Amanogawa, 2006 - Digital Maestro Series(Z0 = 50  )179ZR = 25 + j 100 ( Z0 = 50  )Transmission LinesIm(ZR) &gt; 00.512 dmax = 50.9° dmax = 0.0707 znR R2 30.2 R0 0.2 0.5 1 2 5-0.2 -3 -0.5 -2-12 dmin = 230.9° dmin = 0.3207180© Amanogawa, 2006 - Digital Maestro SeriesZR = 25 - j 100 ( Z0 = 50  )Transmission LinesIm(ZR) &lt; 00.512 dmax = 309.1° dmax = 0.4293 2 30.200.20.5125 R-0.2R-0.5 -2-3znR-12 dmin = 129.1° dmin = 0.1793 © Amanogawa, 2006 - Digital Maestro Series181Transmission LinesGiven R and ZR Find the Voltage Standing Wave Ratio (VSWR)The Voltage standing Wave Ratio or VSWR is defined asVmax 1 +  R VSWR = = Vmin 1 -  RThe normalized impedance at a maximum location of the standing wave pattern is given by1 +  ( d max ) 1 +  R zn ( d max ) = = = VSWR !!! 1 -  ( d max ) 1 -  RThis quantity is always real and  1. The VSWR is simply obtained on the Smith chart, by reading the value of the (real) normalized impedance, at the location dmax where  is real and positive.© Amanogawa, 2006 - Digital Maestro Series182Transmission LinesThe graphical step-by-step procedure is:1. 2. 3. 4.Identify the load reflection coefficient R and the normalized load impedance ZR on the Smith chart. Draw the circle of constant reflection coefficient amplitude |(d)| =|R|. Find the intersection of this circle with the real positive axis for the reflection coefficient (corresponding to the transmission line location dmax). A circle of constant normalized resistance will also intersect this point. Read or interpolate the value of the normalized resistance to determine the VSWR. Find the VSWR forExample:ZR1 = 25 + j 100  ; ZR2 = 25 - j100© Amanogawa, 2006 - Digital Maestro Series(Z0 = 50  )183Transmission LinesCircle with constant |  |0.51zR12 3 0.2R10.2 0.5 1 2 5Circle of constant conductance r = 10.40-0.2R2-3 -0.5 -2z(dmax )=10.4zR2-1For both loads VSWR = 10.4184© Amanogawa, 2006 - Digital Maestro SeriesTransmission LinesGiven Z(d)  Find Y(d) Note: The normalized impedance and admittance are defined as1+ (d ) zn ( d ) = 1-  (d )Since1-  (d ) yn ( d ) = 1+  (d )    d +  = - ( d ) 4     1+   d +   4  1-  (d )   zn  d +  = = = yn ( d )   1+  (d ) 4   1-   d +  4 185© Amanogawa, 2006 - Digital Maestro SeriesTransmission LinesKeep in mind that the equality  z n  d +  = yn ( d ) 4 is only valid for normalized impedance and admittance. The actual values are given by    Z  d +  = Z 0  zn  d +  4 4   yn ( d ) Y (d ) = Y0  yn (d ) = Z0where Y0=1 /Z0 is the characteristic admittance of the transmission line. The graphical step-by-step procedure is:© Amanogawa, 2006 - Digital Maestro Series 186Transmission Lines1. 2. 3.Identify the load reflection coefficient R and the normalized load impedance ZR on the Smith chart. Draw the circle of constant reflection coefficient amplitude |(d)| =|R|. The normalized admittance is located at a point on the circle of constant || which is diametrically opposite to the normalized impedance.Example: GivenZR = 25 + j 100 find YR .with Z0 = 50 © Amanogawa, 2006 - Digital Maestro Series187Transmission LinesCircle with constant |  |0.51zn(d) = 0.5 + j 2.0 Z(d) = 25 + j100 [  ]2 30.200.20.5125-0.2 = 180° = 2/4-3 -0.5yn(d) = 0.11765 ­ j 0.4706 Y(d) = 0.002353 ­ j 0.009412 [ S ] zn(d+/4) = 0.11765 ­ j 0.4706 -1 Z(d+/4) = 5.8824 ­ j 23.5294 [  ]188-2© Amanogawa, 2006 - Digital Maestro SeriesTransmission LinesThe Smith chart can be used for line admittances, by shifting the space reference to the admittance location. After that, one can move on the chart just reading the numerical values as representing admittances. Let's review the impedance-admittance terminology: Impedance = Resistance + j ReactanceZ==R++jXAdmittance = Conductance + j SusceptanceYGjBOn the impedance chart, the correct reflection coefficient is always represented by the vector corresponding to the normalized impedance. Charts specifically prepared for admittances are modified to give the correct reflection coefficient in correspondence of admittance.© Amanogawa, 2006 - Digital Maestro Series 189Transmission LinesSmith Chart for Admittancesyn(d) = 0.11765 ­ j 0.4706-1 -0.5 -2 -3 -0.2Negative (inductive) susceptance5210.50.200.2 3 2 0.5 1 Positive (capacitive) susceptancezn(d) = 0.5 + 2.0© Amanogawa, 2006 - Digital Maestro Series 190Transmission LinesSince related impedance and admittance are on opposite sides of the same Smith chart, the imaginary parts always have different sign. Therefore, a positive (inductive) reactance corresponds to a negative (inductive) susceptance, while a negative (capacitive) reactance corresponds to a positive (capacitive) susceptance. Analytically, the normalized impedance and admittance are related aszn = r + j x1 yn = g + j b = r+ jxr- jx r - jx yn = = 2 ( r + j x )( r - j x ) r + x 2 r x  g= 2 b=- 2 2 r +x r + x2© Amanogawa, 2006 - Digital Maestro Series 191`

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