Page 356 - Engineering Electromagnetics, 8th Edition
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338                ENGINEERING ELECTROMAGNETICS
































                                             Figure 10.12 The Smith chart contains the constant-r circles and
                                             constant-x circles, an auxiliary radial scale to determine | |, and an
                                             angular scale on the circumference for measuring φ.

                                     badly, so the angle is indicated on the circumference of the circle. A straight line from
                                     the origin through the intersection may be extended to the perimeter of the chart. As
                                     an example, if Z L = 25 + j50   ona50   line, z L = 0.5 + j1, and point A on
                                     Figure 10.12 shows the intersection of the r = 0.5 and x = 1 circles. The reflection
                                     coefficient is approximately 0.62 at an angle φ of 83 .
                                                                               ◦
                                        The Smith chart is completed by adding a second scale on the circumference by
                                     which distance along the line may be computed. This scale is in wavelength units, but
                                     the values placed on it are not obvious. To obtain them, we first divide the voltage at
                                     any point along the line,
                                                            V s = V (e − jβz  +  e  jβz )
                                                                   +
                                                                  0
                                     by the current
                                                                 V 0 +  − jβz  jβz
                                                            I s =   (e   −  e   )
                                                                 Z 0
                                     obtaining the normalized input impedance
                                                                 V s   e − jβz  +  e jβz
                                                           z in =   =
                                                                Z 0 I s  e − jβz  −  e jβz
                                     Replacing z with −l and dividing numerator and denominator by e jβl ,wehavethe
                                     general equation relating normalized input impedance, reflection coefficient, and
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