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K. A. Connor

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... impedance is normalized by the characteristic impedance of the line, the ... to add an impedance so that the total impedance is the characteristic impedance ... – PowerPoint PPT presentation

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Title: K. A. Connor


1
Smith Chart
  • Supplemental Information
  • Fields and Waves I
  • ECSE 2100

2
Smith Chart
  • Impedances, voltages, currents, etc. all repeat
    every half wavelength
  • The magnitude of the reflection coefficient, the
    standing wave ratio (SWR) do not change, so they
    characterize the voltage current patterns on
    the line
  • If the load impedance is normalized by the
    characteristic impedance of the line, the
    voltages, currents, impedances, etc. all still
    have the same properties, but the results can be
    generalized to any line with the same normalized
    impedances

3
Smith Chart
  • The Smith Chart is a clever tool for analyzing
    transmission lines
  • The outside of the chart shows location on the
    line in wavelengths
  • The combination of intersecting circles inside
    the chart allow us to locate the normalized
    impedance and then to find the impedance anywhere
    on the line

4
Smith Chart
Imaginary Impedance Axis
Real Impedance Axis
5
Smith Chart
Constant Imaginary Impedance Lines
Constant Real Impedance Circles
6
Smith Chart
  • Impedance divided by line impedance (50
    Ohms)
  • Z1 100 j50
  • Z2 75 -j100
  • Z3 j200
  • Z4 150
  • Z5 infinity (an open circuit)
  • Z6 0 (a short circuit)
  • Z7 50
  • Z8 184 -j900
  • Then, normalize and plot. The points are plotted
    as follows
  • z1 2 j
  • z2 1.5 -j2
  • z3 j4
  • z4 3
  • z5 infinity
  • z6 0
  • z7 1

7
Smith Chart
  • Thus, the first step in analyzing a transmission
    line is to locate the normalized load impedance
    on the chart
  • Next, a circle is drawn that represents the
    reflection coefficient or SWR. The center of the
    circle is the center of the chart. The circle
    passes through the normalized load impedance
  • Any point on the line is found on this circle.
    Rotate clockwise to move toward the generator
    (away from the load)
  • The distance moved on the line is indicated on
    the outside of the chart in wavelengths

8
Toward Generator
Away From Generator
Full Circle is One Half Wavelength Since
Everything Repeats
9
Smith Chart References
  • http//www.maxim-ic.com/appnotes.cfm/appnote_numbe
    r/742/
  • http//www.ece.uvic.ca/whoefer/elec454/Lecture20
    04.pdf
  • http//www.sss-mag.com/smith.html
  • http//www.educatorscorner.com/index.cgi?CONTENT_I
    D2482 to download applet
  • http//www.amanogawa.com/index.html Two examples
    from this page are shown in the following slides

10
Smith Chart Example
  • First, locate the normalized impedance on the
    chart for ZL 50 j100
  • Then draw the circle through the point
  • The circle gives us the reflection coefficient
    (the radius of the circle) which can be read from
    the scale at the bottom of most charts
  • Also note that exactly opposite to the normalized
    load is its admittance. Thus, the chart can also
    be used to find the admittance. We use this fact
    in stub matching

11
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12
Note the cursor is at the load location
13
Single Stub Matching (as in Homework)
  • Load of 100 j100 Ohms on 50 Ohm Transmission
    Line
  • The frequency is 1 GHz 1x109 Hz
  • Want to place an open circuit stub somewhere on
    the line to match the load to the line, at least
    as well as possible.
  • The steps are well described at
    http//www.amanogawa.com/index.html
  • First the line and load are specified. Then the
    step by step procedure is followed to locate the
    open circuit stub to match the line to the load

14
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21
Smith Chart
  • Now the line is matched to the left of the stub
    because the normalized impedance and admittance
    are equal to 1
  • Note that the point on the Smith Chart where the
    line is matched is in the center (normalized z1)
    where also the reflection coefficient circle has
    zero radius or the reflection coefficient is
    zero.
  • Thus, the goal with the matching problem is to
    add an impedance so that the total impedance is
    the characteristic impedance
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