Main source material from Rohde & Schwarz
https://www.youtube.com/watch?v=rUDMo7hwihs
Named after Philip Hagar Smith, first described in January 1939
http://smithchart.org/phsmith.shtml
- When asked why he invented the chart, Smith explained, "From the time I could operate a slide rule, I've been interested in graphical representations of mathematical relationships."
- In 1969 he published the book Electronic Applications of the Smith Chart: In Waveguide, Circuit, and Component Analysis, a comprehensive work on the subject. He retired from Bell Labs in 1970.
The Smith Chart:
- Has many applications.
- the most common are impedance matching and the design of matching networks
- pre-computers this was an intensive process
- the Smith Chart lets you solve the problem graphically with a compass, ruler and pencil
- still useful to help visualize complex impedances, especially as a function of frequency.
- widely used when tuning or verifying the performance of networks
A Smith Chart:
- used when making 1 Port measurements (reflection coefficients e.g. $S_{xy})
- Shows
$Z_{L}$ relative to$Z_{0}$ - can be used as
- a single point
- traces (impedance as a function of frequency)
- essentially bends the right hand side of a cartesian coordinate plane
- this side is all that would be used in measurement
- postitive and negative reactance axes (top and bottom half circles) bend around to meet the resistance axis (horizontal/x axis)
- top half is the Inductive region
- bottom half is the Capacitative region
- horizontal (x-axis) is the resistive axis
- A complex impedance appears as a point on a Smith Chart
- Point in the middle of chart
- corresponds to the source impedance
$Z_{0}$ and a VSWR of 1 - in most RF systems the source is purely resistive 50
$\Omega$ load - using the Smith Chart this value is normalized to 1.0
- 50
$\Omega$ / 50 == 1 - if the point moves to the right along the resistive axis to 2.0, this corresponds to a resistive value of 2 * 50 or 100
$\Omega$ . - moving the point to 4.0 would increase the resistive value to 4 * 50 or 200
$\Omega$ . - All Values on the Smith Chart are normalized by the same Prime Center value.
- This allows the Chart to be used regardless of impedance (50
$\Omega$ or 75$\Omega$ etc)
- This allows the Chart to be used regardless of impedance (50
Significance of the Prime Center:
- ideally
$Z_{L}$ =$Z_{0}$ ("matched") -
$Z_{0}$ is always the Prime Center. - Measured
$Z_{L}$ is plotted on the Smith Chart - The closer the values are to the center the better the impedance match
- the farther away the values to the center, the higher the degree of mismatch
- when viewing a trace (many points):
- the load is resonant at the frequency where the trace moves through the center
- The horizontal centerline
- left of prime center decreases until 0 on the outer edge - A Short Circuit
- right of prime center increases until the outer edge where it reaches
$\infty$ - an Open Circuit - therefore VSWR is
$\infty$ on either end of the resistive axis. 100% reflected power
- Most loads have complex impedances
- have conductive and inductive characteristics, so not flat on the resistive line
Circle R=1 (red):
- all values within represent a normalized resistance of 1
Circle R=.2 (blue):
- all values within represent a normalized resistance of .2
Circle R=4 (green):
- all values within represent a normalized resistance of 4
and so on.
The Normalized Resistance of any point is found by following the resistance circle to the horizontal axis and reading the value
- the Reactive axis is the outer circle (circumference) since it's bent from a cartesian plane.
- Normalized Values along the outside. Get larger from L to R.
- Values increase rapidly as they get closer to the centerline at the right hand side of the chart (Open Circuit)
- Normalized reactance are shown as Curves.
- every point along the reactive curve has the same Imaginary part.
- in the diagram every point along the line has a reactance value of 1
- on the upper half of the chart all values are Inductive (positive)
- on the upper half of the chart all values are Capacitative (negative)
Complex impedance - Z = R
Our value is: 100 + j75
- normalize the impedance by dividing by
$Z_{0}$ - (100 + j75
$\Omega$ ) / 50 == 2 + j1.5 -
$R_{normalized}$ +$X_{normalized}$ (2 + 1.5) - Find and plot the resistance circle for this normalized resistance
-
$R_{normalized}$ == 2
-
- Find and plot the reactance curve
-
$X_{normalized}$ == 1.5
-
- (100 + j75
- determine which resistance circle the point lies on
- determine which reactance curve the point lies on
- multiply the normalized values by the source impedance (
$Z_{0}$ ) to obtain actual values
For R = .3 and X = 0.4,
So in this case:




