Part 9 of 12 · Smith Chart & Impedance Matching Series overview →

This article builds on Part 8: Understanding Smith Chart Parameters and Circles. Next up: Part 10: Impedance Matching Using the Smith Chart.

Smith chart from the NEXT ANTENNAS calculator showing the load 25 + j50 ohms and its constant-VSWR circle traced by a half-wavelength line
Fig 1 — The load 25 + j50 Ω on a 50 Ω chart, with its constant-VSWR circle. The circle was traced in the calculator by adding a half-wavelength 50 Ω line, which rotates the point once around the chart (clockwise, toward the generator). Try it in the Smith Chart Calculator →

Plotting Impedance: The Core Smith Chart Skill

Every Smith chart task — reading a VNA trace, finding a line's input impedance, designing a matching network — starts with the same operation: putting an impedance on the chart and reading information back off it. Part 6 explained the geometry and Part 8 introduced the circles and scales. This article turns that knowledge into a repeatable procedure you can apply to any load.

📌 The procedure at a glance

1. Identify Z_L and Z₀ → 2. Normalise: z = Z_L/Z₀ → 3. Find the r circle → 4. Find the x arc → 5. Mark the intersection → 6. Draw the VSWR circle through it → 7. Read |Γ|, ∠Γ, VSWR and return loss → 8. Convert back to ohms (and to admittance if needed).

Identifying Load Impedance

The load impedance Z_L = R_L + jX_L is whatever terminates the line or network you are analysing: an antenna feed point, the input of an amplifier, a filter, or a component on a test fixture. Before plotting, make sure of four things:

  • The frequency. Impedance changes with frequency, so a single point on the chart is valid at one frequency only. A measured antenna gives a curve, one point per frequency.
  • The reference plane. Know exactly where Z_L is defined — at the antenna terminals or at the end of a feed cable. A cable between them rotates the point (Part 5).
  • Series form. The chart's impedance grid uses the series form R + jX. If a datasheet gives a parallel R ∥ X model, convert it first (or plot it as an admittance).
  • The sign of X. Positive reactance is inductive, negative is capacitive. A sign error puts the point in the wrong half of the chart.

Normalizing Load Impedance

The chart is drawn for a reference impedance of 1. Divide the load by the system's characteristic impedance — usually 50 Ω, or 75 Ω for video and cable-TV systems (Part 7):

Normalised impedance
z=ZLZ0=RLZ0+jXLZ0=r+jx
Example: 25 + j50 Ω in a 50 Ω system gives z = 0.5 + j1. The same load in a 75 Ω system gives z = 0.333 + j0.667 — a different point, because the mismatch is different.

Locating Resistance and Reactance

Resistance. The r circles are labelled along the horizontal axis: 0 at the left edge, 1 at the centre, ∞ at the right edge. Find the circle whose label matches r. If r falls between printed circles (say 0.7 between 0.5 and 1), imagine a circle between them — on a calculator, the exact circle is drawn for you.

Reactance. The x arcs are labelled around the rim: +j values on the upper half, −j values on the lower half, with +j1 at the top and −j1 at the bottom. Follow the arc for your x from the rim inward. Remember that x = 0 is the horizontal axis itself.

Fig 2 — Locating z = 0.5 + j1: the r = 0.5 circle (green) and the x = +1 arc (orange) intersect at a single point
00.20.5125+j0.2−j0.2+j0.5−j0.5+j1−j1+j2−j2+j5−j5∞z = 0.5 + j1
r = 0.5 circlex = +1 arc

Plotting Complex Impedance

The impedance point is the intersection of the r circle and the x arc. Every r circle crosses every x arc exactly once inside the chart, so the point is unique. Two quick sanity checks catch most mistakes:

  • Half: inductive loads (x > 0) must be above the horizontal axis; capacitive loads below.
  • Side: r < 1 puts the point inside the left part of the chart (outside the r = 1 circle); r > 1 puts it inside the r = 1 circle.
NEXT ANTENNAS Smith chart calculator with the load 25 + j50 ohms plotted and the circle and arc through it highlighted
Fig 3 — The same load plotted in the Smith Chart Calculator. The tool highlights the r circle and x arc that pass through the point, so you can confirm the hand plot. Try it in the Smith Chart Calculator →

Drawing Constant VSWR Circles

Place a compass point on the centre of the chart and draw a circle through the load point. This is the load's constant-VSWR circle (also called the constant-|Γ| circle). Every impedance seen looking toward the load along a lossless line lies on this circle, because the line changes only the angle of Γ, not its magnitude.

  • Moving toward the generator (away from the load) rotates the point clockwise.
  • Moving toward the load rotates it anticlockwise.
  • One full turn is λ/2 of line, because Γ rotates by 2βd = 720° per wavelength.

That is how Fig 1 was produced: adding a 0.5λ line in the calculator rotates the point once around its VSWR circle and back to where it started.

Finding the Reflection Coefficient

Magnitude. |Γ| is the distance from the centre to the point, as a fraction of the chart radius. On paper, measure both with a ruler and divide, or transfer the distance to the "reflection coefficient" scale printed below most charts.

Angle. Draw a line from the centre through the point to the rim and read the angle on the outer "angle of reflection coefficient" scale. 0° points to the right (open-circuit end), +90° to the top, ±180° to the left (short-circuit end) and −90° to the bottom.

Calculator readouts for 25 + j50 ohms: input impedance, reflection coefficient 0.620 at 82.9 degrees, S11 minus 4.15 dB and VSWR 4.27
Fig 4 — The calculator reads the same values numerically: Γ = 0.620 ∠ 82.9°, S11 = −4.15 dB, VSWR = 4.27 : 1 and Y = 8 − j16 mS. Try it in the Smith Chart Calculator →

Determining VSWR From the Chart

The VSWR circle crosses the horizontal axis at two points. Where it crosses the right-hand axis (r > 1), the normalised resistance equals the VSWR directly. Where it crosses the left-hand axis, the resistance is 1/VSWR. No calculation is needed — read the r label at the crossing.

Fig 5 — The VSWR circle of z = 0.5 + j1 crosses the right axis at r = 4.27 (= VSWR, a voltage maximum) and the left axis at r = 0.234 (= 1/VSWR, a voltage minimum)
0.115λ00.20.5125+j0.2−j0.2+j0.5−j0.5+j1−j1+j2−j2+j5−j5∞z_Lr = 4.27 = VSWRr = 0.234
VSWR circle, |Γ| = 0.62
VSWR, return loss and mismatch loss from |Γ|
VSWR=1+|Γ|1−|Γ| RL=−20log10|Γ| ML=−10log10(1−|Γ|2)
The relationships behind VSWR and return loss are developed in Part 4. Paper charts print VSWR, return-loss and |Γ| scales below the chart so all three can be read with a pair of dividers.

Converting Plotted Values Back to Actual Impedance

Any point read off the chart is normalised. Multiply by Z₀ to get ohms. For admittance, use the fact that rotating a point by 180° about the centre turns z into its reciprocal y = 1/z — the point diametrically opposite on the VSWR circle. Then divide by Z₀ (or multiply by Y₀ = 1/Z₀) to get siemens:

Denormalising impedance and admittance
Z=z·Z0 y=1z (180° rotation) Y=yZ0
Fig 6 — z = 0.5 + j1 and its admittance y = 0.4 − j0.8 lie at opposite ends of a diameter of the VSWR circle
00.20.5125+j0.2−j0.2+j0.5−j0.5+j1−j1+j2−j2+j5−j5∞z = 0.5 + j1y = 0.4 − j0.8
VSWR circle

Step-by-Step Solved Examples

All examples use Z₀ = 50 Ω. Each load can be entered directly in the Smith Chart Calculator to check the graphical result.

01

Inductive Load: 25 + j50 Ω

Problem: Plot Z_L = 25 + j50 Ω and find Γ, VSWR, return loss and the load admittance.

  1. Normalise: z = (25 + j50)/50 = 0.5 + j1.
  2. Plot: intersection of the r = 0.5 circle and the x = +1 arc (Fig 2) — upper half, inductive.
  3. VSWR circle: centred on the chart through the point; it crosses the right axis at r ≈ 4.27.
  4. Γ: the point is 0.62 of the radius from the centre at 82.9° → Γ = 0.620 ∠ 82.9°.
  5. Return loss: −20 log 0.620 = 4.15 dB.
  6. Admittance: rotate 180° → y = 0.4 − j0.8 → Y = (0.4 − j0.8)/50 = 8 − j16 mS.
Answer: Γ = 0.620 ∠ 82.9°, VSWR = 4.27, RL = 4.15 dB, Y = 8 − j16 mS

All four values match the calculator readout in Fig 4 exactly. With a VSWR above 4, about 38% of the incident power is reflected — this load needs matching (we match it in Part 10).

02

Capacitive Load: 75 − j25 Ω

Problem: Plot Z_L = 75 − j25 Ω and find Γ, VSWR and return loss. Does it meet a −10 dB S11 specification?

z = 1.5 − j0.5
Γ=0.5−j0.52.5−j0.5=0.231−j0.154=0.277∠−33.7° VSWR=1.77 RL=11.1 dB
Smith chart with the load 75 minus j25 ohms plotted inside the r = 1 circle in the lower capacitive half
The point is in the lower (capacitive) half, inside the r = 1 circle because r = 1.5 > 1, and close to the centre. Try it in the Smith Chart Calculator →
Calculator readouts for 75 minus j25 ohms: Γ 0.277 at minus 33.7 degrees, S11 minus 11.14 dB, VSWR 1.77
Calculator readout: S11 = −11.14 dB, better than the −10 dB target. Try it in the Smith Chart Calculator →
Answer: Γ = 0.277 ∠ −33.7°, VSWR = 1.77, RL = 11.1 dB — passes a −10 dB specification

The −10 dB contour is the circle |Γ| = 0.316 (VSWR 1.92). Any load plotted inside that circle meets the spec, which is why VSWR circles are such a fast visual check.

03

Low-Resistance Load: 10 Ω

Problem: A power transistor presents 10 Ω (resistive) to a 50 Ω line. Plot it and read the VSWR without using the formula.

Smith chart with a 10 ohm load on the left part of the horizontal axis
z = 0.2 lies on the horizontal axis, far to the left — between the centre and the short-circuit end. Try it in the Smith Chart Calculator →
Calculator readouts for 10 ohms: Γ 0.667 at 180 degrees, S11 minus 3.52 dB, VSWR 5.00
Calculator readout: Γ = 0.667 ∠ 180°, VSWR 5.00 : 1. Try it in the Smith Chart Calculator →
Answer: z = 0.2, Γ = 0.667 ∠ 180°, VSWR = 5.0

The VSWR circle through z = 0.2 crosses the right axis at r = 1/0.2 = 5, so the VSWR is 5 by inspection. Low-impedance loads like this are typical of power amplifier outputs and are matched with low-pass L or π networks.

04

Reading an Impedance Back From the Chart

Problem: A VNA marker shows a point at |Γ| = 0.45, angle 120°. What are the impedance and the VSWR?

Γ = 0.45∠120° = −0.225 + j0.390; z = (1 + Γ)/(1 − Γ)
z=0.775+j0.3901.225−j0.390=0.483+j0.472 Z=24.1+j23.6 Ω VSWR=1.450.55=2.64
Answer: Z ≈ 24.1 + j23.6 Ω, VSWR ≈ 2.64

On the chart the point sits just outside the r = 0.5 circle and just below the x = +0.5 arc — reading r ≈ 0.48 and x ≈ 0.47 by eye gives the same answer to two figures, which is the usual accuracy of a paper chart.

05

Voltage Maximum and Minimum Positions

Problem: For the 25 + j50 Ω load, how far from the load is the first voltage maximum on the line, and what impedances are seen at the voltage maximum and minimum?

Rotate clockwise from ∠Γ = 82.9° to 0° (right axis); 360° of chart rotation = 0.5λ
dmax=82.9°720°λ=0.115λ Zmax=4.27×50=213 Ω Zmin=504.27=11.7 Ω
Answer: first V_max at 0.115λ from the load (Z = 213 Ω); V_min a further 0.25λ on, at 0.365λ (Z = 11.7 Ω)

The green arrow in Fig 5 shows this rotation. At 2.4 GHz on air-dielectric line (λ = 125 mm) the maximum is 14.4 mm from the load. Measuring the position of a voltage minimum on a slotted line was, for decades, how unknown loads were found — the Smith chart turned that measurement back into an impedance.

Summary

StepActionResult for 25 + j50 Ω
1. Normalisez = Z_L / Z₀0.5 + j1
2. PlotIntersect r circle and x arcUpper half, outside r = 1 circle
3. VSWR circleCentre → through point|Γ| = 0.62
4. ΓRadius ratio and rim angle0.620 ∠ 82.9°
5. VSWRr at right-axis crossing4.27
6. Return loss−20 log|Γ|4.15 dB
7. AdmittanceRotate 180°, divide by Z₀8 − j16 mS
8. Line effectRotate clockwise toward generatorV_max at 0.115λ
  • Always normalise first; the same load is a different point in a 50 Ω and a 75 Ω system.
  • The impedance point is the unique intersection of one r circle and one x arc.
  • The circle centred on the chart through the point is the constant-VSWR circle; a lossless line moves the point around it.
  • The VSWR is the r value where that circle crosses the right-hand axis; the admittance is the diametrically opposite point.

With plotting mastered, Part 10: Impedance Matching Using the Smith Chart uses these moves to bring a load to the centre of the chart — designing real matching networks.

Put It Into Practice

Use the NEXT ANTENNAS calculators to apply the ideas from this article to real designs.