- 2075 Bhadra · 10+2 marks
Double-stub on 75 Ω coax, load 0.4+j0.85
Short answer
For Z0=75 Ω and zL=0.4+j0.85, use stubs at the load and 3λ/8 apart. Solution A: b1=-0.874, b2=-2.847, short stub lengths l1=0.1357λ and l2=0.0538λ, giving Γ=0 and VSWR=1. In microstrip, replace the coax with a 75 Ω trace and short stubs by strips ending in via holes to ground.
A 75-ohm coaxial line is terminated with a normalized complex load of 0.4 + j0.85 ohms. Design a double-stub matching system using short-circuited coaxial line of 75-ohm characteristic impedance. Sketch the network using micro strip.
Given: Z0 = 75 Ω coaxial line, normalised load zL = 0.4 + j0.85 (ZL = 30 + j63.75 Ω). The stubs are short-circuited 75 Ω coaxial lines. Assumptions (not given): the first stub is at the load, and the stub spacing is d = 3λ/8.
Step 1: Normalise and convert to admittance
zL = 0.400 + j0.850
yL = 1/zL = 0.453 − j0.963
ΓL = 0.635∠94.0°, VSWR = 4.483
On the chart, zL is at 0.1195λ WTG and yL is diametrically opposite, at 0.3695λ WTG.
Step 2: First stub at the load
The first stub is placed at the load, so y1 = yL = 0.453 − j0.963.
Step 3: Forbidden-region check and rotated g = 1 circle
βd = 360° × 0.375 = 135°
g must be ≤ 1/sin²βd = 2.000
g1 = 0.4533 → matchable
Rotate the g = 1 circle by 0.375λ (270° on the chart) toward the load. The point just after stub 1 must lie on this rotated circle, so move from y1 along the constant g = 0.453 circle until it meets the rotated circle.
Step 4: Susceptance of stub 1
Analytically (Pozar), with t = tan βd:
t = tan 135° = −1.0000
b1 = −B + [1 ± √((1+t²)g − g²t²)]/t
(1+t²)g − g²t² = 0.7011, √ = 0.8373
Sol A: b1 = −0.8741
Sol B: b1 = +0.8005
Step 5: Move 0.375λ to stub 2 and find b2
Sol A: y after stub 1 = 0.453 − j1.837
(0.3263λ) → after 0.375λ: y2 = 1.000 + j2.847
b2 = −2.8473
Sol B: y after stub 1 = 0.453 − j0.163
(0.4681λ) → after 0.375λ: y2 = 1.000 − j0.847
b2 = +0.8473
Both y2 values lie on the g = 1 circle, as required.
Step 6: Stub lengths
- For a short-circuited stub: y = −j cot βl, so l = (1/2π)·cot⁻¹(−b). Measure toward the generator from the short-circuit point (y = ∞; with y plotted on an ordinary Smith chart, this is the right end, 0.25λ WTG).
Sol A short: l1 = 0.1357λ, l2 = 0.0538λ
Sol B short: l1 = 0.3574λ, l2 = 0.3619λ
| Quantity | Solution A | Solution B |
|---|---|---|
| Stub 1 from load | at load | at load |
| Stub spacing | 0.375λ | 0.375λ |
| b1, b2 | -0.874, -2.847 | 0.800, 0.847 |
| Short l1, l2 | 0.1357λ, 0.0538λ | 0.3574λ, 0.3619λ |
Answer (choice): solution A (l1 = 0.1357λ, l2 = 0.0538λ) has the shorter stubs, so it is preferred.
Check: the input admittance at stub 2 is 1.000 + j0.000, so Γ = 0 and VSWR = 1.
Sketch using microstrip
In microstrip, each "short-circuited" stub is a strip that ends in a via hole to the ground plane. The coax line is replaced by a 75 Ω microstrip trace.
Top view (ground plane underneath)
stub 2 stub 1
l2=0.0538λ l1=0.1357λ
|| ||
● via ● via
|| ||
=======##====== 3λ/8 ===##[ZL]
in (75 Ω microstrip) load
✓ Answer checked by Claude Opus 5.5 (high effort)
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