- Asked 2/23
- 2069 Bhadra (old course) · 3+15 marks
Double-stub tuner for 75+j75 Ω on 50 Ω line
Short answer
A double-stub tuner uses two fixed shunt stubs separated by a fixed distance; only stub lengths are adjusted. For 75+j75 Ω on 50 Ω line with 3λ/8 spacing, place stub 1 at the load and stub 2 0.375λ away. Short-stub lengths: solution A 0.0981λ and 0.0477λ; solution B 0.2625λ and 0.3917λ.
What is double-stub tuner? Assuming a load of 75 + j75 ohm is connected to a 50-ohm transmission line, find the lengths and spacing for a two-stub impedance matching system with three-eighths wavelength separation between the stubs.
Double-stub tuner
A double-stub tuner is an impedance-matching network with two shunt stubs (usually short-circuited) at fixed positions on the line, a fixed distance apart (λ/8, 3λ/8 or λ/4). Only the stub lengths are adjusted. Stub 1 moves the admittance onto the rotated g = 1 circle. After travelling the spacing d this point lands on the g = 1 circle, and stub 2 cancels the remaining susceptance. It suits adjustable coaxial or waveguide tuners because nothing slides along the main line. Its limit is the forbidden region g > 1/sin²βd, which cannot be matched.
Design
Given: ZL = 75 + j75 Ω, Z0 = 50 Ω, spacing 3λ/8. Assumptions: short-circuited stubs, with the first stub at the load.
Step 1: Normalise and convert to admittance
zL = 1.500 + j1.500
yL = 1/zL = 0.333 − j0.333
ΓL = 0.542∠40.6°, VSWR = 3.370
On the chart, zL is at 0.1936λ WTG and yL is diametrically opposite, at 0.4436λ WTG.
Step 2: First stub at the load
The first stub is placed at the load, so y1 = yL = 0.333 − j0.333.
Step 3: Forbidden-region check and rotated g = 1 circle
βd = 360° × 0.375 = 135°
g must be ≤ 1/sin²βd = 2.000
g1 = 0.3333 → 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 = 0.333 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 = 0.5556, √ = 0.7454
Sol A: b1 = −1.4120
Sol B: b1 = +0.0787
Step 5: Move 0.375λ to stub 2 and find b2
Sol A: y after stub 1 = 0.333 − j1.745
(0.3309λ) → after 0.375λ: y2 = 1.000 + j3.236
b2 = −3.2361
Sol B: y after stub 1 = 0.333 − j0.255
(0.4559λ) → after 0.375λ: y2 = 1.000 − j1.236
b2 = +1.2361
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 from the short-circuit point (y = ∞, right end of the chart) toward the generator.
Sol A short: l1 = 0.0981λ, l2 = 0.0477λ
Sol B short: l1 = 0.2625λ, l2 = 0.3917λ
| Quantity | Solution A | Solution B |
|---|---|---|
| Stub 1 from load | at load | at load |
| Stub spacing | 0.375λ | 0.375λ |
| b1, b2 | -1.412, -3.236 | 0.079, 1.236 |
| Short l1, l2 | 0.0981λ, 0.0477λ | 0.2625λ, 0.3917λ |
Answer: stub 1 at the load, stub 2 at 3λ/8 = 0.375λ from it. Solution A: l1 = 0.0981λ, l2 = 0.0477λ (shortest). Solution B: l1 = 0.2625λ, l2 = 0.3917λ.
Z0=50Ω 3λ/8
o------+---------------+--------[75+j75Ω]
| |
stub 2 stub 1
l2=0.0477λ l1=0.0981λ
SC SC
Check: y at stub 2 = 1.000 + j0.000, so VSWR drops from 3.37 to 1.
✓ Answer checked by Claude Opus 5.5 (high effort)
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