Shunt Resistor Attenuator
Overview
The simplest attenuator configurations using a single resistor. Used as a lossy matching network or when impedance matching is not required.
Topology
Input ──┬── Output
│
[R]
│
GND
Single shunt resistor to ground.
Design Equation
Given:
Source impedance: ZS
Load impedance: ZL
Desired power attenuation: α (linear power ratio, α < 1)
The shunt resistor value is:
R = (2√(ZL × ZS × α) × ZL × ZS + (ZL² × ZS + ZL × ZS²) × α) /
(4 × ZL × ZS - (ZL² + 2×ZL×ZS + ZS²) × α)
Simplified for ZS = ZL = Z₀:
R = Z₀ × (1 + √α) / (1 - √α)
Impedances Seen
Input impedance:
Zin = R ∥ ZL = (R × ZL) / (R + ZL)
Output impedance:
Zout = R ∥ ZS = (R × ZS) / (R + ZS)
Power Dissipation
Pdiss = Pin × (1 - α)
Example: 10 dB, ZS = ZL = 50 Ω, Pin = 1 W
α = 0.1
√α ≈ 0.316
R = 50 × (1 + 0.316) / (1 - 0.316)
= 50 × 1.316 / 0.684
≈ 96.2 Ω
Zin = (96.2 × 50) / (96.2 + 50) ≈ 32.9 Ω
Zout = (96.2 × 50) / (96.2 + 50) ≈ 32.9 Ω
Pdiss = 1 × (1 - 0.1) = 0.9 W
VSWR at Input
VSWR_in = 50 / 32.9 ≈ 1.52:1 (better than series, but still mismatched)
Comparison: R-Series vs. R-Shunt
10 dB Example (ZS = ZL = 50 Ω)
Parameter |
R-Series |
R-Shunt |
|---|---|---|
R value |
216.2 Ω |
96.2 Ω |
Zin |
266.2 Ω |
32.9 Ω |
Zout |
266.2 Ω |
32.9 Ω |
VSWR (50Ω system) |
5.32:1 |
1.52:1 |
Power dissipation |
0.9 W |
0.9 W |
Key observations:
R-series: Increases impedance (poor match)
R-shunt: Decreases impedance (better match, but still poor)
Both: Same power dissipation
Shunt has better VSWR for same attenuation
Attenuation Range
Attenuation (dB) |
R-Series (Ω) |
R-Shunt (Ω) |
VSWR_in (Series) |
VSWR_in (Shunt) |
|---|---|---|---|---|
3 |
70.7 |
183.3 |
2.41:1 |
1.37:1 |
6 |
100.0 |
125.0 |
3.00:1 |
1.60:1 |
10 |
216.2 |
96.2 |
5.32:1 |
1.52:1 |
20 |
495.0 |
55.3 |
10.9:1 |
1.11:1 |
Trend:
R-series: VSWR worsens dramatically with attenuation
R-shunt: VSWR improves slightly with attenuation (but output impedance drops)
Advantages
Extremely simple
Low cost:
Broadband: Resistive, works DC to GHz (limited by parasitics)
Small size: Smallest footprint
Predictable: No resonances or complex behavior
Limitations
Poor impedance match: High VSWR at both ports
Attenuation depends on source/load impedances: Not constant like matched designs
Reflections: Standing waves in transmission line systems
Bidirectional mismatch: Both input and output are affected
Not suitable for RF: Mismatch causes measurement errors, signal integrity issues