Objective. Students explain impedance matching, calculate standing-wave ratio (SWR) from a reflected-power or return-loss measurement, and describe the effects of impedance mismatch on transmitted power and equipment.
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A transmission line is any structure that guides electromagnetic energy from one point to another—coaxial cable, twin-lead, waveguide, or printed microstrip. In RF work, the most common type is coaxial cable. Every transmission line has a characteristic impedance (Z₀), a fixed value set by its physical dimensions and the dielectric material between conductors. Common values in telecommunications are 50 Ω (two-way radio, test equipment) and 75 Ω (cable TV, video). Characteristic impedance is not the same as DC resistance; it is determined by the ratio of inductance per unit length to capacitance per unit length and remains essentially constant regardless of line length.
For maximum power transfer, the impedance of the source, the transmission line, and the load must all match. When a load impedance (Z_L) equals Z₀, every watt of forward power is absorbed by the load—nothing is sent back. When Z_L ≠ Z₀, some energy is reflected back toward the source. These reflections combine with the forward wave to create a standing wave on the line. Standing waves cause voltage and current to peak at fixed points along the cable. High voltage peaks can break down dielectric insulation; high current peaks cause localized heating. Transmitter finals and amplifier stages are designed for a specific load impedance; excessive reflections can cause them to overheat, reduce efficiency, or trigger protective shutdown circuits.
The reflection coefficient Γ (Greek capital gamma) is the ratio of the reflected voltage wave to the forward voltage wave at the load:
Γ = (Z_L − Z₀) / (Z_L + Z₀)
Γ is dimensionless and ranges from −1 to +1 in magnitude. A perfect match gives Γ = 0 (no reflection). An open circuit (Z_L = ∞) gives Γ = +1; a short circuit (Z_L = 0) gives Γ = −1. In both extremes, 100% of power is reflected.
SWR (also written VSWR when referring to voltage) describes the severity of the standing wave pattern:
SWR = (1 + |Γ|) / (1 − |Γ|)
SWR is always ≥ 1. An SWR of 1.0:1 is a perfect match. Practical systems aim for SWR ≤ 1.5:1 or better. A two-way radio base station manufacturer may specify maximum SWR of 2.0:1 before the transmitter folds back power. SWR by itself does not tell you where the mismatch is—it only tells you how bad it is.
Return loss (RL) expresses reflected power in decibels relative to forward power:
RL (dB) = −20 × log₁₀(|Γ|)
Return loss is always stated as a positive number of dB when using this convention. A higher return loss means less reflected power and a better match. A perfect match has infinite return loss. Typical acceptable return loss in an antenna system is 14 dB or better (corresponding to SWR ≈ 1.5:1).
To find the percentage of power reflected:
% Reflected Power = |Γ|² × 100
You can also go directly from RL:
% Reflected Power = 10^(−RL/10) × 100
Not all reflected power is lost—some re-reflects at the source and re-enters the line—but in practice, mismatch always reduces delivered power and can stress equipment. At SWR 2.0:1, roughly 11% of forward power is reflected; at SWR 3.0:1, about 25%. Beyond SWR 6.0:1, reflected power exceeds 50%.
A sudden rise in SWR on a base station antenna system almost always points to a physical fault: a corroded or improperly installed connector, a pinched or kinked cable that has damaged the dielectric, water ingress at a connector or at a crack in the jacket, or physical damage to the antenna element. The test sequence is to start at the transmitter and work outward—check the short patch cable and connector at the radio first, then the feedline run, then the antenna.
Before connecting or disconnecting any cable at a transmitter or base station:
Answer each question, then check it. Nothing is recorded; this is your own practice.
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