Differences
This shows you the differences between two versions of the page.
| standing_wave_ratio [2026/10/02 16:22] – Organise Wikiham as an encyclopedia of individual articles 127.0.0.1 | standing_wave_ratio [2026/10/02 21:06] (current) – Add technical encyclopedia coverage, formulas, examples and primary references admin | ||
|---|---|---|---|
| Line 1: | Line 1: | ||
| ====== Standing wave ratio ====== | ====== Standing wave ratio ====== | ||
| - | **Standing wave ratio** (**SWR**) describes the standing-wave pattern | + | **Standing wave ratio (SWR)** describes the standing-wave pattern |
| - | ===== Interpretation | + | ===== Reflection coefficient |
| - | A low SWR indicates | + | For a line with real characteristic impedance Z0 and load impedance Z_L: |
| - | The measurement point, operating frequency and feed-line configuration matter when interpreting a result. Include these details with the instrument and test conditions in any published measurement. | + | < |
| + | Γ = (Z_L - Z0) / (Z_L + Z0) | ||
| + | VSWR = (1 + |Γ|) / (1 - |Γ|) | ||
| + | Reflected power fraction = |Γ|² | ||
| + | </ | ||
| - | ===== See also ===== | + | Γ is the voltage-wave reflection coefficient at the stated reference plane. These expressions assume the relevant travelling-wave model and reference impedance. For a passive load on a lossless line, a perfect match gives Γ = 0 and VSWR = 1:1. |
| - | * [[antenna|Antenna]] | + | ===== Worked example ===== |
| - | * [[transmission_line|Transmission | + | |
| - | * [[radio_experiment|Radio experiment]] | + | A purely resistive 100 Ω load on a 50 Ω line gives: |
| + | |||
| + | < | ||
| + | Γ = (100 - 50) / (100 + 50) = 1/3 | ||
| + | VSWR = (1 + 1/3) / (1 - 1/3) = 2:1 | ||
| + | Reflected power fraction = (1/3)² ≈ 11.1% | ||
| + | </ | ||
| + | |||
| + | The reflected power fraction is 11.1%, not 33.3%. This is not automatically the percentage of transmitter power permanently lost: feed-line losses, source behaviour and repeated reflections affect the complete system. | ||
| + | |||
| + | Return loss expresses the same local reflection using [[decibel|decibels]]: | ||
| + | |||
| + | < | ||
| + | Return loss = -20 log10(|Γ|) | ||
| + | </ | ||
| + | |||
| + | The example gives approximately 9.54 dB return loss. Larger positive return loss means a smaller reflection. | ||
| + | |||
| + | ===== What SWR does not show ===== | ||
| + | |||
| + | A low SWR indicates a good match at the measurement point, not necessarily good radiation efficiency. A dummy load can have a near-perfect match while converting RF into heat. A lossy feed line can also make the transmitter-end SWR look better than the antenna-end value. | ||
| + | |||
| + | A tuner can transform the impedance seen by a transmitter without removing cable or antenna losses. Record frequency, reference impedance, measurement point, cable arrangement and instrument settings when comparing results. | ||
| + | |||
| + | ===== References ===== | ||
| + | |||
| + | * [[https:// | ||
| + | * [[https:// | ||