Audited 29 Jul 2026·Last updated 28 Oct 2026·4 citations·Tier 3·0 uses

VSWR Calculator (Voltage Standing Wave Ratio)

Turn a VSWR reading, return loss, reflection coefficient, wattmeter powers or load and line impedances into all the others, plus power delivered.

VSWR Calculator

What do you already have?
The resistive part of what the line is feeding — an antenna, an amplifier input, a dummy load. Reactance is not modelled here, so a load with significant reactance will really be worse than this figure. Read in the impedances mode only.
Ω
The cable's own impedance, printed on the jacket: 50 Ω for most RF coax such as RG-58 and LMR-400, 75 Ω for RG-6 and video feeds. Read in the impedances mode only.
Ω
Enter 1.5 for a 1.5:1 reading. It can never be below 1 — that is the ratio of the largest voltage on the line to the smallest. Read in the VSWR mode only.
:1
As a positive number of decibels, where bigger is better: 20 dB means one per cent of the power comes back. Some analysers display it as a negative reflection figure instead — if yours shows −20, enter 20. Read in the return loss mode only.
dB
The magnitude |Γ|, between 0 and 1. A value of 1 is total reflection and has no finite VSWR. The sign of Γ only says whether the load is above or below the line impedance and changes nothing here. Read in the reflection coefficient mode only.
The forward reading from a directional wattmeter. Any unit will do as long as both readings share it — only the ratio is used. Read in the powers mode only.
W
The reverse reading, in the same unit. Note that this is a POWER ratio, so 25 W back out of 100 W forward is a reflection coefficient of 0.5, not 0.25. Read in the powers mode only.
W
What this mismatch means
VSWR 1.5:1 with 13.98 dB of return loss. Between one and ten per cent of the power is being reflected — the band between 20 dB and 10 dB of return loss, which is where most working antenna and cable installations sit. The reflection coefficient magnitude is 0.2. Reflected power is 4 % of what went forward, so 96 % reaches the load — a mismatch loss of 0.1773 dB. These figures assume purely resistive impedances and use the magnitude of the reflection coefficient only; a reactive load reflects at least this much. Mismatch loss is power turned back, not power burned in the cable, and it is not an acceptance limit: what counts as an acceptable VSWR is set by your system's own specification, since widely quoted figures such as 2:1 are conventions rather than published standards.
The VSWR and return loss in words, how much forward power reaches the load, and which band of reflected power the mismatch falls in, with its assumptions.
VSWR
1.5 :1
Reflection coefficient |Γ|
0.2
Return loss
13.9794 dB
Mismatch loss
0.1773 dB
Power reflected
4.00
Power reaching the load
96.00

Background.

Feed a 75 Ω antenna through 50 Ω coax and the radio's meter settles at 1.5:1. Is that worth fixing? The reading means the load has sent part of the wave back down the cable, where it overlaps with the outgoing wave and leaves a fixed pattern of voltage peaks and troughs along the line. VSWR is the ratio of the highest of those voltages to the lowest. Here, 4 % of the power returns and 96 % reaches the antenna, a loss of under two tenths of a decibel.

A meter's VSWR, an analyser's return loss, a datasheet's reflection coefficient, a wattmeter's forward and reflected watts and a pair of impedances all describe one number, the magnitude of the reflection coefficient |Γ|, so any one converts into the rest.

Even 2:1 still delivers 88.89 % of the forward power. The often-quoted 2:1 limit is a convention, not a published standard, so judge the result against your own equipment's specification.

What is vswr calculator?

VSWR, the voltage standing wave ratio, is the ratio of maximum to minimum voltage along a transmission line feeding a mismatched load. It equals (1 + |Γ|) ÷ (1 − |Γ|), where the reflection coefficient Γ is the reflected voltage wave divided by the forward one. A perfect match is 1:1; a short, an open or a purely reactive load reflects everything and gives an infinite ratio.

How to use this calculator.

  1. Choose the figure you already have; only the fields for that mode are read.
  2. For impedances, enter the load's resistance and the cable's characteristic impedance from its jacket: 50 Ω for coax such as RG-58 or LMR-400, 75 Ω for RG-6 and video cable.
  3. For a wattmeter, enter forward and reflected power in the same unit. They are powers, so 25 W reflected from 100 W forward means |Γ| = 0.5, not 0.25.
  4. Enter return loss as a positive number of decibels. If your analyser shows −20 dB, enter 20.

The formula.

Γ = (Z_L − Z_0)/(Z_L + Z_0) · VSWR = (1+|Γ|)/(1−|Γ|) · RL = −20·lg|Γ| dB · ML = −10·lg(1−|Γ|²) dB · P_refl = 100·|Γ|² %

Every mode first recovers |Γ|. From impedances, |Γ| = |Z_L − Z_0| ÷ (Z_L + Z_0); from a VSWR reading, (VSWR − 1) ÷ (VSWR + 1); from return loss, 10^(−RL/20); from a wattmeter, √(P_reflected ÷ P_forward), since |Γ| is a voltage ratio and power goes as voltage squared. Then VSWR = (1 + |Γ|) ÷ (1 − |Γ|), return loss = −20 log₁₀|Γ|, reflected power = 100|Γ|² %, and mismatch loss = −10 log₁₀(1 − |Γ|²) dB. Marki Microwave prints all of these relations, and Keysight gives the same definitions of VSWR and return loss.

The reading beside the result sorts the mismatch at 1 %, 10 % and 50 % of power reflected (return losses of 20, 10 and 3.01 dB) as description, not as a pass mark. Impedances are treated as purely resistive, so for a load with reactance the true reflection is larger than shown. A perfect match reports return loss at a labelled 300 dB ceiling in place of infinity, and total reflection, |Γ| = 1, is refused because no finite VSWR exists.

A worked example.

Example

A 75 Ω load on a 50 Ω line, in impedance mode. The reflection coefficient is (75 − 50) ÷ (75 + 50) = 25 ÷ 125 = 0.2. The VSWR is (1 + 0.2) ÷ (1 − 0.2) = 1.2 ÷ 0.8 = 1.5:1 — for purely resistive impedances, simply the larger impedance divided by the smaller. Return loss is −20 × log₁₀ 0.2 = 13.9794 dB. Squaring 0.2 gives 0.04, so 4 % of the power is reflected and 96 % delivered, a mismatch loss of −10 × log₁₀ 0.96 = 0.1773 dB. Two published tables land on the same point from opposite directions: Mini-Circuits lists VSWR 1.50 against 14.0 dB of return loss and 96.0 % transmitted, while Marki's 14 dB row gives VSWR 1.50, |Γ| 0.200 and 3.98 % reflected.

known Quantityimpedances
line Impedance50
load Impedance75

Frequently asked questions.

Why do a 25 Ω load and a 100 Ω load on a 50 Ω line give the same VSWR?
Both are a factor of two away from the line impedance. The reflection coefficients are −1/3 and +1/3; the sign only says whether the load is below or above the line, and VSWR uses the magnitude. Each reflects 11.11 % of the power and reads 2:1.
How do I get VSWR from my wattmeter's forward and reflected readings?
Divide reflected by forward power, take the square root to get |Γ|, then apply (1 + |Γ|) ÷ (1 − |Γ|). With 25 W back from 100 W forward, |Γ| is 0.5 and VSWR is 3:1. Skipping the square root, as if 0.25 were the coefficient, gives a misleading 1.67:1.
What return loss corresponds to common VSWR readings?
1.5:1 is 13.98 dB of return loss with 4 % reflected; 2:1 is 9.54 dB with 11.11 % reflected; 3:1 is 6.02 dB with 25 % reflected. Working the other way, 20 dB of return loss is a VSWR of 1.22:1 and 10 dB is 1.92:1.
Is mismatch loss the same as the loss in my cable?
No. Mismatch loss is power turned back at the load, not power turned into heat. Cable loss is separate, and on a long lossy run a standing wave makes it larger, because current and voltage peak at points along the line. That extra dissipation is not included here.
Does a high VSWR damage a transmitter?
Many solid-state transmitters reduce their output when reflected power rises, so the usual symptom is lost power rather than failure; equipment without that protection can be stressed by the voltage peaks. A sudden change in a once-steady reading is a useful fault signal, often water in a connector or a damaged cable.

References& sources.

  1. [1]Marki Microwave, "Return Loss to VSWR Conversion Table". Read directly from the PDF on 2026-07-29. Prints every relation implemented on this page — Γ = 10^(−RL/20), Return Loss (dB) = −20 log|Γ|, VSWR = (1+|Γ|)/(1−|Γ|), Γ = (VSWR−1)/(VSWR+1), Mismatch Loss (dB) = −10 log(1−Γ²), Through Power (%) = 100(1−Γ²), Reflected Power (%) = 100·Γ² — and tabulates return loss from 1 to 40 dB against all of them. The 14 dB row reads VSWR 1.50, Γ 0.200, mismatch loss 0.176 dB, 3.98 % reflected, 96.02 % through; this calculator reproduces five of its rows.
  2. [2]Mini-Circuits, application note AN-40-013 rev A (14 April 2015), "The Effect of VSWR on Transmitted Power". Read directly from the PDF on 2026-07-29. An independent table from a different manufacturer, indexed by VSWR rather than by return loss, with columns for VSWR in dB, return loss, transmission loss, voltage reflection coefficient, and power transmitted and reflected as percentages. The VSWR 1.50 row reads 14.0 dB return loss, 0.177 dB transmission loss, |Γ| 0.20, 96.0 % transmitted and 4.0 % reflected — the same point as Marki's 14 dB row, reached from the opposite direction. This calculator reproduces five of its rows.
  3. [3]Keysight Technologies, "VSWR / Return Loss Calculator" knowledge page. Retrieved 2026-07-29. A test-and-measurement manufacturer's statement of the same two core relations: VSWR = (1+|Γ|)/(1−|Γ|) and Return Loss (dB) = −20 log10|Γ|. Cited as a third, instrument-maker's confirmation of the definitions the two conversion tables above are built on.
  4. [4]IEC 60050-726, International Electrotechnical Vocabulary, Part 726: Transmission lines and waveguides — the definitional authority of record for the terms standing wave ratio, reflection coefficient, return loss and characteristic impedance. Access: gated. The IEC sells this part and only its front matter was retrievable; no clause of it was opened, and nothing on this page is attributed to a specific IEV entry. It is named here so that a reader who needs the formal definitions knows where they live rather than being sent to a secondary source that paraphrases them. IEEE Std 145, "IEEE Standard for Definitions of Terms for Antennas", is the equivalent authority on the antenna side and is likewise gated and unopened.

How this page was produced

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Quanta Calculator
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Γ = (Z_L − Z_0)/(Z_L + Z_0) · VSWR = (1+|Γ|)/(1−|Γ|) · RL = −20·lg|Γ| dB · ML = −10·lg(1−|Γ|²) dB · P_refl = 100·|Γ|² %
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