Wavelength and Frequency Calculator with Antenna Dimensions
The short answer
Wavelength in metres is 300 divided by the frequency in megahertz, and wavelength in feet is 984 divided by the frequency in megahertz. At 14.175 MHz that is 21.2 metres or 69.4 feet. A half-wave dipole in real wire is 468 divided by frequency in feet, and a quarter-wave vertical radiator is 234 divided by frequency.
- Metres
- 300 / f(MHz)
- Feet
- 984 / f(MHz)
- Half wave, wire
- 468 / f(MHz) ft
- Quarter wave
- 234 / f(MHz) ft
Every antenna dimension in amateur radio comes from one relationship: wavelength is the speed of light divided by frequency. Once that number is in front of you, half waves, quarter waves, spacing between elements, matching stub lengths and the height an antenna needs to be all fall out of it. This page gives the conversion and every derived dimension that follows.
Calculator
Frequency, wavelength and antenna dimensions
Free-space figures unless the wire correction is selected. Real conductors resonate as though about five percent longer than they are.
Full wavelength
Metric
Frequency
Half wave
Quarter wave
Eighth wave
Five-eighths wave
Free-space dimensions. For a real wire antenna, select the bare wire option, which applies the five percent end-effect correction.
Where the constants come from
Light travels at almost exactly 300 million metres per second in a vacuum, and radio waves are light. A wave at one megahertz completes a cycle in one microsecond, during which it travels 300 metres, so one megahertz has a wavelength of 300 metres. Every other frequency scales inversely: ten megahertz gives 30 metres, a hundred gives three.
In feet, the same speed is about 984 million feet per second, which gives the 984 constant. Halving it gives 492 for a half wavelength and 246 for a quarter, and these are the free-space numbers.
Real antennas are not free-space mathematical lines, and this is where the familiar 468 comes in. Two effects make a wire behave electrically longer than its physical length: end effect, which is the capacitance between the wire ends and everything near them, and the wire's own diameter relative to the wavelength. Together they add roughly five percent, so the physical wire has to be about five percent shorter to resonate where you want it. Ninety-five percent of 492 is 468, and 95 percent of 246 is 234.
| Constant | Gives | Use it for |
|---|---|---|
| 300 / f | Full wavelength in metres | Everything metric, and mental arithmetic |
| 984 / f | Full wavelength in feet | Antenna spacing, height in wavelengths, loop circumference |
| 492 / f | Half wavelength in feet, free space | Element spacing, height targets, matching line lengths |
| 468 / f | Half-wave dipole in wire, feet | Cutting a dipole or an end fed half wave |
| 246 / f | Quarter wavelength in feet, free space | Stub lengths before velocity factor |
| 234 / f | Quarter-wave radiator in wire, feet | Vertical radiators, dipole legs, elevated radials |
| 585 / f | Five-eighths wave in feet | VHF and UHF gain verticals, which need a base coil |
| 1005 / f | Full-wave loop circumference in feet | Quad elements and horizontal loop antennas |
Every amateur band, in one table
| Band | Frequency | Wavelength, m | Wavelength, ft | Half wave, ft | Quarter wave, ft |
|---|---|---|---|---|---|
| 160 m | 1.9 MHz | 157.9 | 517.9 | 258.9 | 129.5 |
| 80 m | 3.75 MHz | 80.0 | 262.4 | 131.2 | 65.6 |
| 60 m | 5.358 MHz | 56.0 | 183.7 | 91.8 | 45.9 |
| 40 m | 7.15 MHz | 42.0 | 137.6 | 68.8 | 34.4 |
| 30 m | 10.125 MHz | 29.6 | 97.2 | 48.6 | 24.3 |
| 20 m | 14.175 MHz | 21.2 | 69.4 | 34.7 | 17.4 |
| 17 m | 18.118 MHz | 16.6 | 54.3 | 27.2 | 13.6 |
| 15 m | 21.225 MHz | 14.1 | 46.4 | 23.2 | 11.6 |
| 12 m | 24.94 MHz | 12.0 | 39.5 | 19.7 | 9.86 |
| 10 m | 28.4 MHz | 10.6 | 34.6 | 17.3 | 8.66 |
| 6 m | 52 MHz | 5.77 | 18.9 | 9.46 | 4.73 |
| 2 m | 146 MHz | 2.05 | 6.74 | 3.37 | 1.68 |
| 1.25 m | 223.5 MHz | 1.34 | 4.40 | 2.20 | 1.10 |
| 70 cm | 440 MHz | 0.68 | 2.24 | 1.12 | 0.56 |
| 33 cm | 915 MHz | 0.33 | 1.08 | 0.54 | 0.27 |
| 23 cm | 1270 MHz | 0.24 | 0.77 | 0.39 | 0.19 |
The band names are approximate and historical. Twenty metres is really 21.2 metres at 14.175 MHz, forty metres is really 42, and fifteen metres is really 14.1. The names were rounded when the allocations were made and have been in use for a century, so there is no prospect of them being corrected and no need. There are 16 amateur bands listed in the full plan and every one of them is named this loosely.
Velocity factor: when wavelength gets shorter
Signals travel more slowly through anything denser than a vacuum, and wavelength shrinks in proportion. Frequency never changes, because that is set by the transmitter; only the physical distance one cycle occupies does.
| Medium | Velocity factor | Consequence |
|---|---|---|
| Air or vacuum | 1.00 | The reference. All the constants above assume this. |
| Bare copper antenna wire | About 0.95 | The end-effect correction that turns 492 into 468. |
| Insulated antenna wire | 0.92 to 0.97 | An insulated dipole resonates two to four percent low unless cut shorter. |
| Solid polyethylene coax | 0.66 | RG-58, RG-8X, RG-213. A quarter-wave stub is two thirds the free-space length. |
| Foam dielectric coax | 0.82 to 0.85 | LMR-400 class. Also why foam cables have lower loss. |
| Window or ladder line | 0.88 to 0.95 | Mostly air between the conductors, so close to free space. |
This matters in exactly two situations. The first is cutting an antenna from insulated wire, where the jacket slows the wave and the antenna needs to be two to four percent shorter than the bare-wire figure. The dipole calculator has that correction built in.
The second is any time you need a specific electrical length of transmission line: a quarter-wave matching transformer, a half-wave repeater line, a phasing harness between stacked antennas, or a coaxial stub used as a filter. There the physical length is the free-space length multiplied by the velocity factor, and getting it wrong by using the free-space figure produces a stub that resonates about a third away from where you wanted it. Worked through on the impedance matching calculator.
What wavelength decides beyond antenna length
- How high the antenna needs to be. Takeoff angle depends on height in wavelengths, not in feet, which is why 35 feet is generous on 20 metres and inadequate on 40. See the antenna height calculator.
- How far radials should run. An eighth of a wavelength on the ground, or a resonant quarter wavelength if elevated. See the radial planner.
- Where to put a common-mode choke. A quarter wavelength down the coax from an end fed antenna is the current maximum on the shield and the most effective position for it.
- How close nearby metal can be. Gutters, fences and siding within a small fraction of a wavelength detune an antenna and absorb power. The higher the band, the smaller that distance is in feet.
- Whether an antenna is physically possible. A full-size 160 metre dipole is 246 feet tip to tip. Knowing that in advance saves an afternoon of planning.
Building at the dimensions this page gives you
Cut two to three percent long and trim, always. The arithmetic lands close and the last couple of percent depends on wire diameter, insulation, height and what is nearby, none of which a formula knows about. A Paladin 14 AWG stranded copper wire, 500 ft$74.50 spool gives enough wire for several antennas plus mistakes, which is the right way to buy it, and a NanoVNA H4 vector network analyzer$89.90 tells you where the resonance actually landed rather than where the formula predicted.
For the trimming procedure and the reason it must be done at final height, see the dipole length calculator. For choosing which antenna to build in the first place, see choosing a first HF antenna.
Common questions
Questions people ask about this
How do I convert frequency to wavelength?
Wavelength in metres is 300 divided by the frequency in megahertz, and wavelength in feet is 984 divided by the frequency in megahertz. At 14.175 MHz that is 21.2 metres or 69.4 feet. Those two constants are the speed of light expressed in convenient units, and between them they answer almost every dimension question in antenna work.
Why is the 20 metre band at 14 MHz rather than 15 MHz?
Amateur band names are approximate and historical rather than exact. Three hundred divided by 14.175 is 21.2 metres, which was rounded to 20 for convenience when the bands were named, and the name stuck. The same applies throughout: the 40 metre band is closer to 42 metres and the 15 metre band is closer to 14.1 metres.
Why is a half-wave dipole 468 divided by frequency and not 492?
Because a real wire is not a mathematical line in free space. End effect, which is capacitance between the wire ends and everything nearby, plus the wire diameter itself, make the antenna behave as though it were about five percent longer than it physically is. Shortening the physical wire by that five percent gives the 468 constant that lands a typical wire dipole close to resonance.
What is velocity factor and how does it change wavelength?
Velocity factor is the speed of a signal in a medium as a fraction of the speed of light. In coaxial cable it is typically 0.66 for solid polyethylene and about 0.85 for foam dielectric, so a quarter wavelength of RG-213 is only 0.66 times the free-space quarter wavelength. It matters for matching stubs and phasing lines and is irrelevant for an ordinary feedline run.
How long is a quarter wavelength at 146 MHz?
About 19.2 inches in free space, or 234 divided by 146 which is 1.60 feet. That is the length of a typical quarter-wave mobile whip for the 2 metre band, and it is why those antennas are all about the same length regardless of manufacturer. The 5/8 wave version at 585 divided by 146 is about four feet.
Does wavelength change with the medium?
Yes. Frequency is fixed by the source and never changes, but wavelength depends on propagation speed, which is lower in any medium denser than vacuum. That is why insulated wire resonates at a slightly lower frequency than bare wire of the same length, why coax has a velocity factor, and why a loading coil can make a short antenna behave electrically longer than it is.
Keep going
Related on this site
- Dipole length calculator The most common use of this arithmetic.
- Quarter-wave vertical calculator Same constants, one radiator plus radials.
- Impedance matching calculator Where velocity factor becomes essential.
- The band plan Every band and where its name came from.
- Antenna height calculator Height in wavelengths, which is the number that matters.
- Choosing a first HF antenna Applying all of this to a real lot.
Keeping your own cut lengths, SWR sweeps and exposure record? The Station Build & Antenna Planner is the paid version of these pages: 8 printable worksheets you fill in with your own numbers, plus the full PDF, $29.
Disclaimer Researched guidance for planning purposes, not professional engineering, electrical or legal advice. Antenna work, RF exposure, mast and tower work, grounding and battery handling all carry real risk that depends on your specific site and installation. Verify anything safety-critical against current FCC rules, the National Electrical Code and the manufacturer's own documentation, and hire a professional where the job calls for one. We research equipment from published specifications, regulatory documents and verified owner reviews rather than claiming hands-on testing we have not done.