The Antenna Length Calculator determines the resonant length for dipole, quarter-wave, and full-wave antennas at any frequency, applying velocity factor corrections for wire and conductor type. Used by radio engineers and amateur radio operators to design antennas for any frequency band.
1.424
m
142.4
cm
4.672
ft
56.06
in
2.9979
m
1.424
m
142.4
cm
4.672
ft
56.06
in
2.9979
m
Cut an antenna too long or too short and it won't resonate on your target frequency — SWR will spike, transmitter output will drop, and your signal will suffer. The calculator for antenna length finds the exact physical length for a resonant dipole, quarter-wave vertical, or full-wave loop at any operating frequency, factoring in the velocity factor that accounts for the wave traveling slightly slower in real conductors than in free space.
All resonant antenna lengths derive from the relationship between wavelength λ and frequency f:
λ = c / f — where c = 299,792,458 m/s (speed of light in free space)
For wire antennas, the physical length is shortened by the velocity factor (VF) — typically 0.95–0.98 for bare copper wire and 0.66–0.80 for insulated wire:
The classic shortcut formula — 468/f(MHz) feet for a half-wave dipole in feet — embeds VF ≈ 0.95 and unit conversion. Use this online calculator for any antenna type, frequency, and velocity factor. The frequency-wavelength converter provides the λ calculation as a standalone tool.
Electromagnetic waves travel at exactly c in vacuum, but in real conductors and dielectric materials they travel slower — a fraction of c known as the velocity factor. This slowing shortens the physical antenna length required to achieve electrical resonance. Typical velocity factors:
The quarter-wave stub, commonly used for impedance matching and RF grounding, must account for VF to achieve the correct electrical length at the target frequency. The dipole antenna calculator provides the complete dipole design including feedpoint impedance.
For the most common amateur radio HF bands, approximate half-wave dipole lengths (bare wire, VF = 0.95):
The quarter-wave antenna calculator and antenna and RF calculators category cover the full range of antenna design and RF engineering tools.
Real-world antennas must be trimmed to final resonance after construction because the theoretical length rarely produces exactly 1:1 SWR at the target frequency. End effects from wire termination, surrounding objects, antenna height, and ground conductivity all shift the resonant frequency slightly. The standard practice is to cut the antenna 2–5% longer than the calculated length, then trim 1–2 cm at a time while monitoring SWR with an analyzer until minimum SWR is achieved at the target frequency. This iterative physical trimming is the final step in all wire antenna construction.
The calculator first computes the free-space wavelength as λ = (c / f_MHz) × VF, where c = 299.792458 m/MHz and VF is the velocity factor. The antenna physical length is then L = λ × fraction, where fraction = 1 for full wave, 0.5 for half wave, 0.25 for quarter wave, and 0.625 for 5/8 wave. Results are provided in meters, centimeters, feet, and inches for convenience.
The calculated length is the resonant physical length. In practice, start slightly long (2–3%) and trim while measuring SWR (Standing Wave Ratio). A perfectly resonant antenna will show minimum SWR (ideally below 1.5:1) at the target frequency. If the antenna is too long, it will resonate below the target frequency; too short, above it.
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Results
A half-wave dipole for 98 MHz FM radio is about 145.4 cm (57.2 inches) long — each arm of the dipole would be approximately 72.7 cm.
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Results
A quarter-wave vertical for the 2-meter ham band at 144.5 MHz is approximately 49.3 cm (19.4 inches) long.
Because of the velocity factor — electromagnetic waves travel slightly slower in physical conductors than in free space. For bare wire, the velocity factor is typically 0.95–0.97, meaning the physical antenna is 3–5% shorter than the free-space calculation. End effects at the antenna tips also shorten the effective electrical length slightly.
For bare copper or aluminum wire in free air: 0.95–0.97. For insulated wire: 0.85–0.95 depending on insulation type and thickness. For transmission lines used as antenna elements (e.g., folded dipoles): use the line's published VF. When in doubt, use 0.95 as a starting point and trim to resonance.
A half-wave dipole in free space presents approximately 73 Ω. A quarter-wave monopole over a perfect ground plane presents approximately 36.5 Ω. A full-wave loop is approximately 100–150 Ω. A 5/8-wave vertical presents a moderate impedance around 50 Ω with a matching network. Feed impedance changes significantly with height above ground and nearby objects.
Antenna length is inversely proportional to frequency — higher frequencies require shorter antennas. A 2.4 GHz WiFi antenna is only a few centimeters long, while an HF shortwave antenna for 7 MHz can be 20 meters or more. This inverse relationship is the fundamental constraint of antenna design.
Yes, but the velocity factor on PCB substrates is significantly lower than free space — typically 0.55–0.75 depending on the substrate's dielectric constant (εr). For FR4 (εr ≈ 4.4), the effective wavelength is roughly 1/√εr ≈ 0.476 times the free-space wavelength. Enter the appropriate VF for your substrate for accurate results.
SWR (Standing Wave Ratio) is a measure of impedance mismatch between the antenna and the feed line. A perfectly matched antenna shows SWR = 1:1. When antenna length is off-resonance, the feed point impedance gains a reactive component, increasing SWR. High SWR causes power to be reflected back to the transmitter, reducing efficiency and potentially damaging the final amplifier stage. Target SWR below 1.5:1 for most practical systems.
The 5/8-wave vertical concentrates more radiation toward the horizon (lower elevation angles) compared to the quarter-wave, which results in approximately 3 dBi gain over the quarter-wave in the horizontal direction. This is highly desirable for mobile communications where you want to maximize range to distant stations rather than radiate power upward.
Yes, by reciprocity — the same gain and directivity principles apply to both transmit and receive. However, for receiving only (e.g., AM/FM radios), the antenna does not need to be as precisely resonant because the received signal is small and minor mismatches do not cause damaging reflections. Resonance still improves receive sensitivity, particularly for weak-signal applications.
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