Dipole Antenna Length Calculator

Compute half-wave dipole element lengths, quarter-wave monopole height, and shortened dipole dimensions with velocity factor correction — for any frequency from AM to microwave.

Frequency
Design frequency f
Common bands
VF =
Dipole diagram
Half-wave dipole — —
Total Length (λ/2)
—
mm
Each Element (λ/4)
—
mm
Free-Space λ
—
mm
Quarter-wave monopole
Monopole Length (λ/4)
—
mm
5/8λ Vertical
—
mm
3/8λ Vertical
—
mm
Key formulas
Half-wave dipole
L = 0.4775 · c f
c = 299,792,458 m/s · accounts for end effect
Quarter-wave monopole
L = 0.2388 · c f
= half of half-wave dipole element
With velocity factor
Lvf = L × VF
VF = 0.95 typical for bare wire
End-effect factor
k = 0.955
Actual dipole ≈ 95.5% of ideal λ/2
📡 Need the exact length for your wire, height & ground? Dipole & Monopole Antenna Calculator Method of Moments simulation: resonant length for your conductor, impedance, SWR, gain, takeoff angle, radial droop and matching. →

Common Frequency Bands Using Dipole Antennas

The table below lists the most common RF bands that use dipole or dipole-derivative antennas, with pre-calculated half-wave dipole total length, each element length, and quarter-wave monopole height. All lengths assume ideal free-space with an end-effect factor of 0.955 (VF = 1.0). Multiply by your velocity factor for insulated wire or enclosures.

Band / Application Frequency λ/2 Total Each Element (λ/4) Monopole (λ/4) Notes
AM Broadcast 1 MHz 143.3 m 71.6 m 71.6 m Vertical monopoles used in practice
160m Amateur 1.84 MHz 77.8 m 38.9 m 38.9 m Often end-fed or shortened
80m Amateur 3.6 MHz 39.8 m 19.9 m 19.9 m Popular DX band
40m Amateur 7.1 MHz 20.2 m 10.1 m 10.1 m Most popular HF dipole band
20m Amateur 14.2 MHz 10.1 m 5.04 m 5.04 m Primary DX & contest band
15m Amateur 21.2 MHz 6.76 m 3.38 m 3.38 m Harmonic of 40m
10m Amateur 28.5 MHz 5.02 m 2.51 m 2.51 m Excellent DX when solar cycle active
6m Amateur 50 MHz 2.86 m 1.43 m 1.43 m "Magic band" — sporadic-E propagation
FM Broadcast 98 MHz 1.46 m 730 mm 730 mm Horizontal dipoles used at broadcast towers
2m Amateur / APRS 145 MHz 987 mm 494 mm 494 mm Most popular VHF amateur band
ADS-B Aviation 1090 MHz 131 mm 65.7 mm 65.7 mm Aircraft transponder tracking
GPS L1 1575 MHz 91.0 mm 45.5 mm 45.5 mm Patch antennas preferred in practice
LoRa / ISM 433 433 MHz 330 mm 165 mm 165 mm IoT, remote controls, garage openers
LoRa EU 868 / US 915 868 MHz 165 mm 82.5 mm 82.5 mm LPWAN, smart meters, agriculture
Wi-Fi / Bluetooth 2.4 GHz 2400 MHz 59.7 mm 29.8 mm 29.8 mm PCB trace dipoles common on modules
Wi-Fi 5 GHz (802.11ac) 5500 MHz 26.1 mm 13.0 mm 13.0 mm Dual-band routers use λ/2 dipoles
5G Sub-6 GHz 3500 MHz 40.9 mm 20.4 mm 20.4 mm Dipole arrays in 5G base stations

Why Dipole Antennas Are Everywhere

The half-wave dipole is the fundamental antenna from which almost all other antenna types derive. It has a predictable radiation pattern (figure-of-eight in the plane containing the element), a feed impedance of approximately 73 Ω in free space, and gain of 2.15 dBi referenced to an isotropic radiator. From the simple centre-fed wire dipole to the driven element in a Yagi, the folded dipole in a log-periodic array, and the printed dipole on a PCB, this antenna is the reference from which all antenna engineering starts.

The End-Effect Factor (k = 0.955)

A theoretical half-wave dipole resonates when it is exactly λ/2 long. In practice, a real conductor has finite thickness which alters the charge distribution near the wire ends, effectively lengthening the electrical length. This means a real dipole must be cut slightly shorter than the theoretical λ/2 to achieve resonance. The standard correction is:

Half-wave dipole practical length
L = 0.955 × (c / 2f) = 0.4775 × c / f
Quick approximation: L (mm) ≈ 143,250 / f (MHz)

Velocity Factor and Insulated Wire

When a dipole is constructed from insulated wire — or when it is close to a surface, enclosure, or PCB ground plane — the surrounding dielectric slows the wave along the conductor. The velocity factor (VF) captures this: VF = 1.0 for bare wire in free space, and typically 0.92–0.97 for thin PVC-insulated wire. Coaxial cable dipoles can have VF as low as 0.66. Multiply the free-space dipole length by VF to get the physical cutting length.

The 0.955 factor is an average. The true factor depends on how thick the conductor is relative to the wavelength: about 0.93 for thick tubing (λ/d ≈ 100), 0.96 for typical wire (λ/d ≈ 1000) and 0.97–0.98 for thin wire at HF. Height above ground and nearby objects shift it further. To get the resonant length for your exact wire, mounting height and soil, use the Dipole & Monopole Antenna Calculator, which solves the antenna with the Method of Moments and also shows its impedance, SWR bandwidth and radiation pattern.

Practical rule: Cut your dipole 5% longer than the formula suggests, then trim in small increments (2–3 mm per side) while checking SWR. It is easier to shorten a dipole than to extend it.

Quarter-Wave Monopole vs Half-Wave Dipole

A quarter-wave monopole over a ground plane (radials or counterpoise) is electrically equivalent to half of a centre-fed dipole. The ground plane provides the mirror image of the missing half. The feed impedance is approximately half that of a dipole — about 36.5 Ω — making it a reasonably good match to 50 Ω coaxial cable. Common examples include the rubber-duck antennas on handheld radios, vehicle roof-mount antennas, and PCB whip antennas on IoT modules.

An elevated ground-plane antenna with a few radials is a poorer mirror than a solid plane: with horizontal radials its feed impedance drops to about 22 Ω, and drooping the radials by roughly 40–45° raises it to 50 Ω. The Monopole & Ground-Plane Antenna Calculator solves the radial length and droop angle for a direct 50 Ω feed and shows the gain and takeoff angle over real ground.

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