Dipole Calculator

Calculate dipole antenna length, wavelength, and dimensions for optimal radio frequency performance

Calculate Dipole Antenna Dimensions

The frequency at which the antenna will operate

Use adjustment factor for high frequencies and thick conductors

Example Calculation

FM Radio Dipole (98.5 MHz)

Frequency: 98.5 MHz

Application: FM radio reception

Expected length: ~1.52 meters total

Calculation Steps

L = 468 / 98.5 = 4.751 feet

L = 4.751 × 0.3048 = 1.448 meters

Arm length = 1.448 / 2 = 0.724 meters

Result: Each arm = 72.4 cm

Common Frequency Bands

AM Radio0.5-1.6 MHz
Ham Radio HF3-30 MHz
FM Radio88-108 MHz
Ham Radio VHF144-148 MHz
Ham Radio UHF420-450 MHz
WiFi 2.4GHz2.4-2.5 GHz

Construction Tips

Cut wire 5% longer, then trim for best SWR

Use insulators at both ends and center

Keep antenna away from metal objects

Use 50Ω coaxial cable for feedline

Height above ground affects performance

Understanding Dipole Antennas

What is a Dipole Antenna?

A dipole antenna is the simplest and most fundamental type of antenna. It consists of two conducting elements (poles) separated by an insulator at the center. The total length is typically half the wavelength of the operating frequency.

Why Half-Wavelength?

The half-wavelength dipole is resonant at the design frequency, meaning it has optimal impedance characteristics (approximately 73 ohms) and maximum radiation efficiency. This makes it an excellent reference antenna for gain measurements.

Radiation Pattern

  • Maximum radiation perpendicular to the antenna
  • Nulls along the antenna axis
  • Doughnut-shaped 3D pattern

Calculation Formulas

Basic Formula

L = 468 / f (MHz) [feet]

L = 142.6 / f (MHz) [meters]

l = L / 2 (arm length)

Wavelength Formula

λ = c / f

c = 299,792,458 m/s

Dipole length ≈ λ/2

Adjustment Factor

k = 0.9787 - [11.86497 / (1 + (R/0.000449)^1.7925)^0.3]

R = (λ/2) / conductor_diameter

Note: The adjustment factor k accounts for the finite conductor diameter and becomes important at higher frequencies or with thicker conductors.