What is the array factor?
The array factor AF(θ) = Σ anejn(kd·cosθ + β) describes the pattern of an array of isotropic elements with spacing d, amplitudes an and progressive phase β. For N uniform elements, the normalized magnitude is |AF| = |sin(Nψ/2)/(N·sin(ψ/2))| with ψ = kd·cosθ + β, giving a first sidelobe at −13.26 dB and nulls where Nψ/2 = ±mπ.[1][2]
How do you compute beam direction and nulls?
The main beam lies where ψ = 0, i.e., cosθ0 = −β/(kd). Nulls occur at ψ = ±2πm/N (m = 1, 2, …, not a multiple of N). For a broadside array (β = 0) of length Nd, the half-power beamwidth is approximately 0.886λ/(Nd) radians for large N.[1]
What does an example look like?
Eight elements at d = λ/2, broadside: first nulls at sinθ = ±0.25 from broadside (±14.5°), HPBW ≈ 0.886/4 rad ≈ 12.7°, first sidelobe −12.8 dB (approaching −13.26 dB as N grows), directivity close to N = 8 (9 dBi) for isotropic elements at λ/2 spacing.[1][2]
How do amplitude weights change the array factor?
Non-uniform amplitudes trade beamwidth for sidelobes: binomial weights eliminate sidelobes at λ/2 spacing but broaden the beam a lot; Dolph–Chebyshev gives the narrowest beam for a specified equal sidelobe level; Taylor gives near-in sidelobes at a chosen level with decaying far-out sidelobes.[3][4] See array tapering.
Frequently asked questions
Why −13.26 dB?
It is the first sidelobe of the sin(x)/x function that describes a large uniform array.
Does the array factor include element patterns?
No; multiply by the element pattern for the total.
What is ψ?
The progressive phase difference between adjacent elements’ contributions in a given direction.
See also
References
Online sources accessed October 21, 2026; printed works cited by edition. See all sources.
- “Antenna Theory: Analysis and Design, 4th ed.”. C. A. Balanis, Wiley. 2016.
- “Phased Array Antenna Patterns — Part 1: Linear Array Beam Characteristics and Array Factor”. P. Delos, B. Broughton and J. Kraft, Analog Dialogue (Analog Devices). 2020.
- “A Current Distribution for Broadside Arrays Which Optimizes the Relationship Between Beam Width and Side-Lobe Level”. C. L. Dolph, Proceedings of the IRE, vol. 34, no. 6, pp. 335-348. June 1946.
- “Design of Line-Source Antennas for Narrow Beamwidth and Low Side Lobes”. T. T. Taylor, IRE Transactions on Antennas and Propagation, vol. 3, no. 1, pp. 16-28. January 1955.