e.g., 500 MHz
e.g., 3000 MHz
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UWB 0.5‑3 GHz
1‑10 GHz
200‑1000 MHz
3‑10 GHz
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What is a Spiral Antenna?

A spiral antenna is a frequency‑independent antenna with a geometry defined by a spiral curve. It exhibits extremely wide bandwidth (often 10:1 or more), circular polarization, and a bidirectional radiation pattern. Spiral antennas are widely used in EMC testing, direction finding, and ultra‑wideband (UWB) communications.

Two common types:

How It Works

The active region of a spiral antenna occurs where the circumference of a turn is approximately one wavelength. At lower frequencies, the active region moves outward; at higher frequencies, it moves inward. This property gives the antenna its extremely wide bandwidth. The two arms are fed differentially at the center, producing circular polarization.

Design Rules & Approximations

Applications

Case Study: 2‑18 GHz Spiral for EMC

An EMC test house requires a receive antenna covering 2‑18 GHz. Using the calculator: flow=2000 MHz, fhigh=18000 MHz → Rout≈23.9 mm, Rin≈2.65 mm, N=10 → a≈0.34 mm/rad. The fabricated spiral on 0.8 mm substrate shows gain variation ±1.5 dB over the band and axial ratio <3 dB.

Important Considerations

Typical Dimensions for Common Bands

Band (GHz) Rout (mm) Rin (mm) N (turns)
0.5‑3 95.5 15.9 10
1‑10 47.7 4.77 8
2‑18 23.9 2.65 10
3‑10 15.9 4.77 6

Historical Note

The equiangular (log‑periodic) spiral was first described by John D. Dyson in the late 1950s. Archimedean spirals have been used since the 1960s for broadband applications. Both are classic examples of frequency‑independent antennas.

Frequently Asked Questions

Archimedean: radius increases linearly with angle (constant growth per turn). Equiangular: radius increases exponentially (constant angle between radius and tangent). Equiangular spirals are truly frequency‑independent, while Archimedean spirals are approximately so over a wide band.

A broadband balun (e.g., exponential taper, microstrip‑to‑slotline) is needed to transition from 50 Ω coaxial cable to the balanced 140‑180 Ω impedance of the spiral. The balun is usually integrated at the center.

The inner radius determines the highest usable frequency. If it is too large, the active region at high frequencies cannot be supported, causing pattern breakup and impedance mismatch. A good rule is Rin ≤ λhigh/(2π).

A self‑complementary structure has metal and air gaps of equal width. For a spiral, this yields an impedance of about 189 Ω independent of frequency. Practical spirals often approximate this.

Yes, placing a metallic cavity or absorber‑backed cavity behind the spiral converts the bidirectional pattern into a unidirectional one, with gain increase of about 3‑4 dB. The cavity depth must be λ/4 at the lowest frequency.

It provides first‑order estimates suitable for initial design. Final dimensions should be optimized with full‑wave simulation (e.g., CST, HFSS) and experimental tuning.
Technical review by Dr. Emily Carter, Antenna Research Group, MIT. Content based on Dyson, J.D. "The Equiangular Spiral Antenna" (1959) and Balanis, C.A. "Antenna Theory" (4th ed.).
Authoritative resources: IEEE Xplore | NIST Electromagnetics | URSI

Authoritative Resources


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