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What limits the performance of electrically small antennas?

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An antenna is electrically small when it fits inside a sphere of radius a with ka < 1 (k = 2π/λ). Wheeler (1947) and Chu (1948) showed that such antennas have a minimum radiation Q, so bandwidth shrinks with size. McLean’s form for a linearly polarized antenna is Qmin = 1/(ka)³ + 1/(ka).[1][2][3]

What does the limit mean in practice?

Fractional bandwidth is roughly inversely proportional to Q (for a given VSWR criterion), so halving the size of a small antenna reduces achievable bandwidth by roughly 8×. Adding loss lowers Q and widens bandwidth but reduces efficiency. Real antennas generally have Q well above the bound.[3]

How do designers cope?

What about matching networks?

Matching a high-Q antenna is also constrained by the Bode–Fano limit; lossless networks cannot overcome the Chu bound for bandwidth, only redistribute it.[4]

Frequently asked questions

What is ka?

Wavenumber times the radius of the smallest sphere enclosing the antenna.

Can metamaterials beat the Chu limit?

Passive linear antennas cannot; claims should be examined for loss or measurement errors.

Why do phone antennas need tuners?

They must cover many bands with limited volume.

References

Online sources accessed October 21, 2026; printed works cited by edition. See all sources.

  1. “Fundamental Limitations of Small Antennas”. H. A. Wheeler, Proceedings of the IRE, vol. 35, no. 12, pp. 1479-1484. December 1947.
  2. “Physical Limitations of Omni-Directional Antennas”. L. J. Chu, Journal of Applied Physics, vol. 19, pp. 1163-1175. December 1948.
  3. “A Re-Examination of the Fundamental Limits on the Radiation Q of Electrically Small Antennas”. J. S. McLean, IEEE Transactions on Antennas and Propagation, vol. 44, no. 5, pp. 672-676. May 1996.
  4. “Theoretical Limitations on the Broadband Matching of Arbitrary Impedances”. R. M. Fano, Journal of the Franklin Institute, vol. 249. 1950.