### Abstract

The far field of an antenna is generally considered to be the region where the outgoing wavefront is planar and the antenna radiation pattern has a polar variation and is independent of the distance from the antenna. Hence, to generate a local plane wave in the far field, the radial component of the electric field must be negligible compared to the transverse component. Also, the ratio of the electric and the magnetic far fields should equal the intrinsic impedance of the medium. These two requirements-that the radial component of the field should be negligible when compared with the transverse component and the ratio of the electric and the magnetic fields equal the intrinsic impedance of the medium-must hold in all angular directions from the antenna. So to determine the starting distance for the far field, we need to examine the simultaneous satisfaction of these two properties for all θ and φ angular directions, where θ is the angle measured from the z-axis and φ is the angle measured from the x-axis. It is widely stated in the antenna literature that the far field of an antenna operating in free space, where all the aforementioned properties must hold, starts from a distance of 2D^{2}/λ, where D is the maximum dimension of the antenna and λ is the operating wavelength.

Original language | English (US) |
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Article number | 7590187 |

Pages (from-to) | 115-124 |

Number of pages | 10 |

Journal | IEEE Antennas and Propagation Magazine |

Volume | 58 |

Issue number | 5 |

DOIs | |

State | Published - Oct 2016 |

### ASJC Scopus subject areas

- Condensed Matter Physics
- Electrical and Electronic Engineering

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## Cite this

*IEEE Antennas and Propagation Magazine*,

*58*(5), 115-124. [7590187]. https://doi.org/10.1109/MAP.2016.2594002