**Contents**

Antenna arrays

Two-element arrays

N-element linear array

Arrays with arbitrary geometry

References

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**Antenna arrays**

An antenna array is a group of multiple radiating elements whose signals are combined in such a way the overall radiation pattern is reinforced in certain desired direction and suppressed in other undesired directions. The combined radiation pattern of the system can be controlled by means of five parameters:- The geometrical distribution of the unitary elements (i.e., linear, circular, rectangular, spherical, etc.).
- The relative displacement between the elements.
- The excitation amplitude of the individual elements.
- The excitation phase of the individual elements.
- The relative pattern of the individual elements.

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**Two-element array**

Let us consider the simple case of an antenna array formed by two identical isotropic radiators. The total electric field *E*radiated by the two elements assuming no coupling between elements is proportional to

_{T}(Eq. 1) |

*a*is the magnitude excitation of the

_{i}*i*-th radiator,

*β*is the difference in phase excitation between the elements,

*k*is the phase constant (i.e.,

*k*=2

*π*/

*λ*, being

*λ*the wavelength), and

*r*is the distance to the

_{i}*i*-th radiator. Regarding the scheme shown in Fig. 1, and assuming far-field observations, we can do the next approximations

| (Eq. 2) |

(Eq. 3) |

Fig. 1: Geometry of a two-element antenna array (a) and far-field approximation (b). |

With regard to Eq. (3), it can be seen that the total field of the array can be expressed as the field radiated by a single element multiplied by a term that is widely referred as

*array factor*.

(Eq. 4) |

*AF*) is obtained as

(Eq. 5) |

*AF*of two-antenna arrays are represented in Fig. 2. In the case (a), the

*AF*of two isotropic elements separated half-wavelength is shown. In such a case, the waves are constructively combined in the directions perpendicular to the array, whereas a null is obtained in the array axis because of waves cancellation. In (b), the case of two elements separated a wavelength is analyzed. In this second case, maximums appear in the array axis and perpendicular to it. The

*AF*is cancelled at around 30 degrees. The case (c) shows an array with quarter-wavelength separation between elements, and a relative phase delay

*β*=-

*π*/4. In this third case, waves are combined in phase in one of the directions of the array axis, and cancelled in the opposite one.

Fig. 2: Radiation pattern of two omnidirectional elements: (a) separated λ/2, (b) separated λ, and (c) separated λ/4 and β=-π/2. |

##
**N-element linear array**

The geometry of a *N*-element equispaced linear array is shown in Fig. 3. Let us assume identical amplitudes and that each succeeding element has a progressive phase term

*β*relative to the preceding one. The array factor in this case can be calculated as

(Eq. 6) |

*AF*of a

*N*-element has a maximum when all the signals coming from a given angle

*θm*combine constructively. It occurs when

*kd*cos(

*θm*)+

*β*=0, that is at

(Eq. 7) |

*θm*by modifying the progressive phase difference

*β*between the elements. The antenna arrays whose direction of maximum radiation can be controlled by adjusting the relative phase term are known as

*phased arrays*or

*scanning arrays*.

Fig. 3: Geometry of an N-element linear antenna array. |

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**Arrays with arbitrary geometry**

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**References**

[1] C. A. Balanis, "Arrays: Linear, Planar, and Circular", in *Antenna Theory: Analysis and Design*, 2nd ed. New York, Wiley, 1997.