 Directivity

In electromagnetics, directivity is a figure of merit for an antenna. It measures the power density the antenna radiates in the direction of its strongest emission, versus the power density radiated by an ideal isotropic radiator (which emits uniformly in all directions) radiating the same total power.
An antenna's directivity is a component of its gain; the other component is its (electrical) efficiency. Directivity is an important measure because most emissions are intended to go in a particular direction or at least in a particular plane (horizontal or vertical); emissions in other directions or planes are wasteful (or worse).
The directivity of an actual antenna can vary from 1.76 dBi for a short dipole, to as much as 50 dBi for a large dish antenna^{[1]}.
Contents
Definition
The directivity of an antenna is the maximum value of its directive gain. Directive gain is represented as D(θ,ϕ), and compares the radiation intensity (power per unit solid angle) U that an antenna creates in a particular direction against the average value over all directions:
...where:
 θ and ϕ are the standard spherical coordinates angles
 U is the radiation intensity, which is the power density per unit solid angle such that:
 4π is the total solid angle for a sphere (also the surface area of a unit sphere, similar to 2π being the total angle for a circle and the perimeter of a unit circle).
 The denominator, , represents the average radiated power density
Directivity is represented as simply D, and is the maximum directive gain value found among all possible solid angles:
The equation can also be written as:
The word directivity is also sometimes used as a synonym for directive gain. This usage is readily understood, as the direction will be specified, or directional dependence implied. Later editions of the IEEE Dictionary^{[2]} specifically endorse this usage; nevertheless it has yet to be universally adopted.
Relation to beam width
The beam solid angle, represented as Ω_{A}, is defined as the solid angle which all power would flow through if the antenna radiation intensity were constant and maximum value. If the beam solid angle is known, then directivity can be calculated as:
...which simply calculates the ratio of the beam solid angle to the total surface area of the sphere it intersects.
The beam solid angle can be approximated for antennas with one narrow major lobe and very negligible minor lobes, by simply multiplying the halfpower beamwidths (in radians) in two perpendicular planes. The halfpower beamwidth is simply the angle in which the radiation intensity is at least half of the peak radiation intensity.
The same calculations can be performed in degrees rather than in radians:
...where Θ_{1d} is the halfpower beamwidth in one plane (degrees) and Θ_{2d} is the halfpower beamwidth in a plane at a right angle to the other (degrees).
In planar arrays, a better approximation is:
Expression in decibels
The directivity is rarely expressed as the unitless number D. Rather, the directivity is usually expressed as a decibel comparison to a reference antenna:
The reference antenna is usually the theoretical perfect isotropic radiator which radiates uniformly in all directions and hence has a directivity of 1. The calculation is therefore simplified to:
Another common reference antenna is the theoretical perfect halfwave dipole which radiates perpendicular to itself with a directivity of 1.64:
Accounting for polarization
When polarization is taken under consideration, three additional measures can be calculated:
Partial directive gain
Partial directive gain is the power density in a particular direction and for a particular component of the polarization, divided by the average power density for all directions and all polarizations. For any pair of orthogonal polarizations (such as lefthandcircular and righthandcircular), the individual power densities simply add to give the total power density. Thus, if expressed as dimensionless ratios rather than in dB, the total directive gain is equal to the sum of the two partial directive gains.^{[2]}
Partial directivity
Partial directivity is calculated in the same manner as the partial directive gain, but without consideration of antenna efficiency (i.e. assuming a lossless antenna). It is similarly additive for orthogonal polarizations.
Partial gain
Partial gain is calculated in the same manner as gain, but considering only a certain polarization. It is similarly additive for orthogonal polarizations.
Main article: Antenna gainIn other fields
The term directivity is also used in acoustics, as is a measure of the radiation pattern from a source indicating how much of the total energy from the source is radiating in a particular direction. In electroacoustics, these patterns commonly include omnidirectional, cardioid and hypercardioid microphone polar patterns. A loudspeaker with a high degree of directivity (narrow dispersion pattern) can be said to have a high Q.^{[3]}
References
 ^ Antenna Tutorial
 ^ ^{a} ^{b} Institute of Electrical and Electronics Engineers, “The IEEE standard dictionary of electrical and electronics terms”; 6th ed. New York, N.Y., Institute of Electrical and Electronics Engineers, c1997. IEEE Std 1001996. ISBN 1559378336 [ed. Standards Coordinating Committee 10, Terms and Definitions; Jane Radatz, (chair)]
 ^ Rane Professional Audio Reference Home
 Coleman, Christopher (2004). "Basic Concepts". An Introduction to Radio Frequency Engineering. Cambridge University Press. ISBN 0521834813.
Categories: Antennas (radio)
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