- Antenna Theory Tutorial
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- Antenna Basic Terms
- Antenna Theory - Fundamentals
- Antenna Theory - Basic Parameters
- Antenna Theory - Parameters
- Antenna Theory - Near & Far Fields
- Antenna Theory - Radiation Pattern
- Isotropic Radiation
- Antenna - Beam & Polarization
- Antenna Theory - Beam Width
- Antenna Theory - Reciprocity
- Antenna Theory - Poynting Vector

- Types of Antennas
- Antenna Theory - Types of Antennas
- Antenna Theory - Wire
- Antenna - Half-Wave Dipole
- Antenna - Half-Wave Folded Dipole
- Antenna - Full-Wave Dipole
- Antenna Theory - Short Dipole
- Antenna Theory - Long Wire
- Antenna Theory - V-Antennas
- Inverted V-Antenna
- Antenna Theory - Rhombic
- Antenna Theory - Loop
- Antenna Theory - Helical
- Antenna Theory - Aperture
- Antenna Theory - Horn
- Antenna Theory - Slot
- Antenna Theory - Micro Strip
- Antenna Theory - Lens
- Parabolic Reflector

- Antenna Arrays
- Antenna Theory - Antenna Arrays
- Antenna Theory - Collinear Array
- Antenna Theory - Broad-side Array
- Antenna Theory - End-fire Array
- Antenna Theory - Parasitic Array
- Yagi-Uda Antenna Theory
- Log-periodic Antenna Theory
- Turnstile Antenna Theory

- Wave Propagation
- Antenna - Spectrum & Transmission
- Antenna - Types of Propagation
- Antenna - Lonosphere & its Layers
- Terms in Wave Propagation

- Antenna Theory Useful Resources
- Antenna Theory - Quick Guide
- Antenna Theory - Useful Resources
- Antenna Theory - Discussion

Radiation intensity of an antenna is closely related to the direction of the beam focused and the efficiency of the beam towards that direction. In this chapter, let us have a look at the terms that deal with these topics.

According to the standard definition, “The ratio of maximum radiation intensity of the subject antenna to the radiation intensity of an isotropic or reference antenna, radiating the same total power is called the **directivity**.”

An Antenna radiates power, but the direction in which it radiates matters much. The antenna, whose performance is being observed, is termed as **subject antenna**.

Its **radiation intensity** is focused in a particular direction, while it is transmitting or receiving. Hence, the antenna is said to have its **directivity** in that particular direction.

The ratio of radiation intensity in a given direction from an antenna to the radiation intensity averaged over all directions, is termed as directivity.

If that particular direction is not specified, then the direction in which maximum intensity is observed, can be taken as the directivity of that antenna.

The directivity of a non-isotropic antenna is equal to the ratio of the radiation intensity in a given direction to the radiation intensity of the isotropic source.

The radiated power is a function of the angular position and the radial distance from the circuit. Hence, it is expressed by considering both the terms **θ** and **Ø**.

Where

${\phi(\theta,\phi)_{max}}$ is the maximum radiation intensity of subject antenna.

${\phi_{0}}$ is the radiation intensity of an isotropic antenna (antenna with zero losses).

According to the standard definition, “**Aperture efficiency** of an antenna, is the ratio of the effective radiating area (or effective area) to the physical area of the aperture.”

An antenna has an aperture through which the power is radiated. This radiation should be effective with minimum losses. The physical area of the aperture should also be taken into consideration, as the effectiveness of the radiation depends upon the area of the aperture, physically on the antenna.

The mathematical expression for aperture efficiency is as follows −

$$\varepsilon_{A} = \frac{A_{eff}}{A_{p}}$$where

$\varepsilon_{A}$ is Aperture Efficiency.

${A_{eff}}$ is effective area.

${A_{p}}$ is physical area.

According to the standard definition, “**Antenna Efficiency** is the ratio of the radiated power of the antenna to the input power accepted by the antenna.”

Simply, an Antenna is meant to radiate power given at its input, with minimum losses. The efficiency of an antenna explains how much an antenna is able to deliver its output effectively with minimum losses in the transmission line.

This is otherwise called as **Radiation Efficiency Factor** of the antenna.

The mathematical expression for antenna efficiency is given below −

$$\eta_{e} = \frac{P_{rad}}{P_{input}}$$Where

$\eta_{e}$is the antenna efficiency.

${P_{rad}}$ is the power radiated.

${P_{input}}$ is the input power for the antenna.

According to the standard definition, “**Gain** of an antenna is the ratio of the radiation intensity in a given direction to the radiation intensity that would be obtained if the power accepted by the antenna were radiated isotropically.”

Simply, gain of an antenna takes the directivity of antenna into account along with its effective performance. If the power accepted by the antenna was radiated isotropically (that means in all directions), then the radiation intensity we get can be taken as a referential.

The term

**antenna gain**describes how much power is transmitted in the direction of peak radiation to that of an isotropic source.**Gain**is usually measured in**dB**.Unlike directivity, antenna gain takes the losses that occur also into account and hence focuses on the efficiency.

The equation of gain, G is as shown below.

$$G = \eta_{e}D$$Where

**G**is gain of the antenna.$\eta_{e}$is the antenna’s efficiency.

**D**is the directivity of the antenna.

The unit of gain is **decibels** or simply **dB**.

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