lecture 16 to 24 types of antennas

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Chapter 03 Lecture 16-24 Types of ANTENNAS By :- Engr. Nuzhat Madina Lecturer ISRA university Hyderabad 06/09/22 1

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Types of Antenna

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Page 1: Lecture 16 to 24 Types of Antennas

Chapter 03 Lecture 16-24

Types of ANTENNAS

By :- Engr. Nuzhat Madina

LecturerISRA university Hyderabad

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HISTORY

• The first antennas were built in 1888 by German physicist Heinrich Hertz in his pioneering experiments to prove the existence of electromagnetic waves predicted by the theory of James Clerk Maxwell.

• Hertz placed dipole antennas at the focal point of parabolic reflectors for both transmitting and receiving. He published his work in Annalen der Physik und Chemie (vol. 36, 1889).

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INTRODUCTION• An antenna is an electrical device which converts

electric currents into radio waves, and vice versa. It is usually used with a radio transmitter or radio receiver.

• In transmission, a radio transmitter applies an oscillating radio frequency electric current to the antenna's terminals, and the antenna radiates the energy from the current as electromagnetic waves (radio waves).

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• Transmitting Antenna: Any structure designed to efficiently radiate electromagnetic radiation in a preferred direction is called a transmitting antenna.

• In reception, an antenna intercepts some of the power of an electromagnetic wave in order to produce a tiny voltage at its terminals, that is applied to a receiver to be amplified. An antenna can be used for both transmitting and receiving.

• Receiving Antenna: Any structure designed to efficiently receive electromagnetic radiation is called a receiving antenna

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BASIC STRUCTURE

• It is a metallic conductor system capable of radiating and receiving EM waves.

• Typically an antenna consists of an arrangement of metallic conductors (“elements"), electrically connected (often through a transmission line) to the receiver or transmitter.

• An oscillating current of electrons forced through the antenna by a transmitter will create an oscillating magnetic field around the antenna elements, while the charge of the electrons also creates an oscillating electric field along the elements.

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• These time-varying fields radiate away from the antenna into space as a moving electromagnetic field wave.

• Conversely, during reception, the oscillating electric and magnetic fields of an incoming radio wave exert force on the electrons in the antenna elements, causing them to move back and forth, creating oscillating currents in the antenna.

• Antenna reciprocity : can be used as transmitter and receiver.In two way communication same antenna can be used as transmitter and receiver.

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• Antennas may also contain reflective or directive elements or surfaces not connected to the transmitter or receiver, such as parasitic elements, parabolic reflectors or horns, which serve to direct the radio waves into a beam or other desired radiation pattern.

• Antennas can be designed to transmit or receive radio waves in all directions equally (omnidirectional antennas), or transmit them in a beam in a particular direction, and receive from that one direction only ( directional or high gain antennas).

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WHY ANTENNAS ?

• Need of antenna arisen when two person wanted to communicate between them when separated by some distance and wired communication is not possible.

• Antennas are required by any radio receiver or transmitter to couple its electrical connection to the electromagnetic field.

• Radio waves are electromagnetic waves which carry signals through the air (or through space) at the speed of light with almost no transmission loss.

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• Radio transmitters and receivers are used to convey signals (information) in systems including broadcast (audio) radio, television, mobile telephones , point-to-point communications links (telephone, data networks), satellite links.

• Radio waves are also used directly for measurements in technologies including Radar, GPS, and radio astronomy.

• In each and every case, the transmitters and receivers involved require antennas, although these are sometimes hidden (such as the antenna inside an AM radio or inside a laptop computer equipped with wi-fi).

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WHERE USED?

• Antennas are used in systems such as radio and television broadcasting, point to point radio communication, wireless LAN, radar and space exploration

• Antennas are most utilized in air or outer space

• But can also be operated under water or even through soil and rock at certain frequencies for short distances

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RADIATION MECHANISM• Ideally all incident energy must be reflected back

when open circuit. But practically a small portion of electromagnetic energy escapes from the system that is it gets radiated.

• This occurs because the line of force don’t undergo complete phase reversal and some of them escapes.

G

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• The amount of escaped energy is very small due to mismatch between transmission line and surrounding space.

• Also because two wires are too close to each other, radiation from one tip will cancel radiation from other tip.( as they are of opposite polarities and distance between them is too small as compared to wavelength )

G

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• To increase amount of radiated power open circuit must be enlarged , by spreading the two wires.

• Due to this arrangement, coupling between transmission line and free space is improved.

• Also amount of cancellation has reduced.

• The radiation efficiency will increase further if two conductors of transmission line are bent so as to bring them in same line.

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Types of Antenna

• Wire • Aperture• Arrays

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Wire antenna

• Dipole• Loop• Folded dipoles• Helical antenna• Yagi (array of dipoles)• Corner reflector• Many more types

Horizontal dipole

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Aperture antenna

• Collect power over a well defined aperture• Large compared to wavelength• Various types:

– Reflector antenna– Horn antenna– Lens

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TYPES OF ANTENNAS• According to their applications and technology available,

antennas generally fall in one of two categories: 1.Omnidirectional or only weakly directional antennas

which receive or radiate more or less in all directions. These are employed when the relative position of the other station is unknown or arbitrary. They are also used at lower frequencies where a directional antenna would be too large, or simply to cut costs in applications where a directional antenna isn't required.

2. Directional or beam antennas which are intended to preferentially radiate or receive in a particular direction or directional pattern.

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• According to length of transmission lines available, antennas generally fall in one of two categories:

1. Resonant Antennas – is a transmission line, the length of which is exactly equal to multiples of half wavelength and it is open at both ends.

2.Non-resonant Antennas – the length of these antennas is not equal to exact multiples of half wavelength. In these antennas standing waves are not present as antennas are terminated in correct impedance which avoid reflections. The waves travel only in forward direction .Non-resonant antenna is a unidirectional antenna.

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RADIATION PATTERN

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• The radiation pattern of an antenna is a plot of the relative field strength of the radio waves emitted by the antenna at different angles.

• It is typically represented by a three dimensional graph, or polar plots of the horizontal and vertical cross sections. It is a plot of field strength in V/m versus the angle in degrees.

• The pattern of an ideal isotropic antenna , which radiates equally in all directions, would look like a sphere.

• Many non-directional antennas, such as dipoles, emit equal power in all horizontal directions, with the power dropping off at higher and lower angles; this is called an omni directional pattern and when plotted looks like a donut.

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• The radiation of many antennas shows a pattern of maxima or "lobes" at various angles, separated by “nulls", angles where the radiation falls to zero.

• This is because the radio waves emitted by different parts of the antenna typically interfere, causing maxima at angles where the radio waves arrive at distant points in phase, and zero radiation at other angles where the radio waves arrive out of phase.

• In a directional antenna designed to project radio waves in a particular direction, the lobe in that direction is designed larger than the others and is called the "main lobe".

• The other lobes usually represent unwanted radiation and are called “sidelobes". The axis through the main lobe is called the "principle axis" or “boresight axis".

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ANTENNA GAIN

• Gain is a parameter which measures the degree of directivity of the antenna's radiation pattern. A high-gain antenna will preferentially radiate in a particular direction.

• Specifically, the antenna gain, or power gain of an antenna is defined as the ratio of the intensity (power per unit surface) radiated by the antenna in the direction of its maximum output, at an arbitrary distance, divided by the intensity radiated at the same distance by a hypothetical isotropic antenna.

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• The gain of an antenna is a passive phenomenon - power is not added by the antenna, but simply redistributed to provide more radiated power in a certain direction than would be transmitted by an isotropic antenna.

• High-gain antennas have the advantage of longer range and better signal quality, but must be aimed carefully in a particular direction.

• Low-gain antennas have shorter range, but the orientation of the antenna is relatively inconsequential.

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• For example, a dish antenna on a spacecraft is a high-gain device that must be pointed at the planet to be effective, whereas a typical Wi-Fi antenna in a laptop computer is low-gain, and as long as the base station is within range, the antenna can be in any orientation in space.

• In practice, the half-wave dipole is taken as a reference instead of the isotropic radiator. The gain is then given in dBd (decibels over dipole)

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ANTENNA EFFICIENCY

• Efficiency of a transmitting antenna is the ratio of power actually radiated (in all directions) to the power absorbed by the antenna terminals.

• The power supplied to the antenna terminals which is not radiated is converted into heat. This is usually through loss resistance in the antenna's conductors, but can also be due to dielectric or magnetic core losses in antennas (or antenna systems) using such components.

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POLARIZATION• The polarization of an antenna is the orientation of

the electric field (E-plane) of the radio wave with respect to the Earth's surface and is determined by the physical structure of the antenna and by its orientation.

• A simple straight wire antenna will have one polarization when mounted vertically, and a different polarization when mounted horizontally.

• Reflections generally affect polarization. For radio waves the most important reflector is the ionosphere - signals which reflect from it will have their polarization changed

• LF,VLF and MF antennas are vertically polarized

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BEAM-WIDTH

• Beam-width of an antenna is defined as angular separation between the two half power points on power density radiation pattern OR

• Angular separation between two 3dB down points on the field strength of radiation pattern

• It is expressed in degrees

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Antenna Principles

• Radiation Resistance

• Antenna Pattern2I

PR rad

rad

• Directivity and Directivity and GainGain

• BandwidthBandwidth

• Signal-To-Noise Signal-To-Noise RatioRatio

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½ Wave Dipole

¼ Wave Monopole

Antenna Types

E:

H:

E: H:

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Half Wave Dipole• The world’s most popular antenna is the half-wave dipole. This means

that the total length of the antenna is equal to half of the wavelength of the signal you’re trying to transmit or receive. The dipole is fed by a two wire line where the two currents are equal in amplitude but opposite in direction. This shows the current distribution; the ends are essentially an open circuit, so most of the energy is radiated out the center of the antenna. The electric field radiates in a donut shaped pattern around the dipole axis, and the magnetic field radiates in a circle outward from the antenna.

• The quarter-wave monopole is very similar; it basically consists of one-half a dipole plus a perfectly conducting plane. Most of the parameters are halved, including the total power radiated.

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Loop Antennas

Microstrip Antennas

Antenna Types

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Loop Antennas & Microstrip Antennas

• A third type of antenna is the loop antenna. These are very useful as receivers, especially for low frequencies when dipoles would become very large.

• Microstrip or patch antennas are often manufactured directly on a printed circuit board. The dielectric between the two rectangular conductors is simply the printed-circuit substrate. These antennas are generally built for devices that require small antennas, leading to frequencies usually in the gigahertz.

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Horn Antennas

Helical Antennas

Antenna Types

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Helical Antennas and Horn Antennas

• Helical antennas are used because they are circularly polarized. This means that they radiate in both the vertical and horizontal directions, unlike the dipole which only radiates normal to its axis.

• Horn antennas are obviously very directional. The shape of the horn determines if the electric or magnetic fields are maximized. The gain is very high in the direction of the horn’s axis.

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Antenna ApplicationsVHF and UHF Antennas

UHF/VHF/FMReceiving AntennaTransmitting Tower

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Antenna Applications

• Another application for antennas that I’m sure we’re all familiar with is VHF and UHF antennas, which stand for Very High Frequency and Ultra High Frequency. You’ve all seen the tall transmitting towers. They need to be large enough to achieve the desired frequency and provide a large range of coverage. VHF and UHF covers frequencies from 3 MHz to 3000 MHz and includes television and FM radio broadcasting.

• The most common type of receiving antenna is called a Yagi array antenna. The array has different size conductors to receive different frequencies. Yagi arrays are highly directional, so they should always be pointed towards the transmitter tower.

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Antenna Applications

Wireless Communications

¼ Wave Helical ¼ Wave 2-in-1

¼ Wave Whip

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Antenna Applications• Antennas have lots of applications in wireless communications. Many

different types of antennas can be used, and they all have their own advantages. Two common antennas are the quarter wave helical and quarter wave whip antennas. The whip, which is the same as a monopole, is the most common antenna for cellular phones, and is typically used in the 400 to 500 MHz range. The quarter wave helical antenna is smaller than the whip and has similar performance. Lately it is used in the 800 to 1000 MHz bands.

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ISOTROPIC ANTENNA

• Isotropic antenna or isotropic radiator is a hypothetical (not physically realizable) concept, used as a useful reference to describe real antennas.

• Isotropic antenna radiates equally in all directions. – Its radiation pattern is

represented by a sphere whose center coincides with the location of the isotropic radiator.

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• It is considered to be a point in space with no dimensions and no mass. This antenna cannot physically exist, but is useful as a theoretical model for comparison with all other antennas.

• Most antennas' gains are measured with reference to an isotropic radiator, and are rated in dBi (decibels with respect to an isotropic radiator).

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Dipole antenna• In radio and telecommunications a dipole antenna or doublet[1] is the

simplest and most widely used class of antenna.[2][3] It consists of two identical conductive elements[4] such as metal wires or rods, which are usually bilaterally symmetrical.[3][5][6] The driving current from thetransmitter is applied, or for receiving antennas the output signal to thereceiver is taken, between the two halves of the antenna. Each side of thefeedline to the transmitter or receiver is connected to one of the conductors. This contrasts with a monopole antenna, which consists of a single rod or conductor with one side of the feedline connected to it, and the other side connected to some type of ground.[6] A common example of a dipole is the "rabbit ears" television antenna found on broadcast television sets.

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• The most common form of dipole is two straight rods or wires oriented end to end on the same axis, with the feedline connected to the two adjacent ends. This is the simplest type of antenna from a theoretical point of view.[1] Dipoles are resonant antennas, meaning that the elements serve as resonators, with standing waves of radio current flowing back and forth between their ends. So the length of the dipole elements is determined by the wavelength of the radio waves used.[3] The most common form is the half-wave dipole, in which each of the two rod elements is approximately 1/4 wavelength long, so the whole antenna is a half-wavelength long. The radiation pattern of a vertical dipole is omnidirectional; it radiates equal power in all azimuthal directions perpendicular to the axis of the antenna. For a half-wave dipole the radiation is maximum, 2.15 dBi perpendicular to the antenna axis, falling monotonically with elevation angle to zero on the axis, off the ends of the antenna.[7]

• Several different variations of the dipole are also used, such as thefolded dipole, short dipole, cage dipole, bow-tie, and batwing antenna. Dipoles may be used as standalone antennas themselves, but they are also employed as feed antennas (driven elements) in many more complex antenna types,[3][4] such as the Yagi antenna,parabolic antenna, reflective array, turnstile antenna, log periodic antenna, and phased array.

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• Several different variations of the dipole are also used, such as thefolded dipole, short dipole, cage dipole, bow-tie, and batwing antenna. Dipoles may be used as standalone antennas themselves, but they are also employed as feed antennas (driven elements) in many more complex antenna types,[3][4] such as the Yagi antenna,parabolic antenna, reflective array, turnstile antenna, log periodic antenna, and phased array.

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Impedance of dipoles of various lengths

• The feedpoint impedance of a dipole antenna is very sensitive to its electrical length. Therefore a dipole will generally only perform optimally over a rather narrow bandwidth, beyond which its impedance will become a poor match for the transmitter or receiver (and transmission line). The real (resistive) and imaginary (reactive) components of that impedance, as a function of electrical length, are shown in the accompanying graph.

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• Dipoles that are much smaller than the wavelength of the signal are called short dipoles. These have a very lowradiation resistance (and a high capacitive reactance) making them inefficient antennas. More of a transmitter's current is dissipated as heat due to the finite resistance of the conductors which is greater than the radiation resistance. However they can nevertheless be practical receiving antennas for longer wavelengths. [8]

• Dipoles whose length is approximately half the wavelength of the signal are called half-wave dipoles and are widely used as such or as the basis for derivative antenna designs. These have a radiation resistance which is much greater, closer to the characteristic impedances of available transmission lines, and normally much larger than the resistance of the conductors, so that their efficiency approaches 100%. In general radio engineering, the term dipole, if not further qualified, is taken to mean a center-fed half-wave dipole.

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Radiation pattern and gain• A bare dipole is not considered a directional antenna. However like all

antennas, its radiation is not uniform in all directions. Its radiation pattern in three dimensions is shaped like a toroid (doughnut) symmetric about the axis of the dipole. The radiation is maximum at right angles to the dipole, dropping off to zero on the antenna's axis. Therefore a dipole mounted vertically will be omnidirectional in the horizontal plane, with a modest gain, at the expense of radiation in the vertical direction.

• Dipoles mounted horizontally (as is more common) will have gain in two opposing horizontal directions but nodes (directions of zero gain) at 90° from those directions (along the direction of the conductor). Neglecting electrical inefficiency, the antenna gain is equal to the directive gain, which is 1.5 or 1.76 dBi for a short dipole, increasing to 1.64 or 2.15 dBi for a half-wave dipole. For a 5/4 wave dipole the gain further increases to about 5.2 dBi, making this length desirable for that reason even though the antenna is then off-resonance.

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Feeding a dipole antenna• Ideally, a half-wave dipole should be fed using a balanced transmission

line matching its typical 65 - 70Ω input impedance. Twin lead with a similar impedance is available but seldom used.

• Many types of coaxial cable have a characteristic impedance of 75Ω, which would therefore be a good match for a half-wave dipole

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Short dipole

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51

Antenna Fundamentals

Dipole Antennas (Hertz): simple, old, widely used- root of many advance antennas

• consists of 2 spread conductors of 2 wire transmission lines• each conductor is ¼ in length• total span = ½ + small center gap

Distinct voltage & current patternsdriven by transmission line at midpoint

• i = 0 at end, maximum at midpoint

• v = 0 at midpoint, vmax at ends

• purely resistive impedance = 73• easily matched to many transmission lines

gap

¼ ¼ ½

Transmission Line

+v

-v

i

High Impedance 2k-3k

Low Impedance 73

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HALF WAVE DIPOLE ANTENNA

• The half-wave dipole antenna is just a special case of the dipole antenna.

• Half-wave term means that the length of this dipole antenna is equal to a half-wavelength at the frequency of operation.

• The dipole antenna, is the basis for most antenna designs, is a balanced component, with equal but opposite voltages and currents applied at its two terminals through a balanced transmission line.

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• To make it crystal clear, if the antenna is to radiate at 600 MHz, what size should the half-wavelength dipole be?

• One wavelength at 600 MHz is = c / f = 0.5 meters. Hence, the half-wavelength dipole antenna's length is 0.25 meters.

• The half-wave dipole antenna is as you may expect, a simple half-wavelength wire fed at the center as shown in Figure

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• Dipoles have an radiation pattern, doughnut symmetrical about the axis of the dipole. The radiation is maximum at right angles to the dipole, dropping off to zero on the antenna's axis.

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FOLDED DIPOLE

• Folded antenna is a single antenna but it consists of two elements.

• First element is fed directly while second one is coupled inductively at its end.

• Radiation pattern of folded dipole is same as that of dipole antenna i.e figure of eight (8).

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Advantages

• Input impedance of folded dipole is four times higher than that of straight dipole.

• Typically the input impedance of half wavelength folded dipole antenna is 288 ohm.

• Bandwidth of folded dipole is higher than that of straight dipole.

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HERTZ ANTENNA

• The Hertzian dipole is a theoretical short dipole (significantly smaller than the wavelength) with a uniform current along its length.

• A true Hertzian dipole cannot physically exist, since the assumed current distribution implies an infinite charge density at its ends, and significant radiation requires a very high current over its very short length.

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59

Folded Dipole Antenna

- basic ½ dipole folded to form complete circuit

- core to many advanced antennas

- mechanically more rugged than dipole

- 10% more bandwidth than dipole

- input impedance 292

- close match to std 300 twin lead wire transmission line

- use of different diameter upper & lower arms allows variable impedance

/2

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LOOP ANTENNA

• A loop antenna is a radio antenna consisting of a loop of wire with its ends connected to a balanced transmission line

• It is a single turn coil carrying RF current through it.• The dimensions of coil are smaller than the

wavelength hence current flowing through the coil has same phase.

• Small loops have a poor efficiency and are mainly used as receiving antennas at low frequencies. Except for car radios, almost every AM broadcast receiver sold has such an antenna built inside of it or directly attached to it.

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• A technically small loop, also known as a magnetic loop, should have a circumference of one tenth of a wavelength or less. This is necessary to ensure a constant current distribution round the loop.

• As the frequency or the size are increased, a standing wave starts to develop in the current, and the antenna starts to have some of the characteristics of a folded dipole antenna or a self-resonant loop.

• Self-resonant loop antennas are larger. They are typically used at higher frequencies, especially VHF and UHF, where their size is manageable. They can be viewed as a form of folded dipole and have somewhat similar characteristics. The radiation efficiency is also high and similar to that of a dipole.

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• Radiation pattern of loop antenna is a doughnut pattern.

• Can be circular or square loop

• No radiation is received normal to the plane of loop and null is obtained in this direction.

• Application: Used for direction finding applications

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TURNSTILE ANTENNA

• A turnstile antenna is a set of two dipole antennas aligned at right angles to each other and fed 90 degrees out-of-phase.

• The name reflects that the antenna looks like a turnstile when mounted horizontally.

• When mounted horizontally the antenna is nearly omnidirectional on the horizontal plane.

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• When mounted vertically the antenna is directional to a right angle to its plane and is circularly polarized.

• The turnstile antenna is often used for communication satellites because, being circularly polarized, the polarization of the signal doesn't rotate when the satellite rotates.

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RHOMBIC ANTENNA

• Structure and construction

– 4 wires are connected in rhombic shape and terminated by a resistor.

–Mounted horizontally and placed > ^/2 from ground.

• Highest development of long wire antenna is rhombic antenna.

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• Advantages

– Easier to construct

– Its i/p impedance and radiation pattern are relatively constant over range of frequencies.

–Maximum efficiency

– High gain can be obtained.

• Disadvantages

– Large site area and large side lobes.

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• Application

– Long distance communication, high frequency transmission and reception.

– Point to point communication.

– Radio communication.

– Short wave radio broadcasting.

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ANTENNA ARRAYS

• Antenna arrays is group of antennas or antenna elements arranged to provide desired directional characteristics.

• Generally any combination of elements can form an array.

• However equal elements of regualar geometry are usually used.

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YAGI-UDA ANTENNA

• It is a directional antenna consisting of a driven element (typically a dipole or folded dipole) and additional parasitic elements (usually a so-called reflector and one or more directors).

• All the elements are arranged collinearly and close together.

• The reflector element is slightly longer (typically 5% longer) than the driven dipole, whereas the so-called directors are a little bit shorter.

• The design achieves a very substantial increase in the antenna's directionality and gain compared to a simple dipole.

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• Typical spacing between elements vary from about 1/10 to 1/4 of a wavelength, depending on the specific design.

• The elements are usually parallel in one plane.• Radiation pattern is modified figure of eight• By adjusting distance between adjacent directors it

is possible to reduce back lobe• Improved front to back ratio

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ANTENNA APPLICATIONS

They are used in systems such as

• Radio broadcasting

• Broadcast television

• Two-way radio

• Communication receivers

• Radar

• Cell phones

• Satellite communications.

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ANTENNA CONSIDERATIONS

• The space available for an antenna

• The proximity to neighbors

• The operating frequencies

• The output power

• Money

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78

552.14 dB                               Dipole

                         

3600 dB                               Isotropic                          

Beamwidth -3 dB

Gain (over isotropic)

ShapeName Radiation Pattern

                              

20

30

50

200

25

14.7 dB

10.1 dB

-0.86 dB

3.14 dB

7.14 dB

                              

                              

                              

                              

                              

                              

Parabolic Dipole

Helical

Turnstile

Full Wave Loop

Yagi

                         

                         

                         

                         

                         

Biconical Horn

1515 dBHorn                          

                         360x20014 dB

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Yagi - Uda• Driven element induces currents in

parasitic elements• When a parasitic element is slightly

longer than /2, the element acts inductively and thus as a reflector -- current phased to reinforce radiation in the maximum direction and cancel in the opposite direction

• The director element is slightly shorter than/2, the element acts inductively and thus as a director -- current phased to reinforce radiation in the maximum direction and cancel in the opposite direction

• The elements are separated by ≈ 0.25

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3 Element

Yagi Antenna Pattern

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2.4 GHz Yagi with 15dBi Gain• G ≈ 1.66 * N (not dB)• N = number of

elements• G ≈ 1.66 *3 = 5

= 7 dB• G ≈ 1.66 * 16 =

27 = 16 dB

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• A log periodic is an extension of the Yagi idea to a broad-band, perhaps 4 x in wavelength, antenna with a gain of ≈ 8 dB

• Log periodics are typically used in the HF to UHF bands

Log-Periodic Antennas

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Parabolic Reflectors• A parabolic reflector

operates much the same way a reflecting telescope does

• Reflections of rays from the feed point all contribute in phase to a plane wave leaving the antenna along the antenna bore sight (axis)

• Typically used at UHF and higher frequencies

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Array Antennas

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Patch Antenna Array for Space Craft

• The antenna is composed of two planar arrays, one for L-band and one for C-band.

• Each array is composed of a uniform grid of dual-polarized microstrip antenna radiators, with each polarization port fed by a separate corporate feed network.

• The overall size of the SIR-C antenna is 12.0 x 3.7 meters

• Used for synthetic aperture radar

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THANKS

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