Folded Dipole AntennaYagi-Uda antenna is the most commonly used type of antenna for TV reception...

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A folded dipole is an antenna, with two conductors connected on both sides, and folded to form a cylindrical closed shape, to which feed is given at the center. The length of the dipole is half of the wavelength. Hence, it is called as half wave folded dipole antenna. The directivity of Folded dipole Antenna is bi-directional. The input impedance is higher. Folded Dipole Antenna Frequency range The range of frequency in which half wave folded dipole operates is around 3KHz to 300GHz. This is mostly used in television receivers.

Transcript of Folded Dipole AntennaYagi-Uda antenna is the most commonly used type of antenna for TV reception...

  • A folded dipole is an antenna, with two conductors connected on both sides,

    and folded to form a cylindrical closed shape, to which feed is given at the

    center. The length of the dipole is half of the wavelength. Hence, it is called

    as half wave folded dipole antenna. The directivity of Folded dipole

    Antenna is bi-directional. The input impedance is higher.

    Folded Dipole Antenna

    Frequency range

    The range of frequency in which half wave folded dipole operates is around

    3KHz to 300GHz. This is mostly used in television receivers.

  • If the Radii of the 2 conductors are equal, then equal currents in both the

    conductors, in the same direction, i.e currents are equal in magnitude and

    phase in the 2 dipoles.

    The total power developed in folded dipole is equal to that developed in the

    conventional dipoles, therefore the input or terminal impedance of folded

    dipole is greater than that of the conventional dipole. It can be proved that

    the input impedance at the terminals of a folded dipole antenna is equal to

    the square of number of conductors comprising the antenna times the

    impedance at the terminals of a conventional dipole.

  • V/2= I1Z11+I2Z12

    V/2= I1(Z11+Z12)

    Z11=Z12

    V/2= I1(2Z11)

    Z=V/I1=2x2Z11=22Z11=4x73=292 Ω [Z11= 73 Ω for dipole antenna]

    V/3.= I1Z11+I2Z12+ I2Z13

    V/3= I1(Z11+Z12+ Z13)

    V/3= I1(3Z11)

    Z=V/I1=3x3Z11=32 Z11=9x73=657 Ω

    If I1=I2

  • ratioZZra

    raZZ *

    2/log

    1/log1 11

    2

    11

    V/n= I1(nZ11)

    Z=V/I1=nxnZ11=n2 Z11=n

    2 x73 Ω

    Where r2=r1=radii of elements

    If r2=2r1 then

    2

    1

    1

    2

    1

    211

    21731

    r

    r

    r

    rZZ =73x9=657 Ω

  • Advantages The following are the advantages of half-wave folded dipole antenna −

    Reception of balanced signals.

    Receives a particular signal from a band of frequencies without losing

    the quality.

    A folded dipole maximizes the signal strength.

    High input impedance

    Wide band in frequency

    Acts as built in reactance components network

    Disadvantages The following are the disadvantages of half-wave folded dipole antenna −

    Displacement and adjustment of antenna is a hassle.

    Outdoor management can be difficult when antenna size increases.

    Applications The following are the applications of half-wave folded dipole antenna −

    Mainly used as a feeder element in Yagi antenna, Parabolic antenna,

    turnstile antenna, log periodic antenna, phased and reflector arrays, etc.

    Generally used in radio receivers.

    Most commonly used in TV receiver antennas.

  • Yagi-Uda antenna is the most commonly used type of antenna for TV reception over the last

    few decades. It is the most popular and easy-to-use type of antenna with better performance,

    which is famous for its high gain and directivity

    Frequency range

    The frequency range in which the Yagi-Uda antennas operate is around 30 MHz to 3GHz

    which belong to the VHF and UHF bands.

    Yagi-Uda Antenna

  • ELEMENT SPECIFICATION

    Length of the Driven Element 0.458λ to 0.5λ

    Length of the Reflector 0.55λ to 0.58λ

    Length of the Director 1 0.45λ

    Length of the Director 2 0.40λ

    Length of the Director 3 0.35λ

    Spacing between Directors 0.2λ

    Reflector to dipole spacing 0.35λ

    Dipole to Director spacing 0.125λ

    They are − If the specifications given above are followed, one can design an Yagi-Uda antenna.

  • General Characteristics of Yagi-Uda Antenna

    If 3 elements array (i.e. one reflector, one director and Driven element) is used, then

    such type of antenna is generally referred to as beam antenna.

    It has unidirectional beam of moderate directivity with light weight, low cost and

    simplicity in feed system design.

    With spacing of 0.1 λ to 0.15 λ a frequency band width of the order of 2% is obtained

    It provides gain of the order of 8 db or front to back ratio of about 20 db

    It is also known as super directive or super gain antenna due to its high gain and beam

    width per unit area of the array. An antenna or array which provides directive gain,

    appreciable greater than that obtainable from uniform distribution is known super

    directive or super gain antenna.

    If greater directivity is desired, further elements may be used. For example, five or six

    elements are used with case and arrays up to 40 can be constructed.

    It is essentially a fixed frequency device i.e frequency sensitive and a band width of

    about 3% is obtainable. This much band width is sufficient for television reception.

  • Voltage and Current Relations in Parasitic Antenna

    V1=I1Z11+I2Z12+I3Z13+-----------------+InZ1n

    V2=I1Z21+I2Z22+I3Z23+-----------------+InZ2n

    V3=I1Z31+I2Z32+I3Z33+-----------------+InZ3n

    --------------------------------------------------

    Vn=I1Zn1+I2Zn2+I3Zn3+-----------------+InZnn

    V1, V2, V3------- Vn = Voltage applied to antenna no. 1,2,3 ----- n

    I1, I2, I3----------- In = Current flowing in antenna no. 1,2,3 ----- n

    Z11, Z22, Z33----- Znn= Self impedance of antenna no. 1,2,3, ----n

    Z12, Z21, Z13----- Z31= Mutual impedance of antenna no. 1,2,3, ----n

    I1 I2 I1 I2 I3

  • V1=I1Z11+I2Z12;

    V2=I1Z21+I2Z22; [ As Z12= Z21, Z13= Z31, and V2=0 being parasitic ]

    As V1=I1Z11+I2Z12;

    So 0=I1Z12+I2Z22

    So I1Z12 = - I2Z22

    22

    1212

    Z

    ZII

    22

    121

    Z

    ZIV1=I1Z11 Z12

    22

    2

    121111

    Z

    ZZIV

    22

    2

    1211

    11

    Z

    ZZ

    VI

    12

    221112

    12

    Z

    ZZZ

    VI

    22

    2

    1211

    1

    11

    Z

    ZZ

    I

    VZ

    12

    221112

    2

    22

    Z

    ZZZ

    I

    VZ

    Voltage and Current Relations in Parasitic Antenna

  • Advantages The following are the advantages of Yagi-Uda antennas

    High gain is achieved.

    High directivity is achieved.

    Ease of handling and maintenance.

    Less amount of power is wasted.

    Broader coverage of frequencies.

    Disadvantages The following are the disadvantages of Yagi-Uda antennas

    Prone to noise.

    Prone to atmospheric effects.

    Applications The following are the applications of Yagi-Uda antennas

    Mostly used for TV reception.

    Used where a single-frequency application is needed.

    Advantages, Disadvantages and Applications of Yagi-Uda Antenna