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    Miniaturised Multi-FrequencyPrinted Circuit Antenna

    By

    BINAY K. SARKAR.

    ISRO CHAIR PROFESSOR

    ( Lecture prepared for delivering at the Summer School on Recent Trend in Antenna

    Technology to be held at KIIT , Bhubaneswar on Aug.05,2008 )

    Department of Electrical and Electronic Communication Engineering

    Indian Institute of Technology, KharagpurKharagpur-721302

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    Printed Circuit Antenna: A review In telecommunication, there are several types of microstrip

    antennas, the most common of which is the microstrip patchantennaor patch antenna. Common microstrip antenna shapes are square,

    rectangular, circular and elliptical, but any continuous shape is

    possible.

    Microstrip antennas are also inexpensive to manufacture and design

    because of easy physical geometry.

    The dielectric loading of a microstrip antenna affects both its

    radiation pattern and impedance bandwidth.

    As the dielectric constant of the substrate increases, the antenna

    bandwidth decreases which increases the Q factorof the antenna and

    therefore decreases the impedance bandwidth.

    The basic half-wavelength (/2) center-fed dipole and quarter-

    wavelength (/4) monopole with ground plane are still widely used.

    The most popular types of antenna are the loop, patch, inverted-F, and

    meander line.

    http://en.wikipedia.org/wiki/Telecommunicationhttp://en.wikipedia.org/wiki/Patch_antennahttp://en.wikipedia.org/wiki/Q_factorhttp://en.wikipedia.org/wiki/Q_factorhttp://en.wikipedia.org/wiki/Q_factorhttp://en.wikipedia.org/wiki/Q_factorhttp://en.wikipedia.org/wiki/Patch_antennahttp://en.wikipedia.org/wiki/Patch_antennahttp://en.wikipedia.org/wiki/Patch_antennahttp://en.wikipedia.org/wiki/Telecommunication
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    Miniaturisation Techniques

    The Aim for miniaturisation is that for a given configuration, the

    design of the antenna should be to use the maximum volume available. This

    maximum volume will theoretically give the upper bound for both gain and

    bandwidth.

    Where a is the radius of the sphere enclosing the antenna

    2

    max

    2

    max 2

    2 22 ;

    11

    1 3

    a aG

    a aB

    a

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    The art of antenna miniaturization is to find the best trade offbetween bandwidth and gain for the antenna volume allotted for a given

    application.

    Miniaturizing an antenna will affect its radiation characteristics.

    Antenna miniaturization affects gain, bandwidth, and efficiency, but

    can, in many cases, also affect polarization purity.

    Indeed, there are efficient way to make antennas smaller is to bend their

    geometry, in order to force the current to meander, so that the antennas

    seem electrically larger than it really is.

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    A limitation in antenna miniaturization is the difficulty of correctly feeding

    small antennas. The correct feeding of a very small antenna is often neither

    balanced nor unbalanced, but somewhere in between.

    The microstrip antenna is a simple example that illustrates this effect: A

    microstrip patch (a typical case of an unbalanced antenna) can be made

    electrically small by using a substrate with a high permittivity.

    However, the overall size of the microstrip antenna will also depend on the

    size of its ground plane.

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    The different Miniaturizing techniques are:

    Loading the antenna with lumped elements,

    High-dielectric materials;

    Using ground planes and short circuits;

    Optimizing the geometry;

    Using the antenna environment (such as the Casing) to reinforce the

    radiation.

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    Introduction

    The Objective of choosing ring was a size of the resonant ring is

    substantially smaller than that of the corresponding patch and

    depends on the width of the microstrip used.

    The mean circumference of ring equals the guide wavelength of the

    microstrip used. Input impedance of a ring operated in the TM11mode is considerably higher, whereas its impedance bandwidth is

    smaller, in comparison with the patch.

    As the strip width is increased, the characteristics of a ring approach

    that of the patch.

    In order to reduce the antenna size and provide a suitable input impedance match,

    two techniques are employed; the insertion of strips into the annular ring and

    placing a cross-slot into the ground plane.

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    The proposed design annular-ring patch antennas with a cross-slotted

    ground plane yield a much smaller size for a given frequency and areeasily matched to 50 ohms.

    The antenna can be designed for single band circular-polarization, dual-

    band circular polarization, triple band, or further modification for

    wideband operation, depending on parameter selection.

    Some significant advantages are evident for these structures, such as the

    centre-frequency exhibiting weak dependence on the position of the

    feedpoint as well as compact size.

    Nearly Good circularly polarized properties and obtained for these compact

    antennas. The multi-frequency versions can provide small frequency ratios.

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    Design of Circular patch antenna

    i. The most Popular configuration is the circular patch or disk

    ii. The mode supported by the circular patch antenna can be found by

    treating the patch, ground plane, and the material between the two as a

    circular cavity.

    iii. The modes that are supported primarily by a circular microstrip

    antenna whose substrate height is small (h

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    Design of Circular patch antennai. Resonant frequencyf11:

    The resonant frequencies of the cavity, and thus of the microstripantenna, where the substrate height h is very small, the fields are

    along z are constant. Therefore the resonant frequencies for the

    TMzmn0modes are as

    The dominant mode is the TMz110whose resonant frequency is

    (fr)110 = (1.8412/2a) = (1.8412v0/2ar)

    where vo

    is the speed of light

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    ii. Radius of Circular Disk: A first order approximation to the solution

    of below equation for ais to find ae

    To find ae

    & substituting for ae

    1 2

    21 ln 1.7726

    2r

    Fa

    h F

    F h

    0

    110

    1.8412

    2r e r

    vf

    a

    1 2

    21 ln 1.77262

    e

    r

    h aa aa h

    98.791 10

    r r

    Ff

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    Design Equations for Annular ring

    i. Resonant Frequency :Approximate value of resonant frequency can be

    obtained by the following approaches used for the other patch

    antennas. To the zeroth-order approximation, the resonant frequency is

    obtained by setting

    Or

    nm

    a

    2

    nmnm

    r

    cfa

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    ii. Inner & Outer radius :Approximate value of resonant frequency can

    be obtained by the following approaches used for the other patch

    antennas. To the zeroth-order approximation, the resonant frequency is

    obtained by setting

    Where u = W/h

    The modified values of the inner & outer radius are as

    ae= a (We- W)/2

    be= b + (We- W)/2

    34 2

    4

    0.053

    521 11 ln ln 1

    49 0.432 18.7 18.1

    0.90.564

    0.3

    r

    r

    u u ua

    u

    b

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    Weis the effective width of the ring conductor

    Where 0= 120

    The modified radii equation is as

    ae = a 3h/4

    be = b + 3h/4

    0

    0

    ere

    hZW

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    iii. Radiation fields:The radiation fields of a circular ring antenna can be

    obtained either from the magnetic current approach or the electric

    current distribution on the surface of the ring. The equations are

    Where

    Where the ratio b/a increases, the directivity of the antenna increases

    and the side lobes level also increases. This is because for higher b/a

    ratio the two apertures are electrically far apart, giving rise to higher

    side lobe levels.

    0

    0

    0 0 0

    '2' sin ' sin cos

    '

    n jk rnmn

    n nnm nmn

    J k aE eE j k h J k a J k b n

    k r J k b

    0 0 000

    0 0

    sin ' sin2sin cossin ' sin

    jk rn nm nn

    n

    nm n nm

    k a J k a J k bE eE nj k h J nk r k a J k b k b

    nm nmk a

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    Design for Single Band application

    The geometry of a single band compact circularly polarized antenna is

    shown below. A circular patch is centered in the narrow annular-ring, of

    outer radius Ro and inner radius Ri. These patches are printed on FR4

    substrate, of r = 4.3, a thickness of 1.58mm, and a loss tangent of 0.022.. The

    crossed slot in the ground plane has unequal lateral lengths, Lh and Lv, with

    a slot width w. This structure excites two degenerate orthogonal modes with

    equal amplitude and 90 degree phase difference by tuning various

    parameters (Ri, Rp, Lh, and Lv) right-hand circular polarization (RHCP)

    radiation is obtained.

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    Calculated Parameters for SB

    Parameter Value

    (Ground plane ) a 60

    (Ground plane ) b 60

    (Slot horizontal) c 48

    (Slot width) d 2

    (Slot vertical) e 50

    f 48

    (feed point) fx 1.54

    (feed point) fy 5

    g 2

    h 50

    ri_gdisk 0

    ri_icable 0

    ri_ocable 1.83

    ri_pdisk 0

    ri_ring1 22

    ri_subcable 0

    ro_g1disk 4

    ro_gdisk 4

    ro_icable 0.325

    ro_ocable 2.08

    ro_pdisk 9

    ro_ring1 24.5

    ro_subcable 1.83

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    Simulated Structures

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    Fabricated Structures

    Lh

    Lv

    RpRi

    Ro

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    Simulation Time Signals

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    S11for the Single band antenna

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    Measurement Results

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    Radiation pattern (E-field)

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    Directivity

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    Axial Ratio

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    VSWR

    f l d l

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    Design for Dual Band application

    Dual band operation is achieved by employing an extra annular-ring, in addition

    to the first one which surrounds the small circular patch as shown in below Figure. The

    circularly-polarized frequency ratio of the two resonant modes is tunable to a small

    value, suitable for wireless communications systems. The resonant frequency of the

    lower mode is mainly determined by the larger outer ring radius while the resonant

    frequency of the higher mode is dependent on both the inner ring radius and the

    separation between the inner annular-ring and the inner circular patch.

    By adjusting the lengths of the cross-slot arms, the upper and lower resonances

    can be split into two orthogonal modes with nearly equal amplitude and 90 degree

    phase difference.

    Hence, a dual-frequency circularly-polarized antenna is achieved.

    lateral slot length Lh>Lv, then right-hand circular polarization

    lateral slot length Lh

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    Simulated Structures

    Top containingpatch & 2 Ring

    Bottom containingcross Slot

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    Calculated Parameters for DBParameter Value

    (Ground plane ) a 60

    (Ground plane ) b 60

    (Slot horizontal) c 40

    (Slot width) d 2

    (Slot vertical) e 42.4

    (feed) fx 4

    (feed) fy 5

    ri_ocable 1.83

    ri_ring1 14

    ri_ring2 19.7

    ro_gdisk 4

    ro_icable 0.325

    ro_ocable 2.08

    ro_osubcable 1.83

    ro_patch 6.5

    ro_ring1 18.9

    ro_ring2 24

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    S11for the Dual band antenna

    M t R lt

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    Measurement Results

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    Radiation pattern (E-field)

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    Gain (fr=1.1 GHz)

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    Design for Triple Band application

    To provide triple band operation, the addition of rings on the inner

    circular patch is used. This is shown in below Figure. The crossed slot in the

    ground plane remains, in order for miniaturisation. The additional ring can

    also broaden the lower band by adding them to the outer ring.

    This structure excites three resonant frequencies by using the outer

    annular-ring, inner annular-rings, and the circular patch, which decreases

    the Q-factor and increases surface current path lengths, hence a compact

    triple-frequency antenna is realised. A very small frequency ratio of the

    order of 1.25 is realizable.

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    Simulated Structures

    Top containingpatch & 3 Ring

    Bottom containingcross Slot specifiedfeed loaction

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    Calculated Parameters for TB

    Parameter Value(Ground plane) a 60

    (Ground plane) b 60

    (Slot horizontal) c 40

    (Slot width) d 2(Slot vertical) e 42

    (feed) fx -3

    (feed) fy -3

    ri_icable 0

    ri_ocable 1.83

    ri_patch 0

    ri_ring1 14

    ri_ring2 19.7ri_ring33 7.3

    ri_subcable 0

    ro_gdisk 4

    ro_icable 0.325

    ro_ocable 2.08

    ro_patch 6.5

    ro_ring1 18.9

    ro_ring2 24

    ro_ring33 12.51

    ro_subcable 1.83

    w 1.58

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    Fabricated Structures

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    S11for the Triple band antenna

    f1= 1.082GHz (-19.57), f2= 1.8259GHz (-22.27),f3= 4.9642GHz (-19.43)

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    VSWR(f1)

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    VSWR(f2)

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    VSWR(f3)

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    Radiation pattern (E-field)

    Di ti it

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    Directivity

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    Directivity

    l

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    Detail specifications for the Design ofMulti-frequency antenna

    Sr.No.

    Antenna Types Single Band Dual Band Triple Band

    Ground Plane 60mm x 60mm 60mm x 60mm 50mm x 50mm

    Frequency working 1.8 GHz 1.1GHz, 1.8 GHz 1.1GHz, 1.8 GHz, 5.0 GHz

    Frequency ratios achieved Approx order of 1.6

    Size Reduction achieved Approx. 50 %

    1. Radius circular Patch 9.0 mm 6.5 mm 6.9 mm

    2. Inner Radius Ring 1 22 mm 19.7 mm 14 mm

    3. Outer Radius Ring 1 24.8 mm 24 mm 18.9 mm

    4. Inner Radius Ring 2 --- 16.5 mm 19.7 mm

    5. Outer Radius Ring 2 --- 14 mm 24 mm

    6. Inner Radius Ring 3 --- --- 7.3 mm

    7. Outer Radius Ring 3 --- --- 12.5 mm

    M t R lt f P d

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    Measurement Results for Proposedantenna

    Antenna f1, BW (MHz, %) f2, BW (MHz, %) f3, BW (MHz, %) f2/f1

    ARL_ring1 1.8

    203, 11.27

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

    ARL_ring2 1.1036

    45, 4.07

    1.8698

    139, 7.46

    ------- 1.69

    ARl_ring3 1.125

    180, 16

    1.8

    180, 10

    ** 1.6

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    THANK YOU