miniaturized antenna 2008
TRANSCRIPT
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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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