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Transcript of circularly polarized antenna
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8/10/2019 circularly polarized antenna
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case with 0
=
65 . However. other CP characteristics are similar to
those observed for 0 =
65 .
Centre
frequency
M M
Table
1: Com parison between proposed disk-sec tor microstrip
antennas (antenna 1 with
8
=
65
and antenna
2
with
0
= 70 ) an d reference antenn a (circularly-polarised
equilateral-triangular microstrip antenna with slit [4])
Maximum
dimensions area
h e a r P atc h C P Maximum
bandwidth received
powel-
of patch
inm nm'
MFIr
dBin
Antenna 1
Antenna 2
141
1944 48.4 1149 25 (1.3% ) -50.4
1889
51.6
1237 23 (1.2%) -50.0
1931
48.2
998
19
(1.0%) -50.3
Conclusions: A single-feed circularly-polarised disk-sector micros-
trip antenna has been experimentally investigated. The present
CP
design requires no perturbation elements to be introduced in the
patch, and the excitation of two near-degenerate orthogonal
modes for CP radiation is mainly controlled by the flare angle of
the patch, which is experimentally found to be 65 and
70 .
EE
1998
Eleclronics
Lerrcrs
Online
No
19981587
Wen-Hsiu Hsu and Kin-Lu Wong (Deparznwir
of E/wtr.ir.o/
Enginwring,
Nurional Sun
Yat-Sen University, Kcrohsiung,
Tciiiwm
Republic of China)
16 Septeniher
199%
References
1 J A ME S .
J R ,
and H A L L ,
P.s
(Eds.): 'Handbook of microstrip
antennas' (Peter Peregrinus, London. 1989)
2
WO N G . K . L . , and
L I N . Y
F.: 'Circularly polarised microstrip antenna
with tuning stub', Electron.
Letr. 1998.
34 pp.
831-832
3
W O N G , K L., HSU. w.H and wu. C.K : 'Single-ked circularly polarized
microstrip antenna with
a
slit ',
Mzcvoiv.
Opt.
Technol. Lett. 1998.
18 pp.
306-308
LU. J H , T A N G ,
c
L.. and W O N G ,
K . L
: 'Circular polarisation design of
single-feed eq uilatera l-triang ular microstrip ante nna', Election.
Let t . ,
1998,
34 pp.
319-321
4
Circularly polarised microstrip antenna array
using proximity coupled feed
W . K .
Lo, C.H. Chan
and K . M .
Luk
A
2 x 2 circularly polarised CP) microstrip antenna array using a
proximity coupled feed and sequential rotation is described. As
compared with a previously presen ted single-element circularly
polarised microstrip antenna with a cross-slot, the new array
achieves a much wider
impedance
bandwidth of
11.18' 1
and has
an axial ratio bandwidth of 4. I h. he rcturn
loss,
radiation
patterns anti axial ratio of the a n t c nna array were measured
and
are
prcsented.
Introduction:
Microstrip antennas have been investigated exten-
sively
because
of their advantages such as small size, low profile
and
low
cost. Circularly
polarised CP)
antennas
arc
particularly
useful for a number of radar an d mobile satellite comm unication
systems. It has been demonstrated tha t C P antennas can be real-
ised by cutting
a
cross-slot into a circular patch [l ,
21.
Further-
more, the size of the patch is reduced when compared with that
without the
ci-oss-slot.
In this CP microstrip antenna, flexible
impedance matching is provided by a proximity-coupled feed
[3] .
For the conventional single-element CP antenna, the impedance
bandwidth and the axial ratio ban dwidth are relatively narrow.
The use of sequential rotation
[4,
51 can alleviate these difficulties.
In this study, a 2 x 2 circularly polarised microstrip phased array
antenna was designed and m easured experimentally. Each array
element is a circular microstrip antenna with a cross-slot with a
proximity-coupled feed. With the cross-slot, each element size
is
reduced and therefore the array can be designed with smaller ele-
ment spacing. When comparing the experimental results for the
single element CP antenna with those for the array, it is
found
that the
ne\$
2 x 2 array configuration offers a wider impedance
bandwidth than the single element C P antenna. Similarly, the CP
array also improves the axial ratio bandwidth and the boresight
axial I-atio. Experimental results of retu rn
loss,
radiation pattern
and polarisation aspect ratio are also presented
in
this Letter.
line width
WL t
slot Width w
length
Lb
circular patch with cross
slot
microstrip
ground plane
a
element spacing
D=0 59h0 ~ ~
Fig.
1 Antennci
t o i ~ f i ~ i i r c i t i o n s
U Single element
W
= 2111m,
L , =
20mm.
L ,
= IO W
= 4. 68mm = 23mm,
h
=
1.57min
h
Array
0
-1
m
20
:
3
P 30
-40
50
I I
I I I
1.5
1.6
1.7
1.8 1.9
frequency GHz
3
169412
Fig. 2
R r f u r n
loss against frequency
~._array
single element
An~znznaconfigurmtiun: The configurations of the single-element
antenna and the CP antenna array are shown in Fig. 1. The rela-
tive phases for the array at four feed points are
0,
90, 180 and
270 , respectively. Th e substrate used f or the an tenn a has a dielec-
tric constant E = 2.33 and the substrate thickness h = 1.57mm, the
width of the 50Q microstrip feed W is 4.68 . Th e rad ius of the
circular patch
R is
66 The length of the longer slot
Lo is
2190
ELECTRONICS LETTERS 12th
November
1998
Vol
34 No. 23
-
8/10/2019 circularly polarized antenna
2/2
20mn, the length of the shorter slot
L
is 10inm and the width
W
of the slots is
2
The patch-line overlap length of a single ele-
me nt is 23. Bas ed on the design of the single-elemmt CP
anten na, the design of the 2
x
2
CP
antenna ar ray is shown in Fig.
lh. T he designed frequency of the antenna array is 1.61GIIzand
the element spacing of the array is 0.59
A
and the patch-line
overlap length is the same as the single element.
0
12
10
8 -
m
E 6 -
._
-
4 -
2
270
large phased arrays
- I
R.J. Mailloux
A
technique
is
presented which combines the subarraying qualities
of constrained dual transform beamforming sections and p artial
overlapping netw orks to produce arrays of contiguous subarrays.
This approa ch is shown t o facilitate wideband scanning or limited
Geld
of
view coverage with a minimum number of controls and
low sidelobes.
-
Intvoduction: Elements of large arra:ys are often grouped into sub-
arrays
for
the purpose of decreasing the array feed complexity or
that scan over
a
limited field of view (LFOV) and also in wide-
band scanning systems. In an LFOV system that scans to kO,,,,,
reducing the number of controls. SiibarrdyS are useful
in
systems
the use of only a single phase shifter per subarray results in signif-
icant cost savings since the maxim um subarray spacing
s
of the
-
I
225 \__ 35
180
antennas are shown in F ig. 3. It reveals that the directivity
of
the
CP antenna array is better than that of the single element due to
the sharper radiation pattern.
Also,
from experimental results, it
is
found that the single elenlent and the antenna array generate
RHCP
(right hand circular polarisation) when the microstrip line
excites the circular patch as showri in Fig. 1. The array indeed
provides a much better
RHCP
than does the single element. Fig. 4
shows the measured axial ratio
of
ihe single element and that of
the array antenna where the 3dB axial ratio bandwidth of the
antenna array is 4.1%1which is much wider than the single element
of
O S6/0
The best axial ratio of the array is 0SdB a t 1 .62GHz
which is also much better than
the
single element of 2.8dB
at
the
same frequency.
Aclcnowledgnient: This project is supported by the Research Gran t
Council of H ong K ong (Project number: 9040199 and 9040210).
EE
1998
Electronics Letters
Otzlincj No
19981573
W.K. Lo C.H.
Chan and
K.M. 1,uk
(Wireless
Communications
Luboratory, Department O Electronic Engineering, City
niversity
o j
Honfi Kong, 53 Tat Clzee Avenue, Kowloon, Hong Kong SA R, Peoples
Repuldic o f China)
16
Septeniber
1998