U.S. patent number 3,805,269 [Application Number 05/261,973] was granted by the patent office on 1974-04-16 for diverse type dipole antennas on common mount.
This patent grant is currently assigned to Matsushita Electric Industrial Co., Ltd.. Invention is credited to Kyohei Fujimoto, Hiroshi Haruki, Yoshiyasu Hiroi, Hideo Ito, Tsutomu Kobayashi, Takao Ogawa, Nobuyuki Suyama.
United States Patent |
3,805,269 |
Fujimoto , et al. |
April 16, 1974 |
DIVERSE TYPE DIPOLE ANTENNAS ON COMMON MOUNT
Abstract
An antenna means comprising a linear element of a conductor
having a length sufficiently shorter than a half wavelength and a
plurality of parallel two-wire type distributed constants
transmission lines short-circuited at the free end thereof, said
transmission lines being sequentially arranged along the linear
conductor element and connected to the same element, whereby
compensation of the impedance characteristics of the antenna is
achieved without decreasing the antenna efficiency.
Inventors: |
Fujimoto; Kyohei (Fujisawa,
JA), Suyama; Nobuyuki (Chigasaki, JA),
Hiroi; Yoshiyasu (Yokohama, JA), Ito; Hideo
(Yokohama, JA), Haruki; Hiroshi (Yokohama,
JA), Ogawa; Takao (Yokohama, JA),
Kobayashi; Tsutomu (Kadoma, JA) |
Assignee: |
Matsushita Electric Industrial Co.,
Ltd. (Osaka, JA)
|
Family
ID: |
27293970 |
Appl.
No.: |
05/261,973 |
Filed: |
June 12, 1972 |
Foreign Application Priority Data
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Jun 14, 1971 [JA] |
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46-50485 |
Jun 14, 1971 [JA] |
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46-50484 |
Jun 14, 1971 [JA] |
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46-50487 |
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Current U.S.
Class: |
343/794;
343/802 |
Current CPC
Class: |
H01Q
9/065 (20130101); H01Q 11/16 (20130101); H01Q
9/04 (20130101) |
Current International
Class: |
H01Q
11/00 (20060101); H01Q 11/16 (20060101); H01Q
9/06 (20060101); H01Q 9/04 (20060101); H01q
009/16 () |
Field of
Search: |
;343/802,806,828,794 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lieberman; Eli
Attorney, Agent or Firm: Stevens, Davis, Miller &
Mosher
Claims
1. An antenna means comprising two sets of linear conductors
aligned in a plain dipole antenna fashion and having the total
length substantially shorter than a half wavelength in the
operation frequency band, the linear conductors of each set of said
two sets of linear conductors being spaced at intervals
corresponding to a fraction of the operating wavelength,
a plurality of parallel two-wire type distributed constants
transmission lines having one end thereof short-circuited, said
transmission lines being connected between two adjacent conductors
of each set of said two sets of linear conductors at the other end
of said transmission lines, said plurality of parallel two-wire
type transmission lines being perpendicular to the axis of said two
sets of linear conductors and having a predetermined impedance
characteristic,
a bar of dielectric material, said bar having on the surface
thereof said two sets of linear conductors and said plurality of
parallel two-wire type distributed constants transmission lines,
and
a rod of conductor along the longitudinal axis of said dielectric
bar, said rod being designed to serve as another antenna which
operates at another frequency band, the feeding point for both
antennas being common, whereby said antenna means constitutes a
part of a composite antenna.
Description
This invention relates to an antenna means of comparatively small
size, particularly to such a means designed to have well
compensated impedance characteristics and yet to maintain good
antenna efficiency.
Generally, small linear antennas the length of which is
sufficiently shorter than a half wavelength, have an impedance
characteristics in which the resistive component is comparatively
small and the capacitive component iis comparatively large.
Therefore, the mismatch loss with a receiver is accordingly
large.
Hitherto, in order to compensate such an impedance characteristic,
an inductance of concentrated constants (or a coil) has been
attached to the antenna at the intermediate portion or at the
driving terminals thereof. Such a loading has caused a decrease in
the antenna efficiency due to a loss in the inductance (coil).
Further, the radiation impedance of the antenna is usually
small.
An object of this invention is to remove the above-mentioned
drawbacks of a small antenna by loading it with inductances of
distributed constants.
Another object of this invention is to provide a small antenna
which has a long life and can be easily handled.
A further object of this invention is to provide a small antenna
which can be easily formed as a composite antenna.
In order to achieve the above objects, the antenna of this
invention comprises an aligned series of linear conductors the
total length of which is substantially shorter than a half
wavelength in the operating frequency band and a plurality of
parallel two-wire type distributed constants transmission lines
short-circuited at one end thereof, said transmission lines being
connected between two adjacent conductors of said series of linear
conductors at the other end thereof.
This invention will be described in detail with reference to the
accompanying drawings, in which:
FIG. 1 is a diagram of a fundamental two-wire distributed constants
transmission line;
FIGS. 2, 3, 4 and 5 are schematic diagrams of the antenna of this
invention shown in various forms;
FIG. 6 is a chart showing comparison of the impedance relations
between the antennas of this invention and of the conventional
one;
FIGS. 7, 8 and 9 are schematic diagram of modified forms of the
antenna of this invention;
FIGS. 10a, 10b and 10c are views relating to a practical embodiment
of this invention; and
FIGS. 11 and 12 are views of another embodiment of this
invention.
Referring to FIG. 1 which shows a distributed constnnts transmision
line of parallel two-wire type short-circuited at the load end, the
impedance of the line at the sending end a,a' contains an inductive
component Z expressed by the following formula:
Z = jW.sub.0 tan .beta.l (1)
where
W.sub.o is the characteristic impedance of the line,
.beta. is the phase constant, and
l is the length of the line.
FIG. 2 schematically shows an embodiment of the antenna of this
invention, in which a plurality of short-circuited transmission
lines 2 as shown in FIG. 1 are successively loaded to an antenna
element 1.
with this formation, the inductive component of each transmission
line 2 is added in series to the impedance of the antenna element 1
which has a large capacitive component. Further, the radiation
current is superposed to the transmission lines 2.
FIGS. 3 and 4 are schematic diagrams of other embodiments of this
invention. The embodiment shown in FIG. 3 has a plurality of folded
transmission lines 3, while the one shown in FIG. 4 has curved
transmission lines 4.
Though dipole antennas are shown in the above embodiments, it will
be understood that this invention is also applicable with similar
effects to monopole antennas as shown in FIG. 5.
As described above, the antenna element is loaded with inductive
components of small loss and the antenna efficiency is not
deteriorated. Further, as the radiation current is superposed to
the loading transmission lines, the effective length of the antenna
is equivalently increased, the radiation resistance being thereby
multiplied eight to ten-fold. Thus, a small antenna with which the
loss due to the mismatching thereof with the receiver in the
resonant state is minimized, is realized.
Further, according to this invention, broad-band characteristics
equal to or even better than those of a normal mode helical antenna
of corresponding length are achieved.
The chart of FIG. 6 shows impedance characteristics (A) for an
antenna of this invention of 60 cm in length characteristics (B)
for a helical antenna of corresponding length.
Further, the antenna efficiency can be increased by changing the
length or the characteristic impedance of the loading transmission
lines according to the respective loading positions, or by changing
the spaces between adjacent transmission lines. Namely, as seen
from the hereinbefore shown formula (1), impedance Z can be changed
by varying the value of the characteristic impedance W.sub.o or the
length l of the line. In the embodiment shown in FIG. 7, the
lengths (l.sub.1 . . . . l.sub.5) of respective transmission lines
are changed while the spaces (w) are equal. The embodiment shown in
FIG. 8 is loaded with transmission lines of the same length (l) but
differently spaced (w.sub.1 . . . . w.sub.5). On the other hand,
FIG. 9 shows an embodiment in which the characteristic impedances
(W.sub.01 W.sub.03) of the loading transmission lines are varied
depending on the loading position along The antenna. In FIGS. 7 to
9, distance 2h represents the total length of the antenna.
It is important for the antenna of this invention to be provided in
such a form that simple construction, stable characteristics and
easy handling of the antenna are ensured. An example of such an
antenna is described hereunder.
Referring to FIGS. 10a, 10b and 10c, a supporting cylinder 11 is
made of a dielectric material and provided with a hole 15 which
serves as the outlet for feeders. A conductive material in the
pattern of antenna elements 13 loaded with short-circuited
transmission lines 14 are deposited, by known printed-circuit
technique, on an elastic sheet 12 of an insulating material. This
elastic sheet 12 with the conductive pattern of the antenna
deposited thereon is placed within the supporting cylinder 11 so
that the sheet 12 is pressed against the inner wall of the cylinder
11 by its own elasticity. Thus, the sheet 22 is assuredly held by
the cylinder 11 as shown in FIG. 10c. Though a cylindrical tube is
used in the above embodiment, it will be understood that similar
effects are achieved using a tube having a square section.
The antenna of this invention fabricated in such a form as
described above has the following advantages. Namely, antennas of
any complicated pattern can be easily fabricated in mass-production
scale with very accurate dimensions and good uniformness. Further,
as the antenna element is protected by the dielectric cylinder, it
is little affected by weather or salty wind and also hardly suffers
mechanical damage. Thus, a long operation life can be expected.
Moreover, the antenna assembly described is very simple in
construction, as the printed sheet is certainly within the
supporting cylinder with its own elasticity and no fixing means is
required. Thus, the prduction cost is accordingly low.
Another embodiment of this invention is shown in FIGS. 11 and 12.
In the illustrated arrangement, the antenna 20 according to this
invention constitutes a part of a composite antenna, the other part
being a rod antenna 24. The antenna 20 comprises support 21 which
may be, for example, a square bar of a dielectric material such as
polystyrole, an antenna element 23 which may be a series of
conductive strips, for example, of metal foil attached to the
support 21 along a longitudinal edge thereof, and compensating
elements 22 which are a plurality of parallel two lines of
conductor attached to the support 21, one end of the two lines
being connected with the antenna element and the other end being
short-circuited. The support 21 is provided with a hole along the
longitudinal axis thereof at the center portion of the square
section. This hole serves to support the rod antenna 24 which
operates at a frequency band different from that for the first
antenna 20. Further, as both antennas can be driven through a
common feeding point, a composite antenna of reduced size which may
appear to be a single antenna is obtained. Moreover, the second or
rod antenna 24 contributes to increase the mechanical strength of
the composite antenna.
* * * * *