Field of invention
[0001] The present invention relates to the technical field of wireless or mobile communication
technology via electromagnetic radiation. In particular the present invention relates
to the technical field of antenna arrangements, which are specifically designed for
having an omni-directional transmitting and/or receiving profile within a two dimensional
plane such as the horizontal plane. Further, the present invention relates to a method
for transmitting and/or for receiving electromagnetic radiation by means of an antenna
arrangement as mentioned above.
Art Background
[0002] In recent years mobile telecommunication became more and more important not only
for business but also for private applications. Currently, there have been implemented
a plurality of different services which may be provided for a subscriber of a telecommunication
network. Such services regularly require a stable wireless connection between a mobile
User Equipment and a typically stationary base station. A User Equipment may be for
instance a cellular telephone, a Personal Digital Assistant or a notebook computer.
[0003] One example for a small radio telecommunication network having a comparatively small
cell size is for instance a so called Wireless Local Area Network (WLAN). In order
to serve a cell of a WLAN, base stations are used, which are equipped or connected
to antennas having a simple whip-style monopole or dipole antenna element. In order
to achieve a higher gain with an omni-directional property at least within a two dimensional
plane it is known to use a vertical array of rod-style antenna elements, which consist
of stacked dipole elements extending with a significantly length respectively height
perpendicular to the two dimensional plane.
[0004] For receiving electromagnetic radiation within the frequency range between 10 MHz
and 2000 MHz Yagi Antennas are known. A Yagi antenna is a directional antenna system
consisting of an active driven dipole antenna element and additional closely coupled
parasitic antenna elements, which are usually a reflector and one or more directors.
Such an arrangement gives the antenna directionality that a single dipole lacks.
[0005] In particular for WLAN applications there may be a need for providing a simple, a
low-cost and preferably an on ceiling mountable antenna arrangement, which comprises
an omni-directional gain and sensitivity property in a predefined horizontal plane.
Further, some gain in an elevation view would also be advantageous.
Summary of the Invention
[0006] This need may be met by the subject matter according to the independent claims. Advantageous
embodiments of the present invention are described by the dependent claims.
[0007] According to a first aspect of the invention there is provided an antenna arrangement
and in particular an antenna arrangement based on the principles of Yagi antenna technology.
The provided antenna arrangement comprises (a) a base element having an upper surface,
(b) an active antenna element, which is attached to the base element and which extends
substantially perpendicular to the upper surface, and (c) a plurality of passive antenna
elements, which are attached to the base element and which extend substantially perpendicular
to the upper surface. The active antenna element is located in the center of the whole
antenna arrangement and the passive antenna elements are arranged in at least four
rows, whereby each row extends radially outwards from the center in a different direction.
[0008] The described antenna arrangement is based on the idea that a multi-row arrangement
of passive antenna elements surrounding an active antenna element may provide substantially
within a two dimensional plane an omni-directional property for antenna gain and/or
for antenna sensitivity. This means that when operating the described antenna arrangement
only little radiation is transmitted into respectively received from directions being
oriented significantly inclined with respect to a two dimensional plane, which plane
is oriented parallel to the upper surface.
[0009] The basic idea of the present invention is to use wire and/or strip directors respectively
passive antenna elements being located around a simple feeder respectively active
antenna element in order to increase the directivity of the antenna arrangement in
the two dimensional plane and maintaining the corresponding two dimensional gain as
omni-directional as possible. Of course for the maximum gain slight angular deviations
from the two dimensional plane in the range up to 25° to 30° are possible.
[0010] According to Yagi antenna technology the active antenna element is a feed antenna,
which may be connected in a known manner to a feed line of the antenna arrangement.
Further, the passive antenna elements may be denominated as directors, which are stimulated
by the radiation field of active antenna element. However, by contrast to many Yagi
antennas having a non omni-directional antenna characteristic the described antenna
arrangement comprises no reflector elements.
[0011] The active antenna element and the passive antenna elements as a whole represent
a system of coupled resonators. Thereby, in the transmitting case the passive antenna
elements are driven by the radiation field being emitted by the active antenna element.
The spatial distribution of all the (active and passive) antenna elements is designed
in such a way that the phase shifts between the electromagnetic radiation being emitted
from all the (active and passive) antenna elements is substantially constructive for
radiation being emitted within the two-dimensional plane. This means that the overall
radiation field being emitted from the whole antenna arrangements represents a constructive
interference between all radiation fields being emitted from each of the antenna elements.
Of course, this relies on the matter of fact that the spatial distance between the
various antenna elements is specifically adapted to the electromagnetic wavelength
the described antenna arrangement is optimized for.
[0012] It has to be mentioned that of course all the physical properties described above
in connection with the transmitting case also apply vice versa for the receiving case,
wherein electromagnetic radiation is received by the described antenna arrangement.
[0013] The described antenna arrangement may be realized within a vertically low profile.
Thus the antenna arrangement can be used in many locations which do not allow a spatially
large extension of an antenna. The antenna arrangement, which may allow for a power
gain of 3-6 dBi, can be realized by a simple and low-cost mechanical construction.
The antenna arrangement may be used as a Wireless Local Areas Network (WLAN) base
station in particular for or in small cells. The antenna arrangement may be suitable
for WLAN base station access antennas being adapted for a frequency band between 2.4
and 2.5 GHz.
[0014] Preferably the two dimensional plane of the described antenna arrangement is a horizontal
plane. Thereby, a reliable radio respectively wireless communication may be achieved
for subscribers, which are located predominately within a horizontal plane such as
the floor of one ore more rooms.
[0015] According to an embodiment of the invention the passive antenna elements represent
a symmetrical structure with respect to the active antenna element. This holds at
least within a two dimensional plane being parallel to the upper surface of the base
element
[0016] In particular, the structure of the passive antenna elements may be point symmetric
with respect to the central active antenna element. This means that for each of the
passive antenna elements there is also one another of the passive antenna elements
which represent a pair of antenna elements, wherein the active antenna elements is
located exactly in the middle of a fictive line connecting the two antenna elements
of the respective pair of antenna elements.
[0017] It has to be mentioned that the above described point symmetry is not essential for
realizing the invention. It may also be possible to construct any odd number (for
example 7) of radial rows of directors around the active antenna element.
[0018] The passive antenna elements respectively the directors of the symmetrical structure
may be arranged within a circular, radially periodic geometry. Thereby, horizontally
omni-directional high-gain antennas may be realized in a comparatively simple and
effective manner.
[0019] According to a further embodiment of the invention the base element is a plate. This
may provide the advantage that the whole antenna arrangement can be constructed within
a small vertical extension. Thereby it becomes possible that the antenna arrangement
can be mounted for exampled on ceilings without reducing the effective height of the
corresponding room significantly.
[0020] According to a further embodiment of the invention the base element comprises an
electrically non conductive material.
[0021] The non conductive material may be any dielectric material such as for instance plastic.
Thereby, the active antenna element and/or the passive antenna elements may be round
and thin metal rods which can be attached to the plastic plate.
[0022] According to a further embodiment of the invention the antenna arrangement further
comprises a conducting ground-plane, which is spatially separated from the passive
antenna elements and which laterally extends below all passive antenna elements.
[0023] The passive antenna elements respectively the directors can be realized for example
by means of strips on vertical substrate pieces. The active antenna element may be
for instance a monopole.
[0024] Such an antenna arrangement may provide the advantage that the beam direction can
be located very close to the horizon. Further, electronic components may be located
behind the conducting ground-plane representing an effective shielding against unwanted
electromagnetic radiation.
[0025] According to a further embodiment of the invention the base element comprises an
electrically conductive material.
[0026] The conductive material may be any metallic material such as for instance copper,
which comprises a high electrical conductivity and therefore contributes in reducing
the ohmic loss when operating the described antenna arrangement.
[0027] A metal base element and in particular a metal plate act as an electromagnetic mirror
for the electrical charge respectively for the electrical potential. This may provide
the advantage that the vertical size of the (active and passive) antenna elements
can be further reduced, because the active and passive antenna elements can be operated
quasi as an electromagnetic monopole having only half of the length of a corresponding
electromagnetic dipole. In this respect the vertical size is the dimension of the
antenna elements in a direction perpendicular to the upper surface of the metallic
base element.
[0028] The metallic base plate, which causes all the antenna elements to be operable as
quasi electromagnetic monopoles may further comprise the advantage that the active
antenna element can be supplied by means of a monopole feed. Such a monopole feed
may allow for a straight coaxial connection to the antenna arrangement. Further, a
monopole feed can eliminate the need for a so called balun transformer. In this respect
balun transformers are passive electronic devices that convert between balanced and
unbalanced electrical signals.
[0029] By employing a metal plate it is possible to design the impedance of the described
antenna arrangement to have a good match to an usual 50 Ohm impedance being used for
a feed cable and/or for a transmitting respectively a receiving device being connected
to the antenna arrangement.
[0030] A further advantage of using a metallic base element is an effective shielding of
electromagnetic radiation. Specifically, in the transmitting case the metallic base
element may effectively prevent electromagnetic radiation from undesirably entering
a spatial region being located behind the base element. Thereby, the electromagnetic
compatibility of the described antenna arrangement may further be increased.
[0031] The antenna elements, which may be realized as round thin metal rods or strips, can
be welded into a ground-plane of the upper surface representing a ground-plane of
the base element. Further, the antenna elements, which may be realized as metallic
strips, can be constructed on identical substrate plates, which are assembled radially
on the ground-plane. Thereby, the described antenna arrangement can be realized by
means of a modular assembly.
[0032] According to a further embodiment of the invention the base element extends along
the whole antenna arrangement. This means that all the antenna elements are located
directly in front of a metallic surface representing an electromagnetic mirror. This
kind of antenna arrangement may provide the advantage that it can be realized within
a very flat design. However, a comparatively large metallic ground surface is needed.
[0033] It has to be mentioned that when using a finite metal base plate representing a non
perfect infinite electromagnetic mirror, the maximum gain of the antenna arrangement
cannot be within the two dimensional plane being oriented parallel to the upper surface.
The maximum gain may be rather elevated between 15° and 25° above or below this plane.
If the antenna arrangement is oriented horizontally for instance on the ceiling of
a room, the maximum gain may be realized within a plane being elevated between 15°
and 25° under the horizon.
[0034] It has to be mentioned that for the described antenna arrangement comprising a large
metallic ground plane it may be difficult but however not impossible to optimize both
the impedance and the gain of the antenna arrangement simultaneously.
[0035] According to a further embodiment of the invention the base element extends solely
along a portion of the whole antenna arrangement. This means that only some of the
antenna elements are located directly in front of the metal plate respectively the
metallic surface representing an electromagnetic mirror. Preferably, the metal plate
extends solely below the active antenna element.
[0036] It has to be mentioned that this kind of antenna arrangement cannot be realized within
such a small vertical extension as the above described antenna arrangement having
a large ground plate. The height of the described antenna arrangement having a small
or a reduced ground plate will rather be of the order of one height of a dipole, which
of course also depends on the wavelength being transmitted and/or received by the
antenna arrangement. However, the described small ground plate antenna arrangement
may provide the advantage that it's input impedance, which strongly depends on the
spatial distribution of the antenna elements, can be easily optimized to be nearly
50 Ohm.
[0037] The described small ground plate antenna arrangement may further provide the advantage
that the maximum gain is on the horizon respectively within the two dimensional plane
being oriented parallel to the upper surface and the gain and the ripple in gain profile
can be controlled by a selection of the number of directors in the radial rows and
by the number of radial rows.
[0038] According to a further aspect of the invention there is provided a method for transmitting
and/or for receiving electromagnetic radiation by means of an antenna arrangement
as described above.
[0039] Also this further aspect of the invention is based on the idea that the above described
multi-row arrangement of passive antenna elements surrounding the active antenna element
may provide substantially within a two dimensional plane an omni-directional property
for the gain and the sensitivity of the antenna arrangement. This means that when
operating the described antenna arrangement only little radiation intensity is transmitted
into respectively received from directions being oriented significantly inclined with
respect to the two dimensional plane being parallel to the upper surface.
[0040] It has to be noted that embodiments of the invention have been described with reference
to different subject matters. In particular, some embodiments have been described
with reference to apparatus type claims whereas other embodiments have been described
with reference to method type claims. However, a person skilled in the art will gather
from the above and the following description that, unless other notified, in addition
to any combination of features belonging to one type of subject matter also any combination
between features relating to different subject matters, in particular between features
of the apparatus type claims and features of the method type claims is considered
as to be disclosed with this application.
[0041] The aspects defined above and further aspects of the present invention are apparent
from the examples of embodiment to be described hereinafter and are explained with
reference to the examples of embodiment. The invention will be described in more detail
hereinafter with reference to examples of embodiment but to which the invention is
not limited.
Brief Description of the Drawings
[0042]
Figure 1 shows the basic idea of a Circular Yagi antenna arrangement with one active
dipole-type antenna element and 16 radial rows of passive dipole-type directors in
accordance with an embodiment of the present invention.
Figure 2 shows a three dimensional directivity function of the antenna arrangement
illustrated in Figure 1.
Figure 3 shows the directivity function of the antenna arrangement illustrated in
Figure 1 in the horizontal plane.
Figure 4 shows the directivity function of the antenna arrangement illustrated in
Figure 1 in an elevation view.
Figure 5 shows a modification of the Circular Yagi antenna arrangement comprising
a metal base plate (Large Ground Plane Circular Yagi, LGPCY) resulting in a monopole-type
active antenna element feeding passive monopole-type directors.
Figure 6 shows a three dimensional directivity function of the antenna arrangement
illustrated Figure 5.
Figure 7 shows the directivity function of the antenna arrangement illustrated in
Figure 5 in the horizontal plane in several frequencies.
Figure 8 shows the directivity function of the antenna arrangement illustrated in
Figure 5 in an elevation view in several frequencies.
Figure 9 shows a modification of the Circular Yagi antenna arrangement comprising
a small metal base plate (Small Ground Plane Circular Yagi, SGPCY) resulting in a
monopole-type active antenna element feeding passive dipole-type directors, which
are arranged in 12 rows each comprising four directors.
Figure 10 shows a three dimensional directivity function of the antenna arrangement
illustrated in Figure 9.
Figure 11 shows the directivity function of the antenna arrangement illustrated in
Figure 9 in the horizontal plane in several frequencies.
Figure 12 shows the directivity function of the antenna arrangement illustrated in
Figure 9 in an elevation view in several frequencies.
Figure 13 shows a three dimensional directivity function of a SGPCY antenna arrangement
having 12 rows each comprising three (12x3) directors.
Figure 14 shows the directivity function of a SGPCY antenna arrangement with 12x3
directors in the horizontal plane in several frequencies.
Figure 15 shows the directivity function of a SGPCY antenna arrangement with 12x3
directors in an elevation view in several frequencies.
Figure 16 shows a three dimensional directivity function of a SGPCY antenna arrangement
with 8x2 directors.
Figure 17 shows the directivity function of a SGPCY antenna arrangement with 8x2 directors
in the horizontal plane in several frequencies.
Figure 18 shows the directivity function of a SGPCY antenna arrangement with 8x2 directors
in an elevation view in several frequencies.
Figure 19 shows a further modification of the Circular Yagi antenna arrangement comprising
a conductive ground plane, which is spatially separated from the passive antenna elements
and which laterally extends below all passive antenna elements.
Detailed Description
[0043] The illustration in the drawing is schematical. It is noted that in different figures,
similar or identical elements are provided with the same reference signs or with reference
signs, which are different from the corresponding reference signs only within the
first digit.
[0044] Figure 1 shows the basic idea of a Circular Yagi antenna arrangement 100. The antenna
arrangement 100 comprises a base element 110. According to the embodiment described
here the base element is a base plate 110 made from an electrically non conductive
respectively a dielectric material. On an upper surface 110a of the base plate 110
there is attached a plurality of dipole type antenna elements 120 and 121. The antenna
element 121 is an active antenna element, which is fed by a not depicted feed line
from the bottom side of the base plate 110. The passive antenna elements 121, which
according to Yagi technology represent directors, are also attached to the dielectric
base plate 110. The antenna elements 121 are arranged in a symmetrical way surrounding
the active antenna element 120, which is located in the center of the whole antenna
arrangement 100.
[0045] The antenna elements 121 are grouped in rows, which radially extend from the central
active antenna element 120. As can be seen from Figure 1, the antenna arrangement
comprises altogether sixteen rows 125-1, 125-2, 125-3, 125-4, 125-5, 125-6, 125-7,
125-8, 125-9, 125-10, 125-11, 125-12, 125-13, 125-14, 125-15 and 125-16. As can be
further seen from Figure 1, rows 125-1, 125-3, 125-5, 125-7, 125-9, 125-11, 125-13
and 125-15 have three passive director elements and correspondingly rows 125-2, 125-4,
125-6, 125-8, 125-10, 125-12, 125-14 and 125-16 have four passive director elements.
[0046] It has to be mentioned that antenna arrangements in accordance with the invention
can also comprise a different number of rows. Also the number of directors being assigned
to a row can also differ from three or four. There are many different combinations
possible wherein the number of rows is preferably equal or larger than four and the
number of passive antenna elements being assigned to one row is at least one. There
is no fundamental limitation restricting the number of rows and/or the number of passive
antenna elements being assigned to a single row. However, it has to be mentioned that
there may be a technical limit in that sense, that if the number of passive elements
is large the gain doesn't necessarily increase with the number of passive elements
or the antenna is not omni-directional anymore.
[0047] Figure 2 shows a three dimensional directivity function of the antenna arrangement
100. Thereby, the gain in a certain directions with respect to the point of origin,
which directions are defined by the three coordinates x, y and z, is defined by the
spatial distance between the corresponding point of the surface of the three dimensional
directivity function and the point of origin.
[0048] The illustrated three dimensional directivity function has been calculated for electromagnetic
radiation having a frequency of 2.442 GHz. The maximum gain is 4.9 dBi in certain
horizontal directions. Thereby the unit dBi refers to decibels referring to a fictitious
isotropic antenna, which uniformly distributes the whole available radiation energy
into all directions. This means that in the present case the antenna arrangement 100
comprises a maximum gain in certain horizontal directions, which maximum gain is 4.9
dB higher than the gain of an isotropic antenna.
[0049] It has to be mentioned that according to the mathematical definition of "Decibel"
the axis Gx(dB), Gy(dB) and Gz(dB) represent a logarithmic scale.
[0050] Figure 3 shows the directivity function of the antenna arrangement 100 in the horizontal
plane for seven different frequencies of electromagnetic radiation. The depicted frequencies
are 2.379 MHz, 2.4 MHz, 2.421 MHz, 2.442 MHz, 2.463 MHz, 2.484 MHz and 2.505 MHz.
Since these directivity functions are very close to each other they can hardly be
resolved in Figure 3.
[0051] Figure 4 shows the directivity function of the antenna arrangement 100 in an elevation
view. In the transmitting case most of the radiation intensity is emitted into the
horizontal plane given by the angular values -90° and 90°. Further, there are also
minor intensity peaks of electromagnetic radiation being emitted into directions having
an angle of +45° and -45° with respect to the horizontal plane. However, since again
the axis have a logarithmic scale these intensity peaks only represent comparatively
little radiation intensity.
[0052] Figure 5 shows a further the Circular Yagi antenna arrangement 500 representing a
modification of the antenna arrangement 100. The antenna arrangement 500 comprises
a metal base plate 510, which has an upper surface 510a. The base plate 510 has a
substantially circular size, which extends below the active antenna element 520 and
below all passive antenna elements 521. In the following such an antenna arrangement
having a large metal base plate 510 is denominated a Large Ground Plane Circular Yagi
(LGPCY) antenna arrangement.
[0053] According to the embodiment depicted here the passive antenna elements 521 are arranged
within 8 rows each extending radially outwards from the center of the antenna arrangement
respectively from the active antenna element 520. As can be seen from Figure 5 each
row comprises three passive antenna elements 521. Such an arrangement comprising eight
rows each having three directors 521 will be denominated as an 8x3 director arrangement.
[0054] The metal base plate 510 represents an electromagnetic mirror in particular for the
electric potential being generated by the antenna arrangement 500. This mirror behavior
has the advantage that compared to the antenna arrangement 100 shown in Figure 1,
the height of the antenna elements 520, 521 can be reduced by a factor of two. This
is based on the matter of fact that the electromagnetic mirror has the same effect
as a further antenna element arrangement, which is directly attached to the arrangement
500 in a mirror-inverted way. Therefore, by using a metal plate 510 as a base element
the effective height of the antenna elements and; as a consequence, the effective
height of the whole antenna arrangement 500 can be significantly reduced compared
to an antenna arrangement being assembled on a dielectric base element.
[0055] In other words the metal base plate 510 results in a monopole-type active antenna
element 520, which is feeding passive monopole-type directors 521.
[0056] Figure 6 shows a three dimensional directivity function of the antenna arrangement
500. The illustrated directivity function has been calculated for electromagnetic
radiation having a frequency of 2.442 GHz. The maximum gain is 4.2 dBi in certain
directions seen in Figures 7 and 8.
[0057] Figure 7 shows the directivity function of the antenna arrangement 500 in the horizontal
plane for seven different frequencies of electromagnetic radiation. Again, the depicted
frequencies are 2.379 MHz, 2.4 MHz, 2.421 MHz, 2.442 MHz, 2.463 MHz, 2.484 MHz and
2.505 MHz. Since these directivity functions are very close to each other they can
hardly be resolved in Figure 7.
[0058] Each of the depicted directivity functions exhibits eight bumps protruding outwardly.
In between two neighboring bumps there is a dimple (minimum). Differences between
the different frequency directivity functions can only be seen within the regions
of one of the eight the dimples. The difference between the maximums and minimums
in the antenna gain, ripple in the antenna gain, depends of the number of passive
director element rows used in the antenna.
[0059] Figure 8 shows the directivity function of the antenna arrangement 500 in an elevation
view. In the transmitting case most of the radiation intensity is emitted into a direction
being oriented approximately 20° angularly offset with respect to the horizontal plane
given by the angular values -90° and 90°. This is based on the fact that the metallic
base plate 510, which has a diameter of approximately 350 mm, has a limited lateral
dimension and therefore does not act as a perfect electromagnetic mirror, which would
require an infinite lateral dimension.
[0060] Figure 9 shows a further the Circular Yagi antenna arrangement 900 representing a
modification of the antenna arrangement 500. The antenna arrangement 900 comprises
a small metal base plate 915. The metal base plate 915 has a substantially circular
size, which extends solely below the active antenna element 920.
[0061] Below the passive antenna elements 921 and surrounding the metal base plate 915 there
is formed a dielectric base plate 910, which supports the passive antenna elements
921. In the following such an antenna arrangement having a small metal base plate
915 is denominated a Small Ground Plane Circular Yagi (SGPCY) antenna arrangement.
[0062] According to the embodiment depicted here the passive antenna elements 921 are arranged
within twelve rows 925-1, 925-2, 925-3, 925-4, 925-5, 925-6, 925-7, 925-8, 925-9,
925-10, 925-11 and 925-12 each extending radially outwards from the center of the
antenna arrangement respectively from the active antenna element 920. As can be seen
from Figure 9 each row comprises four passive antenna elements 521. Such an arrangement
comprising twelve rows each having four directors 921 will be denominated a 12x4 director
arrangement.
[0063] Since solely for the active antenna element 920 the metal plate 915 represents an
electromagnetic mirror, the length of the active antenna element 920 can be reduced
by a factor of two compared to an antenna arrangement having no metal plate. Since
the passive antenna elements are supported by a non conductive dielectric base element
910 the length of the directors 921 corresponds to the length of the directors 121
of the antenna arrangement 100 illustrated in Figure 1. According to the embodiment
described here the maximal diameter of the base element 910 is 469 mm.
[0064] In other words, the SGPCY antenna arrangement 900 results in a monopole-type active
antenna element 920, which in operation feeds the surrounding passive dipole-type
directors 921.
[0065] Figure 10 shows a three dimensional directivity function of the antenna arrangement
900. The illustrated directivity function has been calculated for electromagnetic
radiation having a frequency of 2.442 GHz. The maximum gain is 6.2 dBi in certain
horizontal directions.
[0066] Figure 11 shows the directivity function of the antenna arrangement 900 in the horizontal
plane for seven different frequencies of electromagnetic radiation. The depicted frequencies
are again 2.379 MHz, 2.4 MHz, 2.421 MHz, 2.442 MHz, 2.463 MHz, 2.484 MHz and 2.505
MHz. Since also these directivity functions are very close they can hardly be resolved
from each other in Figure 11. Each of the depicted directivity functions exhibits
twelve bumps protruding outwardly. In between two neighboring bumps there is a radially
dimple. Differences between the different frequency directivity functions can only
be seen within the regions of the above described dimples.
[0067] Figure 12 shows the directivity function of the antenna arrangement 900 in an elevation
view. In the transmitting case most of the radiation intensity is emitted into the
horizontal plane given by the angular values -90° and 90°. Further, there are also
minor intensity peaks of electromagnetic radiation being emitted into directions having
an angle of +-45° with respect to the horizontal plane. However, since the axis have
a logarithmic scale these intensity peaks only represent comparatively little radiation
intensity.
[0068] Figure 13 shows a three dimensional directivity function of a SGPCY antenna arrangement,
which is not explicitly depicted in the accompanying drawing. The antenna arrangement
comprises a 12x3 director arrangement and a maximum diameter of 352 mm. The illustrated
directivity function has been calculated again for electromagnetic radiation having
a frequency of 2.442 GHz. The maximum gain is 4.7 dBi in certain horizontal directions.
[0069] Figure 14 shows the directivity function of the above-mentioned SGPCY antenna arrangement
having a 12x3 director arrangement in the horizontal plane. The directivity function
is again depicted for the frequencies of 2.379 MHz, 2.4 MHz, 2.421 MHz, 2.442 MHz,
2.463 MHz, 2.484 MHz and 2.505 MHz. Each of the depicted directivity functions exhibits
twelve bumps respectively protruding outwardly.
[0070] Figure 15 shows the directivity function of the above-mentioned SGPCY antenna arrangement
having a 12x3 director arrangement in an elevation view. Again most of the radiation
intensity is emitted into the horizontal plane given by the angular values -90° and
90°. Further, there are again minor intensity peaks of electromagnetic radiation being
emitted into directions having an angle of +45° or -45° with respect to the horizontal
plane.
[0071] Figure 16 shows a three dimensional directivity function of a further SGPCY antenna
arrangement, which is also not explicitly depicted in the accompanying drawing. This
antenna arrangement comprises an 8x2 director arrangement and a maximum diameter of
235 mm. The illustrated directivity function has been calculated again for electromagnetic
radiation having a frequency of 2.442 GHz. The maximum gain is 4.4 dBi in certain
horizontal directions.
[0072] Figure 17 shows the directivity function of the above-mentioned SGPCY antenna arrangement
having the 8x2 director arrangement in the horizontal plane. The directivity function
is again depicted for the frequencies of 2.379 MHz, 2.4 MHz, 2.421 MHz, 2.442 MHz,
2.463 MHz, 2.484 MHz and 2.505 MHz.
[0073] Each of the depicted directivity functions exhibits eight bumps protruding outwardly.
[0074] Figure 18 shows the directivity function of the above-mentioned SGPCY antenna arrangement
having the 8x2 director arrangement in an elevation view. Again most of the radiation
intensity is emitted into the horizontal plane given by the angular values -90° and
90°.
[0075] Figure 19 shows an antenna arrangement 1900 representing a further modification of
the Circular Yagi antenna arrangement. The antenna arrangement 1900 comprises a conductive
ground plane 1955, which is spatially separated from the passive antenna elements
1921 and which laterally extends below all passive antenna elements 1921. The passive
antenna elements respectively the directors 1921, which can be realized for instance
by strips on vertical substrate pieces, are mounted to a not depicted dielectric support
base element.
[0076] According to the embodiment described here, the active antenna element respectively
the feed element 1920 is a monopole-type antenna element. A feed connector 1960 is
used to electrically connect the active antenna element 1920.
[0077] The antenna arrangement 1900 has the advantage that it directs the beam nearer to
the horizon as compared for instance the antenna arrangement 500 (see Figure 8), but
a nearby ceiling does not disturb its performance as it is a case with the antenna
arrangements 100 and 900 as presented in Figure 1 and Figure 9, respectively. Although
the antenna arrangement 1900 is very similar to the antenna arrangement 900 shown
in Figure 9, when employing the antenna arrangement 1900 a nearby ceiling and electronics
under the conductive ground-plane 1955 are effectively shielded in a more controlled
way.
[0078] It should be noted that the term "comprising" does not exclude other elements or
steps and the "a" or "an" does not exclude a plurality. Also elements described in
association with different embodiments may be combined. It should also be noted that
reference signs in the claims should not be construed as limiting the scope of the
claims.
List of reference signs:
[0079]
- 100
- antenna arrangement
- 110
- base element / base plate
- 110a
- upper surface
- 120
- active dipole-type antenna element
- 121
- passive dipole-type antenna elements / directors
- 125-X
- row of passive antenna elements / directors (X = 1, 2, 3, ..., 16)
- 500
- antenna arrangement
- 510
- metal base element / metal base plate
- 510a
- upper surface
- 520
- active monopole-type antenna element
- 521
- passive monopole-type antenna elements / directors
- 525-X
- row of passive antenna elements / directors (X = 1, 2, 3, ..., 18)
- 900
- antenna arrangement
- 910
- dielectric base element / dielectric base plate
- 910a
- upper surface
- 915
- metal plate / metal coating
- 920
- active monopole-type antenna element
- 921
- passive antenna elements / directors
- 925-X
- row of passive antenna elements / directors (X = 1, 2, 3, ..., 16)
- 1900
- antenna arrangement
- 1920
- active monopole-type antenna element
- 1921
- passive antenna elements / directors
- 1955
- conducting ground-plane
- 1960
- Feed connector
1. An antenna arrangement, in particular an antenna arrangement based on the principles
of Yagi antenna technology, the antenna arrangement (100, 500, 900) comprising
• a base element (110, 510, 910) having an upper surface (110a, 510a, 910a),
• an active antenna element (120, 520, 920), which is attached to the base element
(110, 510, 910) and which extends substantially perpendicular to the upper surface
(110a, 510a, 910a), and
• a plurality of passive antenna elements (121, 521, 921), which are attached to the
base element (110, 510, 910) and which extend substantially perpendicular to the upper
surface (110a, 510a, 910a),
wherein the active antenna element (120, 520, 920) is located in the center of the
whole antenna arrangement (100, 500, 900) and
wherein the passive antenna elements (121, 521, 921) are arranged in at least four
rows (125, 525, 925), whereby each row (125, 525, 925) extends radially outwards from
the center in a different direction.
2. The antenna arrangement according to claim 1, wherein within a two dimensional plane
being parallel to the upper surface (110a, 510a, 910a) of the base element (110, 510,
910)
the passive antenna elements (121, 521, 921) represent a symmetrical structure with
respect to the active antenna element (120, 520, 920).
3. The antenna arrangement according to any one of the claims 1 to 2, wherein
the base element is a plate (110, 510, 910).
4. The antenna arrangement according to any one of the claims 1 to 3, wherein
the base element (110) comprises an electrically non conductive material.
5. The antenna arrangement according to claim 4, further comprising
• a conducting ground-plane (1955), which is spatially separated from the passive
antenna elements (1921) and which laterally extends below all passive antenna elements
(1921).
6. The antenna arrangement according to any one of the claims 1 to 3, wherein
the base element (510, 910) comprises an electrically conductive material.
7. The antenna arrangement according to claim 6, wherein
the base element (510) extends along the whole antenna arrangement (500).
8. The antenna arrangement according to claim 6, wherein
the base element (910) extends solely along a portion of the whole antenna arrangement
(900).
9. A method for transmitting and/or for receiving electromagnetic radiation by means
of an antenna arrangement (100, 500 900) as set forth in any one of the previous claims.