The present invention relates to a hexagonal array structure of a dielectric rod for shaping a flat-topped element pattern (FTEP); and, more particularly, to a hexagonal array structure of a dielectric rod for shaping a flat-topped element pattern (FTEP) for having a wide beam scanning range and a constant electric performance generated from a strong electromagnetic wave mutual coupling by arranging a dielectric rod at a vertex of a regular hexagon as a center dielectric rod and arranging a predetermined size of dielectric rods around the center dielectric rod.
According to a Korea publication No. 10-2002-11503, entitled “Two dimensional multi layers circular radiation array structure for forming FTEP”, a phase control element is a major and expensive element for developing a phased array antenna. The number of the phase control elements is determined according to a gain of an antenna array, a side lobe level and a required sector beam scan angle. The gain of the antenna array and the level of side lobe are used for determining a shape or a size of an array aperture. Also, the required sector beam scan angle is used for determining a distance of array element space.
Also, when a conventional phase control element is designed, a maximum array space of the phase control elements is determined for preventing to generate a grating lobe in a real space in order to wide beam scanning.
In contrary, in a flat-topped element pattern (FTEP) scheme, the maximum array space is determined for preventing to generate the grating lobe in the real space since it has comparative narrow beam scanning range ±5° or 25°. And, the grating lobe can be suppressed by a side lobe characteristic of the FTEP. Accordingly, the space between phase control elements becomes comparatively wider and thus the number of the phase control elements can be minimized. For example, when a phase array requiring 20° of a cone shape beam scanning is designed, the number of phase control elements can be reduced to 1/11by using the FTEP scheme. Inhere, for forming FTEP within a required beam scanning range, an amplitude array characteristic of an array aperture must be satisfied to have overlapped sub-array. Also, the amplitude characteristic of array aperture must be satisfied to
for an one-dimensional array,
for a two-dimensional array, and
for a three-dimensional array.
For obtaining the above-mentioned characteristic, five conventional array structures have been introduced as follows.
As shown in
It is, therefore, an object of the present invention to provide a hexagonal array structure of a dielectric rod for shaping a flat-topped element pattern (FTEP) for having a wide beam scanning range and a constant electric performance generated from a strong electromagnetic wave mutual coupling by arranging a dielectric rod at a vertex of a regular hexagon as a center dielectric rod and arranging a predetermined size of dielectric rods around the center dielectric rod.
In accordance with an aspect of the present invention, there is also provided a hexagonal structure of dielectric rods forming a flat-topped element pattern (FTEP), including: a center element for forming a unit radiation pattern of the FTEP through an electromagnetic wave mutual coupling by receiving a polarization signal of a basic mode; a plurality of first ring elements arranged at vertexes of a regular hexagon based on the center element for forming the unit radiation pattern by electric wave mutual coupling with the center element and an electromagnetic wave; and a circular waveguide array supporting unit for supporting the center element and the plurality of first ring elements.
In accordance with another aspect of the present invention, there is also provided a hexagonal structure of dielectric rods forming a flat-topped element pattern (FTEP), including: a center element and a plurality of first ring elements for forming a unit radiation pattern of the FTEP through an electromagnetic wave mutual coupling by receiving a polarization signal of a basic mode; a plurality of second ring elements arranged at vertexes of a regular triangle grating having one or two first ring elements as a vertex of the regular triangle and forming a shape of a regular hexagon for forming a radiation pattern by mutual coupling with the center element and the first ring elements; and a circular waveguide array supporting unit for supporting the center element, the plurality of first ring elements and the plurality of second ring elements.
In accordance with an aspect of the present invention, there is also provided a hexagonal structure of dielectric rods forming a flat-topped element pattern (FTEP), including: 6(N−1) elements including elements from a center element to a (N−1)th ring for forming a unit radiation pattern of the FTEP by electromagnetic wave mutual coupling by receiving a polarization signal of a basic mode; 6N of N ring elements for forming a unit radiation pattern by being arranged within a regular space and being electromagnetic wave mutual coupled with adjacent element; and a circular waveguide array supporting unit for supporting the 6(N−1) elements and the plurality of N ring elements.
The above and other objects and features of the present invention will become better understood with regard to the following description of the preferred embodiments given in conjunction with the accompanying drawings, in which:
Hereinafter, a hexagonal array structure of a dielectric rod for shaping a flat-topped element pattern (FTEP) in accordance with a preferred embodiment of the present invention will be described in more detail with reference to the accompanying drawings.
The hexagonal array structure of a dielectric rod includes a center element 510, six of first ring elements 520, twelve of second ring elements 530 and a circular waveguide array supporting unit 540.
When a basic mode signal is feed through a polarizer 512 to the center element 510 and the six first rings 520, an electric distribution satisfying a requirement is formed on the twelve second elements 530 and an antenna aperture by electromagnetic wave mutual coupling of twelve second ring elements 530. Also, a FTEP radiation pattern is formed at a far-field region. The center element 510 includes an input circular coaxial cable 511, a polarizer 512 and a dielectric rod 513.
The input circular coaxial cable 511 feeds an input signal and the polarizer 512 is a thin dielectric plate located inside a circular waveguide and forms a required polarization. The dielectric rod 513 forms a traveling wave and radiates the traveling wave signal. Also, the dielectric rod 513 forms a unit radiation pattern forming the FTEP by the electromagnetic wave mutual coupling.
The center element 510 and each of the first ring elements 520 form the FTEP unit radiation pattern by mutually coupling to the second ring elements 530. The first ring elements 520 are arranged around the center element 510. The space between the first ring elements 520 is dx and dy, and accordingly, locations of the first ring elements in a x y coordinate are (dx, dy), (dx, −dy), (−dx, dy) (−dx, −dy), (0, 2dy), (0, −2dy). The second ring elements are arranged at a vertex of regular triangle having one or two first ring elements as a vertex. That is, the second ring elements form a second hexagonal. Locations of the second ring elements in a x y coordinate are (2dx, 0), (−2dx, 0), (2dx, 2dy), (2dx, −2dy), (dx, 3dy), (dx, −3dy), (0, 4dy), (0, −4dy), (0, 2dy), (0, −2dy), (−dx, 3dy), (−dx, −3dy) as shown in
The center element 510 and the six first ring elements include the polarizer 512 for generating polarization and twelve second ring elements do not include the polarizer 512.
As mentioned above, the present invention can suppress the grating lobe and decrease the number of radiation elements by arranging a dielectric rod at a vertex of a regular hexagon as a center dielectric rod and arranging a predetermined size of dielectric rods around the center dielectric rod for shaping a flat-topped element pattern (FTEP). Therefore, the present invention can decreases a cost of antenna system, feeding loss and can be implemented to a comparative wide beam scanning.
Also, the present invention can be easily implemented for a millimeter bandwidth (more than 10 GHz) and would comparatively light by fixing constant size of dielectric rod at a waveguide.
While the present invention has been described with respect to certain preferred embodiments, it will be apparent to those skilled in the art that various changes and modifications may be made without departing from the spirits and scope of the invention as defined in the following claims.
Number | Date | Country | Kind |
---|---|---|---|
10-2003-0098389 | Dec 2003 | KR | national |
Number | Name | Date | Kind |
---|---|---|---|
5767807 | Pritchett | Jun 1998 | A |
6539155 | Broeng et al. | Mar 2003 | B1 |
6597851 | Johnson et al. | Jul 2003 | B2 |
6791757 | Hobbs et al. | Sep 2004 | B2 |
6909729 | Ibanescu et al. | Jun 2005 | B2 |
20010012149 | Lin et al. | Aug 2001 | A1 |
Number | Date | Country |
---|---|---|
2002-016427 | Jan 2002 | JP |
1020030071996 | Sep 2003 | KR |
Number | Date | Country | |
---|---|---|---|
20050140559 A1 | Jun 2005 | US |