1. Field of the Invention
The present invention relates to an antenna to be adapted to an antenna which is used in, for example, wireless LAN.
2. Description of the Related Art
A dipole antenna is non-directional in a horizontal plane. While non-directivity has an advantage of ensuring radiation in all the directions on a horizontal plane, it raises a problem of making it difficult to set an electric scatterer nearby. If an electric scatterer (a metal body, any other dielectric substance or the like) overlaps the peripheral portion of the antenna where the radiation level is high, electromagnetic coupling causes a current which should originally flow to the antenna to flow toward the electric scatterer. This results in deteriorations of the antenna characteristics, such as shifting of the resonance frequency of the antenna and reduction in the radiation efficiency of the antenna.
Recently, there is a need for a built-in dipole antenna from viewpoints of making devices compact and the design. The incorporation of an antenna allows a metal casing, a metal heat sink, a printed wiring board or the like to be positioned close to the antenna, leading to the aforementioned deteriorations of the antenna characteristics.
Possible solutions to this problem include increasing the distance between the antenna and the radio scatterer, and insertion of a radio absorber between the antenna and the radio scatterer. The method of increasing the distance hinders miniaturization of the whole antenna, and the insertion of the radio absorber stands in the way of reducing the cost. To incorporate a dipole antenna in a smaller space in a radio device at a lower cost, it is desirable to control the directivity of the antenna to spatially avoid the nearby radio scatterer.
As one way of controlling the directivity of an antenna, controlling the antenna directivity by using a linear parasitic element has been proposed (see JP-A-2001-185947(Patent Document 1)). The antenna described in Patent Document 1 has a common dipole 5 having a full length of λ/2 (λ: wavelength corresponding to the transmission frequency), shown in
A U-shaped parasitic element 7 is disposed in close vicinity of one end of the common dipole 5. The U-shaped parasitic element 7 includes a bottom portion 7a formed of a cylindrical conductor having a radius D3 and a length L3, and two arm portions 7b each formed of a cylindrical conductor having the radius D3 and a length L2. The U-shaped parasitic element 7 serves to match the impedance of the common dipole 5 with the impedance of the linear parasitic elements.
The electromagnetic wave from the common dipole 5 induces a resonance current in the linear parasitic elements 61 to 6n, so that the electromagnetic waves radiated from the linear parasitic elements 61 to 6n are combined with the electromagnetic wave radiated from the common dipole 5 to change the radiation directivity.
Even equipped with just one of the linear parasitic elements 61 to 6n, because of the provision of the U-shaped parasitic element 7, the antenna described in Patent Document 1 inevitably has a stereo (three-dimensional) arrangement of the common dipole 5 and the U-shaped parasitic element 7. This prevents the antenna from having a planar (two-dimensional) structure. The fact that the planar structure cannot be adopted hinders the miniaturization of the antenna and the formation of the antenna on a printed wiring board, which would otherwise lead to cost reduction.
It is therefore desirable to provide a compact and low-cost antenna whose directivity is controllable.
According to an embodiment of the present invention, there is provided an antenna including a dipole antenna, and a parasitic element arranged in parallel to the dipole antenna and having a linear structure and a meander structure, wherein a directivity and a return loss of the dipole antenna are controlled by setting a distance between the dipole antenna and the parasitic element and a shape and size of the meander structure.
According to another embodiment of the invention, there is provided an antenna including a dipole antenna, and a parasitic element arranged in parallel to the dipole antenna and having a linear structure and a spiral structure, wherein a directivity and a return loss of the dipole antenna are controlled by setting a distance between the dipole antenna and the parasitic element and a shape and size of the spiral structure.
According to a further embodiment of the invention, there is provided an antenna including a dipole antenna, and a parasitic element arranged in parallel to the dipole antenna and having a linear structure and a folded structure, wherein a directivity and a return loss of the dipole antenna are controlled by setting a distance between the dipole antenna and the parasitic element and a shape and size of the folded structure.
According to the embodiments of the invention, the directivity of the antenna and the return loss can be controlled merely by a dipole antenna and a parasitic element which includes a meander structure, a spiral structure or a folded structure, so that the antenna can be configured planarly or by a single printed wiring board. This can ensure cost reduction.
Preferred embodiments of the present invention will be described below with reference to the accompanying drawings. The description will be given in the following order.
Although the embodiments to be described below are favorable specific examples of the invention to which various technically preferable restrictions are given, it should be understood that the scope of the invention is not limited to those embodiments unless otherwise particularly specified.
The first embodiment of the invention will be described below referring to
A parasitic element 4 having meander structures at both ends of a linear structure is provided at a location away from the dipole antenna by an arbitrary distance D. The distance D is the distance between the center of the conductor of the dipole antenna and the center of the linear structure portion of the parasitic element 4. The total length of the parasitic element 4 is substantially equal to that of the dipole antenna. The dipole antenna and the parasitic element 4 are realized by, for example, conductive patterns on a printed wiring board. The printed wiring board in use is a double-sided board on which wiring patterns can be formed on both sides thereof.
The parasitic element 4 serves to control the directivity of the dipole antenna having the dipole antenna (positive port) 1, the power feed point 2 and the dipole antenna (negative port) 3. The parasitic element 4 also serves to obtain impedance matching between the dipole antenna, which has the dipole antenna (positive port) 1, the power feed point 2 and the dipole antenna (negative port) 3, and the parasitic element 4.
The directivity of the dipole antenna and the amount of the return loss thereof can be controlled by adjusting the distance D from the dipole antenna to the parasitic element 4 having the meander structure, and the shape and size of the meander structure. The shape and size of the meander structure mean the number of folds, the diameter (width) of the element, the interval between parallel folded portions, the length between both ends of the folded portion, and so forth.
The radiation pattern of only the dipole antenna which serves as the power feed element becomes a circle about the position of the dipole antenna in the (X-Y) plane and the (X-Z) plane, and is non-directional. When a high-frequency current is supplied to the dipole antenna from the power feed point 2, an electromagnetic wave is radiated. The electromagnetic wave from the dipole antenna induces a current in the parasitic element 4. The amplitude and phase of the current are controlled by the distance D, and the shape and size of the meander structure. The electromagnetic wave radiated from the dipole antenna is combined with the electromagnetic wave radiated from the parasitic element 4 to control the directivity.
The parasitic element 4 serves as a reflector or a radiator, and provides a directivity having a shape extruded toward the parasitic element in the horizontal plane. Further, reception of the electromagnetic wave radiated from the parasitic element 4 changes the impedance of the dipole antenna as viewed from the power feed point 2.
As shown in
A first example of the second embodiment of the invention will be described below referring to
Unlike in the first embodiment, the meander structure is formed concentratedly on the dipole antenna (negative port) 14 side of the linear element that constitutes the parasitic element 15. As shown in
As shown in a side view of
The third embodiment of the invention will be described below referring to
This antenna is configured to control the directivity and the return loss of the dipole antenna by setting the distance D between the dipole antenna and the parasitic element, and the shape and size of the spiral structure. The shape and size of the spiral structure are equivalent to the number of spiral turns, the diameter (width) of the conductor, the interval between conductors, etc. According to the third embodiment, the spiral structure is formed concentratedly on one end side of the linear structure of the parasitic element 23 to enable control of the directivity on the (X-Y) plane, as per the second embodiment.
The fourth embodiment of the invention will be described below referring to
This antenna is configured to control the directivity and the return loss of the dipole antenna by setting the distance D between the dipole antenna and the parasitic element, and the shape and size of the spiral structure. The shape and size of the spiral structure are equivalent to the number of spiral turns, the diameter (width) of the conductor, the interval between conductors, etc. According to the fourth embodiment, the folded structure is formed concentratedly on one end side of the linear structure of the parasitic element 27 to enable control of the directivity on the (X-Y) plane, as per the second embodiment.
It is to be noted that the present invention is not limited to the foregoing embodiments, but may be modified in various forms based on the technical concept of the invention. Although the parasitic element has substantially the same length as the length T of the dipole antenna in the foregoing embodiments, such setting is not essential. The length of the dipole antenna is not limited to λ/2, but may be set to other lengths, such as λ/4.
The present application contains subject matter related to that disclosed in Japanese Priority Patent Application JP 2009-045194 filed in the Japan Patent Office on Feb. 27, 2009, the entire contents of which is hereby incorporated by reference.
It should be understood by those skilled in the art that various modifications, combinations, sub-combinations and alterations may occur depending on design requirements and other factors insofar as they are within the scope of the appended claims or the equivalents thereof.
Number | Date | Country | Kind |
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P2009-045194 | Feb 2009 | JP | national |