JP2008295090A - Broadband antenna - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a broadband antenna capable of achieving band-widening and multi-resonating. <P>SOLUTION: An antenna 100 comprises a plane conductor 1, a linear conductor 2, a feeding point 3, a ground plate 4 and the like. The plane conductor 1 has a rectangular plate shape, the feeding point 3 is formed at one corner thereof, and power feeding is performed. A side 1a (second side) communicating with the one corner is away from the side 4a (first side) of the ground plate 4 approximately in parallel by only a fine gap G. Furthermore, the other side 1b (third side) communicating to the one corner is located in a vertical direction to the side 4a of the ground plate 4. Then, the linear conductor 2 is connected near a terminal at an opposite side to the feeding point 3 on the side 1b. The surface of the plane conductor 1 and the surface of the ground plate 4 are positioned on the same surface and the linear conductor 2 is also disposed on the same surface. A low-frequency distance L=30 mm is about 1/4 with respect to a wavelength λL. A high-frequency distance H=19 mm is about 0.3 times with respect to a wavelength λH. The gap G is about 0.3 times or less of the high-frequency distance H=19 mm. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

  The present invention relates to a wideband antenna having a linear conductor and a planar conductor and capable of achieving multiple resonances and broadening the bandwidth.

(Background Technology 1)
There is a broadband antenna device (see, for example, FIG. 10 of Patent Document 1). The antenna device of Patent Document 1 has a configuration in which a planar microstrip antenna 42 is provided in parallel with the surface of the ground plane 6, and one end of the monopole antenna 1 is connected to one end of the microstrip antenna 42. This antenna device has a single resonance, and the length of the monopole antenna 1 is about half the wavelength of the resonance frequency. The length a of the planar microstrip antenna 42 is also about a half wavelength. If the width b of the planar microstrip antenna 42 is increased, the electrical volume of the antenna increases, so that a wide bandwidth is obtained.

(Background Technology 2)
There is a multi-resonance planar multiple antenna (see, for example, FIG. 5 of Patent Document 2). The planar multiplex antenna of Patent Document 5 has a rectangular conductor pattern 43 and a linear U-shaped conductor pattern 45, and the rectangular conductor pattern 43 is disposed on the same plane as the ground substrate conductor 49. This planar multiple antenna has multiple resonances, and the first resonance frequency f1, which is the frequency at which the current resonates in the entire U-shaped conductor pattern 45, and the inside of the U-shaped portion resonate. And a second resonance frequency f2 (f1 <f2).
JP 2002-64324 A (page 7, paragraph numbers 0096 to 0102, FIG. 10) Japanese Patent Laying-Open No. 2005-94501 (pages 4-5, paragraph numbers 0021, 0022, 0031-0033, FIG. 5)

  In the planar antenna of Background Art 1, a wide band is realized, but a multi-resonance cannot be realized. In the planar multiplex antenna of the background art 2, the multi-resonance resonance frequency is determined by the entire U-shaped conductor pattern 45 and the length of the inner portion, but there is no specific description for widening the band.

  The present invention has been made to solve the above-described problems, and an object of the present invention is to provide a wideband antenna capable of realizing a wide band and multiple resonances.

  In order to achieve the above object, a wideband antenna of the present invention includes a ground plane having a first side, a second side that is substantially in the same plane as the plane formed by the ground plane, and intersects each other. A polygon having a third side is formed, a feeding point is provided at a corner where the second side and the third side intersect, and the second side and the third side are the first side A plane conductor disposed in a direction opposite to and substantially orthogonal to one side and a plane substantially the same as the surface formed by the ground plane, and near the end of the third side opposite to the feeding point. A linear conductor that is connected and has an open end, and is determined by a distance from the feeding point to a diagonal of the corner where the feeding point of the planar conductor is provided via the second side. 1 and the distance from the feeding point to the open end of the linear conductor via the third side. Characterized in that wherein the Sadamari having the first second resonance frequency lower than the resonance frequency by.

  According to the present invention, it is possible to achieve a wideband and multiple resonance, and to obtain a wideband antenna in which the relationship between the resonance frequency and the dimensions of each part of the antenna is clarified.

  Embodiments of the present invention will be described below with reference to the drawings. In addition, when referring to the following figures, up, down, left, right, horizontal, vertical (vertical) means up, down, left, right, horizontal, vertical (vertical) on the paper on which the figure is represented, unless otherwise specified. . Moreover, the same code | symbol shall represent the same structure between each figure.

  Embodiment 1 of the present invention will be described below with reference to FIGS. FIG. 1 is a diagram illustrating the configuration of the wideband antenna according to the first embodiment.

  (A) is demonstrated. The antenna 100 includes a planar conductor 1, a linear conductor 2, a feeding point 3, a ground plane 4, and the like. The planar conductor 1 has a rectangular flat plate shape, and a feeding point 3 is provided at one corner to feed power. The side 1a (second side) connected to this corner is separated from the side 4a (first side) of the base plate 4 by a small gap G substantially in parallel. Further, another side 1 b (third side) connected to this corner is in a direction perpendicular to the side 4 a of the main plate 4. The linear conductor 2 is connected to the vicinity of the end of the side 1b opposite to the feeding point 3.

  Note that the point where the linear conductor 2 is connected does not have to completely coincide with the end of the side 1b opposite to the feeding point 3, but the feeding point 3 near the opposite end, for example, slightly from the opposite end. It may be close. Alternatively, the linear conductor 2 may protrude slightly from the opposite end in the vertical direction opposite to the feeding point 3 and extend in the horizontal direction therefrom.

  The linear conductor 2 is a linear radiating element, and is disposed substantially parallel to the side 4 a of the ground plane 4. The linear conductor 2 may have a rod shape or a narrow flat plate shape. The surface of the planar conductor 1 and the surface of the ground plane 4 are on the same plane, and the linear conductor 2 is also arranged on this same plane.

  A low-frequency distance L indicated by a dotted line is a distance related to one low-frequency resonance frequency of multi-resonance, and is a distance from the feeding point 3 to the open end of the linear conductor 2 via the side 1b of the planar conductor 1. It is. The high-frequency distance H indicated by a dotted line is a distance related to one high-frequency resonance frequency of multi-resonance, and is on the side from the feeding point 3 to the diagonal of the feeding point 3 via the side 1a of the planar conductor 1. The distance along.

  The difference between (b) and (a) will be described. The linear conductor 2 is different in that it is disposed substantially perpendicular to the side 4a of the ground plane 4. The low-pass distance L indicated by the dotted line is the distance from the feeding point 3 to the open end of the linear conductor 2 via the side 1b of the planar conductor 1 as in (a). The high-frequency distance H indicated by the dotted line is a distance along the side from the feeding point 3 to the diagonal of the feeding point 3 via the side 1a of the planar conductor 1 as in (a).

  Next, the relationship between the low frequency L and the low frequency resonance frequency, the relationship between the high frequency H and the high frequency resonance, the gap G, and the like in (a) and (b) will be described. FIG. 2 is a simulation diagram of the VSWR of the wideband antenna according to the first embodiment (FIGS. 1A and 1B). The conditions are a high frequency H = 19 mm, a low frequency L = 30 mm, and a gap G = 0.5 mm.

  (A) is a simulation figure of VSWR. Good regions with a VSWR of 3 or less appear in the low and high regions. Both of them are broadband.

  (B) is a simulation figure of input impedance. A cross point from negative to positive where reactance of input impedance = 0 is a resonance point. The low-band resonance frequency fL = 2.36 GHz, and its wavelength λL = 127.1 mm. The low-pass distance L = 30 mm is 0.24 times the wavelength λL, that is, approximately ¼. The high-band resonance frequency fH is 5.02 GHz, and the wavelength λH is 59.8 mm. The high frequency H = 19 mm is 0.32 times, that is, approximately 0.3 times the wavelength λH.

  FIG. 3 is a simulation diagram of the VSWR of the wideband antenna according to the first embodiment (FIGS. 1A and 1B). The condition is that the side 1a corresponding to the width of the planar conductor 1 in FIG. 1 is changed to 6 to 14 mm. The height portion of the planar conductor 1 is 11 mm, and therefore changes in the high frequency range H = (11 + 6) to (11 + 14) mm. The low-pass distance L = 30 mm and the gap G = 0.5 mm are fixed.

  (A) is a simulation figure of VSWR. When attention is paid to the low frequency region, the bandwidth of the side 1a = 14 mm is wider than the case of the side 1a = 6 mm, which is a good bandwidth with a VSWR of 3 or less.

  (B) is a simulation figure of input impedance. Even if the side 1a is changed, that is, the high-frequency distance H is changed, the low-frequency resonance frequency fL is not changed to 2.36 GHz, and the wavelength λL is 127.1 mm. The low-pass distance L = 30 mm is 0.24 times the wavelength λL, that is, approximately ¼. That is, the low-band resonance frequency fL can be determined independently at the low-band distance L.

  The high-band resonance frequency fH is approximately 3.6 GHz when the side 1a = 14 mm (high-band distance H = 25 mm), and its wavelength λH = 83 mm. The high frequency H = 25 mm is 0.30 times the wavelength λH. Further, when side 1a = 6 mm (high range distance H = 17 mm), it is approximately 5.8 GHz, and its wavelength λH = 51.7 mm. The high frequency H = 17 mm is 0.33 times, that is, approximately 0.3 times the wavelength λH.

  FIG. 4 is a simulation diagram of the VSWR of the wideband antenna according to the first embodiment (FIGS. 1A and 1B). The condition is that the gap G in FIG. 1 is changed to 1 to 6 mm. The high range distance H = 19 mm and the low range distance L = 30 mm are fixed.

  Resonance points occur in the low and high frequencies. The reason why both the low and high frequency resonance points are in a good state of VSWR = 3 or less is that the gap G is 5 mm or less. When the gap G is 6 mm, the high-frequency resonance point is NG.

  The low-pass resonance frequency fL varies somewhat depending on the change in the gap G, but is approximately 2.1 to 2.6 GHz, and the wavelength λL is 115 to 142 mm. The low-pass distance L = 30 mm is 0.21 to 0.26 times the wavelength λL, that is, approximately ¼λL.

  The high-band resonance frequency fH varies somewhat depending on the change in the gap G, but is approximately 4.3 to 5.3 GHz, and the wavelength λH is 57 to 70 mm. The high frequency H = 19 mm is 0.27 to 0.34 times the wavelength λH, that is, approximately 0.3λH.

  If the gap G is about 0.3 times or less of the high-frequency distance H = 19 mm, that is, if the gap G = 5.4 mm or less, a good state of VSWR = 3 or less can be obtained.

  According to the first embodiment, it is possible to obtain a wideband antenna in which a wide band and multiple resonances can be realized and the relationship between the resonance frequency and the dimensions of each part of the antenna is clarified.

  A second embodiment of the present invention will be described with reference to FIGS. FIG. 5 is a diagram illustrating the configuration of the wideband antenna according to the second embodiment. Differences from FIG. 1A will be described. The planar conductor 1 of the antenna 200 is not rectangular but is different in that the left side is slanted and the width of the upper side 1c is widened. The side 1c is longer than the side 1a. The high-frequency distance H indicated by the dotted line is a distance related to one high-frequency resonance frequency of multi-resonance, and, similar to FIG. 1, the high-frequency distance H of the power supply point 3 from the power supply point 3 via the side 1a of the planar conductor 1. The distance along the side to the diagonal.

  FIG. 6 is a simulation diagram of the VSWR of the wideband antenna according to the second embodiment (FIG. 5). The conditions are a high frequency H = 25 mm, among which the side 1a = 10 mm, the low frequency L = 30 mm, and the gap G = 0.5 mm.

  (A) is a simulation figure of VSWR. A good region with a VSWR of 3 or less is connected by a low region and a high region, resulting in an ultra-wide band.

  (B) is a simulation figure of input impedance. There are three resonance points. The low-band resonance frequency fL = 2.30 GHz, and the wavelength λL = 130.4 mm. The low-pass distance L = 30 mm is 0.23 times, that is, approximately a quarter of the wavelength λL. The high-band resonance frequency fH = 3.61 GHz, and its wavelength λH = 83.1 mm. The high frequency H = 25 mm is 0.30 times the wavelength λH.

  Further, a resonance frequency fH = 7.06 GHz is generated on the high frequency side, and its wavelength λH = 42.5 mm. This resonance point is related to the side 1a = 10 mm, and the side 1a = 10 mm is 0.24 times, that is, approximately a quarter of the wavelength λH = 42.5 mm.

  This is because by adjusting the width of the upper side portion of the planar conductor 1, it is possible to adjust the matching between the low-frequency resonance of the linear conductor 2 portion and the high-frequency resonance of the planar conductor 1. Can be obtained.

  According to the second embodiment, resonance points are connected to each other, an ultra-wide band is possible, and a broadband antenna in which the relationship between the resonance frequency and the dimensions of each part of the antenna is clarified can be obtained.

  Hereinafter, Embodiment 3 of the present invention will be described with reference to FIG. FIG. 7 is a diagram illustrating the configuration of the wideband antenna according to the third embodiment. 6 is another example of the shape of the planar conductor 1 of the antenna according to the first embodiment and the second embodiment. The illustration of the base plate 4 is omitted.

  (A) is that the antenna 300 has a side 1a of the planar conductor 1 that is not completely parallel to the side 4a of the ground plane 4 and is slightly inclined. As described with reference to FIG. 4, when the average gap G in this portion is approximately 0.3 times or less of the high frequency H, good multi-resonance can be generated.

  In (b), the planar conductor 1 is a pentagon. The high-frequency distance H indicated by the dotted line is a distance related to the high-frequency resonance frequency, and the side from the feeding point 3 to the diagonal of the feeding point 3 via the side 1a of the planar conductor 1 is the same as in FIG. Is the distance along.

  (C) is a further modification of (b), and the planar conductor 1h is a pentagon. The high-frequency distance H indicated by the dotted line is a distance related to the high-frequency resonance frequency, and the side from the feeding point 3 to the diagonal of the feeding point 3 via the side 1a of the planar conductor 1 is the same as in FIG. Is the distance along.

  Although not shown, the corner portion of the planar conductor 1 may have a slightly rounded shape. Further, the side related to the high frequency distance H indicated by the dotted line may be not only a straight line but also a rounded arc. Similarly, the side 1b related to the low frequency L indicated by a dotted line may be not only a straight line but also a circular arc shape. In that case, the high frequency H and the low frequency L are distances along the arc. Further, the linear conductor 2 may be not only parallel or perpendicular to the side 4a of the ground plane 4 but also oblique.

  According to the third embodiment, as in the first and second embodiments, it is possible to realize a wideband and multiple resonance, and to obtain a wideband antenna in which the relationship between the resonance frequency and the dimensions of each part of the antenna is clarified.

  Hereinafter, Example 4 of the present invention will be described with reference to FIG. FIG. 8 is a diagram illustrating the configuration of the wideband antenna according to the fourth embodiment. Example 4 differs in the shape of the linear conductor 2 compared with Examples 1-3. The linear conductor 2 of the antenna 400 is folded without being opened, and the tip is grounded to the side 4 a of the ground plane 4 in the vicinity of the feeding point 3. In general, when a linear conductor and a ground plane are installed close to each other, the input impedance of the antenna is lowered, impedance matching cannot be obtained, and the antenna characteristics are deteriorated.

  According to the fourth embodiment, when the linear conductor 2 is folded as shown in FIG. 8, it is possible to reduce a decrease in input impedance and to obtain good antenna characteristics.

  In addition, the plane conductor 1 and the linear conductor 2 of each embodiment may be changed in various combinations.

The figure explaining the structure of the wideband antenna which concerns on Example 1 of this invention. The simulation figure of VSWR of the wideband antenna which concerns on Example 1 of this invention. The simulation figure of VSWR of the wideband antenna concerning Example 1 of the present invention (side 1a is changed). The simulation figure of VSWR of the wideband antenna which concerns on Example 1 of this invention (gap G is changed). The figure explaining the structure of the wideband antenna which concerns on Example 2 of this invention. The simulation figure of VSWR of the wideband antenna which concerns on Example 2 of this invention. The figure explaining the structure of the wideband antenna which concerns on Example 3 of this invention. The figure explaining the structure of the wideband antenna which concerns on Example 4 of this invention.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Planar conductor 1a, 1b, 1c Side 2 Linear conductor 3 Feeding point 4 Ground plane 4a Side 100, 200, 300, 400 Antenna

Claims (3)

A main plate having a first side;
A polygon having a second side and a third side that are in a plane substantially the same as the surface formed by the ground plane and intersecting each other is formed at a corner where the second side and the third side intersect. A planar conductor provided with a feeding point, and arranged such that the second side and the third side are opposed to and substantially orthogonal to the first side, respectively.
A linear conductor that is in substantially the same plane as the surface formed by the ground plane, is connected to the vicinity of the end opposite to the feeding point of the third side and has an open end;
A first resonance frequency determined by a distance from the feeding point via the second side to a diagonal of the planar conductor where the feeding point is provided, and a third side from the feeding point. A wideband antenna characterized by having a second resonance frequency lower than the first resonance frequency, which is determined by the distance to the open end of the linear conductor.   The broadband antenna according to claim 1, wherein the first side and the second side are substantially parallel to each other.   The average distance between the first side and the second side is an approximate distance from the feeding point to the diagonal of the corner where the feeding point of the planar conductor is provided via the second side. The wideband antenna according to claim 1, wherein the value is equal to or less than a value corresponding to 0.3 times.

Images