Patent Grant
11664602
The present application is based on PCT filing PCT/JP2019/017062, filed Apr. 22, 2019, which claims priority to JP 2018-090595, filed May 9, 2018, the entire contents of each are incorporated herein by reference.
The present disclosure relates to a lens, an antenna, and a device for vehicle.
PTL 1 discloses a Luneburg lens. A typical Luneburg lens is a spherical lens that has a relative dielectric constant that changes in a radial direction. The lens disclosed in PTL 1 is hemispherical and has a relative dielectric constant that changes stepwise.
NPL 1 (Mushiake Yasuto, “antenna⋅radio wave propagation”, CORONA PUBLISHING CO., LTD., Jun. 25, 1983, P. 106) discloses that regarding a Luneburg lens, a relationship between a refractive index and a distance from the center of the lens satisfies: refractive index=square root of 2−(r/a){circumflex over ( )}2. In the above expression, r is the distance from the center of the lens, and a is the radius of the lens.
The relative dielectric constant is given as the square of the refractive index, and the relative dielectric constant of the Luneburg lens satisfies an expression: relative dielectric constant=2−(r/a){circumflex over ( )}2.
A lens according to the disclosure includes a dielectric having a first surface and a second surface that is spaced from the first surface and that faces the first surface in a direction of a reference axis intersecting the first surface. The dielectric has an equivalent relative dielectric constant that decreases in a direction from the reference axis toward outer circumferences of the first surface and the second surface.
Another aspect of the present disclosure is an antenna. An antenna according to the disclosure includes a lens including a dielectric having a first surface and a second surface that is spaced from the first surface and that faces the first surface in a direction of a reference axis intersecting the first surface, and a radio wave radiator that is disposed on outer circumferences of the first surface and the second surface. The dielectric has an equivalent relative dielectric constant that decreases in a direction from the reference axis toward the outer circumferences of the first surface and the second surface.
Another aspect of the present disclosure is a device for vehicle that includes an antenna. The antenna of the device for vehicle according to the disclosure includes a lens including a dielectric having a first surface and a second surface that is spaced from the first surface and that faces the first surface in a direction of a reference axis intersecting the first surface, and a radio wave radiator that is disposed on outer circumferences of the first surface and the second surface. The dielectric has an equivalent relative dielectric constant that decreases in a direction from the reference axis toward the outer circumferences of the first surface and the second surface.
A spherical or hemispherical Luneburg lens can three-dimensionally change a radio wave radiation direction by three-dimensionally changing the position of a radio wave radiator along a spherical surface. However, it is necessary for the spherical or hemispherical Luneburg lens to have a relative dielectric constant that three-dimensionally changes in a radial direction from the center of a sphere or a hemisphere such that a “relationship between a refractive index and a distance from the center of the lens” disclosed in NPL 1 is satisfied. For this reason, the spherical or hemispherical Luneburg lens is difficult to manufacture.
The present inventors have found that a structure can be simplified and manufacturing is facilitated in the case where it suffices that the radiation direction two-dimensional changes.
The contents of embodiments of the present disclosure will now be listed and described.
(1) A lens according to an embodiment includes a dielectric having a first surface and a second surface that is spaced from the first surface and that faces the first surface in a direction of a reference axis intersecting the first surface. The dielectric has an equivalent relative dielectric constant that decreases in a direction from the reference axis toward outer circumferences of the first surface and the second surface. Since the dielectric is a structure having the first surface and the second surface that is spaced from the first surface and that faces the first surface in the direction of the reference axis intersecting the first surface, the structure is simpler than that in the spherical or hemispherical lens. In the case where the dielectric is composed of a single kind of substance, the equivalent relative dielectric constant is equal to the relative dielectric constant of the substance of which the dielectric is composed. In the case where the dielectric is composed of kinds of substances, the equivalent relative dielectric constant corresponds to a relative dielectric constant when the substances in the direction of the reference axis are regarded as a single substance, and is obtained as the weighted average of relative dielectric constants depending on the proportion of each substance in the direction of the reference axis.
(2) In the dielectric, a first substance that has a first relative dielectric constant and a second substance that has a second relative dielectric constant larger than the first relative dielectric constant are preferably adjacent to each other in the direction of the reference axis. In this case, the equivalent relative dielectric constant corresponds to a relative dielectric constant when the first substance and the second substance are regarded as a single substance.
(3) In the dielectric, a proportion of the second substance in the direction of the reference axis preferably decreases in the direction from the reference axis toward the outer circumferences. The equivalent relative dielectric constant can be decreased by decreasing the proportion of the second substance.
(4) The second substance preferably includes multiple components that are stacked in the direction of the reference axis. A structure that decreases the equivalent relative dielectric constant can be readily obtained by stacking the multiple components in a reference direction.
(5) The second substance is preferably subjected to a cutting process. The cutting process enables a structure that decreases the equivalent relative dielectric constant to be readily obtained.
(6) The second substances are preferably located on both sides of the first substance in the direction of the reference axis. In this case, a structure in which both sides of the first substance are interposed between the second substances is obtained.
(7) The first substance is preferably air. In this case, it is not necessary to process the first substance.
(8) The first relative dielectric constant is preferably less than 2.
(9) The second relative dielectric constant is preferably 2 or more.
(10) The lens preferably further includes a member that prevents a radio wave from leaking through the first surface, and a member that prevents a radio wave from leaking through the second surface. Radio waves can be prevented from leaking through the first surface and the second surface without increasing the length of the lens in the direction of the reference axis.
(11) The lens preferably further includes a waveguide that is disposed on the outer circumferences of the first surface and the second surface. In this case, a radio wave that propagates in a waveguide mode by using the waveguide can be incident on the dielectric, and the radio wave can efficiently propagate.
(12) The lens preferably further includes a member that prevents a radio wave from leaking through the first surface, a member that prevents a radio wave from leaking through the second surface, and a waveguide that is disposed on the outer circumferences of the first surface and the second surface. The waveguide is preferably integrally formed with the member that prevents the radio wave from leaking through the first surface and the member that prevents the radio wave from leaking through the second surface. In this case, a radio wave can be prevented from leaking with more certainty when the radio wave propagates from the waveguide to the lens.
(13) A length of the dielectric in the direction of the reference axis is preferably equal to or less than twice a wavelength of a radio wave that propagates in the dielectric. That is, the length of the dielectric in the direction of the reference axis is preferably 2λ or less where X is the wavelength. The length of the dielectric in the direction of the reference axis is more preferably 1.5λ or less, further preferably λ or less.
(14) A lens according to an embodiment is a two-dimensional Luneburg lens that changes a radio wave radiation direction into a direction parallel to a two-dimensional plane depending on a two-dimensional position of a radio wave radiator in the two-dimensional plane. The lens includes a first substance that has a first relative dielectric constant, and a second substance that is adjacent to the first substance in a direction perpendicular to the two-dimensional plane and that has a relative dielectric constant different from the first relative dielectric constant. As for the two-dimensional Luneburg lens, change in the radio wave radiation direction is preferably limited to the direction parallel to the two-dimensional plane.
(15) An antenna according to an embodiment is an antenna including a lens including a dielectric having a first surface and a second surface that is spaced from the first surface and that faces the first surface in a direction of a reference axis intersecting the first surface, and a radio wave radiator that is disposed on outer circumferences of the first surface and the second surface. The dielectric has an equivalent relative dielectric constant that decreases in the direction from the reference axis toward the outer circumferences of the first surface and the second surface.
(16) A length of the radio wave radiator in the direction of the reference axis is preferably equal to or less than a length of the dielectric in the direction of the reference axis. In this case, a radio wave can be inhibited from leaking near the boundary between the radio wave radiator and the dielectric when the radio wave is radiated.
(17) A length of the radio wave radiator in the direction of the reference axis is preferably equal to or more than a length of the dielectric in the direction of the reference axis. In this case, a radio wave can be inhibited from leaking near the boundary between the radio wave radiator and the dielectric when the radio wave is received.
(18) A length of the radio wave radiator in the direction of the reference axis is preferably equal to a length of the dielectric in the direction of the reference axis. In this case, radio waves can be inhibited from leaking near the boundary between the radio wave radiator and the dielectric when the radio wave is radiated and when the radio wave is received.
(19) A waveguide is preferably disposed between the radio wave radiator and the dielectric. In this case, a radio wave can propagate by using the waveguide between the radio wave radiator and the dielectric.
(20) A device for vehicle according to an embodiment is a device for vehicle including an antenna. The antenna includes a lens including a dielectric having a first surface and a second surface that is spaced from the first surface and that faces the first surface in a direction of a reference axis intersecting the first surface, and a radio wave radiator that is disposed on outer circumferences of the first surface and the second surface. The dielectric has an equivalent relative dielectric constant that decreases in the direction from the reference axis toward the outer circumferences of the first surface and the second surface.
Embodiments of the present disclosure will hereinafter be described with reference to the drawings. In the drawings, portions like or corresponding to each other are designated by like reference signs, and a description thereof is not repeated. At least parts of the embodiments described below may be freely combined.
[Structure]
(Antenna)
Referring to
More specifically, the device for vehicle 401 detects a direction from the vehicle Cr toward the wireless base station device 161 and adjusts a main radiation direction of radio waves that are transmitted from and received by the antenna 301, based on the result of detection. The direction from the vehicle Cr toward the wireless base station device 161 can change into any direction in a horizontal plane as the vehicle Cr runs. For this reason, the antenna 301 can adjust a radio wave radiation direction and a radio wave reception direction into any direction in the horizontal plane.
The antenna 301 may be capable of vertically adjusting the radio wave radiation direction. An angle at which the radio wave radiation direction and the radio wave reception direction can be vertically adjusted may be small.
The antenna 301 is not limited to an antenna that is included in the device for vehicle 401.
The antenna 301 can be used for wireless communication in accordance with a communication method other than 5G. However, the wireless communication in accordance with the communication method of 5G, in which the degree of straightness of radio waves is high, is more suitable to use the antenna 301 that can change the radio wave radiation direction and the radio wave reception direction.
Referring to
Examples of the radio wave radiators 221 include a horn antenna. In
The lens 201 includes a dielectric member 101, an upper member 22, and a lower member 23. The dielectric member 101 is consist of a dielectric. The dielectric member 101 is, for example, a columnar member and has an upper surface 11 and a lower surface 12.
The upper surface 11 and the lower surface 12 of the dielectric member 101 are circular. The radii R of the upper surface 11 and the lower surface 12 are designed to be 30 mm, for example, in the case where the antenna 301 transmits and receives radio waves in a band of 28 GHz. A relationship among the speed of light c, a frequency band f, and a wavelength λ satisfies an expression: c=f×λ, and the wavelength λ of a radio wave in a band of 28 GHz when the speed of light c satisfies c=3×10{circumflex over ( )}8 m/seconds is 10.7 mm.
In the following description, an XY plane in a direction in which the upper surface 11 and the lower surface 12 extend, that is, illustrated in
In the case where the dielectric member 101 is composed of kinds of substances, the dielectric member 101 has an equivalent relative dielectric constant Ere that is equal to the weighted average of relative dielectric constants in a thickness direction at a position a distance r away from the reference axis S and that decreases in a direction from the reference axis S that passes through the upper surface 11 and the lower surface 12 toward the outside of the dielectric member 101. An example of the reference axis S is an axis that passes through the center of the upper surface 11 and the center of the lower surface 12 and that extends in the perpendicular direction.
In the case where at the position the distance r away from the reference axis S, the dielectric member 101 is composed of a single kind of substance, the relative dielectric constant at the position of the distance r is referred to as the “equivalent relative dielectric constant εre”. In this case, the equivalent relative dielectric constant εre at the position the distance r away from the reference axis S is equal to the relative dielectric constant of the material thereof.
The number of the waveguides 151 is, for example, 7. The seven waveguides 151 are disposed at positions at which the waveguides 151 face the respective seven radio wave radiators 221. Specifically, an angle θ that is formed between a straight line L1 that passes through one of the waveguides 151 and the center of the upper surface 11 and a straight line L2 that passes through another waveguide 151 adjacent to the one of the waveguides 151 and the center of the upper surface 11 is, for example, 20°. The waveguides 151 cause radio waves to propagate between the radio wave radiators 221 and the dielectric member 101.
According to an embodiment, each waveguide 151 has a tubular shape that has a rectangular section perpendicular to a direction in which an inner space extends, that is, a waveguide direction. For example, the length of each of sides of the section is designed to be 7.112 mm in the case where the antenna 301 transmits and receives radio waves in a band of 28 GHz. The waveguide direction is a direction in which the waveguide 151 and the dielectric member 101 are connected to each other. The waveguide direction is parallel to the XY plane.
The lens 201 may not include the upper member 22, or the lower member 23, or both. In this case, the thickness of the dielectric member 101 is preferably set to a thickness equal to or more than a predetermined value. This predetermined value is a value that enables radio waves that propagate in the radial direction in the dielectric member 101 to pass through the inside of the dielectric member 101 before the radio waves leak out through the upper surface 11, or the lower surface 12 of the dielectric member 101, or both.
Referring to
The upper member 22 and the lower member 23 are composed of, for example, material containing metal or metal. As illustrated in
The height Hr of an opening portion of each radio wave radiator 221, that is, a length Hr of the radio wave radiator 221 in the perpendicular direction is equal to the distance a between the upper member 22 and the lower member 23, that is, the thickness of the dielectric member 101. This enables a radio wave to be inhibited from leaking near the boundary between the dielectric member 101 and each radio wave radiator 221.
In the case where it is not necessary to consider leakage of a radio wave near the boundary when the radio wave is received by the antenna 301, it suffices that the height Hr of the opening portion of the radio wave radiator 221 is equal to or less than the thickness of the dielectric member 101.
In the case where it is not necessary to consider leakage of a radio wave near the boundary when the radio wave is radiated from the antenna 301, it suffices that the height Hr of the opening portion of the radio wave radiator 221 is equal to or more than the thickness of the dielectric member 101.
Referring to
In this way, metal plates, for example, extend to positions nearer than the body portion 21 of the dielectric member 101 to the radio wave radiators 221, and a radio wave is consequently prevented from leaking near the boundary between the dielectric member 101 and each radio wave radiator 221 with more certainty.
Referring to
The relative dielectric constants εrM of the first member 21a and the second member 21b are referred to as “second relative dielectric constants εrM2”, and the second relative dielectric constants εrM2 are 2 or more. The first member 21a and the second member 21b are composed of, for example, resin that has a second relative dielectric constant εrM2 of 3.
More specifically, the thicknesses h of the first member 21a and the second member 21b decrease in a direction from the reference axis S toward the outside of the dielectric member 101. That is, as schematically illustrated in
Consequently, the equivalent relative dielectric constant εre of the dielectric member 101 decreases in the direction from the reference axis S toward the outside of the dielectric member 101. For example, as illustrated in a diagram of a relationship between the equivalent relative dielectric constant and a relative radius in
That is, the equivalent relative dielectric constant εre at the position the distance r away from the reference axis S has a value obtained by using a proportion between the material of the first member 21a and the second member 21b and the air that is the substance M and calculating the weighted average of the relative dielectric constant εrM2 of the material and the relative dielectric constant εrM1 of the air. For this reason, the dielectric member 101 can change the equivalent relative dielectric constant εre as in a spherical Luneburg lens.
In the case where at the position the distance r away from the reference axis S, the dielectric member 101 is composed of a single kind of substance as described above, the equivalent relative dielectric constant εre at the position the distance r away from the reference axis S is equal to the relative dielectric constant of the material, for example, the relative dielectric constant εrM2 or the relative dielectric constant εrM1.
Specifically, the thicknesses of the first member 21a and the second member 21b at the position the distance r away from the reference axis S in the horizontal plane are referred to as thicknesses hr.
A relationship between the equivalent relative dielectric constant εre and the thicknesses hr satisfies an expression:
εre=εrM1+(εrM2−εrM1)×2hr/a. (1)
Expression (1) is transformed, and the equivalent relative dielectric constant εre satisfies:
εre=(2hr/a)×εrM2+((a−2hr)/a)×εrM1. (2)
In expression (1) described above and expression (2) described above, a is the distance between the upper member 22 and the lower member 23 in the direction Z of the reference axis and corresponds to the thickness of the dielectric member 101. R is the radii of the upper surface 11 and the lower surface 12 of the dielectric member 101, εrM2 is the relative dielectric constant of a material of which the body portion 21 is composed, that is, the second substances, and εrM1 is the relative dielectric constant of the air that is the first substance.
That is, the equivalent relative dielectric constant εre is the total value of a value obtained by multiplying 2hr/a by the second relative dielectric constant εrM2 of the body portion 21 and a value obtained by multiplying (a−2hr)/a by the first relative dielectric constant εrM1 of the air. 2hr/a represents the proportion of the thickness 2hr of the body portion 21 at the position of the distance r to the thickness a of the dielectric member 101. The thickness 2hr of the body portion 21 is the sum of the thickness hr of the first member 21a and the thickness hr of the material of the second member 21b. ((a−2hr)/a) represents the proportion of the thickness of the air at the position of the distance r to the thickness a of the dielectric member 101.
(Body Portion)
Referring to
The first member 21a includes components 31 that are stacked in a direction parallel to the reference axis S. An example of each component 31 is a disk-shaped member that has a circular main surface, and the reference axis S passes through the center of the main surface. Here, the body portion 21 includes the eight components 31, that is, components 31a, 31b, 31c, 31d, 31e, 31f, 31g, and 31h.
The components 31a to 31h contain the same substance and have the same relative dielectric constant εrM. The components 31a to 31h are stacked downward from the upper member 22 in order of the components 31h, 31g, 31f, 31e, 31d, 31c, 31b, and 31a. The radii of the components 31a to 31h are referred to as radii r1 to r8, and the radii r1 to r8 satisfy a relationship in magnitude: r1<r2<r3<r4<r5<r6<r7<r8. That is, the sizes of the components 31a to 31h in the radial direction differ from each other. As a component of the components 31a to 31h is nearer to the plane P at the center of the dielectric member 101 in the thickness direction, the radius thereof is smaller than those of the others.
The second member 21b has the same structure as that of the first member 21a except that these are plane-symmetrical with respect to the plane P. That is, the second member 21b includes components that have different radii and that are stacked upward from the lower member 23. As a component of the components that are included in the second member 21b is nearer to the plane P at the center of the dielectric member 101 in the thickness direction, the radius thereof is smaller than those of the others. The thickness hr of each of the first member 21a and the second member 21b is equal to the total value of the thicknesses of the component or components 31 that are located at the position of the distance r.
In addition to a graph G1 illustrating the relationship between the distance r from the reference axis S of the dielectric member 101 and the equivalent relative dielectric constant εre of the dielectric member 101,
Referring to
εr=2−(r/R)2, (3)
as illustrated in the graph G2. That is, the relative dielectric constant εr continuously changes in the radial direction. Expression (3) is referred to as a Luneburg lens relational expression. The Luneburg lens that has a spherical shape has relative dielectric constant distribution that satisfies the Luneburg lens relational expression of expression (3) in any radial direction in an XYZ three-dimensional space.
Specifically, in the case where the radius R of the dielectric member 101 is 30 mm, the dielectric constant εr at the center of the lens, that is, a position at which the distance r satisfies r=0 mm is 2. The dielectric constant εr at a position near a surface of the lens, that is, a position at which the distance r satisfies r=30 mm is 1.
The dielectric member 101 of the lens 201 according to the present embodiment has relative dielectric constant distribution such that the distance r from the reference axis S and the relative dielectric constant εr satisfy the Luneburg lens relational expression given as expression (3) in the horizontal plane P that is the XY plane. The dielectric member 101 according to the present embodiment does not have the relative dielectric constant distribution that satisfies the Luneburg lens relational expression in the perpendicular direction that is a Z-direction. Thus, the lens 201 according to the present embodiment is a two-dimensional Luneburg lens that satisfies the Luneburg lens relational expression of expression (3) only in the radial direction in an XY two-dimensional space.
The lens 201 according to the present embodiment has the relative dielectric constant distribution that satisfies the Luneburg lens relational expression given as expression (3) in the horizontal plane and consequently defines focal points 171a to 171g on which radio waves are focused on the outer circumference 18 or near the outer circumference 18 of the lens 201 as illustrated in
The lens 201 according to the present embodiment enables change into a direction parallel to the two-dimensional plane P depending on the two-dimensional position of the waveguides 151 or the radio wave radiators 221 in the two-dimensional plane P. That is, as illustrated in
As for the dielectric member 101 according to the first embodiment of the present disclosure, the equivalent relative dielectric constant εre decreases in the direction from the reference axis S toward the outside of the dielectric member 101 as described above. That is, the thickness hr of the body portion 21 of the dielectric member 101 is designed such that the desired equivalent relative dielectric constant εre is obtained.
For example, the thickness hr is designed such that the equivalent relative dielectric constant εre of the dielectric member 101 satisfies expression (3) for the Luneburg lens.
Specifically, the thickness hr is designed to satisfy an expression:
hr={a×(2−(r/R)2−εrM1)}/{(εrM2−εrM1)/2}, (4)
from the relationship of expression (2) described above and expression (3) described above, that is, a relationship:
εre=(2hr/a)×εrM2+((a−2hr)/a)×εrM1=2−(r/R)2.
In addition, the thickness hr is designed to satisfy, for example, expression (2) described above in the case where the equivalent relative dielectric constant εre of the dielectric member 101 is changed stepwise so as to approximate to the relative dielectric constant εr of the Luneburg lens as illustrated in the graph G1 in
For example, the thickness hr is designed such that as the distance r increases, the equivalent relative dielectric constant εre decreases to 1.81, 1.74, 1.68, 1.62, 1.53, 1.39, 1.25, or 1.09, that is, decreases stepwise from 2 to 1.
The radii and thicknesses of the components 31a to 31h are designed, for example, to satisfy expression (1) described above such that the equivalent relative dielectric constant εre of the dielectric member 101 is the equivalent relative dielectric constant in the graph G1 illustrated in
Here, the radius R of the dielectric member 101 is 30 mm, the thickness a of the dielectric member 101 is 7.112 mm, and the relative dielectric constants εrM2 of the first member 21a and the second member 21b are 2.2.
In this case, for example, the thickness hr is designed such that εre=1.81 is satisfied at positions at which the distance r satisfies 0 mm≤r≤7.9 mm, that is, 0≤r/R≤0.264, specifically is designed to be about 2.40 mm. For example, the thickness hr is designed such that εre=1.74 is satisfied at positions at which the distance r satisfies 7.9 mm≤r≤11.7 mm, that is, 0.264≤r/R≤0.389, specifically is designed to be about 2.19 mm.
For example, the thickness hr is designed such that εre=1.68 is satisfied at positions at which the distance r satisfies 11.7 mm≤r≤14.6 mm, that is, 0.389≤r/R≤0.486, specifically, is designed to be about 2.02 mm. For example, the thickness hr is designed such that εre=1.62 is satisfied at positions at which the distance r satisfies 14.6 mm≤r≤17.7 mm, that is, 0.486≤r/R≤0.589, specifically is designed to be about 1.84 mm.
For example, the thickness hr is designed such that εre=1.53 is satisfied at positions at which the distance r satisfies 17.7 mm≤r≤21.2 mm, that is, 0.589≤r/R≤0.708, specifically, is designed to be about 1.57 mm. For example, the thickness hr is designed such that εre=1.39 is satisfied at positions at which the distance r satisfies 21.2 mm≤r≤24.5 mm, that is, 0.708≤r/R≤0.816, specifically is designed to be about 1.16 mm.
For example, the thickness hr is designed such that εre=1.25 is satisfied at positions at which the distance r satisfies 24.5 mm≤r≤27.4 mm, that is, 0.816≤r/R≤0.913, specifically is designed to be about 0.74 mm. For example, the thickness hr is designed such that εre=1.09 is satisfied at positions at which the distance r satisfies 27.4 mm≤r≤30 mm, that is, 0.913≤r/R≤1, specifically is designed to be about 0.27 mm.
Two or more adjacent components of the components 31a to 31h may be integrally formed.
The lens 201 is not limited to a structure in which the reference axis S passes through the center of the upper surface 11 and the center of the lower surface 12, provided that the lens 201 is located at a position at which the radio wave radiation direction is in a desired settable range, and the reference axis S may shift from the center of the upper surface 11, or the center of the lower surface 12, or both.
The dielectric member 101 is not limited to the columnar member, provided that the dielectric member 101 has the upper surface 11 and the lower surface 12.
[Manufacturing Method]
Referring to
Subsequently, the operator manufactures the first member 21a by stacking the components 31a to 31h in the direction parallel to the reference axis S (step S12).
Subsequently, the operator manufactures the second member 21b by stacking the components 31a to 31h in the direction parallel to the reference axis S (step S13).
Subsequently, the operator mounts the first member 21a and the second member 21b between the upper member 22 and the lower member 23. Specifically, the operator mounts the first member 21a on the upper member 22 and mounts the second member 21b on the lower member 23 (step S14).
The operator disposes the radio wave radiators 221 at positions at which the radio wave radiators 221 face the respective waveguides 151 around the lens 201 in which the first member 21a and the second member 21b are mounted (step S15).
The order of stacking the components 31a to 31h (step S12) and stacking the components 31a to 31h (step S13) may be switched.
The first member 21a and the second member 21b may be integrally manufactured by a cutting process. In this case, at step S11, a component A that is used for the first member 21a and a component B that is used for the second member 21b are prepared instead of the components 31a to 31h of the first member 21a and the components 31a to 31h of the second member 21b. At step S12, a cutting process is performed on the component A to manufacture the first member 21a. At step S13, a cutting process is performed on the component B to manufacture the second member 21b.
[Directivity of Antenna]
(Horizontal Plane Directivity of Horizontally Polarized Wave)
Referring to
As illustrated in the graph Gh4 and
The antenna 301 can thus change the radio wave radiation direction of the horizontally polarized waves with the gain ensured.
(Horizontal Plane Directivity of Vertically Polarized Wave)
Referring to
As illustrated in the graph Gv4 and
The antenna 301 can thus change the radio wave radiation direction of the vertically polarized waves with the gain ensured as in the horizontally polarized waves. That is, the antenna 301 can change the radio wave radiation direction by changing the waveguides 151 that are to be used to transmit and receive the radio waves.
The antenna 301 is not limited to a structure including the waveguides 151 but may include a single waveguide 151. In this case, the radio wave radiation direction can be changed from Ba into Bg, for example, by changing the position or direction of the single waveguide 151 from that of the waveguide 151a into that of the waveguide 151g in
The components 31a to 31h illustrated in
For example, the relative dielectric constant εrM of the components 31a to 31d illustrated in
Also, with this structure, the thicknesses of the components 31a to 31h can be designed such that the equivalent relative dielectric constant εre approximates to, for example, that in the graph G1 illustrated in
The first member 21a and the second member 21b may be formed, for example, by performing a cutting process on an integral component instead of stacking the components 31.
[First Modification]
Referring to
The first member 41a includes members that have different relative dielectric constants εrM. For example, the first member 41a is composed of a material that has a relative dielectric constant εrM of about 3 at a position at which the distance r from the reference axis S is 0 mm to a predetermined value rx1 and a material that has a relative dielectric constant εrM of about 2 at a position at which the distance r is more than the predetermined value rx1. The material that has a relative dielectric constant εrM of about 2 is, for example, polytetrafluoroethylene or polyethylene.
The thickness h of the first member 41a decreases stepwise in a direction from the reference axis S toward the outside of the dielectric member 102.
The structure of the second member 41b is the same as that of the first member 41a.
Consequently, the equivalent relative dielectric constant εre of the dielectric member 102 decreases stepwise in the direction from the reference axis S toward the outside of the dielectric member 102. Specifically, the equivalent relative dielectric constant εre of a portion of the dielectric member 102 through which the reference axis S passes is about 2, and the equivalent relative dielectric constant εre of an outer edge portion thereof is about 1.
In the dielectric member 102 according to the first modification to the first embodiment of the present disclosure, a member that has a low relative dielectric constant εrM is thus used for the portion at which the distance r is more than the predetermined value rx1, and the thickness h of this portion is consequently more than that in the dielectric member 101 illustrated in
[Second Modification]
Referring to
The structures of the first member 42a and the second member 42b are the same as the structures of the first member 21a and the second member 21b illustrated in
The dielectric member 103 further includes a low relative dielectric constant member 51 that has a relative dielectric constant εrM of no less than 1 and less than 2 as the substance M that has a relative dielectric constant εrM of less than 2. Examples of the low relative dielectric constant member 51 include polystyrene containing bubbles, that is, polystyrene foam and is disposed so as to fill a space between the first member 42a and the second member 42b.
In the lens 201 according to the second modification to the first embodiment of the present disclosure, the dielectric member 103 thus includes the low relative dielectric constant member 51 that has a relative dielectric constant εrM of more than 1 as the substance M that has a relative dielectric constant εrM of less than 2.
With this structure, for example, the body portion 42 is supported by using the low relative dielectric constant member 51, and the strength of the dielectric member 103 can be increased.
The dielectric member 103 is not limited to a structure in which the low relative dielectric constant member 51 fills the space between the first member 42a and the second member 42b. For example, the first member 42a and the second member 42b may be connected to each other along the plane P, and the low relative dielectric constant member 51 may surround the first member 42a and the second member 42b.
[Third Modification]
Referring to
The structures of the first member 43a and the second member 43b are the same as the structures of the first member 21a and the second member 21b illustrated in
More specifically, the first member 43a and the second member 43b are composed of material that has a relative dielectric constant εrM of about 2 and are connected to each other at a portion through which the reference axis S passes. Consequently, the equivalent relative dielectric constant εre of the portion of the dielectric member 104 through which the reference axis S passes is about 2, and the equivalent relative dielectric constant εre of an outer edge portion of the dielectric member 104 is about 1.
In the lens 201 according to the third modification to the first embodiment of the present disclosure, the body portion 43 includes the first member 43a and the second member 43b that is connected to the first member 43a at the portion through which the reference axis S passes.
With this structure, the strength of the dielectric member 104 can be increased in the case where the body portion 43 includes the members.
Since the dielectric member 104 is composed of the material that has a relative dielectric constant εrM of about 2, the volume of the substance M can be smaller than that in the case where the dielectric member 104 is composed of material that has a relative dielectric constant εrM of about 3. That is, the length of the body portion 43 in the perpendicular direction, that is, the thickness b thereof is less than the distance a illustrated in
[Fourth Modification]
Referring to
The structures of the first member 44a and the second member 44b are the same as the structures of the first member 21a and the second member 21b illustrated in
That is, the first member 44a and the second member 44b are composed of material that has a relative dielectric constant εrM of about 3. The thicknesses h of the first member 44a and the second member 44b decrease stepwise in a direction from the reference axis S toward the outside of the dielectric member 105.
More specifically, the first member 44a and the second member 44b are connected to each other, for example, at a portion at which the distance r from the reference axis S is 0 mm to a predetermined value rx2.
In the portion, a notch 52a is formed in an end portion of the first member 44a opposite the second member 44b. In the portion, a notch 52b is formed in an end portion of the second member 44b opposite the first member 44a. Consequently, the equivalent relative dielectric constant εre of the portion of the dielectric member 105 is about 2.
In the case where the first member 44a and the second member 44b are composed of the material that has a relative dielectric constant εrM of about 3, and the equivalent relative dielectric constant εre of the portion of the dielectric member 105 through which the reference axis S passes is about 2, it is necessary to dispose a substance that has a relative dielectric constant εrM of less than 2 in the portion.
In the dielectric member 105 according to the fourth modification to the first embodiment of the present disclosure, thereforeupon, the notch 52a is formed in the end portion of the first member 44a opposite the second member 44b, and the notch 52b is formed in the end portion of the second member 44b opposite the first member 44a.
With this structure, the equivalent relative dielectric constant εre of the portion of the dielectric member 105 through which the reference axis S passes can be set to about 2, and the strength can be increased by connecting the first member 44a and the second member 44b to each other.
The first member 44a and the second member 44b may be connected by using a coupling member such as a screw. In this case, the depths of the notches 52a and 52b are designed depending on, for example, the size of the coupling member.
The coupling member such as a screw is preferably composed of resin so as not to affect radio waves. In this case, the sizes and depths of the notches 52a and 52b are designed such that the equivalent relative dielectric constant εre of the dielectric member 105 is the desired value in consideration of the relative dielectric constant εrM of the screw.
The coupling member may be composed of material containing metal or metal to ensure sufficient strength. In this case, the coupling member is preferably thin to decrease an influence on radio waves.
[Fifth Modification]
Referring to
The thicknesses hr of the first member 45a and the second member 45b at a position the distance r away from the reference axis S in the horizontal plane continuously decrease in a direction from the reference axis S toward the outside of the dielectric member 106, for example, such that the relationship of expression (4) described above is satisfied, when the relative dielectric constant εrM1 of the air that is the substance M is 1.
In the expression described above, a is the distance between an upper member and a lower member, not illustrated, in the dielectric member 106, R is the radius of the dielectric member 106, and εrM is the relative dielectric constant of material of which the body portion 45 is composed.
The equivalent relative dielectric constant εre of the lens 201 according to the fifth modification to the first embodiment of the present disclosure continuously decreases in the direction from the reference axis S toward the outside of the dielectric member 106.
With this structure, the radio wave radiation direction can be more flexibly set.
The first member 45a and the second member 45b can be manufactured, for example, by grinding a single member consist of resin and having a columnar shape by using a lathe. For this reason, manufacturing is easier than in the case of a dielectric lens disclosed in PTL 1.
Some features according to the first modification to the fifth modification described above can be combined.
Other embodiments of the present disclosure will now be described with reference to drawings. In the drawings, portions like or corresponding to each other are designated by like reference signs, and a description thereof is not repeated.
According to the first embodiment described above, the dielectric member 101 has a plane-symmetrical structure in the perpendicular direction. According to a second embodiment of the present disclosure, however, a dielectric member 111 of an antenna 302 has an asymmetrical structure in the perpendicular direction.
Referring to
The lens 202 includes the dielectric member 111. The dielectric member 111 is, for example, a columnar member and has an upper surface 13 that is defined by an upper member 25 and a lower surface 14 that is defined by a lower member 26.
The upper surface 13 and the lower surface 14 of the dielectric member 111 have, for example, a circular shape that has a radius R of 30 mm.
The dielectric member 111 has an equivalent relative dielectric constant εre that decreases in a direction from the reference axis S that passes through the upper surface 13 and the lower surface 14 toward the outside of the dielectric member 111. The reference axis S passes through, for example, the center of the upper surface 13 and the center of the lower surface 14 and extends in the perpendicular direction.
Referring to
The upper member 25 and the lower member 26 are composed of, for example, material containing metal or metal. A distance a between the upper member 25 and the lower member 26 is, for example, 7.112 mm.
The body portion 24 is composed of material that has a relative dielectric constant εrM of 2 or more, for example, resin that has a relative dielectric constant εrM of 3.
More specifically, the thickness hx of the body portion 24 decreases in a direction from the reference axis S toward the outside of the dielectric member 111, and the volume of the air between the upper member 25 and the lower member 26 consequently increases in the direction from the reference axis S toward the outside of the dielectric member 111.
Consequently, for example, the equivalent relative dielectric constant εre of a portion of the dielectric member 111 through which the reference axis S passes is about 2, and the equivalent relative dielectric constant εre of an outer edge portion thereof is about 1. The equivalent relative dielectric constant εre of the dielectric member 111 changes stepwise from 2 to 1 in the direction from the reference axis S toward the outside of the dielectric member 111.
Specifically, as for a relationship among the relative dielectric constant εrM of the material of which the body portion 24 is composed, the radius R of the dielectric member 111, the distance a between the upper member 25 and the lower member 26, and the thickness hxr of the body portion 24 at a position the distance r away from the reference axis S in the horizontal plane, the thickness hxr is designed so as to approximately satisfy an expression:
hxr=a×(2−(r/R)2−1)/(εrM2−1), (5)
where the relative dielectric constant εrM1 of the air that is the substance M is 1, for example, as in the relationships in the graph G1 and the graph G2 illustrated in
Here, the thickness hx of the body portion 24 changes stepwise in the direction from the reference axis S toward the outside of the dielectric member 111.
More specifically, the body portion 24 includes components 32 that are stacked along the reference axis S. Examples of the components 32 include a disk-shaped member, and the reference axis S passes through the center of a main surface. Here, the body portion 24 includes the eight components 32, that is, components 32a, 32b, 32c, 32d, 32e, 32f, 32g, and 32h.
The components 32a to 32h have the same relative dielectric constant εrM and are stacked in a direction from the lower member 26 toward the upper member 25 in order of the components 32h, 32g, 32f, 32e, 32d, 32c, 32b, and 32a.
The body portion 24 has a conical shape or a truncated cone shape as a whole, and a section that passes through the reference axis S and that is along a YZ plane has a trapezoidal shape or a triangle shape as a whole. The trapezoidal shape includes a shape of a trapezoid that has a stair-like leg portion. Specifically, the radii of the components 32a to 32h are referred to as radii r11 to r18, and the radii r11 to r18 satisfy a relationship in magnitude: r11<r12<r13<r14<r15<r16<r17<r18.
In
The body portion 24 is not limited to being disposed near the lower member 26 and may be disposed near the upper member 25.
The lens 202 may not include the upper member 25, or the lower member 26, or both. In this case, the thickness of the dielectric member 111 is preferably set to a thickness equal to or more than a predetermined value. This predetermined value is a value that enables radio waves that propagate in the radial direction in the dielectric member 111 to pass through the inside of the dielectric member 111 before the radio waves leak out through the upper surface 13 or the lower surface 14 of the dielectric member 111, or both.
In the antenna 302 according to the second embodiment of the present disclosure, the body portion 24 is thus a member that has a conical shape or a conical trapezoidal shape.
With this structure, the radio wave radiation direction of radio waves that are transmitted and received along a plane perpendicular to the reference axis S can be changed.
In addition, the body portion 24 can be manufactured by stacking the components 32, and manufacturing is easier than in the case where both of the first member 21a and the second member 21b are manufactured as in the body portion 21 illustrated in
In addition, the thickness of the outer edge portion of the body portion 24 can be more than that of the body portion 21 illustrated in
[First Modification]
Referring to
The thicknesses of the first member 61a and the second member 61b decrease stepwise in a direction from the reference axis S toward the outside of the dielectric member 112. The first member 61a and the second member 61b are asymmetrical to each other with the plane P centered.
More specifically, the thickness of a portion of the first member 61a at which the distance r from the reference axis S satisfies r=ra (0 mm≤ra≤R) is less than the thickness of a portion of the second member 61b at which the distance r satisfies r=ra.
Also, with this structure, the thickness of the body portion 61 decreases stepwise in the direction from the reference axis S toward the outside of the dielectric member 112. For this reason, the equivalent relative dielectric constant εre of the dielectric member 112 decreases stepwise in the direction from the reference axis S toward the outside of the dielectric member 112.
[Second Modification]
Referring to
The thicknesses of the first member 62a and the second member 62b decrease stepwise in a direction from the reference axis S toward the outside of the dielectric member 113. The first member 62a and the second member 62b are asymmetrical to each other with the plane P centered.
More specifically, the thickness of the first member 62b decreases stepwise at positions at which the distance r from the reference axis S ranges from 0 mm to R. The thickness of the second member 62a decreases stepwise at positions at which the distance r from the reference axis S ranges from 0 mm to rx3 (rx3<R) and is 0 mm at positions at which the distance r ranges from rx3 to R.
Also, with this structure, the thickness of the body portion 62 decreases stepwise in the direction from the reference axis S toward the outside of the dielectric member 113. For this reason, the equivalent relative dielectric constant εre of the dielectric member 113 decreases stepwise in the direction from the reference axis S toward the outside of the dielectric member 113.
[Third Modification]
Referring to
The thicknesses of the first member 63a and the second member 63b decrease stepwise in a direction from the reference axis S toward the outside of the dielectric member 114. The first member 63a and the second member 63b have the same shape.
The first member 63a and the second member 63b have different relative dielectric constants εrM. For example, the relative dielectric constant εrM of the first member 63a is about 2, and the relative dielectric constant εrM of the second member 63b is about 3.
Also, with this structure, the thickness of the body portion 63 decreases stepwise in the direction from the reference axis S toward the outside of the dielectric member 114. For this reason, the equivalent relative dielectric constant εre of the dielectric member 114 decreases stepwise in the direction from the reference axis S toward the outside of the dielectric member 114.
The other structures are the same as those of the antenna 301 according to the first embodiment of the present disclosure described above, and a detailed description is not repeated herein.
The dielectric member 101 according to the first embodiment of the present disclosure described above includes the components 31 that have the same relative dielectric constant εrM and that are stacked along the reference axis S. In a dielectric member 115 according to a third embodiment of the present disclosure, in contrast, components that have different relative dielectric constants εrM are stacked into layers in a direction from the reference axis S toward the outside of the dielectric member 115.
[Structure]
Referring to
The lens 203 includes the dielectric member 115. The dielectric member 115 is, for example, a columnar member and has an upper surface 15 and a lower surface 16.
The thickness of the dielectric member 115 is equal to or more than a predetermined value. This predetermined value is a value that enables radio waves that propagate in the radial direction in the dielectric member 115 to pass through the inside of the dielectric member 115 before the radio waves leak out through the upper surface 15, or the lower surface 16 of the dielectric member 115, or both. That is, since the thickness of the dielectric member 115 is equal to or more than the predetermined value, it is not necessary to dispose, for example, members composed of metal near the upper surface 15 and the lower surface 16 of the dielectric member 115, and the radio waves are prevented from leaking in the vertical direction of the dielectric member 115.
The lens 203 may include an upper member that is disposed near the upper surface 15 of the dielectric member 115, or a lower member that is disposed near the lower surface 16 of the dielectric member 115, or both.
The upper surface 15 and the lower surface 16 of the dielectric member 115 have, for example, a circular shape that has a radius R of 30 mm.
The dielectric member 115 has an equivalent relative dielectric constant εre that decreases in a direction from the reference axis S that passes through the upper surface 15 and the lower surface 16 toward the outside of the dielectric member 115. The reference axis S passes through, for example, the center of the upper surface 15 and the center of the lower surface 16 and extends in the perpendicular direction.
In the dielectric member 115, there is a single kind of substance at the position the distance r away from the reference axis S. For this reason, the equivalent relative dielectric constant εre at the position of the distance r is equal to the relative dielectric constant εrM of the substance at the position of the distance r.
More specifically, the dielectric member 115 includes the components that have different relative dielectric constants εrM and that are stacked in the direction from the reference axis S toward the outside of the dielectric member 115. Specifically, the dielectric member 115 includes a columnar member 71 and annular members 72 as the components. The columnar member 71 is disposed in a portion through which the reference axis S passes.
The number of the annular members 72 is seven. The seven annular members 72 are referred to as annular members 72a, 72b, 72c, 72d, 72e, 72f, and 72g, and the annular members 72a to 72g have a hollow shape and has an annular-shaped section perpendicular to the reference axis S.
The annular member 72a surrounds the outer circumference of the columnar member 71, the annular member 72b surrounds the outer circumference of the annular member 72a, the annular member 72c surrounds the outer circumference of the annular member 72b, the annular member 72d surrounds the outer circumference of the annular member 72c, the annular member 72e surrounds the outer circumference of the annular member 72d, the annular member 72f surrounds the outer circumference of the annular member 72e, and the annular member 72g surrounds the outer circumference of the annular member 72f.
The waveguides 151 are connected to, for example, the annular member 72g.
The descending order of the magnitudes of the relative dielectric constants εrM is the order of those of the columnar member 71, the annular member 72a, the annular member 72b, the annular member 72c, the annular member 72d, the annular member 72e, the annular member 72f, and the annular member 72g. Specifically, the relative dielectric constant εrM of the columnar member 71 is about 2, and the relative dielectric constant εrM of the annular member 72g that forms an outer edge portion of the dielectric member 115 is about 1.
Consequently, the equivalent relative dielectric constant εre of the dielectric member 115 decreases stepwise from 2 to 1 in a direction form the reference axis S toward the outside of the dielectric member 115.
[Manufacturing Method]
Referring to
Subsequently, the operator stacks the columnar member 71 and the annular members 72a to 72g into layers in the direction from the reference axis S toward the outside of the dielectric member 115 (step S22).
The operator disposes the radio wave radiators 221 at positions at which the radio wave radiators 221 face the respective waveguides 151 around the lens 203 in which the columnar member 71 and the annular members 72a to 72g are stacked (step S23).
In the antenna 303 according to the third embodiment of the present disclosure, the dielectric member 115 thus includes the components that have different relative dielectric constants εrM, that is, the columnar member 71 and the annular members 72a to 72g. The columnar member 71 and the annular members 72a to 72g are stacked into the layers in the direction from the reference axis S toward the outside of the dielectric member 115.
The dielectric member 115 can be readily manufactured such that the equivalent relative dielectric constant εre changes by a simple element of stacking the columnar member 71 and the annular members 72a to 72g into the layers.
In the antenna 303 according to the third embodiment of the present disclosure, the thickness of the dielectric member 115 is designed such that the radio waves that propagate in the dielectric member 115 are inhibited from leaking out through the upper surface 15 and the lower surface 16.
With this structure, it is not necessary to dispose, for example, members composed of metal near the upper surface 15 and the lower surface 16 of the dielectric member 115, and the radio waves are prevented from leaking in the vertical direction of the dielectric member 115.
In the method of manufacturing the antenna 303 according to the third embodiment of the present disclosure, the operator first prepares the columnar member 71 and the annular members 72a to 72g that have different relative dielectric constants εrM. The operator manufactures the dielectric member 115 by stacking the columnar member 71 and the annular members 72a to 72g into the layers in the direction from the reference axis S toward the outside described above such that the equivalent relative dielectric constant εre decreases in the direction from the reference axis S that passes through the upper surface 15 and the lower surface 16 of the dielectric member 115 toward the outside of the dielectric member 115.
Since the equivalent relative dielectric constant εre of the lens 203 thus decreases in the direction from the reference axis S toward the outside of the dielectric member 115, the radio wave radiation direction can be readily changed. Since the dielectric member 115 has the upper surface 15 and the lower surface 16, a specific mold, for example, is not needed, and the lens 203 can be readily manufactured unlike the case where a spherical lens is manufactured.
Moreover, the dielectric member 115 can be readily manufactured such that the equivalent relative dielectric constant εre changes by a simple method of stacking the columnar member 71 and the annular members 72a to 72g into the layers.
Accordingly, the method of manufacturing the antenna 303 according to the third embodiment of the present disclosure enables the lens 203 that can change the radio wave radiation direction to be more readily manufactured.
The other structures are the same as those of the antenna 301 according to the first embodiment of the present disclosure described above, and a detailed description is not repeated herein.
The features of the antenna 301 according to the first embodiment of the present disclosure and the first modification to the fifth modification to the first embodiment, the antenna 302 according to the second embodiment and the first modification to the third modification to the second embodiment, and the antenna 303 according to the third embodiment can be appropriately combined.
It should be thought that the embodiments are described above by way of example in all aspects and are not restrictive. The scope of the present invention is not shown by the above description but is shown by the scope of claims and includes all modifications having the same meaning and range as the scope of the claims.
[Additional Remarks]
(A-1) A lens including a dielectric member that has an upper surface and a lower surface and having an equivalent relative dielectric constant that decreases in a direction from a reference axis that passes through the upper surface and the lower surface toward the outside of the dielectric member.
Since the equivalent relative dielectric constant of the lens decreases in the direction from the reference axis toward the outside of the dielectric member as in (A-1) described above, the radio wave radiation direction can be readily changed. Since the dielectric member has the upper surface and the lower surface, a specific mold, for example, is not needed, and the lens can be readily manufactured unlike the case where a spherical lens is manufactured. Accordingly, the lens that can change the radio wave radiation direction can be more readily manufactured.
(A-2) The lens described in (A-1), in which the dielectric member is a columnar member.
With the structure in (A-2) described above, the degree of freedom of a position at which a radio wave radiator can be disposed so as to face a side surface of the dielectric member increases, and the radio wave radiation direction can be consequently changed within an increased range.
(A-3) The lens described in (A-1) or (A-2), in which the dielectric member includes multiple components that have different relative dielectric constants, and the multiple components are stacked into layers in the direction from the reference axis toward the outside of the dielectric member.
The dielectric member can be readily manufactured such that the equivalent relative dielectric constant changes by a simple element of stacking the components into the layers as in (A-3) described above.
(A-4) The lens described in any one of (A-1) to (A-3), in which the thickness of the dielectric member is set such that radio waves that propagate in the dielectric member are inhibited from leaking out through the upper surface and the lower surface.
With the structure in (A-4) described above, it is not necessary to dispose, for example, members composed of metal near the upper surface and the lower surface of the dielectric member, and the radio waves can be prevented from leaking in the vertical direction of the dielectric member.
(A-5) The lens described in (A-1) or (A-2), in which the dielectric member includes a body portion that has a relative dielectric constant of 2 or more, and the thickness of the body portion decreases in the direction from the reference axis toward the outside of the dielectric member.
The dielectric member can be readily manufactured such that the equivalent relative dielectric constant changes because of a simple structure in which the thickness of the body portion decreases in the direction from the reference axis toward the outside of the dielectric member as in (A-5) described above. Since the relative dielectric constant of the body portion is 2 or more, the equivalent relative dielectric constant of a portion of the dielectric member through which the reference axis passes can be set to 2 or more.
(A-6) The lens described in (A-5), in which the body portion is a member that has a conical shape or a conical trapezoidal shape.
With the structure in (A-6) described above, the radio wave radiation direction of radio waves that are transmitted and received along a plane perpendicular to the reference axis can be changed.
(A-7) The lens described in (A-5) or (A-6), in which a portion of the dielectric member other than the body portion contains a substance that has a relative dielectric constant of less than 2.
With the structure in (A-7) described above, the equivalent relative dielectric constant of the dielectric member can be readily changed by changing a volume ratio between the body portion that has a relative dielectric constant of 2 or more and the substance that has a relative dielectric constant of less than 2.
(A-8) The lens described in (A-7), in which the dielectric member includes, as the substance, a member that has a relative dielectric constant of more than 1.
With the structure in (A-8) described above, for example, the body portion is supported by using the member described above, and the strength of the dielectric member can be increased.
(A-9) The lens described in any one of (A-5) to (A-8), in which the lens has an equivalent relative dielectric constant that continuously decreases in the direction from the reference axis toward the outside of the dielectric member.
With the structure in (A-9) described above, the radio wave radiation direction can be more flexibly set.
(A-10) The lens described in any one of (A-5) to (A-8), in which the body portion includes multiple components that are stacked along the reference axis and that have the same relative dielectric constant.
The body portion can be readily manufactured such that the thickness changes by a simple element of stacking the components that have the same relative dielectric constant along the reference axis as in (A-10) described above.
(A-11) The lens described in any one of (A-5) to (A-10), in which the body portion is formed by a cutting process.
With the structure in (A-11) described above, a work such as stacking and sticking members is not needed, the body portion of the dielectric member can be manufactured from an integral component, a manufacturing work can be consequently simplified, and manufacturing costs can be consequently reduced.
(A-12) The lens described in any one of (A-5) to (A-11), in which the body portion includes a first member and a second member that is connected to the first member at the portion through which the reference axis passes.
With the structure in (A-12) described above, the strength of the dielectric member can be increased in the case where the body portion includes the members.
(A-13) The lens described in any one of (A-1) to (A-12), in which the lens further includes an upper member that is disposed near the upper surface of the dielectric member and a lower member that is disposed near the lower surface of the dielectric member.
With the structure in (A-13) described above, radio waves can be prevented from leaking in the vertical direction of the dielectric member.
(A-14) An antenna including a lens that includes a dielectric member and a radio wave radiator that is disposed around the lens, in which the dielectric member has an upper surface and a lower surface and has an equivalent relative dielectric constant that decreases in a direction from a reference axis that passes through the upper surface and the lower surface toward the outside of the dielectric member.
Since the equivalent relative dielectric constant of the lens decreases in the direction from the reference axis toward the outside of the dielectric member as in (A-14) described above, the radio wave radiation direction can be readily changed. Since the dielectric member has the upper surface and the lower surface, a specific mold, for example, is not needed, and the lens can be readily manufactured unlike the case of a spherical lens. Accordingly, the antenna that includes the lens that can change the radio wave radiation direction can be more readily manufactured.
(A-15) The antenna described in (A-14), in which the height of an opening portion of the radio wave radiator is equal to or less than the thickness of the dielectric member.
With the structure in (A-15) described above, a radio wave is inhibited from leaking near the boundary between the radio wave radiator and the dielectric member when the radio wave is radiated from the antenna.
(A-16) The antenna described in (A-14), in which the height of the opening portion of the radio wave radiator is equal to or more than the thickness of the dielectric member.
With the structure in (A-16) described above, a radio wave can be inhibited from leaking near the boundary between the radio wave radiator and the dielectric member when the radio wave is received by the antenna.
(A-17) The antenna described in (A-14), in which the height of the opening portion of the radio wave radiator is equal to the thickness of the dielectric member.
With the structure in (A-17) described above, radio waves can be inhibited from leaking near the boundary between the radio wave radiator and the dielectric member when the radio wave is radiated from the antenna and when the radio wave is received by the antenna.
(A-18) The antenna described in any one of (A-15) to (A-17), in which the opening portion and the dielectric member are coupled with each other with a member that is composed of material that contains metal or metal interposed therebetween.
With the structure in (A-18) described above, a radio wave can be prevented from leaking near the boundary between the radio wave radiator and the dielectric member with more certainty.
(A-19) A device for vehicle including an antenna, in which the antenna includes a lens that includes a dielectric member and a radio wave radiator that is disposed around the lens, and the dielectric member has an upper surface and a lower surface and has an equivalent relative dielectric constant that decreases in a direction from a reference axis that passes through the upper surface and the lower surface toward the outside of the dielectric member.
Since the equivalent relative dielectric constant of the lens decreases in the direction from the reference axis toward the outside of the dielectric member as in (A-19) described above, the radio wave radiation direction can be readily changed. Since the dielectric member has the upper surface and the lower surface, a specific mold, for example, is not needed, and the lens can be readily manufactured unlike the case of a spherical lens. Accordingly, the antenna that includes the lens that can change the radio wave radiation direction can be more readily manufactured.
(A-20) A method of manufacturing a lens that includes a dielectric member, including a step of preparing multiple components that have different relative dielectric constants, and a step of manufacturing the dielectric member by stacking the multiple components into layers in a direction from a reference axis toward the outside such that an equivalent relative dielectric constant decreases in the direction from the reference axis that passes through an upper surface and a lower surface of the dielectric member toward the outside of the dielectric member.
Since the equivalent relative dielectric constant of the lens decreases in the direction from the reference axis toward the outside of the dielectric member as in (A-20) described above, the radio wave radiation direction can be readily changed. Since the dielectric member has the upper surface and the lower surface, a specific mold, for example, is not needed, and the lens can be readily manufactured unlike the case of a spherical lens.
In addition, the dielectric member can be readily manufactured such that the relative dielectric constant changes by a simple method of stacking the components into the layers.
Accordingly, the lens that can change the radio wave radiation direction can be more readily manufactured.
(A-21) A method of manufacturing a lens that includes a dielectric member, including a step of preparing multiple components that have the same relative dielectric constant, and a step of manufacturing the dielectric member by stacking the multiple components along a reference axis such that an equivalent relative dielectric constant decreases in a direction from the reference axis that passes through an upper surface and a lower surface of the dielectric member toward the outside of the dielectric member.
Since the equivalent relative dielectric constant of the lens decreases in the direction from the reference axis toward the outside of the dielectric member as in (A-21) described above, the radio wave radiation direction can be readily changed. Since the dielectric member has the upper surface and the lower surface, a specific mold, for example, is not needed, and the lens can be readily manufactured unlike the case of a spherical lens.
In addition, the dielectric member can be readily manufactured such that the dielectric constant changes by a simple method of stacking the components that have the same relative dielectric constant along the reference axis.
Accordingly, the lens that can change the radio wave radiation direction can be more readily manufactured.
(A-22) A method of manufacturing a lens that includes a dielectric member, including a step of preparing a component and a step of cutting the component such that an equivalent relative dielectric constant decreases in a direction from a reference axis that passes through an upper surface and a lower surface of the dielectric member toward the outside of the dielectric member.
Since the equivalent relative dielectric constant of the lens decreases in the direction from the reference axis toward the outside of the dielectric member as in (A-22) described above, the radio wave radiation direction can be readily changed. Since the dielectric member has the upper surface and the lower surface, a specific mold, for example, is not needed, and the lens can be readily manufactured unlike the case of a spherical lens.
In addition, a work such as stacking and sticking members is not needed, the dielectric member can be manufactured from an integral component, a manufacturing work can be consequently simplified, and manufacturing costs can be consequently reduced.
(B-1) A lens including a dielectric member that has an upper surface and a lower surface, in which
an equivalent relative dielectric constant decreases in a direction from a reference axis that passes through the upper surface and the lower surface toward the outside of the dielectric member,
the reference axis passes through the center of the upper surface and the center of the lower surface and extends in the perpendicular direction,
the dielectric member includes multiple components that are stacked along the reference axis and that have the same relative dielectric constant,
the components are disk-shaped members, and
the reference axis passes through the center of a main surface of each component.
(B-2) An antenna including a lens that includes a dielectric member, and
a radio wave radiator that is disposed around the lens, in which
the dielectric member has an upper surface and a lower surface, and an equivalent relative dielectric constant decreases in a direction from a reference axis that passes through the upper surface and the lower surface toward the outside of the dielectric member,
the lens further includes a waveguide, and
the radio wave radiator is a horn antenna and is disposed at a position at which the radio wave radiator faces the waveguide.
| Number | Date | Country | Kind |
|---|---|---|---|
| JP2018-090595 | May 2018 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2019/017062 | 4/22/2019 | WO |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2019/216181 | 11/14/2019 | WO | A |
| Number | Name | Date | Kind |
|---|---|---|---|
| 3566128 | Arnuad | Feb 1971 | A |
| 4545238 | Kinoshita | Oct 1985 | A |
| 6426814 | Berger | Jul 2002 | B1 |
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