Patent Grant
11431101
The present invention application is a U.S. National Phase filing under 35 U.S.C. § 371 of International Application No. PCT/NZ2021/050003, filed Jan. 15, 2021, which claims priority from New Zealand patent application 760969, filed Jan. 17, 2020. The entire contents of each of these prior applications are hereby incorporated herein by reference.
The present invention relates to artificial dielectric materials comprising conductive elements and focusing lenses made thereof for electromagnetic waves.
Modern mobile communication market needs multi beams antennas creating narrow beams and operating in different frequency bands. Focusing dielectric lens is the main part of the most efficient multi beam antennas. Diameter of a focusing lens has to be several wave length of electromagnetic wave spreading through a lens to create a narrow beam, therefore some lenses of multi beam antennas for mobile communication have diameter more than 1 m. Such lenses made of usual dielectric materials are too heavy, therefore much research was done to create lightweight and low loss lenses providing desirable properties of focusing lenses.
The most well-known lightweight artificial dielectric materials consist of randomly oriented conductive parts mixed with nonconductive parts made of lightweight dielectric material. It is very difficult to manufacture uniform material having desirable dielectric properties by randomly mixing of conductive and nonconductive parts, therefore a focusing lens is the most expensive component of multi-beam antennas. To improve properties and decrease cost of focusing lenses development of such materials is constantly continuing.
U.S. Pat. No. 8,518,537 B2 describes the lightweight artificial dielectric material comprising plurality of randomly orientated small elements of lightweight dielectric material like polyethylene foam containing conductive fibers placed inside of each element.
Patent application US 2018/0034160 A1 describes the lightweight artificial dielectric material comprising plurality of randomly orientated small multilayer elements of lightweight dielectric material containing thin conductive patches between layers. This document describes that such multilayer elements provide more dielectric permittivity than elements containing conductive fibers.
Patent application US 2018/0279202 A1 describes other kinds of the lightweight artificial dielectric material comprising plurality of randomly orientated small elements. One described material includes small multilayer elements of lightweight dielectric material containing thin conductive sheets between layers.
All lightweight artificial dielectric materials mentioned above are made by random mixing of small elements. Elimination of metal-to-metal contacts within the material that could lead to passive intermodulation distortion is needed, therefore manufacturing of such materials comprises many stages and its cost is high.
Randomly mixing provides isotropic properties of a final material consisting of small elements but some applications need dielectric material having anisotropic properties. For example cylindrical lens made of anisotropic dielectric material can reduce depolarization of electromagnetic wave passed through cylindrical lens and improve cross polarization ratio of multi beam antenna (U.S. Pat. No. 9,819,094 B2). The cylindrical lens made of isotropic artificial dielectric material creates depolarization of the electromagnetic wave passed through such lens therefore an antenna comprising such lens can suffer from high cross polarization level.
A lightweight artificial dielectric material providing anisotropic properties and suitable for manufacturing cylindrical lens was described by the NZ patent application 752904, filed Apr. 25, 2019. This material consists of short conductive tubes having thin walls and placed inside of a lightweight dielectric material. Tubes are placed in layers. One layer comprises a sheet of a lightweight dielectric material containing plurality of holes. A lightweight dielectric material can be a foam polymer. Tubes are placed in holes made in a sheet of a lightweight dielectric material and contain air inside. Layers containing tubes are separated by layers of a lightweight dielectric material without tubes. The axes of all conductive tubes are directed in perpendicular from layers.
Such structure could have dielectric permittivity (ε) up to 2.5 for electromagnetic wave spreading along the axes of tubes but its ε is significantly smaller for electromagnetic wave spreading in a perpendicular direction. The reason of such unwanted property of the known artificial dielectric material is the anisotropic property of the tubes.
It is desired to provide an improved light artificial dielectric material for manufacturing such devices as focusing lenses and antennas for radio communication. The provided material has to be simple for manufacturing and have repeatable properties.
In a first aspect of the invention, provided is an artificial dielectric material comprising a plurality of sheets of a dielectric material and a plurality of conductive elements disposed in holes made in the sheets of the dielectric material, wherein each conductive element is a three-dimensional object consisting of side plates connected to a central support and disposed to form conductive surfaces surrounding an empty space.
The side plates may be disposed either perpendicular or non-perpendicular to the support part.
The artificial dielectric material may have at least one surface of the conductive element covered by a dielectric film. Alternatively, at least one surface of the conductive element is covered by a conductive film.
The artificial dielectric material may have holes in the dielectric material which contain projections disposed in the gaps separating the outer parts of the conductive elements.
The artificial dielectric material may have a cruciform slot or a hole in the central support and/or one or more of the side plates.
The axes of the conductive elements of the artificial dielectric material are preferably orientated along at least two different directions, preferably at least two orthogonal directions.
The conductive elements of the artificial dielectric material may have at least two different shapes.
The conductive elements may have a shape of a half of an empty sphere containing slots cutting a surface of the sphere in order to provide side plates.
The dielectric material is preferably a foam polymer, most preferably polyethylene, polystyrene, polypropylene, polyurethane, silicon or polytetrafluoroethylene.
The conductive elements disposed in one layer may form a square lattice providing equal distances between neighboring tubes disposed at the same row or at the same column. Alternatively the conductive elements disposed in one layer may form a honeycomb (hexagonal) lattice providing equal distances between any neighboring elements.
The axes of the conductive elements disposed in one layer may be directed at the same direction. Such axes of the conductive elements disposed in one layer may be directed perpendicular to the layer. Such axes of the conductive elements disposed in one layer may directed parallel to the layer.
The axes of some conductive elements disposed in one layer may be directed perpendicular to the layer and axes of other conductive elements may be directed in parallel to the layer. The axes of the conductive elements directed in parallel to the layer may be directed in different directions.
According to another aspect of the invention, provided is a focusing lens comprising an artificial dielectric material comprising conductive elements according to the invention.
The focusing lens may include layers where the conductive elements of each layer form a sunflower (radial circle) lattice. The focusing lens may include at least one circle of a layer containing conductive elements having axes directed in parallel to the layer and in parallel to the circle. The focusing lens may include at least one circle of a layer containing conductive elements having axes directed in parallel to the layer and perpendicular to the circle.
The focusing lens may include layers with conductive elements having axes directed only perpendicular to the layer and layers containing conductive elements having axes directed only in parallel to the layer.
The focusing lens may include a layer containing conductive elements with axes directed only in parallel to the layer which are directed in perpendicular to axes of the conductive elements of another layer containing the conductive elements with axes directed in parallel to the layer.
The focusing lens may include each layer containing conductive elements with axes directed perpendicular to the layer and conductive elements with axes directed in parallel to the layer.
The focusing lens may include conductive elements with axes directed in parallel to the layer and displaced at even layers which are directed perpendicular to axes of conductive elements directed in parallel to the layer and displaced at odd layers.
The focusing lens may include each layer containing circles of conductive elements having axes directed perpendicular to the layer and circles of conductive elements having axes directed in parallel to the layer.
The focusing lens may include a dielectric rod placed along the longitudinal axis of the focusing lens.
The focusing lens may be cylindrical or may be spherical
Another aspect of the invention provides a method for manufacturing an artificial dielectric material according to the invention, the method comprising placing the conductive elements in a plurality of sheets of a dielectric material, and stacking said sheets together, wherein axes of the conductive elements are orientated along at least two different directions.
In the method, the conductive elements may be placed into pre-existing holes in the sheets of the dielectric material.
In the method the sheets of the dielectric material containing the conductive elements may be separated by sheets of the dielectric material without conductive elements.
The sheets of the dielectric material containing the conductive elements may comprise holes which do not pass through the thickness of the sheet.
The method may include the step of bending the outer parts of the conductive elements at the time of being placed into the sheets of the dielectric material.
Another aspect of the invention provides a conductive element for use in an artificial dielectric material, the element comprising side plates connected to a central support, disposed to form conductive surfaces surrounding an empty space.
The side plates may be disposed either perpendicular or non-perpendicular to the support part.
The side plates may be connected at the outer region of the central support.
A further aspect of the invention provides a method of focusing a radio wave using a focusing lens according to an embodiment of the invention.
By providing the above artificial dielectric material, the invention goes at least some way to overcoming deficiencies of the known lightweight artificial dielectric materials and to provide a light artificial dielectric material providing less dependence from direction and polarization of electromagnetic waves spreading through the material.
An electromagnetic wave propagating through an artificial dielectric material comprising conductive elements excites circular currents flowing on the conductive elements, therefore permeability of such materials is less than 1. This effect was described many years ago (W. E. Kock Metallic delay lenses.//Bell System Technical Journal, v.27, pp. 58-82, January 1948). When an electromagnetic wave propagates through a square or hexagonal lattice of conductive tubes in a direction along the axes of the tubes, delay coefficient (n) does not depend on polarization since any polarization excites the same circular currents. When an electromagnetic wave propagates through square or hexagonal lattice of conductive tubes in direction perpendicular the axes of the tubes n does depend on polarization. The biggest circular currents flow on a wall of the conductive tube in a direction perpendicular to axis of the conductive tube when a magnetic field of an electromagnetic wave is directed in parallel to the axis of the conductive tube. As a result, permeability for such polarization is significantly less than for other polarizations and delay coefficient n is also less than n for other polarizations. It is possible to increase delay coefficient n for such polarization by decreasing distance between the tubes disposed in a layer. Increasing capacity between the tubes disposed in the layer increases permittivity of the artificial dielectric material. As a result the known artificial dielectric material can provide very small difference between n for any polarization of electromagnetic wave spreading in a direction perpendicular to the axes of the conductive tubes but cannot provide the same n for other directions of electromagnetic wave.
Because n depends on the angle between the direction of an electromagnetic wave crossing the material and axes of the tubes, such artificial dielectric material does not suit for many applications requiring an isotropic dielectric material providing the same value of n for any direction and polarization of electromagnetic wave. For example spherical Luneburg lenses have to be made of isotropic dielectric material having the same n for any direction and polarization of electromagnetic wave to keep polarization of an electromagnetic wave passing through spherical lens. Therefore a need exists to create the artificial dielectric material providing less dependence n from direction and polarization of electromagnetic wave crossing the material in compare with the known material described by the NZ752904. At the same time manufacturing of such material has to be simpler than manufacturing of known lightweight artificial materials made by randomly mixing of small elements containing conductive elements isolated from each other.
The focusing properties of an artificial dielectric material such as a tube depend on delay coefficient n=√{square root over (εμ)} where μ is magnetic permeability.
As an electromagnetic wave passes through the known lightweight artificial dielectric material this excites currents in the conductive material and μ of such material is less than 1. The biggest circular currents flow on a wall of a conductive material such as a tube in a direction perpendicular to the axis of a conductive tube when the magnetic field of electromagnetic wave is directed in parallel to axis of a conductive tube. As a result μ for such polarization is less than for other polarizations and delay coefficient n is also less than for other polarizations. Artificial dielectric materials containing short tubes suffer from such effect, therefore it is needed to find other shapes of conductive elements to increase μ and delay coefficient n.
The artificial dielectric material according to the invention provides a light artificial dielectric material having less dependence on direction and polarization of electromagnetic waves spreading through the material.
In further describing the invention, reference is made to the accompanying drawings by way of example only in which:
Throughout the Figures, sectional lines A-A are used to indicate sections in corresponding drawings of the same set. For example, the section indicated in
As described and shown in the figures, the artificial dielectric material includes a plurality of conductive particles, described herein as conductive elements, disposed in holes made in sheets of a lightweight dielectric material. Each conductive element is a three-dimensional object consisting of thin parts (described herein as side plates) directly connected to the middle part (described herein as a central support) and forming an outer contour of the conductive element surrounding an empty space formed inside of the conductive element. Typically, the conductive element is made from a piece of a suitably conductive metal such as aluminium which is bent into the required shape. The metal may alternatively be copper, nickel, silver or gold.
Alternatively, a thin sheet of a lightweight resilient dielectric material formed into a required shape may be coated with a thin layer of conductive material in order to form the conductive element.
Some embodiments of the conductive element comprise a central support disposed at a horizontal plane and side plates connected to the outer contour or region of the central support and disposed at other planes turned by 30-90 degrees from the horizontal plane for example. Thus the relationship between the central support and the side plates may be perpendicular or non-perpendicular. The outer contour of the central support could be a polygon for example triangle, square, hexagon or octagon. The central support could contain holes. In the examples shown in the figures, the outer contour is typically shown as hexagonal by way of example only.
Other embodiments of the conductive element may include side plates which are not flat and are more robust than conductive elements having flat side plates. For example, the conductive element could be a half of an empty sphere having slots disposed across its diameter as shown in
The conductive elements are placed in layers. One layer comprises a sheet of the lightweight dielectric material containing plurality of holes filled by the conductive elements. The lightweight dielectric material can be a foam polymer. The foam polymer is preferably made of a material selected from polyethylene, polystyrene, polypropylene, polyurethane, silicon and polytetrafluoroethylene. The layers containing conductive elements are separated by layers of a dielectric material without conductive elements. The separating layers could be a foam polymer or a thin dielectric film. The separating layers also could contain holes having smaller diameter than diameter of holes for conductive elements to provide air ventilation through the lightweight dielectric material.
Two samples of the artificial dielectric material were manufactured to compare properties of proposed and known material. The first sample was made of the known material containing short conductive tubes shown in
The measured sample of the artificial dielectric material in accordance with the present invention has μ=0.85 since circular currents cannot flow on side plates 2 separated by gaps when magnetic field of electromagnetic wave is directed in parallel to an axis of the conductive element and flow on the central support 1 only as it is shown in
Difference of properties is smaller when magnetic field of electromagnetic wave is directed in perpendicular to an axis of a conductive tube and the conductive element. The measured sample of the known artificial dielectric material has μ=0.83.
Both materials have almost the same c therefore the artificial dielectric material in accordance with the present invention has a bigger delay coefficient n and its dependence from polarization of electromagnetic wave is smaller.
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
Alternatively, the conductive material may be similarly coated with a film or thin layer of a dielectric material in order to form a conductive element having a similar structure to that depicted in
Another embodiment of the present invention is shown in
The conductive elements placed in neighboring layers could be disposed above each other on the same axes. Neighboring layers could be shifted from each other and then the conductive elements placed in neighboring layers have different axes.
The conductive elements could be disposed with different orientations of axes. Axes of some conductive elements are directed perpendicular to the layers and axes of other conductive elements are directed in parallel to the layers. The conductive elements having axes directed in parallel to the layers could have disposition of axes perpendicular to each other. Thus the axes of the conductive elements may have three orthogonal directions. As a result dielectric properties of the artificial dielectric material according to the invention are less dependent on direction and polarization of electromagnetic wave crossing the material.
The conductive elements placed in one layer could have the same orientation of axes or different orientation. Layers containing conductive elements placed above each other could have the same structure or different structures. Differing layers may include different spacing of conductive elements in the respective layers. For example, adjacent layers or sheets of the same size may with the conductive elements arranged in radial circles may have differing numbers of radial circles in order to increase the distance between the circles. Similarly, for honeycomb lattice arrangements, distances between adjacent conductive elements in the same layer may be varied.
Properties of the provided artificial dielectric material depend on orientation of the conductive elements and distances between these and between the layers. Therefore the provided artificial dielectric material comprising conductive elements having different orientation of axes in a layer and layers with different structures provides opportunity to reach desirable dielectric properties compared with known materials. For example it is possible to decrease dependence of delay coefficient n from direction and polarization of electromagnetic waves passing through the provided artificial dielectric material. As a result the provided artificial dielectric material can be applied for manufacturing of many kinds of focusing lenses and antennas.
Several embodiments of the present invention are shown in
Conductive elements having other shapes such as shown in
Several embodiments of a cylindrical lens and layers which may form it made of the artificial dielectric material according to the invention are described below.
The conductive elements placed in one layer may form various lattices of conductive elements in order to adopt suitable properties. These include a square structure (lattice) providing equal distances between neighboring conductive elements disposed at the same row or at the same column as shown in
Additionally, the holes in the dielectric material may be made so that the conductive elements may penetrate both sides of the layer. In this case, the sheets containing conductive elements are separated by intermediate sheets of dielectric material not containing conductive elements.
For other applications and end use requirements, the conductive elements placed in a layer could form other structures, and lenses may comprise other quantities and variety of different layers.
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in in
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
Another embodiment of the present invention is shown in
The above described cylindrical lenses contain the conductive elements shown in
A group of focusing lenses which could be created of the provided artificial dielectric material is not limited by described above embodiments. Layers of focusing lenses could be formed by other structures also. For example by the structures shown in
Such spherical lens can effectively form a beam having a 20-40 degree half power beam width. Large spherical lenses forming narrower beams have increased distances between the conductive elements towards the outer contour of the sphere.
The invention also relates to a method for manufacturing artificial dielectric materials which may be in turn used in the production of lenses comprised of multiple layers of the artificial dielectric materials. The method involves placing conductive elements in holes in a plurality of sheets of a dielectric material, and stacking said sheets together, wherein the sheets of the dielectric material containing the conductive elements are separated by sheets of the dielectric material without the conductive elements, and wherein axes of the conductive elements are orientated along at least two different directions. As an alternative, the sheets not containing the dielectric material may be omitted and the sheets containing the conductive element may have holes which do not pass through the thickness of the sheet. In such manner, the conductive elements of each layer may be kept separated as is desired.
The conductive elements may be placed into pre-existing holes in the sheets of the dielectric material. Further, the manufacturing process may require that the outer parts of the conductive elements are bent at the time of being placed into pre-existing holes in the sheets of the dielectric material. Alternatively, conductive elements which have been pre-formed into their required shape may be placed into the holes at the time of assembly.
The invention also relates to a method of focusing a radio wave using a focusing lens according to the invention. Such lens may be spherical or cylindrical or may have another geometry. Use of such a focusing lens comprising the artificial dielectric material and conductive elements according to the invention allows focusing of radio waves with less dependence on direction and polarization of electromagnetic waves.
While some preferred aspects of the invention have been described by way of example, it should be appreciated that modifications and/or improvements can occur without departing from the scope of the invention as claimed in this specification.
The terms comprise, comprises, comprising or comprised, if and when used herein, should be interpreted non-exclusively, that is, as conveying “consisting of, or including”.
It is to be understood that, if any prior art publication is referred to herein, such reference does not constitute an admission that the publication forms a part of the common general knowledge in the art, in New Zealand or any other country.
| Number | Date | Country | Kind |
|---|---|---|---|
| 760969 | Jan 2020 | NZ | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/NZ2021/050003 | 1/15/2021 | WO |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2021/145780 | 7/22/2021 | WO | A |
| Number | Name | Date | Kind |
|---|---|---|---|
| 9123998 | LoRe | Sep 2015 | B1 |
| 11075452 | Crouch | Jul 2021 | B2 |
| 20100066639 | Ngyuen et al. | Mar 2010 | A1 |
| 20110003131 | Matitsine | Jan 2011 | A1 |
| 20120146881 | McKinzie, III | Jun 2012 | A1 |
| 20130002253 | Werner et al. | Jan 2013 | A1 |
| Entry |
|---|
| International Search Report in International Application No. PCT/NZ2021/050003, dated Mar. 11, 2021. |
| Written Opinion in International Application No. PCT/NZ2021/050003, dated Mar. 11, 2021. |
| International Preliminary Report on Patentability in International Application No. PCT/NZ2021/050003, dated Aug. 13, 2021. |
| Number | Date | Country | |
|---|---|---|---|
| 20220209418 A1 | Jun 2022 | US |
