GRADIENT STRUCTURE FOR TRANSMITTING AND/OR REFLECTING AN ELECTROMAGNETIC SIGNAL
20230275355 · 2023-08-31
Inventors
Cpc classification
H01Q15/0013
ELECTRICITY
International classification
H01Q15/00
ELECTRICITY
Abstract
The present disclosure relates to a gradient structure (100) for transmitting and/or reflecting an electromagnetic signal. The gradient structure comprises a plurality of interconnected cells (110). Each cell comprises a through cavity (112) surrounded by walls (111), wherein the walls of each cell have a gradually varying thickness along a longitudinal direction of each cell. The present disclosure also relates to a cover structure (200) comprising the gradient structure (100), a system (300) comprising the cover structure (200), a structure element (400) having integrated therein the system (300) and to a method for optimizing the transmittance and/or reflectance of an electromagnetic signal of a gradient structure.
Claims
1. A gradient structure (100) for transmitting and/or reflecting an electromagnetic signal, comprising a plurality of interconnected cells (110), wherein each cell comprises a through cavity (112) surrounded by walls (111), wherein the walls of each cell have a gradually varying thickness along a longitudinal direction of the cavity of each cell.
2. The gradient structure (100) according to claim 1, wherein each cell (110) is built up of a plurality of layers extending across a longitudinal direction of each cell.
3. The gradient structure (100) according to claim 2, wherein the density is gradually varying in different layers of the cells (110).
4. The gradient structure (100) according to claim 1, wherein the gradient structure is configured to transmit and/or reflect an electromagnetic signal within at least one predetermined bandwidth range.
5. The gradient structure (100) according to claim 4, wherein a thickness of the walls (t.sub.h) of the cells is selected to obtain a permittivity of each layer of the gradient structure such that the gradient structure is transmissive or reflective to an electromagnetic signal, within the at least one predetermined bandwidth range.
6. The gradient structure (100) according to claim 1, wherein the cells (110) of the plurality of interconnected cells have a different diameter (d.sub.cell) and/or geometrical shape.
7. The gradient structure (100) according to claim 1, wherein the cells (110) has a hexagonal shape or any other geometrical shape.
8. The gradient structure (100) according to claim 4, wherein the gradient structure is provided with an additional layer (120), such as a conductive layer, a frequency selective surface, or a skin, which is arranged to transmit, reflect, filter or absorb wavelengths within the at least one predetermined bandwidth range.
9. The gradient structure (100) according claim 8, comprising a plurality of gradient structures arranged on top of each other, wherein the plurality of gradient structures being separated by at least one additional layer (120).
10. The gradient structure (100) according to claim 4, wherein the diameter of each cell (d.sub.cell) is smaller than the smallest wavelength within the at least one predetermined bandwidth range.
11. The gradient structure (100) according to claim 1, wherein the walls (111) of the cells comprises a dielectric material.
12. The gradient structure (100) according to claim 1, wherein the cavity (112) of the cells comprises a dielectric material, which is different from the dielectric material of the walls (111).
13. The gradient structure (100) according to claim 11, wherein each cell (110) further comprises a conductive material, such as a metal or a conductive polymer.
14. The gradient structure (100) according to claim 1, wherein the gradient structure is planar or curved.
15. The gradient structure (100) according to claim 1, wherein the gradient structure is designed as a lens.
16. A cover structure (200) comprising at least a gradient structure (100) according to claim 1, further comprising at least one skin (210a, 210b) attached to the topmost and/or bottommost portion of the gradient structure.
17. The cover structure (200) according to claim 16, wherein the thickness of the walls (111) is selected to obtain a permittivity of each layer of the gradient structure (100) such that reflections in the gradient structure substantially cancel or increase reflections in the gradient structure caused by the skin (210a, 210b).
18. The cover structure (200) according to claim 16, wherein the at least one skin (210a, 210b) is made of a composite material.
19. A system (300) comprising at least one transmitter and/or receiver (310) and a cover structure (200) according to claim 16.
20. A structure element (400) having integrated therein the system (300) according to claim 19, wherein an outer surface of the cover structure (200) forms part of a surface of the structure element.
21. A method (500) for optimizing the transmittance and/or reflectance of an electromagnetic signal of a gradient structure, said gradient structure comprising a plurality of interconnected cells, wherein each cell comprises a through cavity surrounded by walls, wherein the walls of each cell have a gradually varying thickness along a longitudinal direction of the cavity of each cell, said method comprising: selecting at least one bandwidth range (501), within which the gradient structure should transmit and/or reflect the electromagnetic signal, selecting at least one incident angle (502) of a transmitter and/or a receiver arranged within the gradient structure, selecting a thickness of the gradient structure (503), dividing each cell into a plurality of layers (504) extending across a longitudinal direction of the cell, optimizing values of the permittivity (506) for each of the plurality of layers, in order to maximize the performance of the gradient structure, selecting a cell diameter (507) for the cells, wherein the cell diameter is smaller than the smallest wavelength within the at least one bandwidth range, selecting the wall thickness (508) for each layer of the cell such that the permittivity of each of the plurality of layers corresponds to the optimized permittivity values.
22. The method according to claim 21, comprising a step of providing at least one additional layer (505) with a known permittivity, to the topmost and/or bottommost portions of the gradient structure prior to the step of dividing each cell into a plurality of layers.
23. The method (500) according to claim 21, wherein the step of optimizing values (506) of the permittivity is performed by any optimization method, such as the gradient descent projection method.
24. The method (500) according to claim 21, wherein in the step of optimizing values (506) of the permittivity, the transmittance or reflectance of the gradient structure is calculated by a scattering parameter calculation method for stratified media.
25. The method (500) according to claim 21, wherein inverse homogenization is performed in the step of selecting a wall thickness for each layer of the cell (508) such that the permittivity of each of the plurality of layers corresponds to the optimized permittivity values.
26. The method (500) according to claim 21, comprising a step of converting the plurality of layers into a continuous layer (509).
27. The method (500) according to claim 21, further comprising a step of manufacturing the gradient structure and/or optional additional layers by 3D printing (510).
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION
[0066] The present disclosure relates to a gradient structure for transmitting and/or reflecting an electromagnetic signal, a cover structure comprising the gradient structure, a system comprising the cover structure, and a structure element having integrated therein the system. The present disclosure also a method for optimizing the transmittance and/or reflectance of an electromagnetic signal of a gradient structure.
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[0068] As will be discussed below, all the cells 110 of a gradient structure 100 may have the same geometrical shape, such as the gradient structure 100 illustrated in
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[0070] As illustrated in
[0071] In another example, a first portion of a gradient structure 110 may be comprised of cells having a first geometrical shape while a second portion of the gradient structure 100 may be comprised of cells having a second geometrical shape which is different from the first geometrical shape.
[0072] In yet an example, a first portion of the gradient structure 100 may be comprised of cells 110 of a certain cell diameter d.sub.cell while a second portion of the gradient structure 100 may be comprised of cells 110 of a cell diameter d.sub.cell which is different from the cell diameter of the cells of the first portion of the gradient structure.
[0073] In a further example, a first portion of the gradient structure may be comprised of cells of a certain geometric shape and cell diameter, while a second portion of the gradient structure may be comprised of cells 110 of a geometrical shape and cell diameter d.sub.cell which is different from the first portion of the gradient structure 100. By varying the cell diameter d.sub.cell and/or geometrical shape of the gradient structure, different transmissive and/or reflective properties may be obtained in different portions of the gradient structure.
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[0075] In the example shown in
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[0077] Each layer comprises a wall of a certain wall thickness, t.sub.h and thus a cavity of a certain cavity diameter d.sub.cavity. Since the walls of each cell have a gradually varying thickness along a longitudinal direction of each cell, the relation between the amount of material of the walls and the material of the cavity, may vary in each layer of the cell.
[0078] The walls of the cells may comprise a dielectric material. The cavity may comprise a dielectric material, which is different from the dielectric material of the walls. Hence, the walls may comprise a dielectric material which has a different permittivity as compared to the permittivity of the cavity. The dielectric material of the walls and/or of the cavity may be a so-called lossy dielectric material. Alternatively, the dielectric material of the walls may be a so-called loss-less dielectric material. Dielectric loss relates to the inherent dissipation of electromagnetic energy, such as heat, of the material.
[0079] Each layer of the gradient structure thus has a certain permittivity ε, which also may be referred to as a dielectric constant. The permittivity ε of each layer of the cell hence depends on the wall thickness and cavity diameter, hence the relation between the amount of the dielectric material of the walls and the dielectric material of the cavity.
[0080] In one example, the dielectric material of the walls of the cells may be a plastics material, such as nylon.
[0081] In one example, the dielectric material of the cavity may be air. In yet another example, the cavity may comprise a dielectric material which has permittivity which is close to the permittivity of air.
[0082] Air has a relative permittivity which is close to 1.0. In one example, the dielectric material of the walls has a relative permittivity of about 2.8. Hence, a layer having a relative permittivity of 2.8 would comprise only the dielectric material of the walls, i.e. corresponding to a cell without a cavity, while a layer of relative permittivity of 1.0 would correspond to only air, i.e. corresponding to no other material, and thus no cell at all. Thus, a high permittivity in a layer typically corresponds to a thick wall in that layer. As shown in the lower portion of
[0083] The walls of the cells and/or the cavities of the gradient structure 100 may be made of the same dielectric material throughout the gradient structure. Alternatively, the gradient structure 100 may be comprised of more than one materials, for example of different dielectric materials in different layers of the walls and/or cavities of the gradient structure 100.
[0084] Since the thickness of the walls may vary, the density of the gradient structure may gradually vary in different layers of the cells of the gradient structure. In the example shown in
[0085] When transmitting an electromagnetic signal through the gradient structure it is typically desired that there be as little loss of the electromagnetic signal as possible. Alternatively, it may be desired to reflect electromagnetic signals of at least one predetermined bandwidth. However, upon transmission of an electromagnetic signal through the gradient structure, and optional other layers such as skin(s), a loss of the electromagnetic signal occurs due to reflections within the dielectric material and/or within optional other layers. By optimizing the permittivity of each of the layers of the gradient structure, i.e. selecting the thickness of the walls and the diameter of the cavity in each layer, the loss may be controlled and the transmittance and the reflectance of the gradient structure may thus be optimized.
[0086] The thickness of the walls may be selected to obtain a permittivity of each layer of the gradient structure such that the gradient structure is transmissive or reflective to electromagnetic signals within at least one predetermined bandwidth range. The thickness of the walls may be selected with regard to an application of the gradient structure, i.e. with regard to at least one predetermined bandwidth range in which the transmitter/and or receiver operate within as well as the angles of incidence of a transmitter and/or receiver arranged within the gradient structure.
[0087] Typically, the diameter of each cell d.sub.cell may be chosen such that it corresponds to the size of one wavelength or less of an electromagnetic signal within the at least one predetermined bandwidth range. Thereby the gradient structure appears homogeneous to the electromagnetic signal, and grating lobes, i.e. lobes which occur when the lobe from the transmitter is split into a plurality of lobes upon being transmitted through the gradient structure, from the gradient structure is avoided. In another example, the gradient structure may be designed to reflect electromagnetic signals within at least one predetermined bandwidth range by optimizing the permittivity of each of the layers for that purpose. Hence, the gradient structure may be designed such that it is transmissive to electromagnetic signals within at least one predetermined bandwidth range, while being reflective to electromagnetic signals within at least one other predetermined bandwidth range.
[0088] Each cell of the gradient structure may further comprise a conductive material, such as a metal or a conductive polymer. In one example, the conductive material may be a so-called lossy material. The conductive material may be comprised of interconnected conductive elements (not shown) or of isolated conductive elements 123 as shown in
[0089] In yet an alternative, the gradient structure may be provided with an additional layer of a conductive material, such as a frequency selective surface (FSS), which is arranged to transmit, reflect, filter or absorb wavelengths within at least one predetermined bandwidth range. In one example, the frequency selective surface may be provided on the surface of a skin.
[0090] A frequency selective surface typically comprises of a substrate, such as a composite material (e.g. fibreglass laminate), onto which a pattern of a conductive material is added. The pattern may have any shape, for example having the shape of a plus or minus sign, a dot or any other geometrical shape. Two examples of frequency selective surfaces, 120′, 120″ are shown in
[0091] The gradient structure 100 may be arbitrarily shaped depending on its application, for example, the structure may be planar as shown in
[0092] In a further example, the gradient structure may be designed as a lens (not shown). The purpose of such gradient structure may be to focus electromagnetic signals from a transmitter, thereby improving the performance of the transmitter.
[0093] In one example, a plurality of gradient structures may be joined side by side and/or on top of each other. Each of the plurality of gradient structures may have the same cell diameter d.sub.cell and geometrical shape. Alternatively, each of the plurality of gradient structures may have a cell diameter and a geometrical shape which is different from the cell diameter and the geometrical shape of an adjacent gradient structure. In yet an example, the cell diameter and/or geometrical shape may vary also within each gradient structure of the larger gradient structure as discussed above. Further, gradient structures having different wall thicknesses may be joined. In yet an example, especially when a plurality of gradient structures are joined side by side, gradient structures of different shapes, i.e. planar or curved, may be joined together. Gradient structures comprising different dielectric materials may be joined as well.
[0094] A structure comprising a plurality of joined gradient structures on top of each other may further be separated by a continuous or non-continuous layer of at least one additional material, such as a conductive material, a skin or composite material. The conductive layer may be a frequency selective surface as discussed above.
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[0096] Alternatively, a so-called “bonding prepreg” is used which is adhesive and adheres to the surface of the gradient structure. In yet an alternative, the skin(s) is integrated in the gradient structure. In yet an alternative, the skin may be attached to the gradient structure by any fastening means, such as screws and/or rivets. The thickness of the skin(s) may be chosen depending on the application of the cover structure 200. Typically, the thickness of the skin is in the range of 1 mm.
[0097] Upon transmission of electromagnetic signals, reflections typically occur within the skin(s) 210a. 210b. The gradient structure 100 may be designed such that the thickness of the walls 111 may be selected to obtain a permittivity of each layer of the gradient structure such that reflections in the gradient structure substantially cancel the reflections in the gradient structure caused by the skin 210a, 210b. Thereby, the transmittance of the gradient structure is optimized. Alternatively, the gradient structure may be designed such that the thickness of the walls 111 is selected to obtain a permittivity of each layer of the gradient structure 100 such that reflections in the gradient structure increase reflections in the gradient structure caused by the skin 210a, 210b. Thereby, the reflectance of the gradient structure is optimized.
[0098] In
[0099] In
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[0101] The system described above may be integrated in a structure element 400. In such case, an outer surface of the cover structure 200 may form a part of a surface of the structure element. The outer surface of the cover structure may for example be the skin of the cover structure. The structure element 400 may be a portion of a stationary object, such as a portion of a building. Alternatively, the structure element may be a portion of a moving object, such as an aircraft, a road vehicle or a watercraft. For example, the structure element may be a portion of a nose, tail, wing or a side of an aircraft. Further, the stationary object or moving object may comprise a plurality of structure elements which may be arranged at different portions of the stationary or moving object.
[0102] The cover structure of a system may have any shape, i.e. planar, curved etc., which may be adapted to the structure element.
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[0104] The method comprises a step of selecting at least one bandwidth range 501, within which the gradient structure should transmit and/or reflect the electromagnetic signal. The at least one bandwidth range may for example be one large bandwidth or a plurality of independent frequency bands. The at least one bandwidth range may be selected depending on the application of the gradient structure, such as depending on the operating bandwidths of the at least one transmitter and/or receiver arranged within a cover structure comprising the gradient structure.
[0105] The method further comprises a step of selecting at least one incident angle 502 of a transmitter and/or receiver arranged within the gradient structure. The incident angle corresponds to the angle α between the gradient structure and the electromagnetic signal to a receiver and/or from a transmitter arranged within a gradient structure. All angles from signals that the gradient structure is exposed to may be selected.
[0106] The method further comprises a step of selecting thickness of the gradient structure 503. Typically, a minimum and a maximum thickness of the gradient structure may be selected. The minimum value may be selected such that the gradient structure does not become too weak and physically break upon use. The maximum value may be selected depending on the application of the gradient structure, for example such that the gradient structure may not become too thick in a cover structure or a structure element.
[0107] The method further comprises dividing each cell into a plurality of layers 504 extending across a longitudinal direction of the cell. The number of the layers may depend on the thickness of the gradient structure and/or on the limitation of the manufacturing equipment. The numbers of layers may be in the range of ten, but may be either more or fewer than that.
[0108] Thus, the method may further comprise an optional step of providing at least one additional layer 505 with a known permittivity to the topmost and/or bottommost portions of the gradient structure prior to the step of dividing each cell into a plurality of layers. As discussed above, the additional layer may for example be a skin or a conductive layer. Hence, the additional layers may be taken into account in the method of optimizing the transmittance and/or reflectance of an electromagnetic signal. For example, the thickness of the walls may be selected to obtain a permittivity of each layer of the gradient structure 100 such that reflections in the gradient structure substantially cancel or increase reflections in the gradient structure caused by the skin 210a, 210b, depending on if the gradient structure is arranged to transmit or reflect an electromagnetic signal.
[0109] The method further comprises a step of optimizing values of the permittivity 506 for each of the plurality of layers in order to maximize the performance of the gradient structure. As discussed above, also optional additional layers, such as skin(s) and or conductive layer(s), may be taken into account into the step of optimizing values of the permittivity 506. The permittivity of each layer of the gradient structure is optimized such that the performance is maximized for the gradient structure and optional additional layers. Hence, the performance of a cover structure may be optimized by the present method. The permittivity may be optimized in order to maximize the performance for the at least one bandwidth range and incidence angles selected in the steps 501 and 502 above. Any appropriate optimization method may be used. In one example the gradient descent projection method may be used. In the step of optimizing the values, the best value of the permittivity may be selected for each of the layers, i.e. the permittivity providing for the highest transmittance and/or the highest reflectance for the at least one predetermined bandwidth of the gradient structure or for the gradient structure and optional additional layers. The step of optimizing values 506 of the permittivity may be performed by any optimization method, such as the gradient descent projection method. In the step of optimizing values of the permittivity 506, the transmittance or reflectance of the gradient structure may be calculated by a scattering parameter calculation method for stratified media.
[0110] The method further comprises a step of selecting a cell diameter of the cells 507, wherein the cell diameter is smaller than the smallest wavelength within the at least one bandwidth range. The cell diameter is selected such that the gradient structure appears homogeneous to the electromagnetic signal, and grating lobes, i.e. lobes that occur when the lobe from a transmitter is split into a plurality of lobes upon being transmitted through the gradient structure, from the gradient structure is avoided. Hence, it may be desirable that the cell diameter is as small as possible. However, the manufacturing equipment, e.g. a 3D printer, may determine the limit of the smallest cell diameter obtainable.
[0111] The method further comprises a step of selecting the wall thickness 508 for each layer of the cell such that the permittivity of each of the plurality of layers corresponds to the optimized permittivity values. To achieve a wall thickness which gives a permittivity equal to the optimized permittivity, a method called inverse homogenization may be used.
[0112] Division of each cell into a plurality of layers may be efficient for the purpose of optimizing the transmittance/reflectance of the gradient structure. However, upon manufacturing it is not necessary that the layers are a manufactured as sharp layers. Hence, the method may, but need not, comprise a step of converting the plurality of layers into a continuous layer 509 in which the plurality of layers may merge into one another. Hence, in the manufacturing step below, the cells may be manufactured with the plurality of layers extending across a longitudinal direction of the cell as in the optimization steps. Alternatively, the plurality of layers may be manufactured as a continuous layer extending across a longitudinal direction of the cell.
[0113] The method may further comprise a step of manufacturing the gradient structure and/or optional additional layers 510 by 3D printing.
[0114] The gradient structure according to the present disclosure may preferably be manufactured by 3D printing, i.e. additive manufacturing. In the case of the gradient structure being comprised in a cover structure, optional additional conductive materials, additional layer(s) and/or skin(s) of the cover structure may be manufactured by 3D printing as well. In one example, a cover structure comprising at least one gradient structure and at least one skin is printed in one single piece. Alternatively, the different parts, such as the gradient structure, skin(s) and optional additional layers of the cover structure may be printed separately and be joined after printing.