JP5878260B2 - Radio wave absorber - Google Patents

Description

  The present invention relates to a radio wave absorber, and more particularly to a radio wave absorber having excellent absorption performance with respect to an oblique incident wave.

  In recent years, there are many electromagnetic wave generation sources such as electronic devices, communication devices, and information systems in everyday life, and various electromagnetic waves are radiated. Therefore, there is a possibility that a plurality of devices influence each other due to electromagnetic waves generated from the devices. In order to allow various devices to coexist in such an environment, a so-called EMC (Electro-Magnetic Compatibility) measure is required to prevent the devices from affecting each other.

  Evaluation of EMC in the equipment is performed in a measurement room called an anechoic chamber. The outer wall of the anechoic chamber is covered with a metal plate in order to prevent the entry of external electromagnetic waves into the dark room and the release of electromagnetic waves generated from the measuring device in the dark room. In order to prevent unnecessary reflection of electromagnetic waves, a radio wave absorber made of a lossy material is provided on the wall surface in the dark room.

  As this radio wave absorber, a material in which a plurality of loss materials formed into a quadrangular pyramid shape are arranged (see FIG. 1) or a material in which a plurality of loss materials formed in a wedge shape (see FIG. 2) are arranged (see FIG. 2) is used. I came. However, in the electromagnetic wave absorber having such a shape, the absorption performance with respect to the perpendicular incident wave incident from the tip of the cone or the wedge toward the bottom is good, while the oblique incident on the side of the cone or the wedge is good. The problem is that the absorption performance for incident waves is inferior to that for normal incident waves.

  Therefore, in Patent Document 1, a base made of a dielectric loss material having a triangular prism shape and an upper surface of the base (any two surfaces excluding two opposing surfaces among the five surfaces constituting the triangular prism) are spread. A radio wave absorber comprising a radio wave introduction portion made of a dielectric loss material having a quadrangular pyramid shape has been proposed. In this radio wave absorber, a rectangular pyramid with the same height is placed on the slope of the triangular prism (upper surface of the base), and the entire radio wave absorber has a wedge shape, thereby enhancing the radio wave scattering effect and oblique incidence. It is intended to improve the wave absorption performance.

JP-A-8-274490

  However, there is still room for improvement in the absorption performance against oblique incident waves. In other words, even if the radio wave scattering effect is enhanced by making the entire radio wave absorber in the shape of a wedge as described above, the absorption performance as expected cannot be obtained on the side of the radio wave introduction part having a quadrangular pyramid shape. I understood.

  In recent years, there has been a demand for a smaller and higher performance anechoic chamber, and there is a demand for a radio wave absorber that is superior in its ability to absorb obliquely incident waves. Accordingly, an object of the present invention is to provide a radio wave absorber having better absorption performance with respect to an oblique incident wave.

  The inventors have intensively studied about the means for solving the above problems, and in order to increase the absorption of radio waves also on the side surface of the radio wave absorber, it is important to gently change the impedance on the side surface. The inventors have newly found that it is most effective to use a radio wave absorber as a hexagonal pyramid, and have completed the present invention.

The gist of the present invention is as follows.
(1) A radio wave absorber according to the present invention includes a hexagonal pyramid made of a lossy material and a hexagonal column connected to a bottom surface of the hexagonal pyramid and made of a lossy material and having a bottom surface having the same shape as the bottom surface. A plurality of composites to be arranged without gaps on the bottom surface of the hexagonal column body, and the height of each hexagonal column body constituting the complex is stepwise different for each row, or The height of each of the composites is similarly different in stages by increasing concentrically in a stepwise manner toward the center.
The radio wave absorber of the present invention having such a configuration has excellent absorption performance with respect to an oblique incident wave.

(2) In the radio wave absorber of the present invention, the shape of the bottom surface of the hexagonal pyramid is preferably a convex hexagon.

  According to the present invention, it is possible to provide a radio wave absorber having excellent absorption performance with respect to an oblique incident wave.

It is a perspective view which shows an example of the conventional electromagnetic wave absorber. It is a perspective view which shows another example of the conventional electromagnetic wave absorber. A is a perspective view of a hexagonal pyramid 10 constituting a radio wave absorber according to an embodiment of the present invention, and B is a bottom view thereof. FIGS. 8A to 8C are diagrams illustrating the absorption performance with respect to the oblique incident wave β ₁ for the conventional radio wave absorber of FIG. 1. It is a schematic diagram of the anechoic chamber using the conventional electromagnetic wave absorber. AD is a figure explaining the absorption performance with respect to the oblique incident wave (beta) ₁ about the hexagonal pyramid 10 which comprises the electromagnetic wave absorber by one Embodiment of this invention. A and B are figures explaining the effect at the time of arranging two or more hexagonal pyramids 10 which constitute the wave absorber by one embodiment of the present invention. A and B are figures explaining the subject at the time of arrange | positioning the conventional electromagnetic wave absorber of FIG. 1 in multiple rows. A and B are figures explaining the effect at the time of arranging a plurality of hexagonal pyramids 10 constituting the radio wave absorber according to one embodiment of the present invention. It is a perspective view of the composite_body | complex which comprises the electromagnetic wave absorber 100 by one Embodiment of this invention. It is a perspective view of the electromagnetic wave absorber 110 by other embodiment of this invention. It is a perspective view of the electromagnetic wave absorber 120 by further another embodiment of this invention. A and B are diagrams illustrating a radio wave absorber 130 according to still another embodiment of the present invention. A and B are diagrams illustrating the radio wave absorbers 110, 120, and 130. It is a perspective view of the electromagnetic wave absorber 200 by further another embodiment of this invention. It is a figure explaining the electromagnetic wave absorber 210 by further another embodiment of this invention. It is a bottom view of the electromagnetic wave absorber of the present invention.

Hereinafter, the radio wave absorber according to the present invention will be described by exemplifying embodiments thereof.
In FIG. 3, the structure of the hexagonal pyramid 10 which comprises the electromagnetic wave absorber which concerns on one Embodiment of this invention is shown. FIG. 3A is a perspective view of the hexagonal pyramid 10, and FIG. 3B is a bottom view of the hexagonal pyramid 10.
The radio wave absorber of the present invention is characterized in that it includes a hexagonal pyramid 10, and the reason why the hexagonal pyramid 10 is provided will be described below in comparison with a conventional quadrangular pyramid radio wave absorber.

4A is a perspective view of a quadrangular pyramid 40 constituting the conventional radio wave absorber shown in FIG. 1, and FIG. 4B is a plan view thereof. An arrow α in the figure is an incident wave incident from the front end 44 of the quadrangular pyramid 40 toward the bottom surface, that is, a vertical incident wave α along the Z-axis direction in the figure, and an arrow β ₁ is the quadrangular pyramid 40. The oblique incident wave β ₁ toward the side surface 43 of FIG.

FIG. 4C schematically shows the amount of change in impedance with respect to the air in the Z-axis direction in the figure for the quadrangular pyramid 40. Here, it is shown that the amount of change in impedance increases from light to dark. Since the magnitude of the impedance is based on the volume of the radio wave absorber, as shown in FIG. 4C, when the projected shape of the side surface of the polygonal pyramid is a triangle, the amount of change in impedance tends to increase from the top toward the bottom. It is in. Accordingly, in the normal incident wave α, the radio wave is directed from the portion where the amount of change in impedance with respect to the air is the smallest, that is, from the tip 44 of the quadrangular pyramid toward the larger impedance, and thus, good absorption performance can be obtained. . On the other hand, since the oblique incident wave β ₁ is incident on the middle part of the quadrangular pyramid 40 having a large impedance change amount with respect to the air, the radio wave is reflected due to a sudden change in impedance, which is sufficient. It is difficult to obtain a good absorption performance

That is, a part of the oblique incident wave β ₁ that is not absorbed by the quadrangular pyramid 40 is reflected to the incident side as shown in FIG. 4A, and a reflected wave γ ₁ is generated. FIG. 5 schematically shows an example in which the radio wave absorber made of the quadrangular pyramid 40 is spread on the floor surface, wall surface, ceiling surface, etc. of a miniaturized anechoic chamber. In a miniaturized anechoic chamber, for example, the chance that a part of the radio wave transmitted from the transmitting antenna to the receiving antenna is incident on the radio wave absorber obliquely increases. In this case, radio wave transmitted from the transmitting antenna is reflected by the side surface of the quadrangular pyramid body occurs reflected wave gamma _1, the reflected wave gamma ₁ is again reflected by the wall surface of the other of the four pyramids reflection As a result of the reflected wave reaching the receiving antenna side after a plurality of reflections (two times in the example of FIG. 5) such that the wave γ ₂ is generated, only the direct wave from the transmitting antenna cannot be measured.

On the other hand, FIG. 6A is a perspective view of a hexagonal pyramid 10 constituting a radio wave absorber according to an embodiment of the present invention, and FIG. 6B is a plan view thereof. A hexagonal pyramid 10, the side receiving the incident of the oblique incident waves beta _1, because it has many side 5 than conventional four pyramids, it is possible to enhance the absorption performance against oblique incident wave beta _1. The reason will be described below with reference to FIG. 6C.

FIG. 6C is a diagram schematically showing the amount of change in impedance of the hexagonal pyramid with respect to the air along the Z-axis and the X-axis in the cross section cut along the line AA in FIG. 6A. Here, as in FIG. 4C, the amount of change in impedance increases from a light color to a dark color. The side 5 of the hexagonal pyramid is an edge, the volume of the loss material is relatively small like the tip 4, and the amount of change in impedance with respect to air is also small. Therefore, the oblique incident wave β ₁ incident on the side 5 is similar to the case where the vertical incident wave α is incident on the tip 4 from the portion closest to the impedance of the air, that is, from the side 5 side of the hexagonal pyramid. The radio wave is directed to the one where the amount of change in impedance with respect to the signal is large. Therefore, in the hexagonal pyramid 10 constituting the radio wave absorber according to the present embodiment, the absorption performance with respect to the oblique incident wave β ₁ can be remarkably improved as compared with the conventional _one .

The action and effect relating to the impedance described above are not limited to the oblique incident wave β ₁ incident on the side 5 of the hexagonal pyramid. For example, the oblique incident wave incident on the side surface 3 of the hexagonal pyramid. The same can be said for β ₂ (see FIGS. 6B and 6D). That is, in this case, as shown schematically in FIG. 6D, the amount of change in impedance with respect to the air of the hexagonal pyramid along the Z-axis and the X-axis in the cross section cut along the line BB in FIG. The change in impedance with respect to the air on the outer surface side of 3 is gentler than that of the side surface 43 of the quadrangular pyramid 40, so that reflection of radio waves can be reduced. Therefore, in a hexagonal pyramid 10 constituting the electromagnetic wave absorber according to the present embodiment, as in the case where the edge 5 of a hexagonal pyramid is obliquely incident wave beta ₁ is incident, obliquely incident wave incident on the side surface 3 beta good absorption performance can be obtained for the _two.

Furthermore, in the hexagonal pyramid 10 constituting the radio wave absorber according to the present embodiment, when a plurality of hexagonal pyramids 10 are used side by side, the absorption performance can be further improved.
For example, in FIG. 7A, a plurality of hexagonal pyramids 10 (three in the illustrated example) are arranged in series with one side of the base 2 of each hexagonal pyramid (see FIGS. 3A and 3B) adjacent to each other. In this arrangement, an uneven surface is continuously formed by the six side surfaces 3 of the three hexagonal pyramids in the longitudinal direction of the arrangement (Y-axis direction in the drawing). In this way, on the uneven surface formed facing the incident direction of the radio wave, the reflected wave γ ₁ of the incident wave β ₁ is scattered between the side surfaces 3 of the hexagonal pyramid 10 and absorbed by the surrounding radio wave absorber. can do. Specifically, the reflected wave γ ₁ of the incident wave β ₁ incident on the hexagonal pyramid 10b in FIG. 7 can be absorbed by the hexagonal pyramids 10a and 10c adjacent to the hexagonal pyramid 10b. Therefore, radio wave absorption performance can be enhanced. Note that the lines and the like indicating the incident wave and the reflected wave illustrated in FIGS. 7A and 7B are examples.

On the other hand, although not shown, when three conventional quadrangular pyramids 40 are arranged in series with their bases adjacent to each other, the incident surface of the radio wave is a uniform plane, so the reflected wave in a certain quadrangular pyramid γ ₁ cannot be absorbed by other adjacent wave absorbers.

As shown in FIG. 7B, for example, the three hexagonal pyramids 10 may be arranged in series with only the apexes of the bottom surfaces 1 in contact with each other. In this case, the absorption effect of the reflected wave γ ₁ is inferior to that in the case shown in FIG. 7A, but is superior to the case where the conventional quadrangular pyramids 40 are arranged in series.

Furthermore, when three or more hexagonal pyramids 10 are arranged in two or more rows and used, the radio wave absorption performance can be further enhanced.
Conventionally, radio waves from all directions are incident on a radio wave absorber in an anechoic chamber. At this time, as shown in FIG. 8A, when each of the radio wave absorbers arranged in two rows is a quadrangular pyramid, a trough V where the thickness of the loss material formed between adjacent quadrangular pyramids is zero. The radio waves incident on the are easily reflected. On the other hand, when three or more hexagonal pyramids 10 are arranged and used in two or more rows, it is possible to suppress the reflection of radio waves in the valley V.

Here, with reference to FIG. 8, the reflection at the valley portion V will be described by taking the oblique incident wave β ₁ along the X-axis direction and the oblique incident wave β ₂ inclined at 45 ° with respect to the X-axis direction.
First, as shown in FIG. 8A, in the form in which four quadrangular pyramids 40 are arranged in two rows of two, the valley V does not exist in the incident direction of the oblique incident wave β ₂ , while the oblique incident wave The valley V continues in the incident direction of β ₁ . In this case, since the oblique incident wave β ₁ passes through the valley V or is reflected by the valley V where the thickness of the loss material is zero, radio wave absorption is inefficient. Further, as shown in FIG. 8B, when the arrangement of the quadrangular pyramid 40 is rotated by 45 ° so that the valley V is not arranged in the incident direction of the oblique incident wave β ₁ , the incidence of the oblique incident wave β ₂ is now performed. The valley V continues in the direction, and the radio wave absorption of the oblique incident wave β ₂ becomes inefficient. That is, when the conventional square pyramids 40 are arranged in a plurality of rows, wide valleys V are always continuously formed in two directions as shown in FIG.

On the other hand, as shown in FIG. 9A, in the form in which the three hexagonal pyramids 10d, 10e, and 10f are arranged in two rows with the sides 2 adjacent to each other, the incident directions of the oblique incident waves β ₁ and β ₂ The valleys are not continuously formed. Even if the oblique incident wave β ₁ is incident between the hexagonal pyramids 10d and 10e, it can be absorbed by the hexagonal pyramids 10f arranged adjacent to these. Further, as shown in FIG. 9B, the same can be said for a form obtained by rotating the above form by 45 °.

As described above, when three or more hexagonal pyramids 10 are arranged and used in two or more rows, since there is no portion where valleys V are continuous over 360 °, radio wave absorption is made more efficient, and radio wave absorption performance is further improved. Can be increased.
Incidentally, as appropriate, the height of a hexagonal pyramid H ₁₀ (see FIG. 3A) may be arranged to be different columns from each other. Further, the hexagonal pyramids may be arranged such that the height H ₁₀ of the hexagonal pyramid is concentrically different and is highest at the center of the circle. In accordance with the size and shape of the anechoic chamber, by appropriately adjusting the height H ₁₀ of a hexagonal pyramid, it is possible to increase the electromagnetic absorption performance.

The operation and effect of the radio wave absorber 10 including the hexagonal pyramid according to the embodiment of the present invention has been described above. Thus, if only one polygonal pyramid is considered, for example, even when a hexagonal pyramid other than a hexagonal pyramid such as a heptagonal pyramid or an octagonal pyramid is applied, the same effect as the hexagonal pyramid is expected. be able to. However, in an actual anechoic chamber, it is necessary to install a plurality of polygonal pyramids with no gaps, and hexagonal pyramids are the most suitable as the polygonal pyramids that can be installed without gaps.
Further, when the number of vertices of the polygonal cone increases, the interior angle of the polygonal pyramid at the vertex increases and approaches a conical shape. In this case, the hexagonal pyramid is the most appropriate because the attenuation effect of the impedance at the side 5 is reduced.

In addition, it is preferable that the shape of the bottom face 1 of the hexagonal pyramid of this invention is a convex hexagon.
With reference to FIG. 3B, a convex hexagon is a hexagon in which all internal angles θ are less than 180 °. More strictly speaking, even if any side of the hexagon is extended, the extension line is A hexagon that does not extend inside the hexagon. In this case, the effect of radio wave absorption can be improved.

Furthermore, FIG. 10 is a composite P constituting the radio wave absorber 100 according to an embodiment of the present invention. This composite P is formed by connecting a hexagonal column 12 made of a lossy material having a bottom having the same shape as the bottom 1 to the bottom 1 of the hexagonal pyramid 10 described above.
According to this configuration, even in the valley V of the absorber, the absorption performance is improved because the thickness of the loss material does not become zero.

  In addition, the composite P can be used by arranging a plurality thereof in series, or three or more of them can be used in two or more rows. In this case, the same reason as described above for the hexagonal pyramid 10 is used. Therefore, the radio wave absorption performance can be further improved.

In addition, the radio wave absorber according to the present embodiment is formed by arranging a plurality of composites P such that the heights H ₁₂ of the hexagonal column bodies 12 constituting the composite P are different from each other in the rows. For example, in the radio wave absorber 110 shown in FIG. 11, a plurality of composites P are arranged in three rows along the X-axis direction, but the height of the hexagonal column body 12 for each row S _{1 to} S _3. H ₁₂ is different. More specifically, the height H ₁₂ of the hexagonal column body 12 of the composite P ₁ arranged in the front row S ₁ is the lowest, the height H ₁₂ of the composite P ₃ arranged last column S ₃ is highest.

As described above, when the columns S ₂ and S ₃ having the high height H ₁₂ of the hexagonal columnar body 12 are provided behind the column S ₁ having the lowest height H ₁₂ of the hexagonal column 12, the light enters the back of the column S _1. Since a wave shielding wall is formed, a more efficient absorption performance can be obtained.
In addition, you may combine said hexagonal pyramid 10 with the electromagnetic wave absorber 110 which arrange | positions the some composite_body | complex P shown in FIG. 11 in 2 or more rows. For example, the radio wave absorber 120 shown in FIG. 12, are arranged in three rows along the with a hexagonal pyramid 10 and the complex P in the X-axis direction (S ₁ to S _3), six in the front row S ₁ The pyramid 10 is arranged, the composite P ₃ is arranged in the last row S _3, and the composite P ₂ having a height lower than that of the composite P ₃ is arranged in the intermediate row S ₂ .

In still another embodiment, as described with reference to FIG. 13A, a form in which the height H ₁₂ of the hexagonal column 12 is different for each column (for example, FIG. 11 and FIG. 12) can be repeatedly used. . In the radio wave absorber 130, by increasing the height H ₁₂ of the hexagonal body 12 toward the column S ₁ in column S _4, S ₄ from S ₇ again reduce the height H ₁₂ of the hexagonal body 12 toward the This arrangement is repeated. According to this configuration, as shown in FIG. 13B, the reflected wave γ ₁ reflected by the highest composite P ₄ , P ₁₀ that functions as a shielding wall (reflected by P _{10 in} the example of FIG. 13). ) Is absorbed by the composite P ₆ or P ₅ which is lower on the front side (left side of the drawing), so that more efficient absorption performance can be obtained with respect to the oblique incident wave β.

Incidentally, the shielding wall formed by the complex column S ₄ or S ₁₀ of FIG. 13 is as shown in Figure 14B. This is a wedge shape with respect to the incident direction of the radio wave, the impedance changes gently, and the radio wave can be scattered to the adjacent hexagonal pyramid 10, so that excellent absorption performance can be obtained.
If a composite body is formed by connecting a rectangular pyramid body 42 made of a lossy material having a bottom surface having the same shape as the bottom surface of the quadrangular pyramid body 40 to the quadrangular pyramid body 40 and a plurality of them are arranged in parallel, FIG. It becomes like this. That is, the shielding wall formed by the quadrangular prism body 42 is a flat surface, and since the impedance change in this case is abrupt, good absorption performance cannot be obtained.

Further, as shown in FIG. 15, in still another embodiment of the present invention, the composite P is made so that the height H ₁₂ of the hexagonal column ₁₂ is concentrically different and is highest at the center of the circle. It can also be arranged. For example, in the radio wave absorber 200, around a height H ₁₂ highest complex P ₁ of the hexagonal column body 12, so as to draw a semicircle on the outside of the complex P _1, arranged a complex P ₂ and, on the outside of the complex P _2, are disposed complex P ₃ lower than P _2.

According to such a configuration, the composite P having a low height is formed in the same manner as when the height H ₁₂ of the hexagonal column 12 of the composite P is changed stepwise for each row (see FIGS. 12 to 14). Since the wall which shields an incident wave is formed in the back, improvement of the radio wave absorption performance can be expected.

In addition, in the radio wave absorber 210 according to still another embodiment described with reference to FIG. 16, a circle is drawn around the complex P ₁ having the highest height H ₁₂ of the hexagonal column 12. , it is arranged different in height H ₁₂ of the hexagonal columnar body 12 for each concentric circle C ₁ -C _3.

According to such a configuration, the height H ₁₂ of the hexagonal column 12 of the composite P (in the figure, the height of the composite P or the hexagonal pyramid is higher in the order of black, hatching, and white) is changed for each column. In the same manner as described above, a wall that shields the incident wave is formed behind the composite P having a low height, so that an improvement in radio wave absorption performance can be expected. In the present embodiment, the height H ₁₂ by varying concentrically, the effect of the shielding wall is obtained over 360 °.
Further, as shown in FIG. 16, a plurality of such radio wave absorbers 210 may be adjacently arranged.

As is clear from the description of the drawings, the electromagnetic wave absorber of the present invention has a hexagonal bottom surface, and therefore, when used in an actual electromagnetic anechoic chamber, it is spread without interposing other polygons. Can be installed. For example, a radio wave absorber having a heptagonal or octagonal bottom surface cannot be spread without a gap unless other figures such as a rectangle are interposed. Thus, from the viewpoint of efficiently spreading the radio wave absorber, the bottom surface of the radio wave absorber is preferably a regular hexagon.
Moreover, the operation | work which arrange | positions an electromagnetic wave absorber in an actual electromagnetic wave anechoic chamber can be simplified by integrally forming the one part or the whole of several electromagnetic wave absorbers.

  As shown in FIG. 17, the hexagon forming the bottom surface of the hexagonal pyramid has at least one pair of opposite sides a that are parallel and the same length, and the length x of the side a and the sides The length L along the side a from the one end point be1 to the other end point be2 of the side b adjacent to a (the length L projected from the side b in the direction along the side a) is 0.5x ≦ L It is preferable to satisfy the relationship of ≦ 2.0x.

  If L ≧ 0.5x, a sufficiently gradual impedance change is obtained in the X-axis direction, and if L ≦ 2.0x, large anisotropy is not caused in the performance of the TE wave and TM wave.

  The loss material forming the radio wave absorber of the present invention is a material that loses radio waves internally, for example, a dielectric loss material such as plastic or ceramic containing a conductive material such as carbon, or a magnetic material such as ferrite. Magnetic loss materials such as plastics or ceramics containing can be used.

Examples of the present invention will be described below.
The absorption performance of the radio wave absorber of this embodiment shown in FIGS. 3, 10, and 13 was evaluated. A foamed polypropylene resin containing carbon was used as the loss material. The test frequency was 3 GHz, and the incident angle (angle with respect to the normal of the bottom surface of the polygonal pyramid) was 60 °. Polarization was set to TE wave and TM wave.

Reference Example 1 follows the embodiment shown in FIG. The height of the hexagonal pyramid was 60 cm, and the shape of the bottom surface was a deformed hexagon having x = 5 cm and L = x in FIG.
Invention Example 1 is in accordance with the embodiment shown in FIG. The height of the hexagonal pyramid portion was 60 cm, and the height of the hexagonal columnar body was 10 cm. In addition, the shape of the bottom face of the hexagonal pyramid portion and the hexagonal columnar body is the same as that of Invention Example 1.
Invention Example 2 is in accordance with the embodiment shown in FIG. The height of the hexagonal pyramid portion was set to 60 cm, and the height of the hexagonal columnar body was changed stepwise to 0 cm, 10 cm, 20 cm, 30 cm, 20 cm, 10 cm, and 0 cm. In addition, the shape of the bottom face of the hexagonal pyramid portion and the hexagonal columnar body is the same as that of Invention Example 1.
Invention Example 3 is the same as Invention Example 1 except that the shape of the bottom surface of the hexagonal pyramid portion is x = 5 cm and L = 2 cm.
Invention Example 4 is the same as Invention Example 1 except that the shape of the bottom surface of the hexagonal pyramid is x = 5 cm and L = 12 cm.

Comparative Example 1 is the same as Inventive Example 1 except that a square pyramid having a side of 10 cm and a height of 60 cm is used.
Comparative Example 2 is the same as Inventive Example 2 except that a square pyramid with a side of 10 cm and a height of 60 cm and a square column with a height of 10 cm are used.

(Radio wave absorption performance)
The radio wave absorption performance was evaluated by the arch method.
In addition, the one where a numerical value is large means that it is excellent in the radio wave absorption performance.

  As a result of the above tests, the radio wave absorber according to the present example showed an improvement in absorption performance of 1 to 10 dB compared to the conventional radio wave absorber.

DESCRIPTION OF SYMBOLS 1 Bottom face 2 Sides of bottom face 3, 43 Side face 4, 44 Vertex 5, 45 Side face 10 Hexagonal pyramid 12 Hexagonal cylinder 40 Quadrangular pyramid 42 Square pillar 100, 110, 120, 130, 200, 210 Wave absorber P complex

Claims (2)

A plurality of composites composed of a hexagonal pyramid made of a lossy material and a hexagonal column connected to the bottom surface of the hexagonal pyramid and made of a lossy material and having a bottom surface having the same shape as the bottom surface, It is arranged without gaps at the bottom of the column,
The height of each hexagonal cylinder constituting the composite is stepwise different for each row, or is increased stepwise toward the center concentrically,
Similarly, the height of each said composite body also differs in steps, The electromagnetic wave absorber characterized by the above-mentioned.   The radio wave absorber according to claim 1, wherein a shape of a bottom surface of the hexagonal pyramid is a convex hexagon.

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