EP0439337A2

EP0439337A2 - Broad-band wave absorber

Info

Publication number: EP0439337A2
Application number: EP91300505A
Authority: EP
Inventors: Yoshiyuki Naito; Michiharu Takahashi
Original assignee: Individual
Current assignee: Individual
Priority date: 1990-01-25
Filing date: 1991-01-23
Publication date: 1991-07-31
Anticipated expiration: 2011-01-23
Also published as: EP0439337B1; EP0439337A3; DE69108577T2; DE69108577D1; KR0130755B1

Abstract

The present invention relates to a broad-band wave absorber wherein plates (3) formed of a ferrite magnetic material are placed at an optimal spacing and are aligned in a lattice form in longitudinal and lateral directions on a conductive plate (2). A magnetic substance of a specific thickness tm is formed into cylindrical blocks of a height d (where d ≧ tm) wherein an end surface thereof is polygonal, and the cylindrical blocks are provided with a radio-wave reflecting surface aligned in such a manner that this surface is perpendicular to the axial direction of the blocks, and the end surface of the blocks is approximately perpendicular to a direction from which radio waves are incident. The ferrite magnetic substance could also be formed into rectangular prisms of thickness 2tm, height d, and length in the longitudinal direction thereof L, with the prisms aligned at a spacing b on a radio-wave reflecting surface, the direction of the height dimension of the prisms being approximately parallel to a radio-wave incidence direction, and the surfaces thereof of the dimensions 2tm and L being perpendicular to the radio-wave incidence direction, forming a plane parallel to a magnetic field direction of incident radio waves and the dimension L, wherein the following relationships hold:
L ≧ d ≧ 2tm
20tm ≧ b ≧ 2tm

Description

The present invention relates to a wave absorber constructed using a ferrite magnetic material, and, in particular, to a broad-band wave absorber in which ferrite blocks are arranged at a specific spacing on a conductive plate.
Much research has been performed on conventional wave absorbers that use ferrite, so much so that their capabilities are becoming well-known.
The construction of the wave absorber that has become a conventional standard is such that ferrite tiles (plates) are arranged on a conductive plate, as shown in Fig. 17.
For unidirectional-polarization use, a variation has been proposed (in US Patent No. 4,118,704) in which some of the ferrite plates are removed in a regular pattern in an electric field direction to leave portions where the conductive plate is exposed (called vacant portions), as shown in Fig. 18.
In general, if such vacant portions are provided, characteristics the same as those of the structure of Fig. 17 can be obtained by making the thickness of the ferrite in the ferrite parts greater than that of the ferrite of Fig. 17, but the bandwidth characteristics cannot be expected to be improved thereby. (Problem to be Solved by the Present Invention)
To widen the bandwidth, it is needed to provide some other technologies.
An object of the present invention is to provide a novel wave absorber having an improved characteristic of handwidth. The present invention was designed while taking the above points into consideration, with the aim of providing a broadband wave absorber that has a much broader bandwidth than a conventional absorber, that can be used in the VHF, UHF, and microwave bands, and that has excellent characteristics such that it can not only be used as an absorber with respect to waves polarized in the horizontal and vertical directions, it can also be used as a wave absorber for unidirectional-polarization use.
In order to satisfy the above aim, the present invention provides a broad-band wave absorber wherein beams formed of a ferrite magnetic material are placed at an optimal spacing and are aligned in a lattice form in longitudinal and lateral directions on a conductive plate. A magnetic material of a specific thickness t_m is formed into cylindrical blocks of a height d (where d ≧ t_m) wherein an end surface thereof is polygonal, and the cylindrical blocks are provided with a radio-wave reflecting surface arranged in such a manner that this surface is perpendicular to the axial direction of the blocks, and the end surface of the blocks is approximately perpendicular to a direction from which radio waves are incident. The ferrite magnetic material could also be formed into rectangular prisms of thickness 2t_m, height d, and length in the longitudinal direction thereof L, with the prisms aligned at a spacing b on a radio-wave reflecting surface, the direction of the height dimension of the prisms being approximately parallel to a radio-wave incidence direction, and the surfaces thereof of the dimensions 2t_m and L being perpendicular to the radio-wave incidence direction, forming a plane parallel to a magnetic field direction of incident radio waves and the dimension L, wherein the following relationships hold:
L ≧ d ≧ 2t_m
20t_m ≧ b ≧ 2t_m
The reasons why it was considered that the present invention would broaden the bandwidth of the wave absorber are described below.
In the configuration of Fig. 1, since a surface with a small surface area is aligned perpendicular to the direction from which incident waves are incident, it can be expected that waves reflected from the interface with the ferrite will be reduced. This differs from the single-layer configuration shown in Fig. 17 in that, in the portions where there is ferrite, the ferrite portions and vacant portions are arranged alternately, then no plane waves can exit - transverse-magnetic (TM) waves are propagated. Therefore the interfaces with the ferrite ensures that the waves that are not propagated into free space, are converted into TM waves, increasing the absorption over a wide frequency range and thus broadening the bandwidth.
In other words, in the conventional wave absorber, a surface of the ferrite tiles with a large surface area is aligned perpendicular to the direction of incident radio waves. The wave absorber of the present invention, however, has the characteristic that the equivalent surface with the large surface area is aligned parallel to the direction of incident radio waves, and the resultant electromagnetic characteristics are dramatically different. To put it another way, if the dimensions of the magnetic tiles are defined as a length L, a height d, and a thickness t (where L > d > t), the conventional wave absorber has tiles aligned with L-d surfaces thereof perpendicular to the direction of incident radio waves, but the wave absorber of the present invention, on the other hand, achieves a much broader bandwidth by having- tiles aligned with the L-t surfaces thereof perpendicular to the direction of incident radio waves.
As described above, by providing a construction consisting of blocks of a ferrite magnetic material shaped to specific dimensions and aligned at a specific spacing, the present invention can provide a broadband wave absorber able to absorb radio waves over a wide frequency range, by reducing -wave reflection and by increasing absorption by TM wave.

Figs. 1(a), (b), and (c) are perspective views illustrating an embodiment of the present invention;
Figs. 2(a) and (b) are views of models used in a description of the embodiment of Fig. 1;
Fig. 3 is a graph of the absorption characteristics of the embodiment of Fig. 1;
Fig. 4 is a graph of the variation with height of the absorption characteristics of this embodiment of the present invention;
Fig. 5 is a graph of the variation with thickness of the absorption characteristics of this embodiment of the present invention;
Fig. 6 is a graph of a variation in the spacing of the absorption characteristics of this embodiment of the present invention;
Fig. 7 is a graph of absorption capability, showing the relationship between absorbent bodies and vacant portions used in the present invention;
Fig. 8 is a graph of absorption capability, showing the relationship between frequency and the K constants of the dispersion equation used in the present invention;
Fig. 9 is a graph of absorption characteristics when the product S of the kl and fl [MHz] of the dispersion equation is 8000 MHz;
Figs. 10(a), (b), and (c) are perspective and front views illustrating an embodiment of the present invention configured of coaxial tubes, and a graph showing the characteristic thereof;
Figs. 11 to 13 are side and perspective views illustrating other embodiments of the present invention;
Fig. 14 is a perspective view of an embodiment of the present invention in which ferrite bars are inserted longitudinally and laterally;
Figs. 15 and 16 are perspective views of further embodiments of the present invention;
Fig. 17 is a perspective views of the configuration of a wave absorber that has become a conventional standard; and
Fig. 18 is a perspective view of the configuration of an actual conventional wave absorber.

The present invention will first be described with reference to the embodiment thereof shown in Figs. 1(a), (b), and (c); this embodiment will then be analyzed with reference to the model thereof shown in Figs. 2(a) and (b); the results of experiments will be described with reference to Figs. 3 to 9; and finally other embodiments of the present invention will be described with reference to Figs. 10 to 16.
The perspective view of Fig. 1(a) shows the essential details of an embodiment of the wave absorber of the present invention that uses horizontally and vertically polarized waves. Fig. 1(b) shows a wave absorber similar to that of Fig. 1(a), but in which the vertically aligned magnetic frames are removed and a conductive plate that is in contact with the radio-wave reflecting surface is inserted into the thickness of each lateral frame, and Fig. 1(c) shows a further example in which the conductive plates are omitted from within the ferrite frames.
The explanation that follows is based on the above structure for unidirectional-polarization waves.
The wave absorber of the present invention is configured of a stack of a large number of identical units of the same construction shown in Fig. 1. Each unit consists of ferrite plates 3 formed in a box shape on a conductive plate 2 that forms a radio-wave reflecting surface, the thickness of the ferrite plates 3 being 2t_m, the spacing therebetween being b, and the height thereof being d; and the units are aligned on the conductive plate 2 in such a manner as to form a lattice. Since all of these units act in exactly the same manner, analysis thereof can be conducted by considering a single unit.
Fig. 2(a) shows a single-cell model used in such analysis. The symmetry of the overall structure means that it is possible to assume that a metal plate can be inserted into the central portion of each ferrite plate, parallel thereto, without affecting in any way the magnetic field thereof. Therefore, the analysis below uses the model shown in Fig. 2(b).
In this analysis, the following equation is used to find µ_r, the relative permeability of each ferrite magnetic material:
µ_r = l + {K_l x f_l / (f_l + jf)}
where f is frequency MHz and (l + k_l) is the initial relative permeability under DC conditions.
In this equation, fl [MHz] corresponds to the frequency at which the imaginary part of the relative permeability becomes a maximum.
A value S, the product of kl and fl (i.e., kl x fl), is the quality of ferrite magnetic materials. Of the various compositions of ferrite is 10,000 MHz or less.
This analysis uses a value of 6000 MHz for the product S for ferrite. Therefore, if the value of kl is fixed, the value of fl [MHz] is automatically fixed.
This analysis is based on the use of ferrite whose value of kl is 1000 and fl is 6 MHz.
Since there is virtually no frequency dispersion in the permittivity ε_r of ferrite, so this analysis is based on the assumption that there is no variation therein with the frequency, i.e., that:
ε_r = 16 - j0
It is known that, with a single-layer absorber using ferrite, the thickness that gives the best absorption is more-or-less constant, regardless of frequency, and that it is 8 mm if S is 6000 MHz.
In Fig. 3, curve A shows the absorption frequency characteristics for a single-layer absorber.
The wave absorber of the present invention has three parameters: the thickness 2t_m of the ferrite plates, the spacing b between the ferrite plates, and the height d of the ferrite plates. Since it is not feasible to analyze all variations in these parameters, the description below relates to parameters at which the characteristics were best within the analyzed range: 2t_m = 8 mm, b = 20 mm, and d = 20 mm. In Fig. 3, the absorption characteristic B for a wave absorber for which the above dimensions were selected is shown superimposed on the characteristic A of the conventional single-layer absorber.
In general, the reflectivity that is a characteristic of a wave absorber must be less than or equal to a permissible reflection coefficient. This analysis concerns evaluation at a frequency bandwidth that is 1% of the power level, i.e., at -20 dB or less.
It is clear from the characteristics curves of Fig. 3 that the wave absorber of the present invention has an extremely broad bandwidth.
It is also clear that if a wave absorber of this structure is formed with absorbent bodies of the same surface area as that of the single-layer absorber, roughly the same volume of ferrite as that of the single-layer absorber would be sufficient, proving that adoption of the structure of the present invention will result in a dramatic improvement in characteristics for the same quantity of ferrite.
As mentioned above, the absorber of the present invention has three parameters: the thickness 2t_m of the ferrite plates, the spacing b between the ferrite plates, and the height d of the ferrite plates. Another parameter is (b - 2t_m)/b, the proportion of the metal plate occupied by the empty portions between ferrite plates, hereinafter called the vacancy ratio.
Fig. 4 shows absorption frequency characteristics obtained by varying the height of the ferrite plates while keeping the thickness thereof constant at 8 mm and the spacing therebetween constant at 20 mm. It is clear from the curves of Fig. 4 that when the height d of the ferrite plates becomes less than 20 mm, the characteristic at higher frequencies becomes better, but, in contrast, the characteristic at lower frequencies worsens. Therefore, in this case, it is considered that the best characteristic occurs when the height d is 20 mm.
In a similar way, Fig. 5 shows absorption frequency characteristics obtained by varying the thickness of the ferrite plates, and Fig. 6 shows absorption frequency characteristics obtained by varying the spacing therebetween. In both cases, it was found that an optimal value existed, in roughly the same way as that described above for variations in thickness, and this optimal value was at b = 20 mm.
Fig. 7 shows absorption frequency characteristics obtained by keeping the thickness of the ferrite plates fixed at 20 mm, but varying both b and 2t_m in such a manner that the vacancy ratio (b - 2t_m)/b was constant at 60%.
The sample characteristics shown in the figure were obtained with b = 10 mm, 2t_m = 4 mm; b = 20 mm,2t_m = 8 mm; b = 30 mm, 2t_m = 12 mm; and b = 40 mm, 2t_m = 16 mm. It is clear that the best characteristic occurs when b = 20 mm and 2t_m = 8 mm, showing that the vacancy ratio is not particularly meaningful as a parameter. In other words, with the vacancy ratio kept constant, variations in b and 2t_m are far more important as effects on characteristics.
Now for a look at the absorption frequency characteristics obtained by varying the kl and fl [MHz].
Fig. 8 shows the characteristics obtained by using the above optimal structure at which the product S is fixed at 6000 MHz, but kl and fl [MHz] are varied.
As can be seen from the characteristics curves of Fig. 8, if the value of kl is increased while the product S is kept constant, the bandwidth broadens. In other words, the frequency at which the curve starts to fall below -20 dB is determined by K_l, whereas the frequency at which the curve starts to rise above -20 dB is determined by the configuration of the absorber.
Next is an investigation of the case in which the product S is varied.
Fig. 9 shows the absorption frequency characteristics obtained when the product S was 8000 MHz.
With S = 6000 MHz, the best characteristic was obtained when 2t_m = 8 mm, b = 20 mm, and d = 20 mm, but with S = 8000 MHz, the best characteristic was obtained when 2t_m = 6 mm, b = 15 mm, and d = 15 mm. Experiments with S = 8000 MHz produced the same result that the bandwidth was seen to broaden as kl increased.
In this way, although it is obvious that dimensions will vary with the permeability and frequency characteristics of the ferrite material used in the optimal structure according to the present invention, in most cases, if the product S of kl and fl is between 4000 MHz and 10,000 MHz, 2t_m should be between approximately 3 mm and 12 mm, and b should be equal to d, with both being between approximately 12 mm and 30 mm.
Another embodiment of the present invention, based on exactly the same physical phenomenon as the above model but with a different structure consisting of coaxial conductive tubes, will now be described with reference to Fig. 10.
The wave absorber shown in Figs. 10(a) and (b) has an annular configuration of an inner diameter of 12 mm, a thickness of 1.5 mm, and a length of 5 mm. This absorber is aligned with a coaxial internal conductor in front in the axial direction f a short-circuiting plate of a circular, coaxial conductive tube. Measurements of the absorption frequency characteristics with respect to variations in length of this wave absorber are shown in Fig. 10(c).
As can be seen from Fig. 10(c), the bandwidth within which the absorption is below the permissible reflection is much broader at a length of 20 mm, showing good match with analytic results.
Another alternative to the plate-shaped ferrite magnetic bodies of Fig. 1 is a circular or polygonal prismatic form, as shown in Fig. 11.
Furthermore, disposing pyramid type wave absorber as shown in Fig. 12 and that operates at frequencies above the upper limit of the wave absorber of the present invention, either to the front or between parallel flat of the present invention enables compounding to further broaden the band.
In addition, there was no large change in the characteristics even if there is the dielectric shown in Fig. 13 disposed between the parallel flat plates of the wave absorber of the present invention.
Fig. 14 is effective for horizontal and/or vertical polarized waves.
Fig. 15 shows another embodiment of the present invention, in which the shape of the end surfaces of the ferrite magnetic body is formed into a cylindrical shape so that it forms a perpendicular unit. This perpendicular unit uses ferrite having a thickness t_m so that one side is a, and so that the other side is b. This perpendicular unit is formed as a cylindrical block with a height d.
Fig. 16 shows one portion of a wave absorber of a required area and in which the cylindrical blocks of Fig. 15 are overlapped in the direction of the one side a, and in the direction of the other side b.
The magnetic material used in the present invention can be ferrite of NiZn, MgZn or MnZn or the like, and moreover, can be materials, such as ferrite powder is mixed with glass, ceramic, rubber, plastic, carbon, paper, or fiber, etc.

Claims

A broad-band wave absorber wherein beams formed of a ferrite magnetic material are placed at an optimal spacing and are aligned in a lattice form in longitudinal and lateral directions on a radio-wave reflecting surface.
A wave absorber having a wave absorber structure according to claim 1, wherein at least one of a conductive body, a magnetic body, and a resistive body is inserted within said magnetic material forming said wave absorber, or within said flat plate, or in front thereof.
A wave absorber having a wave absorber structure according to claim 1, wherein said magnetic material is in the shape of polygonal prisms, circular prisms, or combinations thereof.
A wave absorber having a wave absorber structure according to claim 1, wherein said ferrite magnetic material is, the thickness thereof varying in either a continuous manner or a step-wise manner from a direction from which radio waves are incident toward a direction of a radio-wave reflecting surface.
A wave absorber having a wave absorber structure according to claim 1, wherein blocks in at least one of said longitudinal and lateral directions are superimposed.
A wave absorber in which a magnetic material of a specific thickness t_m is formed into cylindrical blocks of a height d (where d ≧ t_m) wherein an end surface thereof is polygonal, and wherein said cylindrical blocks are provided with a radio-wave reflecting surface aligned in such a manner that said surface is perpendicular to the axial direction of said blocks, and said end surface of said blocks is approximately perpendicular to a direction from which radio waves are incident.
A wave absorber having a wave absorber structure according to claim 6, wherein said at least one of a conductive body, a magnetic body, and a resistive body is inserted within said magnetic material forming said wave absorber, or within said flat plate, or in front thereof.
A wave absorber having a wave absorber structure according to claim 6, wherein said magnetic material is in the shape of polygonal prisms, circular prisms, or combinations thereof.
A wave absorber having a wave absorber structure according to claim 6, wherein said ferrite magnetic material is in the shape of cylindrical blocks, the thickness thereof varying in either a continuous manner or a step-wise manner from a direction from which radio waves are incident toward a direction of a radio-wave reflecting surface.
A wave absorber having a wave absorber structure according to claim 6, wherein blocks in at least one of said longitudinal and lateral directions are superimposed.
A broad-band wave absorber wherein a ferrite magnetic material is formed into rectangular prisms of thickness 2t_m, height d, and length in the longitudinal direction thereof L, and said prisms are aligned at a spacing b on a radio-wave reflecting surface, the direction of the height dimension of said prisms being approximately parallel to a radio-wave incident direction, and the surfaces thereof of said dimensions 2t_m and L being perpendicular to said radio-wave incidence direction, forming a plane parallel to a magnetic field direction of incident radio waves and said dimension L, wherein the following relationships hold:
L ≧ d ≧ 2t_m
20t_m ≧ b ≧ 2t_m
A broad-band ferrite wave absorber having a wave absorber structure according to claim 11, wherein said magnetic material is an NiZn-type ferrite with an initial permeability of at least 700, and said prisms have a thickness 2t_m ≦ 8 mm and a height d ≧ 20 mm.
A broad-band ferrite wave absorber having a wave absorber structure according to claim 11, wherein said magnetic material is an MnZn-type ferrite with an initial permeability of at least 2000, and said prisms have a thickness 2t_m ≦ 8 mm and a height d ≧ 35 mm.
A wave absorber having a wave absorber structure according to claim 11, wherein a parallel plate is inserted into approximately the center in the widthwise direction of each of said beams of said magnetic material, one edge thereof being exposed from a direction from which radio waves are incident, whereas the opposite edge thereof is connected to said radio-wave reflecting surface.
A wave absorber having a wave absorber structure according to claim 11, wherein at least one of a conductive body, a magnetic body, and a resistive body is inserted within said magnetic substance forming said wave absorber, or within said flat plate, or in front thereof.
A wave absorber having a wave absorber structure according to claim 11, wherein said magnetic material is in the shape of polygonal prisms, circular prisms, or combinations thereof.
A wave absorber having a wave absorber structure according to claim 11, wherein said ferrite magnetic material is in the shape of rectangular prisms, the thickness thereof varying in either a continuous manner or a step-wise manner from a direction from which radio waves are incident toward a direction of a radio-wave reflecting surface.
A wave absorber having a wave absorber structure according to claim 11, wherein blocks in at least one of said longitudinal and lateral directions are superimposed.