WO2010125626A1

WO2010125626A1 - Electromagnetic absorber for anechoic chamber

Info

Publication number: WO2010125626A1
Application number: PCT/JP2009/058245
Authority: WO
Inventors: 守中野; 一男石塚
Original assignee: 株式会社リケン; 株式会社リケン環境システム
Priority date: 2009-04-27
Filing date: 2009-04-27
Publication date: 2010-11-04

Abstract

Disclosed is an electromagnetic absorber that has excellent electromagnetic absorption properties and is best suited for design of an anechoic chamber having a small size and a high performance. In a ferritic electromagnetic absorber containing Mn, Zn and Li, the content of Li is 0.005 to 0.5% by mass of the total amount of the electromagnetic absorber. In this case, the value μ" of an imaginary part in a complex relative permeability of the electromagnetic absorber at a frequency of 30 MHz and the value μ" of an imaginary part in a complex relative permeability of the electromagnetic absorber at a frequency of 30 to 70 MHz are set so as to satisfy 213 to 530 and 28.5 to 31.5 M/f, respectively, wherein M represents the imaginary part in the complex relative permeability of the electromagnetic absorber at 30 MHz; and f represents frequency, MHz. The plate thickness of the electromagnetic absorber is 1.51 to 1.67/M (m) wherein M represents the imaginary part in the complex relative permeability of the electromagnetic absorber at 30 MHz.

Description

Electromagnetic wave absorber for anechoic chamber

The present invention relates to a radio wave absorber for an anechoic chamber, and more particularly to a radio wave absorber that exhibits excellent radio wave absorption characteristics in a frequency range of 30 MHz to 1 GHz and can be applied to a small and high performance anechoic chamber.

In recent years, with the advancement of advanced information technology, weak electromagnetic waves generated from various types of communication devices and electronic devices have a problem with electromagnetic interference (EMI) causing malfunctions in instruments such as televisions, radios, communications, medical care, ships, and aircraft. Therefore, regulations on electromagnetic waves are also required internationally. Therefore, manufacturers of various communication devices and personal computers that generate noise that may cause electromagnetic interference are required to accurately measure noise generated from electronic devices and take countermeasures. That is, there is a demand for measures for preventing the generation of harmful electromagnetic waves by measuring extremely weak electromagnetic waves generated from electronic devices or the like with a high-performance measuring instrument with high accuracy. Here, the problem is the environment for measuring electromagnetic waves, and in order to accurately measure extremely weak electromagnetic waves, a high-performance anechoic chamber free from disturbances such as noise is required.

In conventional anechoic chambers, magnetic materials such as Mn—Zn ferrite and Ni—Zn ferrite have been mainly used as the electromagnetic wave absorber material. Mn—Zn ferrite has a high permeability at frequencies from 10 kHz to 30 MHz, whereas Ni—Zn ferrite has been widely used in these frequency ranges because it exhibits high permeability at frequencies from 30 MHz to 300 MHz. However, recently, a response to weaker electromagnetic waves is required, and a higher performance anechoic chamber is required. Generally, by increasing the size of the anechoic chamber, the electromagnetic wave absorption performance can be improved. For this reason, in order to enable more accurate measurement, a method of increasing the performance of the anechoic chamber by using a conventional wave absorber such as Mn-Zn ferrite or Ni-Zn ferrite is also considered. It is done. However, considering the difficulty of construction and equipment costs, there is a limit to the increase in size of the anechoic chamber.

In Non-Patent Document 1, Li-Zn ferrite with high magnetic permeability is adopted, the relationship between the Li-ferrite content in the material and the complex magnetic permeability spectrum is evaluated, and its application to a single-layer type wave absorber is studied. ing. However, the value μ ”of the imaginary part of the complex relative permeability in the frequency range of 30 MHz to 1 GHz of the ferrite described in Non-Patent Document 1 is about 100 (see Non-Patent Document 1 Fig. 1 (b)). In order to cope with the extremely weak electromagnetic waves that have been demanded in recent years by using such a radio wave absorber of μ ”value, it is inevitable that the anechoic chamber is enlarged. Furthermore, when Li is added within the range described in Non-Patent Document 1, the shrinkage rate during ferrite sintering increases, warping or cracking occurs in the sintered body, and the desired dimensional accuracy cannot be obtained. There is a possibility. Thus, at present, a radio wave absorber material having a value of an imaginary part μ ″ of a high complex relative permeability that can be applied to a small and high-performance anechoic chamber that can cope with extremely weak electromagnetic waves has been obtained. Absent.

Accordingly, an object of the present invention is to provide a radio wave absorber that is excellent in radio wave absorption characteristics, and is optimal for designing a small and high performance anechoic chamber.

As a result of diligent research in view of the above object, the present inventors, when adding Li to Mn—Zn ferrite, have a value μ ″ (hereinafter referred to as “mu”) of complex relative permeability within a very small amount of Li. , "Μ" ") was found to increase significantly, and the present invention was conceived. That is, the electromagnetic wave absorber for an anechoic chamber of the present invention is a ferrite-based electromagnetic wave absorber containing Mn, Zn and Li, and the Li content is 0.005 to 0.5 mass% with respect to the total amount of the absorber. It is characterized by.

According to the present invention, an electromagnetic wave absorber for an anechoic chamber having a high μ ″ is obtained, and a small and high-performance anechoic chamber is realized. Further, the electromagnetic wave absorber of the present invention has the highest electromagnetic wave absorption. The thickness of the absorber (matching thickness) matches the ideal thickness in terms of the strength, weight and cost of the absorber, which makes it possible to manufacture a high-performance anechoic chamber with good workability and at a lower cost. Furthermore, since the matching thickness of the electromagnetic wave absorber of the present invention is maintained almost constant regardless of the frequency, an anechoic chamber having excellent electromagnetic wave absorption characteristics can be efficiently manufactured in a wide frequency range. can do.

The electromagnetic wave absorber for an anechoic chamber of the present invention will be described in detail below.
In the design of the anechoic chamber, the thickness (plate thickness) of the ferrite (tile) serving as the electromagnetic wave absorber is important from the viewpoint of cost and workability. If the thickness of the ferrite increases, the material cost increases, the weight of the radio wave absorber increases, and the workability deteriorates. For this reason, it is preferable that the thickness of the radio wave absorber is 7.5 mm or less. On the other hand, if the ferrite tile is thin, the strength is insufficient, and problems such as breakage may occur during construction, which may interfere with the production of the anechoic chamber. For the above reasons, it is desirable to design the thickness of the electromagnetic wave absorber to 3 mm to 7.5 mm.

On the other hand, the radio wave absorption characteristics of the radio wave absorber depend on the thickness of the radio wave absorber. Assuming an electromagnetic wave absorber with a metal plate lined on a ferrite tile, the thickness (matching thickness) d of the electromagnetic wave absorber when the electromagnetic wave absorption amount of the electromagnetic wave absorber is maximized is expressed by the following equation from the theory of electromagnetics: (Yoshitaka Shimizu, “Latest absorption and shielding of electromagnetic waves”, Nikkei Technical Books, p. 120-121).
d = λ / (2πμ ") ------------------- (1)
λ is free space wavelength: λ = 300 / f, f is frequency (MHz)
When transforming equation (1),
μ "= λ / (2πd) ------------------- (2)
It becomes.

The most efficient anechoic chamber can be designed by using the above-described electromagnetic wave absorber, ie, an electromagnetic wave absorber having a matching thickness of 3 mm to 7.5 mm. Here, substituting 3 mm to 7.5 mm for d in Equation (2) yields μ "= 213 to 530 at a frequency of 30 MHz. Therefore, if a radio wave absorber with μ" at a frequency of 30 MHz is 213 to 530, it is most efficient. It is possible to design a typical anechoic chamber. However, a material having such a μ ″ has not been obtained with a conventional ferrite-based electromagnetic wave absorber.

FIG. 1 shows the relationship between the Li content of an Mn—Zn ferrite absorber (thickness: 7.0 mm) and μ ″ at a frequency of 30 MHz. The preparation of Li-containing ferrite and the calculation of μ ″ were performed as follows. .
A predetermined amount of Mn—Zn ferrite powder (manufactured by Fair Light Co., Ltd.) was immersed in lithium nitrate aqueous solutions having different concentrations and adjusted so that the Li content became a desired value, and then dried at 80 ° C. Each of the obtained powders was put into a mold and subjected to pressure molding under a pressure of ² t / cm ² , then heated at 300 ° C./hr in an electric furnace and baked at 1250 ° C. for 1 hour. Here, the firing atmosphere is from normal temperature to 600 ° C. in the atmosphere, from 600 ° C. to 1250 ° C. in nitrogen, while holding at 1250 ° C., under 10 Pa of oxygen, and when cooled down from 1250 ° C. to 900 ° C. under 50 Pa of oxygen The atmosphere was from 900 ° C. to room temperature. The obtained Li-added Mn—Zn ferrite sintered bodies were each processed into a plate shape of 100 × 100 × 7 mm and used as samples for evaluation. In addition, it was confirmed by atomic absorption method that the Li content of each sample had a desired value.

The magnetic permeability of each sample was measured by a coaxial tube method using a network analyzer (8753A manufactured by HEWLETTWPACKARD). The sample for evaluation is processed into a donut shape with an outer diameter of 38.8 mm and an inner diameter of 16.9 mm (thickness 7 mm), set in a coaxial tube as shown in Fig. 2, and the amplitude and phase of the reflected and transmitted waves are measured with a network analyzer. Measured μ ”.

From Fig. 1, it was confirmed that the optimum μ "was obtained when the Li content was 0.005 to 0.5 mass%, and the range was 213 to 530, and the cost and workability were excellent. It can be seen that the ideal ferrite thickness (3 mm to 7.5 mm) calculated from the above viewpoint is the matching thickness of the wave absorber. Therefore, by setting the Li content in the Mn—Zn ferrite to 0.005 to 0.5% by mass, it is possible to efficiently produce a small anechoic chamber having excellent radio wave absorption characteristics at low cost. In addition, when the Li content is in such a small range, shrinkage during sintering does not become a problem, generation of warpage and cracks can be suppressed, and a ferrite sintered body can be manufactured with excellent dimensional accuracy.
The Li content in the radio wave absorber is preferably 0.007 to 0.1% by mass, more preferably 0.01 to 0.05% by mass. In this range, μ ″ increases significantly, and it is possible to cope with a thinner wave absorber, which is effective for reducing the cost, size and performance of the anechoic chamber.

The electromagnetic wave absorber for an anechoic chamber of the present invention is a ferrite-based electromagnetic wave absorber containing Mn, Zn and Li, and the Li content is 0.005 to 0.5 mass% with respect to the total mass of the electromagnetic wave absorber. That's fine. Among these ferrites, Mn—Zn ferrite containing 10 to 20% by mass of Mn and 10 to 20% by mass of Zn is particularly preferable.

Next, the frequency dependence of the radio wave absorption characteristics of the electromagnetic wave absorber for an anechoic chamber of the present invention will be examined. The anechoic chamber is required to effectively absorb electromagnetic waves in a predetermined frequency range for the purpose of use, and naturally, the performance of the electromagnetic wave absorber is also required. Since the wavelength λ is inversely proportional to the frequency f, in the expression (1), if μ ″ is not inversely proportional to the frequency, the matching thickness d will vary depending on the frequency. The thickness of the electromagnetic wave absorber is varied depending on the frequency. Since it cannot be changed in practice, it is desirable that the matching thickness be kept constant regardless of the frequency.

From equation (1), the matching thickness d _{30 MHz} at _{30 MHz} is expressed by the following equation.
_{d 30MHz = (300/30) / (} 2πμ "30MHz)
= 5 / (πμ _"30MHz)
This (2) are substituted into the formula _{μ "= λ / (2πd 30MHz} )
= λμ " _30MHz / 10
= (300 / f) μ " _30MHz / 10
= 30μ " _30MHz / f
Here, if M = μ " _30MHz ,
μ "= 30M / f ------------------- (3)
It becomes.

Therefore, if the wave absorber has such frequency characteristics, the matching thickness d is constant regardless of the frequency, and an efficient anechoic chamber capable of exhibiting excellent wave absorption characteristics in a wide frequency range is designed. it can. The performance of the anechoic chamber is often a problem on the low frequency side. For this reason, it is desirable that it be within 5% of the expression (3) in the frequency range of 30 to 70 MHz. That is,

μ "= 28.5M / f to 31.5M / f ------------------- (4)
Therefore, it is desirable that μ ″ is in the above range.
Here, in the conventional Mn—Zn ferrite to which no Li is added, the frequency characteristic of μ ″ is 32.7 M / f, which is out of the above frequency range. Ferrite has a frequency characteristic of μ ″ of 30.4 M / f and falls within the range of the formula (4), and it can be seen that excellent radio wave absorption characteristics can be obtained in the above frequency range.

In addition, the thickness of the radio wave absorber that the radio wave absorber can exhibit the most radio wave absorption performance is obtained from the equation (1) as follows.
d = (300/30) / (2πM)
= 1.59 / M ------------------- (5)
Here, the thickness of the imaginary part of the complex relative permeability at M: 30 MHz is desirably within 5% of the equation (5),
d = 1.51 / M ～ 1.67 / M (m) ------------------- (6)
It becomes.

The effects of the present invention will be described in more detail with reference to the following examples.
Example Mn-Zn ferrite powder was adjusted by the above-described method so that the Li content with respect to the total amount of the ferrite absorber was 0.02% by mass, pressure-molded, and then fired (Example). The obtained Li-added Mn—Zn ferrite sintered body was processed, and the magnetic permeability was measured by a coaxial tube method using a network analyzer (8753A manufactured by HEWLETT PACKARD). Further, as a comparative example, evaluation was similarly performed using Ni—Zn ferrite (30 MHz to 300 MHz) showing higher magnetic permeability on the higher frequency side than Mn—Zn ferrite (10 kHz to 30 MHz).

FIG. 3A shows the result of evaluating the frequency dependence of μ ″ of the radio wave absorber of the example in the frequency range of 30 MHz to 300 MHz. FIG. 3B similarly shows the radio wave of the comparative example. The result of having evaluated the frequency dependence of μ ”of the absorber is shown. Here, the straight line is the equation (3), that is,
μ "= 30M / f. As described above, if the wave absorber has a wave absorption characteristic satisfying the equation (3), the matching thickness is constant regardless of the frequency, so that it is wide. 3, the electromagnetic wave absorber of the comparative example has a deviation from the equation (3), but the electromagnetic wave absorber of the example has almost the same as the equation (3). This confirms that the radio wave absorber of the present invention can exhibit excellent radio wave absorption characteristics over a wider range than the conventional radio wave absorber.

FIG. 4 shows the relationship between the frequency and the matching thickness of the radio wave absorbers of the example and the comparative example. In the comparative example, the matching thickness changes by about 25% from 7.8 mm to 6.2 mm in the frequency range from 30 MHz to 300 MHz. On the other hand, in the examples, it was confirmed that only 5% changed from 6.2 mm to 6.5 mm.

FIG. 5 shows the results of evaluating the radio wave absorption characteristics of samples of matching thicknesses at 30 MHz and 300 MHz for the radio wave absorbers of the example and the comparative example, respectively. Here, the matching thickness of the radio wave absorber of the example is 6.5 mm at 30 MHz and 6.2 mm at 300 MHz, and the matching thickness of the radio wave absorber of the comparative example is 7.8 mm at 30 MHz and 6.2 mm at 300 MHz. .
In the radio wave absorber of the comparative example, the radio wave absorption amount (shown as the reflection amount in the figure) greatly changed depending on the frequency to be matched. On the other hand, in the radio wave absorber of the example, no significant change was observed in the radio wave absorption characteristics when matched to any frequency, and in almost all frequency ranges, the radio wave absorption characteristics were superior to those of the comparative example. showed that. FIG. 5 shows the evaluation results for frequencies from 30 MHz to 300 MHz. It was confirmed that the radio wave absorbers of the examples can obtain good radio wave absorption characteristics even at frequencies of 300 MHz to 1000 MHz (1 GHz).

FIG. 6 shows the results of calculating the performance of each anechoic chamber when the anechoic chamber was designed using the electromagnetic wave absorbers of the example and the comparative example. Here, the length L of the anechoic chamber is 21m, the height H is 8.5m, the measurement distance is 10m, the diameter of the turntable is 3m, and the width W of the room is changed between 12m and 17m. went. The anechoic chamber performance becomes better as the deviation from the open site theoretical value is smaller.
From FIG. 6, when W = 12 m, the deviation from the open site theoretical value was about 4 dB when using the electromagnetic wave absorber of the comparative example, and about 2 dB when using the electromagnetic wave absorber of the example. . Therefore, it can be seen that in a dark room of the same size, when the radio wave absorber of the example is used, about twice the performance can be obtained as compared with the case where the radio wave absorber of the comparative example is used.
On the other hand, if an attempt is made to obtain a performance equivalent to that of a anechoic chamber of W = 12 m using the electromagnetic wave absorber of the embodiment using the electromagnetic wave absorber of the comparative example, W = 17 m is required. As a result, the darkroom volume must be increased by 40% and the ferrite usage must be increased by 20%. From the above results, when using the radio wave absorber of the example, including construction costs, it is confirmed that the cost can be reduced by about 30% compared to the case of using the radio wave absorber of the comparative example. It was done.

It is a figure which shows the relationship between Li content in a Mn-Zn ferrite absorber, and μ "at 30 MHz. It is the schematic of the apparatus used for the measurement of magnetic permeability. It is a figure which shows the frequency dependence of (micro | micron | mu) "of the electromagnetic wave absorber of an Example (A) and a comparative example (B). It is a figure which shows the frequency dependence of the matching thickness of the electromagnetic wave absorber of an Example and a comparative example. It is a figure which shows the electromagnetic wave absorption characteristic of the electromagnetic wave absorber of an Example and a comparative example when it is set as the matching thickness in 30 MHz (A) and 300 MHz (B). It is a figure which shows the result of having calculated the deviation with an open site theoretical value when an anechoic chamber is designed with the electromagnetic wave absorber of an Example and a comparative example.

10 ... Sample 20 ... Network analyzer

Claims

A ferrite-based electromagnetic wave absorber containing Mn, Zn and Li, wherein the Li content is 0.005 to 0.5% by mass with respect to the total amount of the electromagnetic wave absorber. .
2. The electromagnetic wave absorber for an anechoic chamber according to claim 1, wherein the value ″ of the imaginary part of the complex relative permeability at a frequency of 30 MHz is 213 to 530.
The value of the imaginary part of the complex relative permeability at a frequency of 30 MHz to 70 MHz μ "is 28.5 M / f to 31.5 M / f [where M is the imaginary part of the complex relative permeability at 30 MHz and f is the frequency (MHz)] The electromagnetic wave absorber for an anechoic chamber according to claim 1 or 2, wherein:
The thickness of the radio wave absorber satisfies 1.51 / M to 1.67 / M (m) (where M is an imaginary part of the complex relative permeability at 30 MHz). The electromagnetic wave absorber for an anechoic chamber according to claim 1.