JP2005268368A - Li-Zn GROUP FERRITE POWDER FOR WAVE ABSORBER AND THE SAME - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide ferrite powder and a wave absorber by which wave absorbing performance in a frequency band of 1 to 4 GHz can be sharply improved. <P>SOLUTION: The Li-Zn group ferrite powder for the wave absorber consists of ferrite expressed by a constitutional formula Zn<SB>X</SB>Li<SB>(1-X)0.5</SB>Fe<SB>(1-X)0.5</SB>-Fe<SB>2</SB>O<SB>4</SB>(X is 0.1 to 0.8), and preferably the average grain size is ≤2 μm. The wave absorber is obtained by dispersing the powder consisting of the Li-Zn group ferrite expressed by the constitutional formula Zn<SB>X</SB>Li<SB>(1-X)0.5</SB>Fe<SB>(1-X)0.5</SB>-Fe<SB>2</SB>O<SB>4</SB>(X is 0.1 to 0.8) and having the average grain size of 2 μm and less into high molecular matrixes at a rate of 60 to 95 wt%. The wave absorber is effective when it is arranged in the vicinity of an electronic component which is used in the frequency band of 1 to 4 GHz. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

  The present invention relates to a Li-Zn ferrite powder excellent in radio wave absorption characteristics in the 1-4 GHz band and a radio wave absorber using the powder.

  In recent years, communication devices using radio waves in the 1 to 4 GHz band such as mobile phones and wireless LANs have rapidly spread, and those in which the CPU of a computer is driven at a clock frequency of 1 GHz or more have become widespread. In order to effectively prevent malfunctions and mutual interference of these electronic devices, there is a strong demand for the appearance of a radio wave absorber that significantly improves the radio wave absorption performance in the 1 to 4 GHz band.

  Generally, a sheet material formed by mixing a radio wave absorbing powder in a polymer matrix such as a synthetic rubber is used for the radio wave absorber. As the radio wave absorptive powder, ferrite powder is widely used, and various radio absorptive ferrites are put into practical use according to the frequency band. For example, for a frequency band of 5 GHz or more, element substitution type Ti-Co system (5 to 15 GHz), Ti-Mn system (8 to 18 GHz), W type Zn-Sn-Mn system (5 to 19 GHz), A Y-type Co—Zn system (9 to 17 GHz) and the like are known. On the other hand, soft ferrites such as Mn-Zn, Cu-Zn, and Ni-Zn are known as ferrite that can be used in the 0.1 to 2 GHz band.

The following Patent Document 1 describes a microwave absorber using a ferrite powder having a general formula MFe ₂ O ₄ (M is Mn, Ni, Cu, Zn, Mg, Co). Among these, the ferrite powder that can be used in the 1 to 4 GHz band is limited to those having a considerably large particle size of several tens of μm to 1.65 mm. Such a powder having a large particle size is difficult to uniformly disperse in a polymer matrix, and is not suitable for obtaining a thin and high-performance radio wave absorber. In addition, in the ferrite where the M part of the above general formula is simply composed of a divalent metal such as Mn, Ni, Cu, Zn, Mg, Co, etc., a fine particle size powder having excellent radio wave absorptivity in the 1-4 GHz band. It is difficult to get. In fact, according to the disclosure of Patent Document 1, the usable frequency band is shifted to 6 to 12 GHz when the particle size is as small as less than 43 μm.

  Patent Document 2 below describes a ferrite / rubber-based electromagnetic wave absorber using Mn—Zn-based ferrite powder. This is a radio wave absorber for the 800 MHz to 1 GHz band and does not exhibit high performance in the 1 to 4 GHz band. In addition, ferrite powder having a particle size of 5 to 20 μm is disclosed as the ferrite powder used in this, but in view of dispersibility in a polymer matrix, a finer particle is desired.

Japanese Patent Publication No. 55-35002 Japanese Patent Laid-Open No. 5-299882

As described above, most of the electromagnetic wave absorbing ferrite powders that have been developed in the past are of a type exhibiting high performance in a band of 5 GHz or higher, or a band of 1 GHz or lower. Basically, these types are used for the 1-4 GHz band. It is a situation that must divert things. These conventional ferrite powders cannot be said to exhibit radio wave absorption performance that can sufficiently meet recent needs in the frequency band of 1 to 4 GHz.
In view of the current situation, the present invention aims to use in the 1 to 4 GHz band, develops and provides a new ferrite powder capable of greatly improving the radio wave absorption performance in this frequency band, and the ferrite An object is to provide a radio wave absorber using powder.

  As a result of various studies, the inventors have found that when a Li-Zn soft ferrite having a specific composition is used, the radio wave absorption performance in the 1-4 GHz band is greatly improved. Further, it was found that the ferrite powder has a characteristic of improving the radio wave absorption performance in the 1 to 4 GHz band in the state of fine particles having a particle diameter of 2 μm or less. Such fine ferrite powder is advantageous for improving dispersibility in the polymer matrix. The present invention has been completed based on these findings.

That is, in order to achieve the above object, from the ferrite represented by the structural formula of Zn _X Li _{(1-X) 0.5} Fe _(1-X) 0.5.Fe ₂ O ₄ (X is 0.1 to 0.8). An Li-Zn ferrite powder for a radio wave absorber is provided. Further, as a preferred embodiment thereof, a ferrite powder having an average particle size of 2 μm or less is provided.
Here, as the “average particle size”, “HELOS 50% particle size” measured by a laser diffraction type particle size distribution measuring apparatus using Franforfer diffraction theory can be adopted.

Also, the powder of Li-Zn ferrite represented by the structural formula of Zn _X Li _{(1-X) 0.5} Fe _(1-X) 0.5.Fe ₂ O ₄ (X is 0.1 to 0.8) is increased. An electromagnetic wave absorber dispersed in a molecular matrix is provided. As a preferred embodiment thereof, there is provided a powder in which a powder composed of the Li—Zn ferrite and having an average particle diameter of 2 μm or less is dispersed in a polymer matrix in a proportion of 60 to 95% by mass.
Here, the “polymer matrix” refers to a substance composed of a polymer compound.

In addition, these radio wave absorbers, particularly, radio wave absorbers installed near electronic components used in the frequency band of 1 to 4 GHz are provided.
Here, “installed in the vicinity of an electronic component” means that i) absorbs 1 to 4 GHz radio waves leaking from the electronic component to prevent adverse effects on other electronic components or equipment outside the casing, Or, ii) means that it is installed in the vicinity of the electronic component so as to achieve the purpose of absorbing external radio waves of 1 to 4 GHz and preventing the adverse effect on the electronic component.

According to the present invention, it is possible to obtain a radio wave absorber that greatly improves the absorption performance of radio waves in the 1-4 GHz band. Moreover, since such an improvement can be made by using fine ferrite powder having an average particle diameter of 2 μm or less, uniform dispersion in the polymer matrix is easily obtained, and stable performance can be achieved even in a thin wave absorber. Secured.
Accordingly, the present invention has become widespread in recent years, including cellular phones (1.5 GHz band), PHS (1.9 GHz band), wireless LAN (eg, 2.45 GHz band), and CPUs for personal computers driven at a clock frequency of 1 GHz or higher. Can contribute to the prevention of radio wave interference in various electronic devices used at frequencies of 1 to 4 GHz.

  The electromagnetic wave absorber includes a “magnetic powder mixed type” and a “conductive powder mixed type”. The object of the present invention is the former “magnetic powder mixed type”. In this type, a molded product in which a magnetic powder such as ferrite is mixed with a polymer compound is integrated and acts on the magnetic field component of the radio wave due to the imaginary part μ ″ (magnetic loss term) of the complex permeability. It converts radio wave energy into heat. For this reason, the amount of radio wave absorption increases as the imaginary part μ ″ of the complex permeability increases.

In the present invention, the structure of Zn _X Li _{(1-X) 0.5} Fe _(1-X) 0.5.Fe ₂ O ₄ (X is 0.1 to 0.8) is used as the magnetic powder to be mixed with the polymer compound. Li-Zn type soft ferrite represented by the formula is adopted. This has a form in which a part of Zn in the Zn soft ferrite is replaced with Li, and the replacement makes it possible to match the peak of the radio wave absorption performance to the 1 to 4 GHz band. That is, a molded body obtained by mixing this ferrite powder with a polymer compound exhibits a high value of the imaginary part μ ″ of the complex permeability in the frequency band of 1 to 4 GHz, and is excellent in radio wave absorption performance in this band. .

In the structural formula, if the value of X is less than 0.1, necessary magnetism cannot be obtained. On the other hand, if it exceeds 0.8, the imaginary part μ ″ of the complex permeability in the 1 to 4 GHz band is lowered, and sufficient radio wave absorption performance cannot be secured. Therefore, it is necessary to use ferrite whose composition is adjusted to a value in the range of 0.1 to 0.8.
As a result of various studies, it was found that the absorption performance of radio waves in the 1 to 4 GHz band tends to be highest when the value of X is approximately 0.5. Therefore, the value of X is preferably in the range of 0.3 to 0.7, and more preferably in the range of 0.4 to 0.6.

  The inventors have also studied the influence of the particle size of the Li-Zn ferrite powder. As a result, μ ″ in the 1-4 GHz band could be significantly increased in a fine powder having an average particle size of 2 μm or less. However, when the average particle diameter is less than 1 μm, μ ″ in the 1 to 4 GHz band tends to slightly decrease. Therefore, in order to achieve both the dispersibility in the polymer matrix and the radio wave absorption performance in a balanced manner, it is desirable to adjust the average particle size to 1 to 2 μm.

  The Li-Zn ferrite powder of the present invention can be manufactured according to a general soft ferrite manufacturing method. For example, iron oxide, zinc oxide, and lithium carbonate are weighed so as to have a predetermined ferrite composition in terms of oxide, stirred and mixed, then fired, and the resulting fired product is pulverized with a mill. Can be manufactured. At that time, the firing temperature is desirably in the range of 850 to 1000 ° C. so that Li does not volatilize.

  After the obtained Li-Zn ferrite powder is sufficiently kneaded with a polymer compound at a predetermined ratio, for example, if formed into a sheet having a certain thickness, a radio wave absorber having high performance in the 1-4 GHz band is obtained. be able to. At this time, if a powder having an average particle size adjusted to 2 μm or less is used, good kneadability with an organic polymer is secured, which is advantageous in making the dispersed state of ferrite uniform. In particular, the use of a ferrite powder having an average particle size adjusted to a range of 1 to 2 μm is effective because the radio wave absorption performance can be maintained as high as possible.

  Further, it is preferable to use a Li—Zn ferrite powder having an average particle diameter of 2 μm or less and to disperse the ferrite powder in the polymer matrix at a ratio of 60 to 95% by mass. If the proportion of the Li—Zn ferrite powder is less than 60% by mass, both the real part μ ′ and the imaginary part μ ″ of the complex permeability are lowered, and sufficient radio wave absorption performance cannot be obtained. On the other hand, if it exceeds 95% by mass, kneading with the organic polymer becomes difficult. A particularly preferable mixing ratio of the Li—Zn ferrite powder is 80 to 95% by mass, and a more preferable mixing ratio is 85 to 95% by mass.

  As the polymer compound to be mixed with the Li-Zn ferrite powder of the present invention, various compounds satisfying heat resistance, flame retardancy, durability, mechanical strength and electrical characteristics can be used. For example, an appropriate material may be selected from resin (nylon or the like), gel (silicone gel or the like), thermoplastic elastomer, rubber or the like. Moreover, a polymer matrix can also be comprised with the composition which blended 2 or more types of polymer compounds.

In order to improve the compatibility and dispersibility with the polymer compound, the ferrite powder can be subjected to surface treatment with a silane coupling agent, a titanate coupling agent or the like in advance.
In addition, various additives such as a plasticizer, a reinforcing agent, a heat resistance improver, a heat conductive filler, and an adhesive can be added when mixing the ferrite powder and the polymer compound.

  Incidentally, it is generally said that the vicinity of the substrate of the electronic component is a region where the magnetic field component is strong among the electromagnetic field components. As described above, the “magnetic powder mixed type” radio wave absorber targeted by the present invention increases the effect on the magnetic field component of the radio wave by increasing the imaginary part μ ″ (magnetic loss term) of the complex permeability. The electromagnetic wave absorption performance is improved. Therefore, it is effective to place the radio wave absorber near an electronic component having a strong magnetic field component as much as possible. Although there are many restrictions on the place where the radio wave absorber is installed due to the downsizing of electronic equipment, it is desirable that the radio wave absorber of the present invention be installed as close as possible to electronic components used in the frequency band of 1 to 4 GHz.

Weigh iron oxide (Fe ₂ O ₃ ), zinc oxide (ZnO) and lithium carbonate (LiCO ₃ ) so that they have a composition of Zn _0.5 Li _0.25 Fe _0.25 · Fe ₂ O ₄ in terms of oxide. Mixed. The mixing method was a two-stage mixing process in which mixing was performed using a high speed mixer and then further mixing was performed using a 10 L vibration mill. The obtained mixture was put into an electric furnace (roller house furnace) and baked at 920 ° C. The fired product is pulverized using a mill (SK-M10, manufactured by Kyoritsu Riko Co., Ltd.), and Li-Zn ferrite powder having a HELOS 50% particle size of 1.57 μm (structural formula: Zn _0.5 Li _0.25 Fe _0.25 · Fe ₂ O ₄ ) was obtained. This is called “powder A”.

Next, a part of the powder A was further finely pulverized using a dry vibration mill (manufactured by Chuo Kako Co., Ltd., 3L-VM) to obtain a Li-Zn ferrite powder having a HELOS 50% particle size of 0.97 μm. This is referred to as “powder B”.
For measurement of the particle diameter, a HELOS & RODOS laser diffraction particle size distribution measuring device manufactured by JEOL Ltd. was used.

For comparison, a commercially available Zn—Cu based soft ferrite powder (structural formula: Zn _0.5 Cu _0.5 · Fe ₂ O ₄ , average particle diameter: 23.9 μm) was prepared. This is referred to as “powder C”.

85% by mass of each ferrite powder and 15% by mass of NBR rubber-based resin were kneaded at 80 ° C. for 10 minutes with a lab plast mill (manufactured by Toyo Seiki Co., Ltd., R-60), once discharged, and again kneaded under the same conditions. For powder A, a powder mixture ratio of 90% by mass (the balance being NBR rubber resin) was also prepared. The obtained kneaded material was rolled to a thickness of 2 mm with a 6-inch diameter electrothermal rolling roll to obtain a total of four types (powder A; two types, powders B and C; one type each) of radio wave absorber sheets.
Table 1 shows the configuration of each sheet.

The obtained radio wave absorber sheet was examined for radio wave absorption characteristics by the S parameter method. A small piece cut out from each sheet is formed into a cylindrical measurement piece having an outer diameter of 7 mm and an inner diameter of 3 mm, and this is inserted into a φ7 mm × φ3.04 mm coaxial tube, and a network analyzer (trade name: HP85071B, manufactured by Hewlett-Packard Company). The reflection / transmission coefficient (S parameter) was measured over 1 to 11 GHz.
1 to 4 show the frequency dependence of the real part μ ′ and the imaginary part μ ″ of the complex permeability for each sheet.

Further, based on the measured S parameter, the return loss at 1.9 GHz when a sheet having a thickness of about 6 to 7 mm was used was simulated.
Table 2 shows the simulation results.

  Comparing FIG. 1 and FIG. 4, the sheet using the Li-Zn ferrite of the present invention (FIG. 1) is the same as the conventional material (FIG. 4), despite using fine grain ferrite having an average grain size of 2 μm or less. In comparison, it can be seen that μ ″ in the 1-4 GHz band is significantly increased. That is, the radio wave absorption performance in the 1-4 GHz band can be greatly improved.

  When FIG. 1 and FIG. 2 are compared, by increasing the blending amount of the Li-Zn ferrite powder in the sheet to 90% by mass (FIG. 2), μ ″ in the 1-4 GHz band can be further significantly increased. Understand.

  Comparing FIG. 1 and FIG. 3, it can be seen that when the average particle size of the Li-Zn ferrite powder is refined to less than 1 μm (FIG. 3), μ ″ slightly decreases particularly in the 1-2 GHz band. Nevertheless, the level is still considerably higher than that of the conventional material shown in FIG.

  In addition, from Table 2, the sheet of the present invention example using the Li-Zn ferrite powder can exhibit extremely excellent radio wave absorption performance in the 1-4 GHz band as compared with the comparative example (conventional material). Understand. For example, a sheet 2 (example of the present invention) having a thickness of 6.0 mm has a large amount of radio wave absorption at 1.9 GHz and about 20 dB or more compared to a sheet 4 (comparative example) having a thickness of 7.0 mm. .

  FIG. 5 shows an X-ray diffraction pattern using CoKα rays for the powder A of the present invention. From this pattern, it can be seen that the powder A is a ferrite having a spinel structure.

The graph which shows an example of the measurement result of the complex magnetic permeability (micro | micron | mu) 'and (micro | micron | mu)' 'in the electromagnetic wave absorber using the Li-Zn type ferrite powder of this invention. The graph which shows an example of the measurement result of the complex magnetic permeability (micro | micron | mu) 'and (micro | micron | mu)' 'in the electromagnetic wave absorber using the Li-Zn type ferrite powder of this invention. The graph which shows an example of the measurement result of the complex magnetic permeability (micro | micron | mu) 'and (micro | micron | mu)' 'in the electromagnetic wave absorber using the Li-Zn type ferrite powder of this invention. The graph which shows an example of the measurement result of the complex magnetic permeability (micro | micron | mu) 'and (micro | micron | mu)' 'in the electromagnetic wave absorber using the conventional Cu-Zn type ferrite powder. The graph which shows an example of the X-ray-diffraction pattern about the Li-Zn type ferrite powder of this invention.

Claims (5)

Li-Zn for electromagnetic wave absorbers made of ferrite represented by the structural formula of Zn _X Li _{(1-X) 0.5} Fe _{(1-X) 0.5} -Fe ₂ O ₄ (X is 0.1 to 0.8) Ferrite powder.   The Li-Zn ferrite powder for a radio wave absorber according to claim 1, wherein the average particle size is 2 µm or less. Zn _X Li _{(1-X) 0.5} Fe _{(1-X) 0.5} · Fe ₂ O ₄ (X is 0.1 to 0.8) structural formula Li-Zn ferrite powder Radio wave absorber dispersed inside. Zn _X Li _{(1-X) 0.5} Fe _(1-X) 0.5.Fe ₂ O ₄ (X is 0.1 to 0.8) The average particle diameter of the Li-Zn ferrite represented by the structural formula A radio wave absorber in which a powder of 2 μm or less is dispersed in a polymer matrix in a proportion of 60 to 95% by mass.   The radio wave absorber according to claim 3 or 4 installed in the vicinity of an electronic component used in a frequency band of 1 to 4 GHz.

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