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作 者:韩志全[1]
出 处:《磁性材料及器件》2013年第1期73-78,共6页Journal of Magnetic Materials and Devices
摘 要:微波铁氧体的饱和磁化强度Ms是器件设计者选择材料的重要参数之一,但是一些文章常将Bm、Bs与Ms混为一谈,本文旨在讨论这一问题。软磁铁氧体材料因为磁晶各向异性常数K1非常低,饱和磁化场Hs低,其Bs通常由指定测量磁场Hm下测得的Bm(Hm Hs)来确定。为了说明微波铁氧体与软磁铁氧体的不同,给出了小线宽石榴石材料的磁化曲线和微波铁氧体材料的矫顽力,由此推知微波铁氧体材料的饱和磁化场Hs远高于磁滞回线的测量磁场Hm(5Hc 10Hc),相差2 3个数量级。由Li铁氧体的Bm/0Ms(Mm/Ms)63%81%和Mn:YIG的Bm/0Ms 81%86%,说明在Hm下材料磁畴中的磁矩中有14%37%不在磁场方向。因此对微波铁氧体来说,不能像在软磁铁氧体中那样有Bm Bs 0Ms的关系。所以为保证材料被磁化饱和,Ms的测量应该按照IEC60556标准在>300kA/m磁场下进行。最后讨论了经常将剩磁比R=Br/Bm误成Br/Bs问题。To device designers, the saturation magnetization Ms is one of important parameters of microwave ferrite materials. However, there were some confuses on the maximum magnetic flux density Bm, the saturation flux Bs and Ms in some papers, so the purpose of this article is to discuss this problem. To interpret the difference between soft ferrite and microwave ferrite, the magnetizing curve of the garnet with narrow linewidth and coercivities of commercial microwave materials are given, which shows that the saturation magnetizing field Hs for microwave ferrites is larger in order of 2 to 3 then the measuring field Hm(=SHc-10Hc) to the hysteresis loop measurement. By means of the fact that the ratio Bm/μoMs(≈Mm/Ms)〈63%-81% for Li ferrites and the ratio Bm/μoMs(≈Mm/Ms)〈81%-86% for the Mn:YIG, it is revealed that a percentage of 14% -37% of magnetizations in domains of the materials is not orientated by the measuring field Hm and it is indicated that the measured Bm can not be expressed as Bm≈Bs≈μoMs for microwave ferrites like as that in soft ferrites, and the Ms value of microwave ferrites should be determined at the measuring field H〉300kA/m to get the saturation state according to the IEC60556 standard. The problem of mistaking the remanence ratio R as Br/Bs is also discussed at the last.
关 键 词:饱和磁化强度Ms 饱和磁感应强度Bs 测量磁场 饱和磁化场 YIG 石榴石 LI铁氧体 剩磁比
分 类 号:TM277[一般工业技术—材料科学与工程] O482.54[电气工程—电工理论与新技术]
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