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低B_r纳米晶Fe_(73.5)Cu_1Nb_2V_1Si_(13.5)B_9合金的中、高频损耗行为

Behavior of Medium-and High-frequency Core Loss in Nanocrystalline Fe_(73.5) Cu_1Nb_2V_1Si_(13.5)B_9 Alloy with Low B_r
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摘要 在 f=2 0~ 10 3kHz和Bm =0 0 5 ~ 1 0T的范围内 ,考查了低Br 纳米晶合金的每周损耗的频率关系。结果表明 ,在 0 2 ~ 5kHz的范围内 ,惯用的损耗分离原则适用 ,可用Bertotti的统计理论描述P/ f - f行为。大约在 3~ 5kHz以前的相当宽的中、高频区内 ,不能采用惯用的分离法。大致可分为三个区间 ,P/ f- f行为可很好地用P/ f=K(i)eclf +P(i)eh 型线性方程来描述。有效涡流系数K(i)ecl 比经典涡流系数Kcl小得多 ,也明显比高导磁态的K(i)ecl In the range of f =0 2~10 3kHz and B m=0 05~1 0T,the frequency dependence of the total power loss per cycle has been investigated for the nanocrystalline alloy with low B r The results show that the principle of loss decomposition used consistently is applicable and the behavior of P/f vs f can be described by using Bertotti's statistical theory in the range of 0 2~5kHz In the considerable wide medium and high frequency range about above 3~5kHz,the habitual method of loss separation is not applicable This wide interval can be approximately divided into three intervals,in which the behavior of P/f vs f can be well described by linear equation K (i) ecl f+P (i) eh  The effective eddy current coefficient K (i) ecl  is much smaller than the corresponding classical eddy current coefficient K cl ,and also is clearly smaller than the corresponding K (i) ecl  for the high permeability state
作者 张延忠
机构地区 上海钢铁研究所
出处 《金属功能材料》 CAS 2001年第5期18-24,共7页 Metallic Functional Materials
基金 国家非晶微晶合金工程技术研究中心资助
关键词 纳米晶合金 有效涡流损耗 有效磁滞损耗 磁导率 变压器 nanocrystalline alloy with low B r,effective eddy curren loss,effective hystersis loss
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