CN1521770A - Fe2O3含量低于50摩尔%的Mn-Zn铁氧体 - Google Patents
Fe2O3含量低于50摩尔%的Mn-Zn铁氧体 Download PDFInfo
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Abstract
一种Mn-Zn铁氧体,包括的基本组分为44.0-49.8摩尔%的Fe2O3,4.0-26.5摩尔%的ZnO,0.8摩尔%或更少的Mn2O3,余下的为MnO;含有0.20(不含0.20)-1.00质量%的CaO作添加剂;由于该Mn-Zn铁氧体中,Fe2O3的含量低于50.0摩尔%,并含有有限量的Mn2O3 (0.8摩尔%或更低),甚至当CaO的含量超过0.20质量%时也不会产生反常的晶粒生长,可以得到高的电阻。因此可在如1MHz的高频段下实现优异的软磁性。
Description
技术领域
本发明涉及一种典型的软磁性氧化物磁材料,更具体地,涉及一种适于用作用于开关电源,各种电感元件,EMI对抗中的阻抗元件,电磁波吸收件等的低耗材料的Mn-Zn铁氧体。
背景技术
Mn-Zn铁氧体是典型的软磁性氧化物磁材料之一,通常包含的基本组分为:Fe2O3超过50.0摩尔%的化学计量,平均为52.0-55.0摩尔%;ZnO为10.0-24.0摩尔%;剩余部分由MnO组成,通常这样制造,按预定混合配比称量Fe2O3,ZnO和MnO生料粉末,将其混合,煅烧,研磨,调节组分,造粒,然后压成具有预定形状的生坯,将生坯于还原气氛中在1200-1400℃的温度下烧结2-4小时,气氛中的氧分压通过依据(1)式往炉中充入氮气来进行控制,然后在相同的气氛下冷却;
这里T是温度(℃),PO2是氧分压,b是常数(通常设为7-8)。
通常,正如所知,Mn-Zn铁氧体中的锰(Mn)组分可以以Mn3+或者Mn2+存在,Mn3+和Mn2+之间的丰度比依赖于烧结时气氛中的氧分压,Mn3+显著破坏Mn-Zn铁氧体的软磁性。而且已知在Mn3+和Mn2+之间发生的电子转移会引起电阻的下降。因此,为了制造出具有优异的软磁性和高电阻的Mn-Zn铁氧体,必须控制烧结气氛(氧分压)以使Mn3+的生成最小化,并且考虑到工业可行的实质性,将上述(1)式中的常数b设在7-8之间。常数b设在7-8实际上意味着烧结时的氧分压必须控制在一个很窄的范围内,这使烧结步骤因生产成本上升而变得非常棘手。
在传统的Fe2O3含量超过50.0摩尔%的通用Mn-Zn铁氧体中,铁(Fe)组分可以Fe3+或Fe2+存在,当Mn-Zn铁氧体在上述还原气氛下烧结时,Fe3+被部分还原成Fe2+,Fe2+具有正的磁晶各向异性,可以抵消Fe3+的负的磁晶各向异性,因此提高了软磁性,但正像锰(Mn)组分那样,在Fe3+和Fe2+之间发生的电子转移会显著降低电阻。
近来,随着越来越多的具有更高性能和更小尺寸的电子设备的出现,形成的处理信号的频率更高了,所以需要有在高频段显示出优异磁特性的磁材料。用Mn-Zn铁氧体制成的磁芯,在较高的频率下涡电流会增加,因此会增加损耗。结果,为使Mn-Zn铁氧体在最高频的下起到作为磁芯材料的充分功能成为可能,需要使其电阻(电阻率)最大化。然而,由于传统的Mn-Zn铁氧体中Fe2O3含量超过50mol%(化学计量组分),存在的Fe2+数量很大,这加速了Fe3+和Fe2+(离子)之间的电子转移。结果,电阻率低于大约1Ωm的数量级,所以Mn-Zn铁氧体的充分工作只能最高到几百kHz的频率,再往上,其起始磁导率显著降低,因此其作为软磁性材料的特性全部消失。
在此环境下,公开号为H07-230909和H10-208926的日本专利申请中公开了一种Fe2O3含量低于50.0摩尔%,并含有CaO和SiO2作添加剂以提高电阻的Mn-Zn铁氧体。
在上述公开号为H07-230909和H10-208926的日本专利申请中公开的Mn-Zn铁氧体被指定用作一种偏转轭的磁芯材料,所以倾向于仅仅能用到最高100kHz的频率(参照这些日本专利申请中的实施方案),不能确保该Mn-Zn铁氧体可以在超过1MHz的高频段具有优异的磁性能(软磁性)。结果,该Mn-Zn铁氧体在超过1MHz的高频段不能成功地用作磁芯材料。上述公开号为H07-230909的日本专利申请表明在此Mn-Zn铁氧体中可以含有最高达0.50重量%的CaO和SiO2,但其中讨论的实施例包含的CaO少于0.10重量%,这样这些实施例中没有一个含有的CaO超过0.20质量%。并且,其中描述,可以加入适量的Mn2O3以使其与Fe2O3的总量在大约50.0摩尔%,但由于该Mn-Zn铁氧体含有的Fe2O3为45.0-48.5摩尔%,为达到50.0摩尔%,要加入1.4-5.0摩尔%的Mn2O3(即Mn3+)。如果包含了如此大数量的Mn3+,很难使Mn-Zn铁氧体同时满足软磁性和电阻的需要。
发明简述
本发明是考虑到上述问题而做出的,本发明的一个目的就是提供一种具有高电阻,并在超过1MHz的高频段下显示出优异软磁性的Mn-Zn铁氧体。
为了实现这一目的,在本发明的一个方面,Mn-Zn铁氧体包括的基本组分为:44.0-49.8摩尔%的Fe2O3,4.0-26.5摩尔%的ZnO,0.8摩尔%或更少的Mn2O3,剩余的为MnO,包含0.20(不含0.20)-1.00质量%的CaO作添加剂,具有的电阻率为1.5×104Ωm或更大,表面电阻为1.5×107Ω或更大。
在本发明的这一方面,FeO含量可以是0.2摩尔%或更低。
在本发明的这一方面,该Mn-Zn铁氧体可以进一步包含0.01-0.10质量%的SiO2作添加剂。
在本发明的这一方面,该Mn-Zn铁氧体可以进一步包含0.01-0.20质量%的V2O5,0.01-0.20质量%的MoO3,0.01-0.20质量%的ZrO2,0.01-0.20质量%的Ta2O5,0.01-0.20质量%的HfO2,0.01-0.20质量%的Nb2O5和0.01-6.00质量%的CuO中的至少一种作添加剂。
由此,由于依据本发明的该Mn-Zn铁氧体含有少于50.0摩尔%的Fe2O3以及有限数量(0.8摩尔%或更少)的Mn2O3,即使CaO含量超过了0.20质量%,也不会发生反常的晶粒生长,且可以得到高的电阻(电阻率为1.5×104Ωm或更高,表面电阻为1.5×107Ω或更大)。并且由于含有适量的TiO2和/或SnO2,可以将初始磁导率保持足够高,因此可在比如1 MHz的高频段下获得优异的软磁性。
具体实施方案
如上所述,当传统的Fe2O3含量高于50.0摩尔%的通用的Mn-Zn铁氧体在通过将(1)式中的常数b设定在7-8控制的还原气氛中烧结时,已知会破坏软磁性的Mn3+几乎不会产生,但会产生已知能显著降低电阻的Fe2+,因为超过50.0摩尔%的那些Fe2O3(即Fe3+)被还原了。另一方面,由于本发明中的Mn-Zn铁氧体包含的Fe2O3低于50.0摩尔%,具体地为44.0-49.8摩尔%,当该Mn-Zn铁氧体在通过将(1)式中的常数b设定在7-8控制的还原气氛中烧结时,Fe2+几乎不能生成。
Mn3+使晶格扭曲,因而显著降低了初始磁导率,并且引起电阻下降。本发明的Mn-Zn铁氧体包含0.8摩尔%或更低的Mn2O3(即Mn3+),因而可以防止软磁性和电阻的破坏。
这样,本发明中的Mn-Zn铁氧体使得造成电阻显著降低的Fe2+的产生受到抑制,同样也抑制了引起软磁性的破坏和电阻下降的Mn3+的生成,因此成功获得了优异的软磁性和高的电阻。具体地,得到的电阻率为1.5×104Ωm或更高,表面电阻为1.5×107Ω或更大。Mn-Zn铁氧体中的铁组分,包括FeO(Fe2+),通常用Fe2O3表示,并且由于如上所述Fe2+会极大地导致电阻的降低,FeO的含量优选设在0.2摩尔%或更低。
ZnO作为Mn-Zn铁氧体的一种基本组分,可以影响居里温度和饱和磁化强度。具体地,太小的ZnO含量会使初始磁导率降低,然而,太大的ZnO含量会引起居里温度和饱和磁化强度的降低。由于用在电源变压器中的铁氧体经常暴露在80-100℃的温度下,将居里温度和饱和磁化强度保持在很高是重要的,所以,如上所述,将ZnO的含量设在4.0-26.5摩尔%的范围。
如上所述,本发明的Mn-Zn铁氧体含有超过0.20质量%的CaO作添加剂。CaO会在晶粒边界上偏析,并引起电阻的提高,但当CaO含量超过0.20质量%时,会产生导致磁特性严重破坏的反常的晶粒生长。因此,为防止这种反常晶粒生长的产生,在传统的Mn-Zn铁氧体中,CaO的含量设在不大于0.20质量%。另一方面,在本发明的Mn-Zn铁氧体中,Fe2O3的含量设在49.8摩尔%(低于50.0摩尔%,即化学计量组分)或更低,同时将Mn2O3的含量设在微量(0.8摩尔%或更低),而且按需要也可含有微量的FeO(0.2摩尔%或更低)。因此,甚至当CaO的含量超过0.20质量%时也不会产生反常的晶粒生长。为了提高电阻,CaO的含量优选设在大于0.50质量%,但太大的含量会引起软磁性的破坏,所以CaO的含量设定在0.20(不含0.20)-1.00质量%的范围内。SiO2也能有效地提高电阻,所以按需要可以包含0.01-0.10质量%的SiO2。
本发明的Mn-Zn铁氧体可以进一步包含V2O5,MoO3,ZrO2,Ta2O5,HfO2,Nb2O5和CuO中的至少一种作添加剂。这些组分能有效地帮助烧结作用并提高电阻,但当含量太小时并不十分有效,然而当含量太大时反而会引起反常的晶粒生长。因此,V2O5,MoO3,ZrO2,Ta2O5,HfO2和Nb2O5的含量优选设定在0.01-0.20质量%的范围,CuO的含量设在0.01-6.00质量%的范围。
本发明的Mn-Zn铁氧体可以在通过将(1)式中的常数b从7-12的范围内适当选择来控制氧分压的还原气氛中烧结并冷却。这意味着本发明的Mn-Zn铁氧体采用的气氛与传统Mn-Zn铁氧体采用的其中常数b通常选自7-8的范围的气氛相比可以方便地控制。结果,生产成本降低。此时,如果常数b设定超过了12,那么铁氧体中的Mn3+的含量就会超过0.8摩尔%,初始磁导率就会迅速下降。
在制造本发明的Mn-Zn铁氧体时,将基本组分Fe2O3,ZnO和MnO的原材料粉末按预定混合比进行称量,混合,煅烧和研磨。依据目标组分,煅烧进行的温度适当的确定在800-1000℃之间,用通用球磨,磨碎机或类似设备进行研磨。将经过如上处理的原材料粉末进一步与适量的CaO,SiO2以及其它可能需要的添加剂相混合,以得到具有目标组分的混合物粉末。依据一般的制造方法将该混合物粉末进行造粒,比如加入粘结剂,像聚乙烯醇,聚丙稀酰胺,甲基纤维素,聚环氧乙烷,甘油以及其它的相似剂,然后在如80MPa或更高的压力下将其压成生坯。在炉中将生坯在1000-1300℃的温度下,于通过充入惰性气体如氮气控制氧分压的气氛中烧结,并在相同的气氛中冷却。在烧结和冷却步骤中,(1)式中的常数b从7-12的范围内进行选择,这与烧结传统的Fe2O3含量超过50.0摩尔%的Mn-Zn铁氧体限定的7-8的范围相比具有显著宽松的可调性。结果,可以更容易地控制氧分压,并且由于在低于500℃的温度下,无论氧含量如何,氧化或者还原反应都是可以忽略的,所以在气氛的温度冷到500℃以下时,就不必依照(1)式来对气氛进行控制了。
实施例
按表1所示的组分制造9种不同的测试样品,其中包括2种对比样品。将原材料粉末Fe2O3,ZnO和MnO进行混合,用磨碎机搅拌,在空气中于850℃下煅烧2小时,用磨碎机研磨1小时,得到混合物粉末。然后,将CaO,SiO2,CuO,Nb2O5,V2O5和ZrO2粉末适当的加入到混合物粉末中调节组分,然后将调节后的混合物粉末用磨碎机搅拌1小时,加入聚乙烯醇造粒,在80MPa的压力下压成环形芯(生坯),每个外径25mm,内径15mm,高度5mm。将生坯在1200℃下烧结2小时然后在炉中冷却,其中的气氛通过往炉中充入氮气来进行控制,以得到(1)式中常数b设在9时的氧分压。获得了本发明的样品1-7和对比样品1-2。
将如上制得的样品进行荧光X射线分析以得到各自的最终组分组成,滴定测量它们中的Mn2O3和FeO含量,如表1中所示。测量它们在1MHz下的初始磁导率,电阻率和表面电阻,结果在表1中列出。
表1
样品分类 | 基本组分(摩尔%) | 滴定组分(摩尔%) | 添加剂组分(摩尔%) | 初始磁导率 | 电阻率(Ωm) | 表面电阻(Ω) | |||||
Fe2O3 (1) | MnO(2) | ZnO | Mn2O3 | FeO | CaO | SiO2 | 其它 | ||||
对比样品1 | 51.0 | 36.8 | 12.2 | 1.2 | 0.8 | 0.10 | 0.04 | - | 40 | 1.1×101 | 1.2×102 |
发明样品1 | 49.8 | 37.7 | 12.5 | 0.6 | 0.2 | 0.25 | ″ | - | 720 | 1.6×104 | 1.7×107 |
发明样品2 | 47.0 | 40.0 | 13.0 | 0.4 | 0.1 | 1.00 | ″ | - | 820 | 6.1×104 | 8.5×107 |
对比样品2 | ″ | ″ | ″ | ″ | ″ | 1.50 | ″ | - | 330 | 1.2×101 | 1.4×101 |
发明样品3 | ″ | ″ | ″ | ″ | ″ | 0.60 | - | CuO:1.00 | 790 | 3.8×106 | 2.9×108 |
发明样品4 | ″ | ″ | ″ | 0.3 | ″ | ″ | - | Nb2O5:0.05 | 800 | 3.5×105 | 2.7×108 |
发明样品5 | ″ | ″ | ″ | ″ | ″ | ″ | - | V2O5:0.05 | 890 | 3.6×106 | 2.6×108 |
发明样品6 | ″ | ″ | ″ | 0.2 | ″ | ″ | 0.04 | ZrO2:0.05 | 830 | 3.4×105 | 2.6×108 |
发明样品7 | 44.0 | 42.8 | 13.2 | 0.1 | 0 | 0.80 | ″ | - | 810 | 4.4×104 | 3.2×108 |
注释:(1)Fe2O3指FeO和Fe2O3
(2)MnO指Mn2O3和MnO
从表1可以看出,所有的发明样品1-7中含有低于0.8摩尔%的Mn2O3和0.2摩尔%或更低的FeO,并且具有超过700的初始磁导率和大于1.5×104Ωm的电阻率以及大于1.5×107Ω的表面电阻,这些证明获得了优异的软磁性和高的电阻。
另一方面,对比样品1由传统的Fe2O3含量大于50.0摩尔%的通用的Mn-Zn铁氧体制成,所以其具有的电阻显著降低,对比样品2含有大量的CaO,所以产生了反常的晶粒生长,其具有的初始磁导率显著降低。
尽管已依据具体的实施方案对本发明进行了阐释,应该明白本发明并不局限此,而是包括了在所附权利要求范围内的所有可能的更改和完善。
Claims (4)
1.一种Mn-Zn铁氧体:包括的基本组分为44.0-49.8摩尔%的Fe2O3,4.0-26.5摩尔%的ZnO,0.8摩尔%或更少的Mn2O3,余下的为MnO;含有0.20(不含0.20)-1.00质量%的CaO作添加剂;具有的电阻率为1.5×104Ωm或更大,表面电阻为1.5×107Ω或更大。
2.权利要求1中的Mn-Zn铁氧体,其中FeO的含量为0.2摩尔%或更少。
3.权利要求1或2中的Mn-Zn铁氧体,进一步包含0.01-0.10质量%的SiO2作添加剂。
4.权利要求1至3任意之一中的Mn-Zn铁氧体,进一步含有0.01-0.20质量%的V2O5,0.01-0.20质量%的MoO3,0.01-0.20质量%的ZrO2,0.01-0.20质量%的Ta2O5,0.01-0.20质量%的HfO2,0.01-0.20质量%的Nb2O5和0.01-6.00质量%的CuO中的至少一种作添加剂。
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CN102982954A (zh) * | 2012-11-23 | 2013-03-20 | 天长市昭田磁电科技有限公司 | 一种含有HfO2的铁磁芯的制造方法 |
WO2013174100A1 (zh) * | 2012-05-25 | 2013-11-28 | 南通华兴磁性材料有限公司 | 一种用于宽频抗电磁干扰的锰锌铁氧体材料及其制造方法 |
CN103693951A (zh) * | 2013-09-02 | 2014-04-02 | 横店集团东磁股份有限公司 | 一种抗电磁干扰的锰锌铁氧体材料及其制备方法 |
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CN102982954B (zh) * | 2012-11-23 | 2016-11-02 | 天长市昭田磁电科技有限公司 | 一种含有HfO2的铁磁芯的制造方法 |
CN103693951A (zh) * | 2013-09-02 | 2014-04-02 | 横店集团东磁股份有限公司 | 一种抗电磁干扰的锰锌铁氧体材料及其制备方法 |
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CN111138180A (zh) * | 2019-12-25 | 2020-05-12 | 江门安磁电子有限公司 | 一种宽频高阻抗锰锌铁氧体材料及其制备方法 |
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