CN106636846A - 一种变磁性相变临界场降低的MnCoSi基合金 - Google Patents
一种变磁性相变临界场降低的MnCoSi基合金 Download PDFInfo
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Abstract
本发明公开了一种变磁性相变临界场降低的MnCoSi基合金,其成分为Mn1‑xCo1+xSi,其中0.01≤ x ≤0.015。本发明利用Co原子掺杂Mn原子,所得到的Mn1‑xCo1+xSi合金与正分的MnCoSi合金相比,变磁性相变即磁场诱发的螺旋反铁磁到高磁态转变临界场显著降低,其中优选的Mn0.985Co1.015Si合金,能使室温相变临界场降低至0.8 T,室温附近的磁致伸缩效应可逆且无磁滞。
Description
技术领域
本发明涉及一种相变临界场降低的MnCoSi基合金,属于合金制备领域。
背景技术
MnCoSi合金是一种新型无重稀土的巨磁致伸缩材料。其磁致伸缩效应大于现有的Terfenol-D多晶,且可逆无磁滞,具有较大的应用价值。然而MnCoSi合金的室温磁致相变临界场较高,约2.5 T。这大大阻碍了其可能的应用。因此,如何通过有效的方法降低MnCoSi合金的室温相变临界场是其应用的基本前提。
发明内容
本发明的目的是提供一种能有效降低相变临界场的MnCoSi基合金。
实现本发明目的的技术解决方案是:一种MnCoSi基合金,以原子百分比计,所述的合金表达式为Mn1-xCo1+xSi ,其中0.01≤ x ≤0.015。
其中,优选的MnCoSi基合金表达式为Mn0.985Co1.015Si。
与现有技术相比,本发明的优点是:
[1]Co原子掺杂部分的Mn原子,Co原子除了占据原先4c位(Wyckoff position)外,过量的Co原子将占据Mn位。
[2]等温磁化曲线反映出来的变磁性临界场随着Co原子含量的增加而显著降低,其中优选的Mn0.985Co1.015Si合金可以有效将合金的室温相变临界场降低至0.8 T(相变临界场指50 %饱和磁化强度对应的外场大小)。
[3]合金室温磁化曲线无磁滞且室温磁致伸缩效应可逆无磁滞。
附图说明
图1是Mn1-xCo1+xSi合金( 0≤ x ≤ 0.03 )的室温合金XRD衍射数据。
图2是240-320 K范围内正分MnCoSi合金的等温磁化曲线
图3是240-320 K范围内Mn0.99Co1.01Si合金的等温磁化曲线。
图4是240-320 K范围内Mn0.985Co1.015Si合金的等温磁化曲线。
图5是240-320 K范围内Mn0.98Co1.02Si合金的等温磁化曲线。
图6是Mn1-xCo1+xSi(x = 0,0.01,0.015)合金不同温度下的变磁性临界场曲线。
图7是优选合金Mn0.985Co1.015Si在270-300 K间平行和垂直自然取向方向的磁致伸缩量。
具体实施方式
本发明所述的合金的制备方法为高纯氩气氛围保护下电弧熔炼,退火方式为850℃退火60小时,随后经过72小时冷至室温。
实施例1
利用X射线衍射仪(X-ray Diffraction:XRD)测了合金的物相结构。图1是Mn1-xCo1+xSi合金( 0≤ x ≤ 0.03 )的室温合金XRD衍射数据,当x = 0, 0.01, 0.015时,合金为单一的正交TiNiSi型结构,这表明x ≤ 0.015时,Co原子的掺杂不会引起合金结构失稳。而当Co掺杂量达到x=0.02及以上时,可以看出Mn0.98Co1.02Si和Mn0.97Co1.03Si合金在2θ = 43.5°左右还存在少量Mn5Si3杂相。因此,为保证合金结构的稳定,Mn1-xCo1+xSi合金范围确定为0.01≤ x ≤ 0.015。
实施例2
利用超导量子干涉仪(Superconducting Quantum Interference Device:SQUID)测量了Mn1-xCo1+xSi(x = 0,0.01,0.015,0.02)合金的等温磁化曲线。
图2是正分MnCoSi合金的等温磁化曲线,合金在240-320 K的温度范围内均表现出变磁性特征,其中室温300 K时的变磁性临界场为2.5 T(相变临界场指50 %饱和磁化强度对应的外场大小)。
图3是Mn0.99Co1.01Si合金的等温磁化曲线,合金在240-320 K的温度范围内均表现出变磁性特征,其中室温300 K时的变磁性临界场为0.9 T。
图4是Mn0.985Co1.015Si合金的等温磁化曲线,合金在240-320 K的温度范围内均表现出变磁性特征,其中室温300 K时的变磁性临界场为0.8 T。
图5是Mn0.98Co1.02Si合金的等温磁化曲线,合金在240-280 K的温度范围内均表现出变磁性特征,在280-320 K的温度范围内为合金表现出铁磁性行为,变磁性转变消失。
图6是Mn1-xCo1+xSi(x = 0,0.01,0.015)合金不同温度下的变磁性临界场曲线图。合金的变磁性临界场随着温度的增加而降低,且当Co掺杂量增加时,相变临界场显著降低,且伴随着合金三相点的降低(三相点是指温度点,该温度以下合金磁化曲线有磁滞,为一级相变;该温度以下合金磁化曲线无磁滞,为二级相变)。其中优选的Mn0.985Co1.015Si合金变磁性临界场大幅度降低,三相点为260 K,室温300 K时磁化曲线无磁滞。
实施例3
利用综合物性测量系统(Physical Property Measurement System:PPMS)
和应变片技术对优选Mn0.985Co1.015Si合金进行了磁致伸缩测量。
图7是优选合金270-300 K间平行和垂直自然取向方向的磁致伸缩量,在平行取向方向合金表现为正的磁致伸缩效应,300 K时最大磁致伸缩量为1125 ppm;在垂直取向方向表现为负的磁致伸缩效应,300 K时最大磁致伸缩量为-530 ppm。由于优选合金三相点为260 K,所以室温磁致伸缩效应可逆无磁滞。
Claims (5)
1.一种MnCoSi基合金,其特征在于,所述的合金表达式为Mn1-xCo1+xSi ,其中0.01≤ x≤0.015。
2.如权利要求1所述的合金,其特征在于,合金表达式为Mn0.985Co1.015Si。
3.权利要求2所述的合金,其特征在于,使合金的室温相变临界场降低至0.8 T。
4.权利要求1或2所述的合金,其特征在于,合金室温磁化曲线无磁滞且室温磁致伸缩效应可逆无磁滞。
5.如权利要求1或2所述的合金的制备方法。
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
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CN110343931A (zh) * | 2019-08-27 | 2019-10-18 | 洛阳理工学院 | 一种室温磁致伸缩材料及其制备方法 |
CN112575237A (zh) * | 2020-12-09 | 2021-03-30 | 南京航空航天大学 | 一种Co-Ni-Mn-Si-Tb巨磁致伸缩材料及其制备方法 |
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Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
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CN110343931A (zh) * | 2019-08-27 | 2019-10-18 | 洛阳理工学院 | 一种室温磁致伸缩材料及其制备方法 |
CN110343931B (zh) * | 2019-08-27 | 2021-03-16 | 洛阳理工学院 | 一种室温磁致伸缩材料及其制备方法 |
CN112575237A (zh) * | 2020-12-09 | 2021-03-30 | 南京航空航天大学 | 一种Co-Ni-Mn-Si-Tb巨磁致伸缩材料及其制备方法 |
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