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Balancing negative and positive expansion effect in dual-phase La(Fe,Si)13/α -Fe composite with improved mechanical property.

机译:平衡具有改善的力学性能的双相La(Fe,Si) 13 /α-Fe复合材料的正负膨胀效应。

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Most materials exhibit a positive coefficient of thermal expansion (CTE), which leads to expanded lattices with temperature increases due to the population of higher energy levels of anharmonic lattice vibrations. However, small amount of materials contract upon heating and this phenomenon is called negative thermal expansion (NTE).Up to the present time, NTE has been observed in the well-known ZrW2O8 family of materials[1-3], MnCoGebased alloys[4,5], PbTiO3-based compounds[6,7], ScF3-based compounds[8], (Bi,La)NiO3[9] and antiperovskite manganese nitrides[10-12]. NaZn13 type La(Fe,Si13-based alloys are widely known to exhibit large negative thermal expansion during the magnetic transition. However, zero thermal expansion, which is more promising towards the utilization, has been rarely reported. Here, we introduce α-Fe phase naturally to compensate the negative thermal expansion of 1:13 phase, and thus achieve zero thermal expansion in La(Fe,Si)13/α-Fe composite. It is notable that the sample with x = 0 breaks itself during the magnetic transition for its poor mechanical property. In this case, it cannot be machined into regular shapes for the measurement of thermal expansion. Therefore, the average CTEs of the rest 4 samples are measured in this paper. The curves of ΔL/(L×ΔLT) are shown in Fig 1. Here, the reference temperature is 300 K and the average CTE is calculated by ΔL/(L×ΔLT). NTE is observed in the samples with x = 4 and 6. The average CTEs of samples with x = 4 and 6 reach -9.54 × 10-6 K-1 (278-304 K) and -6.25 × 10-6 K-1(270-291 K). With the increase of extra Fe in ingredient, a large amount of α-Fe phase appears and distributes in the 1:13 phase. NTE of 1:13 phase is offset by the PTE of α-Fe phase. An extremely low CTE of -6.55 × 10-7 K-1 between 261 K and 282 K is obtained in sample with x = 8, leading to the establishment of ZTE. Besides the low CTE, good mechanical property is another crucial prerequisite for ZTE or NTE materials. La(Fe,Si)13-based alloys with main 1:13 phase is typical brittle. In this experiment, the cuboid sample used for thermal expansion and stress-strain measurements are processed by diamond wire-sawing. During the machining process, the sample with x = 0 will break itself into some small bulks (right inset of Fig. 2, the small bulks are carefully polished for the microstructure observation on SEM), while the other sample are strong enough to be processed (left inset of Fig. 2). This indirectly proves that the increase of additional α-Fe phase can improve the mechanical property. With increasing x, the values of largest yield compressive stress are sharply enhanced to 864, 900, 970 and 1004 MPa for x = 4, 6, 8 and 10, respectively (see Fig. 2). The improved mechanical property is highly related with the existence of α- Fe phase. It is known that most brittle intermetallics display intrinsic weakness of grain boundaries and insufficient number of slip systems[13,14]. Therefore, the applied stress will easily broke the weaker links between grains and leads to intergranular fractures. However, this situation will greatly changes when introducing a secondary ductile phase. In this experiment, the distributed ductile α-Fe phase is helpful to prevent the movement and slipping of dislocation, thus hinder the cracks propagation along the weak grain boundaries and enhance the mechanical property. On the other hand, additional Fe atoms suppress the formation of La-rich phase, which is detrimental to the mechanical and corrosion properties. It also contributes to the improved mechanical property. In summary, we successfully fabricate dual-phase La(Fe,Si)13/α-Fe composite. The microstructures, magnetic properties, thermal expansion and mechanical properties of samples are investigated. With the increase of extra Fe in ingredient, a large amount of α-Fe phase appears and distributes in the 1:13 phase. NTE of 1:13 phase is offset by the PTE of α-Fe phase. An extremely low CTE of -6.55 × 10-7 K-1 between 261 K and 282 K is obtained in sample with x = 8, leading to the establishment of ZTE. Additionally, as a reinforcing factor, α-Fe phase is helpful to prevent the movement and slipping of dislocation, thus enhancing the mechanical property. Based on these improvement, ZTE and improved mechanical property are achieved simultaneously in La(Fe,Si)13/α-Fe composite.
机译:大多数材料表现出正的热膨胀系数(CTE),由于非谐晶格振动的较高能级的聚集,随着温度的升高,晶格会膨胀。然而,少量材料在加热时会收缩,这种现象称为负热膨胀(NTE)。到目前为止,在著名的ZrW中已观察到NTE 2 Ø 8 材料族 [1-3] ,MnCoGe基合金 [4,5] 铅钛矿 3 基化合物 [6,7] ,scF 3 基化合物 [8] ,(Bi,La)NiO 3 [9] 和抗钙钛矿氮化锰 [10-12] 。钠锌 13 La(Fe,Si型 13 众所周知,铁基合金在磁性过渡过程中会表现出较大的负热膨胀。然而,几乎没有报道过零热膨胀,这对于利用来说是更有希望的。在这里,我们自然引入α-Fe相以补偿1:13相的负热膨胀,从而在La(Fe,Si)中实现零热膨胀 13 /α-Fe复合材料。值得注意的是,x = 0的样品由于其较差的机械性能而在磁跃迁过程中断裂。在这种情况下,不能将其加工成规则形状以测量热膨胀。因此,本文对其余4个样本的平均CTE进行了测量。 ΔL/(L×ΔLT)的曲线示于图1。此处,参考温度为300K,并且平均CTE通过ΔL/(L×ΔLT)计算。 x = 4和6的样本中观察到NTE。x = 4和6的样本的平均CTE达到-9.54×10 -6 ķ -1 (278-304 K)和-6.25×10 -6 ķ -1 (270-291 K)。随着成分中额外铁的增加,大量的α-Fe相出现并分布在1:13相中。 1:13相的NTE被α-Fe相的PTE所抵消。 -6.55×10的极低CTE -7 ķ -1 在x = 8的样本中获得261 K和282 K之间的值,从而建立了ZTE。除了较低的CTE外,良好的机械性能是ZTE或NTE材料的另一个关键先决条件。主相为1:13的La(Fe,Si)13基合金通常是脆性的。在该实验中,用于热膨胀和应力应变测量的长方体样品通过金刚石线锯进行处理。在机加工过程中,x = 0的样品将自身破碎成一些小块(图2的右插图,对这些小块进行了仔细抛光,以便在SEM上观察微观结构),而其他样品则足够坚固以至于可以加工(图2的左插图)。这间接证明增加额外的α-Fe相可以改善机械性能。随着x的增加,当x = 4、6、8和10时,最大屈服压缩应力的值急剧增加至864、900、970和1004 MPa,分别(见图2)。改善的机械性能与α-Fe相的存在高度相关。众所周知,大多数脆性金属间化合物显示出晶界的固有弱点和滑移系统的数量不足 [13,14] 。因此,施加的应力将容易破坏晶粒之间的较弱连接,并导致晶间断裂。但是,当引入次生延性相时,这种情况将发生很大的变化。在该实验中,分布的延展性α-Fe相有助于防止位错的运动和滑移,从而阻止了裂纹沿着弱的晶界扩展并增强了机械性能。另一方面,额外的Fe原子抑制了富La相的形成,这不利于机械和腐蚀性能。它还有助于改善机械性能。总之,我们成功地制备了双相La(Fe,Si)13 /α-Fe复合材料。研究了样品的微观结构,磁性能,热膨胀性和机械性能。随着成分中额外铁的增加,大量的α-Fe相出现并分布在1:13相中。 1:13相的NTE被α-Fe相的PTE所抵消。 -6.55×10的极低CTE -7 ķ -1 在x = 8的样本中获得261 K和282 K之间的值,从而建立了ZTE。另外,作为增强因素,α-Fe相有助于防止位错的运动和滑动,从而增强机械性能。基于这些改进,可以在La(Fe,Si)13 /α-Fe复合材料中同时实现ZTE和改善的机械性能。

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