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Magnetic domain observations on magnetite crystals in biotite and hornblende grains

机译:黑云母和角闪石晶粒中磁铁矿晶体的磁畴观察

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eMagnetic domain structures have been observed on magnetite crystals in 300 μm to 1 mm size biotite and hornblende grains separated from drill core samples of Precambrian granodiorite basement in southern Alberta, Canada. The crystals were mounted in epoxy, and the surface was polished, first mechanically and then with a suspension of amorphous SiO2. Domain structures were observed on 6–60 μm magnetite crystals using the Bitter colloid technique. Observed features include lamellar domains bounded by straight 180° walls, closure domains, bent walls, wavy structures, and areas without visible domains. Crystals ≤50 μm in size generally have simple domain patterns with domain walls parallel to the long axis of the crystal. We studied domain wall displacements in small isolated magnetites as a function of applied magnetic field up to 24 mT. The number of domains decreases with increasing external field. Some walls are relatively mobile and disappear by 20 mT. Other walls remain immobile; in some cases, crystal defects or inclusions are seen to pin these walls, or segments of walls. An interesting observation was made on a 5 × 25 μm elongated magnetite crystal formed in a crack in hornblende. Large quantities of magnetic colloid gathered at either end of the crystal because of the strong flux leakage and pole fields at these locations. Colloid was also concentrated where domain boundaries intersect the sides of the crystal. With increasing applied field the colloid spread out to form patterns tracing complete external flux closure loops.
机译:在加拿大艾伯塔省南部的前寒武纪花岗闪长岩地下室钻芯样品中分离出的300μm至1 mm黑云母和角闪石晶粒的磁铁矿晶体上已观察到电磁域结构。将晶体固定在环氧树脂中,首先对表面进行机械抛光,然后对无定形SiO2进行悬浮。使用Bitter胶体技术在6-60μm磁铁矿晶体上观察到畴结构。观察到的特征包括以直的180°墙为边界的层状区域,闭合区域,弯曲的壁,波浪结构以及无可见区域的区域。尺寸≤50μm的晶体通常具有简单的畴图案,畴壁与晶体的长轴平行。我们研究了小的孤立磁铁矿中的畴壁位移与施加的磁场(高达24 mT)的关系。域的数量随着外部场的增加而减少。一些墙相对活动,消失20 mT。其他墙壁仍然不动;在某些情况下,可以看到晶体缺陷或夹杂物将这些壁或部分壁钉住。对在角闪石裂缝中形成的5×25μm细长磁铁矿晶体进行了有趣的观察。由于这些位置处的强磁通泄漏和极场,大量的磁性胶体聚集在晶体的两端。胶体也集中在畴边界与晶体侧面相交的地方。随着施加场的增加,胶体散布形成跟踪整个外部通量闭合回路的图案。

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