Abstract
Through energy minimization and stability argument, we find the ground states of the magnetorheological fluids to consist of magnetic particles arranged in a body centered tetragonal structure inside spheroidal clusters. The width $D$ of the clusters varies with the length $L$ as $D\ensuremath{\sim}{L}^{n}$, where $n\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.62$ for magnetically saturated particles. In the case of magnetically unsaturated particles, the power law variation is divided into two segments, with $n\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.4$ in the first segment and $n\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.62$ in the large $L$ limit. Our results offer a theoretical framework for the resolution of conflicting experimental observations, with the demagnetization field being the crucial physical consideration.
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