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Hydrodynamics substantially affects induced structure formation in magnetic fluids

Henning Reinken, Markus Heiber, Takeaki Araki, Andreas M. Menzel

Abstract

Magnetorheological fluids consist of micrometer-sized magnetic particles in a carrier liquid. Sufficiently strong external magnetic fields lead to the formation of string-like particle aggregates. We demonstrate that hydrodynamic interactions, that is, mutual couplings via induced flows, play a substantial role during structure formation. Hydrodynamics supports the emergence of string-like aggregates, while magnetic interactions align them. This fundamental insight is substantial from an application perspective, due to the enormous technical importance and potential of magnetorheological fluids.

Hydrodynamics substantially affects induced structure formation in magnetic fluids

Abstract

Magnetorheological fluids consist of micrometer-sized magnetic particles in a carrier liquid. Sufficiently strong external magnetic fields lead to the formation of string-like particle aggregates. We demonstrate that hydrodynamic interactions, that is, mutual couplings via induced flows, play a substantial role during structure formation. Hydrodynamics supports the emergence of string-like aggregates, while magnetic interactions align them. This fundamental insight is substantial from an application perspective, due to the enormous technical importance and potential of magnetorheological fluids.
Paper Structure (13 equations, 3 figures)

This paper contains 13 equations, 3 figures.

Figures (3)

  • Figure 1: Structure formation with and without hydrodynamic interactions (HI) for an area fraction of $\theta \approx 0.15$. (a) Simulations start from the same configuration of roughly equally distributed particles. (b--d) Snapshots of the "dry" system at times $t=1600$, $2400$, and $10000$. The color scale refers to the magnetization field within the particles. (f--h) Snapshots of the system involving hydrodynamic interactions and fluid flows at the same times. Blue arrows indicate the flow field. (e) Magnified part of (f) showing the emergence of large-scale flows and the mutual amplification of local magnetization for particles that are close to each other. The external field strength is set to $|\mathbf{H}_\mathrm{ext}|/M_\mathrm{sat} = 0.2$.
  • Figure 2: Same as in Fig. \ref{['fig:snapshotsLJ_050']}, yet for an elevated area fraction of $\theta \approx 0.31$ and snapshots in (b--d) and (f--h) taken at times $t=400$, $800$, and $10000$. Here, chain formation promoted by hydrodynamic interactions (HI) leads to branching and string-like structures when compared to the more compact clusters that emerge without hydrodynamics.
  • Figure 3: Evolution of the chain-likeness parameter $\chi$ for an area fraction of (a) $\theta \approx 0.15$, (b) $\theta \approx 0.23$, and (c) $\theta \approx 0.31$. Hydrodynamic interactions (HI) consistently lead to more chain-like structures when compared to the "dry" case without HI. Shaded areas indicate standard errors, that is, standard deviations divided by the square root of the sample size.