2021
DOI: 10.1177/1045389x20988082
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Analysis of quasistatic squeeze behavior of magnetorheological fluid from the microstructure variations

Abstract: Magnetorheological fluid is a novel functional material, of which quasistatic squeeze behavior needs to be quantitatively controlled in industrial applications. Since the quasistatic squeeze behavior has a close relation with microstructure variations, thus it is modeled from a microscopic approach. By analyzing compression of single chains, aggregation from single chains to BCT structure and compression of BCT structure, the initial stress [Formula: see text], yield stress [Formula: see text], yield strain [F… Show more

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Cited by 10 publications
(6 citation statements)
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“…The current studies on the normal force of MRF are basically based on experimental methods, generally using a plate-plate rheometer to test the normal force of MRF under different conditions. These studies dealt with the effects of shear rate, strain amplitude, temperature, particle concentration, MRF layer thickness and other factors on the dynamic and static normal force of MRF [11][12][13][14][15][16][17]. Simultaneously, some theoretical models were also developed, and the results showed that the theoretical predictions of the MRF normal force agreed well with the experimental results [8,13].…”
Section: Introductionmentioning
confidence: 90%
“…The current studies on the normal force of MRF are basically based on experimental methods, generally using a plate-plate rheometer to test the normal force of MRF under different conditions. These studies dealt with the effects of shear rate, strain amplitude, temperature, particle concentration, MRF layer thickness and other factors on the dynamic and static normal force of MRF [11][12][13][14][15][16][17]. Simultaneously, some theoretical models were also developed, and the results showed that the theoretical predictions of the MRF normal force agreed well with the experimental results [8,13].…”
Section: Introductionmentioning
confidence: 90%
“…In equation ( 8), r m is the particle radius, H = B/ µ 0 is the magnetic induction intensity, µ is the absolute permeability of the particle, µ s = µ/µ 0 is the relative permeability of the particle, µ 0 = 4π × 10 −7 N A −2 is the vacuum permeability, and χ e = µ s −1 is the effective magnetic susceptibility. Since the external magnetic field is uniform, so B = 0, the particles are only affected by the magnetic force generated by other particles [29,30]. Take particle chain a and b in figure 5 as the research object, and establish the coordinate system as shown in figure 6.…”
Section: Equivalent Magnetic Stiffness Coefficient Kmentioning
confidence: 99%
“…A new intensity theory for the emergence of new forms of transformation of the lattice structure of nanoscale particles in magnetorheological fluids has explained this phenomenon in a scientific way [28]. With a low magnetic induction intensity, a complex structure has appeared inside the magnetorheological fluid with a larger volume fraction, however, the complex structure is not stable enough at this time and is vulnerable to destruction.…”
Section: Observation Experimentsmentioning
confidence: 99%
“…Where, V is the magnetic particles volume, which is always constant during the extrusion process, and f 1 and f 2 are the volume fraction before and after extrusion, respectively. Then the relationship between the post-yield MRF stress and strain can be expressed as [28] H 4…”
Section: Micro-macro Mechanical L Properties In the Extruded Statementioning
confidence: 99%