2010
DOI: 10.1088/0953-8984/22/32/324106
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Synthesis and magnetorheology of suspensions of submicron-sized cobalt particles with tunable particle size

Abstract: . Synthesis and magnetorheology of suspensions of submicronsized cobalt particles with tunable particle size. Journal of Physics: Condensed Matter, IOP Publishing, 2010, 22, pp.324106 Abstract. Different samples of cobalt powder were synthesized. Particle size and shape were characterized by electron microscopy and light scattering. These measurements showed that the synthesized powders consisted of monodisperse spheres with average diameters ranging between 63 and 760 nm. These powders were used for the prepa… Show more

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Cited by 18 publications
(18 citation statements)
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References 22 publications
(28 reference statements)
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“…[22][23][24][25] However, in real applications, the MR suspensions are mostly stressed dynamically. This behavior is usually examined through measurement in the steady shear mode.…”
Section: Rheological Propertiesmentioning
confidence: 99%
See 1 more Smart Citation
“…[22][23][24][25] However, in real applications, the MR suspensions are mostly stressed dynamically. This behavior is usually examined through measurement in the steady shear mode.…”
Section: Rheological Propertiesmentioning
confidence: 99%
“…This behavior is usually examined through measurement in the steady shear mode. [22][23][24][25] However, in real applications, the MR suspensions are mostly stressed dynamically. This indicates that oscillatory shear measurement is an adequate method for performance evaluation.…”
Section: Rheological Propertiesmentioning
confidence: 99%
“…[x, y, z] = sphere (4) x = x * radius (5) y = y * radius (6) z = z * radius (7) xinit(i) = rand*length (8) yinit(i) = rand*width (9) zinit(i) = rand*height (2*uf))^2)*uf) (27) Dworadius = 6*pi*vis (28) cubaf = cuba(f) (29) Qfgfacaf3 = Qfgfac*cuba(f) (30) Q1Bupufaf3 = Q1Bupuf*cuba(f) (31) delx(f,g) = xsys(t,f)-xsys(t,g) (32) dely(f,g) = ysys(t,f)-ysys(t,g) (33) delz(f,g) = zsys(t,f)-zsys(t,g) (34) crit = a(f)+a(g) (35) Fx(f,g) = Fmx(f,g)+Fpx(f,g) (36) Fy(f,g)=Fmy(f,g)+Fpy(f,g) (37) Fz(f,g)=Fmz(f,g)+Fpz(f,g)+dvis(f)*U*(xsys(t,f)-a(f))/length (38)…”
Section: Appendix-iimentioning
confidence: 99%
“…However due to sedimentation problem, usage of larger sized particles [7][8] are discouraged. Similarly, retainability of magnetic field in submicron particles [9] is disadvantageous as quick reversibility in shear stress is an essential functionality of MR fluids.…”
Section: Introductionmentioning
confidence: 99%
“…However due to sedimentation problem, usage of larger sized particles [7][8] are discouraged. Similarly, retainability of magnetic field in submicron particles [9] is disadvantageous as quick reversibility in shear stress is an essential functionality of MR fluids. It is interesting to note that the cost of larger sized particles is just 28% of the cost of smaller sized particles [10].…”
Section: Introductionmentioning
confidence: 99%