The Study of Magnetorheology of Iron Oxide Nanowires

In this work, circular Fe 3 O 4 particles with a diameter of 24 nm and quasicircular Fe 3 O 4 particles with a diameter of 10 nm were synthesized using peptization and coprecipitation methods, respectively. The coprecipitated particles were further formed into Fe 3 O 4 nanowires at high temperature and high pressure in a strongly alkaline environment. The optimal environment for forming nanowire was 15m (molality) NaOH at 120C for three days; the resulting proportional relationship between its width and its height, the aspect ratio, was 50.5/1. In the second part of this study, the nanoparticles and nanowire were dispersed in silicon oil and formed into magnetorheological (MR) fluids of different concentrations, before undergoing various MR tests—a shear test, a compression test, and a creep recovery test. The results revealed that the MR performance of nanowire fluid was better than that of circular particle fluid, in terms of yield stress (35 Pa versus 60 Pa), compression displacement (Δd) (0.19mm versus 0.44mm), and creep recovery ratio (82% versus 48%).The experimental results conclude that the nanowire network ismore robust than the nanoparticle network. The test of the storage shelf time revealed that 12 wt% nanowire fluid retained more than 80% of its original yield stress after three months, indicating slight precipitation in the nanowire fluid. In summary, the nanowire MR fluid had a stronger MR effect than traditional MR fluid that was prepared with spherical MR particles.


Introduction
A magnetorheological (MR) suspension can be promptly transformed from a fluid-like structure to a solid-like structure with a viscoelastic to plastic yielding by subjecting it into a magnetic field [1][2][3][4][5][6][7].Rabinow [8] discovered this phenomenon in 1948.Since then, various metal or ceramic powders with magnetic characteristics have been dispersed in nonmagnetic carrier liquids (such as oil or aqueous liquids) in the preparation of MR suspensions.Smart damper [9] is an important application of magnetorheological (MR) fluid.The releasing of its internal energy depends mainly on the viscosity of the dashpot.Therefore, a method for preparing MR fluid with a wide range of viscosities, ensuring a strong response of the yield stress or creep recovery from low to high magnetic strength, is crucial.Notably, Fe 3 O 4 , having a net ferromagnetic moment arising from the incomplete cancellation of spin materials of Fe 2+ ions, can respond very sensitively to the magnetic fields.More importantly, the permanent magnetization of Fe 3 O 4 nanoparticles is still weak enough that it cannot cause any interparticle agglomeration under zero magnetic field strength; Fe 3 O 4 nanoparticle thus becomes a good candidate for the preparation of MR fluids.This work employs various chemical methods to synthesize Fe 3 O 4 magnetic particles of various sizes and Fe 3 O 4 magnetic nanowire and to form them into MR fluids, whose MR properties, including shear yield stress, compression resistance, creep recovery, and yield strength decay, are then observed.The goal is to find the formulation of MR fluids with optimal performance.[10][11][12].Add iron chloride hexahydrate (10.8 g, 80 mmol), sodium oleate (36.5 g, 240 mmol) to a mixed solution of ethanol (80 mL), deionized water (60 mL), and hexane (140 mL).Stir the mixture well in a 500 mL three-neck flask that is mounted on a condensation system.Heat to 70 ∘ C and maintain this temperature for 4.5 h; then purify three times using deionized water (30 mL) and finally store the iron-oleate complex product in hexane.Add iron-oleate complex 9 g, oleic acid 1.7 g to 30 g tri-n-octylamine and stir well in a 500 mL threeneck flask.Heat at 3.3 ∘ C/min to 366 ∘ C or 300 ∘ C and maintain this temperature for 30 min.Wash the excessive oleic acid from the surface of Fe 3 O 4 nanoparticles using ethanol or hexane, respectively.

Coprecipitation Synthesis of
Nanoparticle II.To 6 g iron chloride tetrahydrate and 12 g iron chloride hexahydrate add 25 mL deionized water and mix to form an ionic solution.Add 50 mL ammonium hydroxide rapidly while agitating mechanically; keep stirring for 6 min and coprecipitate [13][14][15][16] to obtain Fe 3 O 4 nanoparticles.Use deionized water to wash off excessive ammonium hydroxide.Remove remaining deionized water in Fe 3 O 4 nanoparticles by freeze-drying.Then, lower the upper plate until the clearance is 0.1 cm.The temperature of the rheometer is held constant, 25 ∘ C. Apply various currents and measure the yield stress, the compression displacement, and the creep recovery rate of the specimen.The electronic micrographs were taken using transmission electron microscope at 300 kV (TEM Hitachi: H-7100).The X-ray powder diffractometer (XRD PANalytical X'Pert PRO MPD), operated at 45 kV and 20 mA under CuK radiation, was applied to analyze the crystal phase.The detector was scanned over a range of 4 angles from 0 ∘ to 70 ∘ at a speed of 4 ∘ per minute.

Results and Discussion
Figure 1 presents a TEM image of Fe 3 O 4 nanoparticles that were synthesized by oleic acid peptization.The diameters of the particles are uniformly distributed with an average of 24 nm.X-ray diffraction proves that the nanoparticles are pure Fe 3 O 4 (Figure 2 lower curve).The peaks are consistent with the previous study [20].Figure 3 presents a TEM image of Fe 3 O 4 nanoparticles that were formed by coprecipitation.As is seen, the distribution of particle sizes is very broadmuch broader than achieved by peptization.The particles are not spherical but appear quasicircular or even polygonal.However, X-ray diffraction pattern (Figure 2-upper curve) proves that they are still pure Fe 3 O 4 particles.5(a), including a temperature of 120 ∘ C, in which the fewest particles were unreacted, were obviously optimal.Analysis of the image reveals that the aspect ratio of 50.5 : 1 obtained at 120 ∘ C is also the maximum value.The optimal conditions for forming Fe 3 O 4 nanowire formation are thus determined to be 15 m NaOH, 120 ∘ C, high pressure, and a strongly alkaline ambient.
As shown in Figure 6, the yield stress of Fe 3 O 4 nanowire fluid, 60 Pa, is nearly double that of Fe 3 O 4 nanoparticle fluid, 35 Pa, at the same concentration (6 wt%).This result indicates that the asymmetry of nanowire can enhance the MR effect.Figure 7 plots the dependence of shear stress on shear rate for various concentrations of Fe 3 O 4 nanowires that were suspended in silicon oil with various viscosities (10 cp, 100 cp).The MR fluid exhibits typical Bingham character [21], with a yield stress threshold at which fluidity in a magnetic field is first exhibited.Figure 7 demonstrates that the yield stress increases with the nanowire concentration.Moreover, when the solid loading is 12 wt%, the yield stress of the 100 cp suspension is 1.5 times that of the 10 cp suspension (1100 Pa versus 720 Pa).This result demonstrates that an increase of PDMS viscosity results in a higher yield stress at a given Fe 3 O 4 loading.Figure 8 plots the yield stress against Fe 3 O 4 solid concentrations when 0-36 wt% of Fe 3 O 4 nanowires are suspended in 100 cp silicon oil.In the plot, as the solid loading increases, the yield stress increases as approximately a second-order polynomial (slope = 2.35) function.Even though the increase of Fe 3 O 4 loading positively affects the MR effect, the nanowire agglomeration that arises from high loading may occur seriously.This work demonstrates that the solid loading of Fe 3 O 4 nanowires can be increased to 36 wt% without causing serious agglomeration.The authors' ultimate goal is to formulate a highly effective MR fluid at a sufficiently high concentration so that it can flow freely in a nonmagnetic field without solid-liquid separation but has a yield stress that can increase to 10 4 Pa in a magnetic field.
Along with the shear test, the compression test can also be employed to characterize MR fluids.When a magnetic fluid is placed in a magnetic field, MR particles are temporarily in a network state, as shown in Figure 9(a).The purpose of shear test, as stated previously, is to determine the critical shear stress, also known as the yield stress that disrupts the network state.Similarly, the action of compression stress on the network can alter the network structure.Figure 9(b) demonstrates that under a given compression stress, a smaller change in volume, or a smaller Δd, corresponds to a greater magnetic attractive force among the magnetic particles within the network.When subjected to an external force, a more robust network is associated with a greater displacement resistance, and the displacement in the direction of the force is smaller.Figure 10 reveals that the compression displacements of the Fe 3 O 4 nanoparticle are 0.39 mm and 0.44 mm in 10 cp and 100 cp silicon oil, respectively.In contrast, the compression displacements (Δd) of the nanowires dispersed in 10 cp and 100 cp silicon oil are 0.19 mm and 0.07 mm, respectively.The experimental result demonstrates that nanowire can exhibit favorable MR behavior.Additionally, the nanowire network has a higher compact density and toughness than the nanoparticle network.In fact, the particles are orientated and line up along the magnetic line of force with fewer joints.However, the line derived from the circular nanoparticles has more junctions than that derived from a nanowire.These junctions are the weakest points of the line.They usually collapse under a shear force or compression stress (Figures 11(a) and 11(b)).
The resistance of the nanowire network to an external force is better because it has fewer junctions.The results also reveal that 10 cp silicon oil is associated with a shorter compression displacement than 100 cp silicon oil, perhaps because the former lubricates the joints less well than the latter.Better lubrication is generally associated with longer compression displacement.
The creep and recovery test [22,23] focuses on investigating the recovery behavior of a magnetic network following deformation by shearing, which has rarely been studied as part of MR investigations.In this work, the elasticity of the magnetic network structure is determined by applying a constant shear stress less than the yield stress to the MR fluid.The transient displacement of the MR structure reaches a constant, and then the stress is removed to observe the recovery of the MR fluid.A high recovery ratio demonstrates excellent elasticity of the magnetic network.It also indicates that the arrangement of magnetic particles inside the network is in a very stable state.Notably, the stress applied herein is less than the yield stress, and none of the magnetic fluids flows; rather, it exhibits various degrees of displacement.If obvious damage or permanent displacement occurs in the creep test, then the stress has permanently and detrimentally affected the relative positions of the network particles, such that the magnetic network structure fails to recover after shearing.This situation reveals that the solid character of the magnetic network is not strong.Figure 12 plots the result of the creep and recovery test for nanoparticles and nanowire.When the shear stress (10 Pa or 20 Pa) is much less than the yield stresses of the MR fluids (35 Pa for nanoparticles and 60 Pa for nanowire), the recovery ratio of elasticity is nearly 100%.However, at a shear stress of 30 Pa, which is close to the yield stress of nanoparticles, the recovery ratio is only 48%.In contrast, 30 Pa is far below the yield stress of the nanowire, for which the recovery ratio is 82%.This result confirms that a nanowire network is more robust than a nanoparticle network.Additionally, Figure 12 shows that a network formed by the magnetic field suffers serious damage when the applied stress is only slightly less than the yield stress. Figure 13 plots the creep and recovery of MR fluids when the applied stress exceeds the yield stress.In the creep stage in Figure 13, the creep strain is not constant but increases with time.
When the creep recovery stage is triggered 100 seconds later, the recovery is unobservable because the previous magnetic network structure had completely disintegrated.Even if the applied stress were terminated, a new network that is oriented with the magnetic field would gradually form, but it would have no relation to the previously damaged network in terms of structure or relative position of particles.Accordingly, recovery cannot occur when the applied stress exceeds the yield stress.
To determine whether the nanowire fluid meets the operating requirements, 12 wt% nanowire suspensions were stored for one, two, and three months, restirred, and then individually subjected to the MR shear test.Figure 14 shows that the yield stress decays from an initial value of 400 Pa at a rate from 20 Pa-30 Pa per month to 325 Pa after three months.This result shows that, because the size of the suspended nanowires is of the order of microns, their Brownian motion cannot overcome gravity, and precipitation eventually occurs.However, after restirring, this suspended matter is again dispersed, reducing the agglomeration.Figures 15(a

Conclusions
This systematic study of the preparation of magnetic particles preparation and their MR characterization supports the following conclusions.
(1) Circular Fe 3 O 4 particles with a diameter of 24 nm and quasicircular Fe 3 O 4 particles with a diameter of 10 nm were synthesized by peptization and coprecipitation.The peptized particles were formed into Fe 3 O 4 nanowire at high temperature and high pressure in strongly alkaline environment.The optimal reaction conditions for forming nanowires are 15 m NaOH at 120 ∘ C for three days.An aspect ratio as high as 50.5 : 1 can thus be achieved.
(  (4) The creep and recovery test showed that a network formed by the magnetic field had serious damage once the applied stress was close to the yield stress.
(5) In the storage test, 12 wt% nanowire fluid retained more than 80% of its original yield stress after three months.
In summary, nanowire magnetic particles can exhibit a better MR effect than traditional magnetic particles that were prepared with spherical MR particles.and filed by the authors and the financial founder: NSC of Taiwan.There is no conflict of interests for any commercial application at present time or in the future.
Nanowire III.Put 0.5 g Fe 3 O 4 nanoparticles in a pressurized reaction flask and add sodium hydroxide solution to a concentration of 15 M. Place the flask in an oven and allow the hydrothermal reaction [17-19] to proceed at 120 ∘ C (2 atm) for three days to yield Fe 3 O 4 nanowires.Use deionized water to remove the excess sodium hydroxide solution.Remove the remaining deionized water from the Fe 3 O 4 nanowires by freeze-drying.

2. 4 .
Preparation of Magnetic Fluid.Add materials I, or II, or III to silicon oil with viscosities of 10 cp and 100 cp (polydimethylsiloxane PDMS).Stir well to obtain MR fluid.Pour the MR fluid into the groove on the lower plate of the rheometer (Anton Paar Physica MCR301 MRD).

Figure 1 :
Figure 1: The TEM image of Fe 3 O 4 nanoparticles synthesized by oleic acid peptization.

Figure 2 :
Figure 2: The X-ray diffraction spectrum of Fe 3 O 4 nanoparticle and nanowire.

Figure 3 :
Figure 3: The TEM image of Fe 3 O 4 nanoparticles formed by coprecipitation.

Figure 8 :
Figure 8: The yield stress is a function of solid loading of Fe 3 O 4 MR fluids.

Figure 9 :Figure 10 :
Figure 9: (a), (b) The illustration of structure change for an MR fluid under the compression test.

Figure 11 :Figure 12 :
Figure 11: The illustration of Fe 3 O 4 nanowires lining up along the magnetic line of force for the MR fluid (a) without shear and (b) under shear.
) to 15(c) are TEM images of nanowire fluid with various storage periods.A comparison with Figure5(b) reveals slight wire agglomeration, which, while not severe, should be reduced.

Figure 13 :Figure 14 :
Figure 13: The plot of creep and recovery test for MR fluids containing 6 wt% of Fe 3 O 4 nanoparticles and nanowires under shear stress of 70 Pa, which is far above the yield stresses of both MR fluids.The experiment was repeated 3 times and a good reproducibility is shown.

Figure 15 :
Figure 15: (a)∼(c) The TEM images of a MR fluid containing 12 wt% Fe 3 O 4 nanowires, which were stored at various periods of time: (a) 1 month, (b) 2 months, and (c) 3 months.
) The MR shear test revealed that the yield stress of Fe 3 O 4 nanowire fluid is double that of the same concentration of Fe 3 O 4 nanoparticle fluid.Furthermore, as the Fe 3 O 4 particle concentration increases, the yield stress increases following a second-order polynomial (slope = 2.35) curve.(3) The compression displacement (Δd) of the Fe 3 O 4 nanowire MR fluid is far less than that of the Fe 3 O 4 nanoparticle MR fluid (0.19 mm versus 0.44 mm).The creep recovery capacity of Fe 3 O 4 nanowire also exceeds that of Fe 3 O 4 nanoparticle.