42 research outputs found

    Enhancing magnetorheological effect using bimodal suspensions in the singlemultidomain limit

    Get PDF
    We demonstrate a new route to enhance the magnetorheological effect using bimodal suspensions in the single-multidomain limit. Experimental results are satisfactorily compared to 3D finite element method simulations. The physical reason behind this enhancement is the coating of the larger particles by the smaller ones due to the remnant magnetization of the latter.This work was supported by MAT 2016-78778-R and PCIN 2015-051 projects (FEDER FUNDS and MINECO, Spain). A J F Bombard is grateful to FAPEMIG grants: APQ-01824-17, PEE-00081-16, RED-00144-16, ETC-00043-15, PEP-00231- 15, APQ-00463-11 and RDP-00164-10. J R Morillas acknowledges FPU14/01576 fellowship

    Non-linear stress response of non-gap-spanning magnetic chains suspended in a Newtonian fluid under oscillatory shear test : A direct numerical simulation

    Get PDF
    The corresponding author wishes to express his sincerest thanks to the Iran National Science Foundation (INSF) for supporting this work under Contract Number 92021291.Peer reviewedPostprintPublisher PD

    Start-up rheometry of highly polydisperse magnetorheological fluids: experiments and simulations

    Get PDF
    An extensive experimental and simulation study is carried out in conventional magnetorheological fluids formulated by dispersion of mixtures of carbonyl iron particles having different sizes in Newtonian carriers. Apparent yield stress data are reported for a wide range of polydispersity indexes (PDI) from PDI = 1.63 to PDI = 3.31, which for a log-normal distribution corresponds to the standard deviation ranging from to . These results demonstrate that the effect of polydispersity is negligible in this range in spite of exhibiting very different microstructures. Experimental data in the magnetic saturation regime are in quantitative good agreement with particle-level simulations under the assumption of dipolar magnetostatic forces. The insensitivity of the yield stresses to the polydispersity can be understood from the interplay between the particle cluster size distribution and the packing density of particles inside the clusters

    Magneto-Sensitive Smart Materials and Magnetorheological Mechanism

    Get PDF
    Magneto-sensitive smart materials, also named as magnetorheological (MR) materials, are a class of smart composites prepared by dispersing nanometer- or micrometer-sized ferromagnetic fillers into the different carrier matrix. As the rheological properties can be controlled by an external magnetic field rapidly, reversibly, and continuously, magneto-sensitive smart materials have great application potential in construction, automotive industry, artificial intelligence, etc. In this chapter, a brief history and classification of magneto-sensitive smart materials are firstly summarized. Next, we discuss the state-of-the-art of the magnetorheological mechanism through experimental and theoretical studies, respectively. Finally, the prospect for this material in the future is presented

    Rheological Characterization of Magnetorheological Fluids

    Get PDF
    Magnetorheological (MR) ๏ฌ‚uids are smart materials that respond to an external magnetic ๏ฌeld by changing their rheological properties. These ๏ฌeld dependent properties are typically studied by rotational rheometry. Since the data of the rotational rheometer measurements may include errors caused by various sources, it is essential to study the rheological characterization of the MR ๏ฌ‚uids before the results are used in research. A major drawback of MR ๏ฌ‚uids is sedimentation that may weaken ๏ฌ‚uids MR response over time. The sedimentation is settling of magnetic particles induced by the large density mismatch between the particles and the carrier ๏ฌ‚uid. In this study, the rheological characterization of MR ๏ฌ‚uids by a rotational rheometer is ๏ฌrst examined to reveal how the measurements should be done in order to gain reliable knowledge about their properties. Secondly a bidisperse size distribution of magnetic particles, consisting of micron- and nano-sized particles, was studied as a way to improve the sedimentation stability.The study of rheological characterization of MR ๏ฌ‚uids by rotational rheometer involved determination ๏ฌeld dependent yield stresses by using various measuring procedures and plate-plate measuring geometries with di๏ฌ€erent surfaces. The results demonstrated that the measured static and dynamic yield stresses are strongly a๏ฌ€ected by the plate surface characteristics as the magnetic and roughened plates provided considerably higher values than the smooth non-magnetic plates. A likely source for the di๏ฌ€erence is wall slip that may happen during rotational rheometer measurements. Furthermore, it was shown that the wall slip of MR ๏ฌ‚uid does not cause measuring gap height dependency of the results, which is surprising, as its existence is commonly used as an indicator of the wall slip.The bidisperse MR ๏ฌ‚uids were prepared by dispersing micron- and nano-sized particles in Silicone Oil (SO) or Ionic liquid (IL). The impact of the carrier ๏ฌ‚uid type and nanoparticle fraction, composition and size on the o๏ฌ€-state viscosity, sedimentation stability and MR response were studied. The maghemite (ฮณ โˆ’ Fe2O3) nanoparticles used in the study were synthesized by Liquid Flame Spray (LFS) method that o๏ฌ€ers an interesting alternative for the chemical co-precipitation commonly used to prepare magnetic nanoparticles as it is a very versatile process. The dispersion of the micron-sized particles was better IL than in SO indicated by lower o๏ฌ€-state viscosity and higher MR response. A partial substitution of micron-sized particles by nanoparticles provided improved sedimentation stability with both carrier ๏ฌ‚uids. The impact became stronger as the nanoparticle fraction was increased or the nanoparticle size was decreased. Both lead to higher particle surface to volume ratio and greater number of particles. These can improve the sedimentation stability by inducing higher drag between the particles and the carrier ๏ฌ‚uid or by forming a thicker nanoparticle halo around the micron-sized particles. The nanoparticles had only a minor impact on the ๏ฌ‚uids MR response, but often increased the ๏ฌeld independent viscosity, which can be considered as a disadvantage in some applications

    Rheological Characterization of Magnetorheological Fluids

    Get PDF
    Magnetorheological (MR) ๏ฌ‚uids are smart materials that respond to an external magnetic ๏ฌeld by changing their rheological properties. These ๏ฌeld dependent properties are typically studied by rotational rheometry. Since the data of the rotational rheometer measurements may include errors caused by various sources, it is essential to study the rheological characterization of the MR ๏ฌ‚uids before the results are used in research. A major drawback of MR ๏ฌ‚uids is sedimentation that may weaken ๏ฌ‚uids MR response over time. The sedimentation is settling of magnetic particles induced by the large density mismatch between the particles and the carrier ๏ฌ‚uid. In this study, the rheological characterization of MR ๏ฌ‚uids by a rotational rheometer is ๏ฌrst examined to reveal how the measurements should be done in order to gain reliable knowledge about their properties. Secondly a bidisperse size distribution of magnetic particles, consisting of micron- and nano-sized particles, was studied as a way to improve the sedimentation stability.The study of rheological characterization of MR ๏ฌ‚uids by rotational rheometer involved determination ๏ฌeld dependent yield stresses by using various measuring procedures and plate-plate measuring geometries with di๏ฌ€erent surfaces. The results demonstrated that the measured static and dynamic yield stresses are strongly a๏ฌ€ected by the plate surface characteristics as the magnetic and roughened plates provided considerably higher values than the smooth non-magnetic plates. A likely source for the di๏ฌ€erence is wall slip that may happen during rotational rheometer measurements. Furthermore, it was shown that the wall slip of MR ๏ฌ‚uid does not cause measuring gap height dependency of the results, which is surprising, as its existence is commonly used as an indicator of the wall slip.The bidisperse MR ๏ฌ‚uids were prepared by dispersing micron- and nano-sized particles in Silicone Oil (SO) or Ionic liquid (IL). The impact of the carrier ๏ฌ‚uid type and nanoparticle fraction, composition and size on the o๏ฌ€-state viscosity, sedimentation stability and MR response were studied. The maghemite (ฮณ โˆ’ Fe2O3) nanoparticles used in the study were synthesized by Liquid Flame Spray (LFS) method that o๏ฌ€ers an interesting alternative for the chemical co-precipitation commonly used to prepare magnetic nanoparticles as it is a very versatile process. The dispersion of the micron-sized particles was better IL than in SO indicated by lower o๏ฌ€-state viscosity and higher MR response. A partial substitution of micron-sized particles by nanoparticles provided improved sedimentation stability with both carrier ๏ฌ‚uids. The impact became stronger as the nanoparticle fraction was increased or the nanoparticle size was decreased. Both lead to higher particle surface to volume ratio and greater number of particles. These can improve the sedimentation stability by inducing higher drag between the particles and the carrier ๏ฌ‚uid or by forming a thicker nanoparticle halo around the micron-sized particles. The nanoparticles had only a minor impact on the ๏ฌ‚uids MR response, but often increased the ๏ฌeld independent viscosity, which can be considered as a disadvantage in some applications

    Rheological and stability properties of magnetorheological fluid with superparamagnetic maghemite nanoparticles

    Get PDF
    This research is focused on the development of a new magnetorheological (MR) fluid which contains maghemite (ฮณ-Fe2O3) nanoparticles so as to improve its performance. The performance of MR fluid is presented in terms of physical and rheological properties and its application in MR device. In this work, the ฮณ-Fe2O3 has been synthesized using co-precipitation method and coated with oleic acid. Two types of MR fluids were prepared, bidisperse MR fluid containing carbonyl iron (CI) microparticles substituted with ฮณ-Fe2O3 and MR fluid utilizing ฮณ-Fe2O3 additive. MR fluid containing ฮณ-Fe2O3 showed great improvement exhibiting reduced sedimentation rate and enhanced re-dispersibility. During the period of 50 hours, the bidisperse MR fluid with 5 wt% of ฮณ-Fe2O3 reduced 15% of sedimentation rate and MR fluid with 1 wt% of ฮณ-Fe2O3 additive reduced 9.6% of sedimentation rate compared to pure CI MR fluid. The rheological properties of the MR fluid were analyzed with respect to the rheological models of Bingham Plastic, Herschel Bulkley and Casson models. The rheological properties of bidisperse MR fluid revealed that the substitution of 5 wt% ฮณ-Fe2O3 increased the yield stress by 8.5% but further substitution of ฮณ-Fe2O3 would slightly decrease the yield stress. On the other hand, the MR fluid added with ฮณ-Fe2O3 additive showed improvement in yield stress over the entire range of magnetic field applied. The results indicated that the addition of 1 wt% of ฮณ-Fe2O3 in MR fluid increased the yield stress by 11.7%. The performance of MR fluid using MR valve equipped with a hydraulic bypass damper resulted in improvement of damping force when ฮณ-Fe2O3 is added. The MR fluid with 1 wt% ฮณ-Fe2O3 additive improved the maximum damping force up to 11.1% compared to the pure MR fluid. Therefore, the substitution and addition of ฮณ-Fe2O3 nanoparticles in the MR fluid improved both its physical and rheological properties, hence it can potentially be used in commercial application as a simple and reliable damping device

    ์นจ๊ฐ• ์•ˆ์ •์„ฑ์ด ํ–ฅ์ƒ๋œ ๊ณ ์„ฑ๋Šฅ ์ž๊ธฐ์œ ๋ณ€์œ ์ฒด์— ๋Œ€ํ•œ ์—ฐ๊ตฌ

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์žฌ๋ฃŒ๊ณตํ•™๋ถ€, 2020. 8. ์„œ์šฉ์„.Magnetorheological (MR) fluids are typically consist of magnetic particles (Carbonyl Iron, Fe2O3, Fe3O4 and so on) in a magnetically insulating fluid (water, silicon oil and so on). When a magnetic field induces attractive interactions between the magnetic particles, these particles form a solid-like network of fibril shapes within a few milliseconds oriented along the direction of the magnetic field. Reverse transition occurs as soon as the magnetic field is switched off. These features lead to remarkable changes in the rheological properties of the fluid which shows wide potential applications such as dampers, brakes, shock observers, drug delivery, and robotics, etc and could be controlled by adjusting the strength of the magnetic field depending on applications. Despite substantial advanced in commercialization, MR fluids have long-term stability issues that significantly limit their usefulness and also need to be predicted the precise flow behavior. In this thesis, we propose the constitutive equation to predict the flow behavior of MR fluid and investigate a number of MR fluid composed of soft-magnetic composite particles to overcome the sedimentation drawback. Firstly, as modeling and analysis are essential to optimize material design, describe the flow behavior over a wide range of shear rate and distinguish between static yield stress and dynamic yield stress, the precise knowledge of the relationships between the suspension rheological properties and such variables as the deformation rate, the applied magnetic field strength, and the composition are required. So we re-analyze the constitutive equation proposed before to describe the MR fluids flow and propose new constitutive equation. The proposed Seo-Seo model predicted the flow behavior precisely compared to pre-exist constitutive model and also yielded a quantitatively and qualitatively precise description of MR fluid rheological behavior based on relatively few experimental measurements. To overcome sedimentation drawback, the core/shell structured Foamed polystyrene/Fe3O4 Particles were synthesized by applying a dual-step processing comprising pickering emulsion polymerization, subsequently by the foaming of polystyrene core using the supercritical carbon dioxide fluid foaming process. Through these processes, the density of composite was dropped significantly and the long-term stability was improved. As polystyrene located core part and magnetic particle contact directly, the magnetorheological properties of the Foamed polystyrene/Fe3O4 were considerable compared to pure Fe3O4. Even though the core/shell structured Foamed polystyrene/Fe3O4 showed considerable level, the magnetorheological properties got worsen because polystyrene is magnetically non-active. So, we synthesized hollow shape Fe3O4 particles without any magnetically non-active template. As a result, compared to the core/shell structured Foamed polystyrene/Fe3O4, the density of hollow shape Fe3O4 particles rise slightly and the magnetorheological properties reached outstanding level, and the long-term stability maintained. Also, the conformation of solid-like network of fibril shapes changes were investigated by using micro/nano size Fe3O4 particles to verify the reinforcement effect. As the particle size increases, the magnetorheological properties improve due to a rise of the magnetic saturation level. However, depending on the ratio of the nano size Fe3O4 particles, an overturning of the magnetorheological properties and the magnetic saturation was observed. This phenomenon is because of the cavity among the micro size Fe3O4 particles. The micro size Fe3O4 particles develops a relatively coarse solid-like network of fibril shapes. The chain conformation of a bidisperse MR fluid shows quite different from that of the micron size Fe3O4 particles-based fluids. The nano size Fe3O4 particles appear to fill in the cavity among the micro size Fe3O4 particles. As a result, this distinct conformation reinforced the magnetorheological properties. Finally, the shape effect of the magnetic particle on magnetorheological properties and sedimentation stability was investigated by using two types of sendust which are bulk and flake type. The flake type sendust has a small demagnetization factor because its domain orients one direction. This feature lead to extraordinary behavior which is a rapid transition to solid-like network at low magnetic field. Also, its high aspect ratio leads to a large drag coefficient which improve the long-term stability.์ž๊ธฐ์œ ๋ณ€์œ ์ฒด๋Š” ๋ฌผ ๋˜๋Š” ๋น„์ˆ˜๊ณ„(์‹ค๋ฆฌ์ฝ˜ ์˜ค์ผ ๋“ฑ)์˜ ์œ ์ฒด์— ์žํ™” ๊ฐ€๋Šฅํ•œ ๋ฏธ์„ธ์ž…์ž(์ฒ  ๋งˆ์ดํฌ๋กœ ์ž…์ž)๋ฅผ ๋ถ„์‚ฐ์‹œํ‚จ ํ˜„ํƒ์•ก์œผ๋กœ์„œ, ์™ธ๋ถ€๋กœ๋ถ€ํ„ฐ ์ œ๊ณต๋˜๋Š” ๊ฐ•ํ•œ ์ž๊ธฐ์žฅ์— ๋”ฐ๋ผ ์งง์€ ์‹œ๊ฐ„์•ˆ์— ํƒ„์„ฑ, ์†Œ์„ฑ, ์ ๋„ ๊ฐ™์€ ์ž๊ธฐ์œ ๋ณ€ํšจ๊ณผ๋ฅผ ๋‚˜ํƒ€๋‚ด๋Š” ์œ ์ฒด๋ฅผ ๋งํ•œ๋‹ค. ์ž๊ธฐ์œ ๋ณ€์œ ์ฒด๋Š” ์™ธ๋ถ€ ์ž๊ธฐ์žฅ์— ์˜ํ•ด ์œ ๋ณ€ํšจ๊ณผ๋ฅผ ์กฐ์ ˆํ•  ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์— ๋‹ค์–‘ํ•œ ์‘์šฉ๋ถ„์•ผ๋กœ์˜ ์ ์šฉ ๊ฐ€๋Šฅ์„ฑ์— ๋Œ€ํ•œ ๊ด€์‹ฌ์ด ์ฆ๊ฐ€ํ•˜๊ณ  ์žˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์ž์„ฑ์ž…์ž์™€ ํ˜„ํƒ ์œ ์ฒด์™€์˜ ๋ฐ€๋„ ์ฐจ์— ์˜ํ•ด ๋ฐœ์ƒํ•˜๋Š” ์นจ์ „ํ˜„์ƒ์œผ๋กœ ์ธํ•ด ์ž๊ธฐ์œ ๋ณ€์œ ์ฒด์˜ ์‹ค์ œ์ ์ธ ์‘์šฉ์ด ์ œํ•œ๋˜๊ณ  ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ž๊ธฐ์œ ๋ณ€์œ ์ฒด์˜ ๊ฑฐ๋™์„ ์˜ˆ์ธกํ•˜๋Š” ๊ตฌ์„ฑ๋ฐฉ์ •์‹์„ ์ œ์•ˆํ•˜๊ณ , ์นจ์ „ ๋ฌธ์ œ๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ์—ฐ์ž์„ฑ ๋ณตํ•ฉ์ฒด๋กœ ๊ตฌ์„ฑ๋œ ์ž๊ธฐ์œ ๋ณ€์œ ์ฒด๋ฅผ ์กฐ์‚ฌํ•œ๋‹ค. ์žฌ๋ฃŒ ์„ค๊ณ„๋ฅผ ์ตœ์ ํ™”ํ•˜๊ธฐ ์œ„ํ•ด ํ•„์ˆ˜์ ์œผ๋กœ ๊ด‘๋ฒ”์œ„ํ•œ ์ „๋‹จ ์†๋„์— ๊ฑธ์นœ ํ๋ฆ„ ๋™์ž‘์„ ์„ค๋ช…ํ•˜๊ณ  ์ •์  ํ•ญ๋ณต ์‘๋ ฅ๊ณผ ๋™์  ํ•ญ๋ณต ์‘๋ ฅ์„ ๊ตฌ๋ถ„ํ•˜์—ฌ์•ผ ํ•œ๋‹ค. ๋˜ํ•œ, ํ˜„ํƒ์•ก์˜ ์œ ์ „ํ•™์  ํŠน์„ฑ๊ณผ ๋ณ€ํ˜•๋ฅ , ์ ์šฉ๋œ ์ž๊ธฐ์žฅ ๊ฐ•๋„ ๋ฐ ๊ตฌ์„ฑ๊ณผ ๊ฐ™์€ ๋ณ€์ˆ˜ ์‚ฌ์ด์˜ ๊ด€๊ณ„์— ๋Œ€ํ•œ ์ •ํ™•ํ•œ ์ง€์‹์ด ํ•„์š”ํ•˜๋‹ค. ๋”ฐ๋ผ์„œ, ์ž๊ธฐ์œ ๋ณ€์œ ์ฒด์˜ ํ๋ฆ„์„ ์„ค๋ช…ํ•˜๊ธฐ ์œ„ํ•œ ๊ธฐ์กด์˜ ์ œ์•ˆ๋œ ๊ตฌ์„ฑ๋ฐฉ์ •์‹์„ ๋ถ„์„ํ•˜๊ณ  ์ƒˆ๋กœ์šด ๊ตฌ์„ฑ๋ฐฉ์ •์‹์„ ์ œ์•ˆํ•œ๋‹ค. ์ƒˆ๋กญ๊ฒŒ ์ œ์•ˆํ•œ ๊ตฌ์„ฑ ๋ฐฉ์ •์‹์ธ ์„œ-์„œ ๋ชจ๋ธ์€ ๊ธฐ์กด์— ์กด์žฌํ•˜๋Š” ๊ตฌ์„ฑ๋ฐฉ์ •์‹๊ณผ ๋น„๊ตํ•˜์—ฌ ์œ ์ฒด์˜ ํ๋ฆ„์„ ์ •ํ™•ํ•˜๊ฒŒ ์˜ˆ์ธกํ•˜์˜€๊ณ , ๋น„๊ต์  ์ ์€ ์‹คํ—˜ ๊ฐ’์„ ๋ฐ”ํƒ•์œผ๋กœ ์ž๊ธฐ์œ ๋ณ€์œ ์ฒด์˜ ํ๋ฆ„์— ๋Œ€ํ•œ ์ •๋Ÿ‰์ , ์งˆ์ ์œผ๋กœ ์ •๋ฐ€ํ•œ ์„ค๋ช…์„ ๋„์ถœํ•˜์˜€๋‹ค. ์นจ์ „ ๋ฌธ์ œ๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ํ”ผ์ปค๋ง ์—๋ฉ€์ „ ์ค‘ํ•ฉ์„ ๋ฐ ์ดˆ์ž„๊ณ„ ์ด์‚ฐํ™”ํƒ„์†Œ๋ฅผ ์ด์šฉํ•œ ๋ฐœํฌ๊ณต์ •์˜ ์ด์ค‘ ๊ณต์ • ์ฒ˜๋ฆฌ๋ฅผ ํ†ตํ•ด ์ฝ”์–ด-์‰˜ ๊ตฌ์กฐ์˜ ๋ฐœํฌ ์Šคํƒ€์ด๋ Œ ๊ณ ๋ถ„์ž-์ฒ  ๋ณตํ•ฉ์ฒด๋ฅผ ํ•ฉ์„ฑํ•˜์˜€๋‹ค. ์ด์ค‘ ๊ณต์ • ์ฒ˜๋ฆฌ๋ฅผ ํ†ตํ•ด ๋ณตํ•ฉ์ฒด์˜ ๋ฐ€๋„๊ฐ€ ํ˜„์ €ํžˆ ๋–จ์–ด์ง€๊ณ  ์žฅ๊ธฐ ์•ˆ์ •์„ฑ์ด ํ–ฅ์ƒ๋˜์—ˆ๋‹ค. ๋˜ํ•œ, ์Šคํƒ€์ด๋ Œ์ด ์ฝ”์–ด ๋ถ€๋ถ„์— ์œ„์น˜ํ•˜์—ฌ, ์ฒ  ์ž…์ž๊ฐ€ ์ง์ ‘์ ์ธ ์ ‘์ด‰์„ ํ†ตํ•ด ๋†’์€ ์ž๋ ฅ ํŠน์„ฑ์„ ์–ป์—ˆ๋‹ค. ์ฝ”์–ด-์‰˜ ๊ตฌ์กฐ์˜ ๋ฐœํฌ ์Šคํƒ€์ด๋ Œ ๊ณ ๋ถ„์ž-์ฒ  ๋ณตํ•ฉ์ฒด์˜ ์ž๋ ฅ ํŠน์„ฑ์ด ์ƒ๋‹นํ•œ ์ˆ˜์ค€์„ ๋ณด์˜€์Œ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ , ์Šคํƒ€์ด๋ Œ์ด ์ž๋ ฅ์ ์œผ๋กœ ๋น„ํ™œ์„ฑํ™” ๋ฌผ์งˆ์ด๋ฏ€๋กœ ์ˆœ์ˆ˜ํ•œ ์ฒ ์— ๋น„ํ•ด ์ž๋ ฅ ํŠน์„ฑ์€ ์•ฝํ™”๋˜์—ˆ๋‹ค. ๋”ฐ๋ผ์„œ ์ž๋ ฅ์ ์œผ๋กœ ๋น„ํ™œ์„ฑํ™” ๋ฌผ์งˆ์ธ ์Šคํƒ€์ด๋ Œ์„ ์ œ๊ฑฐํ•˜์—ฌ ์ง€์ง€๋Œ€๊ฐ€ ์—†๋Š” ์ค‘๊ณตํ˜•์ƒ์˜ ์ฒ  ์ž…์ž๋ฅผ ํ•ฉ์„ฑํ•˜์˜€๋‹ค. ๊ทธ ๊ฒฐ๊ณผ, ์ฝ”์–ด-์‰˜ ๊ตฌ์กฐ์˜ ๋ฐœํฌ ์Šคํƒ€์ด๋ Œ ๊ณ ๋ถ„์ž-์ฒ  ๋ณตํ•ฉ์ฒด์— ๋น„ํ•ด ์ค‘๊ณตํ˜•์ƒ์˜ ์ฒ  ์ž…์ž๋Š” ๋ฐ€๋„๊ฐ€ ์•ฝ๊ฐ„ ์ƒ์Šนํ•˜์˜€์œผ๋‚˜ ๋†’์€ ์ž๋ ฅํŠน์„ฑ์„ ๋ณด์˜€๊ณ  ์žฅ๊ธฐ ์•ˆ์ •์„ฑ์ด ์œ ์ง€๋˜์—ˆ๋‹ค. ์ถ”๊ฐ€์ ์œผ๋กœ ๋งˆ์ดํฌ๋กœ/๋‚˜๋…ธ ํฌ๊ธฐ์˜ ์ฒ  ์ž…์ž๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ํ”ผ๋ธŒ๋ฆด ๊ตฌ์กฐ์˜ ๋ณด๊ฐ•ํšจ๊ณผ๋ฅผ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ์ž…์ž ํฌ๊ธฐ๊ฐ€ ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ ์ž๊ธฐ ํฌํ™” ์ˆ˜์ค€์˜ ์ƒ์Šน์œผ๋กœ ์ž๋ ฅํŠน์„ฑ์ด ๊ฐœ์„ ๋˜์—ˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜, ๋‚˜๋…ธ ํฌ๊ธฐ์˜ ์ฒ  ์ž…์ž์˜ ๋น„์œจ์— ๋”ฐ๋ผ ์ž๋ ฅํŠน์„ฑ๊ณผ ์ž๊ธฐ ํฌํ™” ํ˜„์ƒ์˜ ์—ญ์ „ํ˜„์ƒ์ด ๊ด€์ฐฐ๋˜์—ˆ๋‹ค. ์ด ํ˜„์ƒ์€ ๋งˆ์ดํฌ๋กœ ํฌ๊ธฐ์˜ ์ฒ  ์ž…์ž์˜ ํ”ผ๋ธŒ๋ฆด ๊ตฌ์กฐ๋ฅผ ํ˜•์„ฑ์‹œ์— ์ฒ  ์ž…์ž ์‚ฌ์ด์˜ ๊ณต๋™๋•Œ๋ฌธ์ด๋‹ค. ๋งˆ์ดํฌ๋กœ ํฌ๊ธฐ์˜ ์ฒ  ์ž…์ž๋Š” ๋น„๊ต์  ๊ฑฐ์นœ ํ”ผ๋ธŒ๋ฆด ๊ตฌ์กฐ๋ฅผ ํ˜•์„ฑํ•œ๋‹ค. ํ˜ผ์„ฑ ์ž๊ธฐ์œ ๋ณ€์ฒด๋Š” ๋งˆ์ดํฌ๋กœ ํฌ๊ธฐ์˜ ์ฒ  ์ž…์ž์™€๋Š” ๋‹ค๋ฅธ ํ”ผ๋ธŒ๋ฆด ๊ตฌ์กฐ๋ฅผ ํ˜•์„ฑํ•œ๋‹ค. ๋‚˜๋…ธ ํฌ๊ธฐ์˜ ์ฒ  ์ž…์ž๋“ค์ด ๋งˆ์ดํฌ๋กœ ํฌ๊ธฐ์˜ ์ฒ  ์ž…์ž ์‚ฌ์ด์˜ ๊ณต๋™์„ ์ฑ„์›€์œผ๋กœ ์ธํ•ด์„œ ์ž๋ ฅํŠน์„ฑ์ด ํ–ฅ์ƒ๋˜์—ˆ๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, ๋ฒŒํฌํ˜•๊ณผ ๋ฐ•๋ฆฌํ˜•์˜ ์„ผ๋”์ŠคํŠธ๋ฅผ ์ด์šฉํ•˜์—ฌ ์ž๊ธฐ์ž…์ž์˜ ๋ชจ์–‘์ด ์œ ๋ณ€์  ํŠน์„ฑ์— ๋ผ์น˜๋Š” ์˜ํ–ฅ์„ ์กฐ์‚ฌํ•˜์˜€๋‹ค. ๋ฐ•๋ฆฌํ˜• ์„ผ๋”์ŠคํŠธ์˜ ์ž๊ตฌ๋Š” ํ•œ ๋ฐฉํ–ฅ์œผ๋กœ ์ •๋ ฌ๋˜์–ด ์žˆ์–ด ์ž‘์€ ๊ฐ์ž์œจ์„ ๊ฐ–๊ณ , ์ด ํŠน์ง•์€ ์ €์ž๊ธฐ์žฅ์—์„œ ํ”ผ๋ธŒ๋ฆด ๊ตฌ์กฐ๋กœ์˜ ๋น ๋ฅธ ์ „ํ™˜์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•œ๋‹ค. ๋˜ํ•œ, ๋ฐ•๋ฆฌํ˜• ์„ผ๋”์ŠคํŠธ์˜ ๋†’์€ ์ข…ํšก๋น„๋กœ ์ธํ•œ ํ•ญ๋ ฅ๊ณ„์ˆ˜๋Š” ์žฅ๊ธฐ ์•ˆ์ •์„ฑ์„ ํ–ฅ์ƒ์‹œ์ผฐ๋‹ค.Chapter 1. Introduction and Background . 0 1.1. Magnetorheological (MR) Fluids 0 1.2. Applications of MR fluids . 2 1.3. Rheology 2 1.3.1. Flow behavior . 3 1.3.1.1. Definition of terms 3 1.3.1.1.1. Shear stress 5 1.3.1.1.2. Shear rate 5 1.3.1.1.3. Shear viscosity . 5 1.3.1.2. Flow and viscosity curve 7 1.3.1.2.1. Ideal viscous flow. 7 1.3.1.2.2. Shear-thinning flow and Shear-thickening . 9 1.3.1.2.3. Yield stress 9 1.3.2. Viscoelastic behavior 11 1.3.2.1. Storage modulus and Loss modulus . 11 Reference 12 Chapter 2. Constitutive Equation . 14 2.1. Introduction . 14 2.2. Rheological Models for the Yield Stress . 18 2.2.1. Static Yield Stress versus Dynamic Yield Stress . 18 2.2.2. Yield Stress Dependency on the Magnetic Field Strength 22 2.2.3. Mechanism of Structure Evolution . 24 2.3. Conclusion . 26 Reference . 27 Chapter 3. High-Performance Magnetorheological Suspensions of Pickering Emulsion Polymerized Polystyrene/Fe3O4 Particles with Enhanced Stability 31 3.1. Introduction 31 3.2. Experimental Section 33 3.2.1. Synthesis of Polystyrene/Fe3O4 particles . 33 3.2.2. Synthesis of Foamed Polystyrene/Fe3O4 particles 34 3.2.3. Characterization 37 3.3. Results and Discussion 41 3.3.1 Morphology . 41 3.3.2. Magnetorheological Behaviors . 42 3.3.3. Yield Stress of the MR Fluids 47 3.3.4. Structure Evolution Mechanism and the Suspension Stability . 54 3.4. Conclusion . 59 References . 61 Chapter 4. Template Free Hollow Shaped Fe3O4 Micro-Particles for Magnetorheological Fluid . 65 4.1 Introduction . 65 4.2. Experiment Section . 67 4.2.1. Synthesis of Fe3O4 particles (Pure Fe3O4) . 67 4.2.2. Synthesis of PS/Fe3O4 particles (Picker) . 68 4.2.3. Synthesis of PS/Fe3O4@Fe3O4 particles (C-picker) 68 4.2.4. Synthesis of templet free hollow shaped Fe3O4 (H-Picker) . 69 4.2.5. Characterization 69 4.3. Results and Discussion . 70 4.3.1. Particle Morphologies and Magnetic Hysteresis Curve 70 4.3.2. Magnetorheological Behaviors . 76 4.3.3. Yield Stress of the MR Fluids . 80 4.3.4. Mechanism of Structure Evolution and Suspension Stability . 84 4.4. Conclusion 89 Reference 90 Chapter 5. Bidisperse MR Fluids Using Nano/micro Size Fe3O4 particles . 95 5.1. Introduction 95 5.2. Experiment Section 99 5.2.1. Material. 99 5.2.2. Characterization Methods . 99 5.3. Results and Discussion . 99 5.4. Conclusion 106 References . 107 Chapter 6. Shape effect of magnetic particle on magnetorheological (MR) properties and sedimentation stability 108 6.1. Introduction . 108 6.2. Experiment Section . 109 6.2.1. Material . 109 6.2.2. Characterization Methods 109 6.3. Results and Discussion 110 6.3.1. Particle Morphologies and Magnetic Hysteresis Curve . 110 6.3.2. Magnetorheological Behaviors 116 6.3.3. Yield Stress of the MR Fluids . 120 6.3.4. Mechanism of Structure Evolution and Suspension Stability . 124 6.4. Conclusion . 129 References 130 Chapter 7. Conclusions 135 ๊ตญ๋ฌธ์ดˆ๋ก 139 List of Publication 141 Appendix . 142 Appendix A. Improvement of Mechanical Properties by Introducing Curable Functional Monomers in Stereolithography 3D PrintingDocto

    Chain formation and phase separation in ferrofluids: The influence on viscous properties

    Full text link
    Ferrofluids have attracted considerable interest from researchers and engineers due to their rich set of unique physical properties that are valuable for many industrial and biomedical applications. Many phenomena and features of ferrofluids' behavior are determined by internal structural transformations in the ensembles of particles, which occur due to the magnetic interaction between the particles. An applied magnetic field induces formations, such as linear chains and bulk columns, that become elongated along the field. In turn, these structures dramatically change the rheological and other physical properties of these fluids. A deep and clear understanding of the main features and laws of the transformations is necessary for the understanding and explanation of the macroscopic properties and behavior of ferrofluids. In this paper, we present an overview of experimental and theoretical works on the internal transformations in these systems, as well as on the effect of the internal structures on the rheological effects in the fluids. ยฉ 2020 by the authors.The research was carried out within the state assignment of the Ministry of Science and Higher Education of the Russian Federation, (theme โ€œMagnet,โ€ contract no. 02.A03.21.006 and project no. FEUZ-2020-0051)
    corecore