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Journal articles on the topic 'Electrorheological fluids'

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1

OTSUBO, Yasufumi. "Electrorheological Fluids." Journal of the Japan Society of Colour Material 72, no. 5 (1999): 319–27. http://dx.doi.org/10.4011/shikizai1937.72.319.

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2

Agafonov, A. V., and A. G. Zakharov. "Electrorheological fluids." Russian Journal of General Chemistry 80, no. 3 (March 2010): 567–75. http://dx.doi.org/10.1134/s1070363210030382.

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3

Halsey, Thomas C., and James E. Martin. "Electrorheological Fluids." Scientific American 269, no. 4 (October 1993): 58–64. http://dx.doi.org/10.1038/scientificamerican1093-58.

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4

Halsey, T. C. "Electrorheological Fluids." Science 258, no. 5083 (October 30, 1992): 761–66. http://dx.doi.org/10.1126/science.258.5083.761.

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5

Duclos, Theodore G. "Electrorheological fluids." Journal of the Acoustical Society of America 88, S1 (November 1990): S100. http://dx.doi.org/10.1121/1.2028465.

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6

Hao, T. "Electrorheological Fluids." Advanced Materials 13, no. 24 (December 2001): 1847. http://dx.doi.org/10.1002/1521-4095(200112)13:24<1847::aid-adma1847>3.0.co;2-a.

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7

Gun Ko, Young, and Ung Su Choi. "Negative electrorheological fluids." Journal of Rheology 57, no. 6 (November 2013): 1655–67. http://dx.doi.org/10.1122/1.4821857.

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8

Zhang, Liucheng, Kai Su, and Xiucuo Li. "Electrorheological effects of polyaniline-type electrorheological fluids." Journal of Applied Polymer Science 87, no. 5 (December 3, 2002): 733–40. http://dx.doi.org/10.1002/app.11356.

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9

Halsey, Thomas C., James E. Martin, and Douglas Adolf. "Rheology of electrorheological fluids." Physical Review Letters 68, no. 10 (March 9, 1992): 1519–22. http://dx.doi.org/10.1103/physrevlett.68.1519.

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10

Halsey, Thomas C., and Will Toor. "Structure of electrorheological fluids." Physical Review Letters 65, no. 22 (November 26, 1990): 2820–23. http://dx.doi.org/10.1103/physrevlett.65.2820.

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11

Zgaevskii, V. É. "Description of electrorheological fluids." Doklady Physics 48, no. 5 (May 2003): 224–27. http://dx.doi.org/10.1134/1.1581316.

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12

Klingenberg, Daniel J., Peyman Pakdel, Young Dae Kim, Brett M. Belongia, and Sangtae Kim. "Protein-enhanced electrorheological fluids." Industrial & Engineering Chemistry Research 34, no. 10 (October 1995): 3303–6. http://dx.doi.org/10.1021/ie00037a016.

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13

Tao, R., J. Zhang, Y. Shiroyanagi, X. Tang, and X. Zhang. "ELECTRORHEOLOGICAL FLUIDS UNDER SHEAR." International Journal of Modern Physics B 15, no. 06n07 (March 20, 2001): 918–29. http://dx.doi.org/10.1142/s0217979201005441.

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The behavior of an electrorheological (ER) chain under a shear force is investigated theoretically and experimentally. Contrary to the conventional assumption that the ER chain under a shear force becomes slanted and breaks at the middle, we have found that there is symmetry breaking. When the shear strain is small, the chain becomes slanted with a space gap between the first and second particles (or between the last and next last particles). As the shear strain increases, the gap becomes wider and wider. When the shear strain exceeds a critical value, the chain breaks at the gap. The experiment also confirms that an ER chain under the shear breaks at either end, not at the middle. This symmetry breaking reflects the space's anisotropy, which is the result of the applied electric field.
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14

Dassanayake, U., S. Fraden, and A. van Blaaderen. "Structure of electrorheological fluids." Journal of Chemical Physics 112, no. 8 (February 22, 2000): 3851–58. http://dx.doi.org/10.1063/1.480933.

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15

Jekal, Suk, Jiwon Kim, Qi Lu, Dong-Hyun Kim, Jungchul Noh, Ha-Yeong Kim, Min-Jeong Kim, et al. "Development of Novel Colorful Electrorheological Fluids." Nanomaterials 12, no. 18 (September 8, 2022): 3113. http://dx.doi.org/10.3390/nano12183113.

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Herein, the electrorheological (ER) performances of ER fluids were correlated with their colors to allow for the visual selection of the appropriate fluid for a specific application using naked eyes. A series of TiO2-coated synthetic mica materials colored white, yellow, red, violet, blue, and green (referred to as color mica/TiO2 materials) were fabricated via a facile sol–gel method. The colors were controlled by varying the thickness of the TiO2 coating layer, as the coatings with different thicknesses exhibited different light interference effects. The synthesized color mica/TiO2 materials were mixed with silicone oil to prepare colored ER fluids. The ER performances of the fluids decreased with increasing thickness of the TiO2 layer in the order of white, yellow, red, violet, blue, and green materials. The ER performance of differently colored ER fluids was also affected by the electrical conductivity, dispersion stability, and concentrations of Na+ and Ca2+ ions. This pioneering study may provide a practical strategy for developing new ER fluid systems in future.
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16

Wei, Kexiang, Guang Meng, and Shisha Zhu. "Fluid Power Control Unit using Electrorheological Fluids." International Journal of Fluid Power 5, no. 3 (January 2004): 49–54. http://dx.doi.org/10.1080/14399776.2004.10781201.

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17

McLeish, T. C. B. "Anisotropic Hydrodynamic Screening in Electrorheological Fluids." International Journal of Modern Physics B 10, no. 23n24 (October 30, 1996): 3375–81. http://dx.doi.org/10.1142/s0217979296001823.

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We present an approximate calculation of the effective hydrodynamic interaction in a complex fluid of aligned strings in a solvent, an appropriate model for semi-dilute electrorheological fluids in which the string formation has not proceeded to “clumping”. Earlier results indicated that the presence of weak screening could be detected in the frequency-dependent modulus of ER fluids with field applied. This calculation supports the conclusion that weak (logarithmic) modification of the imposed fluid flow is effective for relaxation modes which couple to the transverse deformations of the strings, but that shear waves parallel to the aligned strings are much less effectively screened.
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18

DROUOT, R., G. NAPOLI, and G. RACINEUX. "Continuum modelling of electrorheological fluids." International Journal of Modern Physics B 16, no. 17n18 (July 20, 2002): 2649–54. http://dx.doi.org/10.1142/s0217979202012797.

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A thermodynamical continuum modelling is proposed for electrorheological fluids. This theormodynamical approach tries to describe the response of an electrorheological fluid in the solid phase (which means with an applied adequate electric field) under mechanical solicitations. Thermodynamic formulations distinguish the contributions due to reversible and irreversible process. In an electrorheological fluid the microstructure generated by the application of an electric field introduces parameters whose the evolution of which influence the behavior. These parameters will be defined as internal variables, or hidden variables, in the formulation of thermodynamics. They are used for the description of dissipative effects. The choice and the number of pertinent parameters are crucial and need to be selected according to the nature of microscopic mechanism and experimental observations. The presence of fibrous structures in the E.R. fluid, when an electric field is applied, is an observed fact. In the theory of thermodynamics with internal variables, the introduction of internal variables doesn't modify, by hypothesis, the balance equations. Nevertheless, the experiments show the existence of hysteresis phenomenon due to the reorganization, at the microscopic level, of the particle that compose the fibers. In order to describe these phenomena, we introduce two internal variables following an idea of Kiryushin.
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19

CONRAD, H., Y. CHEN, and A. F. SPRECHER. "THE STRENGTH OF ELECTRORHEOLOGICAL (ER) FLUIDS." International Journal of Modern Physics B 06, no. 15n16 (August 1992): 2575–94. http://dx.doi.org/10.1142/s0217979292001304.

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The definition of the strength of an ER fluid is discussed. Studies on the electrorheology of ER fluids containing zeolite particles in various oils indicate that the order of magntiude difference between the measured values of the yield stress and those calculated based on the axial force of interaction between particles in a single-row chain can be explained by an enhancement of the force due to the observed clustering of particles into multi-row chains. The force enhancement factor varied with the shear rate and the concentration of particles, but was relatively independent of the electric field, temperature and host fluid. Reasonable agreement existed between the predicted and the measured shear stress-shear strain curves and the concentration dependence of the yield stress when the appropriate force enhancement factor was taken into account. The present theoretical-experimental considerations suggest that ER fluids may attain a yield strength of ~ 50 kPa .
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20

Santos, Jenifer, Sumita Goswami, Nuria Calero, and Maria Teresa Cidade. "Electrorheological behaviour of suspensions in silicone oil of doped polyaniline nanostructures containing carbon nanoparticles." Journal of Intelligent Material Systems and Structures 30, no. 5 (January 10, 2019): 755–63. http://dx.doi.org/10.1177/1045389x18818776.

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Electrorheological fluids have been paying a lot of attention due to their potential use in active control of various devices in mechanics, biomedicine or robotics. An electrorheological fluid consisting of polarizable particles dispersed in a non-conducting liquid is considered to be one of the most interesting and important smart fluids. This work presents the effect of the dopant, camphorsulphonic acid or citric acid, on the electrorheological behaviour of suspensions of doped polyaniline nanostructures dispersed in silicone oil, revealing its key role. The influence of carbon nanoparticle concentration has also been studied for these dispersions. All the samples showed an electrorheological effect, which increased with electric field and nanostructure concentration and decreased with silicone oil viscosity. However, the magnitude of this effect was strongly influenced not only by carbon nanoparticle concentration but also by the dopant material. The electrorheological effect was much lower with a higher carbon nanoparticle concentration and doped with citric acid. The latter is probably due to the different acidities of the dopants that lead to a different conductivity of polyaniline nanostructures. Furthermore, the effect of the carbon nanoparticles could be related to its charge trapping mechanism, while the charge transfer through the polymeric backbone occurs by hopping. Polyaniline/camphorsulphonic acid composite nanostructures dispersed in silicone oil exhibited the highest electrorheological activity, higher than three decades increase in apparent viscosity for low shear rates and high electric fields, showing their potential application as electrorheological smart materials.
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21

YANOVSKY, YU G., V. E. ZGAEVSKII, Z. P. SHULMAN, and E. V. KOROBKO. "ER-FLUID RHEOLOGICAL PROPERTIES IN TERMS OF THE MULTIPARTICLE MODEL OF A COMPOSITE." International Journal of Modern Physics B 16, no. 17n18 (July 20, 2002): 2676–82. http://dx.doi.org/10.1142/s0217979202012839.

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The three-dimensional multi-particle well-ordered model could be considered as an analogy to a crystal body. We use this model for describing rheological properties of concentrated electrorheological fluids (ER fluids). According to this model, the particles of the suspension take their places at sites of a grid with specified type of symmetry and then an electric field is applied to the fluid. Taking into account hydrodynamic couple interaction of particles and forces of electrostatic interaction of particles polarized under the action of an external electric field and employing the mathematical apparatus of the microscopic theory of crystals, we construct the basic relationships for describing viscoelastic electrorheological properties of ER fluids.
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22

TAKIMOTO, Jun-ichi. "Cluster Formation in Electrorheological Fluids." Nihon Reoroji Gakkaishi(Journal of the Society of Rheology, Japan) 20, no. 2 (1992): 95–100. http://dx.doi.org/10.1678/rheology1973.20.2_95.

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23

Yu, K. W., Jones T. K. Wan, M. F. Law, and K. K. Leung. "Electrorheological Fluids of Coated Microspheres." International Journal of Modern Physics C 09, no. 08 (December 1998): 1447–57. http://dx.doi.org/10.1142/s012918319800131x.

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We study model electrorheological (ER) fluids which consist of three material components in an attempt to explain recent experimental results, in which the ER effects can be promoted by adding some water. At low water concentration, the droplets tend to aggregate on the surfaces of the dispersed particles, forming coated microspheres. The ER effects are analyzed via spectral representation, and the experimental conditions for optimal ER responses are obtained. At low frequencies, it is found that by tuning the thickness and dielectric properties of the coating materials, it is possible to enhance the effective dielectric constant, thereby increasing the applicability of the ER fluids.
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24

Wen, Weijia, Xianxiang Huang, and Ping Sheng. "Electrorheological fluids: structures and mechanisms." Soft Matter 4, no. 2 (2008): 200–210. http://dx.doi.org/10.1039/b710948m.

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25

Hill, John C., and Thomas H. Van Steenkiste. "Response times of electrorheological fluids." Journal of Applied Physics 70, no. 3 (August 1991): 1207–11. http://dx.doi.org/10.1063/1.349574.

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26

Bullough, W. A. "Solidifying fluids: the electrorheological dutch." IEE Review 38, no. 10 (1992): 348. http://dx.doi.org/10.1049/ir:19920149.

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27

TIAN, Yu. "Conductivity effect in electrorheological fluids." Science in China Series G 47, no. 7 (2004): 59. http://dx.doi.org/10.1360/03yw0313.

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28

Wen, Weijia, Ning Wang, Wing Yim Tam, and Ping Sheng. "Magnetic materials-based electrorheological fluids." Applied Physics Letters 71, no. 17 (October 27, 1997): 2529–31. http://dx.doi.org/10.1063/1.120108.

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29

Goodwin, James W., Gavin M. Markham, and Brian Vincent. "Studies on Model Electrorheological Fluids." Journal of Physical Chemistry B 101, no. 11 (March 1997): 1961–67. http://dx.doi.org/10.1021/jp962267j.

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30

KRZTON-MAZIOPA, ANNA, MONIKA CISZEWSKA, and JANUSZ PLOCHARSKI. "Electrorheological fluids materials, phenomena, applications." Polimery 48, no. 11/12 (November 2003): 743–52. http://dx.doi.org/10.14314/polimery.2003.743.

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31

Lemaire, E., G. Bossis, and Y. Grasselli. "Rheological behavior of electrorheological fluids." Langmuir 8, no. 12 (December 1992): 2957–61. http://dx.doi.org/10.1021/la00048a018.

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32

Kita, Yoshinori, Tatsuya Ohshima, Hideo Takase, Ichiroo Kondoo, and Shinpei Fujisawa. "Fundamental Study of Electrorheological Fluids." Transactions of the Japan Society of Mechanical Engineers Series B 59, no. 562 (1993): 1816–21. http://dx.doi.org/10.1299/kikaib.59.1816.

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33

Odenbach, Stefan, and Dmitry Borin. "Electrorheological fluids and magnetorheological suspensions." Journal of Physics: Condensed Matter 22, no. 32 (July 14, 2010): 320301. http://dx.doi.org/10.1088/0953-8984/22/32/320301.

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34

Wen, Weijia, Wing Yim Tam, and Ping Sheng. "Electrorheological fluids using bidispersed particles." Journal of Materials Research 13, no. 10 (October 1998): 2783–86. http://dx.doi.org/10.1557/jmr.1998.0381.

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We report very large enhancement of static yield stress for electrorheological fluids by adding ferroelectric nanoparticles of lead zirconate titanate (PZT) or lead titanate (PbTiO3) to ER fluids consisting of 50 μm glass spheres. It is found that the enhancement peaks at certain nanoparticle/microparticle ratios for fixed solid/liquid volume fractions. The results are explained by calculations using an effective medium approach, based on the physical picture that the nanoparticles modify the properties of the liquid and solid components.
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35

Bonnecaze, R. T., and J. F. Brady. "Yield stresses in electrorheological fluids." Journal of Rheology 36, no. 1 (January 1992): 73–115. http://dx.doi.org/10.1122/1.550343.

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36

Otsubo, Yasufumi, and Kazuya Edamura. "Creep behavior of electrorheological fluids." Journal of Rheology 38, no. 6 (November 1994): 1721–33. http://dx.doi.org/10.1122/1.550601.

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37

Zhao, He-ping, Zheng-you Liu, Jia-rui Shen, You-yan Liu, and P. M. Hui. "Mechanical Properties of Electrorheological Fluids." Chinese Physics Letters 15, no. 3 (March 1, 1998): 232–34. http://dx.doi.org/10.1088/0256-307x/15/3/030.

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38

TADA, Shigeru, Naoki KABEYA, Hideo YOSHIDA, and Ryozo ECHIGO. "Hydrodynamic Behavior of Electrorheological Fluids." Transactions of the Japan Society of Mechanical Engineers Series B 63, no. 613 (1997): 2985–92. http://dx.doi.org/10.1299/kikaib.63.2985.

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39

Tao, Rongjia. "International Conference on Electrorheological Fluids." Materials and Processing Report 7, no. 2 (February 1992): 5–7. http://dx.doi.org/10.1080/08871949.1992.11752486.

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40

Mokeev, A. A., E. V. Korobko, and L. G. Vedernikova. "Structural viscosity of electrorheological fluids." Journal of Non-Newtonian Fluid Mechanics 42, no. 1-2 (March 1992): 213–30. http://dx.doi.org/10.1016/0377-0257(92)80010-u.

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41

LU, KUNQUAN, RONG SHEN, XUEZHAO WANG, GANG SUN, WEIJIA WEN, and JIXING LIU. "POLAR MOLECULE TYPE ELECTRORHEOLOGICAL FLUIDS." International Journal of Modern Physics B 21, no. 28n29 (November 10, 2007): 4798–805. http://dx.doi.org/10.1142/s0217979207045682.

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The static and dynamic shear stress of newly developed electrorheological (ER) fluids can reach more than 100 kPa and over 60 kPa at 3 kV/mm, respectively. The high yield stress of those ER fluids and its near linear dependence on the electric field are different from the conventional ER fluids and can not be explained with traditional dielectric theory. Experiment demonstrates that the polar molecules adsorbed on the particles play crucial role in those ER fluids, which can be named as polar molecule type electrorheological (PM-ER) fluids. To explain PM-ER effect a model is proposed based on the interaction of polar molecule-charge in between the particles, where the local electric field is much higher than the external one and can cause the polar molecules aligning. The main effective factors for achieving high-performance PM-ER fluids are discussed.
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42

VERNESCU, BOGDAN. "MULTISCALE ANALYSIS OF ELECTRORHEOLOGICAL FLUIDS." International Journal of Modern Physics B 16, no. 17n18 (July 20, 2002): 2643–48. http://dx.doi.org/10.1142/s0217979202012785.

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We construct a microscale model for a rigid particle suspension in a viscous fluid that includes Maxwell electrostatic forces. Via homogenization techniques we characterize the properties the material exhibits at the macroscale. The change in the effective constitutive equations is due to the highly oscillating electrostatic forces. The material properties are determined by both hydrodynamic and electrostatic particle interactions.
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43

TIAN, Y., K. Q. ZHU, Y. G. MENG, and S. Z. WEN. "MECHANICAL PROPERTIES OF ELECTRORHEOLOGICAL FLUIDS." International Journal of Modern Physics B 19, no. 07n09 (April 10, 2005): 1311–17. http://dx.doi.org/10.1142/s0217979205030232.

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Electrorheological (ER) fluids are usually described by the continuous theory, Newtonian model and Bingham model. But during recent years, experiments showed that the mechanical properties of ER fluids were much complex than the traditional definitions. Many-body effect, modeling mechanical properties of ER fluids from particle chains or columns, and other problems are thought to be some key issues in ER effect and for ER mechanism.
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44

Tian, Yu, Shizhu Wen, and Yonggang Meng. "Conductivity effect in electrorheological fluids." Science in China Series G: Physics, Mechanics and Astronomy 47, S1 (January 2004): 59–64. http://dx.doi.org/10.1007/bf02690242.

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45

Halsey, Thomas C. "Electrorheological fluids — structure and dynamics." Advanced Materials 5, no. 10 (October 1993): 711–18. http://dx.doi.org/10.1002/adma.19930051004.

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46

Seo, Youngwook P., and Yongsok Seo. "Analysis of giant electrorheological fluids." Journal of Colloid and Interface Science 402 (July 2013): 90–93. http://dx.doi.org/10.1016/j.jcis.2013.03.046.

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47

Gast, Alice P., and Charles F. Zukoski. "Electrorheological fluids as colloidal suspensions." Advances in Colloid and Interface Science 30 (1989): 153–202. http://dx.doi.org/10.1016/0001-8686(89)80006-5.

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48

Toor, William R. "Structure Formation in Electrorheological Fluids." Journal of Colloid and Interface Science 156, no. 2 (March 1993): 335–49. http://dx.doi.org/10.1006/jcis.1993.1121.

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49

Olszak, Artur. "DURABILITY INVESTIGATION OF A DISC-TYPE CLUTCH WITH ELECTRORHEOLOGICAL FLUID." Tribologia 302, no. 4 (December 30, 2022): 39–50. http://dx.doi.org/10.5604/01.3001.0016.1608.

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The article concerns experimental research on the durability of a viscotic disc-type clutch with an electrorheological fluid. Viscotic clutches are currently used in the power transmission of multiple machines. The development of the viscotic clutch design is possible due to the use of working fluids with electrorheological properties, which renders it possible to control the drivetrain with the use of an electric current. The durability of the clutches with electrorheological fluid is important in determining the possibility of industrial use. On the basis of bench tests of a viscotic disc clutch, the article presents considerations regarding the operating factors of the clutch. These factors considerably impact the durability of the clutch and its components, including the working fluid.
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50

Choi, Young-Tai, Norman M. Wereley, and Young-Sik Jeon. "Semi-Active Isolators Using Electrorheological/Magnetorheological Fluids." Noise & Vibration Worldwide 33, no. 11 (December 2002): 16–19. http://dx.doi.org/10.1260/09574560260459657.

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ER (electrorheological)/MR (magnetorheological) fluids are colloidal suspensions that can control their rheological properties such as viscosity and yield stress in response to external signal. As a result, applications using ER/MR fluids have useful features such as fast response time and continuous control ability. These kinds of inherent advantages of ER/MR fluids trigger a lot of research activities on ER/MR applications including controllable vibration isolation systems, torque-transmission devices, and others. Among them, semi-active ER/MR fluid-based vibration isolators will be studied in this paper. The semi-active isolators can effectively isolate systems from various external disturbances with low power consumption, so that the system should not expose to significant dynamic stress and fatigue damage.
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