Field-induced gelation, yield stress, and fragility of an electro-rheological suspension

Abstract Electro-rheological suspensions (ERS) are known to undergo liquid-to-solid transition under the application of an electric field. Long-range interaction between neighboring particles results in sample-spanning particulate structures which behave as soft solids. Here, we studied the rheological expression of this field-induced transition which has many similarities with chemical gelation. This similarity shows in mechanical spectroscopy on a suspension of monodisperse silica in PDMS as model ERS. Upon application of the electric field, dynamic moduli G′, G′′ grow by orders of magnitude and evolve in a pattern which is otherwise typical for gelation of network polymers (random chemical or physical gelation). At the gel point, the slow dynamics is governed by power-law relaxation behavior (frequency-independent tan δ). A low field strength is sufficient to reach the gel point and, correspondingly, the percolating particle structure at the gel point is still very fragile. It can be broken by the imposition of low stress. For inducing a finite yield stress, the field strength needs to be increased further until the long-range electrostatic interaction generates string-like particle alignments which become clearly visible under the optical microscope. The onset of fragile connectivity was defined experimentally by the tan δ method. The ERS was probed dynamically at low frequencies where the transition is most pronounced, and also in steady shear where the rate of structure formation equals the rate of internal breaking.

[1]  Charles F. Zukoski,et al.  Material Properties and the Electrorheological Response , 1993 .

[2]  Martin,et al.  Rheology of electrorheological fluids. , 1992, Physical review letters.

[3]  X. Tang,et al.  On the conductivity model for the electrorheological effect , 1995 .

[4]  G. McKinley,et al.  Structural limitation to the material strength of electrorheological fluids , 1997 .

[5]  D. V. Boger,et al.  Direct Yield Stress Measurement with the Vane Method , 1985 .

[6]  L. C. Davis Polarization forces and conductivity effects in electrorheological fluids , 1992 .

[7]  J. W. Goodwin,et al.  Effects of electric fields on the rheology of non-aqueous concentrated suspensions , 1989 .

[8]  Thomas C. Halsey,et al.  Electrorheology of a model colloidal fluid , 1994 .

[9]  F. E. Filisko,et al.  High frequency dynamic mechanical study of an aluminosilicate electrorheological material , 1991 .

[10]  H. Henning Winter,et al.  Rheology of Polymers Near Liquid-Solid Transitions , 1997 .

[11]  H. Winter,et al.  Linear Viscoelasticity at the Gel Point of a Crosslinking PDMS with Imbalanced Stoichiometry , 1987 .

[12]  Daniel J. Klingenberg,et al.  Simulation of the dynamic oscillatory response of electrorheological suspensions: Demonstration of a relaxation mechanism , 1993 .

[13]  M. Shaw,et al.  Viscoelastic response of electrorheological fluids. II. Field strength and strain dependence , 1992 .

[14]  A. D. Shine,et al.  Steady-State Electrorheology of Nematic Poly(n-hexyl isocyanate) Solutions , 2000 .

[15]  Howard A. Barnes,et al.  The yield stress—a review or 'panta roi'—everything flows? , 1999 .

[16]  H. Henning Winter,et al.  Analysis of Linear Viscoelasticity of a Crosslinking Polymer at the Gel Point , 1986 .

[17]  Tom C. B. McLeish,et al.  Viscoelastic response of electrorheological fluids. I. Frequency dependence , 1991 .

[18]  Daniel J. Klingenberg,et al.  Electrorheology : mechanisms and models , 1996 .

[19]  O. Park,et al.  Effects of Conductivity and Dielectric Behaviors on the Electrorheological Response of a Semiconductive Poly(p-phenylene) Suspension , 1998 .

[20]  G. V. Vinogradov,et al.  Electric fields in the rheology of disperse systems , 1984 .

[21]  James W. Goodwin,et al.  Studies on Model Electrorheological Fluids , 1997 .

[22]  H. Winter,et al.  Relaxation patterns of endlinking polydimethylsiloxane near the gel point , 1998 .

[23]  S. Safran,et al.  Defect-induced phase separation in dipolar fluids. , 2000, Science.

[24]  Norman M. Wereley,et al.  Analysis of electro- and magneto-rheological flow mode dampers using Herschel-Bulkley model , 2000, Smart Structures.

[25]  W. M. Winslow Induced Fibration of Suspensions , 1949 .

[26]  Roger T. Bonnecaze,et al.  Yield stresses in electrorheological fluids , 1992 .

[27]  Yasufumi Otsubo,et al.  Electrorheological properties of silica suspensions , 1992 .

[28]  James E. Martin,et al.  STRUCTURE AND DYNAMICS OF ELECTRORHEOLOGICAL FLUIDS , 1998 .

[29]  Daniel J. Klingenberg,et al.  Studies on the steady-shear behavior of electrorheological suspensions , 1990 .

[30]  T C Halsey Electrorheological fluids. , 1992, Science.

[31]  L. E. Scriven,et al.  Some Rheological Measurements on Magnetic Iron Oxide Suspensions in Silicone Oil , 1986 .

[32]  Lincoln Paterson,et al.  Gel transition studies on nonideal polymer networks using small amplitude oscillatory rheometry , 1998 .

[33]  M. Doi,et al.  The role of water capillary forces in electro-rheological fluids , 1993 .