The Performance of an Electrorheological Fluid in Dynamic Squeeze
Flow: The Influence of Solid Phase Size
Ali K. El Wahed,* John L. Sproston,*
,1
and Roger Stanway†
*Department of Engineering, University of Liverpool, Liverpool L69 3GH, United Kingdom; and †Department of Mechanical Engineering,
University of Sheffield, Mappin Street, Sheffield S1 3JD, United Kingdom
Received May 13, 1998; accepted November 9, 1998
This paper is concerned with an experimental investigation of a
comparison of the rheological performance of an ER fluid, con-
sisting of a carrierwith a range of solid phase sizes, in oscillatory
squeeze-flow under DC conditions. The fluid is sandwiched be-
tween two parallel plane electrodes, the upper one stationary and
the lower one oscillating normal to its plane. It is seen that the
dynamic performance of the fluid, in terms of the capacity for the
transmission of imposed forces across the fluid, is highly depen-
dent on the size of the dispersed solid phase and has an optimum
value which is dependent on the mean value of the interelectrode
gap. In addition the paper includes some measurements of the
current through the fluid which may help to shed some further
light on the mechanism of the ER effect. Finally the implications
of the results to vibration control are discussed. © 1999 Academic Press
Key Words: ER fluids; suspensions; vibration control.
INTRODUCTION
The majority of vibration damping devices utilizing an elec-
trorheological (ER) fluid has employed the fluid in simple
shear mode where the fluid is deformed in a direction orthog-
onal to the arrays of particulate chains and where the gap
between the shearing electrodes remains constant. Stanway et
al. (1) and Stevens et al. (2) have already demonstrated the
feasibility of constructing a simple vibration damper using this
mode of operation. An alternative arrangement, called squeeze
mode, in which the fluid is subjected to compressive and
tensile stresses in a direction parallel to the chains (resulting in
a variable fluid layer thickness) has been identified and inves-
tigated by Stanway et al. (3) and Monkman (4) where it was
shown that the yield stress in this mode is greater than that
available in shear typically by a factor of ten. These results are
in accordance with those, for example, of Lukharinen and
Kaski (5) and Gong and Lim (6). Papers by El Wahed et al. (7),
Stanway and Sproston (8), and Stanway et al. (9) provide
substantial overviews of the classification of the modes of
operation of ER fluids and of their potential applications in
vibration control, respectively.
In parallel with device investigations, during the last decade
numerous studies have been carried out aimed at improving the
mechanical and electrical characteristics of ER fluids, but the
influence of particulate size on their rheological performance
remains unclear. Jordan and Shaw (10) referred to particulate
sizes in the range 0.04 to 50 m while Block (11) mentioned
the range 5 to 50 m and Conrad (12) 0.1 to 100 m. Recently
the influence of the shape of the particulates was assessed by
Yatsuzuka et al. (13) and Asano et al. (14) and also their
electrical properties by Barry et al. (15) on the magnitude of
the ER effect. However the limits beyond which no ER activity
will exist or the optimum size of the particulate for a particular
application have not been clearly defined. It is this which
prompted this particular investigation. This paper is concerned
with the assessment of an ER fluid in dynamic squeeze-flow
under DC excitation and the influence of the solid phase size on
its rheological performance. The relevance of this work in the
application to vibration control in a short-stroke damper is
discussed.
EXPERIMENTAL ARRANGEMENT
Experimental Facility
The experimental rig shown in Fig. 1 consisted of a Ling
Dynamic Systems electromagnetic shaker (Model No. 406)
which was capable of providing vertical oscillatory motion
with a minimum and maximum amplitude of 0.1 mm and 7
mm, respectively, over a frequency in the range DC to 9 kHz.
The shaker head was attached rigidly to a Kistler (Model No.
9311A) piezoelectric force link and an earthed brass electrode
having a recessed cylindrical cavity of diameter 95 mm which
provided the reservoir for the ER fluid. The high voltage upper
electrode was a circular brass disk of diameter 56 mm, its
circumferential edge and rear face surrounded and supported
by a PTFE collar. This was rigidly attached to a second
identical force link and positioning assembly to the supporting
frame.
The instantaneous displacement of the lower electrode was
determined using an RDP (type GTX 2500) LVDT and the
acceleration using an Endevco (type 7254-100) accelerometer
1
To whom correspondence should be addressed.
Journal of Colloid and Interface Science 211, 264 –280 (1999)
Article ID jcis.1998.5972, available online at http://www.idealibrary.com on
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0021-9797/99 $30.00
Copyright © 1999 by Academic Press
All rights of reproduction in any form reserved.