Elsevier

Physica B: Condensed Matter

Volume 371, Issue 1, 15 January 2006, Pages 145-148
Physica B: Condensed Matter

The influence of temperature and of a longitudinal magnetic field upon the electrical conductivity of magnetorheological suspensions

https://doi.org/10.1016/j.physb.2005.09.046Get rights and content

Abstract

The magnetorheological suspension (MRS) is based on mineral oil, stearic acid and iron micro-particles. The mean diameter of the iron micro-particles is 2.10 μm. MRS becomes conductive only in magnetic field, starting from intensities of 72 kA/m. By means of an experimental installation, described in this paper, the MRS function of temperature is measured (300 K⩽T⩽400 K) for intensities of the longitudinal magnetic field of 72, 112, 148 and 175 kA/m. From measurements of electrical resistance the electrical conductivity of MRS is determined, and the results obtained are discussed.

Introduction

The magnetorheological suspension (MRS) resembles electrorheological fluids (ERF). Both modify their rheological properties dramatically—the former, in magnetic field, the lather, in electric field.

In both cases, chains of micro-particles are formed [1], [2], [3] along the field lines. There results the growth, by some magnitude orders, of the value of the apparent viscosity. This phenomenon is used in various applications [4], [5], [6], [7].

Of great interest is the study of the electrical conductivity of the metal micro-particles systems dispersed in non-conductive matrices. Thus, Ref. [8] details a method of prediction of the actual electrical conductivity of such systems. On the other hand, Refs. [9], [10] detail methods for determining the electrical conductivity of MRS, while Ref. [11] describes a method for the simultaneous measuring of viscosity and electrical conductivity of ERF.

The phenomenon of electrical conductivity of MRS, in the presence of magnetic field of well-chosen intensities and directions, is used for the devising of sensors for detection of fringe fields in magnetic fields [12], as well as of warfare agents [13], etc.

In considering these applications, we set ourselves to show how the temperature and longitudinal magnetic field influence the electrical conductivity of MRS.

Section snippets

MRS

MRS is obtained by the thermal decomposition of Fe2(CO)9 in mineral oil mixed up with stearic acid. The experimental installation and the procedure are described in Ref. [14]. At temperatures of 423 K±10% for 150 s, the thermal decomposition of Fe2(CO)9 in the liquid matrix (mineral oil with stearic acid) occurs. On this occasion, a mixture of iron micro-particles and liquid matrix (Fig. 1a), called MRS, is formed. The mean diameter of the micro-particles is dm=2.10μm (Fig. 1b), at a standard

Experimental installation

The block scheme of the experimental installation, used for the study of the influence of magnetic field and temperature upon the electrical resistance is described in Fig. 3.

The installation comprises the electromagnet A, the measuring cell B, measurement apparatus and power sources. The core of the electromagnet is made of carbon steel. Its cross-section is a square with the side of 0.020 m. The poles of the electromagnet have their section equal to that of the core. Between the poles, the

Experimental results and discussion

The study of the influence of longitudinal magnetic field and temperature upon the electrical resistance of MRS is achieved by means of the experimental installation in Fig. 3. In the measuring cell, MRS has a volume concentration of the solid phase of Φ=0.30.

The temperature T of MRS is a mean value. It is obtained from the values of the temperatures measured by means of the thermometers 8 and 9 in Fig. 3. Regulation of the temperature of MRS is achieved by means of the power source S1.

The

Conclusions

  • The MRS formed of mineral oil with stearic acid and iron micro-particles (dm=2.1μm, φ=0.30) is electroconductive in a longitudinal magnetic field, starting with intensities of 72 kA/m.

  • In the interval of temperatures ranging between 300 and 400 K, the electrical conductivity of MRS increases by up to 96.8%, and it depends on the intensity of the magnetic field applied (Fig. 5).

  • The electrical conductivity of MRS at fixed T (Fig. 5) increases considerably with the intensity H of the longitudinal

Acknowledgements

I am thankful to Professors E. Papp and. C.T. Cheveresan of the West University of Timisoara for interesting discussions.

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