The influence of temperature and of a longitudinal magnetic field upon the electrical conductivity of magnetorheological suspensions
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 (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 .
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
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The MRS formed of mineral oil with stearic acid and iron micro-particles (, ) is electroconductive in a longitudinal magnetic field, starting with intensities of 72 kA/m.
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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).
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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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