An actual instrument employs a 100μm-diameter 50mm-length tungsten wire. Constant tensioning is accomplished by a two-weights assembly at its bottom. The volumes of the two weights (the inner one is made from tungsten and the outer one from stainless steel), are chosen so that the net effect of changing the density of the surrounding liquid results in a negligible effect upon the frequency of oscillation. This arrangement also ensures that wire oscillations occur in only one plane of oscillation (in the case of gases, the non-boyancy mechanism is replaced by a small weight). Two permanent samarium-cobalt magnets, placed around the wire, are employed for the electromagnetic initiation of the oscillations as well as for their detection. Following initiation of the motion, the signal induced in the vibrating wire is observed with a bridge in which the wire forms one arm. The out-of-balance signal, amplified by 30,000 times, is then observed with an A/D converter coupled to a microcomputer at a rate of 50 kHz with a resolution of 12 bits. The logarithmic decrement and the frequency of oscillation, are then obtained from the recorded data with the aid of a non-linear least squares fitting procedure, and from them the viscosity is obtained by a full theoretical analysis. Work currently is concentrated in the measurement of the viscosity of high-viscosity fluids over extended temperatures and pressures. From left to right: a) Vibrating wire for liquids b) Vibrating wire for gases. |
Both electrically conducting and non-conducting fluids have been studied