Viscosity of Fluids at High Pressures. Rotating Cylinder Viscometer and Viscosity ofn-Pentane

1959 ◽  
Vol 31 (8) ◽  
pp. 1422-1428 ◽  
Author(s):  
H. H. Reamer ◽  
G. Cokelet ◽  
B. H. Sage
Author(s):  
J. Wonham

This paper records some of the recent experimental methods used to determine the viscosity of water. In drawing attention to the many techniques used (most relying upon calibration of the instrument by a fluid of known viscosity), the conclusion may be drawn that an absolute instrument is required which will produce results over a wide range of temperature and pressure. It has long been known that the rotating cylinder viscometer is capable of a high degree of accuracy, but technical considerations have, in the past, restrained most workers from pursuing this method at high pressures. Progress in the development of the rotating cylinder instrument for these conditions is described and specific problems encountered with this method are discussed. This work is a continuation of the design studies of Kjelland-Fosterud (1)† and Whitelaw (2) who both gave considerable thought to the problems associated with this type of instrument. The first instrument to be tested by the author was based on Whitelaw's design but it was found that certain aspects of this instrument required major alteration. A new instrument was set up and has been found suitable for accurate viscosity determination.


2019 ◽  
Vol 285 ◽  
pp. 391-397
Author(s):  
Kang Lu ◽  
Shu Sen Wu ◽  
Shu Lin Lü ◽  
Chong Lin

The apparent viscosity and rheological behavior of nanoSiCP/Al-5Cu composites were studied by using a high temperature coaxial rotating cylinder viscometer. The results show that mass fraction of nanoSiCP is an important factor for apparent viscosity of the nanoSiCP/Al-5Cu composites, and there is a great enhancement of apparent viscosity of the slurry with the increase of nanoSiCp content. It can attribute to the viscous force between nanoSiCp and matrix alloy melt above the liquidus. The increased amplitude of apparent viscosity in semi-solid state is far less than those in liquid state with the increase of mass fraction of nanoSiCp. The apparent viscosities of the composites reinforced with 0.5%, 1%, 1.5% and 2% nanoSiCp at 700°C were 24.78%, 95.25%, 160.29% and 228.62% higher than that of Al-5Cu alloy, respectively. Besides, the rheological model of nanoSiCP/Al-5Cu composites was established based on the fitting curve, which can precisely describe the relationship between the apparent viscosity of nanocomposites slurry and nanoSiCp mass fraction.


Author(s):  
A. C. Hollis-Hallett

ABSTRACTLiquid helium II was contained in the annular space between two co-axial cylinders, the inner of which was suspended by a torsion fibre while the outer was rotated at constant speeds. The torque upon the inner cylinder produced by the rotating fluid was measured for various steady velocities between 0·1 and 3 cm.sec.1, and was not found to be directly proportional to the velocity of rotation at any temperature between the lambda-point and 1·15° K. This result suggests that there must be some new type of non-linear frictional force acting in the liquid, possibly in addition to the Gorter-Mellink force of mutual friction.Extrapolation of the experimental results to zero velocity gives values of the coefficient of viscosity of the normal component which agree with the oscillating disk values between the lambda-point and about 1·6° K. At lower temperatures, the present results are significantly lower, suggesting, perhaps, that the values of the normal component density used in the analysis of the oscillating disk results were too low.


1937 ◽  
Vol 10 (2) ◽  
pp. 214-223 ◽  
Author(s):  
M. Mooney

Abstract The scientific measurement of the rheological properties of raw or unvulcanized rubber is a problem that has required new methods in rheological laboratory technic. Hot, moderately milled, or masticated raw rubber exhibits to a very marked degree each of the three properties of elasticity, plasticity, and thixotropy. It is highly elastic (not perfectly elastic), in that if deformed and released quickly it can take a large deformation and still return to its initial form. It is highly plastic, in that under proper conditions it can be deformed to any given extent permanently and without rupture. It is highly thixotropic, in that its viscosity or stiffness is very considerably decreased by brief mechanical working or mastication, and the lost viscosity is largely regained again when the mastication ceases. Obviously such a wide and varied range in rheological properties cannot be measured in either of the two types of rheological instruments, the compression and the extrusion plastometers, commonly used for raw rubber. There is no way in either instrument to determine or correct for thixotropy; and the viscosity can only be calculated with considerable uncertainty and difficulty. For example, thixotropy has not been considered in either of the already very complicated analyses of parallel plate plastometry by Peek and by Scott. Peek and Erickson have attempted to analyze the effects of thixotropy and elasticity in capillary tube viscometry without obtaining a complete or generally useful solution. However useful the compression and extrusion plastometers may be in factory control work, they are inadequate as scientific research instruments. The rotating cylinder viscometer seems to be the only type of instrument that meets the requirements of the problem considered. It allows an unlimited deformation of the test material, the previous deformation history can be controlled at will, and the subsequent elastic recovery can be measured if desired. There are two serious deficiencies of the conventional cylindrical viscometer, as applied to raw rubber, in that, first, the rubber, being semi-solid, would be likely to slip on the moving surfaces; secondly, if the rubber did not slip but sheared as it should, it would soon roll and climb out of the viscometer against the force of gravity. These deficiencies can be corrected, first, by fluting or otherwise roughening the cylindrical surfaces so that they grip the rubber and prevent slipping; secondly, by adding means for compressing and holding the rubber in place. The combined use of these two devices in a factory control instrument, the rotating disc plastometer, has already been described; and a rotating cylinder viscometer with similar features was referred to in the same article. The cylindrical viscometer there referred to was used in the experimental researches described below. Since this instrument is so different in several respects from the conventional cylindrical viscometers and, furthermore, is designed to facilitate the measurement of thixotropy and elastic recovery as well as viscosity, it seems appropriate to give it a new name and call it a rubber rheometer.


1955 ◽  
Vol 33 (8) ◽  
pp. 420-435 ◽  
Author(s):  
W. J. Heikkila ◽  
A. C. Hollis Hallett

It has been found possible to use the rotating cylinder viscometer to measure the viscosity of liquid helium II between 1.13°K. and 2.18°K. provided that the fluid velocities do not exceed about 0.08 cm. sec.−1. The results, which are calculated directly from experimental observations and do not require any knowledge of the density of the normal component, can be made to fit the Landau and Khalatnikov theory for the temperatures below 1.8°K. for which the theory is applicable. The results are somewhat higher than the oscillating disk results above 1.4°K.


1969 ◽  
Vol 40 (8) ◽  
pp. 992-997 ◽  
Author(s):  
H. A. Snyder

1973 ◽  
Vol 81 (934) ◽  
pp. 221-227
Author(s):  
Hironobu SAKATA ◽  
Satoshi NOGUCHI ◽  
Michihiko UEMURA

1962 ◽  
Vol 48 (6) ◽  
pp. 905-911 ◽  
Author(s):  
B. H. Zimm ◽  
D. M. Crothers

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