1976
DOI: 10.1007/bf01517228
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Der Einflu� von Druck und Temperatur auf die effektive Viskosit�t in geschmierten kontra-formen Kontakten

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Cited by 5 publications
(2 citation statements)
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“…Instead of a phenomenological SLS with the well known bulk modulus of the kind: (5) (N gives the number of particles and c defines a parameter connected with the volume of an individual particle) and a subsequent Young's modulus time dependency like we have a resulting phenomenological Young's modulus structure of the form: (6) With a known principle structure for the temperature distribution function deduced from the shear stress distribution (adiabatic approach) such an approach seems to be manageable by the means of iterations. With a typical dependency for the temperature dependent relaxation time like [37,38]: (7) (with a constant W A and the T = T 0 -viscosity η 0 and the Boltzmann-constant k B ) one can evaluate the mechanical contact situations applying the techniques elaborated in [2] (theory part II) under the assumption of completely adiabatic temperature fields resulting from shear and completely following the second stress invariant distribution. Please note, the positive sign in the exponential function for the relaxation time assuring decreasing viscosity η with increasing temperature.…”
Section: First Principle Based Interatomic Potential Description Of Mmentioning
confidence: 99%
“…Instead of a phenomenological SLS with the well known bulk modulus of the kind: (5) (N gives the number of particles and c defines a parameter connected with the volume of an individual particle) and a subsequent Young's modulus time dependency like we have a resulting phenomenological Young's modulus structure of the form: (6) With a known principle structure for the temperature distribution function deduced from the shear stress distribution (adiabatic approach) such an approach seems to be manageable by the means of iterations. With a typical dependency for the temperature dependent relaxation time like [37,38]: (7) (with a constant W A and the T = T 0 -viscosity η 0 and the Boltzmann-constant k B ) one can evaluate the mechanical contact situations applying the techniques elaborated in [2] (theory part II) under the assumption of completely adiabatic temperature fields resulting from shear and completely following the second stress invariant distribution. Please note, the positive sign in the exponential function for the relaxation time assuring decreasing viscosity η with increasing temperature.…”
Section: First Principle Based Interatomic Potential Description Of Mmentioning
confidence: 99%
“…When smooth walled capillary or rotational rheometers are applied, this effect causes that the measured viscosities do not correspond to that of bulk material (too low viscosities are measured). The postulation by Jastrzebski [1] that the slip velocity mainly depends on the wall shear stress is generally accepted, although Ehlert et al state that the wall normal pressure has an additional influence [2].…”
Section: Introductionmentioning
confidence: 99%