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The aim of this experiment is to measure how the viscosity of motor oil changes with temperature.
In contrast, in the presence of viscosity, there is no such equivalence.
Uncertainties in the magnetized plasma viscosity remain as an obstacle to unambiguous tests of the results in the case of real plasmas.
Flow approaching the sphere from upstream accelerates, forms a vortex jump beyond the equator and then decelerates slowly downstream under the action of viscosity.
There is a large increase in potential vorticity generated by the artificial viscosity, which again results in layers of enhanced static stability near the boundaries.
The dynamical system is determined by travelling-wave solutions of the associated viscosity equation.
For instance, the isotropic eddy viscosity hypothesis does not predict the observed fact that the shear stress and mean velocity gradient vectors have different directions.
The viscosity dissipates the fluctuation energy with conservation of helicity.
An alternative way of deriving a cutoff for (1.5) at high frequencies is to retain the effect of viscosity.
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