Abstract

SECOND approximation equations are derived from a simple quasilinear hypothetical model of a viscous fluid. The model is obtained by introducing supplementary non-linear terms into the expressions for the deformation rate tensor components. The defining equation retains its classical linear tensorial form. The model is suggested by the analogy between the vortex equation in hydrodynamics and the equation of induction in magnetohydrodynamics. A method for determining the physical parameter in the proposed equations experimentally is outlined. As an example, we consider the behaviour of perturbations in the flow of a viscous incompressible fluid possessing “transverse fluidity”.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.