1 / 1

Introduction

v. X =(t , R ). x =(t, r ). Material manifold. y. Z. x.

micah
Télécharger la présentation

Introduction

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. v X=(t,R) x=(t,r) Material manifold y Z x Objectivity and continuum mechanicsCs. Asszonyi1, T. Fülöp1 and P. Ván1,21MONTAVID Thermodynamic Research Group, Budapest, Hungary; 2Dept. of Theoretical Physics, KFKI, RMKI, Budapest, Hungary,asszonyi@gmail.com, tamas.fulop@gmail.com, vpet@rmki.kfki.hu Introduction Principle: Material is independent of the observer (reference frame) → material frame indifference, → objective time derivatives. Consequences: deformation concept, material manifold concept, restricted constitutive relations, rheology. Problems: too restrictive, paradoxes, compatibility with kinetic theory. Suggestion: observer independent treatment (4malism). velocity deformation gradient Derivative of a vector: Problem with the formulation of Noll Rigid rotating frames: →inertial forces brought in Noll (1958) upper convected Four-transformations, four-Jacobian: Tensorial property – form of the derivative. Constitutive theory – nonequilibrium thermo [3] where  four-velocity is an objective vector. force flux objective time derivative Simple shear with a single internal variable: Non-relativistic spacetime [1] spacetime ≠space + time viscosity and viscometric functions Absolute time. Conclusions Space-time M: four dimensional affine space (over the vector spaceM), Time I: is a one-dimensional affine space, Time evaluation : MI: is an affine surjection. Distance: Euclidean structure on E=Ker() Objectivity is best formulated objectively, without introducing reference frames. Four-quantities and a non-relativistic 4malism is elaborated. Kinematical consequence(Fülöp in GS-CM10): no reference configuration for fluidsdistinguished deformation and strain for solids Constitutive theory:frame independent Liu procedure (spacetime-nonlocal)[4] rheological models (preliminary) Open questions: Relativistic correspondence Mass-momentum or energy-momentum?  TIME CANNOT BE NEGLECTED! Consequences: 4-quantities: Restrictions: vectors and covectors Four manifolds - objective derivatives [2] References [1] T. Matolcsi. Spacetime Without Reference Frames. Akadémiai Kiadó(Publishing House of theHungarian Academy of Sciences), Budapest, 1993. [2] T. Matolcsi and P. Ván. Absolute time derivatives. Journal of Mathematical Physics,2007,48:053507–19, (math-ph/0608065). [3] P. Ván. Objective time derivatives in non-equilibrium thermodynamics, Proceedings of the Estonian Academy of Sciences,2008, 57/3, 127–131. [4] P. Ván. Internal energy in relativistic dissipative fluids, Journal of Mechanics and Materials and Structures, 2008, 3/6, 1161-1169. Kinematics: deformation gradient – existence gradient Id. 804

More Related