inteq.s23.j
... curvature and that quadratic in the Ricci tensor.) It was a quite different route that led us to the specific form of Lagrangian that leads to our vacuum equation. More that 10 years ago I sought to find a natural equation suitable for what I thought of as a Yukawa-like gravitational field where th ...
... curvature and that quadratic in the Ricci tensor.) It was a quite different route that led us to the specific form of Lagrangian that leads to our vacuum equation. More that 10 years ago I sought to find a natural equation suitable for what I thought of as a Yukawa-like gravitational field where th ...
Lecture 39
... streamlines are straight (not curved, which leads to pressure changes) at point 2. Dynamic pressure V2/2 = difference between stagnation and static pressure = Pstag – P. This is the “extra” pressure that is felt at the stagnation point at the nose of a probe in the flow. ...
... streamlines are straight (not curved, which leads to pressure changes) at point 2. Dynamic pressure V2/2 = difference between stagnation and static pressure = Pstag – P. This is the “extra” pressure that is felt at the stagnation point at the nose of a probe in the flow. ...
Trends in Applications of Pure Mathematics to Mechanics
... two-component model in which a mobile component co-exists with the immobile one. In particular, a gas diffusing into a solid body may be described by such a model (also diffusion in stable solutions.) A crystal lattice of the immobile component can be assumed as a reference system for the diffusion ...
... two-component model in which a mobile component co-exists with the immobile one. In particular, a gas diffusing into a solid body may be described by such a model (also diffusion in stable solutions.) A crystal lattice of the immobile component can be assumed as a reference system for the diffusion ...
