𝔖 Bobbio Scriptorium
✦   LIBER   ✦

A spectral method for the numerical solutions of a kinetic equation describing the dispersion of small particles in a turbulent flow

✍ Scribed by Tao Tang; S McKee; M.W Reeks


Publisher
Elsevier Science
Year
1992
Tongue
English
Weight
147 KB
Volume
101
Category
Article
ISSN
0021-9991

No coin nor oath required. For personal study only.


πŸ“œ SIMILAR VOLUMES


A Spectral Multidomain Method for the Nu
✍ A. Pinelli; A. Vacca; A. Quarteroni πŸ“‚ Article πŸ“… 1997 πŸ› Elsevier Science 🌐 English βš– 579 KB

come several intrinsic limitations of spectral methods, allowing for the use of the latter in a wider context . The primitive variable formulation of the unsteady incompressible Navier-Stokes equations in three space dimensions is discretized The most obvious application of spectral multidomain wit

A Numerical Method for the Computation o
✍ K. Domelevo; L. Sainsaulieu πŸ“‚ Article πŸ“… 1997 πŸ› Elsevier Science 🌐 English βš– 975 KB

the exchanges of mass, momentum, and of course energy between the two phases. However, for the sake of simplic- The paper is concerned with the construction of a numerical method for the computation of the dispersion of a cloud of liquid ity, we do not introduce combustion models in this work dropl

Analytical solutions of the advection-di
✍ Erick Carlier πŸ“‚ Article πŸ“… 2008 πŸ› John Wiley and Sons 🌐 English βš– 163 KB

## Abstract An analytical transport‐model was developed to simulate the propagation of a contaminant in one‐ and two‐dimensional transient flow in groundwater. It is proved that the distribution of concentration at a given time and for a given discharge is identical to that obtained for a different

A numerical method for the solution of t
✍ Mailand R. Strunk; Frank F. Tao πŸ“‚ Article πŸ“… 1964 πŸ› American Institute of Chemical Engineers 🌐 English βš– 509 KB

T = pressure, atm. u = collision diameter, A (a = azimuthal angle between the axes of the two di-(p(r) = Stockmayer potential, Equation (6) f i ( l J ) \* [ T ~] = reduced collision integral for the Lennardfi(2,2)\* [ T N ] = reduced collision integral for the Lennard-O ( l J ) \* [ TN, S o ] = redu