By T.I. Zohdi
ISBN-10: 0898716276
ISBN-13: 9780898716276
The particularly fresh bring up in computational energy on hand for mathematical modeling and simulation increases the chance that sleek numerical tools can play an important function within the research of complicated particulate flows. This introductory monograph specializes in easy types and bodily established computational answer suggestions for the direct and swift simulation of flowing particulate media. Its emphasis is totally on fluidized dry particulate flows during which there's no major interstitial fluid, even if totally coupled fluid-particle platforms are mentioned to boot. An creation to uncomplicated computational tools for ascertaining optical responses of particulate structures is also integrated. The winning research of a variety of purposes calls for the simulation of flowing particulate media that concurrently consists of near-field interplay and get in touch with among debris in a thermally delicate atmosphere. those structures clearly take place in astrophysics and geophysics; powder processing pharmaceutical industries; bio-, micro- and nanotechnologies; and functions bobbing up from the research of spray procedures related to aerosols, sputtering, and epitaxy. viewers An creation to Modeling and Simulation of Particulate Flows is written for computational scientists, numerical analysts, and utilized mathematicians and should be of curiosity to civil and mechanical engineers and fabrics scientists. it's also compatible for first-year graduate scholars within the technologies, engineering, and utilized arithmetic who've an curiosity within the computational research of advanced particulate flows. Contents record of Figures; Preface; bankruptcy 1: basics; bankruptcy 2: Modeling of particulate flows; bankruptcy three: Iterative answer schemes; bankruptcy four: consultant numerical simulations; bankruptcy five: Inverse problems/parameter identity; bankruptcy 6: Extensions to swarm-like structures; bankruptcy 7: complicated particulate move types; bankruptcy eight: Coupled particle/fluid interplay; bankruptcy nine: basic optical scattering equipment in particulate media; bankruptcy 10: final feedback; Appendix A. simple (continuum) fluid mechanics; Appendix B. Scattering; Bibliography; Index
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For more general analyses of the validity of mechanical models involving friction, see, for example, Oden and Pires [154], Martins and Oden [147], Kikuchi and Oden [123], Klarbring [125], Tuzun and Walton [196], or Cho and Barber [42]. Remark. 2 Velocity-dependent coefficients of restitution It is important to realize that, in reality, the phenomenological parameter e depends on the severity of the impact velocity. For extensive experimental data, see Goldsmith [79], or see Johnson [111] for a more detailed analytical treatment.
The total kinetic energy in the system per unit mass. 25 (Zohdi [212]). 3). 2, as the near-field strength is increased, the component of the kinetic energy corresponding to the relative motion does not decay and actually becomes dominant with time. Essentially, the near-field interaction becomes strong enough that the flowing system experiences a transition to a vibrating ensemble. 8) the simulations took under a minute on a single laptop. 2. 9) d being a constant of damping and f (t) an external forcing term.
The explicit method has the major drawback that the step size t may have to be very small to achieve acceptable numerical results. Therefore, an explicit simulation will usually require many more time steps than an implicit simulation. 21 ✐ ✐ ✐ ✐ ✐ ✐ ✐ 22 05 book 2007/5/15 page 22 ✐ Chapter 3. 2 An example of stability limitations Generally speaking, a key difference between the explicit and implicit schemes is their stability properties. By stability, we mean that errors made at one stage of the calculations do not cause increasingly larger errors as the computations are continued.
An introduction to modeling and simulation of particulate flows by T.I. Zohdi
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