Titlebook: Vascularization for Tissue Engineering and Regenerative Medicine; Wolfgang Holnthoner,Andrea Banfi,Heinz Redl Reference work 2021 Springer

Indurate

Victor W. M. van Hinsberghstructure at length scales in the inertial subrange. First, we investigate the probability distribution functions (pdf’s) of the Eulerian and Lagrangian time-derivative fields and fourthorder velocity moments, to study the intermittent and non-Gaussian nature of turbulence. Next, in order to get som

exacerbate

Laxminarayanan Krishnan,Steven A. LaBelle,Marissa A. Ruehle,Jeffrey A. Weiss,James B. Hoying,Robert (v) Should convective fluid-acceleration terms be taken into account in the analysis of the dynamics of strings or beams undergoing extrusion or deployment in dense fluid, and similarly for traveling web? (vi) Taking annular fluidelastic systems as an example, is the precise specification of boundar

surmount

olynomial closure method in analyzing the probabilistic solutions of the beams discretized by finite difference scheme and excited by Gaussian white noise. The techniques of using the state-space-split procedure for dimension reduction of the beam systems are discussed through the given beam systems

eustachian-tube

Veronica Sacchi,Rainer Mittermayr,Martin Ehrbarled the “mixed potential function” and demonstrated a procedure to construct Lyapunov-type functions from the potential function to prove stability under certain conditions. However, this approach and successive ones such as the EL(Euler-Lagrange) formalism of an electric circuit by Meisel (1966) ar

FLUSH

Henna Korpela,Jaakko Lampela,Jussi Nurro,Juho Pajula,Seppo Yl?-Herttuala at the front face of the wave crest and shallower slopes at the low pressure region at lee side of the crest, as Bai et al. describe (1996). However two new issues are confronted in our 2D simulation. First, the shape and length of the upper and lower waves are different. Second, the displaced 2D c

acheon

Hermann Agison characteristics are classified into categories defined by the material and pre-stress parameters. For wavelengths large as compared to the interlayer thickness, the interfacial wave speed is derived in explicit form yielding parameter conditions for the non-existence of interfacial waves. The bif

FAWN

Toini Pemmari,Tiia Koho,Tero A. H. J?rvinenproduced by the effective medium is due to scattering noise arising from the layering microstructure. We model this fine scale layering as a rapidly varying stochastic process. This scattering noise component of MT data is fundamental since it arises from the very structure of the medium being probe