1966
DOI: 10.1016/s0006-3495(66)86671-7
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Wave Propagation through a Viscous Incompressible Fluid Contained in an Initially Stressed Elastic Tube

Abstract: To have a better understanding of the flow of blood in arteries a theoretical analysis of the pressure wave propagation through a viscous incompressible fluid contained in an initially stressed tube is considered. The fluid is assumed to be Newtonian. The tube is taken to be elastic and isotropic. The analysis is restricted to tubes with thin walls and to waves whose wavelengths are very large compared with the radius of the tube. It is further assumed that the amplitude of the pressure disturbance is sufficie… Show more

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Cited by 179 publications
(101 citation statements)
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“…Most of the works on wave propagation in compliant tubes have considered small amplitude waves ignoring the nonlinear effects and focused on the dispersive character of waves (see Atabek and Lew [2], Rachev [13], and Demiray [5]). However, when the nonlinear terms arising from the constitutive equations and kinematical relations are introduced, one has to consider either finite amplitude or small-but-finite amplitude waves, depending on the order of nonlinearity.…”
Section: Introductionmentioning
confidence: 99%
“…Most of the works on wave propagation in compliant tubes have considered small amplitude waves ignoring the nonlinear effects and focused on the dispersive character of waves (see Atabek and Lew [2], Rachev [13], and Demiray [5]). However, when the nonlinear terms arising from the constitutive equations and kinematical relations are introduced, one has to consider either finite amplitude or small-but-finite amplitude waves, depending on the order of nonlinearity.…”
Section: Introductionmentioning
confidence: 99%
“…The model we use for the elastic response of the wall was originally derived by Atabek & Lew (1966) and used by Halpern & Grotberg (1992) in modelling airway closure. The tube wall is characterized by a constant longitudinal tension T l and a circumferential tension that is constituted in terms of its Young's modulus, E, thickness, d, and Poisson's ratio, ν.…”
Section: Introductionmentioning
confidence: 99%
“…Witzig (1914) was the first to show the effects of fluid viscosity on propagation characteristics, impedance and velocity profiles. Significant developments of the theory took place in the 1950s and 1960s: Womersley (1955Womersley ( , 1957, Atabek & Lew (1961) and Atabek (1968), among † Email address for correspondence: g.papadakis@ic.ac.uk 466 G. Papadakis many others). A survey of the work in the area until the late 1960s is provided by Cox (1969).…”
Section: Introductionmentioning
confidence: 99%