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Validity of Korteweg-de-Vries Equation for Arterial Pulse Waves

机译:Korteweg-de-Vries方程对动脉脉搏波的有效性

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Korteweg-de-Vries equation (KdV) is very popular tool to describe nonlinear waveform like cnoidal waves or solitons. The long waves within environments with weak dispersion are the object of it. Many authors recognize pulse waves (PW) in blood vessels as varieties of such nonlinear waves. Therefore, the solution of the problem of the dispersion for pulse waves is either solid scientific support or vice versa of this widespread viewpoint. This paper first presents the solution of above problem with methods of dimension analysis. This technique is utterly independent of assumptions that are backbone of KdV theory. The results of analysis show that the dispersion of PW depends just of two parameters. Both of them are proportional to wavenumber. The ratio of them is equal to large Reynolds number. Thus, we can keep only one of them. It is dimensionless wave number: u = 2 π D λ 1, where D is inner diameter of vessel, and λ is the wavelength. For our purposes important is the result about weak dispersion of pulse waves. The dependence of frequency vs. the wavenumber is almost linear with minor cubic adding. Pulse wave is quite long wave as it follows from dimensional analysis. Both these outcomes confirm the validity of KdV equation for pulse waves into blood vessels.
机译:Korteweg-de-Vries方程(KdV)是非常流行的工具,用于描述非线性波形,例如正弦波或孤子。其目的是在色散较弱的环境中产生长波。许多作者认识到血管中的脉搏波(PW)是此类非线性波的变体。因此,对于脉冲波的色散问题的解决方案是该广泛观点的可靠科学支持,反之亦然。本文首先用尺寸分析方法提出了上述问题的解决方案。该技术完全独立于作为KdV理论基础的假设。分析结果表明,PW的色散仅取决于两个参数。它们都与波数成正比。它们的比率等于大的雷诺数。因此,我们只能保留其中之一。它是无量纲的波数:u = 2πDλ 1,其中D是血管的内径,而λ是波长。就我们的目的而言,重要的是有关脉搏波的弱散射的结果。频率与波数的相关性几乎是线性的,并且增加了三次立方。脉搏波是很长的波,因为它来自尺寸分析。这些结果都证实了KdV方程对于脉搏波进入血管的有效性。

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