P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGN

The increase of arterial volume during the systole (‘pulse volume’) is essential for buffering the pulsatile ventricular output. Objectives: Deriving some mechanical properties of arteries by assuming pulse volume homeostasis. Methods: A model that includes a generalized nonlinear relationship bet...

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Main Author: B. Gavish
Format: Article
Language:English
Published: Atlantis Press 2013-11-01
Series:Artery Research
Online Access:https://www.atlantis-press.com/article/125939063/view
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spelling doaj-1391f719ad52478aaf8688057190410a2020-11-25T03:20:19ZengAtlantis PressArtery Research 1876-44012013-11-0171010.1016/j.artres.2013.10.185P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGNB. GavishThe increase of arterial volume during the systole (‘pulse volume’) is essential for buffering the pulsatile ventricular output. Objectives: Deriving some mechanical properties of arteries by assuming pulse volume homeostasis. Methods: A model that includes a generalized nonlinear relationship between arterial pressure P and volume V (see figure below). Results: If the pulse volume ΔV is constant, then for a given diastolic volume VD and pressure D the systolic volume VD+ΔV and pressure S are uniquely determined. For this reason, an infinitesimal increase of the diastolic pressure by dD would result in an increase of the systolic pressure by dS with the same volume change dV for both pressures. Since the systolic and diastolic stiffness is defined by G(S)=dS/dV and G(D)=dD/dV, respectively, we find that dS/dD=G(S)/G(D) (Eq.1). As D and ΔV determine S uniquely, dS/dD is a function of D and ΔV only. However, if dS/dD is independent of D and ΔV is constant, then K=dS/dD is a constant (Eq.2) equal to the relative increase of arterial stiffness during the systole. The only solution of Eq.2 is the well-documented linear relationship between the systolic and diastolic pressures with slope K and constant A, i.e., S=A+KD (Eq.3). The solution of Eq.3, rewritten as P(V+ΔV)=A+KP(V), is the observed exponential pressure-volume relationship in arteries that is also expressed by the demonstrated linear dependence of arterial stiffness on pressure. s: Arterial stiffening at elevated pressures may reflect an arterial design principle that aims at preserving the arterial buffering function via pulse volume homeostasis.https://www.atlantis-press.com/article/125939063/view
collection DOAJ
language English
format Article
sources DOAJ
author B. Gavish
spellingShingle B. Gavish
P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGN
Artery Research
author_facet B. Gavish
author_sort B. Gavish
title P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGN
title_short P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGN
title_full P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGN
title_fullStr P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGN
title_full_unstemmed P6.04 PULSE VOLUME HOMEOSTASIS AS A HYPOTHESIZED PRINCIPLE OF ARTERIAL DESIGN
title_sort p6.04 pulse volume homeostasis as a hypothesized principle of arterial design
publisher Atlantis Press
series Artery Research
issn 1876-4401
publishDate 2013-11-01
description The increase of arterial volume during the systole (‘pulse volume’) is essential for buffering the pulsatile ventricular output. Objectives: Deriving some mechanical properties of arteries by assuming pulse volume homeostasis. Methods: A model that includes a generalized nonlinear relationship between arterial pressure P and volume V (see figure below). Results: If the pulse volume ΔV is constant, then for a given diastolic volume VD and pressure D the systolic volume VD+ΔV and pressure S are uniquely determined. For this reason, an infinitesimal increase of the diastolic pressure by dD would result in an increase of the systolic pressure by dS with the same volume change dV for both pressures. Since the systolic and diastolic stiffness is defined by G(S)=dS/dV and G(D)=dD/dV, respectively, we find that dS/dD=G(S)/G(D) (Eq.1). As D and ΔV determine S uniquely, dS/dD is a function of D and ΔV only. However, if dS/dD is independent of D and ΔV is constant, then K=dS/dD is a constant (Eq.2) equal to the relative increase of arterial stiffness during the systole. The only solution of Eq.2 is the well-documented linear relationship between the systolic and diastolic pressures with slope K and constant A, i.e., S=A+KD (Eq.3). The solution of Eq.3, rewritten as P(V+ΔV)=A+KP(V), is the observed exponential pressure-volume relationship in arteries that is also expressed by the demonstrated linear dependence of arterial stiffness on pressure. s: Arterial stiffening at elevated pressures may reflect an arterial design principle that aims at preserving the arterial buffering function via pulse volume homeostasis.
url https://www.atlantis-press.com/article/125939063/view
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