Computational Fluid and Solid Mechanics 2003 2003
DOI: 10.1016/b978-008044046-0/50436-x
|View full text |Cite
|
Sign up to set email alerts
|

On deriving lumped models for blood flow and pressure in the systemic arteries

Abstract: Abstract. Windkessel and similar lumped models are often used to represent blood flow and pressure in systemic arteries. The windkessel model was originally developed by Stephen Hales (1733) and Otto Frank (1899) who used it to describe blood flow in the heart. In this paper we start with the onedimensional axisymmetric Navier-Stokes equations for time-dependent blood flow in a rigid vessel to derive lumped models relating flow and pressure. This is done through Laplace transform and its inversion via residue … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
36
0

Year Published

2013
2013
2020
2020

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 22 publications
(36 citation statements)
references
References 20 publications
0
36
0
Order By: Relevance
“…Considering conservation of linear momentum in each compartment depicted in Figure , the 0D reduced pressure‐flow relation reads Lnormaldqnormaldt+Rq=p, with the individual compartment's inertance L and its resistance R . Note that these relations can be derived from considering axisymmetric flow of incompressible Newtonian fluid of density ϱ and dynamic viscosity η through a rigid vessel with length l 0 and radius r 0 …”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Considering conservation of linear momentum in each compartment depicted in Figure , the 0D reduced pressure‐flow relation reads Lnormaldqnormaldt+Rq=p, with the individual compartment's inertance L and its resistance R . Note that these relations can be derived from considering axisymmetric flow of incompressible Newtonian fluid of density ϱ and dynamic viscosity η through a rigid vessel with length l 0 and radius r 0 …”
Section: Methodsmentioning
confidence: 99%
“…Therein, λq=1false/β12, with β 1 being the first root of the zeroth‐order Bessel function of the first kind. Further details of fluid mechanics derivations of 0‐dimensional flow models can be found in the work of Olufsen et al…”
Section: Methodsmentioning
confidence: 99%
“…In contrast, the present preliminary study proposes a new concept of a mechanical extracorporeal device, which is capable to mobilize at least four In general, the clinical applications of ESS with cardiac-assist devices (CAD) are controlled by several diversities between the cardiovascular system and lumped models (45,46). As shown in (Fig.…”
Section: Discussionmentioning
confidence: 99%
“…Considering that an artery is cylindrical, we can study the Poiseuille flow in the artery . Because of the cylindrical symmetry of the artery and assuming that the blood flow is axisymmetric in one dimension through a rigid artery that means the pressure inside the artery will be assumed to be independent of the radial coordinate, then the Navier–Stokes equation becomes ρtυx(rMathClass-punc,t)MathClass-bin−η[]r2MathClass-bin+1rrυx(rMathClass-punc,t)MathClass-rel=MathClass-bin−rp(rMathClass-punc,t) The boundary and initial conditions for υ χ (r,t) are υx(aMathClass-punc,t)MathClass-rel=0MathClass-punc,1emquadxυx(0MathClass-punc,t)MathClass-rel=0MathClass-punc,1emquadυx(rMathClass-punc,0)MathClass-rel=Δp4ηℓ()a2MathClass-bin−r2MathClass-punc,1emquadυx(rMathClass-punc,MathClass-rel∞)MathClass-rel=0 where Δ p is the change in pressure between the inlet and the outlet of the artery, and ℓ is the length of the artery taking into account that the blood stops flowing in the end (Figure ).…”
Section: Methodsmentioning
confidence: 99%