scholarly journals YI 1.1 Aortic Impedance and Total Arterial Compliance from Regional Pulse Wave Velocities

2020 ◽  
Vol 26 (Supplement 1) ◽  
pp. S1
Author(s):  
Vasiliki Bikia ◽  
Georgios Rovas ◽  
Stamatia Pagoulatou ◽  
Nikolaos Stergiopulos
1996 ◽  
Vol 84 (2) ◽  
pp. 368-376. ◽  
Author(s):  
Dermot Lowe ◽  
Douglas A. Hettrick ◽  
Paul S. Pagel ◽  
David C. Warltier

Background Systemic vascular resistance incompletely describes left ventricular afterload because of the phasic nature of arterial pressure and blood flow. Aortic input impedance is an experimental description of left ventricular afterload that incorporates the frequency- dependent characteristics and viscoelastic properties of the arterial system. The effects of propofol on aortic input impedance were examined using three variables derived from the three-element Windkessel model: characteristic aortic impedance, total arterial compliance, and total arterial resistance. Methods Eight dogs were chronically instrumented for measurement of aortic pressure, left ventricular pressure, +dP/dt, subendocardial segment length, and aortic blood flow. Systemic hemodynamics and aortic blood pressure and flow waveforms were recorded in the conscious state and after a bolus of 5 mg x kg(-1) propofol and infusion for 15 min at 25, 50 and 100 mg x kg(-1) x h(-1). Aortic input impedance spectra were generated using power spectral analysis of aortic pressure and flow waveforms corrected for the phase responses of the pressure and flow transducers. Characteristic aortic impedance, total arterial resistance, and total arterial compliance were calculated from the aortic input impedance spectrum and the aortic pressure waveform. Parameters describing the net site and magnitude or arterial wave reflection were determined from aortic impedance. Results Propofol decreased total arterial resistance (3.05 +/- 0.20 during control to 2.29 +/- 0.18 dynes x s x cm(-5) x 10(3) at the high dose) and increased total arterial compliance (0.53 +/- 0.04 during control to 1.15 +/- 0.17 ml x mmHg(-1) at the high dose) in a dose- related manner. Propofol increased characteristic aortic impedance (1.49 +/- 0.15 during control to 2.20 +/- 0.20 dynes x s x cm(-5) x 10(2) at the high dose). The net site and the magnitude of arterial wave reflection were unchanged by the propofol. Conclusions In chronically instrumented dogs, propofol decreased total arterial resistance, a property of arteriolar resistance vessels, consistent with the known actions of this drug on systemic vascular resistance. Propofol also increased total arterial compliance and characteristic aortic impedance, indicating that this anesthetic affects the mechanical properties of the aorta. Propofol had no effect on arterial wave reflection patterns. The results indicate that propofol reduces left ventricular afterload via decreases in peripheral resistance and increases in arterial compliance.


1998 ◽  
Vol 274 (4) ◽  
pp. H1393-H1403 ◽  
Author(s):  
Christopher M. Quick ◽  
David S. Berger ◽  
Abraham Noordergraaf

Recently, there has been renewed interest in estimating total arterial compliance. Because it cannot be measured directly, a lumped model is usually applied to derive compliance from aortic pressure and flow. The archetypical model, the classical two-element windkessel, assumes 1) system linearity and 2) infinite pulse wave velocity. To generalize this model, investigators have added more elements and have incorporated nonlinearities. A different approach is taken here. It is assumed that the arterial system 1) is linear and 2) has finite pulse wave velocity. In doing so, the windkessel is generalized by describing compliance as a complex function of frequency that relates input pressure to volume stored. By applying transmission theory, this relationship is shown to be a function of heart rate, peripheral resistance, and pulse wave reflection. Because this pressure-volume relationship is generally not equal to total arterial compliance, it is termed “apparent compliance.” This new concept forms the natural counterpart to the established concept of apparent pulse wave velocity.


2007 ◽  
Vol 103 (1) ◽  
pp. 66-79 ◽  
Author(s):  
Roberto Burattini ◽  
Paola Oriana Di Salvia

Aortic impedance data of infants, children and adults (age range 0.8–54 yr), previously reported by others, were interpreted by means of three alternative four-element windkessel models: W4P, W4S, and IVW. The W4P and W4S are derived from the three-element windkessel (W3) by connecting an inertance ( L) in parallel or in series, respectively, with the aortic characteristic resistance ( Rc). In the IVW, L is connected in series with a viscoelastic windkessel (VW). The W4S and IVW (same input impedance) fit the data best. The W4S, however, suffers from the assumption that Rc is part of total peripheral resistance ( Rp). The IVW model offers a new paradigm for interpretation of resistive properties in terms of viscous ( Rd) properties of vessel wall motion, distinguished from Rp. Results indicated that rapid reduction of Rd/ Rp during early development is functional to modulation of decay time constant (τd) of pressure in diastole, such that normalization over heart period (τd/T) is independent of body size. Estimates of total arterial compliance ( C) vs. age were fitted by a bell-shaped curve with a maximum at 33 yr. With body weight (BW) factored out by normalization, the C/BW data scattered about a bell-shaped curve centered at 66 mmHg. Inertance was significantly higher in pediatric patients than in adults, in accordance with a lower cross-sectional area of the vasculature, commensurate to a lower aortic flow. Changes of arterial properties appear functional to control the ratio of pulsatile power to active power and keep arterial efficiency as high as 97% in infants and children.


2012 ◽  
Vol 40 (12) ◽  
pp. 2619-2626 ◽  
Author(s):  
Orestis Vardoulis ◽  
Theodore G. Papaioannou ◽  
Nikolaos Stergiopulos

Author(s):  
Vasiliki Bikia ◽  
Georgios Rovas ◽  
Stamatia Pagoulatou ◽  
Nikolaos Stergiopulos

In-vivo assessment of aortic characteristic impedance (Zao) and total arterial compliance (CT) has been hampered by the need for either invasive or inconvenient and expensive methods to access simultaneous recordings of aortic pressure and flow, wall thickness, and cross-sectional area. In contrast, regional pulse wave velocity (PWV) measurements are non-invasive and clinically available. In this study, we present a non-invasive method for estimating Zao and CT using cuff pressure, carotid-femoral PWV (cfPWV), and carotid-radial PWV (crPWV). Regression analysis is employed for both Zao and CT. The regressors are trained and tested using a pool of virtual subjects (n = 3,818) generated from a previously validated in-silico model. Predictions achieved an accuracy of 7.40%, r = 0.90, and 6.26%, r = 0.95, for Zao, and CT, respectively. The proposed approach constitutes a step forward to non-invasive screening of elastic vascular properties in humans by exploiting easily obtained measurements. This study could introduce a valuable tool for assessing arterial stiffness reducing the cost and the complexity of the required measuring techniques. Further clinical studies are required to validate the method in-vivo.


1952 ◽  
Vol 30 (2) ◽  
pp. 125-129
Author(s):  
J. P. Adamson ◽  
J. Doupe

Intra-arterial pressures and pulse wave velocities were measured in 18 subjects whose auscultatory diastolic pressures ranged from 45 to 120 mm. Hg. Various methods were used to lower the blood pressure in the hypertensive and to raise it in nonhypertensive subjects so that pulse wave velocities might be compared in all subjects at a common diastolic pressure. The pulse wave velocities were calculated for a diastolic pressure of 80 mm. Hg. No significant differences were found between hypertensive and nonhypertensive subjects. It was concluded that a defect of arterial elasticity as gauged by pulse wave velocity is not a factor in the pathogenesis of hypertension.


1999 ◽  
Vol 276 (2) ◽  
pp. H424-H428 ◽  
Author(s):  
N. Stergiopulos ◽  
P. Segers ◽  
N. Westerhof

We determined total arterial compliance from pressure and flow in the ascending aorta of seven anesthetized dogs using the pulse pressure method (PPM) and the decay time method (DTM). Compliance was determined under control and during occlusion of the aorta at four different locations (iliac, renal, diaphragm, and proximal descending thoracic aorta). Compliance of PPM gave consistently lower values (0.893 ± 0.015) compared with the compliance of DTM (means ± SE; r = 0.989). The lower compliance estimates by the PPM can be attributed to the difference in mean pressures at which compliance is determined (mean pressure, 81.0 ± 3.6 mmHg; mean diastolic pressure, over which the DTM applies, 67.0 ± 3.6 mmHg). Total arterial compliance under control conditions was 0.169 ± 0.007 ml/mmHg. Compliance of the proximal aorta, obtained during occlusion of the proximal descending aorta, was 0.100 ± 0.007 ml/mmHg. Mean aortic pressure was 80.4 ± 3.6 mmHg during control and 102 ± 7.7 mmHg during proximal descending aortic occlusion. From these results and assuming that upper limbs and the head contribute as little as the lower limbs, we conclude that 60% of total arterial compliance resides in the proximal aorta. When we take into account the inverse relationship between pressure and compliance, the contribution of the proximal aorta to the total arterial compliance is even more significant.


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