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Computational characterizations of aortic valve hemodynamics have typically discarded the effects of coronary flow. The objective of this study was to complement our previous fluid-structure interaction aortic valve model with a physiologic coronary circulation model to quantify the impact of coronary flow on aortic sinus hemodynamics and leaflet wall shear stress (WSS). Coronary flow suppressed vortex development in the two coronary sinuses and altered WSS magnitude and directionality on the three leaflets, with the most substantial differences occurring in the belly and tip regions.
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Computer Methods in Biomechanics and Biomedical
Engineering
ISSN: 1025-5842 (Print) 1476-8259 (Online) Journal homepage: http://www.tandfonline.com/loi/gcmb20
Aortic valve leaflet wall shear stress
characterization revisited: impact of coronary flow
K. Cao & P. Sucosky
To cite this article: K. Cao & P. Sucosky (2016): Aortic valve leaflet wall shear stress
characterization revisited: impact of coronary flow, Computer Methods in Biomechanics and
Biomedical Engineering, DOI: 10.1080/10255842.2016.1244266
To link to this article: http://dx.doi.org/10.1080/10255842.2016.1244266
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COMPUTER METHODS IN BIOMECHANICS AND BIOMEDICAL ENGINEERING, 2016
http://dx.doi.org/10.1080/10255842.2016.1244266
Aortic valve leaet wall shear stress characterization revisited: impact of
coronary ow
K. Caoa and P. Sucoskyb
aDepartment of Aerospace and Mechanical Engineering, University of Notre Dame, Notre Dame, IN, USA; bDepartment of Mechanical and
Materials Engineering, Wright State University, Dayton, OH, USA
ABSTRACT
Computational characterizations of aortic valve hemodynamics have typically discarded the eects
of coronary ow. The objective of this study was to complement our previous uid–structure
interaction aortic valve model with a physiologic coronary circulation model to quantify the impact
of coronary ow on aortic sinus hemodynamics and leaet wall shear stress (WSS). Coronary ow
suppressed vortex development in the two coronary sinuses and altered WSS magnitude and
directionality on the three leaets, with the most substantial dierences occurring in the belly and
tip regions.
1. Introduction
Aortic valve (AV) leaets are sensitive to their surround-
ing hemodynamic stress environment. While physiologic
ow promotes AV homeostasis, wall shear stress (WSS)
abnormalities trigger pathological cascades that may lead
ultimately to calcic aortic valve disease (CAVD) (Sucosky
et al. 2009; Hoehn et al. 2010; Sun et al. 2012, 2013; Sun &
Sucosky 2015). is hypothetical hemodynamic etiology of
valvular disease has motivated the characterization of the
native leaet WSS environment using uid–structure inter-
action (FSI) modeling (Chandra et al. 2012; Cao & Sucosky
2015; Gilmanov & Sotiropoulos 2016; Cao & Sucosky
forthcoming 2016). While those studies have shed new light
on valvular mechanics and function, the impact of the cor-
onary circulation on valvular ow has been discarded. As
observed experimentally, the coronary ow established dur-
ing diastole generates complex vortex dynamics in the aortic
sinus, which interacts with the leaets and may alter their
regional stress distribution (Moore & Dasi 2015). e aim
of this study was to complement our previous FSI AV model
with a physiologic coronary circulation model to quantify
the impact of coronary ow on AV ow and leaet WSS.
2. Materials and methods
Our previous FSI AV model (Cao et al. 2016) was used
as the basis for this study. e aortic root geometry was
modied to include the coronary ostia and the proximal
segments of the coronary arteries. e le- and right-cor-
onary ostia were modeled as circular (diameter: 4.0 and
3.2mm, respectively) and were positioned 18mm above
the valve annulus (Waller et al. 1992) (Figure 1(a)). e
proximal le- and right-coronary arteries (LCA and RCA,
respectively) were modeled as cylindrical extensions
(length: 6.0mm) with a wall thickness of 0.4mm (Dong et
al. 2015). e coronary arteries were approximated as iso-
tropic linear elastic materials (Young’s modulus: 0.4MPa,
Claes et al. 2010).
Two Windkessel models were implemented to pre-
scribe realistic LCA and RCA ow rates (Q):
where P is the aortic pressure, R1 is the coronary arterial
resistance, R2 is the coronary venous resistance and C is
the coronary arterial compliance (Figure 1(b)) (Westerhof
et al. 2009). Each model was calibrated using two sets of
parameters (Table 1) to generate physiologic human cor-
onary ow rates during systole and diastole, respectively
(Koeppen & Stanton 2009) (Figure 1(c)).
Arbitrary Lagrangian Eulerian simulations were car-
ried out in ANSYS 15.0 over three cardiac cycles and all
results were extracted during the last cycle. All model
parameters, numerical treatments and mesh sensitivity
analyses have been described in our previous FSI AV
(1)
CR
1
dQ
dt+
(
1+
R
1
R
2)
Q=CdP
dt+1
R
2
P
,
KEYWORDS
Aortic valve; coronary flow;
fluid–structure interaction;
hemodynamics; wall shear
stress; aortic sinus
ARTICLE HISTORY
Received 4 May 2016
Accepted 29 September 2016
© 2016 Informa UK Limited, trading as Taylor & Francis Group
CONTACT P. Sucosky philippe.sucosky@wright.edu
The supplementary material for this paper is available online at http://dx.doi.org/10.1080/10255842.2016.1244266.
2 K. CAO AND P. SUCOSKY
3. Results
Coronary ow resulted in asymmetric hemodynamics in
the aortic sinuses during diastole, marked by recirculation
and intense vorticity in the non-coronary sinus and more
moderate vorticity in the coronary sinuses (Figure 2(a)
and Supplemental Material – video.mp4). Quantication
of the peak-systolic valve geometric orice area (GOA)
revealed a 7% increase in the presence of coronary ow
model (Cao et al. 2016). Valvular ow was characterized in
terms of vorticity and velocity. Regional WSS magnitude
and directionality were quantied in terms of temporal
shear magnitude (TSM) and oscillatory shear index (OSI)
in the base, belly and tip of the non-, right- and le-cor-
onary leaets (i.e. NC, RC and LC leaets, respectively)
and compared to those captured by our previous model
in the absence of coronary ow (REF leaet).
Figure 1.Model setup: (a) AV geometry; (b) Windkessel electrical analog; and (c) coronary flow rates generated by the Windkessel models
at the LCA and RCA outlets (physiologic values adapted from Koeppen & Stanton 2009).
Table 1.Windkessel parameters.
Systole Diastole
R1 (kg/(m4s) R2 (kg/(m4s) C (m4s2/kg) R1 (kg/(m4s) R2 (kg/(m4s) C (m4s2/kg)
LCA 5.7 × 1091.9 × 1011 4.9 × 10−11 3.8 × 1092.1 × 1011 9.7 × 10−11
RCA 1.7 × 1010 5.7 × 1011 1.6 × 10−11 3.9 × 1010 1.9 × 1011 9.6 × 10−12
Figure 2.Comparison of AV hemodynamics without and with coronary flow: (a) diastolic velocity and vorticity fields; (b) TSM and (c) OSI
regional distributions on the leaflet fibrosa.
COMPUTER METHODS IN BIOMECHANICS AND BIOMEDICAL ENGINEERING 3
relative to our previous model (Supplemental Material
– Figure S1), demonstrating the benecial impact of the
coronary circulation on valvular function.
As compared to our previous model, coronary ow
generated an overall increase in WSS magnitude and uni-
directionality on the leaet brosa (up to 30% increase
in TSM, up to 0.10 decrease in OSI vs. REF leaet), with
the most apparent changes occurring in the belly and
tip regions (Figure 2(b) and (c)). e asymmetry in vor-
ticity dynamics introduced by the coronary circulation
translated into discrepancies in WSS magnitude and
directionality between the three leaets. e LC and RC
leaets were subjected to WSS overloads (30 and 15%
increase, respectively) relative to the NC leaet. While
this increase aected the belly and tip of the LC leaet, it
only occurred in the tip of the RC leaet. Coronary ow
also generated asymmetric and spatially-dependent OSI
distributions on the leaets, with mixed directionality in
the base (0.26<OSI<0.30), more pronounced bidirec-
tionality in the belly (OSI>0.31) and strong unidirec-
tionality in the tip (OSI<0.15). While WSS directionality
was essentially similar in the base of all three leaets, it
was markedly more bidirectional in the belly of the RC
and NC leaets (0.13 and 0.12 OSI increase, respectively)
relative to the LC leaet and more unidirectional in the
tip of the LC and RC leaets (0.09 OSI decrease) relative
to the NC leaet.
4. Discussion
In summary, coronary ow suppressed vortex devel-
opment in the coronary sinuses and promoted valvular
function. ose results are consistent with particle image
velocimetry measurements of aortic sinus ow with phys-
iologic coronary ow (Moore & Dasi 2015). Coronary
ow resulted in contrasted WSS patterns on the three
leaets, with the most substantial dierences occurring
in the belly and tip regions. e distinctly lower and more
bidirectional WSS on the NC leaet may explain its higher
vulnerability to calcication (Freeman & Otto 2005). To
conclude, coronary ow impacts the leaet WSS environ-
ment and should be accounted for in the characterization
of the native valvular hemodynamic stresses.
Disclosure statement
No potential conict of interest was reported by the authors.
Funding
is work supported by Division of Civil, Mechanical and Man-
ufacturing Innovation, National Science Foundation [grant
number CMMI-1148558], [grant number CMMI-1550144];
American Heart Association [grant number 14PRE18940010].
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... 4 AV diseases. [6][7][8] Preliminary data suggest that a large aortic root aneurysm is a risk factor for the failure of a valve-sparing aortic root replacement (VSARR), highlighting the detrimental effects of a large aneurysm on the leaflet. 9, 10 We hypothesized that an aortic root aneurysm would alter the fluid dynamics around the AV, placing abnormal mechanical stress on the leaflets. ...
... Second, while we included the patients who underwent CABG as controls, mechanical stress on the AV could be abnormal due to decreased coronary flow and co-existing atherosclerotic changes of the aorta or the AV leaflets. 6 We mitigated these concerns by selecting the belly of the non-coronary cusp to minimize the effects of coronary flow and by excluding patients with any abnormal appearance of the aortic root and valve. Our methodology required the using an epiaortic echocardiogram, so we selected a control cohort from the patients who were undergoing open-heart surgery. ...
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Calcific aortic valve disease (CAVD) is an active process presumably triggered by interplays between cardiovascular risk factors, molecular signaling networks and hemodynamic cues. While earlier studies demonstrated that alterations in fluid shear stress (FSS) on the fibrosa could trigger inflammation, the mechanisms of CAVD pathogenesis secondary to side-specific FSS abnormalities are poorly understood. This knowledge could be critical to the elucidation of key CAVD risk factors such as congenital valve defects, aging and hypertension, which are known to generate FSS disturbances. The objective of this study was to characterize ex vivo the contribution of isolated and combined abnormalities in FSS magnitude and frequency to early valvular pathogenesis. The ventricularis and fibrosa of porcine aortic valve leaflets were exposed simultaneously to different combinations of sub-physiologic/physiologic/supra-physiologic levels of FSS magnitude and frequency for 24, 48 and 72 hours in a double cone-and-plate device. Endothelial activation and paracrine signaling were investigated by measuring cell-adhesion molecule (ICAM-1, VCAM-1) and cytokine (BMP-4, TGF-β1) expressions, respectively. Extracellular matrix (ECM) degradation was characterized by measuring the expression and activity of the proteases MMP-2, MMP-9, cathepsin L and cathepsin S. The effect of the FSS treatment yielding the most significant pathological response was examined over a 72-hour period to characterize the time-dependence of FSS mechano-transduction. While cytokine expression was stimulated under elevated FSS magnitude at normal frequency, ECM degradation was stimulated under both elevated FSS magnitude at normal frequency and physiologic FSS magnitude at abnormal frequency. In contrast, combined FSS magnitude and frequency abnormalities essentially maintained valvular homeostasis. The pathological response under supra-physiologic FSS magnitude peaked at 48 hours but was then maintained until the 72-hour time point. This study confirms the sensitivity of valve leaflets to both FSS magnitude and frequency and suggests the ability of supra-physiologic FSS levels or abnormal FSS frequencies to initiate CAVD mechanisms.
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The bicuspid aortic valve (BAV) is the most common congenital cardiac anomaly and is frequently associated with calcific aortic valve disease (CAVD). The most prevalent type-I morphology, which results from left-/right-coronary cusp fusion, generates different hemodynamics than a tricuspid aortic valve (TAV). While valvular calcification has been linked to genetic and atherogenic predispositions, hemodynamic abnormalities are increasingly pointed as potential pathogenic contributors. In particular, the wall shear stress (WSS) produced by blood flow on the leaflets regulates homeostasis in the TAV. In contrast, WSS alterations cause valve dysfunction and disease. While such observations support the existence of synergies between valvular hemodynamics and biology, the role played by BAV WSS in valvular calcification remains unknown. The objective of this study was to isolate the acute effects of native BAV WSS abnormalities on CAVD pathogenesis. Porcine aortic valve leaflets were subjected ex vivo to the native WSS experienced by TAV and type-I BAV leaflets for 48 hours. Immunostaining, immunoblotting and zymography were performed to characterize endothelial activation, pro-inflammatory paracrine signaling, extracellular matrix remodeling and markers involved in valvular interstitial cell activation and osteogenesis. While TAV and non-coronary BAV leaflet WSS essentially maintained valvular homeostasis, fused BAV leaflet WSS promoted fibrosa endothelial activation, paracrine signaling (2.4-fold and 3.7-fold increase in BMP-4 and TGF-β1, respectively, relative to fresh controls), catabolic enzyme secretion (6.3-fold, 16.8-fold, 11.7-fold, 16.7-fold and 5.5-fold increase in MMP-2, MMP-9, cathepsin L, cathepsin S and TIMP-2, respectively) and activity (1.7-fold and 2.4-fold increase in MMP-2 and MMP-9 activity, respectively), and bone matrix synthesis (5-fold increase in osteocalcin). In contrast, BAV WSS did not significantly affect α-SMA and Runx2 expressions and TIMP/MMP ratio. This study demonstrates the key role played by BAV hemodynamic abnormalities in CAVD pathogenesis and suggests the dependence of BAV vulnerability to calcification on the local degree of WSS abnormality.
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Calcific aortic stenosis is the most common aortic valve (AV) disease and is triggered by an active inflammatory process involving endothelial activation and cytokine expression. Interfacing between the leaflet and the surrounding blood flow, shear stress is presumed to play an important role in endothelial injury. This study investigated the hypothesis that pathologic alterations in shear stress magnitude contribute to valvular endothelial activation via BMP-4- and TGF-β1-dependent mechanisms. The fibrosa of porcine AV leaflets was subjected to physiologic, sub-physiologic and supra-physiologic magnitudes of native oscillatory shear stress for 48h. Endothelial activation was assessed via immunohistochemistry in terms of ICAM-1 and VCAM-1 expressions. Cytokine expression was investigated in terms of BMP-4 and TGF-β1. Pro- and anti-osteogenic media were used to characterize the role of those cytokines in the shear stress-induced pathological response. Supra-physiologic shear stress increased the expression of all biomarkers in a shear stress magnitude-dependent manner. In contrast, neither physiologic nor sub-physiologic shear stress elicited a pro-inflammatory response. While BMP-4 inhibition and supplementation had limited effects on endothelial activation, TGF-β1 supplementation increased the overall leaflet pro-inflammatory state and TGF-β1 inhibition reduced endothelial activation in response to elevated shear stress. Combined TGF-β1 and BMP-4 inhibition completely suppressed shear stress-induced endothelial activation. The results demonstrate that elevated shear stress activates the valvular endothelium on the fibrosa via a BMP-4- and TGF-β1-dependent pathway. The suggested synergy between those cytokines also provides new insights into the transduction of valvular hemodynamic alterations into a pathological response. KeywordsAortic valve-Endothelial activation-Shear stress-Cytokines-Adhesion molecules
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Mechanical stresses on aortic valve leaflets are well-known mediators for initiating processes leading to calcific aortic valve disease. Given that non-coronary leaflets calcify first, it may be hypothesized that coronary flow originating from the ostia significantly influences aortic leaflet mechanics and sinus hemodynamics. High resolution time-resolved particle image velocimetry (PIV) measurements were conducted to map the spatiotemporal characteristics of aortic sinus blood flow and leaflet motion with and without physiological coronary flow in a well-controlled in vitro setup. The in vitro setup consists of a porcine aortic valve mounted in a physiological aorta sinus chamber with dynamically controlled coronary resistance to emulate physiological coronary flow. Results were analyzed using qualitative streak plots illustrating the spatiotemporal complexity of blood flow patterns, and quantitative velocity vector and shear stress contour plots to show differences in the mechanical environments between the coronary and non-coronary sinuses. It is shown that the presence of coronary flow pulls the classical sinus vorticity deeper into the sinus and increases flow velocity near the leaflet base. This creates a beneficial increase in shear stress and washout near the leaflet that is not seen in the non-coronary sinus. Further, leaflet opens approximately 10% farther into the sinus with coronary flow case indicating superior valve opening area. The presence of coronary flow significantly improves leaflet mechanics and sinus hemodynamics in a manner that would reduce low wall shear stress conditions while improving washout at the base of the leaflet.