Abstract
Purpose
To assess the impact of aortic valve morphology on aortic hemodynamicsbetweennormal tricuspid and congenitally anomalous aortic valvesranging from unicuspid to quadricuspid morphology.
Materials and Methods
Aortic 3D blood flow was evaluated by 4D flow MRI in 14 healthy volunteers with normal trileaflet valves and 14 patients withunicuspid(n=3), bicuspid (n=9, 3 ‘true’ bicuspid, 3 right-left (RL), 3 right-non (RN) coronary leaflet fusion, and quadricuspid aortic valves (n=2). Data analysis included the co-registered visualization of aortic valve morphology with systolic 3D blood flow. The influence of valve morphology on aortic hemodynamics was quantified by valve flow angle.
Results
All RL-BAV were associated with flow jets directed towards the right anterior aortic wallwhile RN-fusion and unicuspid valves resulted in flow jet patterns towards the right-posterior or posterior wall. Flow angles were clearly influenced by valve morphology(47°±10, 28°±2, 29°±18, 18°±12, 15°±2 for unicuspid, trueBAV, RN-BAV, RL-BAV, quadricuspid valves) and increased compared to controls (7.2°±1.1, p=0.001).
Conclusions
Altered 3D aortic hemodynamics are impacted by the morphology of congenitally malformed aortic valves.
Keywords: 4D flowMRI, aortic valve, unicuspid valve, bicuspid valve, quadricuspid valve, hemodynamics
INTRODUCTION
Aortic valve anatomy can vary over a wide range of morphologiesranging from unicuspid to quadricuspid valve type 1. The most common valve abnormality is the congenitalbicuspid valve (BAV) with two functional leaflets1. BAV occurs in the general population at a rate of 1-2% and is associated with significantcomplications such as aortic aneurysm and dissection2,3. BAVhas several subtypes grouped by the valve leaflet fusion patterns (type 1right-left leaflet fusion, RL; type 1 right-non-coronary leaflet fusion, RN; and type 0, or a ‘true’bicuspid valve)1. Additional rarer variants include unicuspid (or unicommisural/monocuspid) and quadricuspid (four leaflets) valves which have been foundwith an incidence of 0.02% and 0.043%, respectively. Both phenotypes have beenassociated with aortic stenosis and dilation45.
Recently, the effect of valve morphology on 3D blood flow changes in the ascending aorta has been identified as a potential contributing factor to the development of aortic pathologies6-10. These studies, based on 4D flow MRI, have shown that the 3D alterations in blood flow in the presence of BAV can result in alteredaortic hemodynamics and thus wall shear forces which are suspected to promote aortic remodeling. Prior studies have also directly linked BAVRL and RN fusion patterns to altered aortic hemodynamics6,9-11.Additionally, relationships between valve morphology and aortopathy have also been shown in previous studies using CTA and MR8,12,13. The purpose ofthis study was toevaluatechanges in aortic hemodynamics in a case series representing the wide range of congenitally abnormal aortic valvesincluding rare unicuspid and quadricuspid cup fusion phenotypes. We hypothesize that the different valve morphologies will directly influence these metrics of ascending aorta hemodynamics.
METHODS
Study Population
Our study cohort was comprised of 14 patients and 14 healthy volunteers. All subjectsunderwent MRI of the thoracic aorta between November 2011 and August2012to evaluate ascending aortadimensions, aortic valve morphology, and aortic 3D blood flow.Patients with congenitally abnormal valves were retrospectively selected toinclude three main groups: group 1) those with a unicuspid aortic valve (n=3, age: 43 ±4 years, 1 female), group 2) those with BAV (n= 9, age: 44±9 years, 4 females), and group 3) those with a quadricuspid aortic valve (n=2, 41±1years old, 1 female).BAV patients were further selected according to the type of leaflet fusion pattern, comprising of those with a right-left coronary leafletfusion (RL, n=3), a right-noncoronaryleaflet fusion (RN, n=3), and a ‘true’ bicuspid (n=3, defined as twoequally-sized leafletswith no raphe, and the orifice opening parallel to the inter-atrial septum,or referenced by Sievers at al. as type 0-lat)1. In addition, 14healthy controls with a normal trileaflet aortic valve were included in the study cohort (age:33.1±7.7years, 4females). The study was approved by the Institutional Review Board of Northwestern University (IRB). Informed consent was obtained from all healthy controls. Patients were included in accordance with an IRB protocol which permitted retrospective chart review.
MR Imaging
Cardiac MRI was performedat 1.5T or 3T(Magnetom Espree,Avanto or Skyra,Siemens Medical Systems, Germany).To assess valve morphology and global cardiac function, breath-held, ECG-gatedtime-resolved (CINE) 2DbalancedSSFPimages were acquired in all patients14. For valve imaging, a 2D imaging plane was positioned orthogonal to the aorta at the level of the aortic valve(Figure 1). The 2D CINE SSFP sequenceparameters were as follows: spatial resolution = 1.33×1.33-1.82×1.82mm, slice thickness = 6-8 mm, temporal resolution =11.32-46.72ms, and a flip angle of 74-78°. For the assessment of aortic blood flow, time-resolved 3D phase-contrast MRI with three-directional velocity encoding (4D flow MRI) was employedto measure 3D blood flow velocities with full volumetric coverage of the thoracic aorta15.4D flow MRI was acquired during free breathing using respiratory and prospective ECG gating in a sagittal oblique 3D volumeof the thoracic aorta using a velocity sensitivity of 150-200 cm/s along all three directions, a flip angle of15°, spatial resolution of 1.67-3.22×1.77-2.38×2.2-2.8mm, and a temporal resolution of38.4-43.2ms.
Data Analysis
4Dflow data were pre-processedfor noise filtering, eddy currentcorrection and velocity aliasing, as previouslydescribed16. 3D visualization of the velocity data was performed using commercialsoftware (EnSight, CEI, Inc. Apex, NC). Flow characteristics were visualized by 3D streamlines (lines tangent to the velocity field) at peak flow systole. 3D streamlines were color coded to reflect the local systolic blood flow velocity. In addition, time-resolved 3D pathlines were calculated to visualize 3D aortic blood flow over the cardiac cycle. To improve anatomic orientation, 2D CINE SSFP images of the aortic valve were co-registered to the 4D flow data as shown in Figure 2 and the supplemental video files.
Flow Jet Patterns
3D streamlines were evaluated to identify the existence of ascending aortic flow jets, defined as the existence of streamlines with high flow velocity > 1m/s (color coding = red, see Figures 2 and 3) away from the aortic centerline.Flow impingement zoneswere assessed to evaluate the relationship between the valve morphology and flow pattern. The position of flow impingement wasdetermined by visually identifying the anatomic location (R: right, L: left, A: anterior, P: posterior)of the aortic wall reached by the flowjet at the level of the mid-ascendingaorta.
Flow Angle
A 2D analysis plane was positioned in the proximal ascending aorta approximately 2 cm above the aortic valve (Figure 2b, white rectangle). Segmentation of the aortic lumen at each time step was used to quantify the lumen diameter and flow angle. The flow angle, i.e. the angle between the vector orthogonal to the analysis plane (n) and the mean flow vector (q) was calculated using θ = cos-1n.q (Figure 2b).
Statistical Analysis
Results are presented as mean ± standard deviation. Group comparisonswere performed using the Kruskal-Wallis test between the control population and the valve disease cohorts. A p value <0.05 was considered significant.
RESULTS
Patient demographics are summarized in Table 1. Examples of different valve morphologies are shown in Figure 1. The degree of aortic valve stenosis (AS) or insufficiency (AI) did not exceed “mild” for all subjects. The aorta was dilated in all patient groups compared to the trileafletpopulation with normal aortic size (3.6±0.4 cm vs. 2.6±0.3cm, p = 0.005).
Table 1.
congenitally deformed valves (n=14) |
p-value controls vs. all patients | ||||||
---|---|---|---|---|---|---|---|
control |
bicuspid |
||||||
tricuspid | unicus pid | true (lat) | right-non | right-left | quadricuspid | ||
n (female) | 14(4) | 3(1) | 3(2) | 3(2) | 3(0) | 2(1) | - |
Age | 33.1±7.7 | 43.1±4.0 | 39.1±2.9 | 42.2±10.8 | 51.9±9.1 | 40.6±0.5 | 0.030 |
AAo Diameter (cm) | 2.6±0.3 | 3.9±0.6 | 3.4±0.1 | 3.4±0.7 | 3.9±0.5 | 3.5±1.1 | 0.005 |
Flow Angle(°) | 7±1 | 47±10 | 28±2 | 29±18 | 18±12 | 15±2 | 0.001 |
Flow Imp. (A,R,P,L) | - | P | RA,RP,- | P | RA | RA,- | - |
(R: right, L: left, A: anterior, P: posterior, RA: right anterior, LA: left anterior, RP: right posterior, LP: left posterior). The p-value represents differences between normal tricuspid controls (n=14) and and the entire group of patients with congenitally altered valves (n=14).
Flow Jet Patterns
Figure 3 illustrates typical systolic aortic 3D flow patterns for all valve types. Normal trileaflet valves (Figure 3,controls on left) showed cohesive streamlines (mostly parallel to the ascending aortawithout flow jet impinging on the aortic wall). In contrast, 3D flow visualization for all congenitally abnormal valves showed marked flow derangement.Elevated velocity jets along the aortic wall could be clearly identified and associated with distinct flow impingement locations (Table 1). While all RL-BAV were associated with flow jets directed towards the right anterior aortic wall, RN-fusion and unicuspid valves resulted in flow jet patterns towards the right-posterior or posterior wall. Note that the differences in aortic flow pattern can visually be best appreciated in the supplemental video files.
Flow Angle
Results of flow angle analysis aresummarized in Table 1 and Figure 3. Markedly higher flow angles for unicuspid(47±10°) and BAV with true and RN fusion patterns(28°±2and 29°±18,respectively)confirmthat aortic flow was directed more towards the aortic wall compared to controls (7°±1). Changes in flow angle for RL-BAV and quadricuspid patients wereless pronounced (18°±12 and 15°±2, respectively).
DISCUSSION
4D flow MRI was employed to study in-vivo post-valvular flow dynamics in the ascending aorta of patients with congenitally malformed aortic valves.The findingssupport the hypothesis that variations in valve morphology will exhibit distinct changes in aortic hemodynamics according to the valve structure.In our small cohort of patients we found evidence for distinct changes in flow jet patterns and flow angle betweensubjects with unicuspid, bicuspid, trileaflet, and quadricuspid valves. Specifically, our findings indicate that the position of flow impingement zones may bedirectly related to the valve leaflet morphology.
In accordance to recent studies6,17, we found different 3D flowpatterns in the ascending aorta of our RL-BAV and RN-BAV patients compared to controls. In addition, even unicuspid and quadricuspid valves with more symmetric valve geometry exhibited clearly visible flow jets and impingement zones as well as marked differences in flow angle compared to tricuspid controls. Thesefindings indicate that differences in aortic hemodynamics canpotentially provide correlative (although not causative) evidence for an underlying mechanism behind the heterogenic expression of aortopathy in BAV patients with conjoined RL and RN leaflets1,8,13,18.If altered aortic hemodynamics do indeed contribute to the progression of aortopathy, then the data presented here illustrates a differentiating characteristic beyond genetic predisposition that mightbe used for risk stratification and clinical decision making. In contrast to previous studies measuring wall shear forces6,19, we chose to analyze our cohort using simple hemodynamic metrics that may act as proxy metrics of wall forces, such as the average blood flow angle in the ascending aorta and flow/wall impingement location. This is similar to efforts to simplify burden of WSS measurement, as highlighted in the recently published studies investigating the concept of ‘flow displacement’ 19,20
Aninter-leaflet raphe or false commissure was present in the unicuspid, RL, and RN patient cohorts. It is notable that flow impingement was observed at the aortic wall opposite to the fused leaflets in those patients with a raphe. Differences in leaflet fusion patterns maythus play a role in changing the flow impingement zone and aortic regions experiencing increased wall shear forces.
It is important to note that even without aortic valve stenosis, the morphology of BAV leads to changes in flow patternsbeyond those with healthy trileaflet valves6. For example, Della Corteet al. reported a decreased opening angle and restricted motility of valves as the main source of abnormal flow patternwhich was also correlated to greater aorta growth rates in BAV patients9. In addition, the correlation between the type of leaflet fusion and the local expression of aortopathy has been demonstrated8. While RN fusion has been associated with aortic arch aneurysms, the RL fusion has been correlated with aortic root dilatation13. In this context, previous studies by Barker et al. and Hope et al. demonstrated a correlation between leaflet fusion pattern and flow direction (RL and RN fusion resulting in right anterior and left posterior flow jet patterns, respectively)6,7.In the present study, the same flow impingement pattern was observed in patients with RL and RN valve fusion. If flow eccentricity isacontributor to aneurysm formation in BAV patients, increased flow angle and the anatomical location of flow impingement might help topredict the specific aorta wall segments at higher risk fordilatation.
The findings of this study indicate that 4D flow MRI and the possibility for a comprehensive assessment of aortic hemodynamics has the potential to improve the evaluationof an abnormal aortic valve and its impact on aortic flow and geometry. Nevertheless, we believe that knowledge of the valve morphology (fusion pattern, presence of stenosis or insufficiency) provides and important addition to information on regional aortic hemodynamics. Specifically, the structure-function relationship between valve abnormality, changes in aortic hemodynamics and development of aortopathy and not yet fully understood. Further longitudinal studies are needed to determine which combination of parameters (i.e. risk score) provides the best predictive value for patient prognosis.
An obvious limitation of this study is related to the small sample sizes of the individual valve morphology groups which precluded the use of subgroup statistical tests to quantify differences between specific morphologies of congenitally abnormal valves and trileaflet controls.In addition, the control group had smaller aortic diameters than the patients. Nevertheless, the data indicates a notable relationship between valve phenotype and and eccentric flow impingementzone.To our knowledge this is the first study providing a detailed comparison of aortic flow characteristics in a wide range of congenitally abnormal valves including rare subtypes such as those with unicuspid and quadricuspid morphologies.
3D analysis methods are needed for measuring and comparing the alignment of the aortic outflow jet relative to the curved axis (centerline at each level) of the ascending aorta, distinguishing jet flow angles from jet flow offset relative to local center line. In addition, new methods are needed for determining whether or not certain ascending aortic geometries are related to valve morphology and whether the flow jet angle and its direction relative to the aortic geometry is a determinant of altered hemodynamics. Application of these methods in larger patient cohorts are warranted to distinguish cause and effect among flow impingement zones, flow angle, aortic dilatation and BAV cusp fusion phenotype.
In conclusion, thisstudy provides evidence to support the hypothesis thatalterations in 3D aortic hemodynamics are closely linked with the morphology of congenitally abnormalaortic valves. Specifically, the measurement of outflow angle and the observation of the flow impingement regions were different between the valve phenotypes included in this study. Future studies in larger cohorts and longitudinal follow-up are warranted to further evaluate the implications for the development and progression of aortic disease.
Supplementary Material
ACKNOWLEDGMENTS
The authors also gratefully acknowledge preliminary review of the manuscript by Amir Davarpanah.
Grant support: NIH NHLBI grant R01HL115828, DFG (German Research Foundation) SCHN-1170/2-1 and SIR Foundation Pilot Research Grant. American Heart Association Scientist Development Grant 13SDG14360004. Additional support by the Northwestern's Bicuspid Aortic Valve Program at the Bluhm Cardiovascular Institute.
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