Joseph R Leach1, Chengcheng Zhu1, David Saloner1, and Michael D Hope1
1Radiology and Biomedical Imaging, University of California, San Francisco, San Francisco, CA, United States
Synopsis
Computational stress analyses of abdominal aortic aneurysms
(AAA) are of great interest for individual aneurysm rupture risk assessment. The
vast majority of patient-specific stress analyses are based on features seen at
computed tomography, which is incapable of resolving material heterogeneity within
intraluminal thrombus. Using T1-weighted black blood MRI, we imaged and explicitly
modeled MRI-discerned intraluminal thrombus heterogeneity in multiple AAA stress
analyses. Results demonstrate a limited effect of thrombus heterogeneity on the predicted vessel wall stresses, but suggest a possible role for MRI to inform
thrombus material stiffness assignment in stress computations.
Introduction
Abdominal aortic aneurysms (AAA) are common, and their
rupture is often fatal. Much work has focused on assessing rupture risk for
individual patients using finite element wall stress estimations incorporating
aneurysm features from medical imaging, principally computed tomography
(CT). CT cannot resolve the material
heterogeneity of the intraluminal thrombus (ILT) common in larger aneurysms,
and the disparate stiffnesses of distinct thrombus layers, known from specimen
testing, have not been incorporated in a patient-specific fashion. Using a T1-weighted
black-blood fast spin echo acquisition as part of an MRI protocol for comprehensive
AAA evaluation1, we delineate ILT layers in 4 AAA patients and study the effects of explicitly
modeling ILT heterogeneity in stress analyses. Methods
Four AAA patients (cases a-d) undergoing MRI surveillance in an IRB-approved study were
selected for having significant ILT burden with two distinct layers on T1-weighted
black-blood imaging: low signal in thrombus adjacent to the lumen and high
signal closer to the vessel wall (Figure 1, a-d). A 5th case (e) was
selected for uniformly high signal intensity throughout the ILT (Figure 1, e). The geometric boundaries
of different ILT layers were segmented manually from black blood imaging, while
CE-MRA and post-contrast VIBE imaging were used to segment the flow lumen and
vessel wall, resulting in a set of 3-dimensional surfaces that served as the
basis for computational mesh generation. Following a sensitivity analysis, the
AAA wall was meshed with a linear hexahedra dominant scheme. ILT was meshed with
hybrid linear tetrahedra and boundary pyramid elements (Figure 2). The vessel wall and ILT were considered incompressible,
with hyperelastic constitutive relations selected from the literature. The stiffer
luminal ILT was represented by a polynomial strain energy density function
derived from Di Martino and Vorp2, and the weaker abluminal ILT
was represented as an Ogden-type material as derived by Gasser et al3. The specific parameters describing ILT types
were motivated by the work of Riveros et al4, wherein the effects of
different ILT stiffness were considered for uniform thrombus. For cases a-d, ILT was modeled as heterogeneous,
uniformly stiff, and uniformly weak. Case e
with uniform ILT signal intensity considered only stiff or weak thrombus. A
fixed-point iterative technique was used to estimate the unloaded geometry of
each AAA, with subsequent pressurization to 120 mmHg. Vessel displacements at
the inlet and outlets were constrained to be radially oriented. Von Mises
stresses in the AAA were computed using the ABAQUS solver. Results
Example AAA wall stress distributions are shown for case c in Figure 3 and listed for all cases in Figure 4. Explicit modeling of ILT heterogeneity based on MRI had
virtually no effect on peak wall stress compared to the results of models
assuming uniformly stiff ILT. Peak stress location was unchanged for each case,
while the stress magnitude differed by only 6% for case b, and was within 1% for cases a,
c, and d. Average vessel wall stress increased minimally with the
incorporation of ILT heterogeneity when compared to the uniformly stiff ILT
models, reflecting modestly higher stresses in the most dilated aneurysm segments,
where the adjacent weak thrombus layer is thickest. Peak wall stress magnitude increased
by an average 27% (SD = 23%) when thrombus was considered uniformly weak, though
peak stress location was not significantly changed in any case. As an example,
case e is shown in Figure 5.Discussion
MRI has the unique capability to discern heterogeneity within
intraluminal thrombus in AAAs, which has thus been considered homogeneous in
the dominantly CT-based AAA stress analysis literature. Results for cases a-d demonstrate that for the combination of ILT material models
considered, incorporation of MRI-discerned ILT heterogeneity may have little
effect on aneurysm wall stress estimates. This is important, as segmentation and
mesh generation become more complicated and time consuming each time an
additional material boundary is represented in a patient-specific simulation. Eliminating
complexity, when reasonable, can increase simulation throughput, which has
traditionally been limited when considering patient-specific geometries. However,
MRI may help inform the assignment of uniform ILT stiffness in simulations, as
suggested by case e, potentially
improving stress prediction accuracy. This hinges on verification that thrombus
signal intensity is indeed correlated with mechanical stiffness, and work is
ongoing to examine this relationship. As this work considered a small variety
of ILT distributions, further investigation is continuing over a broader set of
geometries and ILT material models. Conclusion
MRI-discerned intraluminal thrombus heterogeneity may have
limited influence in computational AAA wall stress analyses, although further
investigation over a larger set of material models is warranted. Acknowledgements
Work
supported by
the National Institutes of Health (NIBIB) T32 Training Grant, T32EB001631References
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T.C., et al., Failure properties of
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