Evan M Masutani1, Joseph Y Cheng2, Marcus T Alley2, Shreyas S Vasanawala2, and Albert Hsiao1
1University of California, San Diego, La Jolla, CA, United States, 2Stanford University, Stanford, CA, United States
Synopsis
We demonstrate a volumetric technique for
calculation and visualization of great vessel wall shear stress (WSS) from 4D
Flow MRI data. Traditional methods for
WSS have relied on planar sections of the data followed by explicit manual
segmentation of vessel boundaries, which can be labor-intensive to
perform. We propose a volumetric
strategy for computation and visualization of WSS, which may facilitate its
clinical translation.
PURPOSE
Wall shear stress is implicated in a variety of cardiovascular
diseases, including atherosclerosis, aortic dissection, and aneurysm formation.1-4 WSS is the drag force per area the
endothelium exerts on luminal fluid. Cellular
mechanotransducers may sense altered shear stress and actuate changes in
vascular cell state.1 It may therefore
be beneficial to routinely evaluate wall shear stress in patients with
cardiovascular disease. 4D Flow MRI has
potential for enabling non-invasive in
vivo measurement of WSS. Previous
work has shown feasibility of calculation of WSS from 4D Flow MRI by
calculating the numerical gradient of velocity at user-defined boundaries.5 Explicit manual demarcation of boundaries is cumbersome
and potentially subjective.6
We present a method for calculation and visualization of WSS without
manual segmentation to enable routine characterization of WSS, building on previous
volumetric techniques.7METHODS
With
HIPAA-compliance and IRB approval, we identified three 4D Flow MRI acquisitions
obtained as part of clinical imaging examinations at our institution. 4D Flow
MRI was performed using a four-point encoded variable-density pseudo-randomly-ordered
Cartesian sequence, followed by iterative compressed-sensing and parallel
imaging reconstruction with respiratory self-navigation previously described.8,9 Calculations of shear stress (τ) throughout the vector field was
performed in MATLAB 2015b, shown in further detail in figure 1. Volumetric visualization was performed using
the Arterys software (Arterys, San Francisco, CA). Spatial resolution ranged
from [1.5-2.08 x 1.4-2.5 x 1.41-1.88 mm].
Temporal resolution ranged from [45 - 76 ms]. Acquisition times ranged from [11 – 13 mins].
We use a previously reported value of 3.2 mPa*sec for blood viscosity.5
Our
primary assumption is that the gradient of velocity at the wall is
approximately equal to the partial derivative of velocity with respect to the
vessel wall unit normal. To reduce
dimensionality to three spatial and one temporal dimensions for visualization,
we compute the gradient of fluid speed using the Sobel operator and approximate
the partial derivative for each dimension.
To emphasize vascular boundaries for visualization, we employed a
similar process for the anatomic 4D Flow data, and computed the Hadamard
product of the signal intensity gradient magnitude and the original intensity
data. RESULTS
We
present three examples of our algorithm to illustrate the ease and
effectiveness of this approach. In a
patient with aortic coarctation with severe stenosis, there is focally elevated
WSS (>250 cPa) along the posterior wall of the distal arch (figure 2). The second example (figure 3) depicts WSS of
the lower thoracic and abdominal aorta in a patient with presumed giant cell arteritis
involving the abdominal aorta. The
abdominal aorta exhibits locally elevated WSS (>200 cPa), due to abdominal
aortic stenosis. In the third example, a
focal right common iliac artery aneurysm demonstrates low WSS (figure 4). Outside of these regions, WSS during
peak-systole is normal, approximately 40-60 cPa along the thoracic aorta and
approximately 30-50 cPa along the abdominal aorta.5,10DISCUSSION
Regions of high and low WSS may contribute to the
formation and evolution of aortic dissection and aneurysm. It has been hypothesized that locally high
WSS may activate WSS-dependent vasodilatory and remodeling mechanisms.1 The case of aortic coarctation presented here
is suggestive that certain sections of the aortic wall may experience a greater
tendency toward remodeling than others.
It is worth noting that our estimates for WSS are similar to “normal” values
reported in the literature.5,10
Our method offers two potential advantages. First, the compressed-sensing 4D Flow
implementation enables collection of higher resolution and higher
signal-to-noise data, which may improve accuracy of estimates of WSS. Second, the implicit display of WSS
eliminates potential mismatch between the fluid velocity boundary and
user-defined boundaries for calculation of WSS. CONCLUSION
We present a novel method to calculate and
visualize WSS from 4D Flow MRI data, utilizing implicit rather than user-defined
boundaries. This may enable greater
accessibility of WSS for potential use in a clinical setting by removing the up-front
need for manual segmentation, thus streamlining the computational process. Future work may include further refinement of
the algorithm to account for vessel contractility, assessment of its
sensitivity to acquired spatial resolution and application of the technique to
study WSS in specific patient populations.Acknowledgements
No acknowledgement found.References
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