Runyu Yang1, yuze li1, and Huijun Chen1
1Center for Biomedical Imaging Research, Tsinghua University, Beijing, China
Synopsis
The
rupture of intracranial atherosclerotic plaque is a major cause of ischemic
stroke. The atherosclerotic plaque burden was proposed to measure the risk of
plaque vulnerability, which can be quantified by the volume of the vessel wall
calculated on MR images. However, due to the complex shape of intracranial
blood vessels, the traditional calculation method may reduce the accuracy of
plaque burden measurement,especially
overlapped in the curved vessels. Therefore, a tetrahedral based method was proposed
to reduce the volume calculation error of intracranial vessel wall. The
proposed method was validated in simulation and in-vivo datasets.
Introduction
Intracranial atherosclerotic disease (ICAD) is a
major cause of ischemic stroke worldwide and an important public health concern
globally1-5. The rupture of intracranial atherosclerotic plaque is a major
cause of ischemic stroke. The atherosclerotic plaque burden was proposed
to measure the risk of plaque vulnerability6, which can be
quantified by the volume of the vessel wall calculated on MR images. However,
due to the large curvature of intracranial blood vessels, the traditional
calculation method, i.e., image slice thickness multiplies the vessel area, may
cause the overlap when the slice thickness is larger than the radius of curvature,
thus reducing the accuracy of plaque burden measurement. Therefore, in this
study a tetrahedral based method was proposed to reduce the
volume calculation error by reconstructing the vessel into lots of small tetrahedron
and summing the volume of them. The performance of the proposed method was
validated in simulation and in-vivo datasets.Method
Volume Calculation
In
the traditional volume calculation method, the central line of the vessel was
first obtained, and then the lumen and outer wall of the vessel were delineated
with a series of points in the vessel cross-section. The vessel area can be
calculated using these delineated points. Finally, the vessel volume was
obtained by multiplying the vessel area in the cross-section and the slice
thickness7-9. After
getting the delineated points, order f(v) represents
the connection function of two adjacent blood vessel:
$${\rm{F}} = \mathop{{\int\!\!\!\!\!\int\!\!\!\!\!\int}\mkern-31.2mu \bigodot}\nolimits_\Omega {f(v)dV} $$
$$v \in \Omega ,Bv = g$$
v is the boundary control point delineating the
vascular region, Ω is the set of control points , g is the boundary function for the two
adjacent slices. The solution of F with respect to the boundary condition g can be solved by partial differential
equations. Finite element analysis is often used to solve discrete partial
differential equations10. Finite element method divides the computational domain into finite
non-overlapping elements, and select some appropriate nodes as interpolation
points of the solution function in each element. In three dimensions, F can be
expressed as the sum of the volumes of the tetrahedron. The whole workflow as shown in FIG.1.
Simulation and In-vivo Experiments
The simulation experiment
was performed to validate the proposed method (Fig. 2). We designed the
different regular shapes (Sim. a and b) to simulate the vessel lumen and outer
wall, which the volume can be calculated analytically as the golden standard. Furthermore,
we simulated some vessels under different stenosis conditions (Sim. c and d).
In the in-vivo
experiment, with the approval of institutional review board, three patients
with intracranial arterial stenosis underwent the black-blood T1-weighted VISTA
(volume isotropic turbo spin echo acquisition, VISTA) sequence with the spatial
resolution of 0.6 mm isotropic on a 3T scanner (Achieva CX, Philips Healthcare,
The Netherlands). For each subject, lumen and outer wall were outlined manually
on the vessel cross-sections using an in-house software.
Results
As shown in Table
1, in simulation dataset the proposed method achieved less volume calculation error
than the traditional methods in regular shapes (Sim. a-b). In practice, the
shape of intracranial blood vessels is more complex, so we took more attention
to the simulation of curved blood vessels. The proposed method still had less errors
than the traditional method (Sim. c-d).
In in-vivo
experiment, the proposed method can accurately reconstruct the shape of
intracranial blood vessels. Reconstructed vessel lumen and outer walls are shown
in Fig.3. Visually, the result of the traditional method was the rough approximation
for the real condition, while the proposed method can reflect the shape of real
blood vessels.
Quantitative results of in-vivo datasets are
shown in Table 2. The volume of lumen showed the larger difference between two
methods, thus resulting in the vessel wall volume calculation.Discussion and Conclusions
A novel
tetrahedral based volume calculation method was introduced. The proposed approach has an improved accuracy for vessel wall volume calculation, validated in the simulation and in-vivo datasets.Acknowledgements
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