Yuxi Pang1
1Dept. of Radiology, University of Michigan, Ann Arbor, MI, United States
Synopsis
Collagen fibril microstructural distributions
in articular cartilage are extremely complex. The simplistic two halves radially
segmented cartilage in clinical T2W sagittal knee images may not truly represent histologically
defined deep and superficial zones. Furthermore, the normal to femoral
cartilage surface varies considerably within imaging slices from the lateral to
medial side of knee. Consequently, the standard magic angle effect (MAE)
functions become inadequate for characterizing the observed anisotropic T2W signals in knee cartilage. Thus, a generalized MAE model is presented for better
quantifying anisotropic T2W signals in the clinical studies of human knee
articular cartilage.
INTRODUCTION
Anisotropic transverse relaxation rate, $$$R_2^a(θ)$$$, reportedly possesses the best sensitivity in
detecting cartilage early degenerations.1 Recently, an efficient $$$R_2^a(θ)$$$ measurement method
has been developed, where an internal reference (REF) has to be deduced from T2W
femoral cartilage sagittal images, based on the standard magic angle effect (sMAE)
model.2 Unfortunately, the vast majority of imaging slices can not be adequately characterized due to complex collagen microstructural distributions
and an irregular femoral cartilage surface. This work is thus to propose a
generalized MAE (gMAE) model to better characterize anisotropic T2W signals in human
knee cartilage.METHODS
(1) Theory: Relative to cartilage surface normal, collagen fibers
are respectively in perpendicular, random and parallel orders in the superficial
(SZ), transitional (TZ), and deep (DZ) zones.3-4 Water proton dipolar interactions within collagen fibers are on average along the fiber direction.5 Given a voxel comprising
fibers distributed in an axially symmetric system (Figure 1A), the orientation
dependence of $$$R_2^a(θ)$$$ can be derived by averaging an ensemble of dipolar
interactions associated with differently orientated fibers. A representative
fiber is shown (Figure 1A) forming angle $$$θ$$$ to $$$B_0$$$, and angle $$$α$$$ to cartilage
surface normal ($$$\overrightarrow{n}$$$) that makes angle $$$ε$$$ with $$$B_0$$$. Note, $$$α$$$ and $$$ε$$$ are
stationary but $$$φ$$$ (azimuthal
angle) and $$$θ$$$ become
spatial or time dependent.6 With spherical law of cosines (i.e. $$$\cos\theta=\cos\alpha\cos\epsilon+\sin\alpha\sin\epsilon\cosφ$$$) and after an average over $$$φ$$$ from 0 to 2π, the function $$$⟨(3cos^2θ-1)^2⟩$$$ can be expressed
by Eq. 1, here called the gMAE function.$$f(α,ε)=(1/4)(3cos^2α-1)^2 (3cos^2ε-1)^2+(9/8)(sin^4α sin^4ε+sin^22αsin^22ε) \; (1) $$When $$$α$$$=0°
and 90°, $$$f(α,ε)$$$ returns respectively
to the standard MAE (sMAE) functions of $$$(3cos^2ε-1)^2$$$ and $$$1-3sin^2ε+(27⁄8)sin^4ε$$$ for collagen
fibers in the DZ and SZ.4 (2) T2W MR imaging: T2W sagittal images were acquired from an asymptomatic knee of one consented subject at 3T, using an interleaved MSME
(n=8) TSE sequence and a 16-channel T/R knee coil. Key parameters were listed here: FOV
= 128*128*96 mm3; voxel size = 0.6*0.6*3.0 mm3; Compressed SENSE factor = 2.5; TR = 2500 ms; scan time =7.42 minutes. Only T2W images with TE=48.8
ms were evaluated. A
high-resolution 3D image of the same knee was also acquired (Figure 2).
(3) Modeling MAE in T2W: Femoral cartilage was segmented angularly
and radially following an established protocol2, average signal
intensities ($$$S$$$) from segmented ROIs can be expressed by Eq. 2, $$S=S_0exp\{-(R_2^i+R_2^a*f(α,ε))TE\} \;(2) $$ where $$$S_0, R_2^i, R_2^a$$$ and $$$TE$$$ represent respectively initial signal ($$$TE$$$=0), isotropic and anisotropic $$$R_2$$$, and echo time. In a logarithmic scale, Eq. 2 was
fitted to segmented ROIs, i.e. $$$y(ε)=A-B*f(α,ε)$$$. An independent variable was
$$$ε$$$ and three model parameters were $$$A=(Log S_0-R_2^i TE)$$$, called an REF2; $$$B=R_2^a*TE$$$ and $$$α$$$. For comparison, the fitting using Eq. 2 was named
“Fit A” for both the DZ and SZ data, whereas the fittings were called “Fit B” with $$$α$$$=0 for the DZ
data, and “Fit C” with $$$α$$$=90° for the SZ
data. Goodness of fit was measured by the root-mean-square error (RMSE), and statistical
significant differences were assessed by an F-test, with
significance indicated by P <
.05. All data analysis was performed with in-house software written in IDL 8.5.RESULTS AND DISCUSSION
Figures 1B-D present
respectively four $$$f(α,ε)$$$ profiles with $$$α$$$=0°
(red), 33°(green), 57° (blue) and 90° (black) (B),
two schematic sagittal imaging slices with surface normal vectors $$$\overrightarrow{n}$$$ (red) and $$$\overrightarrow{m}$$$ (green)
making an angle $$$α$$$ (C), and the spatial
distribution of $$$f(α,ε)$$$ when considering
a spherical femoral cartilage containing 11 different fibril microstructural distributions from the innermost ($$$α$$$=0°) to outermost ($$$α$$$=90°) layers. Because of $$$f(α,ε)$$$ symmetry, e.g. $$$f(α,0)$$$=$$$f(0,α)$$$, $$$α$$$ can be interpreted
either as the spread of fiber directions around a preferential orientation
axis (i.e. $$$\overrightarrow{n}$$$) or as the deviation of an orientation axis from $$$B_0$$$ (i.e. $$$\overrightarrow{m}$$$
) when $$$ε$$$=0°.
Figure
2A highlights the curved femoral cartilage surface in a volume-rendered knee
image, and Figure 2B pinpoints the spatial locations on a coronal image of six T2W
sagittal imaging slices, i.e. S13, S09, and S05 from medial side (Figures 3A-C)
and S29, S25, and S20 from lateral side (Figures 4A-C). Clearly, Fit A provided
significantly (P<.01) better fits
for the edged imaging slices when compared with Fit B or Fit C, for instance, for
Slice 05 (Figure 3A) and Slice 29 (Figure 4C) in the DZ, and Slice 20 (Figure 4A)
in the SZ, signifying a curved surface in consistence with theoretical
predictions.
Overall, Fit A significantly
outperformed Fit B (Figure 5A) in the DZ (0.239±0.122 vs. 0.267±0.097, P=.014) and Fit C (Figure 5B) in the SZ
(0.183±0.081 vs. 0.254±0.085, P<.001).
A relatively smaller average angle $$$α$$$ was observed in
the DZ when compared to that in the SZ, i.e. 38.5±34.6° vs. 45.1±30.1°,
P<.43, in good agreement with the
reported fibril microstructural arrangements. Moreover, an REF was
significantly larger when using Fit A (red solid line) in both the DZ (Figure
5C) and the SZ (Figure 5D).
These comparison
results demonstrate that the proposed gMAE function could not only better
characterize anisotropic T2W signals in femoral cartilage but it also provides an REF from both the DZ and SZ cartilage. CONCLUSION
The proposed
generalized MAE model is demonstrated for better characterizing anisotropic T2W signals in the human knee femoral cartilage.Acknowledgements
This work was
in part supported by the Eunice Kennedy Shriver National Institute of Child
Health & Human Development of the National Institutes of Health (NIH) under
Award Number R01HD093626 (to Prof. Riann Palmieri-Smith).References
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