Amy R McDowell1, Matthew G Hall1,2, Thorsten Feiweier3, and Chris A Clark1
1GOS UCL Institute of Child Health, London, United Kingdom, 2Medical Radiation Physics, National Physical Laboratory, London, United Kingdom, 3Siemens Healthcare GmbH, Erlangen, Germany
Synopsis
Muscle fibres have a complex hierarchical internal structure
which leads to a marked decrease in the observed MR diffusion coefficient with
diffusion time. We expect the form of this diffusion time dependence to be
highly sensitive to changes in this internal structure. However, characterising
the diffusion time dependence in tissue can be highly demanding of total acquisition
time. We examine the time-dependence of diffusion indices in human calf muscle
in healthy volunteers in a clinically feasible scan time. We find significant
time dependence and diffusion restriction in all directions, including longitudinally,
due to the internal structure of muscle fibres.
Introduction
Muscle fibres are much larger than
white matter axons, a more common area of application of diffusion imaging, and
have a complex hierarchical internal structure1. This is unlike axons which
are usually modelled as empty cylinders. The presence of a hierarchical
structure in muscle leads to a marked decrease in the observed diffusion
coefficient with diffusion time, which has been demonstrated in mice2.
From previous investigations3, we expect the form of this
diffusion time dependence to be highly sensitive to changes in this internal
structure and therefore a good candidate for a probe of microstructural change
due to the action of pathology. However, characterising the diffusion time
dependence in tissue can be highly demanding for total acquisition time. Using
a highly optimised diffusion acquisition protocol, we examine the
time-dependence D(t) of diffusion indices in human calf muscle in healthy
volunteers in a clinically feasible scan time.Methods
Five volunteers were imaged on a 3T
MAGNETOM Prisma scanner (Siemens Healthcare, Erlangen, Germany) using a
15-channel knee coil. Volunteers were positioned with their right calf in the
centre of the coil. Diffusion data were acquired with a prototype sequence
using echo-planar imaging and
a stimulated-echo (STEAM)
preparation with pulse duration (δ)
10ms at 5 different diffusion times (Δ)
of 70, 130, 190, 250, 330ms each acquiring 6 directions (orthogonal x, y, and z
and diagonal xy, xz, and yz) at b-values of 0, 200, 400,
600, and 800 s/mm2. Acquisition
time per Δ value
was 7:03 mins with a total acquisition time of 35:15mins. Voxel size was 2x2 mm2
with a slice thickness of 3 mm, and a TE and TR of 50ms and 2800ms,
respectively, with Spectral Attenuated Inversion Recovery (SPAIR) fat suppression. Data were pre-processed using Tractor [http://www tractor-mri.org.uk/] and tensor fitting was performed at each diffusion time using FSL [https://fsl.fmrib.ox.ac.uk/fsl/fslwiki/] using a weighted least-squares fit. Regions of
interest in the tibialis anterior (Figure 1) were drawn on the MD images reconstructed
at the shortest diffusion time. MD, FA and principle eigenvectors were analysed
in each voxel of interest. Angular dispersion of eigenvectors was calculated
relative to the spherical mean of all directions in the ROI using the dot
product. Statistical
analysis was performed using two-tailed unpaired t-tests. A two-point Dixon sequence (TE 73ms, TR 3500ms, voxel size 0.36x0.36mm2
with slice thickness of 3mm) was also acquired to provide anatomical images.Results
Example fat, water, B0, MD and FA images
from one volunteer are shown in Figure 2. The B0 image shows good delineation
of the muscle groups with acceptable distortion, though incomplete fat
suppression. Quantitative results are shown in Figure 3. The mean MD decreases
from 130.5 x 10-5mm2/s at Δ=70ms
to 107.6 x 10-5mm2/s at Δ=330
ms. Mean FA increases from 0.31 at Δ=70
ms to 0.40 at Δ=330ms.
Significance between the minimum and maximum diffusion times was P<0.0001
for MD and P<0.0004 for FA.
Angular dispersion of eigenvectors
was calculated relative to the spherical mean of all directions in the ROI
using the dot product and is shown in Figure 4. We observe a
mean
angular deviation of 13.3 degrees (standard deviation (SD) 6.31 degrees) at Δ=70
ms and of 12.32 degrees (SD 5.34 degrees) at Δ=330 ms. There was no significant difference in angular dispersion between these two diffusion times (P=0.62).Discussion/Conclusion
We have acquired time-dependent
diffusion in muscle in a clinically feasible scan time. Mean diffusivity shows
a strong time dependence, decreasing with diffusion time, which is in agreement
with the results found by Porcari et al2
in mice. Results show restriction in all three directions, including longitudinally
which is due to the hierarchical internal structure of muscle fibres.
Fractional anisotropy also shows a distinct increase with diffusion time, which
follows from the differing rates of reduction in λ1, λ2,
and λ3.
We expect this protocol to be a useful
marker of microstructural change and pathology in such diseases as muscular
dystrophy which can affect size, packing fraction and permeability of muscle
fibres.Acknowledgements
MGH and AM are supported in part by a grant from Great Ormond St Hospital’s Biomedical Research Centre. AM is also supported by a grant from theNational Physical Laboratory.References
1. Feher
J. Contractile Mechanisms in Skeletal Muscle. 2nd Edition Elsevier; 2017.
2. Porcari P, Hall MG, Clark CA, Greally
E, Straub V, Blamire AM. The effects of ageing on mouse muscle microstructure:
a comparative study of time-dependent diffusion MRI and histological
assessment. NMR in biomedicine 2018; 31(3).
3. Marschar AM,
Kuder TA, Stieltjes B, Nagel AM, Bachert P, Laun FB. In vivo imaging of the time-dependent apparent
diffusional kurtosis in the human calf muscle. Journal of magnetic resonance imaging : JMRI 2015; 41(6): 1581-90.