Faisal Fakhouri1,2, Stephan Kannengiesser3, Josef Pfeuffer3, and Arunark Kolipaka1,2
1Department of Biomedical Engineering, The Ohio State University, Columbus, OH, United States, 2Department of Radiology, The Ohio State University, Wexner Medical Center, Columbus, OH, United States, 3MR Application Development, Siemens Healthcare GmbH, Erlangen, Germany
Synopsis
Lung stiffness is altered in many diseases making it an important
biomarker of understanding lung mechanics. Many patients struggle to hold their
breath during scanning due to shortness of breath. We have developed a
free-breathing spin-echo-spiral magnetic resonance elastography (MRE) sequence,
and a feasibility study was performed on 5 healthy volunteers. It was found that the shear
stiffness of the lung during normal breathing was 1.9±0.51kPa and 8.87±1.44kPa with and without considering
lung density correction, respectively. Also the measurements were repeatable
and reproducible.
Introduction
Lung diseases alter mechanical properties of the lung
parenchyma making it an important parameter to understand1. The changes in
mechanical properties such as stiffness of the lungs play an important role in
patients’ ability to breathe properly. Due to the altered functionality of the
diseased lung, patients often have limitations in holding their breath. Several
studies have shown the feasibility of magnetic resonance elastography (MRE) to
quantify the shear stiffness of the lungs during breathhold at residual volume
(RV) and total lung capacity (TLC)1–3. However, a
breathhold might be very challenging for lung disease patients. The aim of this
study was to investigate the feasibility of quantifying lung’s shear stiffness
by using MRE under free breathing and demonstrate the repeatability and
reproducibility of the measurements.Methods
Five healthy volunteers (4 males and 1 female,
26.6±3.3 years old) were scanned using an approved IRB. Lung MRE scans covering
the entire right lung were performed using a Spin-Echo Dual-Density Spiral
(SE-DDS) sequence (Figure 1) in a 1.5T MR scanner (MAGNETOM Aera, Siemens
Healthcare, Erlangen, Germany). Mechanical vibrations (Resoundant Inc,
Rochester, MN, USA) of 50Hz were introduced into the lung. The SE-DDS sequence
was used due to its robustness to motion and short TE. With a TR of 1020ms and
10 spiral interleaves, the scan time was 1:30 minute for each motion-encoding
direction (i.e. X, Y, Z). Depending on the size of the lung, 10 to 16 transverse
slices were acquired with a thickness of 10mm. All scans were acquired during
free breathing without the use of respiratory navigators and without the need
of noble gas. The scan parameters included FOV of 45x45cm2,
acquisition matrix of 128x128, and TE of 6.8ms. As shown in figure 1, two
unipolar MEGs were placed around the 180° refocusing pulse with a period of
2.275ms (i.e. fractional encoding with a frequency of 220Hz combined) to
achieve minimum possible TE. In addition, the MEGs were used as crushers for
the 180° refocusing pulse to further reduce the TE and avoid stimulated echoes.
Scans were repeated with inverted MEG polarity for phase-difference
calculations. To avoid motion/swirling artifacts that appear in spiral
acquisition, a dual-density spiral was used in which the center of k-space was
fully sampled, and the edges were under-sampled by a factor of four4. Additionally, non-Cartesian SPIRiT image reconstruction was used instead
of non-uniform Fourier transform to further reduce spiral motion/swirling
artifacts5. 4 out of 5
volunteers went through a repeatability study and 3 out of 5 went through a
reproducibility study. For the repeatability study, MRE scans were performed
back to back without moving the subject. And for the reproducibility study, the
subjects were asked to step out of the scanner room and were repositioned for a
second scan.
Lung density (LD) estimation scans were performed by
using a GRE sequence to estimate the lung’s stiffness3,6,7. LD scans
involved four acquisitions with different TEs of 0.98, 1.28, 1.58, and 1.88ms
to calculate T2* decay from which LD was
estimated as described elsewhere3,6,7. Since LD changes
during the respiratory cycle, and to match the free-breathing MRE measurements,
which is an average signal across the respiratory cycle, LD scans were
performed at the mid-point of the respiratory cycle under a 16-seconds breathhold. Lung shear stiffness was
calculated by using the 2D direct inversion algorithm (MRElab software, Mayo
Clinic, Rochester, Minnesota, USA)8.Results
Figure 2 shows example
magnitude images, 4 snapshots of wave images, and a stiffness map of the right
lung. The wave images demonstrate excellent wave propagation during free
breathing without any artifacts in the lungs. The stiffness map shows a mean
shear stiffness of 1.21±0.48kPa for the whole lung after considering LD in this
particular volunteer. The mean shear stiffness value for the whole right lung
for all of the 5 volunteers was 1.9±0.51kPa and 8.87±1.44kPa with and without considering
LD correction, respectively. Figure 3 shows Bland-Altman analysis demonstrating
the repeatability and reproducibility of measurements obtained using the SS-DDS
MRE sequence with low mean bias and a narrow confidence interval (repeatability:
Bias = 0.01kPa; 95% CI from -0.39kPa to 0.40kPa; reproducibility: Bias = 0.29kPa; 95% CI from -0.05kPa to 0.62kPa).Discussion and Conclusion
This study demonstrated the feasibility of
free-breathing MRE of the lungs for the first time. MRE-derived stiffness
during free breathing was 1.9±0.51kPa and 8.87±1.44kPa with and without considering LD correction, respectively.
Furthermore, this study showed good reproducibility and repeatability of the
stiffness measurements under free breathing. Further studies are warranted in
different disease states also to establish baseline stiffness values in healthy
volunteers.Acknowledgements
We thank Department of
Biomedical Technology, King Saud University, Riyadh, Kingdom of Saudi Arabia,
for providing scholarship to F.Fakhouri and NIH-R01HL124096 for funding.References
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