Arnd Jonathan Obert1,2, Marcel Gutberlet1,2, Agilo Luitger Kern1,2, Frank Wacker1,2, and Jens Vogel-Claussen1,2
1Institute of Diagnostic and Interventional Radiology, Hannover Medical School, Hannover, Germany, 2Biomedical Research in Endstage and Obstructive Lung Disease Hannover (BREATH), German Center for Lung Research (DZL), Hannover, Germany
Synopsis
Since Perfluoropropane is
highly inert, and can be mixed with oxygen, patients can inhale up to 30 liters
of gas during one examination without a significant physiological impact. This
enables detailed measurements of gas wash-in dynamics using 19F magnetic
resonance imaging.
In this work,
an experimental setup for volume-controlled imaging of multiple breath-holds is
realized using a pneumotachometer and pneumatic valves as well as MR triggering.
In three healthy volunteers, the
stability of the breathing
volumes and the positions of the diaphragm, as well as the standard deviation
of wash-in times, were analyzed comparing volume-controlled to non-controlled
scans.
Introduction
Due to the low spin density of
gaseous Perfluoropropane (PFP) and the limited acquisition time of one breath-hold
in pulmonary imaging, 19F magnetic resonance (MR) lung imaging naturally lacks
high signal-to-noise ratio (SNR). However, since PFP is highly inert, has a low
solubility in blood and water, and can be mixed with oxygen without degrading
the 19F MR signal, patients can inhale up to 30 liters of gas during one
examination1. This
enables detailed measurements of gas wash-in dynamics in consecutive breath-holds2,3.
Previous work on the
experimental setup focused on the patient’s safety monitoring, automated gas
delivery and the assessment of the inhaled gas volume4.
However, to improve inter- and
intra-patient comparability, the patient’s breathing volume must be controlled
over the whole exam, ensuring a fixed value proportional to the patient’s forced
vital capacity (FVC)5.
Furthermore, fitting algorithms describing the voxel-wise wash-in dynamics benefit
from a constant position of the diaphragm. Therefore, the purpose of this work
was to develop an experimental setup for volume-controlled fluorinated gas
wash-in measurements using 19F MRI.Methods
In this preliminary study, three
healthy volunteers were examined on a 1.5 T scanner (MAGNETOM Avanto, Siemens
Healthcare, Erlangen, Germany). The study participants inhaled a mixture of 79%
fluorinated gas (PFP) and 21% oxygen while being monitored by a physician. During
eight consecutive inspiratory breath-holds (duration of 6 seconds each), 19F
pulmonary gas MR imaging was performed using a transmit and 16 channel receive
coil dedicated to the 19F frequency (RAPID Biomedical, Rimpar, Germany) and a custom-made
3D gradient echo pulse sequence with a golden-angle stack-of-stars k-space
encoding. Imaging parameters are shown in Table 1.
The breathing volume was fixed
to 1/8 FVC using a pneumotachometer and a pneumatic valve integrated into the
gas tubing. MR scans were triggered exactly when the desired gas volume was
inhaled using a real-time assessment of the inhaled gas flow. Figure 1 shows a
schematic representation of the experimental setup.
The whole procedure was
repeated without volume control for comparison. Lung function testing was
performed prior to the MR scan to determine the FVC.
A generalized parallel imaging
and compressed sensing (PICS) reconstruction from the BART toolbox6, minimizing
the total variation in the spatial (λs = 0.0001) and the temporal
domain (λt = 0.01), is used to reconstruct images from all breath-holds
jointly.
The position of the diaphragm
in each breath-hold was measured as the vertical difference compared to the
last breath-hold in a central slice.
Wash-in time (TW)
maps were computed by fitting the signal intensity of the time points for each
voxel inside the lung to a monoexponential model:
$$I(t) \propto 1- \exp\left(-t/T_W\right)$$
Here, the sum of squared residuals
of the fit and the standard deviation of TW over the whole lung were
measured.Results
All participants underwent the MR imaging examinations without any
adverse effects, discomfort or stress. The volume control and the trigger for
the sequence worked reliably.
The mean SNR for the first breath-hold in all participants was 6.0 with
volume control and 5.9 without and for the 8th breath-hold 10.3 with
volume control and 10.0 without. SNR was calculated using Kellman’s method7.
The breathing volume and the position of the diaphragm were more stable
when using the volume control. Figure 2 shows the comparison of integrated
inspiratory flow for one subject and Figure 4(a) shows the mean difference in
the vertical position of the diaphragm for all subjects.
Figure 3 shows TW maps for one subject achieved with volume control (a)
and without (b). The standard deviation of TW and the sum of squared residuals were
lower in volume-controlled scans. Figure 4(b) and (c) shows the comparison of the
standard deviation and the sum of squared residuals for all subjects.Discussion and Conclusion
The comparison of the
breathing volume and position of the diaphragm indicates, that the given method
could align the breathing volumes in multiple breath-holds. The reduction of
the standard deviation of TW and the sum of squared residuals in the
wash-in fit may suggest, that the monoexponential model fits better with the
data when the breathing volume is controlled.
The presented experimental
setup enables potentially reproducible and comparable measurements of pulmonary
gas wash-in dynamics with 19F MRI.Acknowledgements
This work was funded by the
German Center for Lung Research (DZL). Furthermore, the authors thank Robert
Grimm for support in sequence programming, as well as Lea Behrendt, Christoph
Czerner, Tawfik Moher Alsady, Melanie Pfeifer and Frank Schröder for
experimental assistance.References
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