Felix C Horn 1 and Jim M Wild1
1University of Sheffield, Sheffield, United Kingdom
Synopsis
Single breath washout (SBW) is a whole lung pulmonary function test that
has been shown to be sensitive to early changes in lung disease. Of particular clinical interest has been the
Phase III slope (SIII) as the concentration decay between 25-75% of the
exhaled volume.
In this work rapid lung imaging of exhaled hyperpolarized gas is used to
acquire 2D images of SBW of subjects expiring to residual lung volume. The ability to calculate regional SIII from those time resolved
images is demonstrated in healthy volunteers.
Purpose
Single breath washout
(SBW) is a whole lung pulmonary function test that has been shown to be
sensitive to early changes in lung disease1. Of particular clinical interest has been the Phase III slope (SIII)
as the concentration decay between 25-75% of the exhaled volume. Commonly nitrogen
is used as tracer gas, but SBW can also be performed with Helium. In this work
rapid lung imaging of exhaled hyperpolarized gas is used to acquire 2D images of
SBW of subjects expiring to residual lung volume. We demonstrate the ability to
measure regional SIII slopes from time resolved images.
Methods
Single breath washout imaging
(SBW-I) was performed on a 1.5T scanner with a quadrature flex coil tuned to
Helium-3 frequency. A gas mixture of Helium-3 (~30% polarisation,100ml) topped
up to one liter with N
2 was inhaled. Sequence parameters of the time resolved 2D spoiled gradient
echo sequence were: 64x64 Matrix, a single slice with thickness = 300mm, FOV=
38cm, TR/TE = 2.7/0.8ms, receiver bandwidth=62.5kHz, phase FOV = 0.82, flip
angle = 1°. A total of 80 images
were acquired with no delay between acquisitions, resulting in a total
breath-hold of 15s. Subjects were instructed to exhale to functional residual
capacity before inhaling the 1l of tracer gas mix as per SBW lung function test
2-4. Upon inhalation data
acquisition was started and subjects aimed for a constant flow of 400ml/s
breathing through a restricted flow meter
5 (RS 100 Pneumotachograph,
Hans Rudolph Shawnee, KS, USA).
Images were corrected for RF depolarisation and registered for
lung motion6. Flow recordings were interpolated and aligned with the timings
of the MRI acquisition (Figure1). MRI images were converted into maps of regional gas fraction
7. This allowed
quantification of SIII slope in %/liters as commonly expressed for
the SBW test in the pulmonary function lab. SIII was calculated as
the linear slope of fractional signal decay per liter expired volume between
25%-75% of the exhaled volume
5.
Single breath washout imaging (SBW-I) was performed in two healthy
subjects. One subject was imaged twice to show repeatability of the imaging
method using a coronal and a sagittal whole lung projection.
Results
A representative time series of exhaled gas SBW-I is shown in Figure 2. Single breath washout integrated over the whole lung alongside signal from
the trachea is shown in Figure 3. In addition Figure 4 shows maps of S
III
slopes from both subjects SBW-I.
Data were shown to be highly reproducible (Subject 2: S
III
mean(standard deviation) (1) -0.142(0.084) (2) -0.148(0.084)). The whole lung
average values from both volunteers (Subject 1 S
III= -0.15; Subject 2 S
III=
-0.22) are in the range of those in the literature for the SBW lung function
test for sitting healthy subjects using a similar breathing manoeuvre albeit with
slightly lower Helium concentration: 0.2(0.06)3.
In the sagittal S
III map from subject 2 a gravitational
effect with an increase of slope from anterior to posterior can be observed
which reflects the postural gradient in ventilation observed in static
ventilation imaging and multi breath washout imaging
8.
Discussion
The mean average S
III
values from both volunteers matches the literature and a good repeatability was
demonstrated when imaging the same subject twice. The well-known gravitational
effect
9 was also found in the S
III indicating a faster concentration decay in the posterior part
of the lung compared to the anterior one.
Expiration was shorter than 8s in both cases, with a T
1 in the range of 25-30s
signal depolarisation from T
1 decay was therefore neglected in this preliminary work. Rapid
signal decay in the trachea shows quick washout of the dead space gas similar
to SBW in the PFT (Figure 3). However the dead space signal (Figure 1,DS) is
difficult to fully assess using SBW-imaging, as only parts of the trachea were visible
at the edge of the FOV. This could be addressed with a larger FOV and a coil
that covers the upper airways. In the rest of the lung signal decay is
dominated by gas washout from the respiratory zone of the lung (small airways
and alveolar gas space; airway generation >16) rather than the conducting
zone.
In future work acceleration techniques like parallel imaging and
compressed sensing could be used to allow imaging with a higher temporal
resolution or to increase the spatial resolution of images to 3D.
Conclusion
Regional Phase III slope (S
III) mapping from single breath washout
imaging of hyperpolarized gas is demonstrated. Future work could investigate
how regional distribution in Phase III slope changes in disease and compare it
to ventilation imaging and fractional ventilation from multiple breath washout.
Acknowledgements
The authors would like to acknowledge Laurie Smith for useful discussions and help with experiments. References
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