Fuchang Jiang1, Bhumi Bhusal2, Bach Nguyen2, Michael Monge3, Gregory Webster4, Daniel Kim2, Giorgio Bonmassar5, Andrada R. Popsecu6, and Laleh Golestanirad1,2
1Department of Biomedical Engineering, McCormick School of Engineering, Northwestern University, Evanston, IL, United States, 2Department of Radiology, Feinberg School of Medicine, Northwestern University, Chicago, IL, United States, 3Division of Cardiovascular-Thoracic Surgery, Ann & Robert H. Lurie Children's Hospital of Chicago, Chicago, IL, United States, 4Division of Cardiology, Ann & Robert H. Lurie Children's Hospital of Chicago, Chicago, IL, United States, 5A. A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Boston, MA, United States, 6Division of Medical Imaging, Ann & Robert H. Lurie Children’s Hospital of Chicago, Chicago, IL, United States
Synopsis
Infants with congenital
heart defects, inherited arrhythmia syndromes, and congenital disorders of
cardiac conduction often require cardiac implantable electronic devices
(CIEDs). Some infants receive a CIED within hours, or even minutes, of birth. The
presence of an epicardial CIED is a relative contraindication for cardiac
magnetic resonance imaging (MRI) due to the risk of RF heating. We present
results of phantom experiments and electromagnetic simulations showing that a
simple surgical modification in the trajectory of epicardial leads can reduce
RF heating more than 40-fold during MRI at 1.5 T.
Introduction
Congenital heart defects (CHD) are the most
common type of birth defect in the United States, affecting 1 in every 100
babies born per year 1. Infants with CHD often require cardiac implantable electronic
devices (CIEDs), some implanted within hours, or minutes, from birth 2. The optimal approach to affixing a CIED to the heart of a young
patient is to open the chest and sew the cardiac lead directly to the
myocardium (“epicardial leads”) as opposed to passing it through veins and
affix to the inside of the heart (“endocardial leads”). Unfortunately, once
epicardial leads are implanted, the risk of RF heating results in a relative
contraindication to MRI, which inhibits optimal imaging in young people 3. Here, we show that
a simple surgical modification in the trajectory of epicardial leads can
substantially reduce RF heating during MRI at 1.5 T. We designed and
constructed a multi-material anthropomorphic pediatric phantom based on
segmented MR images of a 29-months-old child and measured temperature rise ΔT
at the tip of an implanted epicardial
CIED during RF exposure at 1.5 T. We found that ΔT could be reduced on average by 40-fold when
the epicardial lead looped was placed on the inferior surface of the heart as
opposed to the anterior surface of the heart. Electromagnetic simulations confirmed
the experimental results, showing that the coupling between MRI electric fields
and implanted leads was substantially reduced in the case of inferior loop
compared to an anterior loop. The results were robust against perturbations in
lead positioning, suggesting that a simple easy-to-implement surgical
modification can lead to a significant and reliable increase in MRI safety. Methods
Phantom
experiments
We designed, and 3D printed a pediatric
phantom consisting of a human-shaped container, skull, rib cage, and heart,
based on MR images of a 29-month-old child (Figure 1). A Medtronic Azure™ XT DR
MRI SureScan pulse generator was connected to a 35 cm epicardial lead
(Medtronic CapSure® EPI 4965) and placed in the phantom's abdomen approximately
10 cm caudal to the center of the heart, in a typical position for epicardial
pulse generators. Fiber optic temperature probes (OSENSA,
Vancouver BC, Canada) were secured at the tip of the lead using threads (Figure
1G). The lead electrode was
fixed to the surface of the heart phantom in a position analogous to the right
atrial epicardium. RF heating was measured
during 453 seconds of scanning with a high-SAR T1-TSE sequence (TE=7.3
ms, TR= 814 ms, B1+rms= 4.13μT).
We investigated two distinct lead
trajectories. In the first, the excess length of the lead was looped on the
inferior surface of the heart (Figure 2B). In the second, the loop was placed
on the anterior surface of the heart. Both techniques are used in pediatric surgical
practice. To assess the sensitivity of results to variations in setup, each
trajectory was implanted three times with small perturbations in the loop
diameter and position (Figure 2A).
Electromagnetic
simulations
Electromagnetic
simulations were implemented in ANSYS Electronics Desktop 2020 R2 (ANSYS Inc.,
Canonsburg, PA) with the same body model that was used to create the phantom
(Figure 3A). The lead was modeled as a 35-cm insulated wire with a
semi-sphere exposed tip positioned on the surface of the right atrium (Figure 3B).
The body+CIED model was placed inside a shielded RF body coil with dimensions
mimicking that of the Siemens 1.5 T Aera system. The maximum of 0.1g-averaged
SAR around the lead's tip was recorded for each trajectory, for the input power
of the coil adjusted to produce a mean B1+= 2μT on an axial plane (a common RF
power limit for scanning in the presence of electronic implants). Results
The measured temperature rise at the tip of
the lead was 5.53±0.95 °C for trajectories with the excess loop placed on the anterior
surface of the heart, compared to 0.14±0.03 °C for trajectories with the excess loop on the inferior surface of
the heart showing a 40-fold reduction in RF heating (Figure 4). Simulations confirmed
a substantial reduction in 0.1g-averaged SAR from 107 W/kg for loop
on the anterior surface to 9 W/kg for the loop on the inferior
surface of the heart.Discussion and Conclusion
Excessive tissue heating is the primary
reason preventing patients with conductive implants from receiving MRI exams,
especially those with elongated leads that are part of cardiovascular or
neuromodulation devices. It is well established that the trajectory of an
implanted lead and its orientation with respect to MRI electric fields substantially
affects the RF heating 4, 5. The idea that the lead trajectory
can be manipulated to potentially reduce RF heating was originally suggested
for neuromodulation devices 6 and recently proved promising in
patients with deep brain stimulation devices 7. Here we demonstrated that this simple
yet highly effective technique could be adopted in children with epicardial
leads to substantially reduce the risk of RF heating of the device during MRI
at 1.5 T in a pediatric phantom model. If validated in biological systems,
these mapping techniques could have a substantial impact on surgical technique
and pre-surgical planning.Acknowledgements
Disclosures
This work was supported, in part, by
in-kind lead donations from the Medtronic Corporation (Minneapolis, MN). K23HL130554
supported Dr. Webster.
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