Jessica A. Martinez 1,2, Volkan Acikel3, and Daniel B. Ennis4,5,6
1Radiological Sciences, Stanford University, Stanford, CA, United States, 2Radiological Sciences, UCLA, Los Angeles, CA, United States, 3UCLA, Los Angeles, CA, United States, 4Stanford University, Stanford, CA, United States, 5Division of Radiology, Veteran Affairs Health Care System, Palo Alto, CA, United States, 6Stanford University, Cardiovascular Institute, Palo Alto, CA, United States
Synopsis
In situ RF-induced lead-tip heating was compared for cadavers with
previously implanted cardiac-AIMDs to the same AIMDs positioned in the ASTM
phantom following an identical lead path at 1.5T
Introduction
Patients with MR-unsafe cardiac active
implantable medical devices (AIMDs) that undergo an MRI exam are susceptible to
RF-induced lead-tip heating (LTH) risks. LTH depends on many parameters including
the RF-electric field magnitude and phase, tissue conductivity, body shape, distance
to isocenter, and the cardiac AIMD lead path and construction. The American
Society for Testing and Materials (ASTM) testing method (F2182−11a) [1] outlines LTH
tests in a homogeneous tissue-mimicking phantom that corresponds to the
worst-case device configuration. However, little is known regarding the
correspondence of LTH following the ASTM method compared to LTH in the human
body. The objective of this work was
to compare directly LTH in cadavers with previously implanted cardiac-AIMDs to
the same AIMDs positioned in the ASTM phantom following an identical lead path. Methods
LTH was evaluated in two setups at 1.5T
(Siemens Avanto Fit). The first setup corresponded to an in situ configuration. LTH analysis was performed for three human
cadavers (N=3) with previously implanted MR-unsafe cardiac AIMDs (Table 1). The
second setup corresponded to an in vitro
configuration where the in situ lead-paths
were 3-D printed and placed in the ASTM phantom.
In
situ experiments
In
situ LTH data was
acquired using fluoroptic
temperature probes (Lumasense Technologies). Probes were positioned <4.5mm
from the lead-tip under x-ray guidance (Artis Zeego, Siemens). Thermal data was
recorded during 5 minutes of maximum applied RF (whole-body SAR ≤4 W/kg). LTH as
a function of the distance to isocenter was analyzed by placing the cadavers at
five isocenter positions (Landmarks, LMc). The
first landmark (LM1c) was 6 cm superior to the chin. The subsequent landmarks
(LM2c-LM5c) were in 15cm increments inferior to LM1c
(Figure 1-A).
In
vitro experiments
LTH experiments were repeated in an in vitro setup. After device
extraction, the cardiac AIMD was placed in the ASTM phantom filled with a saline gel with electrical
conductivity of 0.47S/m. To ensure that both in situ and
in vitro experiments maintained the
same lead path, the pulse generator position and lead paths were rendered from each
cadaver CT scans (OsiriX, Pixmeo SARL) and used to create 3D-printed scaffolds
to secure each device within the ASTM phantom (Figure 1-B). The temperature probes were placed at 2mm
from the lead tip in a tip-to-tip configuration. LTH as a function of the
distance to isocenter was analyzed by placing the phantom at nine landmarks
(LMP) (whole-body
SAR ≤4 W/kg, 5 minutes). The first landmark (LM1p) was at
the center of the ASTM phantom’s head. The following landmarks (LM2p-LM9p)
were in 9cm increments inferior to LM1p (Figure 1-B).
For both
in situ and in vitro studies, the maximum
observed LTH (LTHmax) during the application of the RF-pulse was
compared at all landmarks. Linear interpolation of LTHmax at each LMP
was used to compare to LTHmax at each LMc. Results
Figure 2
shows LTHmax observed for both in
situ and in vitro experiments as
a function of landmark. As expected, the results suggest that LTHmax depends on both the lead-path and landmark. For the three analyzed lead-paths,
a similar heating pattern was observed for both in situ and in vitro configurations. LTHmax
was observed to increase when the lead tip was closer to isocenter. Greater LTHmax
was observed at landmarks LM2C and LM3C.
A
comparison of LTHmax for both configurations is shown in Figure 3. For
the in situ configuration, only 1/19 (5.2%)
measurements exceeded 2C. On the other hand, 13/36 (36.1%) measurements
exceeded 2C for the in vitro configuration.
Hence, LTHmax was observed to be greater for the in vitro configuration
compared to the in situ configuration
for Lead-Path I (3.9C vs. 2.4C, LM2C), Lead-Path II (4.1C vs. 1.3C,
LM3C) and Lead-Path III (RV:3.8C vs. 0.5C; RA:1.8C vs.0.4C, LM3C).
In general, there was no scenario in which LTH was observed to be greater for
the in situ configuration compared to
the in vitro configuration.Discussion
The analysis of RF-induced
heating is often performed as indicated by the ASTM standard. This describes the
analysis of RF-induced heating under well-controlled conditions that should represent
an upper limit for RF-induced lead-tip heating. Results here suggest that the
analysis of RF-induced heating for MR-unsafe cardiac AIMDs following a
realistic path can induce greater temperature increase compared to an in situ
configuration. Therefore, the data herein suggests that RF-heating analysis using
the ASTM testing standard and phantom at 1.5T provides an upper limit on the
heat that may be expected in situ. In particular, as there is no tissue
perfusion for the in situ cadaver experiments, it is expected that
lead-tip heat would lower in vivo.Conclusion
RF-induced heating analysis
for an in vitro configuration following the ASTM testing standard at
1.5T shows greater heating than in situ configuration. Acknowledgements
This work was supported
by NIH/NHLBI R21 HL127433 and the UCLA Donated Body Program. References
1. ASTM International. F2182-19 Standard Test Method for Measurement of Radio Frequency Induced Heating On or Near Passive Implants During Magnetic Resonance Imaging. West Conshohocken, PA; ASTM International, 2019. doi: https://doi-org.stanford.idm.oclc.org/10.1520/F2182-19