Agazi Samuel Tesfai1, Simon Reiss1, Thomas Lottner1, Andreas Vollmer2, Michael Bock1, and Ali Caglar Özen 1
1Dept. of Radiology, Medical Physics, Medical Center – University of Freiburg, Faculty of Medicine, University of Freiburg, Freiburg, Germany, 2Department of Oral and Craniomaxillofacial Surgery, Center for Dental Medicine, University Medical Center Freiburg, Freiburg, Germany
Synopsis
Intraoral coils (IOCs)
increase the signal-to-noise ratio in dental MRI exams several times over
external coils. However, the intraoral coil placement might be associated with
safety hazards such as RF heating. This study evaluates the safety of different
IOCs using temperature and E-field measurements to detect temperature hotspots.
An inductively-coupled and a wired IOC were constructed, E-field hotspots were
detected and the temperature increase was measured showing that it remains below
1K over 6min RF exposure.
Introduction
Dental examinations
require soft tissue and hard dental material depiction for an accurate
diagnosis. MRI provides an excellent soft tissue contrast, and recent MR studies
also showed promising results in imaging of hard tissue. To improve image
quality and achievable resolution during dental MRI, intraoral coils (IOCs)
were proposed recently1-4, but a detailed safety evaluation of the IOCs has
so far not been performed.
IOCs are placed
inside the oral cavity (e.g. as a dental bite). Similar to active implants
or interventional devices, IOCs can induce high electric fields in tissues that
come in close contact with the IOC, which poses a potential safety hazard if
the temperature rise of 1K is exceeded5. Unlike elongated implant leads and
devices, IOCs do not have a single tip or electrodes around which the scattered
E-fields cause high local SAR deposition. Thus, it is necessary to investigate
the complete coil and find local hotspots. In this study, we propose a test
method for safety evaluation of IOCs and provide a safety analysis of an
intraoral Tx/Rx loop coil (IOL), and an inductively-coupled flexible coil (IFC)
at 1.5T and 3T using E-field and temperature measurements. Materials and Methods
Two IFCs (ø=15mm/30mm @3T/1.5T, width=2mm on 0.3mm-thick PCB) were
constructed and inductively coupled to
external Rx coils of the MR systems. MR images were acquired at a clinical 3T
(PrismaFit, Siemens) and 1.5T (Aera, Siemens) systems with T2-SPACE sequence
(see4). IFCs were covered in a dental x-ray film (Fig.1a). In addition, an IOL was built by
cutting out a loop (dental bite form)
from a 1mm-thick copper plate, which was isolated using dental resin and
water-tight disposable plastic (Fig.1b)2.
To assess coil safety, a workflow
was defined starting with an electric (E) field mapping using an electro-optic
E-field sensor (EOS)6-7. The IFCs were positioned in a water bath (13x13cm²), and an excitor loop
coil was placed in parallel (distance=20mm) outside the the bath . E-field
maps were acquired on a planar grid 1mm above the IFC surface with 1x1mm² resolution
for tuned and detuned IFC. E-field measurements were also performed with the IOL,
which was also the excitor. In the E-field maps the location of the maximum
(hotspot) was determined. Afterwards, temperature measurements were performed with 3 fiber-optic temperature
probes (FOTEMP6-19;
Optocon AG, Dresden, Germany) that were placed on the hotspots (Fig.1b). During
the measurement the coils were placed in an ASTM phantom filled
with 30L of HEC-gel (31g/L hydroyethylcellulose, 1.55g/L NaCl) at two different
positions P1 or P2 (Fig.1c). First, the IFCs were measured with cross-diodes for
passive detuning. Then, the crossed-diodes were removed to simulate resonant coil coupling with the body coil as
a potential component failure. For RF
heating a SPACE sequence (whole body SAR of 0.6W/kg) and an RF-only
sequence (maximum RF power deposition of 4W/kg) were applied over a duration of 360s. Measurements were repeated with the IOL where the RF power was directly applied to the
coil via an RF signal generator and power amplifier (3.2W and 100% duty cycle).Results
In-vivo measurements of IFC (3T) provide an SNR=91 compared to an
external loop giving an SNR=15 yielding an SNR gain of 6 (Fig.2a-d). The MR
images of the 1.5T acquisition also show a 3-fold signal enhancement around the
coil in Figs.2e,f respectively.
In Fig.3, the E-field map of the IFC with a crossed diode shows no detectable
increase of the E-field whereas the IFC without diodes (Fig.3b) has a distinct
local hotspot around the coil capacitor used for tuning. The same behavior was
observed at 1.5T (64MHz) with increased intensity. The IOL shows the highest
E-field at the feed port in Fig.3f. (Fig.3e). At 1.5T, a 40% reduction in the
peak E field value was observed compared to 3T.
The temperature measurements show no heating during low-power deposition
with the SPACE sequence, but the maximum-SAR protocol resulted in a
detectable temperature increase of 0.6K for the side position P2 (Fig.4). Without
diodes a temperature increase of 0.3K was detectable at P1. IOL data resulted
in a max. temperature increase of 0.3K (shielded) and 0.5K (unshielded). All
temperature increase values are listed in Table 1. Discussion
The hotspot location of the EOS is in agreement with the measured temperature
results, giving a maximum temperature increase around the capacitors. Overall,
the MR safety standard specified
in the International Electrotechnical Commission (IEC 60601-2-33) that
evaluates temperature rise after 6 minutes to be below 1K is fulfilled for
this specific coil case. Current ASTM safety standards
do not explicitly mention intra-oral coils, but guidelines for active implanted
devices are applicable as a reference8.
IOL E-field maps were consistent with previous
simulation studies showing that E-fields are concentrated around the feed port.
This can be prevented by feeding the IOL using a shielded and balanced port,
i.e., a dual strip-line. A simple shielding of the feedport already reduces the
peak E-field by 50% (Fig.3e-f). Conclusion
Dental MRI
with IOCs provides a clear SNR gain and can be performed without apparent RF safety
hazard when the patient is in a typical central position. Even if safety components
such as crossed diodes fail, patient safety can be guaranteed for the tested
coil setup. Acknowledgements
No acknowledgement found.References
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