Sossena Wood1, Tales Santini1, Narayanan Krishnamurthy1, Shailesh Raval1, and Tamer S. Ibrahim, PhD1,2
1Bioengineering, University of Pittsburgh, Pittsburgh, PA, United States, 2Radiology, University of Pittsburgh, PA, United States
Synopsis
In this work, a developed refillable multi-compartment 3D-printed head
phantom (established from MRI scans obtained in-vivo) was compared to a
homogeneous commercial spherical phantom, the phantom itself with homogeneous
loading in all of its compartments and in-vivo (the same volunteer on whom the
phantom was based). Through B1 mapping
and SAR analysis within an RF coil, the heterogeneous multi-compartment head
phantom results were most accurate to the in-vivo volunteer.
Purpose
Experimental phantom studies lack the accuracy of comparison to in-vivo
humans. The purpose of this work is to
evaluate the performance and characterization of a physical (3D printed) anthropomorphic
heterogeneous head phantom using an RF head coil through simulations of B1 fields
and SAR distributions and experiments (in-vivo and phantom B1 field mapping). The designed phantom was compared to a
homogeneous commercial spherical phantom, the phantom itself with homogeneous
loading (saline) in all of its compartments and in-vivo (the same volunteer on
whom the phantom was based).Methods
Fabrication. Wood et. al established an eight-tissue
multi-compartment heterogeneous head phantom developed from a high resolution
3T MRI dataset of a healthy male volunteer for various electromagnetic
applications 1.
The dielectric properties of the heterogeneous head phantom were modeled
from Table 1 in 1. Unlike 2, hydrophobic SLA resin is used to hold
the liquids of each refillable designed tissue chamber.
Numerical
Modeling. In-house
numerical simulation software was used to generate magnetic and electric fields
at 297.2 MHz (7T). Numerical simulations
are performed on the model of the anthropomorphic heterogeneous head phantom
(with the plastic), a commercial homogeneous spherical phantom and the model
based on the actual segmentation (no plastic) of the in-vivo images within a
16-strut TEM resonator using finite difference time domain method (FDTD) (Fig 1.)
B1
Mapping. Experimental studies
are performed using 7T Siemens MAGNETOM® scanner (Siemens, Erlangen, Germany). To quantify the magnetic field through experimentation,
we use SAT Turbo flash (SatTFL) sequence for B1 mapping method, with a
rectangular RF pulse of 1 ms at 500V. The MR protocol uses the following image
parameters: FOV: 64 x 64 mm2; TE: 1.16 ms; TR: 2000 ms; FA: 6⁰; BW:
1502 MHz; Resolution: 3.125 x 3.125 x 2.0 mm3.
Sample
Size. One healthy adult
human subject was scanned using the 7T scanner for the in-vivo experimental
study with proper consent and IRB approval.
Results
Fig 2 highlights the distributions of
the normalized B1+
magnetic field with respect to various planes of view through numerical and
experimental studies. The normalized B1
mean values are 1.483uT, 1.545uT, 1.576uT and 1.101uT for the 4 different
phantoms. Fig 3 highlights the SAR of the
model of each phantom. The calculations
for the peak SAR of the various models are 15.2232 W/kg/10g, 12.3558 W/kg/10g,
6.56 W/kg/10g and 6.73 W/kg/10g, according to the order that the images in Fig
3 from left to right.Discussion
Fig 2 depicts the similarities and
differences of the normalized B1 magnetic field distribution in the
various phantoms compared to the in-vivo volunteer. According to B1 profiles of the experimental
data, the magnetic field distribution of the heterogeneous multi-compartment head
phantom is most similar to the in-vivo distribution. Although the same phantom was used with
homogeneous loading, the magnetic field distribution proved to be most similar
to the spherical phantom. This finding
indicates that the dielectric properties and complexity of the head phantom
have a great role in the accuracy of the phantom’s comparison to the in-vivo
volunteer. Fig 3 highlights the
distribution of the SAR using the numerical models scaled by the maximum peak
SAR among all models. The peak SAR is the greatest in the numerical model of
the in-vivo volunteer followed by the heterogeneous phantom. The absence of SAR
in the averaged bone/fat/skin tissue or plastic leads to the difference among
the four models. The homogeneous multi-compartment phantom is similar in terms
of peak SAR value to the spherical phantom.Conclusion
The experiment supports the initial statement being that a commercial
spherical phantom or homogeneous multi-compartment phantom lacks accuracy of
comparison to in-vivo. While the heterogeneous
head phantom is still an estimation, our work demonstrates that the use of a
heterogeneous head phantom provides a greater estimation of the electromagnetic
behavior (B1 and SAR) occurred in-vivo. Future
work should be completed to evaluate the temperature rise in the different
compartments of the phantoms and compared to temperature calculations.Acknowledgements
The
work reported in this abstract is supported by National Institute of
Biomedical Imaging and Bioengineering of the National Institutes of Health under
award number 1F31EB019872.
(https://projectreporter.nih.gov/project_info_details.cfm?icde=0&aid=8838518)
The
content is solely the responsibility of the authors and does not necessarily represent
the official views of the National Institutes of Health (https://www.nibib.nih.gov/).
References
1. Wood S, Krishnamurthy N, Zhao Y, et al.: Anatomically Detailed Human
Head Phantom for MR Testing Purposes. In Jt Annu Meet ISMRM-ESMRMB 2014;
2013:3067.
2. Grädel NN, Polimeni
JR, Guerin B, Gagoski B, Wald LL: An Anatomically Realistic Temperature Phantom
of the Head for Validation of {SAR} Calculations {[Abstract]}. Proc Int Soc
Magn Reson Med 2012; 20:314.