Niklas Wehkamp1, Philipp Rovedo1, Jochen Leupold1, Sebastien Bär1, and Maxim Zaitsev1
1Division of Medical Physics, Department of Diagnostic and Interventional Radiology, University Medical Center Freiburg, Faculty of Medicine, University of Freiburg, Freiburg, Germany
Synopsis
Keywords: Software Tools, Susceptibility
Motivation: The magnetic susceptibility is a fundamental material property for MR and NMR equipment engineering. The literature provides several theoretical solutions to measure the magnetic susceptibility. However, an openly available implementation that allows to determine the magnetic susceptibility automatically is missing.
Goal(s): Develop a non-proprietary approach to determine the magnetic susceptibility from measured field maps.
Approach: Measure the field map of a cylindrical sample. Develop a Python program to extract the magnetic susceptibility of the sample.
Results: The measured reference samples reflect the magnetic susceptibility of the literature. Code for data processing is available through the open access repository.
Impact: Our
research provides a programmatic
solution to automatically
determine the magnetic susceptibility of cylindrical samples from
field map measurements in MRI
systems. This
will aid MR
and NMR equipment engineers
to measure the magnetic
susceptibility of
any
material of interest.
Introduction:
Achieving
a consistent magnetic field is crucial for most magnetic resonance
experiments. Therefore, from
an MR engineering perspective,
it's essential to carefully manage and minimize any magnetic field
distortions in the design of equipment located near the object
of interest during
measurements, including the object
itself.
The
literature provides several theoretical solutions to measure and
determine the
magnetic susceptibility. Furthermore,
many materials have already been characterized and can be found in
the literature [1] and material databases. However, the
ever expanding zoo of polymers
and
available metal alloys can make it difficult to find adequate values
for the magnetic susceptibility. The magnetic susceptibility of a
cylindrical sample can be measured with an MRI system as described by
Wappler et al. [1].
In
practice, writing the data processing pipeline just for one or two
measurements is often a barrier to perform the measurements.
Potentially
resulting
in the
use
of
roughly estimated values for the magnetic susceptibility and
suboptimal equipment design.
With
this work, we provide an
openly available python script that allows
anyone with access to an MRI system to measure a field map of a
cylindrical sample and determine its magnetic susceptibility.Methods:
In
this study, we measured
the
field
map of
cylindrical samples.
The
samples
were
placed
in the center of a 50 ml Falcon tube orthogonal to its rotational
symmetry axis and
immersed in demineralized water.
The
prepared sample is depicted in Figure 1.
The
field maps
were obtained with a 9.4 T Bruker BioSpec 94/21 system. A
quadrature birdcage Tx/Rx coil with 38 mm inner diameter for RF
excitation and signal acquisition was
used.
The
field maps were
obtained
with a 3D double gradient echo sequence with TE1 = 1.5 ms TE2 = 3.5
ms and TR = 30 ms and
isotropic resolution of 0.117 mm.
The
developed python
program was
used to
do
the following:
Determine
the sample position using a discrete convolution to find the position
of the sample. Then, the measured data are masked to exclude the
values at the position of the cylinder in the measurement. The left
side of Figure 2 shows an example of this masked data. A second order
polynomial is subtracted from the masked field map data, to
compensate for imperfect shimming during the measurement. This is illustrated on the right
side of Figure 2. Figure 3a) shows the field map after subtraction of
the second order polynomial.
The prepared field maps were then fitted with an analytical model derived from the
first order solution to Maxwell equations in integral form. The susceptibility was
determined by varying the susceptibility value in the analytical
simulation, until the difference of measurement and simulation was
minimized. The resulting simulated dipole is illustrated in Figure 3
b). Figure 3
c) shows the difference of the measured and matched dipole simulation
data. The reference value for the magnetic susceptibility of water χV
= −9.032 × 10−6 from [2] was used for the calculations.
A
link to the python script
for
the data processing can be found in the Acknowledgment section.Results:
We
determined the volume susceptibility in the SI system (dimension less
number) for Poly(methyl methacrylate) (PMMA),
High-density polyethylene (HDPE)
and
Copper.
The
results are listed in Table 1. The measured magnetic susceptibility
values confirmed the literature values reasonably well.
Table 1: Volume susceptibility (SI system) Material | Measured | Literature |
PMMA | -9.065×10−6 | −9.06×10−6 [1] |
HDPE | -9.510×10−6 | −9.67 ×10−6 [1] |
Copper | -9.307×10−6 | −9.30×10−6 [3] |
Discussion:
Our
proposed method allows to measure
the magnetic susceptibility of cylindrical samples. Providing
the Open-Source Python Algorithm (see
Acknowledgements)
will
lower the barrier to measure the magnetic susceptibility.Acknowledgements
This work was funded in part through the German Federal Ministry of
Education and Research under grant number 13GW0356B. And in part through
the National Institute of Health under grant Nr. NIH R01 EB032378 and
NIH
U24 NS120056.
The
authors thank the Core Facility AMIRCF (DFG-RIsources N° RI_00052)
for support with
measurements at
James
and Enno
with funding number: INST 39/1224-1.
The
python code for the data processing can be found at:
“https://gitlab.com/fpm9000/mag
_sus_finder”.
References
[1] M. C. Wapler, et al., Magnetic properties of materials for MR engineering, micro-MR and beyond, Journal of Magnetic Resonance, vol. 242, pp. 233–242, May 2014.
[2] J. F. Schenck, The role of magnetic susceptibility in magnetic
resonance imaging:MRI magnetic compatibility of the first and second
kinds, Medical Physics, vol. 23,pp. 815–850, June 1996.
[3] Bowers, R. Magnetic Susceptibility of Copper Metal at Low Temperatures. Phys. Rev. 102, 1486–1488 (1956).