|
Computer # |
|
4866.
|
49 |
Worst-Case Analysis of
RF-Induced Heating During MRI Scanning in a Generic
Multi-Component Orthopedic Medical Implant Applying the
Design of Experiment Method (DoE)
Mahdi Abbasi1,2, Gregor Schaefers1,
Juan D. Sánchez1, and Daniel Erni2
1MR:comp GmbH, Gelsenkirchen, NRW, Germany, 2General
and Theoretical Electrical Engineering (ATE), University
of Duisburg-Essen, Duisburg, NRW, Germany
MRI is known as a non-invasive imaging technique of the
inner parts of the body. Temperature rise in surrounding
tissue of a metallic implant needs to be calculated
carefully for the patient’s safety. Calculating spatial
induced electric field and SAR become more complex when
the implant is non-uniform in shape and contains several
parts. The effect of each component of a multi-component
generic hip implant on RF heating has been studied by
applying the Design of Experience (DoE) method. By using
Taguchi method, the effect of each variable could be
estimated as well as any arbitrary configuration of the
implant including worst and safest configurations.
|
4867. |
50 |
Evaluation of Multi-Section
Resistive Tapered Stripline (RTS) Lead Wires to Reduce SAR
Near Implanted DBS Electrodes During MRI
Peter Serano1,2, Leonardo M. Angelone3,
and Giorgio Bonmassar1
1Athinoula A. Martinos Center for Biomedical
Imaging, Charlestown, MA, United States, 2Electrical
and Computer Engineering, University of Maryland,
College Park, MD, United States, 3U.S.
Food and Drug Administration CDRH/OSEL/DP, Silver
Spring, MD, United States
When performing MRI in patients with DBS implants, one
of the major issues is the heating of tissue surrounding
the implant due to radiofrequency (RF) pickup of the
implant acting as an antenna. We present an extensive
evaluation of the design parameters of a novel DBS lead
for MRI based on Resistive Tapered Stripline (RTS)
technology. Our results show this innovative high
scattering technology can allow for up to a 40% decrease
in tissue specific absorption rate (SAR) near the DBS
electrode while maintaining low lead resistivity for
continuous current injection.
|
4868. |
51 |
SAR reduction in deep brain
stimulation patients using parallel transmission
Bastien Guerin1, Sara Sprinkhuizen1,
Cristen LaPierre1,2, Yigitcan Eryaman1,3,
and Lawrence L Wald1,4
1A. A. Martinos Center for Biomedical
Imaging, Dpt. of Radiology, Massachusetts General
Hospital, Charlestown, MA, United States, 2Dpt.
of Physics, Harvard Univerity, Cambridge, MA, United
States, 3Madrid-MIT
M+Vision Consortium in RLE, Massachusetts Institute of
Technology, Cambridge, MA, United States, 4Division
of Health Sciences Technology, Harvard-MIT, Cambridge,
MA, United States
Deep brain stimulation (DBS) is used to treat Parkinson
disease, essential tremor and depression. DBS involves
implanting electrodes permanently in the patient’s
brain. When placed inside an MRI scanner the DBS lead
heats up because of strong coupling with the RF field,
which is dangerous to the patient. We show in
simulations and phantom experiments that parallel
transmission can excite the MRI signal without creating
significant SAR at the tip of the DBS lead by minimizing
the electric field along the DBS lead wire. Application
of this approach in vivo could elucidate the mechanisms
of action of DBS.
|
4869. |
52 |
Measuring RF currents
induced in implants using B1+ maps
Mélina Bouldi1 and
Jan M. Warnking1,2
1Grenoble Institut des Neurosciences - UJF,
Grenoble, Rhônes Alpes, France, 2Inserm
U836, Grenoble, Rhônes Alpes, France
In the presence of conductive implants, the B1+ field
presents distortions generated by induced RF currents,
which can be linked to the expected SAR. We fitted a
theoretical model of the induced B1+ distortions to
experimental B1 data obtained in an ASTM phantom to
measure the current in a conducting wire. This indirect
measurement of wire current was compared to EM
simulations in a numerical model. This work may lead to
methods allowing rapid evaluation of the RF safety of
conductive wire in a given configuration.
|
4870. |
53 |
Subjective Assessment of
Sensations Experienced by 7 Tesla Magnetic Resonance Imaging
-permission withheld
Ikuko Uwano1, Tsuyoshi Metoki1,
Fusako Sendai1, Ryoko Yoshida1,
Kohsuke Kudo1,2, Fumio Yamashita1,
Satomi Higuchi1, Kenji Ito1,
Jonathan Goodwin1,2, Taisuke Harada1,2,
and Makoto Sasaki1
1Division of Ultrahigh Field MRI, Institute
for Biomedical Sciences, Iwate Medical University,
Yahaba, Iwate, Japan, 2Department
of Diagnostic and Interventional Radiology, Hokkaido
University Hospital, Sapporo, Hokkaido, Japan
We investigated the unpleasant sensations experienced by
large number of the Japanese subjects during MRI
examination using a 7T scanner that has a slow
table-feed speed, and then compared these sensations to
the previous reports. Unpleasant sensations such as
vertigo were experienced at 7T especially when the table
is moving, but were infrequent and weak when compared
with the previous studies presumably do to the slow
table-feed speed, indicating that the degree of
subjective discomforts at 7T is tolerable and may be
acceptable in the usage of the clinical practice in the
future.
|
4871. |
54 |
MRI Gradient Field-Induced
Heating and its Frequency Dependency for Different Materials
Juan D. Sánchez1, Mahdi Abbasi1,
Amin Douiri2, Morwan Choli3,
Wolfgang Goertz2, and Gregor Schaefers3
1Dept. of Numerical Simulation, MR:comp GmbH,
Gelsenkirchen, NRW, Germany, 2Test
Laboratory, MR:comp GmbH, Gelsenkirchen, NRW, Germany,3Dept.
of Consulting, MR:comp GmbH, Gelsenkirchen, NRW, Germany
This study evaluated the gradient-induced heating of a
pair of metallic plates (dimensions similar to
commercial medical implantable pulse generators IPGs)
made of different materials in order to determine a
suitable test procedure for the test of gradient induced
heating. From the obtained results, it is observed that
a worst-case exposure cannot be concluded only by a
particular set of gradient field conditions for all
different implants.
|
4872. |
55 |
Torque and Translational
force Considerations for ferromagnetic shells in MR Imaging
Vahid Ghodrati1 and
Abbas N Moghaddam1,2
1BME, Tehran Polytechnic, Tehran, Tehran,
Iran, 2School
of Cognitive Sciences, Institute for Studies in
Theoretical Physics and Mathematics, Tehran, Iran
In some injuries, such as those happen in the battle
field, part of shells or foreign objects that may
include magnetic materials remain in victim’s body. In
this research we calculate the torque and translational
force for specific ferromagnetic objects. Translational
force reaches its maximum value near the opening to the
bore. Near the isocenter, however, there is no
translational force acting on the ferromagnetic
spherical object. For a long cylindrical shell, such as
a niddle, or for a flat cylindrical shell, like a disk,
the torque inside the bore is quite significant. Torque
can be managed by a prior knowledge about the object
orientation from an auxiliary imaging modality.
|
4873. |
56 |
MRI Safety and Cardiac
Pacemakers/ICDs
Karl K. Vigen1, Kurt S. Hoffmayer2,
and Scott B. Reeder1,3
1Radiology, University of Wisconsin-Madison,
Madison, WI, United States, 2Medicine,
University of Wisconsin-Madison, Madison, WI, United
States,3Medicine, Medical Physics and
Biomedical Engineering, University of Wisconsin-Madison,
WI, United States
Cardiac pacemakers and implantable cardioverter
defribrillators (ICDs) have been traditionally been
contraindicated for MRI. Recently, device manufacturers
have developed pacemakers and ICDs that are specifically
designed and approved as MRI-compatible. In addition,
several sites have reported successfully imaging
patients with conventional pacemakers and ICDs, and a
large clinical trial is underway which is investigating
the use of MRI for patients with conventional devices.
|
4874. |
57 |
Perfluorocarbon Lung
Clearance Evaluated with Dual-Nuclei 19F
and 1H
MRI in the Context of Total Liquid Ventilation
Ludovic de Rochefort1, Mourad Chenoune2,
Anis Ben Yahmed1, Charlotte Alibert1,
Jérémy Pépin1, Fanny Lidouren2,
Lys Darbera2, Alain Berdeaux2,
Matthias Korn1, Rose-Marie Dubuisson1,
Luc Darrasse1, Daniel Isabey3, and
Renaud Tissier2
1IR4M, Univ. Paris-Sud, CNRS, UMR 8081, Orsay,
France, 2Inserm
UMR 955-3, Univ Paris Est, Ecole Nationale Vétérinaire
de Maisons-Alfort, Maisons-Alfort, France, 3Inserm
UMR 955-13, Univ Paris Est, Créteil, France
Fast hypothermia induced by Total Liquid Ventilation (TLV)
with Perfluorocarbons (PFC) has been shown to be
cardioprotective. TLV procedure includes a lung filling
phase, the ventilation, and a final clearance during
which PFCs are eliminated from the lungs. For the
potential clinical transfer, it is important to select
PFCs that are better tolerated, as the clearance phase
may vary with the PFC physical properties. Here, we
present the evaluation of the clearance from pig lungs
for three different liquid PFCs with a quantitative
dual-nuclei (1H, 19F) MRI protocol at 1.5 T providing
insights for selecting PFCs for human use
|
4875. |
58 |
Gd-enhanced MRI after
therapeutic ferumoxytol for iron deficiency anemia - An
in-vitro study for optimal contrast timing and dose
determination.
Sandeep Arora1, Judy Yee1, David
Saloner1, Rizwan Aslam1, and
Thomas Hope1
1Radiology and Biomedical Imaging, University
of California, San Francisco, San Francisco, California,
United States
Therapeutic ferumoxytol injections can confound
subsequently performed magnetic resonance imaging using
gadolinium based contrast agents due to its
superparamagnetic effects. In this in vitro study, we
image various concentrations of ferumoxytol and
gadolinium to determine concentration of ferumoxytol
which will not affect arterial enhancement in subsequent
contrast enhanced scans. Our images demonstrate that
significant enhancement can be seen after single dose
gadolinium enhanced scans two half-lives with initial
ferumoxytol concentration being 300 microgram/ml. Even
after one half-life, significant enhancement can be seen
with double or triple dosing of gadolinium based
contrast agents.
|
4876. |
59 |
RF Heating of Gold Cup and
Conductive Plastic Electrodes during Simultaneous MRI and
EEG
Mukund Balasubramanian1, William M. Wells2,
John R. Ives3, Patrick Britz4,
Tobias Loddenkemper5, Padmavathi Sundaram1,
Robert V. Mulkern1, and Darren B. Orbach1
1Department of Radiology, Boston Children's
Hospital, Boston, Massachusetts, United States, 2Department
of Radiology, Brigham and Women's Hospital, Boston,
Massachusetts, United States, 3Ives
EEG Solutions, Inc., Newburyport, Massachusetts, United
States, 4Brain
Products GmbH, Gilching, Germany, 5Department
of Neurology, Boston Children's Hospital, Boston,
Massachusetts, United States
The EEG electrodes used in clinical settings are
typically removed prior to MRI scanning at 3T due to RF
heating concerns. Since it would be advantageous to
leave these electrodes on during routine clinical scans
and to record from them during functional MRI scans, we
measured the temperature changes under two types of
clinical electrodes during a variety of 3T MRI scans,
using watermelons as phantoms. Our results suggest that
these electrodes could be used safely at 3T, as long as
the EEG wire lengths and the SAR of the MRI sequences
are both carefully taken into consideration.
|
4877. |
60 |
Magnetic Forces on Medical
Implants
Robert J. Deissler1, Michael Martens1,
Tanvir Baig1, Zhen Yao1, Charles
Poole1, and Robert Brown1
1Department of Physics, Case Western Reserve
University, Cleveland, Ohio, United States
Medical implants raise important safety concerns for
patients receiving MRI due to the forces and torques
acting on the implants during patient scanning or entry.
The implant can be deemed MRI safe if the magnetic
forces and torques are less than the forces due to
gravity. Using a representative contour plot of B|grad
B| for a 1.5 T magnet design we determine safe zones
which also depend on the material susceptibility. We
show that if the implant is deemed safe for static
forces it will also be safe for static torques.
|
4878. |
61 |
Heating of bilateral hip
prostheses in a human body model induced by a multi-axis
gradient coil set
Hector Sanchez-Lopez1, Luca Zilberti2,
Oriano Bottauscio2, Jeffrey Hand3,4,
Annie Papadaki5, Fangfang Tang1,
Mario Chiampi6, and Stuart Crozier1
1School of Information Technology &
electrical Engineering, The University of Queensland,
Brisbane, QLD, Australia, 2Istituto
Nazionale di Ricerca Metrologica, Torino, Torino, Italy, 3Centre
for the Developing Brain, Kings College London, London,
United Kingdom, 4Division
of Imaging Sciences and Biomedical Engineering, Kings
College London, London, United Kingdom, 5Neuroimaging
Analysis Centre, University College London Hospitals,
London, United Kingdom, 6Dip.
Energia, Politecnico di Torino, Torino, Italy
Heating Ti6Al4V and CoCrMo bilateral hip prostheses in a
human body voxel model exposed to individual and
combined 1 kHz magnetic fields associated with a
conventional multi-axis gradient (30 mT m-1) coil set
was predicted using a non-commercial frequency-domain
code based on hybrid finite element (FE) - boundary
element (BE) method. For CoCrMo (Ti6Al4V) prostheses,
maximum increases of 1.2 (0.7), 0.3 (0.18) and 1.4 (1.2)
oC were predicted, respectively, for x, y and z coils
individually and of 2.0 (1.2) oC when combined. The
temperature rise when all three gradients are used
intensively is of concern, particularly for CoCrMo
implants.
|
4879. |
62 |
An 8 Channel Transmit
Receive Sodium & Nested 8 Channel Transmit Receive Proton
Coil for 3.0 T Brain Imaging
Karthik Lakshmanan1, Ryan Brown1,
Guillaume Madelin1, Fernando Boada1,
and Graham Wiggins1
1Department of Radiology, New York University
School of Medicine, NewYork, NewYork, United States
Nested 8 Channel Tx/Rx Sodium array & A 8 Channel Proton
array for 3.0 T Brain Imaging
|
4880. |
63 |
Design and Application of a
Nested Multi-Channel Sodium/Proton Knee Array at 3T
Ryan Brown1, Karthik Lakshmanan1,
Guillaume Madelin1, Gregory Chang1,
Daniel K Sodickson1, Ravinder R Regatte1,
and Graham C Wiggins1
1The Bernard and Irene Schwartz Center for
Biomedical Imaging, Dept. of Radiology, New York
University School of Medicine, New York, NY, United
States
We describe a six channel proton/sodium 3T knee array
whose design counteracts low coil-tissue coupling that
is characteristic of low-gamma coils and can make the
potential gains from a phased array difficult to
realize. This issue was addressed by implementing 1) a
mechanically flexible former to minimize coil-to-tissue
distance and reduce the overall diameter of the array,
and 2) a wideband matching scheme that counteracts
preamplifier noise degradation caused by resonance
frequency splitting and a high loaded coil quality
factor. The sodium array provided at least 30% SNR gain
over a birdcage coil, while proton channel performance
was sufficient for clinical imaging.
|
4881. |
64 |
Design and Testing of a
9-Channel Phased Array Coil for Magnetic Resonance Guided
Focused Ultrasound Treatment of the Abdominal Region in
Large Animal Models.
Emilee Minalga1, Robb Merrill1,
Allison Payne1, Nassir F. Marrouche2,
Dennis L. Parker1, and J. Rock Hadley1
1Radiology, University of Utah, Salt Lake
City, UT, United States, 2Comprehensive
Arrhythmia Research and Management (CARMA) Center,
University of Utah, Salt Lake City, UT, United States
Coils that increase the SNR for MRgFUS treatments are
very important. More signal-to-noise ratio can give
better temperature measurements which increases the
treatment efficacy and safety. This work describes the
design and testing of a 9-channel radio-frequency coil
array designed for abdominal magnetic resonance guided
focused ultrasound research in large animal models.
|
4882. |
65 |
Excitation Performance and
SAR Control with Z-Stacked Body RF Coil Arrays in Parallel
Transmission at 3T
Xiaotong Zhang1, Xiaoping Wu2,
Jinfeng Tian2, Sebastian Schmitter2,
Lance DelaBarre2, Michael Hamm3,
Josef Pfeuffer3, Dingxin Wang2,4,
Bin He1,5, Thomas Vaughan2, Kamil
Ugurbil2, and Pierre-Francois Van de Moortele2
1Department of Biomedical Engineering,
University of Minnesota, Minneapolis, MN, United States, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, MN, United States, 33Siemens
Healthcare, MR Application Development, Erlangen,
Germany, 4Siemens
Medical Solutions USA Inc, Minneapolis, MN, United
States, 5Institute
for Engineering in Medicine, University of Minnesota,
Minneapolis, MN, United States
A High Pass birdcage (32 rungs) driven on two quad ports
(1x2) and three TEM whole body arrays consisting of one
ring (1x8), 2 z-stacked rings (2x8) or 3 z-stacked rings
(3x8) of TEM elements (8 per ring) have been modeled.
Their performance in parallel transmission on spine and
brain+c-spine imaging has been evaluated, in which the
excitation fidelity, RF power, global SAR and peak
10gSAR are compared. RF Spoke placement impact is also
detailed for different coil designs.
|
4883. |
66 |
Adaptive Head Array
Victor Taracila1, Miguel Navarro1,
Darren Gregan1, Sarah Ortman1, and
Fraser Robb1
1General Electric Healthcare, Aurora, Ohio,
United States
Brain imaging became one of the main applications in
MRI. A high performance brain coil needs to have the
receiving elements as close as possible to the ROI.
Unfortunately with the big variation within the human
population head sizes, the head coils are usually made
to fit the 99 percentile of the people, therefore for
smaller size people the coil could under perform. There
are attempts to address different head size populations
with appropriately sized coils. We propose to change the
paradigm of a rigid head coil, but still accomplish the
goal of one-size-fits-all coil – the Adaptive Head Array
(AHA).
|
4884. |
67 |
B1 Homogenization
and Local SAR Reduction Using B1-control Receive
Array Coil at 3T
Yukio Kaneko1, Yoshihisa Soutome1,2,
and Hisaaki Ochi1
1Hitachi Ltd., Central Research Laboratory,
Kokubunji, Tokyo, Japan, 2Hitachi
Medical Corporation, Kashiwa, Chiba, Japan
B1 inhomogeneity increases as the strength of a magnetic
field increases. Various methods to reduce the B1
inhomogeneity have been developed. However, B1
inhomogeneity still remains in some cases of abdominal
imaging. A more effective method is therefore required.
In this study, a B1-control receive array coil (BRAC),
which has the inductive mode during the RF transmit
period, was designed. The B1 field and local SAR field
in a human model were calculated in FDTD simulation. It
is shown that the BRAC can reduce B1 inhomogeneity and
local SAR in the human body.
|
4885. |
68 |
A 60-Channel Ex-Vivo
Brain-Slice Coil Array for 3T Imaging
Bernhard Gruber1,2, Boris Keil2,
Thomas Witzel2, Aapo Nummenmaa2,
and Lawrence L Wald2
1School of Applied Health and Social Sciences
- Medical Engineering, University of Applied Sciences,
Linz, Upper Austria, Austria, 2Department
of Radiology, Massachusetts General Hospital, Harvard
Medical School, A.A. Martinos Center for Biomedical
Imaging, Charlestown, Massachusetts, United States
The parallel acquisition of brain images is standard
nowadays. A wide range of coils offering specialized
solutions to problems in clinical diagnosis, preclinical
science and research already exists but to proceed with
the imaging of the human brain for the “Human Connectome
Project” a 60 Channel Receive Array Coil for ex-vivo
brainslices at 3 Tesla was constructed. This coil was
developed for research purposes only, but other
applications, especially in pathology or clinical
applications, are possible out of the design.
|
4886. |
69 |
Combined Transmit-Only
Asymmetric Birdcage and Receive-Only Endorectal Surface RF
Coils
Adam Farag1, Justin Peterson2,
Trevor Wade1, Trevor Szekeres1,
Alexei Ouriadove3, Eli Gibson4,
Aaron Ward4, Joseph Chin5, Steven
Pautler6, Glenn Bauman5, Cesare
Romagnoli5, Robert Bartha1,2, and
Timothy Scholl1,2
1Robarts Research Institute, Western
University, London, ON, Canada, 2Medical
Biophysics, Western University, London, ON, Canada, 3Thunder
Bay Regional Research Institute, ON, Canada, 4Biomedical
Engineering, Western University, ON, Canada, 5London
Health Science Center, ON, Canada, 6St.
Joseph's Health Care, ON, Canada
Though radio frequency (RF) coil is a well-established
science, the challenges that an RF designer faces when
applying them to MRI are unique. Particularly, the
challenges of developing confined RF coil for the
purpose of insertion and imaging small parts in the
human body, is different. In this work we present a low
frequency Endorectal RF coil for measuring sodium tissue
concentration (TSC) in the prostate. This has the
potential to enable researchers to understand the sodium
and cancerous cells relationship. First images at 3T
were obtained and analysed, coil sensitivity was
corrected and measurements of TSC is possible.
|
4887. |
70 |
Why do dipole antennas
work? A comparison to loop coils as a function of element
size
Alexander Raaijmakers1, Peter R. Luijten1,
and Cornelis A.T. van den Berg2
1Radiology, UMC Utrecht, Utrecht, Utrecht,
Netherlands, 2Radiotherapy,
UMC Utrecht, Utrecht, Netherlands
More and more institutes have recognized the potential
of dipole antennas. However, many coil engineers are
still reluctant to adopt this new technology. This
abstract will provide a meaningful insight into why
dipoles can outperform more conventional coil array
elements at ultra-high fields. A comparison to loop
coils is performed by FDTD simulations at 300 MHz with
varying dimensions. Results show that large dimensions
are only beneficial at large depths. Dipole antennas
outperform loop coils from a depth of only 5 cm. These
results confirm again that dipole antennas form a
promising candidate to improve ultra-high field imaging
performance.
|
|
|
Computer # |
|
4888. |
49 |
SAR characterisation for
parallel transmission MRI – comparison between modelling
different decoupling regimes
Arian Beqiri1, Jeff W. Hand1,
Francesco Padormo1,2, Joseph V. Hajnal1,2,
and Shaihan J. Malik1
1Division of Imaging Sciences and Biomedical
Engineering, King's College London, London, United
Kingdom, 2Centre
for the Developing Brain, King's College London, London,
United Kingdom
In this study we compare different ways of modelling
decoupling in parallel transmission MRI systems using EM
solver simulations. One method is to model the
individual transmit elements independently without
including any decoupling networks leading to an ideally
decoupled system. The other method involves using
circuit co-simulation to model the entire system fully
along with the decoupling networks. Here we compare the
fields produced between the two methods and their
estimates of SAR showing that they both give comparable
results.
|
4889. |
50 |
A Novel Method for MRI Safe
Lead Design
Volkan Acikel1,2 and
Ergin Atalar1,2
1Department of Electrical and Electronics
Engineering, Bilkent University, Ankara, Turkey, 2National
Magnetic Resonance Research Center (UMRAM), Ankara,
Turkey
In this study a novel method for designing MRI safe
leads using Modified Transmission Line Method (MoTLiM)
is presented. SAR at the tip of a lead is formulated and
it is shown that by adjusting the wavenumber along the
lead SAR can be decrease significantly. A way to
increase wavenumber is multilayer wound leads. In
multilayer wound leads, resistance increases due to the
proximity effect and inductance increase due to the
number of windings. It is shown that by increasing
number of layers SAR can be decreased such that the
implant lead tip heating is no longer a significant
problem.
|
4890. |
51 |
Experience in imaging
healthy volunteers and patients with implants at 7T
Yacine Noureddine1,2, Andreas K. Bitz2,3,
Markus Thürling2,4, Karsten H. Wrede5,
Mark E. Ladd2,3, Gregor Schaefers1,
and Oliver Kraff2,6
1MR:comp GmbH, Dept. of Consulting, MR safety
testing Laboratory, Gelsenkirchen, NRW, Germany, 2Erwin
L.Hahn Institute for MRI, University Duisburg-Essen,
Essen, NRW, Germany, 3Division
of Medical Physics in Radiology, German Cancer Research
Center (DKFZ), Heidelberg, BW, Germany, 4Department
of Neurology, University Duisburg-Essen, Essen, NRW,
Germany, 5Clinic
for Neurosurgery, University Hospital Essen, Essen, NRW,
Germany, 6Department
of Diagnostic and Interventional Radiology and
Neuroradiology, University Hospital Essen, Essen, NRW,
Germany
Examination of patients with implants has become
relevant at research facilities with ultra-high field
strength systems. Nevertheless, no standards or tests
currently exist for implants at 7T due to the more
complex and specific challenges at this field strength.
Many 7T research centers conservatively exclude all
subjects with implants, regardless of type or loca-tion.
This study presents our 7-year experience in imaging
patients and healthy volunteers with implants other than
dental implants at 7T.
|
4891. |
52 |
Reliable and robust RF
safety assessment of transmit array coils at ultrahigh
fields
Frank Seifert1, Antonino Cassara1,
Gerd Weidemann1, and Bernd Ittermann1
1Physikalisch-Technische Bundesanstalt (PTB),
Berlin, Germany
A reliable simulation based assessment of RF safety of
pTX-coil-arrays requires an elaborate estimation of
upper limits of local SAR for all reasonable steering
conditions and model assumptions. Limiting the forward
power of each individual transmit channel is the
simplest and most reliable approach to comply with
applicable safety standards. For these circumstances we
propose a simple estimation procedure to find an upper
limit for local SAR from the Q-matrix. When applying
this procedure to a 7T 8-channel transmit head coil the
resulting local SAR related power limit is only 25
percent lower than the power limit for the head SAR
which has to be maintained anyway.
|
4892. |
53 |
RF safety evaluation of
different configurations of high-permittivity pads used to
improve imaging of the cerebellum at 7 Tesla
Andreas K. Bitz1,2, Oliver Kraff2,
Stephan Orzada2, Tim Herrmann3,
Johannes Mallow3, Johannes Bernarding3,
and Mark E. Ladd1,2
1Medical Physics in Radiology, German Cancer
Research Center (DKFZ), Heidelberg, Germany, 2Erwin
L. Hahn Institute for Magnetic Resonance Imaging,
University Duisburg-Essen, Essen, Germany, 3Department
of Biometrics and Medical Informatics,
Otto-von-Guericke-University Magdeburg, Magdeburg,
Germany
Dielectric pads with high permittivity can be used to
improve image quality in UHF brain imaging. To achieve
this, the positions of the pads have to be optimized
individually for each examination, leading to different
configurations which need to be analyzed w.r.t. RF
safety. Therefore, detailed RF exposure analysis based
on RF simulations has been performed to check whether
the maximum permissible input power of the Tx coil needs
to be readjusted. Results show that the SAR distribution
is influenced by the high-permittivity pads and depends
on their size and orientation. For certain
configurations, a significant SAR elevation was found.
|
4893. |
54 |
The Feasibility of
Predicting Temperature Increase through Local SAR Estimation
via Electrical Properties Tomography: A Phantom Study at 7T
Xiaotong Zhang1, Jiaen Liu1,
Pierre-Francois Van de Moortele2, Sebastian
Schmitter2, and Bin He1
1Department of Biomedical Engineering,
University of Minnesota, Minneapolis, MN, United States, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, MN, United States
It has been shown that Electrical Properties (EPs) of
biological tissues can be derived from MR-based B1
measurement. A strong appeal for these ‘Electrical
Property Tomography’ (EPT) methods is to estimate
real-time and subject-specific local SAR induced by RF
pulsing. In order to investigate the feasibility of
EPT-based SAR estimation in predicting possible local
temperature change, following previously proposed EPT
protocols, in this preliminary study, induced local SAR
in a saline phantom has been estimated for a heating
sequence at 7T, as compared to measured temperature
changes using MRI Thermometry based on the proton
chemical shift (PRF).
|
4894. |
55 |
Investigation of Different
RF Coil Safety Assessment Techniques: E-field Measurements,
EM Field Simulations and MR Thermometry
Cem Murat Deniz1,2, Leeor Alon1,2,
Gene Y Cho1,2, Ryan Brown1,
Christopher M Collins1,2, and Daniel K.
Sodickson1,2
1The Bernard and Irene Schwartz Center for
Biomedical Imaging, Department of Radiology, New York
University School of Medicine, New York, NY, United
States, 2The
Sackler Institute of Graduate Biomedical Sciences, New
York University School of Medicine, New York, NY, United
States
Electromagnetic field simulations and MR thermometry
measurements have been used for evaluating the safety of
RF coils. Increasingly, electric field measurements have
been employed as an additional validation of
electromagnetic field simulations, and as a means of
assessing the safety of RF antennas. In this work, we
investigated the application of these RF coil safety
assessment techniques using a dipole antenna and "SAM"
head phantom. Our results indicate that all three
methods provide comparable RF safety information both in
pattern and in magnitude.
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4895. |
56 |
Fast method to compute the
electromagnetic field inside a model of the human head
surrounded by a dielectric pad
Giuseppe Carluccio1, Switt Kittivittayakul2,
Piergiorgio Uslenghi2, Christopher Michael
Collins1, and Danilo Erricolo2
1Bernard and Irene Schwartz Center for
Biomedical Imaging, New York University School of
Medicine, New York, New York, United States, 2Electrical
and Computer Engineering, University of Illinois at
Chicago, Chicago, Illinois, United States
High permittivity dielectric pads have become popular
for their ability to locally enhance the B_1 field in
the region of interest, especially in tissues close to
the pad. Commonly, it is challenging to have a strong
signal in regions close to the center of the head, and
it is hard to predict the effect of the use of
dielectric materials in those locations. In this work a
fast exact analytical method is proposed to compute the
electromagnetic field at the center of a model of the
human head. The method can be useful to design optimal
dielectric pads.
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4896. |
57 |
Numerical simulations of RF
heating for infants within MR body coil
Xin Chen1, Charles Poole2, Michael
Steckner1, and Robert Brown2
1MR, Toshiba Medical Research Institute USA,
Inc., Mayfield Village, OH, United States, 2Physics,
Case Western Reserve University, Cleveland, OH, United
States
MRI is useful for neonatal/pediatric imaging since no
ionizing radiation is used. Nevertheless, MRI has unique
safety concerns: RF power deposition and resultant
tissue heating. Numerical simulations have been widely
applied to investigate specific absorption rate (SAR)
and tissue temperature rise. However, most work
published on adults and only a few showed results for
infants. Infants’ (especially neonates) thermoregulation
is not as developed as adults, and may be further
impaired under unique scan conditions (sedation,
swaddling). Furthermore, there are no special
considerations in regulatory limits for these patients.
This work investigates SAR and temperature rise in
infants due to RF heating.
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4897. |
58 |
Fast Local SAR Simulation
by Domain-Decomposition
Shumin Wang1
1Auburn University, Auburn, AL, United States
Real-time Local SAR simulation is critical to the
success of multi-channel RF transmission at high fields.
The speed of conventional electromagnetic simulation
methods is insufficient even on parallel computation
platforms. We propose a novel domain-decomposition
method that applies different numerical algorithms in
the interior and the exterior of a human body model.
These different methods then interface on the surface of
the human body model. Preliminary studies show that on a
single-core CPU, simulating an eight-channel brain
imaging array only in 30 seconds.
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4898. |
59 |
Direct SAR Mapping by
Thermoacoustic Imaging: A Feasibility Study
Simone Angela Winkler1, Paul Picot2,
Michael Thornton2, and Brian K Rutt1
1Dept of Radiology, Stanford University,
Stanford, California, United States, 2Endra,
Inc., Ann Arbor, Michigan, United States
We propose a new concept for direct measurement of
specific absorption ratio (SAR), to be used as a safety
assessment / monitoring tool for MRI. The concept uses
short bursts of RF energy and measures the resulting
thermoacoustic excitation pattern by an ultrasound
transducer array, followed by image reconstruction to
yield the 3D SAR distribution. We developed a simulation
framework to model this thermoacoustic SAR mapping
concept; results of these simulations show good
agreement between reconstructed and original SAR
distributions and support the feasibility of direct
experimental mapping of SAR distributions in vivo.
|
4899. |
60 |
RF Safety Evaluation for
Neonatal MRI at 3T
Shaihan J Malik1, Arian Beqiri1,
Anthony N Price1,2, Jeff W Hand1,
and Joseph V Hajnal1,2
1Division of Imaging Sciences and Biomedical
Engineering, Kings College London, London, London,
United Kingdom, 2Centre
for the Developing Brain, Kings College London, London,
London, United Kingdom
Algorithms used by scanner manufacturers usually control
SAR using adult based models. In this study whole body
and 10 g local averaged SARs in a newborn neonate head-
or heart-centred in a 127 MHz birdcage coil were
predicted numerically. SARs were scaled to match the
duty cycle used in a Philips 3T Achieva when run at body
scanning and head scanning SAR limits, mimicking the
scanner set-up process during automated power scaling
when an adult subject is present. Results indicate that
under these conditions, exposure of a neonate is
conservative from a safety point of view.
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4900. |
61 |
B1+-based SAR assessment
using a birdcage coil at 7 Tesla: experimental evaluation
using magnetic resonance thermometry
Nicolas Boulant1, Ulrich Katscher2,
Michel Luong1, Aurelien Massire1,
Alexis Amadon1, and Alexandre Vignaud1
1Neurospin, CEA, Saclay, Ile de France,
France, 2Philips
Research Europe, Hamburg, Germany
The emerging field of Electric Properties Tomography has
shown great promise to provide patient-specific
information about the electric field via the
post-processing of measured B1+ data utilizing Maxwell’s
equations. The work of Voigt et al furthermore showed a
good correlation between the numerically determined SAR
distribution and the one based on the post-processing of
the B1+ field at up to 3T, but with a global offset
between the two. The purpose of this work was to
experimentally evaluate this B1+-based SAR determination
via MR temperature-based measurements at 7T with a
birdcage coil on a phantom of known electrical
properties.
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4901. |
62 |
The Effect of Brain Tumors
on Local SAR Levels at 7T
Matthew C. Restivo1, Cornelis A.T. van den
Berg1, Astrid L.H.M.W. van Lier1,
Daniël L. Polders1, Alexander J.E. Raaijmaker1,
Peter R. Luijten1, and Hans Hoogduin1
1Imaging Division, University Medical Center
Utrecht, Utrecht, Netherlands
It is well known that specific absorption rate (SAR) is
highly dependent on tissue conductivity. Previous work
has shown that brain tumors have increased conductivity
compared to surrounding tissues. In this work, we
analyzed the effects of brain tumors on simulated local
SAR levels at 7T. We segmented dielectric tissues from
T1w scans of three actual tumor patients. We then
assigned realistic conductivity values that were known
from 7T Electrical Property Tomography of the same
patients. We are able to show that the presence of
tumors increases SAR locally, although not to the extent
that we predict.
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4902. |
63 |
Calculation of 10g average
SAR via inversion of the heat equation using MRI Thermometry
and Thermal Property Measurements
Leeor Alon1,2, Gene Cho1,2, Leslie
F. Greengard3, Ricardo Otazo1,2,
Daniel K. Sodickson1,2, and Cem M. Deniz1,2
1Department of Radiology, Bernard and Irene
Schwartz Center for Biomedical Imaging, New York
University School of Medicine, New York, NY, United
States, 2Sackler
Institute of Graduate Biomedical Sciences, New York
University School of Medicine, New York, NY, United
States, 3Courant
Institute of Mathematical Sciences, New York University,
NY, United States
RF safety of MRI coils is often evaluated by conducting
RF heating experiments on tissue mimicking phantoms
inside the scanner room. Because of power delivery
capabilities of RF amplifiers, long RF heating durations
(>6 minutes) are required to create a temperature change
that can be accurately detected by MR thermometry
measurements. In such cases when the heating duration is
long, conversion from temperature-change to SAR is
nontrivial, since the heat-diffusion effect is prominent
and direct scaling of the temperature change with heat
capacity yields large 10g average SAR errors (~55% ,
shown as in this abstract ). In this work, a method for
3D calculation of 10g average SAR is presented via
inversion of the heat equation using high-resolution 3D
temperature maps and measured thermal properties of the
phantom. The algorithm can be used to calculate 10g
average SAR experimentally for limiting RF energy
deposition from physical coils in the scanner room with
small errors, %3.1.
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4903. |
64 |
Building a computational
model of a transmit body coil: considerations for RF safety.
Elena Lucano1, Gonzalo Mendoza1,
Tom Lloyd2, Steve Wedan2, Wolfgang
Kainz1, and Leonardo Angelone1
1Office of Science and Engineering
Laboratories, Division of Physics, US Food and Drug
Administration, Center for Devices and Radiological
Health, Silver Spring, MD, United States, 2Imricor
Medical Systems, Burnsville, MN, United States
Numerical models have been used to evaluate the
potential for radiofrequency induced heating of medical
devices in a MR environment. The aim of this study was
to evaluate three model designs with respect to their
accuracy in simulating the electromagnetic field
generated by a body coil. The experimental validation
showed that all three of the numerical models properly
simulated the magnetic field distribution. However, to
represent the true electric field and avoid possible
overestimation by several orders of magnitude, accurate
modeling of the tuning capacitors, coil losses, and
source configuration was required.
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4904. |
65 |
A Fast Method to Estimate
SAR Distribution from Temperature Images Highly Affected by
Noise
Giuseppe Carluccio1, Florian Knoll1,
Cem Murat Deniz1, Leeor Alon1, and
Christopher Michael Collins1
1Bernard and Irene Schwartz Center for
Biomedical Imaging, New York University School of
Medicine, New York, New York, United States
Even though temperature increase has a direct
relationship to risk, local 10g average SAR is still the
quantity most used to assess safety with reference to
existing guidelines. MR thermometry allows measurements
of temperature distribution through a cross-section of
the sample. Inverting a method to estimate temperature
from SAR, we have proposed a method to estimate SAR from
temperature maps which is highly insensitive to noise,
which often strongly affects temperature maps acquired
with MR thermometry.
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4905. |
66 |
Fast Whole-Body Temperature
Estimation for Real-Time MRI Safety Assurance
Giuseppe Carluccio1 and
Christopher Michael Collins1
1Bernard and Irene Schwartz Center for
Biomedical Imaging, New York University School of
Medicine, New York, New York, United States
A method to quickly estimate the temperature increase by
SAR absorption through the entire MRI exam. Using the
linearity of the bioheat equation, the method convolves
the precalculated temperature responses of the body
tissues with the sequence of SAR segments applied during
the exam. The predicted temperature distribution has
been compared with the one obtained with a full Finite
Difference Method solving the Pennes’ bioheat equation.
The difference in the maximum temperature between the
two methods was less than 1%, but in a computation time
more than 30 times shorter.
|
4906. |
67 |
Automatic Segmentation
Pipeline for Patient-Specific MRI Tissue Models
Angel Torrado-Carvajal1,2, Juan A.
Hernandez-Tamames1,2, Joaquin L. Herraiz2,
Yigitcan Eryaman2,3, Elfar Adalsteinsson4,5,
Lawrence L. Wald3,5, and Norberto Malpica1,2
1Dept. of Electronics, Universidad Rey Juan
Carlos, Mostoles, Madrid, Spain, 2Madrid-MIT
M+Vision Consortium in RLE, MIT, Cambridge,
Massachusetts, United States, 3Dept.
of Radiology, MGH, Martinos Center for Biomedical
Imaging, Charlestown, Massachusetts, United States, 4Dept.
of Electrical Engineering and Computer Science, MIT,
Cambridge, Massachusetts, United States, 5Harvard-MIT
Health Sciences and Technology, MIT, Cambridge,
Massachusetts, United States
Specific absorption rate (SAR) may cause unsafe tissue
heating in High-Field MRI scanners. We propose a
pipeline for patient-specific tissue modeling based only
on MRI data that could enable patient-specific pulse
design in High-Field MRI. We used open-source tools to
automatically segment eleven tissue classes: brain white
matter (WM), gray matter (GM), cerebrospinal fluid
(CSF), cerebellum WM and GM, skull, skin, eyeballs, main
arteries, muscle and fat/cartilage. The method was
tested in 12 healthy subjects, and its accuracy was
confirmed by an expert radiologist. The models are
automatically meshed and exported in a format compatible
with EM simulation software.
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4907. |
68 |
Anatomically Detailed Human
Head Phantom for MR Testing Purposes
Sossena Wood1, Narayanan Krishnamurthy1,
Yujuan Zhao1, Shailesh Raval1,
Tiejun Zhao2,3, J. Andy Holmes4,
and Tamer Ibrahim, PhD1
1Bioengineering, University of Pittsburgh,
Pittsburgh, PA, United States, 2Siemens
Medical System, Pittsburgh, PA, United States, 3University
of Pittsburgh, Pittsburgh, PA, United States, 4Swanson
Center for Product Innovation, University of Pittsburgh,
Pittsburgh, PA, United States
This research was performed because there are several
issues experienced at higher field strengths that hinder
its clinical potential resulting in a concern of the
radiofrequency (RF) power absorption in tissue and local
temperature rising. These concerns, mainly safety, are
evaluated through electromagnetic simulations that are
compared to phantoms. However, most phantoms are not
realistic nor comparable to the anatomical detail of a
human head.
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4908. |
69 |
A Statistical Study of Head
Models for Local SAR Simulation
Yu Shao1, Peng Zeng2, and Shumin
Wang2
1Auburn University, Auburn, Alabama, United
States, 2Auburn
University, Alabama, United States
Subject-specific local SAR analysis is critical to the
safety of multi-channel transmission at high fields. In
order to calculate the local SAR, subject numerical
models need to be constructed at first. However, highly
detailed subject models may not be available because
they require high-resolution images, which in turn
require the local SAR problem to be solved at first
place. In a previous study, it was found that
three-tissue water/fat/air model is sufficiently
accurate for local SAR analysis at 3 Tesla. In this
study, we shall apply a statistical approach to find the
appropriate simplification of head models and its
accuracy.
|
4909. |
70 |
Body Models of Big People
for MRI Safety Assessment
Ingmar Graesslin1, Hanno Homann1,
Holger Eggers1, Kay Nehrke1, Paul
Harvey2, Cecilia Possanzini2, and
Peter Börnert1
1Philips Research Laboratories, Hamburg,
Germany, 2Philips
Healthcare, Best, Netherlands
Estimating the specific absorption rate (SAR) is a
challenge for parallel transmission MRI systems, because
the SAR depends on subject- and coil-specific
parameters. In this work, we present a novel approach to
generate whole-body models for SAR simulations of very
large subjects. The new concept uses 2D multi-station
imaging with lateral virtual FOV enlargement and a
water/fat separating imaging sequence. The main
application area is the development of patient-specific
body models for SAR assessment, which may enable
improved SAR management and reduced scan time in
parallel transmit MRI. This approach can be used for
potential basic diagnostic applications using 2D and 3D
imaging techniques.
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4910. |
71 |
Rapid, Direct Measurement
of Bulk RF Power Deposition using Free Induction Decay
Acquisitions
Leeor Alon1,2, Assaf Tal1,2,
Giuseppe Carluccio1,2, Cem M. Deniz1,2,
Karthik Lakshmanan1,2, Daniel K. Sodickson1,2,
and Christopher C. Collins1,2
1Department of Radiology, Bernard and Irene
Schwartz Center for Biomedical Imaging, New York
University School of Medicine, New York, NY, United
States, 2Sackler
Institute of Graduate Biomedical Sciences, New York
University School of Medicine, New York, NY, United
States
Whole body and partial body RF power deposition is
typically monitored by estimating the RF power delivered
to the patient in the scanner. In practice however, some
portion of the energy gets deposited in the transmit
chain and coil electronics and different subjects couple
to the coil differently so that the RF power deposited
into the patient may be overestimated. In this work, we
utilize a single excitation pulse and acquire a single
FID before and after exposure to SAR to measure the RF
thermal energy change. Results are shown for phantom and
in-vivo heating experiments.
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