Darmstadt April 2010 Field Simulation Software to Improve Magnetic Resonance Imaging a joint project with the NRI in South Korea CST Usergroup Meeting 2010 Darmstadt OvG University Magdeburg Institute for Biometry and Medicine Informatics J. Mallow, T.Herrmann
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Field Simulation Software to Improve Magnetic Resonance ... · SAR distribution of the body coil at 1.5 Tesla whole body MRI-system The Billie biological model of the Virtual Family
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Darmstadt April 2010
Field Simulation Software to Improve
Magnetic Resonance Imaging
a joint project with the NRI in South Korea
CST Usergroup Meeting 2010
Darmstadt
OvG University Magdeburg
Institute for Biometry and Medicine Informatics
J. Mallow, T.Herrmann
OvG University Magdeburg
J. Mallow, T. Herrmann
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OvG University Magdeburg
Institute for Biometry and Medical Informatics
Prof. J. Bernarding, J. Mallow, T.Herrmann
Chair of Biomedical Magnetic Resonance
Prof. O. Speck, M. Kladeck
Chair of Microwave and Communication Engineering
Prof. A. Omar, I. Ali Elabyad
Neuroscience Research Institute, Gachon University, Incheon, South
Korea
Prof. Z-H. Cho
Leibniz Institute for Neurobiology, Magdeburg, Germany
Dr. J. Stadler
Working group
OvG University Magdeburg
J. Mallow, T. Herrmann
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MRI RF-coil development with
CST Microwave Studio 2009-2010
Goals:
Simulation based development of 1T, 1.5T, 3T and 7T MRI RF-coils
Designing of RF-coils for special fMRI-experiments
Designing of surface coils and phased array coils for 3T and 7T
Optimizing the B1-Field homogeneity for better image quality
Optimizing the matching for better Q-factor (S-parameter)
Verifying of RF-coils by calculating SAR with “biological models”
Investigation of the travelling wave concept to allow whole
body MRI excitation at ultra-high field
Surface-coils for different applications
Phased- Array 7T- Monkey head coil
CST Microwave Studio in MRI at OvG
University Magdeburg
OvG University Magdeburg
J. Mallow, T. Herrmann
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8-Channel receive head coil for 3T MRI Helmholtz Tx-Rx head coil for 7T
Doty - CP 7T extremity RF-coilB1-field homogeneity 8-Ch. head coil for 3T MRI
CST Microwave Studio in MRI at OvG
University Magdeburg
OvG University Magdeburg
J. Mallow, T. Herrmann
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Simulation and Construction of an 8-Channel
Receive Head Coil for 3T MRI
human head transversal slice imageB1-field homogeneity 8-Ch. head coil for 3T MRI
OvG University Magdeburg
J. Mallow, T. Herrmann
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Finding the optimized loop-distance for phased-array surface coils with CST
CST Microwave Studio in MRI at OvG
University Magdeburg
OvG University Magdeburg
J. Mallow, T. Herrmann
8
One or more RF-coils are necessary to acquire MR images
A close distance between RF-coil and subject as well as and a good filling factor is recommended to get highest SNR
Standard procedure for clinical MRI-systems ( 1.5T and 3T):
use a body coil for excitation Tx combined with one or more phased array coils for receive Rx
To have the possibility to use flexible and close distance Rx RF-coils a body coil for excitation is very important to get homogenous B1+ distribution
In this case all SAR calculation have to be done one time just for the body coil
Whole Body MRI excitation
OvG University Magdeburg
J. Mallow, T. Herrmann
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CST Microwave Studio in MRI at OvG
University Magdeburg
Simulation model of 1.5 Tesla (63MHz) MRI whole body
system. Model designed with CST MWS 2010
B1+ field distribution of the body coil at 1.5 Tesla whole body MRI-
system. Calculations performed with CST MWS 2010
Siemens Sonata 1.5T and Trio 3T
whole body MRI
body coil for excitation Tx of B1+ and
receive with Rx phased array coils
Body Coil in Standard MRI-Systems
OvG University Magdeburg
J. Mallow, T. Herrmann
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Combination of Biological Model
and Field Simulation for SAR calculation
SAR distribution of the body coil at 1.5 Tesla whole
body MRI-system
The Billie biological model of the Virtual Family The Gustav biological model of the
CST Family
OvG University Magdeburg
J. Mallow, T. Herrmann
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Known problems:
At UHF conditions there is no body coil resonator available such as for 1.5T and 3T whole body MRI-systems
Reasons: SAR too high at 7T (5x SAR in compare to 3T) for standard
body coil architecture
Instable field distribution in loaded condition
Present state:
Every UHF RF-coil needs separate excitation and SAR calculation to work in UHF MRI-system
New solutions required
Body coil at Ultra High Field (UHF) MRI
OvG University Magdeburg
J. Mallow, T. Herrmann
12OvG University Magdeburg
J. Mallow, T. Herrmann
Travelling Wave for Transmit (Tx) in
7T MRI Whole Body System
Reference: Brunner DO, De Zanche N, Fröhlich J, Paska J, Pruessmann KP; Travelling-
wave nuclear magnetic resonance; Nature, 2009, 457(7232):994-8
The useable B1+ field in RF-coils is restricted to dimensions
and geometry of the RF-coils itself
The useable B1+ field in travelling wave concept is restricted
to dimensions of the waveguide (RF-shield) only
The condition of travelling wave related to near field and far
field The physical near field condition is described from 0-10λthe far field begins at 10λ The behavior of the EM-wave is different in near field and far field This condition is depend on load in side of RF-shield
OvG University Magdeburg
J. Mallow, T. Herrmann
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Field simulation model of the 7T MRI system with turnstile dipole and scheme of
the travelling wave concept
Travelling Wave Near Field (NF-Tx) for Tx
OvG University Magdeburg
J. Mallow, T. Herrmann
14OvG University Magdeburg
J. Mallow, T. Herrmann
RF-Shield & Gradient Coil: length = 158cm
RF-Shield diameter d= 64,1cm
RF-Shield
The cut-off frequency for propagating TE11 (H11) mode is 275 MHz for an RF-shield diameter d=64,1cm
The RF-shield of the bore is used as circular waveguide
Only Rx coils with passive or active detuning could be used
Turnstile Dipole and Patch Antenna are used for transmit Tx
Travelling Wave Near Field (NF-Tx) for Tx
OvG University Magdeburg
J. Mallow, T. Herrmann
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basic principle using an turnstile dipole to create a circular polarized B1-field
Port 1 Port 2
Port 1 + Port 2 (90° phased-shift)
Travelling Wave Near Field (NF-Tx) for Tx
OvG University Magdeburg
J. Mallow, T. Herrmann
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With tuning and matching capacitors for port 1 & 2
to allow optimal adjustments inside the bore
patch antenna prototype
optimization using software model implemented with CST MWS 2009
Patch Antennas for Near Field Tx (NF-Tx)
OvG University Magdeburg
J. Mallow, T. Herrmann
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inside bore for free space
Reflection parameter of the designed patch antenna
Patch antenna is matched and tuned for bore condition
The reflection parameters depend of position inside of the bore
Patch Antennas for Near Field Tx (NF-Tx)
OvG University Magdeburg
J. Mallow, T. Herrmann
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Depiction of antenna positioning for image acquisition