Dielectric shading artifacts in high field
Magnetic Tomography systems
Poster No.: C-0027
Congress: ECR 2018
Type: Educational Exhibit
Authors: V. G. Syrgiamiotis1, V. Maliakas2, T. Thomas2, L. G. Astrakas2, M. Argyropoulou2, A. Plousi1; 1Athens/GR, 2Ioannina/GR
Keywords: Radiographers, MR physics, MR, Education, Physics, Technical
aspects, Education and training,
Artifacts
DOI: 10.1594/ecr2018/C-0027
Learning objectives
Interpretation of dielectric shadow artifact - occurring due to the
dielectric phenomenon and one of the disadvantages of imaging in high field
magnetic resonance imaging systems (# 3.0 Tesla). The term dielectric effect
refers to the interaction of matter – and in this case of biological tissues
and materials - with the coexisting electric field (E1) of an electromagnetic
field.
Background
Magnetic and Electrical Fields in MRI
In the MRI, together with the B1 of the RF coexists an electric field (E1).
As described by the Maxwell equations, the fields B1 and E1 oscillate
vertically with each other in the direction of wave propagation. When
electromagnetic waves meet the human body, various phenomena occur
The main ones are the following:
(i) wavelength reduction
(ii) electrical current generation and
(iii) somewhat reflection / refraction of wave during the transition
between different tissues.
In all of the images a central area of reduced intensity ("dark
area") is observed due to the dielectric phenomenon, which develops
strongly due to the strong magnetic field (3T) and the presence of the cystic
large structure, which is a tissue with high conductivity, the creation of stagnant
waves and the intense appearance of the phenomenon.
vii, viii and ix: T2 images TSE sequences at transverse, sagittal and
frontal plane. (MT 1.5 Tesla University hospital of Ioannina)
Images
for this section:
Fig. 1: The diagram shows three phases of a transmitted
linearly polarized wave emitted from left to right with the same wave
equations, where E = E0 sin (-#t + k#r) and B = B0sin (-#t + k#r). © https://en.wikipedia.org – modified
Fig. 2: #n magnetic fields of intensity #1.5 T, RF wavelengths
are larger compared to body size. As the intensity of B0 increases, the
resonance frequency of B1 increases and wavelengths become equal or smaller
than the anatomical regions we wish to depict. © https://en.wikipedia.org – modified
Fig. 3: i, ii and iii: T2 images TSE sequences at transverse,
sagittal and frontal levels. (MT 3.0 Tesla University Hospital of Ioannina) iv,
v and vi: T1 DIXON images in the transverse plane without suppressing the fat
signal and suppressing the fat signal before and after the i.v. the granting of
NSA. (MT 3.0 Tesla University hospital of Ioannina). © University Hospital of Ioannina
Fig. 4: x, xi and xii: T1 TSE images at transverse level
without suppressing the fat signal, T1 TSE on sagittal and transverse level by
suppressing the fat signal after i.v. administration of a NSA (MT 1.5 Tesla
WNI). In all of the images there is a central area of reduced intensity
("dark area") due to the dielectric phenomenon, which develops due to
the presence of the cystic large structure, which is a tissue with high
conductivity, which intensifies the creation of stagnant waves and the intense
appearance of the phenomenon. The dielectric effect on 1.5 T magnetic resonance
imaging is significantly milder compared to the corresponding effect in the 3.0
T magnetic resonance imaging. © University
Hospital of Ioannina.
Findings and procedure details
The degree to which matter interacts with electric and magnetic fields
can be described by three parameters: i) Magnetic permeability (μ).(ii) Electrical permeability (e).iii) Electrical conductivity (#).For
weakly conductive dielectric materials such as those of the human body, the
internal RF field is disturbed by a jump current (JC) and displacement current flux
(JD) that can be described by Ampère's law with the Maxwell correction # X B = μJC + μJD = μ#E + i##EIn human tissues, the RF frequencies used in JC and JD are
of the same order of magnitude. As the frequency increases, the
dielectric term (JD) becomes more important. Even in 7.0T (300 MHz) static
field magnetic field tomography, the conduction / displacement current ratios
for fat, gray matter, muscles and CSF are about 0.4, 0.6, 0.7 and 1.7
respectively.
To avoid the heterogeneous distribution of RF in the anatomical area
under consideration, many #3.0T magnetic resonance imaging systems use the
"MultiTransmit" technology, which catalyzes the prevention of
dielectric phenomenon expression as a dielectric shadow
In 3.0T systems without Multi Transmit technology, dielectric shading
effects may occur depending onthe patient, particularly in body imaging. To
avoid this, it is recommended to use the body-coordinated CLEAR technique - a B1
special filter designed to eliminate the inconsistencies in the body imaging.
Images
for this section:
Fig. 5: MultiTransmit" technology. Left without and Right with
"MultiTransmit" to avoid dielectric shading. © https://en.wikipedia.org – modified.
Conclusion
Dielectric phenomena and associated pseudo-images are progressively more
important and more complex as the field strength increases. With MultiTransmit
technology, the power, range, phase and waveform of all RF sources are
automatically adjusted for optimal homogeneity in each
patient's unique anatomy. In this way, MultiTransmit technology provides
optimal signal homogeneity and stability
Personal information
V.G.Syrgiamiotis RT,BSc,MSc,PhD(c) ,EFRS Treasurer, Lab assistant ATEI
of Athens, General Childrens hospital of Athens Agia Sophia CT-MRI Department
Thomas Theofanis RT,BSc,MSc (c) ,University hospital of Ioannina
Maliakas Vasileios RT,BSc,MSc,PhD(c) ,University hopsital of Ioannina
Loukas Astrakas Assistant Professor Medical Physists ,University hospital of Ioannina
Argyropoulou Maria Professor Radiology , University hospital of Ioannina
Ploussi Agapi Medical Physist ,BSc,MSc,PhD(c)
University hospital of Athens , Attiko
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