Computation of electromagnetic fields for high-frequency magnetic resonance imaging applications.

A numerical method is presented to compute electromagnetic fields inside a 2 mm high resolution, anatomically detailed model of a human head for high-frequency magnetic resonance imaging (MRI) applications. The method uses the biconjugate gradient algorithm in combination with the fast Fourier transform to solve a matrix equation resulting from the discretization of an integrodifferential equation representing the original physical problem. Given the current distribution in an MRI coil, the method can compute both the electric field (thus the specific energy absorption rate (SAR)) and the magnetic field, also known as the B1 field. Results for the SAR and B1 field distribution, excited by a linear and a quadrature birdcage coil, are calculated and presented at 64 MHz, 128 MHz and 256 MHz, corresponding to the operating frequencies of the 1.5 T, 3 T and 6 T MRI systems. It is shown that compared with that at 64 MHz, the SAR at 128 MHz is increased by a factor over 5 and the SAR at 256 MHz is increased by a factor over 10, assuming the same current strength in the coil. Furthermore, compared with the linear excitation, the average SAR for the quadrature excitation is reduced by a factor over 2 and the maximum SAR is reduced by a factor over 3. It is also shown that the B1 field at high frequencies exhibits a strong inhomogeneity, which is attributed to dielectric resonance.

[1]  W. Chew,et al.  BiCG-FFT T-Matrix method for solving for the scattering solution from inhomogeneous bodies , 1996 .

[2]  R. Stollberger,et al.  Spatial distribution of high-frequency electromagnetic energy in human head during MRI: numerical results and measurements , 1996, IEEE Transactions on Biomedical Engineering.

[3]  Weng Cho Chew,et al.  A discrete BCG-FFT algorithm for solving 3D inhomogeneous scatterer problems , 1995 .

[4]  P. Dimbylow,et al.  SAR calculations in an anatomically realistic model of the head for mobile communication transceivers at 900 MHz and 1.8 GHz. , 1994, Physics in medicine and biology.

[5]  On the field inhomogeneity of a birdcage coil , 1994, Magnetic resonance in medicine.

[6]  K. Paulsen,et al.  Finite element computations of specific absorption rates in anatomically conforming full-body models for hyperthermia treatment analysis , 1993, IEEE Transactions on Biomedical Engineering.

[7]  Dennis M. Sullivan,et al.  A frequency-dependent FDTD method for biological applications , 1992 .

[8]  P. M. Berg,et al.  The three dimensional weak form of the conjugate gradient FFT method for solving scattering problems , 1992 .

[9]  O P Gandhi,et al.  A frequency-dependent finite-difference time-domain formulation for induced current calculations in human beings. , 1992, Bioelectromagnetics.

[10]  J W Carlson,et al.  Electromagnetic fields of surface coil in vivo NMR at high frequencies , 1991, Magnetic resonance in medicine.

[11]  T K Foo,et al.  An analytical model for the design of RF resonators for MR body imaging , 1991, Magnetic resonance in medicine.

[12]  O. Gandhi,et al.  Currents induced in an anatomically based model of a human for exposure to vertically polarized electromagnetic pulses , 1991 .

[13]  O. Gandhi,et al.  Magnetic resonance imaging: calculation of rates of energy absorption by a human-torso model. , 1990, Bioelectromagnetics.

[14]  K. J. Glover,et al.  The discrete Fourier transform method of solving differential-integral equations in scattering theory , 1989 .

[15]  M. Cátedra,et al.  A numerical scheme to obtain the RCS of three-dimensional bodies of resonant size using the conjugate gradient method and the fast Fourier transform , 1989 .

[16]  P. Röschmann Radiofrequency penetration and absorption in the human body: limitations to high-field whole-body nuclear magnetic resonance imaging. , 1987, Medical physics.

[17]  T. Sarkar On the Application of the Generalized BiConjugate Gradient Method , 1987 .

[18]  W. Barber,et al.  Comparison of linear and circular polarization for magnetic resonance imaging , 1985 .

[19]  J. Schenck,et al.  Estimating radiofrequency power deposition in body NMR imaging , 1985, Magnetic resonance in medicine.

[20]  J. Schenck,et al.  An efficient, highly homogeneous radiofrequency coil for whole-body NMR imaging at 1.5 T , 1985 .

[21]  Om P. Gandhi,et al.  Fast-Fourier-Transform Method for Calculation of SAR Distributions in Finely Discretized Inhomogeneous Models of Biological Bodies , 1984 .

[22]  D. Hoult,et al.  Quadrature detection coils—A further √2 improvement in sensitivity , 1983 .

[23]  Stuchly,et al.  DIELECTRIC PROPERTIES OF BIOLOGICAL SUBSTANCES–TABULATED , 1980 .

[24]  P A Bottomley,et al.  RF magnetic field penetration, phase shift and power dissipation in biological tissue: implications for NMR imaging. , 1978, Physics in medicine and biology.

[25]  A. C. Eycleshymer,et al.  A cross-section anatomy , 1970 .

[26]  M. Hestenes,et al.  Methods of conjugate gradients for solving linear systems , 1952 .