On the SAR and field inhomogeneity of birdcage coils loaded with the human head

被引:73
作者
Jin, JM [1 ]
Chen, J [1 ]
机构
[1] UNIV ILLINOIS,DEPT ELECT & COMP ENGN,ELECTROMAGNET LAB,URBANA,IL 61801
关键词
RF coils; specific absorption rate; B-1-field inhomogeneity; finite-element analysis;
D O I
10.1002/mrm.1910380615
中图分类号
R8 [特种医学]; R445 [影像诊断学];
学科分类号
1002 ; 100207 ; 1009 ;
摘要
Birdcage coils are widely used as a radiofrequency (RF) resonator in magnetic resonance imaging (MRI) because of their capability to produce a highly homogeneous B-1 field over a large volume within the coil, When they are employed for high-frequency MRI, the interaction between the electromagnetic field and the object to be imaged deteriorates the B-1-field homogeneity and increases the specific absorption rate (SAR) in the object, To investigate this problem, a finite-element method (FEM) is developed to analyze the SAR and the B-1 field in a two-dimensional (2D) model of a birdcage coil loaded with a 2D model of a human head, The electric field, magnetic field, and SAR distributions are shown, and a comprehensive study is carried out for both linear and quadrature birdcage coils at 64, 128, 171, and 256 MHz, It is shown that to generate the same value of the B-1 field, the SAR is increased significantly with the frequency, and for the same imaging method the SAR produced by a quadrature coil is significantly lower than that of a linear coil, It is also shown that the B-1-field inhomogeneity is increased significantly with the frequency.
引用
收藏
页码:953 / 963
页数:11
相关论文
共 22 条
[1]   A PERFECTLY MATCHED LAYER FOR THE ABSORPTION OF ELECTROMAGNETIC-WAVES [J].
BERENGER, JP .
JOURNAL OF COMPUTATIONAL PHYSICS, 1994, 114 (02) :185-200
[2]   RF MAGNETIC-FIELD PENETRATION, PHASE-SHIFT AND POWER DISSIPATION IN BIOLOGICAL TISSUE - IMPLICATIONS FOR NMR IMAGING [J].
BOTTOMLEY, PA ;
ANDREW, ER .
PHYSICS IN MEDICINE AND BIOLOGY, 1978, 23 (04) :630-643
[3]   ESTIMATING RADIOFREQUENCY POWER DEPOSITION IN BODY NMR IMAGING [J].
BOTTOMLEY, PA ;
REDINGTON, RW ;
EDELSTEIN, WA ;
SCHENCK, JF .
MAGNETIC RESONANCE IN MEDICINE, 1985, 2 (04) :336-349
[4]  
DIMBYLOW PJ, 1994, PHYS MED BIOL, V39, P361
[5]   AN ANALYTICAL MODEL FOR THE DESIGN OF RF RESONATORS FOR MR BODY IMAGING [J].
FOO, TKF ;
HAYES, CE ;
KANG, YW .
MAGNETIC RESONANCE IN MEDICINE, 1991, 21 (02) :165-177
[6]   COMPARISON OF LINEAR AND CIRCULAR-POLARIZATION FOR MAGNETIC-RESONANCE IMAGING [J].
GLOVER, GH ;
HAYES, CE ;
PELC, NJ ;
EDELSTEIN, WA ;
MUELLER, OM ;
HART, HR ;
HARDY, CJ ;
ODONNELL, M ;
BARBER, WD .
JOURNAL OF MAGNETIC RESONANCE, 1985, 64 (02) :255-270
[7]  
HAN Y, 1993, P SMRM 12 ANN M, P1327
[8]  
HARRISON JG, 1996, 12 ANN REV PROGR APP, P1220
[9]   AN EFFICIENT, HIGHLY HOMOGENEOUS RADIOFREQUENCY COIL FOR WHOLE-BODY NMR IMAGING AT 1.5-T [J].
HAYES, CE ;
EDELSTEIN, WA ;
SCHENCK, JF ;
MUELLER, OM ;
EASH, M .
JOURNAL OF MAGNETIC RESONANCE, 1985, 63 (03) :622-628
[10]  
Jin J., 1993, FINITE ELEMENT METHO