Athey T W, Ross R J, Ruggera P S
Magn Reson Imaging. 1982;1(3):149-54. doi: 10.1016/0730-725x(82)90206-5.
Measurements were made of magnetic and electric field levels in and around a nuclear magnetic resonance imaging system undergoing a clinical trial. Magnetic field levels ranged from 0.04 tesla (T) in the imaging volume down to about 0.0006 T at the end of the patient table. The peak radio-frequency magnetic field level was 15 amperes per meter (A/m) in the imaging volume, while the rms value was 4.6 A/m. The specific absorption rate resulting from the radio-frequency magnetic field was calculated to be no more than 0.017 watts per kilogram (W/kg). The radio-frequency electric field was detectable only within a few centimeters of the coil assembly, and does not significantly contribute to the specific absorption rate. These exposure levels were much lower than existing guidelines for clinical NMR procedures.
对正在进行临床试验的核磁共振成像系统内部及周围的磁场和电场水平进行了测量。成像区域内的磁场水平范围为0.04特斯拉(T),在检查床末端降至约0.0006 T。成像区域内射频磁场的峰值水平为每米15安培(A/m),均方根值为4.6 A/m。计算得出,射频磁场产生的比吸收率不超过每千克0.017瓦(W/kg)。仅在线圈组件几厘米范围内可检测到射频电场,且其对比吸收率的贡献不显著。这些暴露水平远低于临床核磁共振程序的现有指导标准。