Carmichael David W, Thornton John S, Rodionov Roman, Thornton Rachel, McEvoy Andrew, Allen Philip J, Lemieux Louis
Department of Clinical and Experimental Epilepsy, Institute of Neurology, University College London, and Lysholm Department of Neuroradiology, National Hospital for Neurology and Neurosurgery, London, United Kingdom.
J Magn Reson Imaging. 2008 Nov;28(5):1233-44. doi: 10.1002/jmri.21583.
To investigate heating during postimplantation localization of intracranial electroencephalograph (EEG) electrodes by MRI.
A phantom patient with a realistic arrangement of electrodes was used to simulate tissue heating during MRI. Measurements were performed using 1.5 Tesla (T) and 3T MRI scanners, using head- and body-transmit RF-coils. Two electrode-lead configurations were assessed: a "standard" condition with external electrode-leads physically separated and a "fault" condition with all lead terminations electrically shorted.
Using a head-transmit-receive coil and a 2.4 W/kg head-average specific absorption rate (SAR) sequence, at 1.5T the maximum temperature change remained within safe limits (<1 degrees C). Under "standard" conditions, we observed greater heating (<or=2.0 degrees C) at 3T on one system and similar heating (<1 degrees C) on a second, compared with the 1.5T system. In all cases these temperature maxima occurred at the grid electrode. In the "fault" condition, larger temperature increases were observed at both field strengths, particularly for the depth electrodes. Conversely, with a body-transmit coil at 3T significant heating (+6.4 degrees C) was observed (same sequence, 1.2/0.5 W/kg head/body-average) at the grid electrode under "standard" conditions, substantially exceeding safe limits. These temperature increases neglect perfusion, a major source of heat dissipation in vivo.
MRI for intracranial electrode localization can be performed safely at both 1.5T and 3T provided a head-transmit coil is used, electrode leads are separated, and scanner-reported SARs are limited as determined in advance for specific scanner models, RF coils and implant arrangements. Neglecting these restrictions may result in tissue injury.
通过磁共振成像(MRI)研究颅内脑电图(EEG)电极植入后定位过程中的加热情况。
使用具有逼真电极排列的模拟患者来模拟MRI过程中的组织加热。使用1.5特斯拉(T)和3T MRI扫描仪,采用头部和身体发射射频线圈进行测量。评估了两种电极引线配置:一种是外部电极引线物理分离的“标准”状态,另一种是所有引线终端电气短路的“故障”状态。
使用头部发射-接收线圈和2.4 W/kg头部平均比吸收率(SAR)序列,在1.5T时,最大温度变化保持在安全范围内(<1℃)。在“标准”条件下,与1.5T系统相比,在一个系统上3T时观察到更大的加热(≤2.0℃),在第二个系统上观察到类似的加热(<1℃)。在所有情况下,这些温度最大值都出现在网格电极处。在“故障”状态下,在两个场强下都观察到温度有更大的升高,特别是对于深部电极。相反,在3T时使用身体发射线圈,在“标准”条件下,在网格电极处观察到显著的加热(+6.4℃)(相同序列,1.2/0.5 W/kg头部/身体平均),大大超过安全限度。这些温度升高忽略了灌注,而灌注是体内主要的散热源。
只要使用头部发射线圈、电极引线分离且扫描仪报告的SAR按照针对特定扫描仪型号、射频线圈和植入物配置预先确定的那样受到限制,1.5T和3T时均可安全地进行颅内电极定位的MRI检查。忽略这些限制可能会导致组织损伤。