Datta Abhishek, Elwassif Maged, Battaglia Fortunato, Bikson Marom
Department of Biomedical Engineering, The City College of New York of the City University of New York, NY 10031, USA.
J Neural Eng. 2008 Jun;5(2):163-74. doi: 10.1088/1741-2560/5/2/007. Epub 2008 Apr 28.
We calculated the electric fields induced in the brain during transcranial current stimulation (TCS) using a finite-element concentric spheres human head model. A range of disc electrode configurations were simulated: (1) distant-bipolar; (2) adjacent-bipolar; (3) tripolar; and three ring designs, (4) belt, (5) concentric ring, and (6) double concentric ring. We compared the focality of each configuration targeting cortical structures oriented normal to the surface ('surface-radial' and 'cross-section radial'), cortical structures oriented along the brain surface ('surface-tangential' and 'cross-section tangential') and non-oriented cortical surface structures ('surface-magnitude' and 'cross-section magnitude'). For surface-radial fields, we further considered the 'polarity' of modulation (e.g. superficial cortical neuron soma hyper/depolarizing). The distant-bipolar configuration, which is comparable with commonly used TCS protocols, resulted in diffuse (un-focal) modulation with bi-directional radial modulation under each electrode and tangential modulation between electrodes. Increasing the proximity of the two electrodes (adjacent-bipolar electrode configuration) increased focality, at the cost of more surface current. At similar electrode distances, the tripolar-electrodes configuration produced comparable peak focality, but reduced radial bi-directionality. The concentric-ring configuration resulted in the highest spatial focality and uni-directional radial modulation, at the expense of increased total surface current. Changing ring dimensions, or use of two concentric rings, allow titration of this balance. The concentric-ring design may thus provide an optimized configuration for targeted modulation of superficial cortical neurons.
我们使用有限元同心球人体头部模型计算了经颅电流刺激(TCS)期间大脑中感应的电场。模拟了一系列圆盘电极配置:(1)远极双极;(2)近极双极;(3)三极;以及三种环形设计,(4)带状,(5)同心环,和(6)双同心环。我们比较了每种配置针对垂直于表面定向的皮质结构(“表面径向”和“横截面径向”)、沿脑表面定向的皮质结构(“表面切向”和“横截面切向”)以及非定向皮质表面结构(“表面幅度”和“横截面幅度”)的聚焦性。对于表面径向场,我们进一步考虑了调制的“极性”(例如浅层皮质神经元胞体的超极化/去极化)。与常用的TCS方案相当的远极双极配置在每个电极下产生了具有双向径向调制和电极间切向调制的扩散(非聚焦)调制。增加两个电极的接近度(近极双极电极配置)增加了聚焦性,但代价是更多的表面电流。在相似的电极距离下,三极电极配置产生了相当的峰值聚焦性,但降低了径向双向性。同心环配置导致了最高的空间聚焦性和单向径向调制,但代价是总表面电流增加。改变环的尺寸或使用两个同心环,可以调节这种平衡。因此,同心环设计可能为浅层皮质神经元的靶向调制提供一种优化配置。