Laeseke Paul F, Lee Fred T, Sampson Lisa A, van der Weide Daniel W, Brace Christopher L
Department of Radiology, University of Wisconsin, 600 Highland Avenue, Madison, WI 53792, USA.
J Vasc Interv Radiol. 2009 Sep;20(9):1224-9. doi: 10.1016/j.jvir.2009.05.029. Epub 2009 Jul 18.
To determine whether microwave ablation with high-power triaxial antennas creates significantly larger ablation zones than radiofrequency (RF) ablation with similarly sized internally cooled electrodes.
Twenty-eight 12-minute ablations were performed in an in vivo porcine kidney model. RF ablations were performed with a 200-W pulsed generator and either a single 17-gauge cooled electrode (n = 9) or three switched electrodes spaced 1.5 cm apart (n = 7). Microwave ablations were performed with one (n = 7), two (n = 3), or three (n = 2) 17-gauge triaxial antennas to deliver 90 W continuous power per antenna. Multiple antennas were powered simultaneously. Temperatures 1 cm from the applicator were measured during two RF and microwave ablations each. Animals were euthanized after ablation and ablation zone diameter, cross-sectional area, and circularity were measured. Comparisons between groups were performed with use of a mixed-effects model with P values less than .05 indicating statistical significance.
No adverse events occurred during the procedures. Three-electrode RF (mean area, 14.7 cm(2)) and single-antenna microwave (mean area, 10.9 cm(2)) ablation zones were significantly larger than single-electrode RF zones (mean area, 5.6 cm(2); P = .001 and P = .0355, respectively). No significant differences were detected between single-antenna microwave and multiple-electrode RF. Ablation zone circularity was similar across groups (P > .05). Tissue temperatures were higher during microwave ablation (maximum temperature of 123 degrees C vs 100 degrees C for RF).
Microwave ablation with high-power triaxial antennas created larger ablation zones in normal porcine kidneys than RF ablation with similarly sized applicators.
确定使用高功率三轴天线的微波消融是否比使用尺寸相似的内部冷却电极的射频(RF)消融产生明显更大的消融区。
在体内猪肾模型中进行了28次12分钟的消融。使用200W脉冲发生器进行RF消融,使用单个17号冷却电极(n = 9)或三个间距为1.5cm的切换电极(n = 7)。使用一个(n = 7)、两个(n = 3)或三个(n = 2)17号三轴天线进行微波消融,每个天线输送90W连续功率。多个天线同时供电。在每次RF和微波消融的两个过程中测量距施加器1cm处的温度。消融后对动物实施安乐死,并测量消融区直径、横截面积和圆度。使用混合效应模型进行组间比较,P值小于.05表示具有统计学意义。
手术过程中未发生不良事件。三电极RF(平均面积,14.7cm²)和单天线微波(平均面积,10.9cm²)消融区明显大于单电极RF区(平均面积,5.6cm²;P分别为.001和.0355)。单天线微波和多电极RF之间未检测到显著差异。各组间消融区圆度相似(P>.05)。微波消融期间组织温度更高(最高温度为123℃,而RF为100℃)。
在正常猪肾中,使用高功率三轴天线的微波消融比使用尺寸相似的施加器的RF消融产生更大的消融区。