Cockburn J F, Maddern G J, Wemyss-Holden S A
Department of Radiology, Norfolk and Norwich University Hospital, Norwich, UK.
Clin Radiol. 2007 Mar;62(3):213-20. doi: 10.1016/j.crad.2006.11.008. Epub 2007 Jan 23.
To examine the effect of applying increasing amounts of direct current (DC) before and during alternating current radiofrequency ablation of porcine liver.
Using a Radiotherapeutics RF3000 generator, a 9 V AC/DC transformer and a 16 G plain aluminium tube as an electrode, a control group of 24 porcine hepatic radiofrequency ablation zones was compared with 24 zones created using a bimodal electric tissue ablation (BETA) technique in three pigs. All ablations were terminated when tissue impedance rose to greater than 999 Omega or radiofrequency energy input fell below 5 W on three successive measurements taken at 1 min intervals. BETA ablations were performed in two phases: an initial phase of variable duration DC followed by a second phase during which standard radiofrequency ablation was applied simultaneously with DC. During this second phase, radiofrequency power input was regulated by the feedback circuitry of the RF3000 generator according to changes in tissue impedance. The diameters (mm) of each ablation zone were measured by two observers in two planes perpendicular to the plane of needle insertion. The mean short axis diameter of each ablation zone was subjected to statistical analysis.
With increased duration of prior application of DC, there was a progressive increase in the diameter of the ablation zone (p<0.001). This effect increased sharply up to 300 s of pre-treatment after which a further increase in diameter occurred, but at a much lesser rate. A maximum ablation zone diameter of 32 mm was produced (control diameters 10-13 mm).
Applying a 9 V DC to porcine liver in vivo, and continuing this DC application during subsequent radiofrequency ablation, results in larger ablation zone diameters compared with radiofrequency ablation alone.
研究在猪肝脏的交流电射频消融术前及术中施加逐渐增加的直流电(DC)的效果。
使用放射治疗RF3000发生器、9V交流/直流变压器以及一根16G普通铝管作为电极,将24个猪肝脏射频消融区的对照组与采用双峰电组织消融(BETA)技术在3头猪身上创建的24个消融区进行比较。当组织阻抗升至大于999Ω或在以1分钟间隔连续进行的三次测量中射频能量输入降至5W以下时,所有消融均终止。BETA消融分两个阶段进行:第一阶段为持续时间可变的直流电,随后第二阶段在施加标准射频消融的同时施加直流电。在第二阶段,射频功率输入由RF3000发生器的反馈电路根据组织阻抗的变化进行调节。由两名观察者在与针插入平面垂直的两个平面上测量每个消融区的直径(mm)。对每个消融区的平均短轴直径进行统计分析。
随着直流电预先施加时间的增加,消融区直径逐渐增大(p<0.001)。在预处理300秒之前,这种效应急剧增加,之后直径进一步增加,但速率要小得多。产生的最大消融区直径为32mm(对照组直径为10 - 13mm)。
在体内对猪肝脏施加9V直流电,并在随后的射频消融过程中持续施加该直流电,与单独进行射频消融相比,可导致更大的消融区直径。