Department on Diagnostic and Interventional Radiology, Eberhard-Karls-University of Tübingen, Tübingen, Germany.
Invest Radiol. 2009 Dec;44(12):763-8. doi: 10.1097/RLI.0b013e3181b66d11.
To evaluate the feasibility of ex vivo ablation implementing a cryo-based internally cooled bipolar radiofrequency (RF) applicator and to determine the influence of power and gas pressure on the size and shape of the resulting ablation zones.
Two hundred twenty-five ablations were performed using a custom-built internally CO2-cooled bipolar cryo RF applicator in ex vivo bovine livers. The active tip of the applicator was 55 mm long. RF power (32-50 watts) and gas pressure of cooling medium (500-600 psi) were varied independently. Power was applied in continuous mode. Control group experiments were carried out solely using the RF function at 32, 40, and 50 watts. Ablation duration was 15 minutes for all applications. Experiments were repeated 5 times for all parameter combinations. Short and long axes of the induced white ablation zone were macroscopically assessed. The ablation zone was referred to as homogeneous if complete ablation was observed without spots of untreated tissue. The short axis diameters for the simultaneous application of cryo and RF function were analyzed using a multiple linear regression analysis. An unpaired Mann-Whitney U test was used to analyze the differences between the short axes with RF alone and RF using cryo cooling.
All ablation zones were homogeneous. Using simultaneous RF ablation function and gas cooling with a single applicator, the long axes of the ablation zones ranged between 42 +/- 2 mm (mean +/- SD) and 59 +/- 5 mm, the short axes between 24 +/- 1 and 44 +/- 1 mm, depending on the parameter combination. At a stable gas pressure level, short axes increased with rising power levels and decreased after reaching a maximum. The maxima of the short axis increased with higher gas pressure levels and were shifted to higher power values. Optimal parameter settings were 46 to 50 watts and 600 psi gas pressure, resulting in a short axis of 44 +/- 1 mm. Short axis weakly correlated with gas pressure (r2 = 0.10) and power (r2 = 0.34) alone, whereas the correlation was r2 = 0.76 for the combined factors. Without cooling, short axis diameters were significantly shorter (P < 0.05), ranging between 13 +/- 2 mm at 50 watts and 15 +/- 2 mm at 32 watts.
The results of this initial ex vivo study show that the combined cryo RF ablation device allows for large ablation volumes using a single needle, which is superior to RF ablation alone.
评估使用内置 CO2 冷却的双极冷冻射频(RF)消融器进行离体消融的可行性,并确定功率和气体压力对消融区域大小和形状的影响。
在离体牛肝中使用定制的内置 CO2 冷却双极冷冻 RF 消融器进行了 225 次消融。消融器的有效尖端长 55 毫米。分别独立改变 RF 功率(32-50 瓦)和冷却介质的气体压力(500-600 磅/平方英寸)。功率以连续模式施加。对照组实验仅在 32、40 和 50 瓦时使用 RF 功能进行。所有应用的消融持续时间为 15 分钟。对于所有参数组合,实验重复进行了 5 次。宏观评估诱导的白色消融区域的短轴和长轴。如果观察到无未处理组织的完整消融,则将消融区域称为均匀。使用多元线性回归分析分析同时应用冷冻和 RF 功能的短轴直径。使用非配对的曼-惠特尼 U 检验分析单独使用 RF 与使用冷冻冷却的 RF 之间的短轴差异。
所有消融区域均为均匀的。使用单个消融器同时进行 RF 消融功能和气体冷却,消融区域的长轴范围为 42±2 毫米(平均值±标准差)至 59±5 毫米,短轴范围为 24±1 毫米至 44±1 毫米,具体取决于参数组合。在稳定的气体压力水平下,短轴随功率水平的升高而增加,达到最大值后减小。短轴的最大值随气体压力水平的升高而升高,并向更高的功率值移动。最佳参数设置为 46 至 50 瓦和 600 磅/平方英寸的气体压力,导致短轴为 44±1 毫米。短轴与气体压力(r2=0.10)和功率(r2=0.34)单独相关较弱,而综合因素的相关系数为 r2=0.76。没有冷却时,短轴直径明显缩短(P<0.05),在 50 瓦时范围为 13±2 毫米,在 32 瓦时范围为 15±2 毫米。
这项初步的离体研究结果表明,组合式冷冻 RF 消融装置可使用单个针进行大体积消融,优于单独使用 RF 消融。