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大功率微波消融小口径、气冷天线:初步离体和体内结果。

High-powered microwave ablation with a small-gauge, gas-cooled antenna: initial ex vivo and in vivo results.

机构信息

Department of Radiology, University of Wisconsin School of Medicine and Public Health, Madison, WI 53792-3252, USA.

出版信息

J Vasc Interv Radiol. 2012 Mar;23(3):405-11. doi: 10.1016/j.jvir.2011.11.003. Epub 2012 Jan 24.

Abstract

PURPOSE

To evaluate the performance of a gas-cooled, high-powered microwave system.

MATERIALS AND METHODS

Investigators performed 54 ablations in ex vivo bovine livers using three devices-a single 17-gauge cooled radiofrequency(RF) electrode; a cluster RF electrode; and a single 17-gauge, gas-cooled microwave (MW) antenna-at three time points (n = 6 at 4 minutes, 12 minutes, and 16 minutes). RF power was applied using impedance-based pulsing with maximum 200 W generator output. MW power of 135 W at 2.45 GHz was delivered continuously. An approved in vivo study was performed using 13 domestic pigs. Hepatic ablations were performed using single applicators and the above-mentioned MW and RF generator systems at treatment times of 2 minutes (n = 7 MW, n = 6 RF), 5 minutes (n = 23 MW, n = 8 RF), 7 minutes (n = 11 MW, n = 6 RF), and 10 minutes (n = 7 MW, n = 9 RF). Mean transverse diameter and length of the ablation zones were compared using analysis of variance (ANOVA) with post-hoc t tests and Wilcoxon rank-sum tests.

RESULTS

Single ex vivo MW ablations were larger than single RF ablations at all time points (MW mean diameter range 3.5-4.8 cm 4-16 minutes; RF mean diameter range 2.6-3.1 cm 4-16 minutes) (P < .05). There was no difference in mean diameter between cluster RF and MW ablations (RF 3.3-4.4 cm 4-16 minutes; P = .4-.9). In vivo lesion diameters for MW (and RF) were as follows: 2.6 cm ± 0.72 (RF 1.5 cm ± 0.14), 3.6 cm ± 0.89 (RF 2.0 cm ± 0.4), 3.4 cm ± 0.87 (RF 1.8 cm ± 0.23), and 3.8 cm ± 0.74 (RF 2.1 cm ± 0.3) at 2 minutes, 5 minutes, 7 minutes, and 10 minutes (P < .05 all time points).

CONCLUSIONS

Gas-cooled, high-powered MW ablation allows the generation of large ablation zones in short times.

摘要

目的

评估一种气体冷却、高功率微波系统的性能。

材料与方法

研究人员使用三种设备(单个 17 号冷射频(RF)电极、RF 电极簇和单个 17 号气体冷却微波[MW]天线)在离体牛肝中进行了 54 次消融,在三个时间点(n = 6,分别在 4 分钟、12 分钟和 16 分钟)进行了实验。使用基于阻抗的脉冲施加 RF 功率,最大发生器输出 200 W。以 2.45 GHz 持续输送 135 W 的 MW 功率。在 13 只国内猪中进行了一项经批准的体内研究。使用单极子和上述 MW 和 RF 发生器系统进行肝消融,治疗时间分别为 2 分钟(MW,n = 7;RF,n = 6)、5 分钟(MW,n = 23;RF,n = 8)、7 分钟(MW,n = 11;RF,n = 6)和 10 分钟(MW,n = 7;RF,n = 9)。使用方差分析(ANOVA)比较消融区域的平均横径和长度,并进行事后 t 检验和 Wilcoxon 秩和检验。

结果

在所有时间点,单个离体 MW 消融均大于单个 RF 消融(MW 平均直径范围 3.5-4.8 cm,4-16 分钟;RF 平均直径范围 2.6-3.1 cm,4-16 分钟)(P <.05)。RF 电极簇与 MW 消融的平均直径无差异(RF 3.3-4.4 cm,4-16 分钟;P =.4-.9)。MW(和 RF)体内病变直径分别为:2 分钟时 2.6 cm ± 0.72(RF 1.5 cm ± 0.14),5 分钟时 3.6 cm ± 0.89(RF 2.0 cm ± 0.4),7 分钟时 3.4 cm ± 0.87(RF 1.8 cm ± 0.23),10 分钟时 3.8 cm ± 0.74(RF 2.1 cm ± 0.3)(P <.05,所有时间点)。

结论

气体冷却、高功率 MW 消融可在短时间内产生大的消融区域。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/48d7/3289683/87f36da13c7e/nihms352437f1.jpg

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