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在犬大腿肌肉制备中,使用盐水灌注电极进行射频消融时体内组织温度分布和损伤几何形状与温度控制的比较。

Comparison of in vivo tissue temperature profile and lesion geometry for radiofrequency ablation with a saline-irrigated electrode versus temperature control in a canine thigh muscle preparation.

作者信息

Nakagawa H, Yamanashi W S, Pitha J V, Arruda M, Wang X, Ohtomo K, Beckman K J, McClelland J H, Lazzara R, Jackman W M

机构信息

Department of Medicine, University of Oklahoma Health Sciences Center, Oklahoma City 73190-3048, USA.

出版信息

Circulation. 1995 Apr 15;91(8):2264-73. doi: 10.1161/01.cir.91.8.2264.

Abstract

BACKGROUND

It is thought that only a thin layer of tissue adjacent to the electrode is heated directly by electrical current (resistive heating) during radiofrequency ablation. Most of the thermal injury is thought to result from conduction of heat from the surface layer. The purpose of this study was to determine whether lesion depth could be increased by producing direct resistive heating deeper in the tissue with higher radiofrequency power, allowed by cooling the ablation electrode with saline irrigation to prevent the rise in impedance that occurs when the electrode-tissue interface temperature reaches 100 degrees C.

METHODS AND RESULTS

In 11 anesthetized dogs, the thigh muscle was exposed and bathed with heparinized canine blood (36 degrees C to 37 degrees C). A 7F catheter, with a central lumen, a 5-mm tip electrode with six irrigation holes, and an internal thermistor, was positioned perpendicular to the thigh muscle and held at a constant contact weight of 10 g. Radiofrequency current was delivered to 145 sites (1) at high constant voltage (66 V) without irrigation (CV group, n = 31), (2) at variable voltage (20 to 66 V) to maintain tip-electrode temperature at 80 degrees C to 90 degrees C without irrigation (temperature-control group, n = 39), and (3) at high CV (66 V) with saline irrigation through the catheter lumen and ablation electrode at 20 mL/min (CV irrigation group, n = 75). Radiofrequency current was applied for 60 seconds but was terminated immediately in the event of an impedance rise > or = 10 omega. Tip-electrode temperature and tissue temperature at depths of 3.5 and 7.0 mm were measured in all three groups (n = 145). In 33 CV irrigation group applications, temperature was also measured with a separate probe at the center (n = 18) or edge (n = 15) of the electrode-tissue interface. In all 31 CV group applications, radiofrequency energy delivery was terminated prematurely (at 11.6 +/- 4.8 seconds) owing to an impedance rise associated with an electrode temperature of 98.8 +/- 2.1 degrees C. All 39 temperature-control applications were delivered for 60 seconds without an impedance rise, but voltage had to be reduced to 38.4 +/- 6.1 V to avoid temperatures > 90 degrees C (mean tip-electrode temperature, 84.5 +/- 1.4 degrees C). In CV irrigation applications, the tip-electrode temperature was not > 48 degrees C (mean, 38.4 +/- 5.1 degrees C) and the electrode-tissue interface temperature was not > 80 degrees C (mean, 69.4 +/- 5.7 degrees C). An abrupt impedance rise with an audible pop and without coagulum occurred in 6 of 75 CV irrigation group applications at 30 to 51 seconds, probably owing to release of steam from below the surface. In the CV and temperature-control group applications, the temperatures at depths of 3.5 (62.1 +/- 15.1 degrees C and 67.9 +/- 7.5 degrees C) and 7.0 mm (40.3 +/- 5.3 degrees C and 48.3 +/- 4.8 degrees C) were always lower than the electrode temperature. Conversely, in CV irrigation group applications, electrode and electrode-tissue interface temperatures were consistently exceeded by the tissue temperature at depths of 3.5 mm (94.7 +/- 9.1 degrees C) and occasionally 7.0 mm (65.1 +/- 9.7 degrees C). Lesion dimensions were smallest in CV group applications (depth, 4.7 +/- 0.6 mm; maximal diameter, 9.8 +/- 0.8 mm; volume, 135 +/- 33 mm3), intermediate in temperature-control group applications (depth, 6.1 +/- 0.5 mm; maximal diameter, 11.3 +/- 0.9 mm; volume, 275 +/- 55 mm3), and largest in CV irrigation group applications (depth, 9.9 +/- 1.1 mm; maximal diameter, 14.3 +/- 1.5 mm; volume, 700 +/- 217 mm3; P < .01, respectively).

CONCLUSIONS

Saline irrigation maintains a low electrode-tissue interface temperature during radiofrequency application at high power, which prevents an impedance rise and produces deeper and larger lesions. A higher temperature in the tissue (3.5 mm deep) than at the electrode-tissue interface indicates that direct resistive heating occurred deeper

摘要

背景

人们认为在射频消融过程中,只有紧邻电极的一薄层组织会被电流直接加热(电阻性加热)。多数热损伤被认为是由表层传导而来的热量导致的。本研究的目的是确定通过用盐水冲洗冷却消融电极以防止电极 - 组织界面温度达到100℃时出现的阻抗升高,从而在组织更深层产生直接电阻性加热,是否能够增加损伤深度。

方法与结果

在11只麻醉犬中,暴露大腿肌肉并用肝素化犬血(36℃至37℃)冲洗。将一根带有中心腔、带有六个冲洗孔的5毫米尖端电极和一个内部热敏电阻的7F导管垂直放置于大腿肌肉上,并保持10克的恒定接触重量。射频电流被输送到145个部位:(1)在高恒定电压(66V)下不进行冲洗(CV组,n = 31);(2)在可变电压(20至66V)下以将尖端电极温度维持在80℃至90℃且不进行冲洗(温度控制组,n = 39);(3)在高CV(66V)下通过导管腔和消融电极以20 mL/分钟的速度进行盐水冲洗(CV冲洗组,n = 75)。施加射频电流60秒,但如果阻抗升高≥10Ω则立即终止。在所有三组(n = 145)中测量了3.5毫米和7.0毫米深度处的尖端电极温度和组织温度。在CV冲洗组的33次应用中,还使用单独的探头在电极 - 组织界面的中心(n = 18)或边缘(n = 15)测量了温度。在CV组的所有31次应用中,由于与电极温度98.8±2.1℃相关的阻抗升高,射频能量输送提前终止(在11.6±4.8秒)。所有39次温度控制应用均持续60秒且无阻抗升高,但必须将电压降至38.4±6.1V以避免温度>90℃(平均尖端电极温度,84.5±1.4℃)。在CV冲洗应用中,尖端电极温度不>48℃(平均,38.4±5.1℃)且电极 - 组织界面温度不>80℃(平均,69.4±5.7℃)。在CV冲洗组的75次应用中有6次在30至51秒时出现突然的阻抗升高并伴有可闻的爆裂声且无凝块,可能是由于表面下方蒸汽的释放。在CV组和温度控制组的应用中,3.5毫米(62.1±15.1℃和67.9±7.5℃)和7.0毫米(40.3±5.3℃和48.3±4.8℃)深度处的温度始终低于电极温度。相反,在CV冲洗组的应用中,3.5毫米深度处(94.7±9.1℃)的组织温度始终超过电极和电极 - 组织界面温度,7.0毫米深度处(65.1±9.7℃)偶尔超过。CV组应用中的损伤尺寸最小(深度,4.7±0.6毫米;最大直径,9.8±0.8毫米;体积,135±33立方毫米),温度控制组应用中的损伤尺寸居中(深度,6.1±0.5毫米;最大直径,11.3±0.9毫米;体积,275±55立方毫米),CV冲洗组应用中的损伤尺寸最大(深度,9.9±1.1毫米;最大直径,14.3±1.5毫米;体积,700±217立方毫米;P均<.01)。

结论

在高功率射频应用期间,盐水冲洗可维持较低的电极 - 组织界面温度,这可防止阻抗升高并产生更深更大的损伤。组织(3.5毫米深处)温度高于电极 - 组织界面温度表明在更深层发生了直接电阻性加热

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