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首页> 外文期刊>Medicine. >Heat Sink Effect on Tumor Ablation Characteristics as Observed in Monopolar Radiofrequency, Bipolar Radiofrequency, and Microwave, Using Ex Vivo Calf Liver Model
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Heat Sink Effect on Tumor Ablation Characteristics as Observed in Monopolar Radiofrequency, Bipolar Radiofrequency, and Microwave, Using Ex Vivo Calf Liver Model

机译:使用体外小牛肝模型在单极射频,双极射频和微波中观察到的散热对肿瘤消融特性的影响

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Abstract: Thermal ablation of liver tumors near large blood vessels is affected by the cooling effect of blood flow, leading to incomplete ablation. Hence, we conducted a comparative investigation of heat sink effect in monopolar (MP) and bipolar (BP) radiofrequency ablation (RFA), and microwave (MW) ablation devices. With a perfused calf liver, the ablative performances (volume, mass, density, dimensions), with and without heat sink, were measured. Heat sink was present when the ablative tip of the probes were 8.0?mm close to a major hepatic vein and absent when >30?mm away. Temperatures (T1 and T2) on either side of the hepatic vein near the tip of the probes, heating probe temperature (T3), outlet perfusate temperature (T4), and ablation time were monitored. With or without heat sink, BP radiofrequency ablated a larger volume and mass, compared with MP RFA or MW ablation, with latter device producing the highest density of tissue ablated. MW ablation produced an ellipsoidal shape while radiofrequency devices produced spheres. Percentage heat sink effect in Bipolar radiofrequency : Mono-polar radiofrequency : Microwave was (Volume) 33:41:22; (mass) 23:56:34; (density) 9.0:26:18; and (relative elipscity) 5.8:12.9:1.3, indicating that BP and MW devices were less affected. Percentage heat sink effect on time (minutes) to reach maximum temperature (W)?=?13.28:9.2:29.8; time at maximum temperature (X) is 87:66:16.66; temperature difference (Y) between the thermal probes (T3) and the temperature (T1?+?T2)/2 on either side of the hepatic vessel was 100:87:20; and temperature difference between the (T1?+?T2)/2 and temperature of outlet circulating solution (T4), Z was 20.33:30.23:37.5. MW and BP radiofrequencies were less affected by heat sink while MP RFA was the most affected. With a single ablation, BP radiofrequency ablated a larger volume and mass regardless of heat sink.
机译:摘要:大血管附近肝肿瘤的热消融受血流冷却作用的影响,导致不完全消融。因此,我们对单极(MP)和双极(BP)射频消融(RFA)和微波(MW)消融设备中的散热效果进行了比较研究。使用灌注小牛肝,测量有无散热片的消融性能(体积,质量,密度,尺寸)。当探头的消融尖端靠近肝大静脉有8.0?mm时存在散热片,而当距离> 30?mm时则不存在。监测探头尖端附近肝静脉两侧的温度(T1和T2),加热探头温度(T3),出口灌注液温度(T4)和消融时间。有或没有散热器,与MP RFA或MW消融相比,BP射频消融的体积和质量更大,后者的设备产生的组织消融密度最高。兆瓦消融产生椭圆形,而射频装置产生球形。双极射频中的散热百分比效应:单极射频:微波为(体积)33:41:22; (质量)23:56:34; (密度)9.0:26:18; 5.8:12.9:1.3(相对隐性),表明BP和MW装置受到的影响较小。散热片对达到最高温度(W)的时间的影响(分钟)≥13.28:9.2:29.8;最高温度(X)的时间为87:66:16.66;热探头(T3)与肝容器任一侧的温度(T1 ++ T2)/ 2之间的温度差(Y)为100∶87∶20。 (T1 ++ T2)/ 2与出口循环液温度(T4)之间的温差Z为20.33:30.23:37.5。 MW和BP射频受散热器的影响较小,而MP RFA受影响最大。通过单次消融,BP射频消融了更大的体积和质量,而与散热片无关。

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