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Effects of intracavitary blood flow and electrode-target distance on radiofrequency power required for transient conduction block in a Langendorff-perfused canine model

机译:腔内血流和电极目标距离对Langendorff灌注犬模型中瞬时传导阻滞所需的射频功率的影响

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摘要

OBJECTIVES: We sought to quantify the effects of electrode-target distance and intracavitary blood flow on radiofrequency (RF) power required to induce transient conduction block, using a Langendorff-perfused canine ablation model. BACKGROUND: Given the thermally mediated nature of RF catheter ablation, cooling effects of intracavitary blood flow and electrode-target distance will influence lesion extension and geometry and electrophysiologic effects. METHODS: In eight Langendorff-perfused canine hearts, the right ventricular free wall was opened, and the right bundle branch (RBB) carefully localized by multielectrode activation mapping. The right atrium was paced at cycle length of 500 ms. Proximal and distal electrodes were attached at the endocardial aspect of the RBB, and the perfused heart was submerged in heparinized blood at 37 degrees C. A standard 4-mm tip ablation electrode was positioned at a constant contact pressure of 5 g between the two electrodes at the site of maximal RBB potential (0 mm) and 2 and 4 mm distant from this site along a line perpendicular to the RBB. RF pulses (500 kHz) were delivered for 30 s at 0.5-W increments until transient bundle branch block. In four hearts, intracavitary flow was simulated by directing a 30-cm/s jet of blood parallel to the septum at the ablation site, and the protocol was repeated to assess the effects on power required for block. In one heart, the effect of variable flow was assessed (0, 15 and 30 cm/s). RESULTS: An exponential distance-related increase was seen in power required for block, from 1.8 +/- 0.9 W (mean +/- SD) at 0 mm to 5.4 +/- 1.1 W at 4 mm. In the presence of 30-cm/s flow, an increase to 3.9 +/- 0.8 W at 0 mm and 13.1 +/- 2.4 W at 2 mm was seen. At 4 mm, coagulum formation invariably occurred before block could be induced. For 15-cm/s flow, less power was required: 3 and 7 W at 0 and 2 mm, respectively. CONCLUSIONS: Increasing the ablation electrode-target distance causes an exponential increase in power required for conduction block; this relation is profoundly influenced by intracavitary flow. Given the geometry of endomyocardial RF lesions, these findings are particularly relevant for directly subendocardial ablation targets
机译:目的:我们试图使用Langendorff灌注犬消融模型来量化电极靶距和腔内血流对诱导瞬时传导阻滞所需的射频(RF)功率的影响。背景:鉴于射频导管消融的热介导性质,腔内血流的冷却效果和电极-目标距离将影响病变的扩展以及几何形状和电生理效果。方法:在八个Langendorff灌注犬的心脏中,右心室游离壁被打开,右束支(RBB)通过多电极激活作图仔细定位。右心房以500毫秒的周期长度起搏。在RBB的心内膜一侧连接近端和远端电极,并将灌注的心脏浸入37摄氏度的肝素化血液中。将标准的4毫米尖端消融电极放置在两个电极之间的5 g恒定接触压力下在最大RBB电位(0 mm)的位置,并且沿着垂直于RBB的线与该位置相距2和4 mm。 RF脉冲(500 kHz)以0.5 W的增量传送30 s,直到出现瞬态束支传导阻滞为止。在四个心脏中,通过在消融部位平行于隔垫引导30-cm / s的血流来模拟腔内血流,并重复该方案以评估对阻塞所需的功率的影响。在一颗心脏中,评估了流量可变的影响(0、15和30 cm / s)。结果:阻滞所需的功率呈指数增长,从0毫米处的1.8 +/- 0.9 W(平均+/- SD)增加到4毫米处的5.4 +/- 1.1W。在流量为30 cm / s的情况下,在0 mm处增加到3.9 +/- 0.8 W,在2 mm处增加到13.1 +/- 2.4W。在4 mm处,凝块的形成总是在诱发阻塞之前发生。对于15 cm / s的流量,需要的功率更少:分别在0和2 mm时为3 W和7W。结论:消融电极-目标距离的增加导致传导阻滞所需功率的指数增长;这种关系深受腔内流动的影响。考虑到心内膜RF病变的几何形状,这些发现与直接心内膜下消融靶特别相关

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