首页> 外文期刊>Journal of endourology >Effect of Holmium:YAG Laser Pulse Width on Lithotripsy Retropulsion in Vitro.
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Effect of Holmium:YAG Laser Pulse Width on Lithotripsy Retropulsion in Vitro.

机译::: YAG激光脉冲宽度对体外碎石反冲的影响。

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Background and Purpose: The effect of laser pulse width on calculus retropulsion during ureteroscopic lithotripsy is poorly defined because of the limited availability of variable pulse-width lasers. We used an adjustable pulse-width Ho:YAG laser to test the effect of pulse width on in vitro phantom-stone retropulsion and fragmentation efficiency. Methods and Materials: An Odyssey 30 Ho:YAG laser (Convergent Laser Technologies, Oakland, CA) with adjustable pulse width (350 or 700 microsec) was used to treat spherical 10-mm plaster calculi in a model ureter (N = 40) and calix (N = 16) utilizing 200- and 400-microm fibers (10 Hz, 1.0 J). Calculi were placed in a waterfilled clear polymer tube, and laser energy was applied continuously in near contact until the stone had moved 8 cm. The time (seconds) and energy (joules) needed to cause the stone to traverse this distance was recorded. Stones were also placed in a stainless-steel mesh calix model in which retropulsion was limited. Laser energy was appliedfor 5 minutes at each pulse width. A laser-energy meter (Molectron Detector Inc, Portland OR) was used to quantify fiber transmission efficiency after 1 minute of continuous lithotripsy for each fiber at each pulse width. Results: Retropulsion was greater for stones treated at 350 microsec, indicated by a shorter time to traverse the model ureter. For the 200-microrm fiber at 350 microrsec, the average time was 11.5 seconds v 20.3 seconds at 700 microsec (P < 0.001). The average total energy delivered was 114.9 J at 350 microsec v 199.8 J at 700 microsec (P < 0.001). For the 400-microm fiber at 350 microsec, the average time was 5.8 seconds v 11.9 seconds at 700 microsec (P < 0.001). The average total energy was 57.1 J at 350 microsec v 127.3 J at 700 microsec (P < 0.001). In the caliceal model, at 350 and 700 microsec with the 200- and 400-microm fibers, mass loss was 34.9% and 33.4% (P = 0.8) and 14.6% and 21.6% (P = 0.04), respectively. The reduction in energy transmission at 350 microsec and 700 microsec with the 200- microm fiber after 60 seconds of continuous lasing was 8.82% v 9%, respectively (P = 0.95). For the 400-microm fiber, the transmission loss was 18.4% at 350 microsec v 4.4% at 700 microsec (P = 0.0002). Conclusion: When treating ureteral calculi, retropulsion can be reduced by using a longer pulse width without compromising fragmentation efficiency. For caliceal calculi, the longer pulse width in combination with a 400-microm fiber provides more effective stone fragmentation.
机译:背景与目的:由于可变脉宽激光的可用性有限,因此在输尿管镜碎石术中激光脉冲宽度对结石反冲的影响定义不清。我们使用可调脉冲宽度的Ho:YAG激光来测试脉冲宽度对体外幻影石反冲和破碎效率的影响。方法和材料:使用可调节脉冲宽度(350或700微秒)的Odyssey 30 Ho:YAG激光(Convergent Laser Technologies,奥克兰,加利福尼亚)在模型输尿管(N = 40)中处理球形10毫米石膏结石,并杯(N = 16)使用200和400微米的光纤(10 Hz,1.0 J)。将结石放置在充满水的透明聚合物管中,并以接近接触的方式连续施加激光能量,直到石头移动了8厘米。记录使石材穿过该距离所需的时间(秒)和能量(焦耳)。石头也被放置在不锈钢网状杯模型中,在该模型中反冲受到限制。在每个脉冲宽度处施加激光能量5分钟。使用激光能量计(Molectron Detector Inc,波特兰或俄勒冈州)来量化每个脉冲宽度下每根光纤连续碎石1分钟后的光纤传输效率。结果:350微秒处理的结石的反冲力更大,这表明横穿模型输尿管的时间较短。对于在350微秒下200微米的光纤,平均时间为700微秒下的11.5秒对20.3秒(P <0.001)。在350微秒下传递的平均总能量为114.9 J,在700微秒下传递为199.8 J(P <0.001)。对于350微秒时的400微米光纤,平均时间为700微秒时的5.8秒对11.9秒(P <0.001)。 350微秒时的平均总能量为57.1 J,700微秒时的平均总能量为127.3 J(P <0.001)。在caliceal模型中,使用200和400微米纤维在350和700微秒处的质量损失分别为34.9%和33.4%(P = 0.8)和14.6%和21.6%(P = 0.04)。连续发射激光60秒钟后,使用200微米光纤在350微秒和700微秒处的能量传输减少分别为8.82%对9%(P = 0.95)。对于400微米的光纤,传输损耗在350微秒时为18.4%,在700微秒时为4.4%(P = 0.0002)。结论:在治疗输尿管结石时,可以通过使用更长的脉冲宽度来减少反冲,而不会影响碎裂效率。对于钙结石,较长的脉冲宽度与400微米的纤维相结合可提供更有效的碎石效果。

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