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Comparison of temperature change and resulting ablation size induced by a 902–928 MHz and a 2450 MHz microwave ablation system in in-vivo porcine kidneys

机译:温度变化的比较和诱导的902-928MHz诱导的烧蚀尺寸,在体内猪肾脏中的2450MHz微波消融系统诱导

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摘要

Introduction: Microwave ablation (MWA) uses heat to ablate undesired tissue. Development of pre-planning algorithms for MWA of small renal masses requires understanding of microwave-tissue interactions at different operating parameters. The objective of this study was to compare the performance of two MWA systems in in-vivo porcine kidneys. Methods: Five ablations were performed using a 902–928 MHz system (24 W, 5 min) and a 2450 MHz system (180 W, 2 min). Nonlinear regression analysis of temperature changes measured 5 mm from the antenna axis was completed for the initial 10 s of ablation using the power equation and after the inflection point using an exponential equation. Thermal damage was calculated using the Arrhenius equation. Long and short axis ablation diameters were measured. Results: The average ‘a’ varied significantly between systems (902–928 MHz: 0.0299 ± 0.027, 2450 MHz: 0.1598 ± 0.158), indicating proportionality to the heat source, but ‘b’ did not (902–928 MHz: 1.910 ± 0.372, 2450 MHz: 2.039 ± 0.366), signifying tissue type dependence. Past the inflection point, average steady-state temperature increases were similar between systems but reached more quickly with the 2450 MHz system. Complete damage was reached at 5 mm for both systems. The 2450 MHz system produced significantly larger short axis ablations (902–928 MHz: 2.40 ± 0.54 cm, 2450 MHz: 3.32 ± 0.41cm). Conclusion: The 2450 MHz system achieved similar steady state temperature increases compared to the 902–928 MHz system, but more quickly due to higher output power. Further investigations using various treatment parameters and precise thermal sensor placement are warranted to refine equation parameters for the development of an ablation model.
机译:简介:微波消融(MWA)使用热量来消融不良组织。小肾群体MWA预先规划算法的开发需要了解不同操作参数的微波 - 组织相互作用。本研究的目的是比较两种MWA系统在体内猪肾脏的性能。方法:使用902-928MHz系统(24W,5分钟)和2450MHz系统(180W,2分钟)进行五次消融。使用指数方程,完成从天线轴线测量5mm的温度变化的温度变化的非线性回归分析,以便使用指数方程在拐点之后的拐点。使用Arrhenius方程计算热损坏。测量了长短的轴消融直径。结果:平均值'A'在系统之间显着变化(902-928MHz:0.0299±0.027,2050MHz:0.1598±0.158),表明对热源的比例,但'B'没有(902-928 MHz:1.910± 0.372,2450 MHz:2.039±0.366),表示组织类型依赖。经过拐点,系统之间平均稳态温度越来越相似,但与2450 MHz系统更快地达到。两个系统的5毫米达到完全损坏。 2450 MHz系统产生明显较大的短轴消融(902-928MHz:2.40±0.54厘米,2450MHz:3.32±0.41cm)。结论:与902-928 MHz系统相比,2450 MHz系统达到了类似的稳态温度升高,但由于输出功率较高,更快。使用各种治疗参数和精确的热传感器放置的进一步调查是为了细化用于开发消融模型的方程参数。

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