Department of Urologic Sciences, University of British Columbia, Vancouver, British Columbia, Canada.
J Urol. 2012 Mar;187(3):914-9. doi: 10.1016/j.juro.2011.10.147. Epub 2012 Jan 20.
We determined the optimal Ho:YAG lithotripsy power settings to achieve maximal fragmentation, minimal fragment size and minimal retropulsion.
Stone phantoms were irradiated in water with a Ho:YAG laser using a 365 μm optical fiber. Six distinct power settings were tested, including 0.2 to 2.0 J and 10 to 40 Hz. For all cohorts 500 J total radiant energy were delivered. A seventh cohort (0.2 J 40 Hz) was tested post hoc to a total energy of 1,250 J. Two experimental conditions were tested, including with and without phantom stabilization. Total fragmentation, fragment size and retropulsion were characterized. In mechanism experiments using human calculi we measured crater volume by optical coherence tomography and pressure transients by needle hydrophone across similar power settings.
Without stabilization increased pulse energy settings produced increased total fragmentation and increased retropulsion (each p <0.0001). Fragment size was smallest for the 0.2 J cohorts (p <0.02). With stabilization increased pulse energy settings produced increased total fragmentation and increased retropulsion but also increased fragment size (each p <0.0001). Craters remained symmetrical and volume increased as pulse energy increased. Pressure transients remained modest at less than 30 bars even at 2.0 J pulse energy.
Holmium:YAG lithotripsy varies as pulse energy settings vary. At low pulse energy (0.2 J) less fragmentation and retropulsion occur and small fragments are produced. At high pulse energy (2.0 J) more fragmentation and retropulsion occur with larger fragments. Anti-retropulsion devices produce more efficient lithotripsy, particularly at high pulse energy. Optimal lithotripsy laser dosimetry depends on the desired outcome.
我们确定了 Ho:YAG 碎石术的最佳激光功率设置,以实现最大的碎石效果、最小的碎石粒径和最小的后向反冲。
使用 365µm 光纤,将结石模型置于水中用 Ho:YAG 激光照射。共测试了 6 种不同的功率设置,包括 0.2 至 2.0 J 和 10 至 40 Hz。所有组别的总辐射能量均为 500 J。第七组(0.2 J 40 Hz)的总能量为 1250 J。在无结石模型稳定和有结石模型稳定两种实验条件下,对所有组进行了总碎石效果、碎石粒径和后向反冲的评估。在使用人结石的机制实验中,我们通过光学相干断层扫描(OCT)测量了空化效应形成的凹坑体积,通过针状水听器测量了压力瞬变,所用功率设置与上述实验相同。
无结石模型稳定时,增加脉冲能量会增加总碎石效果和后向反冲(均 p<0.0001)。0.2 J 组的碎石粒径最小(p<0.02)。有结石模型稳定时,增加脉冲能量会增加总碎石效果和后向反冲,但也会增加碎石粒径(均 p<0.0001)。凹坑始终保持对称,随着脉冲能量的增加而增大。即使在 2.0 J 脉冲能量下,压力瞬变也保持在 30 巴以下。
钬激光碎石术随脉冲能量设置而变化。在低脉冲能量(0.2 J)时,碎石效果和后向反冲较小,产生的碎石粒径较小。在高脉冲能量(2.0 J)时,碎石效果和后向反冲较大,产生的碎石粒径较大。反后向冲装置可提高碎石效率,尤其是在高脉冲能量时。最佳碎石激光剂量取决于预期的结果。