Maeda T, Mori H, Hisada K, Kadoya S
Invest Radiol. 1977 Nov-Dec;12(6):555-8. doi: 10.1097/00004424-197711000-00017.
We have investigated the assessment of fluid flow through a Pudenz and a Rickham shunt using radioactive tracer. Experimentally, the radioactivity clearance curve obtained, using either shunt, is defined by two exponents. The relationship between flow-rate (F) and clearance half-time (T1/2) of the first component is identical with the clearance formula (formula: see text) or log10(F) =-LOG10(T1/2) + LOG100.693V using the physical volume. The value of the second component in a Pudenz 12 mm and a standard Rickman reservoir is log10(F) = -1.3LOG10(T1/2) + 0.087 and log 10(F) =-1.8log10(T1/2) + 0.019 respectively. In clinical practice, the first component may not be recorded adequately because the interval between appearance of the first and second components is very short. To calculate the CSF flow, we recommend referring to the line of "radioactivity clearance half-time and flow-rate" of the second component instead of the calculation based on clearance formula using a physical volume.
我们使用放射性示踪剂研究了通过普登兹分流管和里克姆分流管的液体流动评估。在实验中,使用任一分流管获得的放射性清除曲线由两个指数定义。第一成分的流速(F)与清除半衰期(T1/2)之间的关系与清除公式(公式:见正文)相同,或使用物理体积时为log10(F)=-LOG10(T1/2)+LOG100.693V。在12毫米的普登兹分流管和标准里克曼贮液器中,第二成分的值分别为log10(F)=-1.3LOG10(T1/2)+0.087和log10(F)=-1.8log10(T1/2)+0.019。在临床实践中,由于第一成分和第二成分出现的间隔非常短,第一成分可能无法得到充分记录。为了计算脑脊液流量,我们建议参考第二成分的“放射性清除半衰期和流速”曲线,而不是基于使用物理体积的清除公式进行计算。