作为气动管道输送(PTT)操作变量的抖动(d(加速度)/dt)。

Christopher J Mattiello, Douglas F Stickle
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引用次数: 0

摘要

背景:加速度变化率(d(acceleration)/dt)是公共交通安全中的一个已知操作变量,但这一术语从未出现在有关气动管道输送(PTT)和标本完整性的文献中。我们调查了本医院系统内 2 条 PTT 线路的加速度和颠簸曲线:方法:使用加速度计收集了 2 条 PTT 线路(A、B)的加速度数据。分析了加速度矢量(a)的颠簸分布(da/dt)和连续加速度矢量间夹角θ的分布:加速度矢量(a)的大小从 0 到 8 g 不等。在 B 线路中,a > 1.2 g 的结果占 29.0%,而在 A 线路中,a > 1.2 g 的结果占 13.5%(比率 = 2.1)。挺举范围为 0 至 94 克/秒。对于 B,挺举 > 0.5 g/s 的结果占 71.9%,而 A 的结果占 32.5%(比率 = 2.2)。对于 B,θ > 5 度的结果占 59.3%,而 A 的结果占 26.6%(比率 = 2.2):结论:加速度、挺举和θ的分布差异是两种 PTT 路线并行比较的变量。挺举和θ很可能是影响 PTT 的有效变量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Jerk (d(acceleration)/dt) as an operative variable in pneumatic tube transport (PTT).

Background: Jerk, the rate of change of acceleration (d(acceleration)/dt), is a known operative variable in public transportation safety, but this term has never appeared in the literature regarding pneumatic tube transport (PTT) and specimen integrity. We investigated profiles of acceleration and jerk for 2 PTT routes within our hospital system.

Methods: Acceleration data were collected for PTT for 2 routes (A, B) using an accelerometer. Acceleration vectors (a) were analyzed in terms of distributions of jerk (da/dt), and distributions of θ, the angle between successive acceleration vectors.

Results: Routes A and B had transit times of approximately 300 s. Acceleration vectors (a) ranged in magnitude from 0 to 8 g. For B, a > 1.2 g comprised 29.0% of results, compared to 13.5% of results for A (ratio = 2.1). Jerk ranged from 0 to 94 g/s. For B, jerk > 0.5 g/s comprised 71.9% of results, compared to 32.5% of results for A (ratio = 2.2). θ ranged from 0 to 180 degrees. For B, θ > 5 degrees comprised 59.3% of results, compared to 26.6% of results for A (ratio = 2.2).

Conclusion: Differences in distribution in acceleration, jerk, and θ ran in parallel as variables for comparison between 2 PTT routes. Jerk and θ are likely to be operative variables in effects of PTT.

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