Deuerling Julian, Keck Shaun, Moelyadi Inasya, Repke Jens-Uwe, Rädle Matthias
Center for Mass Spectrometry and Optical Spectroscopy, Mannheim University of Applied Sciences, 68163 Mannheim, Germany.
Technical University of Berlin, Fakultät 3 Prozesswissenschaften, 10623 Berlin, Germany.
Micromachines (Basel). 2021 Jan 22;12(2):116. doi: 10.3390/mi12020116.
This work presents a novel method for the non-invasive, in-line monitoring of mixing processes in microchannels using the Raman photometric technique. The measuring set-up distinguishes itself from other works in this field by utilizing recent state-of-the-art customized photon multiplier (CPM) detectors, bypassing the use of a spectrometer. This addresses the limiting factor of integration times by achieving measuring rates of 10 ms. The method was validated using the ternary system of toluene-water-acetone. The optical measuring system consists of two functional units: the coaxial Raman probe optimized for excitation at a laser wavelength of 532 nm and the photometric detector centered around the CPMs. The spot size of the focused laser is a defining factor of the spatial resolution of the set-up. The depth of focus is measured at approx. 85 µm with a spot size of approx. 45 µm, while still maintaining a relatively high numerical aperture of 0.42, the latter of which is also critical for coaxial detection of inelastically scattered photons. The working distance in this set-up is 20 mm. The microchannel is a T-junction mixer with a square cross section of 500 by 500 µm, a hydraulic diameter of 500 µm and 70 mm channel length. The extraction of acetone from toluene into water is tracked at an initial concentration of 25% as a function of flow rate and accordingly residence time. The investigated flow rates ranged from 0.1 mL/min to 0.006 mL/min. The residence times from the T-junction to the measuring point varies from 1.5 to 25 s. At 0.006 mL/min a constant acetone concentration of approx. 12.6% was measured, indicating that the mixing process reached the equilibrium of the system at approx. 12.5%. For prototype benchmarking, comparative measurements were carried out with a commercially available Raman spectrometer (RXN1, Kaiser Optical Systems, Ann Arbor, MI, USA). Count rates of the spectrophotometer surpassed those of the spectrometer by at least one order of magnitude at identical target concentrations and optical power output. The experimental data demonstrate the suitability and potential of the new measuring system to detect locally and time-resolved concentration profiles in moving fluids while avoiding external influence.
这项工作提出了一种使用拉曼光度技术对微通道中的混合过程进行非侵入式在线监测的新方法。该测量装置通过利用最新的定制光子倍增管(CPM)探测器,区别于该领域的其他工作,无需使用光谱仪。这通过实现10毫秒的测量速率解决了积分时间的限制因素。该方法使用甲苯 - 水 - 丙酮三元体系进行了验证。光学测量系统由两个功能单元组成:针对532纳米激光波长激发优化的同轴拉曼探头和以CPM为中心的光度探测器。聚焦激光的光斑尺寸是该装置空间分辨率的决定性因素。在光斑尺寸约为45微米时,焦深测量约为85微米,同时仍保持相对较高的数值孔径0.42,后者对于非弹性散射光子的同轴检测也至关重要。该装置中的工作距离为20毫米。微通道是一个T型结混合器,方形横截面为500×500微米,水力,水力直径为500微米,通道长度为70毫米。跟踪从甲苯中提取丙酮到水中的过程,初始浓度为25%,作为流速和相应停留时间的函数。研究的流速范围为0.1毫升/分钟至0.006毫升/分钟。从T型结到测量点的停留时间从1.5秒到25秒不等。在0.006毫升/分钟时,测量到丙酮浓度恒定约为12.6%,表明混合过程在约12.5%时达到了系统平衡。为了进行原型基准测试,使用市售拉曼光谱仪(RXN1,美国密歇根州安阿伯市凯泽光学系统公司)进行了对比测量。在相同的目标浓度和光功率输出下,分光光度计的计数率比光谱仪至少高出一个数量级。实验数据证明了新测量系统在检测流动流体中局部和时间分辨浓度分布的适用性和潜力,同时避免了外部影响。