Chemical Sciences Division, Lawrence Berkeley National Laboratory , Berkeley, California 94720, United States.
Department of Chemistry, University of California , Berkeley, California 94720, United States.
Anal Chem. 2017 Nov 21;89(22):12494-12501. doi: 10.1021/acs.analchem.7b03601. Epub 2017 Nov 8.
In-depth investigations of the kinetics of aqueous chemistry occurring in microdroplet environments require experimental techniques that allow a reaction to be initiated at a well-defined point in time and space. Merging microdroplets of different reactants is one such approach. The mixing dynamics of unconfined (airborne) microdroplets have yet to be studied in detail, which is an essential step toward widespread use and application of merged droplet microreactors for monitoring chemical reactions. Here, we present an on-demand experimental approach for initiating chemical reactions in and characterizing the mixing dynamics of colliding airborne microdroplets (40 ± 5 μm diameter) using a streak-based fluorescence microscopy technique. The advantages of this approach include the ability to generate two well-controlled monodisperse microdroplet streams and collide (and thus mix) the microdroplets with high spatial and temporal control while consuming small amounts of sample (<0.1 μL/s). Mixing times are influenced not only by the velocity at which microdroplets collide but also the geometry of the collision (i.e., head-on vs off-center collision). For head-on collisions, we achieve submillisecond mixing times ranging from ∼900 μs at a collision velocity of 0.1 m/s to <200 μs at ∼6 m/s. For low-velocity (<1 m/s) off-center collisions, mixing times were consistent with the head-on cases. For high-velocity (i.e., > 1 m/s) off-center collisions, mixing times increased by as much as a factor of 6 (e.g., at ∼6 m/s, mixing times increased from <200 μs for head-on collisions to ∼1200 μs for highly off-center collisions). At collision velocities >7 m/s, droplet separation and fragmentation occurred, resulting in incomplete mixing. These results suggest a limited range of collision velocities over which complete and rapid mixing can be achieved when using airborne merged microdroplets to, e.g., study reaction kinetics when reaction times are short relative to typical bulk reactor mixing times. We benchmark our reactor using an aqueous-phase oxidation reaction: iron-catalyzed hydroxyl radical production from hydrogen peroxide (Fenton's reaction) and subsequent aqueous-phase oxidation of organic species in solution. Kinetic simulations of our measurements show that quantitative agreement can be obtained using known bulk-phase kinetics for bimolecular reactions in our colliding-droplet microreactor.
深入研究发生在微滴环境中的水相化学反应动力学需要实验技术,该技术允许在明确的时间和空间点引发反应。合并不同反应物的微滴就是这样一种方法。未约束(空气传播)微滴的混合动力学尚未得到详细研究,这是广泛使用和应用合并微滴微反应器来监测化学反应的关键步骤。在这里,我们提出了一种按需实验方法,用于在碰撞空气传播微滴(40 ± 5 μm 直径)中引发化学反应,并使用基于条纹的荧光显微镜技术对混合动力学进行表征。该方法的优点包括能够生成两个控制良好的单分散微滴流并以高时空控制碰撞(从而混合)微滴,同时消耗少量样品(<0.1 μL/s)。混合时间不仅受微滴碰撞速度的影响,还受碰撞几何形状(即迎面碰撞与偏心碰撞)的影响。对于迎面碰撞,我们实现了亚毫秒级的混合时间,范围从 0.1 m/s 的碰撞速度下的约 900 μs 到 6 m/s 下的 <200 μs。对于低速度(<1 m/s)偏心碰撞,混合时间与迎面碰撞情况一致。对于高速(即>1 m/s)偏心碰撞,混合时间增加了多达 6 倍(例如,在约 6 m/s 下,混合时间从迎面碰撞的 <200 μs 增加到高度偏心碰撞的约 1200 μs)。在碰撞速度>7 m/s 时,液滴分离和碎裂发生,导致混合不完全。这些结果表明,在使用空气传播的合并微滴来研究例如与典型的批量反应器混合时间相比反应时间较短的反应动力学时,碰撞速度存在有限的范围,可以实现完全和快速的混合。我们使用水相氧化反应来基准测试我们的反应器:铁催化过氧化氢产生羟基自由基(芬顿反应)和随后溶液中有机物质的水相氧化。我们测量的动力学模拟表明,在我们的碰撞微滴微反应器中,对于双分子反应,可以使用已知的体相动力学获得定量一致性。