Ahmed Junaid U, Lutkenhaus John A, Alam Muhammad S, Marshall Ivan, Paul Dilip K, Alvarez Julio C
Chemistry Department, Virginia Commonwealth University, Richmond, Virginia 23284, United States.
Electrical and Computer Engineering, Virginia Commonwealth University, Richmond, Virginia 23284, United States.
Anal Chem. 2021 Jun 8;93(22):7993-8001. doi: 10.1021/acs.analchem.1c01027. Epub 2021 May 27.
Current-time recordings of emulsified toluene microdroplets containing 20 mM Ferrocene (Fc), show electrochemical oxidation peaks from individual adsorption events on disk microelectrodes (5 μm diameter). The average droplet diameter (∼0.7 μm) determined from peak area integration was close to Dynamic Light Scattering measurements (∼1 μm). Random walk simulations were performed deriving equations for droplet electrolysis using the diffusion and thermal velocity expressions from Einstein. The simulations show that multiple droplet-electrode collisions, lasting ∼0.11 μs each, occur before a droplet wanders away. Updating the Fc-concentration at every collision shows that a droplet only oxidizes ∼0.58% of its content in one collisional journey. In fact, it would take ∼5.45 × 10 collisions and ∼1.26 h to electrolyze the Fc in one droplet with the collision frequency derived from the thermal velocity (∼0.52 cm/s) of a 1 μm-droplet. To simulate adsorption, the droplet was immobilized at first contact with the electrode while the electrolysis current was computed. This approach along with modeling of instrumental filtering, produced the best match of experimental peaks, which were attributed to electrolysis from single adsorption events instead of multiple consecutive collisions. These results point to a heightened sensitivity and speed when relying on adsorption instead of collisions. The electrochemical current for the former is limited by the probability of adsorption per collision, whereas for the latter, the current depends on the collision frequency and the probability of electron transfer per collision ( , , 16923-16931).
含有20 mM二茂铁(Fc)的乳化甲苯微滴的当前时间记录显示,在圆盘微电极(直径5μm)上,单个吸附事件产生了电化学氧化峰。通过峰面积积分确定的平均液滴直径(约0.7μm)与动态光散射测量结果(约1μm)相近。利用爱因斯坦的扩散和热速度表达式进行随机游走模拟,推导出液滴电解的方程。模拟结果表明,在液滴游走之前,会发生多次液滴与电极的碰撞,每次碰撞持续约0.11μs。每次碰撞时更新Fc浓度表明,一个液滴在一次碰撞过程中仅氧化其含量的约0.58%。事实上,以1μm液滴的热速度(约0.52 cm/s)得出的碰撞频率来计算,电解一个液滴中的Fc大约需要5.45×10次碰撞和约1.26小时。为了模拟吸附,在液滴与电极首次接触时将其固定,同时计算电解电流。这种方法以及仪器滤波建模,产生了与实验峰的最佳匹配,这些峰归因于单个吸附事件的电解,而不是多次连续碰撞。这些结果表明,依靠吸附而不是碰撞时,灵敏度和速度会提高。前者的电化学电流受每次碰撞吸附概率的限制,而后者的电流则取决于碰撞频率和每次碰撞电子转移的概率(,,16923 - 16931)。