“…According to the Grotthuss–Draper law, light must be absorbed by a chemical substance for a photochemical reaction to occur; when applied to Figure b in the dark area no reaction occurs, emphasizing why mixing is a key parameter in photochemical transformations. , The work of Sczechowski et al on heterogeneous photocatalysis in a Taylor–Couette (Taylor vortex) reactor and the more recent work from Lee et al on the large-scale Taylor–Couette (Taylor vortex) reactor with a predicted productivity of up to 7.45 kg/day was of interest to us. , The mixing that occurs within Taylor–Couette reactors (or Taylor vortex reactors) has been well-characterized via computational fluid dynamics (CFD) modeling; Reynolds numbers and flow structures (flow regimes) for Taylor–Couette reactors are discussed by Grossmann et al , Taylor–Couette flow reactors have a rotating inner smooth or channelled cylinder inside a cylindrical outer to form an annular gap . By varying the rotating cylinder speed, flow rate, and rotating cylinder design, different flow regimes can be achieved . It has also been documented that using a Taylor–Couette-type flow with photochemistry works well due to the increased mass transfer throughout the system. ,,, …”