Abstract
Traditional trial-and-error methods for materials discovery are too slow to meet the urgent demands posed by the rapid progression of climate change. This urgency has driven the increasing interest in integrating robotics and machine learning into materials research to accelerate experimental learning. However, idealized decision-making frameworks to achieve maximum sampling efficiency are not always compatible with high-throughput experimental workflows inside a laboratory. For multistep chemical processes, differences in hardware capacities can complicate the digital framework by introducing constraints on the maximum number of samples in each step of the experiment, hence causing varying batch sizes in variable selection within the same batch. Therefore, designing flexible sampling algorithms is necessary to accommodate the multi-step synthesis with practical sampling constraints unique to each high-throughput workflow. In this work, we designed and employed three strategies on a high-throughput robotic platform to optimize the sulfonation reaction of redox-active molecules used in flow batteries. Our strategies adapt to the multi-step experimental workflow, where their formulation and heating steps are separate, causing varying batch size requirements. By strategically sampling using clustering and mixed-variable batch Bayesian optimization, we were able to iteratively identify optimal conditions that maximize the yields. Our work presents a new approach that allows tailoring the ML decision-making to suit the practical constraints in individual HTP platforms, followed by performing resource-efficient yield optimization using already existing and available open-source Python libraries.
Supplementary materials
Title
Supporting Information: Autonomous Organic Synthesis for Redox Flow Batteries via Flexible Batch Bayesian Optimization
Description
The supporting information contains figures from the results and the experimental methods section. Figures 1, 2, and 3 are the results of the 4D representation of the posterior mean and uncertainties of the three models in the paper. Figure 4 is a screenshot of the experimental setup for running the high-throughput experimentation.
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