Peichun Amy Tsai
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The organizations/institutes from the scholar's latest article
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Research Interests
Peichun Amy Tsai has a total of 126 co-authors. Here are the top co-authors by number of shared publications:
- Rob G. H. Lammertink
Membrane Science and Technology, Faculty of Science and Technology (TNW), University of Twente, Drienerlolaan 5, 7522 NB Enschede, The Netherlands
10 shared publications - Detlef Lohse
University of Twente
7 shared publications Junyi Yang
Department of Mechanical Engineering, University of Alberta, Edmonton, Alberta, Canada T6G 2R3
6 shared publicationsAhmed Aldhaleai
Mechanical Engineering, University of Alberta, Edmonton, Alberta T6G 1H9, Canada
5 shared publications- Lihui Liu
University of Alberta
5 shared publications - Adrien Bussonnière
Matière et Systèmes Complexes, Université Paris Cité
4 shared publications
Latest Publications
- Open Access
- 10 November 2026
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 26 (22) , 6010-6028
Transport dynamics of supercritical CO 2 foam in microfluidic porous media: mobility control, oil displacement, and foam–oil interactions
Using high-pressure microfluidics, we visualized oil displacement by supercritical CO 2 (scCO 2 ) foam and examined pore-scale mechanisms affecting foam transport and mobility control in enhanced oil recovery (EOR) under reservoir-relevant conditions.
- 10 November 2026
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 26 (22) , 6010-6028
Open AccessTransport dynamics of supercritical CO 2 foam in microfluidic porous media: mobility control, oil displacement, and foam–oil interactions
Using high-pressure microfluidics, we visualized oil displacement by supercritical CO 2 (scCO 2 ) foam and examined pore-scale mechanisms affecting foam transport and mobility control in enhanced oil recovery (EOR) under reservoir-relevant conditions.
- 4 September 2026
- Published by American Chemical Society (ACS) in Langmuir
Impact Dynamics of Oxidized Galinstan Droplets on Rough and Heated Substrates
Liquid-metal droplet impact plays a key role in thermal management, coating, and additive manufacturing, yet its dynamics on rough and heated surfaces remain to be elucidated. This study experimentally investigates the impact of oxidized Galinstan droplets on solid substrates, isolating the effects of surface roughness and substrate temperature in the absence of solidification. Experiments were conducted over wide ranges of Weber number (0.15 ≤ We ≤ 720), average surface roughness (0.2 nm ≤ Ra ≤ 19.5 μm), and surface temperature (25 °C ≤ Ts ≤ 400 °C). Our results show that surface roughness promotes splashing by reducing the critical impact velocity. By fitting the experimental data within the explored parameter range, an empirical splashing threshold, ReOh4/5 = 9.8r–0.28, is established by incorporating the dimensionless roughness (r), Reynolds number (Re), and Ohnesorge number (Oh). Despite its strong influence on splashing, surface roughness has a negligible effect on the maximum spreading factor (βmax) due to Galinstan’s high surface tension. Substrate temperature likewise exerts only a minor influence, as the droplet temperature variation during spreading causes only minor changes in the liquid properties and subsequent impact dynamics under our conditions. For all Ts and Ra conditions, the experimental data of βmax collapse onto an empirical correlation, βmax = 0.1(2154 + We/Oh)0.3 for Oh∼O(10−4) and 0.15 ≤ We ≤ 720.
- 4 September 2026
- Published by American Chemical Society (ACS) in Langmuir
Impact Dynamics of Oxidized Galinstan Droplets on Rough and Heated Substrates
Liquid-metal droplet impact plays a key role in thermal management, coating, and additive manufacturing, yet its dynamics on rough and heated surfaces remain to be elucidated. This study experimentally investigates the impact of oxidized Galinstan droplets on solid substrates, isolating the effects of surface roughness and substrate temperature in the absence of solidification. Experiments were conducted over wide ranges of Weber number (0.15 ≤ We ≤ 720), average surface roughness (0.2 nm ≤ Ra ≤ 19.5 μm), and surface temperature (25 °C ≤ Ts ≤ 400 °C). Our results show that surface roughness promotes splashing by reducing the critical impact velocity. By fitting the experimental data within the explored parameter range, an empirical splashing threshold, ReOh4/5 = 9.8r–0.28, is established by incorporating the dimensionless roughness (r), Reynolds number (Re), and Ohnesorge number (Oh). Despite its strong influence on splashing, surface roughness has a negligible effect on the maximum spreading factor (βmax) due to Galinstan’s high surface tension. Substrate temperature likewise exerts only a minor influence, as the droplet temperature variation during spreading causes only minor changes in the liquid properties and subsequent impact dynamics under our conditions. For all Ts and Ra conditions, the experimental data of βmax collapse onto an empirical correlation, βmax = 0.1(2154 + We/Oh)0.3 for Oh∼O(10−4) and 0.15 ≤ We ≤ 720.
- 16 April 2026
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 11 (4)
Ionic liquid drop impact on solid surfaces under an electric field
- 16 April 2026
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 11 (4)
Ionic liquid drop impact on solid surfaces under an electric field
- Open Access
- 21 March 2026
- Published by Elsevier in Journal of Rock Mechanics and Geotechnical Engineering
- Vol. 18 (9) , 7182-7197
Microscale mineral dissolution and mechanical degradation in lacustrine shale during supercritical CO2–water interaction
- 21 March 2026
- Published by Elsevier in Journal of Rock Mechanics and Geotechnical Engineering
- Vol. 18 (9) , 7182-7197
Open AccessMicroscale mineral dissolution and mechanical degradation in lacustrine shale during supercritical CO2–water interaction
- Open Access
- 18 March 2026
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 26 (7) , 2146-2162
Microfluidic determination of minimum miscibility pressure (MMP) in dynamic CO 2 / n -decane flow
This work presents a novel microfluidic method for dynamically determining the minimum miscibility pressure (MMP) of CO 2 –oil systems with high precision and direct visualization.
- 18 March 2026
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 26 (7) , 2146-2162
Open AccessMicrofluidic determination of minimum miscibility pressure (MMP) in dynamic CO 2 / n -decane flow
This work presents a novel microfluidic method for dynamically determining the minimum miscibility pressure (MMP) of CO 2 –oil systems with high precision and direct visualization.
- Top Cited PapersOpen Access
- 7 January 2026
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 26 (5) , 1352-1393
Lab-on-a-chip insights: advancing subsurface flow applications in carbon management and hydrogen storage
The transition to sustainable energy is crucial for mitigating climate change impacts, with hydrogen and carbon storage and utilization technologies playing pivotal roles. This review highlights the integral and useful role of microfluidic technologies in advancing subsurface fluid dynamics for carbon capture, utilization, and storage (CCUS), enhanced oil recovery (EOR), and underground hydrogen storage (UHS). In particular, microfluidic platforms provide clear and insightful visualization of fluid–fluid and fluid–solid interactions at the pore scale, crucial for understanding and further optimizing processes for CO2 sequestration, hydrogen storage, and oil displacement in various geological formations. We first discuss the development of lab-on-a-chip devices that accurately mimic subsurface conditions, allowing detailed studies of complex phenomena including viscous fingering, capillary trapping, phase behavior during CCUS and EOR processes, and the hysteresis effects unique to hydrogen storage cycles. We also discuss the dynamics of CO2 gas and foam in enhancing oil recovery and the innovative use of hydrogen foam to mitigate issues associated with pure hydrogen gas storage. The integration of advanced imaging, spectroscopic techniques, and machine learning (ML) with microfluidic experiments has enriched our understanding and opened new pathways for predictive capabilities and operational optimization in CCUS, EOR, and UHS applications. We further emphasize the critical need for continued research into microfluidic applications, e.g., incorporating state-of-the-art ML to optimize microfluidic experiments and parameters, and UHS enhancement through favorable microbial activities and suppression of reactions in H2 foam, aiming at refining storage strategies and exploiting the full potential of these technologies towards a sustainable energy future.
- 7 January 2026
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 26 (5) , 1352-1393
Top Cited PapersOpen AccessLab-on-a-chip insights: advancing subsurface flow applications in carbon management and hydrogen storage
The transition to sustainable energy is crucial for mitigating climate change impacts, with hydrogen and carbon storage and utilization technologies playing pivotal roles. This review highlights the integral and useful role of microfluidic technologies in advancing subsurface fluid dynamics for carbon capture, utilization, and storage (CCUS), enhanced oil recovery (EOR), and underground hydrogen storage (UHS). In particular, microfluidic platforms provide clear and insightful visualization of fluid–fluid and fluid–solid interactions at the pore scale, crucial for understanding and further optimizing processes for CO2 sequestration, hydrogen storage, and oil displacement in various geological formations. We first discuss the development of lab-on-a-chip devices that accurately mimic subsurface conditions, allowing detailed studies of complex phenomena including viscous fingering, capillary trapping, phase behavior during CCUS and EOR processes, and the hysteresis effects unique to hydrogen storage cycles. We also discuss the dynamics of CO2 gas and foam in enhancing oil recovery and the innovative use of hydrogen foam to mitigate issues associated with pure hydrogen gas storage. The integration of advanced imaging, spectroscopic techniques, and machine learning (ML) with microfluidic experiments has enriched our understanding and opened new pathways for predictive capabilities and operational optimization in CCUS, EOR, and UHS applications. We further emphasize the critical need for continued research into microfluidic applications, e.g., incorporating state-of-the-art ML to optimize microfluidic experiments and parameters, and UHS enhancement through favorable microbial activities and suppression of reactions in H2 foam, aiming at refining storage strategies and exploiting the full potential of these technologies towards a sustainable energy future.
- Open Access
- 5 September 2025
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1018, A42
On the maximum spreading of viscous droplets impacting flat solid surfaces
We experimentally and theoretically examine the maximum spreading of viscous droplets impacting ultra-smooth solid surfaces, where viscosity plays a dominant role in governing droplet spreading. For low-viscosity droplets, viscous dissipation occurs mainly in a thin boundary layer near the liquid–solid interface, whereas for high-viscosity droplets, dissipation is expected to extend throughout the droplet bulk. Incorporating these dissipation mechanisms with energy conservation principles, two distinct theoretical scaling laws for the maximum spreading factor ( $\beta _m$ ) are derived: $\beta _m \sim ({\textit{We}}/ {\textit{Oh}})^{1/6}$ for low-viscosity regimes ( ${\textit{Oh}} \lesssim 0.1$ ) and $\beta _m \sim \textit{Re}^{1/5}$ for high-viscosity regimes ( ${\textit{Oh}} \gt 1$ ), where $\textit{We}$ , $\textit{Re}$ and $\textit{Oh}$ are the Weber, Reynolds and Ohnesorge numbers, respectively. Both scaling laws show good agreement with the experimental data for their respective validity ranges of $\textit{Oh}$ . Furthermore, to better model experimental data at vanishing $\textit{Re}$ , we introduce a semi-empirical scaling law, $\beta _m \sim (A + {\textit{We}}/ {\textit{Oh}})^{1/6}$ , where $A$ is a fitting parameter accounting for finite spreading ( $\beta _m \approx 1$ ) at negligible impact velocities. This semi-empirical law provides an effective description of $\beta _m$ for a broad experimental range of $10^{-3} \leqslant {\textit{Oh}} \leqslant 10^0$ and $10^1 \leqslant {\textit{We}} \leqslant 10^3$ .- 5 September 2025
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1018, A42
Open AccessOn the maximum spreading of viscous droplets impacting flat solid surfaces
We experimentally and theoretically examine the maximum spreading of viscous droplets impacting ultra-smooth solid surfaces, where viscosity plays a dominant role in governing droplet spreading. For low-viscosity droplets, viscous dissipation occurs mainly in a thin boundary layer near the liquid–solid interface, whereas for high-viscosity droplets, dissipation is expected to extend throughout the droplet bulk. Incorporating these dissipation mechanisms with energy conservation principles, two distinct theoretical scaling laws for the maximum spreading factor ( $\beta _m$ ) are derived: $\beta _m \sim ({\textit{We}}/ {\textit{Oh}})^{1/6}$ for low-viscosity regimes ( ${\textit{Oh}} \lesssim 0.1$ ) and $\beta _m \sim \textit{Re}^{1/5}$ for high-viscosity regimes ( ${\textit{Oh}} \gt 1$ ), where $\textit{We}$ , $\textit{Re}$ and $\textit{Oh}$ are the Weber, Reynolds and Ohnesorge numbers, respectively. Both scaling laws show good agreement with the experimental data for their respective validity ranges of $\textit{Oh}$ . Furthermore, to better model experimental data at vanishing $\textit{Re}$ , we introduce a semi-empirical scaling law, $\beta _m \sim (A + {\textit{We}}/ {\textit{Oh}})^{1/6}$ , where $A$ is a fitting parameter accounting for finite spreading ( $\beta _m \approx 1$ ) at negligible impact velocities. This semi-empirical law provides an effective description of $\beta _m$ for a broad experimental range of $10^{-3} \leqslant {\textit{Oh}} \leqslant 10^0$ and $10^1 \leqslant {\textit{We}} \leqslant 10^3$ . - Open Access
- 25 July 2025
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 25 (22) , 5976-5992
Microfluidic investigation of CO 2 foam flow in a heterogeneous porous medium
Direct visualization reveals how CO 2 foam enhances fluid mobility control in heterogeneous porous media, outperforming surfactant solution and CO 2 gas injection to improve sweep efficiency and oil recovery.
- 25 July 2025
- Published by Royal Society of Chemistry (RSC) in Lab on a Chip
- Vol. 25 (22) , 5976-5992
Open AccessMicrofluidic investigation of CO 2 foam flow in a heterogeneous porous medium
Direct visualization reveals how CO 2 foam enhances fluid mobility control in heterogeneous porous media, outperforming surfactant solution and CO 2 gas injection to improve sweep efficiency and oil recovery.
- Open Access
- 15 July 2025
- Published by Elsevier in International Journal of Multiphase Flow
- Vol. 192
Viscous droplets impact on rough surfaces
- 15 July 2025
- Published by Elsevier in International Journal of Multiphase Flow
- Vol. 192
Open AccessViscous droplets impact on rough surfaces
- 5 June 2025
- Published by American Chemical Society (ACS) in Journal of Chemical Information and Modeling
- Vol. 65 (12) , 6273-6286
Machine Learning Based Quantitative Structure–Dissolution Profile Relationship
Determining accurate drug dissolution processes in the gastrointestinal tract is critical in drug discovery as dissolution profiles provide essential information for estimating the bioavailability of orally administered drugs. While various methods have been developed to predict drug solubility based on chemical structures, no reliable tools currently exist for predicting the dissolution rate constant. This study presents a novel two-stage machine learning approach, termed Machine Learning based Quantitative Structure-Dissolution Profile Relationship, which integrates physics-informed neural networks (PINNs) and deep neural networks (DNNs) to predict drug dissolution profiles in water, with varying concentrations of surfactant Sodium Lauryl Sulfate. In the first stage, PINNs extract key dissolution parameters─namely the dissolution rate constant (k) and the dissolved mass fraction at saturation (ϕs)─from existing dissolution data. By leveraging a physical law governing the dissolution process, PINNs aim to enhance prediction performance and reduce data requirements. Assuming first-order kinetics of the drug dissolution process as described by the Noyes-Whitney equation, PINNs, with 8 hidden layers and 40 neurons per layer, may outperform traditional nonlinear regression by effectively filtering noise and focusing on physically meaningful data. In the second stage, these extracted parameters (k and ϕs) are used to train a DNN to predict dissolution profiles based on the drug's chemical structure and dissolution medium. Using the FDA-recommended metrics: the difference and similarity factors (f1 and f2), the DNN─with 128 neurons in two hidden layers and a learning rate of 10-2.8─achieved an average testing accuracy of 61.7% at an 80:20 train-to-test split. Although this current accuracy is below the generally acceptable range of 70-80%, this approach shows significant potential as a low-cost, time-efficient tool for early phase drug formulation. Future improvements are expected as data quality and diversity increase.
- 5 June 2025
- Published by American Chemical Society (ACS) in Journal of Chemical Information and Modeling
- Vol. 65 (12) , 6273-6286
Machine Learning Based Quantitative Structure–Dissolution Profile Relationship
Determining accurate drug dissolution processes in the gastrointestinal tract is critical in drug discovery as dissolution profiles provide essential information for estimating the bioavailability of orally administered drugs. While various methods have been developed to predict drug solubility based on chemical structures, no reliable tools currently exist for predicting the dissolution rate constant. This study presents a novel two-stage machine learning approach, termed Machine Learning based Quantitative Structure-Dissolution Profile Relationship, which integrates physics-informed neural networks (PINNs) and deep neural networks (DNNs) to predict drug dissolution profiles in water, with varying concentrations of surfactant Sodium Lauryl Sulfate. In the first stage, PINNs extract key dissolution parameters─namely the dissolution rate constant (k) and the dissolved mass fraction at saturation (ϕs)─from existing dissolution data. By leveraging a physical law governing the dissolution process, PINNs aim to enhance prediction performance and reduce data requirements. Assuming first-order kinetics of the drug dissolution process as described by the Noyes-Whitney equation, PINNs, with 8 hidden layers and 40 neurons per layer, may outperform traditional nonlinear regression by effectively filtering noise and focusing on physically meaningful data. In the second stage, these extracted parameters (k and ϕs) are used to train a DNN to predict dissolution profiles based on the drug's chemical structure and dissolution medium. Using the FDA-recommended metrics: the difference and similarity factors (f1 and f2), the DNN─with 128 neurons in two hidden layers and a learning rate of 10-2.8─achieved an average testing accuracy of 61.7% at an 80:20 train-to-test split. Although this current accuracy is below the generally acceptable range of 70-80%, this approach shows significant potential as a low-cost, time-efficient tool for early phase drug formulation. Future improvements are expected as data quality and diversity increase.