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Ahmadpour A, Shojaeian M, Tasoglu S. Deep learning-augmented T-junction droplet generation. iScience 2024; 27:109326. [PMID: 38510144 PMCID: PMC10951907 DOI: 10.1016/j.isci.2024.109326] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/19/2023] [Revised: 01/13/2024] [Accepted: 02/20/2024] [Indexed: 03/22/2024] Open
Abstract
Droplet generation technology has become increasingly important in a wide range of applications, including biotechnology and chemical synthesis. T-junction channels are commonly used for droplet generation due to their integration capability of a larger number of droplet generators in a compact space. In this study, a finite element analysis (FEA) approach is employed to simulate droplet production and its dynamic regimes in a T-junction configuration and collect data for post-processing analysis. Next, image analysis was performed to calculate the droplet length and determine the droplet generation regime. Furthermore, machine learning (ML) and deep learning (DL) algorithms were applied to estimate outputs through examination of input parameters within the simulation range. At the end, a graphical user interface (GUI) was developed for estimation of the droplet characteristics based on inputs, enabling the users to preselect their designs with comparable microfluidic configurations within the studied range.
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Affiliation(s)
- Abdollah Ahmadpour
- Mechanical Engineering Department, School of Engineering, Koç University, Istanbul 34450, Türkiye
| | - Mostafa Shojaeian
- Mechanical Engineering Department, School of Engineering, Koç University, Istanbul 34450, Türkiye
| | - Savas Tasoglu
- Mechanical Engineering Department, School of Engineering, Koç University, Istanbul 34450, Türkiye
- Koç University Arçelik Research Center for Creative Industries (KUAR), Koç University, Istanbul 34450, Türkiye
- Koç University Is Bank Artificial Intelligence Lab (KUIS AILab), Koç University, Sariyer, Istanbul 34450, Türkiye
- Koç University Translational Medicine Research Center (KUTTAM), Koç University, Istanbul 34450, Türkiye
- Boğaziçi Institute of Biomedical Engineering, Boğaziçi University, Istanbul 34684, Türkiye
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Tone CM, Zizzari A, Spina L, Bianco M, De Santo MP, Arima V, Barberi RC, Ciuchi F. Sunset Yellow Confined in Curved Geometry: A Microfluidic Approach. LANGMUIR : THE ACS JOURNAL OF SURFACES AND COLLOIDS 2023; 39:6134-6141. [PMID: 37072936 PMCID: PMC10157883 DOI: 10.1021/acs.langmuir.3c00275] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/03/2023]
Abstract
The behavior of lyotropic chromonic liquid crystals (LCLCs) in confined environments is an interesting research field that still awaits exploration, with multiple key variables to be uncovered and understood. Microfluidics is a highly versatile technique that allows us to confine LCLCs in micrometric spheres. As microscale networks offer distinct interplays between the surface effects, geometric confinement, and viscosity parameters, rich and unique interactions emerging at the LCLC-microfluidic channel interfaces are expected. Here, we report on the behavior of pure and chiral doped nematic Sunset Yellow (SSY) chromonic microdroplets produced through a microfluidic flow-focusing device. The continuous production of SSY microdroplets with controllable size gives the possibility to systematically study their topological textures as the function of their diameters. Indeed, doped SSY microdroplets produced via microfluidics, show topologies that are typical of common chiral thermotropic liquid crystals. Furthermore, few droplets exhibit a peculiar texture never observed for chiral chromonic liquid crystals. Finally, the achieved precise control of the produced LCLC microdroplets is a crucial step for technological applications in biosensing and anticounterfeiting.
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Affiliation(s)
- Caterina Maria Tone
- Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
- CNR-Nanotec, c/o Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
| | - Alessandra Zizzari
- CNR NANOTEC - Institute of Nanotechnology, c/o Campus Ecotekne, University of Salento, via Monteroni, 73100 Lecce, Italy
| | - Lorenza Spina
- Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
- CNR-Nanotec, c/o Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
| | - Monica Bianco
- CNR NANOTEC - Institute of Nanotechnology, c/o Campus Ecotekne, University of Salento, via Monteroni, 73100 Lecce, Italy
| | - Maria Penelope De Santo
- Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
- CNR-Nanotec, c/o Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
| | - Valentina Arima
- CNR NANOTEC - Institute of Nanotechnology, c/o Campus Ecotekne, University of Salento, via Monteroni, 73100 Lecce, Italy
| | - Riccardo Cristoforo Barberi
- Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
- CNR-Nanotec, c/o Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
| | - Federica Ciuchi
- CNR-Nanotec, c/o Physics Department, University of Calabria, Ponte Bucci, cubo 31C, 87036 Arcavacata di Rende, CS, Italy
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