Biomicrofluidics

Biomicrofluidics

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Online ISSN: 1932-1058

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(a) Computational domain of paper strip with length L and width W. (b) FESEM image of Grade-4 paper depicting pores (red highlighted region), (c) pore size distribution of the paper using lognormal fit, (d) food-dye solution at different concentration, (e) food-dye particle size distribution using dynamic light scattering instrument (Anton Paar Particle Analyzer Litesizer 500) for Mayur brand dye having a grand average particle size of 848 nm, (f) step for measuring liquid saturation-pressure data: (i) paper stuffed in 0.5 ml Eppendorf tube, (ii) 0.5 ml microcentrifuge tube inserted in 2 ml microcentrifuge tube, (iii) 2 ml microcentrifuge tube inserted in centrifuge (top view). (g) Schematic diagram of microcentrifuge tube filled with paper inside the centrifuge depicting inclination, length of the paper inside the tube and radii ( r 1 , r 2 ) at the extreme end points.
(a) Variation of experimentally measured capillary pressure with water saturation at different concentration for food-dye solution with an average particle diameter of 0.848 μm. (b) The variation of model parameter a with respect to the concentration and the fitted curve with R 2 value of 0.95. (c) The variation of model parameter b with respect to the change in concentration and the fitted curve with R 2 value of 1. (d) The variation of model parameter m with respect to the concentration and the fitted curve with R 2 value of 1. (e) The variation of model parameter n with respect to the change in concentration and the fitted curve with R 2 value of 1. (f) The variation of parameter l with respect to the concentration and the fitted curve with R 2 value of 1. For all cases, the food die used has an average particle diameter of 0.848 μm.
(a) Experimental results for liquid saturation inside the paper at different concentration for food dye (with an average diameter of 0.848 μm) at t = 34 s, (b) comparison of experimental and numerical saturation contours at different time when food-dye concentration is 1 and 2 mg/ml with paper strip length (L) and width (W) are 5 cm and 5 mm, respectively. (c) Quantitative comparison of experimental and numerical wicking length (interface at normalized saturation level 0.5) with paper strip length (L) and width (W) are 5 cm and 5 mm, respectively.
(a) Comparison of experimental and numerical saturation contour at different widths (W) when L = 5 cm. Wicking length according to the Lucas–Washburn model is also depicted. (b) Contours of water saturation level at different widths when t = 38 s and L = 5 cm and food-dye concentration is 1 mg/ml. Temporal variation of (c) mass rate, (d) Darcy resistance, and (e) maximum capillary pressure at different paper-strip width when L = 5 cm and food-dye concentration is 1 mg/ml.
(a) Experimental and numerical liquid saturation contours at different lengths when food-dye concentration is 1 mg/ml and width is 5 m. Wicking length according to the Lucas–Washburn model is also depicted. (b) Pressure gradient contours at different lengths when width is 5 mm at t = 32 s, (c) Darcy resistance contours at different lengths when width is 5 mm at t = 32 s. The temporal variation of (d) mass rate, (e) average Darcy resistance, and (f) maximum capillary pressure at different lengths when width is 5 mm and food-dye concentration is 1 mg/ml.

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Paper-based microfluidics: Analyte-driven imbibition under the lens

May 2025

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60 Reads

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Shubham Kumar

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Amy Q. Shen

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Aims and scope


Biomicrofluidics offers rapid publication of fundamental and applied research across all areas pertaining to micro/nanoscale transport phenomena or micro/nanofluidics for diagnostic, medical, biological, pharmaceutical, environmental, and chemical applications. With a primary focus on high-quality original research articles, the journal also organizes special sections that help explain and define specific challenges unique to the interdisciplinary field of micro/nanofluidics and biophysics.

Recent articles


(a) Schematic representation of different manufacturing processes for fabricating the Y-shaped microchannel. (b) Schematic of the Y-shaped microchannels, highlighting its dimensions and several crucial parts for production. (c) Flow chart showing the CPA pattern for zebrafish: (i) pre-train stage for the zone preference assessment of zebrafish, (ii) installation of acoustic sensors in the preferred zone (arm) for training, and (iii) memory test stage, evaluating spatial memory capabilities post-stimuli removal.
(a) displays a visual representation outlining the experimental setup utilized in the study. (b) illustrates how zebrafish larvae of different ages responded to varying frequencies of acoustic stimulation. Furthermore, (b) also shows the variation in the swimming behavior of zebrafish larvae subjected to acoustic stimuli, with the heading change angle indicating the degree of deviation in the fish's head position before and after the stimulus. The concentric plots inserted on the right side examine the startle response of zebrafish larvae at different developmental stages (5, 7, and 9 d.p.f.) to different frequencies (200, 600, and 1200 Hz) of acoustic stimulation. In particular, it can be seen that under the 1200 Hz stimulus, zebrafish larvae across all ages exhibited the most significant deviation angle in swimming. Each group's results were derived from 15 independent experiments. (c) showcases the C-start startle response of 5 d.p.f. zebrafish larvae post-acoustic stimulation. The onset of the C-start response (red color) can be observed at 0.07 s, with clear body curvature at 0.08 and 0.23 s, leading to a successful escape from the channel (arm) by 0.4 s.
The quantification of learning and memory among the considered developmental stages of zebrafish larvae by employing EF and OC scores. (a) illustrates the variations of EF score among 5, 7, and 9 d.p.f. larvae during three different stages of manipulation such as pre-training (transducer OFF), training (transducer ON/learning phase), and post-training (memory test). It can be observed from (a)(i), (a)(iii), and (a)(v) that the value of the EF score was positive during the transducer OFF stage. This can indicate that the larvae spent most of their time swimming in their preferred zone. However, during the transducer ON stage, this value can be observed to decrease and reach a negative score. This suggested that the larvae showed a strong aversion to the sound stimulus that was placed in their preferred zone. Furthermore, a decreasing trend in the EF score during the transducer ON stage indicated that the larvae were successfully learning spatial information different from their natural habituation. This decreasing trend can be seen to be more consistent in 9 d.p.f. larvae [(a)(v)] compared to other ages. However, during the memory test stage, the EF score can be observed to increase and reach a positive value after a certain period. This suggested that the acquired memory was slowly decaying, and the larvae had lost all the memory (positive value of EF) gained during the learning phase. Compared to 5 and 7 d.p.f. larvae, the learning that was retained (memory) in 9 d.p.f. [(a)(v)] was observed to be significantly higher (sustained negative EF for an extended period). (a)(ii), (a)(iv), and (a)(vi) compare the EF scores of 5, 7, and 9 d.p.f. larvae at the end and the beginning of the pre-training and training stages. Again, a significant difference can be observed in the EF score of 9 d.p.f. larvae during the pre-training and training stages. This suggested that the 9 d.p.f. larvae were more responsive to the aversion induced by sound stimuli than other ages. (b) illustrates the variations of OC score among 5, 7, and 9 d.p.f. larvae during the three different stages of zebrafish manipulation. A similar trend, as mentioned in the discussion of the EF score, was also observed during the analysis of the OC score. (c) compares the EF score (i) and OC score (ii) among 5, 7, and 9 d.p.f. larvae during the first 2 min of the memory test. The EF and OC values of 9 d.p.f. larvae can be observed to be significantly lower than other age groups. This suggested that the 9 d.p.f. larvae possessed stronger memory compared to 5 and 7 d.p.f.
An investigation on the effect of MB drug toward the learning and memory of 5 d.p.f. zebrafish larvae. (a) illustrates the total travel distance covered by larvae treated with various concentrations of MB. During the test, larvae were placed within a Petri dish, and their movements were monitored to measure the distance covered within a 3-min timeframe. (b)(i) shows the movement of larvae inside the Petri dish that was immersed for a range of immersion times. It can be seen from (b)(ii) that the total travel distance of larvae with an immersion time of 12 h was observed to be greater compared to other immersion time scales. (c)(i) and (c)(ii) show the variation of OC score in the control and drug-treated groups, respectively. The value of the OC score in the drug-treated group was observed to be significantly negative [(c)(ii)] during the transducer ON and memory test stages compared to the control group. Eventually, the learning and memory in the drug-treated group were enhanced by 2-fold and 20-fold, respectively, compared to the control group. (d)(i), (d)(ii), and (d)(iii) show the variation in the OC score among the control and drug-treated (experimental) group at the transducer OFF, transducer ON, and memory test stages, respectively. During the last 2 min of the transducer OFF stage (pre-training), no significant difference was observed in the OC score among the control and experimental groups [(d)(i)]. However, during the training and memory test stages, the OC values were observed to vary significantly between the control and experimental groups. This suggested that the employed memory enhancer drug methylene blue not only enhanced the memory of larvae but also substantially improved their learning abilities in acquiring spatial information.
The effect of environmental complexities on the learning and memory capabilities of zebrafish larvae. (a)(i), (a)(ii), and (a)(iii) represent the series, parallel, and combined microchannel configurations, respectively. The red color line indicates the indented flow path of larvae in which they were trained (learning) by employing the aversion sound stimuli. The series microchannel configuration can be seen to encompass the mentioned swimming pattern [(a)(i)], the parallel microchannel configuration [(a)(ii)], and the combined microchannel configuration [(a)(iii)]. (b)(i) and (b)(ii) show the variations in latency and habituated intensity of 5 d.p.f. larvae inside the series microchannel for the control and medicine (drug-treated) groups. Similar to parallel microchannels, the value of latency in parallel [(c)(i)] and combined [(d)(i)] microchannels can be observed to be significantly reduced after eight training trials compared to the pre-training stages in both the control and medicine groups. However, a significant difference was observed in the value of habituated intensity among the control and medicine groups in both the parallel [(c)(ii)] and combined [(d)(ii)] microchannel configurations.
Cognitive dynamics of drug-mediated zebrafish under sound stimuli in a microfluidic environment
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June 2025

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Larval zebrafish are an appropriate animal and laboratory model for exploring the neural mechanisms underlying cognitive abilities, especially concerning their applicability to human cognition. To replicate the natural habitats of such organisms at the laboratory level, microfluidic platforms are employed as a valuable tool in mimicking the intricate spatiotemporal stimuli together with high-throughput screening. This work investigated the memory capabilities of zebrafish larvae across different developmental stages (5–9 days post-fertilization) by employing sound stimuli within the microfluidic environment. Notably, the sound signal with 1200 Hz frequency was observed to be significantly sensitive among all the considered developmental stages in stimulating the responses. In addition, the impact of the memory enhancer drug methylene blue (MB) was tested, revealing a significant enhancement in cognitive performance compared to controls. Specifically, learning (training) and memory (post-training) were observed to exhibit 2-fold and 20-fold increases, respectively, in MB-exposed larvae. In addition to sound stimuli and memory enhancer drugs, the impact of environmental complexity on cognitive abilities was examined by employing different designs of microchannels, such as series, parallel, and combined configurations. The presented experimental paradigm provides a robust framework for various zebrafish studies, including sensory processing mechanisms, learning capabilities, and potential therapeutic interventions.


A comprehensive review on electrically modulated transport of soft, multiphase systems in microflow: Perspectives on drops and vesicles

With the transport of soft and multiphase systems such as droplets and vesicles, the controlled movement of these systems could be regulated in microfluidic channels using an external electrical field is a convenient method for further studying and even tuning micro-transport behaviors. The electric field induces complex electrohydrodynamic behaviors in such systems with considerable impact on their deformation, motion, and interaction with the surrounding fluid. Introducing an electric field exerts stresses at the interface of these fluids, which ensures precise control over their deformation and motion with the features of droplets or vesicles that are vital for their subsequent manipulation inside confined microchannels. Here, electrically modulated transport dynamics in soft multiphase systems, specifically droplets and vesicles, in microfluidic systems are studied meticulously. In this review work, we study how the electric field strength, fluid properties, and membrane characteristics, all of which are important to the directed motion of these systems, are coupled to one another. It also notes that vesicles, with their bilayer lipid membranes, have unique dynamics—such as the formation of membrane tensions and bending rigidity—that affect their electrohydrodynamic behaviors, unlike simple droplets. Studying the electrically driven dynamics of the soft matter, this review offers useful perspectives on the creation of next-generation microfluidics devices, ranging from drug delivery to synthetic biology and materials manufacturing. The effects of the field strength, frequency, and geometry on the transport properties of the droplets and vesicles and highlighting the rich interplay between the electrostatic forces and the inherent properties of soft matter are studied systematically. Recent advances in experimental methods (such as high-precision imaging, micro-manipulation, and sophisticated computational modeling) have also taken our understanding of these electrohydrodynamic processes to new heights. This review further explores potential applications of these technologies in lab-on-a-chip platforms, drug delivery systems, and bioanalytical tools and highlights challenges, including stability, scalability, and reproducibility. The conclusion includes proposed directions for future research aimed at enhancing the localization, control, and efficiency of electrokinetic manipulation in soft matter-based microfluidic systems.


Droplet acoustofluidics: Recent progress and challenges

Acoustofluidics, offering contact-free and precise manipulation of micro-objects, has emerged as a transformative tool for various biological and medical applications. In recent years, significant advancements have been made in droplet manipulation using acoustic waves. This review provides an in-depth exploration of acoustofluidic techniques for droplet manipulation, presenting a balanced perspective on the role of this versatile platform across diverse applications. The paper begins by introducing the underlying mechanism of acoustic forces acting on the droplets, followed by a comprehensive discussion of acoustofluidic techniques tailored for essential unit operations, such as droplet generation, separation, merging, splitting, steering, trapping, in-droplet sample manipulation, sample control within sessile droplets, and digital acoustofluidics. Finally, the prospects and limitations of acoustofluidics for droplet manipulations are also discussed, suggesting the future direction of droplet acoustofluidics research.


Paper-based microfluidics: Analyte-driven imbibition under the lens

Paper-based microfluidic devices are widely used in point-of-care diagnostics, yet the fundamental mechanisms governing analyte transport under partially saturated conditions remain insufficiently characterized. Here, we systematically investigate the concentration-dependent imbibition dynamics and particle trapping behavior of analyte/colloid-laden fluids in porous paper substrates. Using model food-dye colloids of varying particle sizes (∼0.3–4.5 μm) and concentrations (0.5–2 mg/ml), we quantify key saturation-dependent parameters and reveal their strong influence on wicking length and analyte retention. A semiempirical numerical model incorporating experimentally derived van Genuchten and Brooks–Corey parameters is developed to predict analyte flow under varying conditions. Our study demonstrates that particle size, concentration, and paper properties critically modulate transport behavior, with implications for reproducibility and sensitivity in lateral flow assays. Furthermore, through Damköhler number analysis, we propose practical design guidelines for optimal test line placement based on flow and reaction dynamics. This combined experimental and modeling framework offers new insights for the rational design and optimization of paper-based diagnostic platforms.


Overview of biochip attack vectors (in red) and corresponding countermeasures (in green) across material, structure, IP, and sample levels.
Structural attack and defense concerning FMBs. (a) Fluorescence intensity (PCR-amplified DNA, SYBR Green dye) decreases with reduced-height chambers, compared to the original 270 μm chambers. Deviant chamber heights are noted below each. (b) Scale bar: 250 μm. (c) Light microscope image showing original-height (270 μm) and deviant-height (<270 μm) chambers; 9 out of 12 are deviant, marked with black boxes. (d) Linear regression between normalized height and intensity of SYBR green-labeled DNA. (e) ResNet-34 training and validation accuracy. Adapted with permission from Baban et al., IEEE Trans. Biomed. Circuits Syst. 16(6), 1261–1275 (2022). Copyright 2022 IEEE.²
Material-level countermeasures for FMBs. (a) Punch test response for the 40:1 PDMS sample. (b) Bar graph illustrating modulus variation with curing ratios, as determined by the punch test. (c) Finite element modeling results for a 3 mm circular PDMS valve actuated at 1000 mbar through a 350 μm hole, showing maximum principal strain contours. (d) Biaxial response indicating normalized excimer intensity changes strongly correlated with maximum principal strains; linear regression yields a slope of 0.392 and R² = 0.971. Adapted with permission from Singh Baban et al., Lab Chip 23(19), 4213–4231 (2023). Copyright 2023 Royal Society of Chemistry,³ and Baban et al., Sci. Rep. 14, 19806 (2024). Copyright 2024 Nature Publishing Group.⁵
Cyber-physical security of biochips: A perspective

Microfluidic biochips (MBs) are transforming diagnostics, healthcare, and biomedical research. However, their rapid deployment has exposed them to diverse security threats, including structural tampering, material degradation, sample-level interference, and intellectual property (IP) theft, such as counterfeiting, overbuilding, and piracy. This perspective highlights emerging attack vectors and countermeasures aimed at mitigating these risks. Structural attacks, such as stealthy design code modifications, can result in faulty diagnostics. To address this, deep learning -based anomaly detection leverages microstructural changes, including optical changes such as shadows or reflections, to identify and resolve faults. Material-level countermeasures, including mechano-responsive dyes and spectrometric watermarking, safeguard against subtle chemical alterations during fabrication. Sample-level protections, such as molecular barcoding, ensure bio-sample integrity by embedding unique DNA sequences for authentication. At the IP level, techniques like watermarking, physically unclonable functions, fingerprinting, and obfuscation schemes provide robust defenses against reverse engineering and counterfeiting. Together, these approaches offer a multi-layered security framework to protect MBs, ensuring their reliability, safety, and trustworthiness in critical applications.


Schematic of the post-array devices and microscope images of droplet generation. (a) Premix emulsion feeding system. Reproduced with permission from Amstad et al., Lab Chip 14, 705 (2014). Copyright 2014 Royal Society of Chemistry.¹⁵ (b) Sheath flow configuration. Reproduced with permission from Masui et al., Lab Chip 23, 4959 (2023). Copyright 2023 Royal Society of Chemistry.¹⁶
Particles synthesized from various precursor droplets generated by post-array and their combined device. (a) PDMS beads. Reproduced with permission from Amstad et al., Lab Chip 14, 705 (2014). Copyright 2014 Royal Society of Chemistry.¹⁵ (b) Poly(ethylene glycol) hydrogel beads encapsulating fluorescent labeled MDA-MB231 cell. Reproduced with permission from Akbari et al., Lab Chip 17, 2067 (2017). Copyright 2017 Royal Society of Chemistry.¹⁷ (c) PLGA microparticle prepared by combination of post-array and cross-flow device. Reproduced with permission from Yeh et al., Microfluid. Nanofluidics 27, 47 (2023). Copyright 2023 Springer Nature.¹⁸
Two droplet generation modes governed by the magnitude of shear force, along with their characteristic differences. (a) Variation in the normalized mean droplet diameter Dmean/Dh as a function of Caeff, with error bars representing the standard deviation. (b and c) Microscope images of droplet generation in (b) obstruction mode (Caeff = 0.003) and (c) shear-induced mode (Caeff = 0.16). Time-sequenced magnified views of droplet breakup are shown below each image, with time intervals of (b) 2 and (c) 0.3 ms. Reproduced with permission from Masui et al., Lab Chip 23, 4959 (2023). Copyright 2023 Royal Society of Chemistry.¹⁶
Scaling up microdroplet production with post-array devices

Microfluidic systems capable of generating uniform droplets are gaining attention in food, cosmetics, biochemical, and materials applications. While conventional shear- or interfacial tension-driven nozzle devices can generate highly monodisperse droplets (CV < 5%), their scalability is limited by complex flow designs and clogging. Post-array devices have recently emerged as a high-throughput alternative, producing quasi-monodisperse droplets (CV > 12%) by sequentially breaking larger droplets using micro-post structures. These devices offer shear-dependent tunability of droplet sizes, greater resistance to clogging, and scalability. Notably, droplet size is strongly influenced by the dispersed phase fraction, enabling potential decoupling of droplet size and dispersed phase fraction. This study reviews the principles and performance of post-array devices, compares them with other droplet generation methods, and examines their similarities to droplet splitting in T-junctions and premix membrane emulsification. Challenges such as improving droplet uniformity and miniaturization are also discussed to highlight the potential of post-array systems for practical emulsification applications.


A tracking algorithm for finite-size particles

May 2025

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20 Reads

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2 Citations

Particle-wall interaction is important in various applications such as cell sorting, particle separation, the entire class of hydrodynamic filtration and its derivatives, etc. Yet, accurate implementation of interactions between the wall and finite-size particles is not trivial when working with the currently available particle tracking algorithms/packages as they typically work with point-wise particles. Herein, we report a particle tracking algorithm that takes into account interactions between particles of finite size and nearby solid objects. A particle is modeled as a set of circumferential points. While fluid–particle interactions are captured during the track of particle center, interactions between particles and nearby solid objects are modeled explicitly by examining circumferential points and applying a reflection scheme as needed to ensure impenetrability of solid objects. We also report a modified variant of auxiliary structured grid method to locate hosting cells, which in conjunction with a boundary condition scheme enables the capture of interactions between particles and solid objects. As a proof-of-concept, we numerically and experimentally study the particles’ motion within a deterministic lateral displacement microfluidic device. The results successfully demonstrate the zigzag and bump modes observed in our experiments. We also study a microfluidic device with pinched flow numerically and validate our results against experimental data from the literature. By demonstrating an almost 8 × speedup on a system with eight performance threads, our investigations suggest that the algorithm can benefit from parallel processing on multi-thread systems. We believe that the proposed framework can pave the way for designing related microfluidic chips precisely and conveniently.


Investigation of pressure balance in proximity of sidewalls in deterministic lateral displacement

May 2025

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5 Reads

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2 Citations

Deterministic lateral displacement (DLD) is a popular technique for the size-based separation of particles. A key challenge in the design of DLD chips is to eliminate the fluid flow disturbance caused by channel sidewalls intersecting with pillar matrix. While there are numerous reports attempting to mitigate this issue by adjusting the gaps between pillars on the sidewalls and the closest ones residing on the bulk grid of DLD, there are only a few works that also configure the axial gap of pillars adjacent to the accumulation sidewall. Herein, we study various designs numerically to investigate the effects of geometrical configurations of sidewalls on the critical diameter and first stream flux fraction variations across the channel. Our results show that regardless of the model used for the boundary gap profile, applying a pressure balance scheme can improve the separation performance by reducing the critical diameter variations. In particular, we found that for a given boundary gap distribution, there can be two desired parameter sets with relatively low critical diameter variations. One is related to sufficiently low lateral resistance of interface unit cells next to the accumulation sidewall, while the other one emerges by reducing the axial resistance of the interface unit cells to an appropriate extent. This work should pave the way for designing DLD systems with improved performance, which can be critically important for applications such as the separation of rare cells, among others, wherein target species need to be concentrated into as narrow a stream as possible downstream of the device to enhance purity and the recovery rate simultaneously.


Recent advances in microscale techniques for red blood cells manipulation

Manipulation of red blood cells (RBCs) in microscale has proven to play a pivotal role in various applications, such as disease diagnosis and drug delivery. Over the past decades, the capabilities of microscale manipulation techniques have evolved from simple particle manipulation to cells and organisms, with numerous microfluidic-based research tools being developed for RBC manipulation. This review first introduces the reported microscale manipulation techniques and their principles, including passive microfluidic methods based on microstructures and hydrodynamics, as well as active methods such as acoustic, optical, and electrical techniques. It then focuses on the application scenarios of these micro-scale manipulation methods for RBC manipulation, including the investigation of RBC mechanical properties, the preparation of RBC carriers, the control of RBC rotation, and RBC lysis. Finally, the future prospects of microscale techniques in RBC manipulation are discussed. This review offers a comprehensive comparison of various techniques, aiming to provide researchers from different fields with a broad perspective and to guide the continued development of microscale manipulation methods for RBC applications. It seeks to help researchers from diverse backgrounds stay informed about the latest trends and advancements in the field.


Schematic representation of the direct electrification of silicon microfluidics: (a) Oxidized perforation patterns enable sections of the silicon layer to become electrically insulated from the rest of the channel walls, including the bottom and top ones, resulting in an electrically addressable wall segment transversal to the flow direction (light blue arrow). (b) Cross-sectional view through one channel depicting the homogeneous electric fields with two opposite electrodes. (c) Scanning-electron microscopy image of a device with two electrode pairs. An additional channel protrudes from the right (dotted light blue arrow) as this specific device is used for pico-injection. Scale bar: 100  μ m. Adapted from Fig. 2 of Monserrat Lopez et al., Microsyst. Nanoeng. 9, 81 (2023); licensed under a Creative Commons Attribution (CC BY) license. Copyright 2023 Author(s), licensed under a Creative Commons Attribution (CC BY) License.
Rational design and fabrication steps for realizing wall-embedded electrodes in silicon microfluidics: Top view (upper row) and cross-sectional view (bottom row) of the three main fabrication steps. (a) Starting with masking (green) the silicon-on-insulator (SOI) stack to expose the channel and perforation segments of diameter d and pitch p to reactive ion etching across the entire silicon layer of height h while protecting the masked area. (b) Channels and perforations are etched simultaneously in this self-aligned process that is automatically stopped at the buried oxide layer. (c) The self-limited thermal oxidation of silicon penetrates for a certain length l into the silicon bulk, therefore, creates insulating segments, located in between the perforations elements (c). The sum of the initial perforation size, d, and twice the oxidation length, l, defines the width of the insulating segment, w = d + 2 × l. (d) Generic layout depicting the total area occupied for one electrode pair as defined by the insulation widths and the area in between them. Adapted from Fig. 2 of Monserrat Lopez et al., Microsyst. Nanoeng. 9, 81 (2023); licensed under a Creative Commons Attribution (CC BY) license. Copyright 2023 Author(s), licensed under a Creative Commons Attribution (CC BY) License.
Ultimately scaled, complex electrode arrays across and along microfluidic channels with some of the most prominent applications enabled by them: (a) Electrophoretic or direct, electric field-based manipulation. (b) Reaction control in micro- and nanoscale compartments. (c) Electrochemical synthesis. (d) Impedimetric sensing and analytics.
Opportunities of scalable and electrostatically optimized electrodes for electric field- and current-driven microfluidic applications

Silicon-based microfluidics enable the creation of highly complex, three-dimensional fluid networks. These comprise scalable channel sizes and monolithically integrated functionalities available from complementary–metal–oxide–semiconductor technology. On this versatile, solid-state platform, advanced manufacturing techniques exist that allow the channel walls to be directly electrified with one or multiple pairs of electrodes along the fluid-carrying channel. The electrodes have ideal electrostatic geometries, yielding homogeneous electric field distributions across the entire cross section of the microfluidic channel. As these are located directly at the channel, only low supply voltages are needed to achieve suitable field strengths. Furthermore, a controlled supply of charge carriers to the microfluidic channel is feasible. These configurations may serve numerous applications, including highly efficient mechanisms to manipulate droplets, cells, and molecular compounds, perform pico-injection or poration, trigger and control chemical reactions, or realize electrochemical and capacitive sensing modalities. In this perspective, we describe the generic design and fabrication of these electrodes and discuss their miniaturization and scaling properties. Furthermore, we forecast novel use cases and discuss challenges in the context of the most interesting applications.


Microfluidic systems with several steps of thermal cycling in (a) PCR and (b) LAMP analysis. (c) Temperature control for hyperthermia testing with nanoheat agents and its application in controlling tumor cell death. (d) A schematic illustration of thermal cell lysis and implementation in a microchannel. Figures reproduced with permission from the following: P. Skaltsounis et al., Micromachines 14, 172 (2023), Copyright 2023 Authors, licensed under a Creative Commons Attribution 4.0 License; J. H. Seo et al., Sens. Actuators B: Chem. 246, 146–153 (2017), Copyright 2017 Elsevier; E. Grigorov et al., Micromachines 12, 498 (2021), Copyright 2021 Authors, licensed under a Creative Commons Attribution 4.0 License; and P. Montazersaheb et al., Life Sci. 323, 121714 (2023), Copyright 2023 Elsevier.
(a) Hyperthermia process with magnetic nanoparticles for tumor cells. (b) Transparent heating systems with ITO integration for two-step heating. (c) A PDMS microchip for disposable PCR. (d) A PCB electrode layout designed for heat-spreading integration. (e) A SiC MEMS glass microchannel heater. Figures reproduced with permission from the following: M. C. Horny et al., Sensors 21, 185 (2021), Copyright 2021 Authors, licensed under a Creative Commons Attribution 4.0 License; B. H. Ha et al., Sci. Rep. 5, 11851 (2015), Copyright 2015 Authors, licensed under a Creative Commons Attribution 4.0 License; F. Talebi et al., Sens. Actuators A: Phys. 333, 113220 (2022), Copyright 2022 Elsevier; L. Wan et al., Biosens. Bioelectron. 242, 115711 (2023), Copyright 2023 Elsevier; and T. Dinh et al., Adv. Mater. Interfaces 5, 1800764 (2018), Copyright 2018 Wiley.
(a) A thermoelectric heater and thermopile attached below the microfluidics for precise temperature control. (b) An on-chip microscale platinum temperature sensor embedded along with a microfabricated heater. (c) Confocal luminescence spectroscopy images enabling higher spatial resolution to visualize the temperature gradient in the channel. Figures reproduced with permission from the following: G. G. Nestorova et al., Sens. Actuators B: Chem. 225, 174-180 (2016), Copyright 2016 Elsevier; and R. G. Geitenbeek et al., Lab Chip 19, 1236–1246 (2019), Copyright Authors 2019, licensed under a Creative Commons Attribution 3.0 Unported License.
(a) Schematic representation of a quantum magnetometer based on the nitrogen-vacancy (NV) center in diamond. (b) Illustration of a suspended microchannel resonator used to measure the resonant frequency shift ( Δ f ) due to mass of nanoparticles or microparticles flowing through the channel. Figures reproduced with permission from the following: T. F. Segawa and R. Igarashi, Prog. Nucl. Magn. Reson. Spectrosc. 134–135, 20–38 (2023), Copyright Authors 2023, licensed under a Creative Commons Attribution 4.0 License; and M. Gagino et al., ACS Sens. 5, 1230–1238 (2020), Copyright 2020 American Chemical Society.
Various applications of suspended microchannel resonators when integrated with thermal, quantum, and optical multi-modal sensing or aided by advanced microfluidic controls. Figures reproduced with permission from the following: T. F. Segawa and R. Igarashi, Prog. Nucl. Magn. Reson. Spectrosc. 134–135, 20–38 (2023), Copyright Authors 2023, licensed under a Creative Commons Attribution 4.0 License; K. Jiang et al., Appl. Phys. Lett. 114, 173703 (2019), Copyright 2019 AIP Publishing LLC; J. Ko et al., Nano Lett. 22, 7768–7775 (2022), Copyright 2022 American Chemical Society; J. Do et al., Microsyst. Nanoeng. 9, 127 (2023), Copyright 2023 Authors, licensed under a Creative Commons Attribution 4.0 License; H. Etayash et al., Nat. Commun. 7, 12947 (2016), Copyright 2016 Authors, licensed under a Creative Commons Attribution 4.0 License; and A. Martín-Pérez et al., ACS Sens. 4, 3325–3332 (2012), Copyright 2019 American Chemical Society.
Advanced microfluidic systems with temperature modulation for biological applications

Recent advances in microfluidic technology have shown the importance of precise temperature control in a wide range of biological applications. This perspective review presents a comprehensive overview of state-of-the-art microfluidic platforms that utilize thermal modulation for various applications, such as rapid nucleic acid amplification, targeted hyperthermia for cancer therapy, and efficient cellular lysis. We detail various heating mechanisms—including nanoparticle–driven induction, photothermal conversion, and electrothermal approaches (both external and on-chip)—and discuss how they are integrated within lab-on-a-chip systems. In parallel, advanced multi-modal sensing methods within microfluidics, ranging from conventional integrated sensors to cutting-edge quantum-based techniques using nanodiamond nitrogen-vacancy centers and suspended microchannel resonators, are highlighted. By integrating advanced multi-modal sensing capabilities into these microfluidic platforms, a broader range of applications are enabled, including single-cell analysis, metabolic profiling, and scalable diagnostics. Looking ahead, overcoming challenges in system integration, scalability, and cost-effectiveness will be essential to harnessing their full potential. Future developments in this field are expected to drive the evolution of lab-on-a-chip technologies, ultimately enabling breakthroughs in precision medicine and high-throughput biomedical applications.


Temperature-dependent microfluidic impedance spectroscopy for non-invasive biofluid characterization

Remote health monitoring has the potential to enable individuals to take control of their own health and well-being and to facilitate a transition toward preventative and personalized healthcare. Sweat can be sampled non-invasively and contains a wealth of information about the metabolic state of an individual, making it an excellent candidate for remote health monitoring. An accurate, rapid, and low-cost biofluid characterization technique is required to enable the widespread use of remote health monitoring. We previously introduced microfluidic impedance spectroscopy for the detection of electrolyte concentration in fluids, whereby a novel device architecture, measurement method, and analysis technique were presented for the characterization of cationic species. The purely electrical nature of this measurement technique removes the intermediate steps inherent in common rival technologies such as optical and electrochemical sensing, offering a range of advantages. In this work, we investigate the effect of temperature on microfluidic impedance spectroscopy of ionic species commonly present in biofluids. We find that the impedance spectra and concentration determination are temperature-dependent; remote health monitoring devices must be calibrated appropriately as they are likely to experience temperature fluctuations. Importantly, we demonstrate the ability of the method to measure the concentration of anionic species alongside that of cationic species, enabling the detection of chloride and lactate, which are useful biomarkers for hydration, cystic fibrosis, fatigue, sepsis, and hypoperfusion. We show that the presence of neutral species does not impair accurate determination of ionic concentration, thus, demonstrating the suitability of microfluidic impedance spectroscopy for non-invasive biofluid characterization.


Improved acoustic holograms using simulated annealing

April 2025

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47 Reads

Acoustic holography offers the ability to generate designed acoustic fields, enhancing the versatility of acoustic micromanipulation. However, the quality of the generated holograms depends on the nature of the iterative algorithm that is utilized, where the iterative angular spectrum approach (IASA) has been the standard method to date. Here, we introduce a novel approach that categorically improves IASA performance, where we apply the principles of simulated annealing for the generation of high-quality acoustic holograms. We utilize this to realize significant improvements in hologram quality via simulations, fabricated holograms, experimental particle patterning, and high-resolution 2D hydrophone scans. Comparing holograms produced from IASA and/or simulated annealing, we demonstrate that the use of simulated annealing in acoustic holography results in sharper reconstructions and improved hologram outputs across a range of evaluation metrics.


Mechanical interaction between a hydrogel and an embedded cell in biomicrofluidic applications

Thanks to their softness, biocompatibility, porosity, and ready availability, hydrogels are commonly used in microfluidic assays and organ-on-chip devices as a matrix for cells. They not only provide a supporting scaffold for the differentiating cells and the developing organoids, but also serve as the medium for transmitting oxygen, nutrients, various chemical factors, and mechanical stimuli to the cells. From a bioengineering viewpoint, the transmission of forces from fluid perfusion to the cells through the hydrogel is critical to the proper function and development of the cell colony. In this paper, we develop a poroelastic model to represent the fluid flow through a hydrogel containing a biological cell modeled as a hyperelastic inclusion. In geometries representing shear and normal flows that occur frequently in microfluidic experiments, we use finite-element simulations to examine how the perfusion engenders interstitial flow in the gel and displaces and deforms the embedded cell. The results show that pressure is the most important stress component in moving and deforming the cell, and the model predicts the velocity in the gel and stress transmitted to the cell that is comparable to in vitro and in vivo data. This work provides a computational tool to design the geometry and flow conditions to achieve optimal flow and stress fields inside the hydrogels and around the cell.


Design automation for deterministic lateral displacement by leveraging deep Q-network

Despite the widespread application of microfluidic chips in research fields, such as cell biology, molecular biology, chemistry, and life sciences, the process of designing new chips for specific applications remains complex and time-consuming, often relying on experts. To accelerate the development of high-performance and high-throughput microfluidic chips, this paper proposes an automated Deterministic Lateral Displacement (DLD) chip design algorithm based on reinforcement learning. The design algorithm proposed in this paper treats the throughput and sorting efficiency of DLD chips as key optimization objectives, achieving multi-objective optimization. The algorithm integrates existing research results from our team, enabling rapid evaluation and scoring of DLD chip design parameters. Using this comprehensive performance evaluation system and deep Q-network technology, our algorithm can balance optimal separation efficiency and high throughput in the automated design process of DLD chips. Additionally, the quick execution capability of this algorithm effectively guides engineers in developing high-performance and high-throughput chips during the design phase.


Structure of lung-on-a-chips and the human bronchial tree respiratory system. (a) Schematic representation of the structure and operation of a typical lung-on-a-chip, which has two parallel microfluidic channels separated by a porous membrane, representing airway and vascular compartments lined with epithelial and endothelial cells, respectively. The membrane allows gas exchange, while cyclic stretching is applied to simulate breathing-induced mechanical forces (F)—mimicking breathing—and an air–liquid interface supports cell function, mimicking key lung physiology. (b) Schematic of the branching structure of the lungs and the gas-exchange region. Within the lungs, air travels through branching bronchioles until reaching the alveoli, tiny air sacs where gas exchange occurs.
Various in vitro human lung models for cell cultures. (a) Standard 2D air–liquid interface configuration.⁶⁰ Reproduced with permission from Bennet et al., Cells 10(7), 1602 (2021); licensed under a Creative Commons Attribution (CC BY) license. (b) A scaffold-free hanging drop spheroid formation method.⁶¹ Reproduced with permission from Nath et al., Pharmacol. Ther. 163, 94 (2016). Copyright 2016 Elsevier. (c) Organoid culture methods.⁶² Reproduced with permission from Gunti et al., Cancers 13(4), 874 (2021); licensed under a Creative Commons Attribution (CC BY) license. (d) Different types of scaffold-based 3D cellular models.⁶³ Reproduced with permission from Unnikrishnan et al., Front. Oncol. 11, 733652 (2021); licensed under a Creative Commons Attribution (CC BY) license. (e) A typical lung-on-a-chip structure with alveolar epithelial cells and pulmonary microvascular endothelial cells are cultured at the top and bottom of the ECM-coated membrane, respectively.³⁵ Reproduced with permission from Francis et al., Drug Discov. Today 27(9), 2593 (2022). Copyright 2022 Elsevier.
Fabrication methods for lung-on-a-chip models. (a) PDMS-based fabrication of lung-on-a-chips, the typical soft lithography technique.¹¹⁵ Reproduced with permission from Man et al., ACS Appl. Mater. Interfaces 15(30), 36888 (2023). Copyright 2023 ACS. (b) A PMMA-based thermoplastic methods lung airway-on-a-chip.¹¹⁶ Reproduced with permission from Humayun et al., Lab Chip 18(9), 1298 (2018). Copyright 2018 RSC. (c) Bioprinting techniques in different ways.¹¹⁷ Reproduced with permission from Mandrycky et al., Biotechnol. Adv. 34(4), 422 (2016). Copyright 2016 Elsevier.
Lung-on-a-chip models for aerosol transport and deposition. (a) A full-scale experimental model of the pulmonary alveolus to study particle transport and deposition.¹⁰⁷ Reproduced with permission from Fishler et al., Sci. Rep. 5, 11 (2015); licensed under a Creative Commons Attribution (CC BY) license. (b) A breathing lung model using multilayer fabrication technology to mimic the respiratory tract.¹⁰⁶ Reproduced with permission from Lin et al., Biomicrofluidics 13(4), 044109 (2019). Copyright 2019 AIP Publishing LLC. (c) A real-scale single alveolar chip with movable walls to experimentally study micro/nanoparticle transport.¹⁰⁴ Reproduced with permission from Dong et al., Micromachines 12(2), 184 (2021); licensed under a Creative Commons Attribution (CC BY) license. (d) A multilayer microfluidic lung chip designed to accurately mimic human respiratory bronchi for particle deposition studies.¹⁷⁶ Reproduced with permission from Qiu et al., Lab Chip 23(19), 4302 (2023). Copyright 2023 RSC.
Lung-on-a-chip: From design principles to disease applications

March 2025

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38 Reads

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1 Citation

To address the growing need for accurate lung models, particularly in light of respiratory diseases, lung cancer, and the COVID-19 pandemic, lung-on-a-chip technology is emerging as a powerful alternative. Lung-on-a-chip devices utilize microfluidics to create three-dimensional models that closely mimic key physiological features of the human lung, such as the air–liquid interface, mechanical forces associated with respiration, and fluid dynamics. This review provides a comprehensive overview of the fundamental components of lung-on-a-chip systems, the diverse fabrication methods used to construct these complex models, and a summary of their wide range of applications in disease modeling and aerosol deposition studies. Despite existing challenges, lung-on-a-chip models hold immense potential for advancing personalized medicine, drug development, and disease prevention, offering a transformative approach to respiratory health research.


Envisioned microphysiological platform to study the gut–brain axis (GBA). A representative in vitro platform with three microfluidic chambers: (i) gut epithelium consisting of the monolayer obtained from intestinal organoids including epithelial cells and enteroendocrine cells. (ii) Vagal afferent cell bodies that project neurites to both epithelium chamber and the cortical chamber. (iii) Cortical cell culture that consists of neurons, astrocytes, microglia, pericytes, and vascular endothelial cells. The neuronal cells in all chambers would be embedded in a hydrogel to establish a quasi-3D-culture environment. Both the epithelium unit and cortical unit would have a perforated membrane to support culturing gut epithelial cells and vascular endothelial cells, respectively, to mimic the intestinal barrier and blood–brain barrier. This configuration can then be used for a diverse set of experiments. For example, the epithelium unit can be spiked with individual effector compounds from gut microbiota, which can modulate epithelium function and activate the VANs by signaling to the neurite terminals within the “lamina propria” below the epithelial monolayer. VANs in the middle chamber can transduce this information to the cortical unit. The VAN projections that bridge the epithelium unit and cortical unit can be used for studying the retrograde transport of molecules (e.g., aberrant proteins) from the gut to the brain. Together with this neuronal route of communication, molecules of interest (e.g., toxins, pharmaceuticals) can be directly added to the “vascular lumen” to mimic the humoral transport of such molecules to the CNS selectively through the blood–brain barrier. The microfluidic device can contain various electrodes to monitor and modulate microphysiological processes: (i) electrophysiological recording and stimulation electrodes within the chambers and microchannels; (ii) counter electrodes (immersed in apical space) paired with the surface electrodes (located in basolateral space) to monitor barrier function via trans-epithelial-electrical-resistance (TEER) measurements; (iii) electrochemical measurement electrodes for monitoring cytokines, neurotransmitters, and other electrochemically active metabolites. This platform will also allow for live cell imaging-based monitoring and optogenetic stimulation of the cultures.
Representative state-of-the-art microfluidic devices for GBA studies. (a) A two fluidically-isolated lateral-channel chip connected with narrow microchannels designed to separate the axonal terminals (yellow) to cell bodies (black).¹³ Reproduced with permission from Taylor et al., Nat. Methods 2, 599–605 (2005). Copyright 2005 Springer Nature. The epifluorescence image illustrates one chamber populated with neural cells, where only axons and not cell bodies permeate the microchannels. (b) Parkinson's disease model on a lateral-channel platform plated with primary cortical cells to model the retrograde transport of fluorescently-labeled α-synuclein.¹⁴ Reproduced with permission from Freundt et al., Ann. Neurol. 72, 517–524 (2012). Copyright 2012 John Wiley and Sons. (c) Alzheimer's disease (AD) model in the compartmentalized microfluidic platform with human 3D neuron/astrocyte co-culture in the inner chamber and microglia culture in the outer radial channel to establish a neuro-glial AD model to advance drug discovery.¹⁶ Reproduced with permission from Park et al., Nat. Neurosci. 21, 941–951 (2018). Copyright 2018 Springer Nature. (d) A platform for co-culturing human epithelial cells with gastrointestinal microbiota consists of elastomeric gaskets fixed with semi-permeable membranes sandwiched between two polycarbonate enclosures. The system includes dedicated normoxic and hypoxic culture media, O2 sensors, and trans-epithelial-electrical-resistance (TEER) monitoring.¹⁹ Reproduced with permission from Shah et al., Nat. Commun. 7, 11535 (2016). Copyright 2016 Author(s), licensed under a Creative Commons Attribution (CC BY) license. (e) The microfluidic culture system represents enteric neuron–intestinal epithelium interactions observed in vivo.²⁰ Reproduced from de Hoyos-Vega et al., Microsyst. Nanoeng. 9, 144 (2023). Copyright 2023 Author(s), licensed under a Creative Commons Attribution (CC BY) license. (f) A schematic illustration of a blood–brain barrier (BBB) model using a layered-channel architecture with iPSC-derived brain endothelial-like cells cultured on the bottom channel while iPSC-derived glutamatergic and GABAergic neurons, primary human brain astrocytes, pericytes, and microglia cultured on the top channel.²² Reproduced with permission from Pediaditakis et al., iScience 25, 104813 (2022). Copyright 2022 Elsevier. (g) A schematic of a neurovascular-unit-on-a-chip that utilizes a lateral-channel architecture, which was used for investigating stem cell therapy for ischemic stroke.²⁷ Reproduced with permission from Lyu et al., Nat Biomed Eng. 5, 847–863 (2021). Copyright 2021 Springer Nature. (h) Microfluidic device emulating anatomical layout of VANs, where cell bodies (nuclei stained with 4′,6-diamidino-2-phenylindole, blue) are located within the inner chamber projecting neurites (βIII-tubulin, red) toward the outer chamber mimicking innervation of propria lamina.¹⁵ Reproduced with permission from Girardi et al., Bioelectron. Med. 10, 3 (2024). Copyright 2024 Author(s), licensed under a Creative Commons Attribution (CC BY) license. (i) Extracellular electrophysiological recordings of VAN activity via surface microelectrode arrays (MEAs) in response to stimulation with capsaicin, cholecystokinin (CCK), and potassium chloride (KCl).³⁰ Reproduced with permission from Girardi et al., Biosensors. 13, 601 (2023). Copyright 2023 Author(s), licensed under a Creative Commons Attribution (CC BY) license. Guiding figures were created with BioRender.com.
Microfluidic tools to model, monitor, and modulate the gut–brain axis

March 2025

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30 Reads

The gut–brain axis (GBA) connects the gastrointestinal tract and the central nervous system (CNS) via the peripheral nervous system and humoral (e.g., circulatory and lymphatic system) routes. The GBA comprises a sophisticated interaction between various mammalian cells, gut microbiota, and systemic factors. This interaction shapes homeostatic and pathophysiological processes and plays an important role in the etiology of many disorders including neuropsychiatric conditions. However, studying the underlying processes of GBA in vivo, where numerous confounding factors exist, is challenging. Furthermore, conventional in vitro models fall short of capturing the GBA anatomy and physiology. Microfluidic platforms with integrated sensors and actuators are uniquely positioned to enhance in vitro models by representing the anatomical layout of cells and allowing to monitor and modulate the biological processes with high spatiotemporal resolution. Here, we first briefly describe microfluidic technologies and their utility in modeling the CNS, vagus nerve, gut epithelial barrier, blood–brain barrier, and their interactions. We then discuss the challenges and opportunities for each model, including the use of induced pluripotent stem cells and incorporation of sensors and actuator modalities to enhance the capabilities of these models. We conclude by envisioning research directions that can help in making the microfluidics-based GBA models better-suited to provide mechanistic insight into pathophysiological processes and screening therapeutics.


Conditions for a microfluidic creep experiment for microparticles using a cross-slot extensional flow device

The micromechanical measurement field has struggled to establish repeatable techniques because the deforming stresses can be difficult to model. A recent numerical study [Lu et al., J. Fluid Mech. 962, A26 (2023)] showed that viscoelastic capsules flowing through a cross-slot can achieve a quasi-steady strain near the extensional flow stagnation point that is equal to the equilibrium static strain, thereby implying that the capsule's elastic behavior can be captured in continuous device operation. However, no experimental microfluidic cross-slot studies have reported quasi-steady strains for suspended cells or particles to our knowledge. Here, we demonstrate experimentally the conditions necessary for the cross-slot microfluidic device to replicate a uniaxial creep test at the microscale and at relatively high throughput. By using large dimension cross-slots relative to the microparticle diameter, our cross-slot implementation creates an extensional flow region that is large enough for agarose hydrogel microparticles to achieve a strain plateau while dwelling near the stagnation point. This strain plateau will be key for accurately and precisely measuring viscoelastic properties of small microscale biological objects. We propose an analytical mechanical model to extract linear viscoelastic mechanical properties from observed particle strain histories. Particle image velocimetry measurements of the unperturbed velocity field is used to estimate where in the device particles experienced extensional flow and where the mechanical model might be applied to extract mechanical property measurements. Finally, we provide recommendations for applying the cross-slot microscale creep experiment to other biomaterials and criteria to identify particles that likely achieved a quasi-steady strain state.


From specialization to broad adoption: Key trends in droplet microfluidic innovations enhancing accessibility to non-experts

Droplet microfluidics has emerged as a versatile and powerful tool for various analytical applications, including single-cell studies, synthetic biology, directed evolution, and diagnostics. Initially, access to droplet microfluidics was predominantly limited to specialized technology labs. However, the landscape is shifting with the increasing availability of commercialized droplet manipulation technologies, thereby expanding its use to non-specialized labs. Although these commercial solutions offer robust platforms, their adaptability is often constrained compared to in-house developed devices. Consequently, both within the industry and academia, significant efforts are being made to further enhance the robustness and automation of droplet-based platforms, not only to facilitate technology transfer to non-expert laboratories but also to reduce experimental failures. This Perspective article provides an overview of recent advancements aimed at increasing the robustness and accessibility of systems enabling complex droplet manipulations. The discussion encompasses diverse aspects such as droplet generation, reagent addition, splitting, washing, incubation, sorting, and dispensing. Moreover, alternative techniques like double emulsions and hydrogel capsules, minimizing or eliminating the need for microfluidic operations by the end user, are explored. These developments are foreseen to facilitate the integration of intricate droplet manipulations by non-expert users in their workflows, thereby fostering broader and faster adoption across scientific domains.


Microfluidics for the biological analysis of atmospheric ice-nucleating particles: Perspectives and challenges

February 2025

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118 Reads

Atmospheric ice-nucleating particles (INPs) make up a vanishingly small proportion of atmospheric aerosol but are key to triggering the freezing of supercooled liquid water droplets, altering the lifetime and radiative properties of clouds and having a substantial impact on weather and climate. However, INPs are notoriously difficult to model due to a lack of information on their global sources, sinks, concentrations, and activity, necessitating the development of new instrumentation for quantifying and characterizing INPs in a rapid and automated manner. Microfluidic technology has been increasingly adopted by ice nucleation research groups in recent years as a means of performing droplet freezing analysis of INPs, enabling the measurement of hundreds or thousands of droplets per experiment at temperatures down to the homogeneous freezing of water. The potential for microfluidics extends far beyond this, with an entire toolbox of bioanalytical separation and detection techniques developed over 30 years for medical applications. Such methods could easily be adapted to biological and biogenic INP analysis to revolutionize the field, for example, in the identification and quantification of ice-nucleating bacteria and fungi. Combined with miniaturized sampling techniques, we can envisage the development and deployment of microfluidic sample-to-answer platforms for automated, user-friendly sampling and analysis of biological INPs in the field that would enable a greater understanding of their global and seasonal activity. Here, we review the various components that such a platform would incorporate to highlight the feasibility, and the challenges, of such an endeavor, from sampling and droplet freezing assays to separations and bioanalysis.


Modeling the dynamics of circulating tumor cell clusters inside a microfluidic channel

February 2025

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32 Reads

Circulating tumor cells are central to metastasis, a particularly malign spread of cancer beyond its original location. While rare, there is growing evidence that the clusters of circulating tumor cells are significantly more harmful than individual cells. Microfluidic platforms constitute the core of circulating tumor cell cluster research, allowing cluster detection, analysis, and treatment. In this work, we propose a new mathematical model of circulating tumor cell clusters and apply it to simulate the dynamics of the aggregates inside a microfluidic channel with the external flow of a fluid. We leverage our previous model of the interactions of circulating tumor cells with varying clustering affinities and introduce explicit bonds between the cells that makeup a cluster. We show that the bonds have a visible impact on the cluster dynamics and that they enable the reproduction of known cluster flow and deformation patterns. Furthermore, we demonstrate that the dynamics of these aggregates are sensitive to bond properties, as well as initialization and flow conditions. We believe that our modeling framework represents a valuable mesoscopic formulation with an impact beyond circulating tumor cell clusters, as cell aggregates are common in both nature and applications.


A microfluidic sucrose gap platform using trilaminar flow with on-chip switching and novel calibration: Challenges and limitations

Gap junction connectivity is crucial to intercellular communication and plays a key role in many critical processes in developmental biology. However, direct analysis of gap junction connectivity in populations of developing cells has proven difficult due to the limitations of patch clamp and dye diffusion based technologies. We re-examine a microfluidic technique based on the principle of laminar flow, which aims to electrically measure gap junction connectivity. In the device, the trilaminar flow of a saline sheathed sucrose solution establishes distinct regions of electrical conductivity in the extracellular fluid spanning an NRK-49F cell monolayer. In theory, the sucrose gap created by laminar flow provides sufficient electrical isolation to detect electrical current flows through the gap junctional network. A novel calibration approach is introduced to account for stream width variation in the device, and elastomeric valves are integrated to improve the performance of gap junction blocker assays. Ultimately, however, this approach is shown to be ineffective in detecting changes in gap junction impedance due to the gap junction blocker, 2-APB. A number of challenges associated with the technique are identified and analyzed in depth and important improvements are described for future iterations.


Processing and inspection of high-pressure microfluidics systems: A review

January 2025

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48 Reads

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1 Citation

In the field of microfluidics, high-pressure microfluidics technology, which utilizes high driving pressure for microfluidic analysis, is an evolving technology. This technology combines microfluidics and pressurization, where the flow of fluid is controlled by means of high-pressure-driven devices greater than 10 MPa. This paper first reviews the existing high-pressure microfluidics systems and describes their components and applications. Then, it summarizes several materials used in the microfabrication of high-pressure microfluidics chips, reviewing their properties, processing methods, and bonding methods. In addition, advanced laser processing techniques for the microfabrication of high-pressure microfluidics chips are described. Last, the paper examines the analytical detection methods employed in high-pressure microfluidics systems, encompassing optical and electrochemical detection methods. The review of analytical detection methods shows the different functions and application scenarios of high-pressure microfluidics systems. In summary, this study provides an efficient and advanced microfluidics system, which can be widely used in chemical engineering, food industry, and environmental engineering under high pressure conditions.


Design of 3D printed chip to improve sensitivity of platelet adhesion through reinjection: Effect of alcohol consumption on platelet adhesion

Monitoring platelet aggregation is crucial for predicting thrombotic diseases and identifying the risk of bleeding or resistance to antiplatelet drugs. This study developed a microfluidic device to measure platelet activation with high sensitivity. By controlling exposure time through repeated reinjections, the device enables the detection of subtle changes in platelet activity influenced by lifestyle factors, such as alcohol consumption. Using computational fluid dynamics simulations, the design was optimized to achieve moderate shear stresses and fabricated with 3D printing. Experimental results revealed that pillars biased to one side partially accelerate the flow and inhibit platelet adhesion. A distinct difference in platelet adhesion was clearly observed before and after alcohol consumption. Despite the high standard deviations in platelet adhesion area, hematocrit, and viscosity after alcohol consumption, the area covered by adhered platelets increased by 3.12 times compared to that before alcohol consumption. This microfluidic chip offers potential for personalized health monitoring by distinguishing platelet variations caused by lifestyle or dietary habits. However, challenges such as reinjection procedures and large sample volumes require further investigation.


Impact of dcEF on microRNA profiles in glioblastoma and exosomes using a novel microfluidic bioreactor

December 2024

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9 Reads

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1 Citation

Glioblastoma multiforme, the most common type of highly aggressive primary brain tumor, is influenced by complex molecular signaling pathways, where microRNAs (miRNAs) play a critical regulatory role. Originating from glial cells, glioblastoma cells are affected by the physiological direct current electric field (dcEF) in the central nervous system. While dcEF has been shown to affect glioblastoma migration (electrotaxis), the specific impact on glioblastoma intercellular communication and miRNA expression in glioblastoma cells and their exosomes remains unclear. This study aims to fill this gap by investigating the differential expression of microRNAs in glioblastoma cells and exosomes under dcEF stimulation. We have developed a novel, reversibly sealed dcEF stimulation bioreactor that ensures uniform dcEF stimulation across a large cell culture area, specifically targeting glioblastoma cells and primary human astrocytes. Using microarray analysis, we examined differential miRNA profiles in both cellular and exosomal RNAs. Our study identified shared molecular targets and pathways affected by dcEF stimulation. Our findings reveal significant changes in miRNA expression due to dcEF stimulation, with specific miRNAs, such as hsa-miR-4440 being up-regulated and hsa-miR-3201 and hsa-mir-548g being down-regulated. Future research will focus on elucidating the molecular mechanisms of these miRNAs and their potential as diagnostic biomarkers. The developed platform offers high-quality dcEF stimulation and rapid sample recovery, with potential applications in tissue engineering and multi-omics molecular analysis.


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