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TA : Pelin Kübra İşgör |
Topics covered:
Microfluidic systems
Droplet generation devices
Fabrication of microfluidic devices
Introduction to Elveflow pressure pump and Microqubic 3D digital microscope
Droplet generation at varying sizes
Droplet detection using via video/image processing
Experiment details:
DROPLET GENERATION EXPERIMENT
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Microfluidics is the key science and technology that enables fluid manipulation and control in channels that have dimensions on the order of micrometers (Fig.1). The change in fluid physics in microscale ensures novel use of microfluidic systems. Although the first microfluidic device was a gas chromatograph invented in 1975, these systems have not used for biological or chemical applications since 1990s [4]. Microfluidic device fabrication technology was derived from microelectromechanical system (MEMS) technology.
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During the last decades, microfluidic systems became a widespread research area and gave birth to easy-to-use and miniaturized platforms that can be applied to biological and chemical analysis. Microfluidics can be divided into three groups as continuous microfluidics, discrete (multi-phase flow, droplet-based, segmented flow) microfluidics and digital microfluidics (Fig.2.).
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Continuous microfluidics is based on continuous liquid flow manipulation. These systems are usually used for simple and well-defined functions such as chemical separation and biochemical applications. Since the surface property of the entire system affects fluid flow at any location in the system, these systems are not suitable for integration and scalability. Discrete microfluidics compartmentalizes and manipulates small volumes of liquid with two immiscible phases. Microdroplets are suitable for very small amount of liquid handling. Since droplet is isolated from its surrounding, any material inside droplet (reagent, cell, protein etc.) is preserved throughout the system. Droplet loading, mixing, sorting, merging, break-up enables high-throughput chemical and biological experimentation due to kHz level droplet generation. Both continuous and discrete microfluidics operate in microchannels. However, digital microfluidics is manipulation of small liquid volumes on open structures using electrowetting method. Electrowetting is changing surface properties of a material by applying electric field. On independently addressed electrodes, a small volume of liquid is moved from one electrode to another. These systems enable merging of different material loaded droplets. Electrowetting on-dielectric (EWOD) is a common method in digital microfluidics.
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Paper-based microfluidic systems are considered Microfluidics 2.0. This method is inexpensive and easy-to-use. Changing hydrophobicity of the paper at different zones using a printer and wax, channels are fabricated [5]. Printing reagents and other materials to the test zones makes microfluidic paper-based analytical devices (µPADs) cheaper point-of-care diagnostic devices. Being user-friendly and cheap, paper-based microfluidic systems are developed for disease diagnostics in third world countries [6].
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Glass, Si and polymers are the three main materials for fabricating microchannels. According to application, any of these three materials can be used. Si wafer is not a suitable material for optical measurement techniques due to its opacity. Glass is a fragile material and etching it rather difficult than etching a Si wafer. The bonding process requires high voltages or temperatures. Also, a clean room was needed for the fabrication process [7]. The dimensions of polymers change when they interact with some chemicals such as alcohols. Silicon can be used for applications requiring high temperatures such as quantum dot synthesis [8]. Glass microchannels are resistant to chemicals and reusable. A polymer type, polymethylmethacrylate (PMMA), is suitable for high volume production of cartridges. On the other hand, polydimethylsiloxane (PDMS), is the "working horse" of scientists, since it is a non-toxic, opaque material and can be cured at low temperatures. PDMS is a rather cheap material and fabrication of a microfluidic device becomes quite easy with soft lithography techniques. Microfluidic systems are integrated with different components to operate properly. Pumps, valves, mixers, pressure and flow sensors are some of the fluidic components that are integrated with microfluidic systems.
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Two immiscible fluids are driven from two separate channels and meet at a junction that is determined by the specific geometry of the channels. In 2001, Thorsen et al. published an article titled "Dynamic pattern formation in a Vesicle-Generating Microfluidic Device" [16]. For the first time, they accomplished droplet generation with two immiscible fluids using a T-junction. Both water and oil were continuously driven to the microchannel (Fig.3). The water obstructs the main channel at the junction, while oil flows through the channel. At this moment, high shear forces occur. The flow is not linear and static due to interactions between the boundary of two liquids. This instability arises from the competition between surface tension and shear forces. The competition generates droplets. The size and speed of droplets are finely tuned by adjusting water and oil flow rates or pressures.Fig. x Droplet generation strategies: (ii) T-Junction in a planar chip format ; (iii) flow focusing in a planar chip
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Anna et al. used flow-focusing technique in a planar microchannel to form droplets [17]. In this technique, two immiscible phases are driven to the one orifice, where the outer channel carries oil, and the inner channel carries water. These three channels form a cross at the intersection. The oil comes from two sides of the water and applies pressure to it so that water breaks into droplets. Using this technique, varying size of droplets can be generated at very high speeds. Three regimes occur during droplet formation depending on physical properties of fluids and external variables. These regimes are categorized as squeezing, dripping and jetting [18]. The physical properties of liquids such as interfacial tensions, viscosities, and external variables as flow rates of fluids, channel dimensions and geometry are used to categorize droplet formations [19]. The dimensionless numbers originated from aforementioned variables determine these regimes. Capillary (Ca) number is the most important dimensionless number for droplet formation and its value varies between 10-3 and 10 (Eq. 1). In Eq. 1, µ is the dynamic viscosity of the fluid, V is velocity of the fluid and is interfacial tension between two liquids. Capillary number relates viscous forces with interfacial tension.
Eq Ca=(μ*V)/γ Eq.1
Abate et al. stated that monodisperse droplets are generated at low capillary numbers for T-junctions and at high capillary numbers for flow-focusing devices [19]. In a T-junction two regimes occur: squeezing and dripping. When dispersed phase (water) completely blocks the mainstream channel and there is pressure drop along the droplet due to channel blockage, the regime is called squeezing regime. In dripping regime, droplets do not completely block the main channel and are smaller than the dimension of the main channel. In a flow-focusing device dripping and jetting are two regimes that occur during droplet formation. In dripping regime, the dispersed phase breaks now it enters the junction and turns into droplets. These droplets are immediately carried away by continuous phase. In jetting regime, dispersed phase goes into continuous phase and for a while they co-exist in the main channel [18].
How do we use Navier-Stokes eqn for microfluidics?
Fabrication of microfluidic devices
For fabrication of microchannel molds, a negative photoresist, SU-8 2050, can be used by applying photolithography techniques. During this process, a transparency mask can be used. SU-8 2050 can be spin coated on Si wafer. At the end of the process, SU8 developer was used for getting the microchannel structure. Process flow is given in Figure 3.1. The Navier-Stokes equations are a set of partial differential equations that describe the motion of viscous fluids (Fig.4). These equations are crucial in understanding fluid dynamics, including the behavior of fluids in microfluidic devices.
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In microfluidics, the flow regime is often laminar, meaning the fluid particles move in parallel layers without significant mixing. This is due to the small scale of microfluidic channels, where viscous forces dominate over inertial forces. The Navier-Stokes equations, when simplified for laminar flow, provide a powerful tool for analyzing and predicting the behavior of fluids in these devices.
Key aspects of how the Navier-Stokes equations define microfluidics include:
Laminar flow: The equations can be simplified for laminar flow, making them easier to solve and analyze.
Viscous forces: The equations account for viscous forces, which are particularly significant in microfluidic channels due to their small size.
Pressure gradients: The equations can be used to calculate pressure gradients, which drive fluid flow in microfluidic devices.
Velocity profiles: The equations can be used to determine the velocity profile of the fluid within the channel, which is important for understanding flow behavior.
Design and optimization: The equations can be used to design and optimize microfluidic devices, ensuring that the desired flow characteristics are achieved.
In summary, the Navier-Stokes equations are fundamental to understanding and designing microfluidic systems. By providing a mathematical framework for describing fluid flow, these equations enable researchers and engineers to analyze and optimize the performance of microfluidic devices for various applications.
Fabrication of microfluidic devices
Photolithography is a cornerstone technique in microfluidic device fabrication. It involves transferring a pattern from a photomask onto a substrate using light.
Si wafer Preparation: A Si wafer is cleaned and prepared for the lithography process.
Photoresist Application: A light-sensitive negative SU-8 photoresist is spin-coated onto the substrate, forming a thin, uniform layer.
Photomask Exposure: The photomask, containing the desired pattern, is placed over the photoresist. UV light is then shone through the mask, exposing the photoresist in the patterned areas.
Development: The exposed photoresist is developed in a chemical solution. The exposed areas are either removed (positive photoresist) or remain (negative photoresist), depending on the type of photoresist used.
Channel Formation with soft lithography : Soft lithography is a method that refers to replicating mold structure using polymeric, "soft", materials by stamping. For fabrication of microchannels, PDMS (polydimethylsiloxane) is poured on Si wafer and heated on a hot plate. Cured PDMS is peeled off from the Si wafer, cut and punched.
Bonding :The cut PDMS substrate that contains 3 edges of the microfluidic channel is then bonded to a glass slide to close the microchannels via oxygen plasma.
Other Fabrication Techniques: While photolithography is a widely used method, other techniques can also be employed for microfluidic device fabrication, such as:
Laser Ablation: A laser beam is used
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to remove material from a substrate, creating microchannels or features.
3D Printing: Additive manufacturing techniques can be used to directly fabricate microfluidic devices.
The choice of fabrication technique depends on factors such as the desired device complexity,material properties, and cost. Careful optimization of the fabrication process is essential to ensure the desired performance and reproducibility of microfluidic devices.
Process flow is given in Fig.5.
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Hardware
The experimental system comprised of Elveflow pressure pump, Microqubic 3D digital microscope and microfluidic flow focusing device.
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Figure X : Set-up photo with insets