Here, we present a protocol to investigate multi-component phase diagrams using externally controlled magnetic beads as liquid carriers in a lab-in-tube approach. This approach can aid in applications that seek to gather further information on phase change in complex liquid systems.
Magnetic beads with ~1.9 µm average diameter were used to transport microliter volumes of liquids between contiguous liquid segments with a tube for the purpose of investigating phase change of those liquid segments. The magnetic beads were externally controlled using a magnet, allowing for the beads to bridge the air valve between the adjacent liquid segments. A hydrophobic coating was applied to the inner surface of the tube to enhance the separation between two liquid segments. The applied magnetic field formed an aggregate cluster of magnetic beads, capturing a certain liquid amount within the cluster that is referred to as carry-over volume. A fluorescent dye was added to one liquid segment, followed by a series of liquid transfers, which then changed the fluorescence intensity in the neighboring liquid segment. Based on the numerical analysis of the measured fluorescence intensity change, the carry-over volume per mass of magnetic beads has been found to be ~2 to 3 µl/mg. This small amount of liquid allowed for the use of comparatively small liquid segments of a couple hundred microliters, enhancing the feasibility of the device for a lab-in-tube approach. This technique of applying small compositional variation in a liquid volume was applied to analyzing the binary phase diagram between water and the surfactant C12E5 (pentaethylene glycol monododecyl ether), leading to quicker analysis with smaller sample volumes than conventional methods.
Magnetic beads (MBs) on the order of 1 micrometer in diameter have been used1,2 quite often in microfluidic-based applications, particularly for biomedical devices. In these devices, MBs have offered capabilities such as cell and nucleic acid separation, contrast agents, and drug delivery, to name a few. The combination of external (magnetic field) control and droplet-based microfluidics has enabled3 control of immunoassays using small volumes (<100 nl). MBs have also shown promise when used for liquid handling4. This approach uses the MBs to transport biomolecules between liquid segments within a tube separated by an air valve. This method is not as powerful as other more complex lab-on-chip devices seen in the past, but it is much simpler and does offer the capability of handling microliter-sized volumes of liquid. A similar approach has recently been reported5 by Haselton’s group and applied to biomedical assays.
One of the most important aspect of this device is the liquid segment separation offered by the surface-tension-controlled air valve. Microliter volumes of liquid attached to MBs are transported through this air gap between liquid segments using an externally applied magnetic field. Microparticle MBs (from ~0.4-7 µm in diameter with an average of 1.9 µm) under the effect of the external magnetic field create a micro-porous cluster that traps liquid within. The strength of this liquid entrapment is sufficient to withstand the forces of surface tension when transporting the MBs from one reservoir to the next. Typically, this effect is undesirable, as most approaches only want transport of specific molecules (such as biomarkers) contained within the liquids6. However, as can be seen in our work, this effect can be utilized to become a positive aspect of the device.
We have utilized this ‘lab-in-tube’ approach, shown schematically in Figure 1, for analyzing phase diagrams in binary materials systems. The surfactant C12E5 has been chosen as the main focus of characterization, as it is widely used in industrial applications such as pharmaceuticals, food products, cosmetics, etc. In particular, the H2O/C12E5 binary system was investigated because it provides a rich set of phases to explore. We have focused on one specific aspect of this chemical mixture, namely the transitions to liquid crystalline phases under certain concentrations7-9. This transition is readily observed in our device by incorporating polarizers in the optical microscopy studies in order to highlight phase boundaries.
Being able to map phase diagrams is a very important area of study in order to understand the kinetics involved with phase transition10. The ability to precisely determine the interaction of surfactants with solvents and other components is crucial due to their complexity and many distinct phases11. Many other techniques have previously been used to characterize phase change. The conventional approach involves making many samples, each consisting of different concentrations and allowing them to equilibrate, which requires lengthy processing times and high quantity of sample volumes. Then, samples are typically analyzed by optical methods such as diffusive interfacial transport (DIT), which offers high-resolution of such surfactant compositions12,13. Similar to the method we have utilized, the DIT method uses polarized light to image distinct phase boundaries.
1. Preparation of One-Time Use Materials in Device
2. Preparation of Experimental Setup for Fluorescence Experiments
3. Experimental Procedure for Fluorescence Experiments
4. Numerical Analysis of Fluorescent Data
5. Preparation of Experimental Setup for Surfactant Experiments
6. Experimental Procedure for Surfactant Experiments
Using the Lab-in-Tube approach for transporting µl-volume amounts of liquid with magnetic beads along with MATLAB for numerical analysis, average liquid carry-over volumes, as a function of magnetic bead mass, were found (Figure 2). Higher mass of magnetic beads provides higher carry-over volume in the rate of 2-3 µl/mg. The experimental setup (Figure 1) was used to observe phase change within the H2O/C12E5 binary system. Since the H2O/C12E5 system is well-known and has many distinct phases, which can be seen in Figure 3B, it served as an appropriate point of reference to further characterize our device. The dashed line in Figure 3B shows the nominal temperature that experiments were performed at of ~ 20 °C. Reactions were carefully observed from short times, such as 0 to 90 sec seen in Figure 3C, to longer times, such as 1.5 to 25 min seen in Figure 4. The L1 to Lα phase change was used to verify carry-over volume in the H2O/C12E5 binary system. Short term observation shows phase transitions into various liquid crystalline phases when the carried water is transferred into the C12E5 surfactant chamber. However, this phase change can be temporal as diffusion continues to reach a homogenous state in the liquid chamber. Eventually, the multiple transfers will lead to a permanent phase change as shown in Figure 5B. Even though a hydrophobic coating was applied to the inner-wall of the tube, one concern of our device was variation in carry-over volume due to liquid sticking to the inner-wall of the tube as larger volumes were pumped back-and-forth. One way to disprove this concern was to remove the magnetic beads from the device and carry out the same experiments exactly as if the magnetic beads were still in place. This would eliminate the carry-over volume, allowing us to observe any effects on chemical composition originating from this undesired liquid transfer. A comparison of phase change seen when the magnetic beads are in place (Figure 5 A, B) versus when they’re removed from the system (Figure 5 C, D) was made. Fortunately, this concern was found to be insignificant when compared to the carry-over volume.
Figure 1. Schematic diagram of experimental setup and photo of tube used showing two liquid segments separated by an air valve. Reprinted (adapted) with permission from Blumenschein, N., Han, D., Caggioni, M., Steckl, A. Magnetic Particles as Liquid Carriers in the Microfluidic Lab-in-Tube Approach To Detect Phase Change. ACS Applied Materials & Interfaces. 6 (11), 8066-8072, doi: 10.1021/am502845p (2014). Copyright 2014 American Chemical Society. Please click here to view a larger version of this figure.
Figure 2. Average liquid carry-over volume per transfer vs. magnetic bead mass. Numerical analysis of plot using MATLAB. Reprinted (adapted) with permission from Blumenschein, N., Han, D., Caggioni, M., Steckl, A. Magnetic Particles as Liquid Carriers in the Microfluidic Lab-in-Tube Approach To Detect Phase Change. ACS Applied Materials & Interfaces. 6 (11), 8066-8072, doi: 10.1021/am502845p (2014). Copyright 2014 American Chemical Society. Please click here to view a larger version of this figure.
Figure 3. (A) Lab-in-tube experimental setup. (B) Phase change plot of the H2O/C12E5 binary system. (C) Observed phase change of H2O/C12E5 from 0 to 90 sec. Reprinted (adapted) with permission from Blumenschein, N., Han, D., Caggioni, M., Steckl, A. Magnetic Particles as Liquid Carriers in the Microfluidic Lab-in-Tube Approach To Detect Phase Change. ACS Applied Materials & Interfaces. 6 (11), 8066-8072, doi: 10.1021/am502845p (2014). Copyright 2014 American Chemical Society. Please click here to view a larger version of this figure.
Figure 4. H2O/C12E5 phase change over period of 1.5 to 25 min. Reprinted (adapted) with permission from Blumenschein, N., Han, D., Caggioni, M., Steckl, A. Magnetic Particles as Liquid Carriers in the Microfluidic Lab-in-Tube Approach To Detect Phase Change. ACS Applied Materials & Interfaces. 6 (11), 8066-8072, doi: 10.1021/am502845p (2014). Copyright 2014 American Chemical Society. Please click here to view a larger version of this figure.
Figure 5. Two devices prepared with a test chamber initial concentration of 1:1 H2O/C12E5 and reservoir containing pure C12E5. Using ~0.2 mg beads from initial condition (A) to 6 transfers (B), the sample transitions from L1 to Lα phase. In the absence of MBs, no phase change is seen (C, D). Experiment was performed at 25 °C. Reprinted (adapted) with permission from Blumenschein, N., Han, D., Caggioni, M., Steckl, A. Magnetic Particles as Liquid Carriers in the Microfluidic Lab-in-Tube Approach To Detect Phase Change. ACS Applied Materials & Interfaces. 6 (11), 8066-8072, doi: 10.1021/am502845p (2014). Copyright 2014 American Chemical Society. Please click here to view a larger version of this figure.
In most common techniques for phase diagram investigation, multiple samples with different compositions and ratios need to be prepared and have to reach thermodynamic equilibrium which causes a lengthy process and a significant amount of material. Some challenges can be resolved by DIT (diffusive interfacial transport) method using flat capillary and the infrared analysis method, but none of them can resolve all challenges with low cost investment.
The feasibility of using magnetic beads as liquid carriers in this microfluidic “lab-in-tube” approach was demonstrated for the use of detecting phase change between adjacent liquid segments. This method allows for precise composition change, which can be predetermined using the shown numerical analysis technique. The ability to view live changes in a water-surfactant system while making miniscule alterations to the chemical make-up proved to be a valuable asset in this device. Current techniques used in industry for analyzing phase change have some undesirable aspects associated. Cost is always a concern, and having the ability to use such small volumes of expensive chemicals like C12E5 during experimentation is certainly an advantage. Likewise, when reducing sample size, the wait time for the diffusion process to take place is reduced significantly. The H2O/C12E5 system is fairly complex and can take a long time to settle into a specific phase when its composition is altered. These lengthy diffusion times may appear to be undesirable, but when comparing it to diffusion times of methods practiced in industry, it is quickly seen as a progressive step in analyzing composition of intricate systems.
When analyzing phase change of a binary system, or any number of mixed chemicals, it is crucial to have adequate precision in the method being used. Much time was spent finding a relationship between the carry-over volume and magnetic bead mass. A few different variables, such as magnetic bead cluster porosity, test chamber volume versus reservoir volume, and magnetic bead cluster mass, were studied, allowing us to amalgamate different sets of data and create a model. During this process, the big takeaway was the obtained linear relationship between carry-over volume and magnetic bead cluster mass. We found the carry-over volume to be ~2 to 3 µl/mg of beads. Of course, this relationship doesn’t correlate with the test chamber and reservoir volumes, allowing for more complex experimentation methods. Meaning, since the carry-over volume acts almost as a constant depending on magnetic bead mass, the liquid volumes in the system can be predetermined to create desired step changes in the composition of the two liquids. This can come in handy when the user wants to see composition fluctuations anywhere from 0.25% to 10%.
The protocol provides high feasibility for exploring phase diagram with small sample quantity and fine resolution on the composition. However, current protocol still requires several minutes for single transfer, leading to days for complete phase diagram investigation. This limitation can be overcome either by using thinner tube diameter or mechanical actuation induced by external magnetic field variation.
The authors have nothing to disclose.
The authors acknowledge many useful discussions with M. Caggioni and support from Proctor and Gamble in the form of an internship for NAB.
AccuBead | Bioneer Inc. | TS-1010-1 | Magnetic beads |
C12E5 Surfactant | Sigma-Aldrich | 76437 | |
Thermo Scientific Nalgene 890 | Fisher Scientific | 14176178 | |
Cube Magnet | Apex Magnets | M1CU | |
Polarizer Film | Edmund Optics | 38-493 | |
Teflon AF | Dupont | 400s1-100-1 | Fluoropolymer solution |
Keyacid Red Dye | Keystone | 601-001-49 | Fluorescent dye |
Luer-Lock | Cole-Parmer | T-45502-12 | Female |
Luer-Lock | Cole-Parmer | T-45502-56 | Male |
Syringe | Fisher Scientific | 14-823-435 | 3 mL |
Syringe Pump | Stoelting | 53130 | |
Stereo Microscope | Nikon | SMZ-2T | |
Inverted Microscope | Nikon | Eclipse Ti-U | The filter cube used had an excitation wavelength range from 540-580 nm and a dichroic mirror at 585 nm, allowing for photoemission ranging from 593-668 nm. |
Balance | Denver Instruments | PI-225D | |
Microscope-Mounted Camera | Motic | 5000 |