Julian
Menges
abc,
Claude
Meffan
bc,
Fabian
Dolamore
ac,
Conan
Fee
cd,
Renwick
Dobson
*acef and
Volker
Nock
*bcf
aSchool of Biological Sciences, University of Canterbury, Christchurch, New Zealand. E-mail: renwick.dobson@canterbury.ac.nz
bDepartment of Electrical and Computer Engineering, University of Canterbury, Christchurch, New Zealand. E-mail: volker.nock@canterbury.ac.nz
cBiomolecular Interaction Centre, University of Canterbury, Christchurch, New Zealand
dSchool of Product Design, University of Canterbury, Christchurch, New Zealand
eDepartment of Biochemistry and Molecular Biology, Bio21 Molecular Science and Biotechnology Institute, University of Melbourne, Victoria, Australia
fThe MacDiarmid Institute for Advanced Materials and Nanotechnology, Wellington, New Zealand
First published on 26th November 2020
Capillary systems are a promising technology for point-of-care microfluidics, since they are pre-programmable and self-powered. This work introduces “off valves” as a key building block for capillaric circuits, providing easy-to-use, multi-purpose valving functionality and autonomous flow control. To this end we present a set of switching valve designs that use trigger channels and liquid input alone to close or open connections between channels in a highly controllable fashion. The key element of all these valve designs is a new off trigger valve, which is characterised in detail here and holds the potential for transistor-like switching and resistance tuning. As an example for the potential applications of switching valves, we demonstrate how they can be used for flow resistance control in a complex microfluidic circuit and for sequential chemical loading into a reaction chamber. Use of the switching valves for the latter in particular allowed for the tuning of incubation times and volumetric measurement, thus confirming applicability of the valves for automated and self-powered immunoassays in point-of-care environments.
Key to the success of these systems is the control of liquid flow, commonly achieved by sequential filling of the capillary channels.1,5–10 To enable autonomous on-chip control of liquid flow, several basic operation units have been developed. Key units include inlets (), reservoirs (
), vents (
), capillary pumps (
), resistors (
), reaction pads (
) and, perhaps most importantly, passive trigger valves (
),1,2,10 which are crucial for the construction of retention burst valves that allow autonomous sequential filling.10
All systems described so far only allow for linear or tree-like setups with input channels, whereby reaction units and output units/capillary pumps are arranged in a sequential manner. Currently, there are no reports of feedback loops that change conditions upstream of a channel depending on the arrival of the fluid meniscus at a point further downstream. In addition, mixing of components on these devices has proven problematic because of the high flow resistance from mixers.11 In particular, the dissolution of solid reagents can be difficult because it requires a dwelling time for complete dissolution. Thus, there is a need for operation units that enable timed retention of the liquid, which would increase the applicability of capillarics.
We present a novel valve system, termed switching valves in analogy to electronics,12 where a trigger input acts as an on or off gate for a main channel, as shown in Fig. 1(a). In this particular case, the valves act as binary switches, but they also hold the potential for more transistor-like switching and resistance tuning. Key to the on gates is a self-sealing trigger channel that uses the novel off valve to close right after the trigger event. Depending on the on-chip system requirements, on valves come in two basic setups. First, connecting valves are used to form a bridge between filled channels, enabling sequential filling or reduction of flow resistance in long capillaric systems. Second, releasing valves are used to retain liquid for chemical uptake or synchronisation of channels. Finally, trigger channels can also be designed to time the trigger event by introducing flow resistors. Here, we describe the working principle of the off valves, their fabrication and experimental validation. We further characterise the dynamics of valve closing, as well as the quality of the seal, and demonstrate the use of the valves to realise related fluid control structures: and-off functionality, or-off functionality, on valves, connecting valves and release valves. Finally, we demonstrate the application of the valves in trigger timing and the reduction of flow resistance. The resulting fluid control structures are unique in their simplicity, and are capable of adding improved and novel functionalities to capillarics devices.
In brief, each sample was fabricated by an initial face cut (3.175 mm cutter) to level out the surface, followed by milling of each channel. Milling shallower channels was carried out first to avoid burring on the edges, and all channel steps were repeated at bottom height at the end of milling to remove burrs. The surface was then polished using acrylic polish (aluminium oxide-based CRC, code 9230), followed by ultrasonication for 1 min in ∼5% (v/v) aqueous isopropyl alcohol solution, washing with acetone, isopropyl alcohol and water and blow drying with nitrogen. To close microscopic cracks that arose during the milling process, the surface was coated with high molecular weight PMMA solution (average Mw = 996000, 2.5% in xylene; Sigma Aldrich, St Louis, MO, USA). Any remaining solvent was removed by drying samples at 90 °C for 5 min on a hotplate and keeping the hot sample under vacuum for at least 1 min. This process did not significantly alter the geometry, although the edge flow that is common among rectangular channels13 was reduced, indicating a slight channel rounding. However, the geometry change was too small to be observed on a light microscope. Finally, samples were plasma-treated ten times for 1 min, each time at 25 W, pulsed mode (ratio 50) using oxygen gas (3 sccm; Tergeo plasma cleaner, Pie Scientific, Union City, CA, USA), and 30 nm of SiO2 were sputtered (Edwards Auto500 DC/RF magnetron sputtering system, Edwards, UK) onto the surface to generate a robust and permanently hydrophilic layer. The samples were covered with a thin (2–3 mm) polydimethylsiloxane (PDMS; Sylgard 184, Electropar, NZ; mixed as given in instructions (10
:
1 w:w base:curing agent) and then cured at 80 °C for 2 h) layer, which acted as a hydrophobic cover-film. A frame holder was used to ensure a tight seal.
Microscope images (ESI,† Fig. S1) were captured using an Olympus BX60 fluorescence microscope or, for angled views, with a digital microscope (AM411, Dino-Lite).
Channel depth and surface roughness from milling were determined by coating the surface with sodium fluorescein and confocal microscope-based measurement (SP5 confocal laser scanning microscope system with a DMI6000 inverted microscope, Leica). Channels were found to be milled with ±5 μm z-tolerance, which is in the same range as the measured height of each cut (ESI,† Fig. S2).
The main component of the valve is a void volume, indicated in Fig. 1(a and b), which connects a large opening to a trigger channel, such that the small trigger channel opening and the large opening are separated. The width and height of the trigger channel is significantly smaller than that of the large opening. The small opening can be placed at any non-connecting point but, as discussed below, a ≥90° opening angle is beneficial because it acts as a stop valve.16
Incoming liquid from the main channel is pinned on the first sharp corner of the large opening and the valve is filled by meniscus progression along the remaining three walls until the valve is filled, as shown in Fig. 1(c), effectively widening the meniscus radius. The large opening has an opening angle of ≥90° to pin17 the meniscus and stop it from progressing into the void volume of the valve. In this way, the system acts in a similar fashion to a capillary stop valve.18 Once water enters the trigger channel, the proceeding meniscus builds up pressure that forces the meniscus in the big opening to recede (see Fig. 1(d)). The volume of the trigger channel needs to be sufficient to create a bubble that closes the main channel. To facilitate these mechanisms, the channels were sealed reversibly with a pressed on PDMS layer as illustrated by Fig. 1(e). The difference between contact and meniscus line in this configuration is described in Fig. 1(f).
Fig. 2(a) shows a sequence of experimentally obtained images illustrating the capillary flow inside the trigger valve, as described. Initially, the meniscus was pinned on one side of the opening, slowing down the progression. When the fluid front reached the other side (after 0.2 s), it cut off the opening and rapidly caught up with the meniscus front (0.24 s). In the rectangular channel used here, capillary flow was dominated by edge-flow, a phenomenon that appears as a result of very high capillary pressure in sharp edges of a channel.13,19
The speed at which the meniscus recedes is determined by the difference in capillary pressure between the menisci in the trigger channel and by the size of the large opening. Receding contact angles are commonly much lower than the static contact angle,20 which reduces the closing speed. In the case presented here, contact angles of θstat = 9.75° (±1.25°, static) and θrec ∼ 0° (not detectable, receding) were measured, which is typical for freshly cleaned and stabilised silicon dioxide surfaces.21 This implies that the true capillary pressure for a receding meniscus would be significantly higher than for the proceeding meniscus in a channel of the same geometry. Therefore, the larger the size difference between the cross-sections of the opening and triggering channel, the faster and more effective the closing of the channel is expected to be.
Assuming a receding contact angle (θrec) of approximately 0°, the meniscus would form a half dome in the opening, which then further recedes. The necessary pressure to push back the meniscus can be determined by the Laplace equation,22 but the model needs to be adjusted for rectangular channels with different contact angles on each wall. In our experiments, the large opening and the trigger channel had a rectangular cross-section, were made from hydrophilised PMMA and were enclosed on the fourth side with PDMS. Therefore, the pressure can be approximated using the equations for capillary pressure in rectangular channels,23 which are derived from the Young–Laplace equations:24
As illustrated in Fig. 2(b–d), the time taken to close each valve was dependent on the geometry of the trigger channels and off valves. For narrow (100 μm) channels, closing was fast with times below 0.4 s and the main influence of the geometry appeared to be the flow resistance,2 as the closing times increased towards smaller channels. In wider channels, capillary action appeared to be the main influence, as channels above 50 μm depths had significantly increased closing times. For off valves, a depth of at least 200 μm appeared best for fast closing using 250 × 50 μm trigger channels. Note: errors here appear high, but the results suggest that this is largely due to the sealing method used, as the plots between experiments are offset from each other. Pressing PDMS onto the chip can result in small variations in effective channel height and thus offset the whole graph. Additionally, the environmental parameters air moisture and temperature also affect the chip. As such, within one experiment the error range could not be determined, but appears to be significantly smaller than the error bars suggest. Research is ongoing to find a more reliable sealing method, which can provide the ease of handling of the PDMS lid.
As time progressed, the bubble was pushed further into the main channel if the difference in capillary pressure was sufficiently high. This problem can be addressed by adding a small barrier at the in- and outlet sections of the off valve. We found this to be moderately stable at 25 μm height, with full stability achieved at 100 μm (total channel height 200 μm; ESI,† Fig. S3). Future designs could instead vary the width in the trigger channel to achieve fast closing. Other designs may feature connected trigger channels to close off several channels at once. Video footage of this experiment is provided in the ESI† (V1).
Occasionally, a thin fluid connection was observed within the valves, which was attributed to the air bubble being unable to push completely into the edges of the channel. This issue could be resolved by rounding the channel profile and further optimising the geometry, similar to previous work on valves in PDMS25 or as depicted in the following. The meniscus at the large opening of the off valve was bent slightly inwards during capillary filling, enhancing meniscus stability at the opening. This was attributed to the difference in capillary pressure. In later experiments, off valves were used in a channel that was not drained on one end, and minor manufacturing errors destabilised the meniscus, leading to valve failure. To counteract this, the opening angle was simply increased beyond 180° resulting in long-term stability.
Next, we performed a qualitative test of the seal provided by the gas bubble. The blue dye solution from the inlet reservoir was removed and yellow dye was added to the outlet reservoir to apply a counter pressure (ESI,† Fig. S4). Mixing at the inlet section and diffusion were observed. As a result of the counter-pressure applied from the yellow dye reservoir, the trigger channels continued to fill up, further increasing the size of the bubble. Additionally, the bubbles could be pushed in the direction of the blue dye reservoir, occasionally pushing them into the distributor channel. Because this channel had greater width and height, the bubble drained into it very quickly, leaving a smaller bubble to seal the channel. However, the seal remained intact, as indicated by the remaining blue dye. Issues like these may simply be addressed in future applications by limiting the trigger channel volume to about the volume of the maximum desired bubble or by adding a tight junction in the main channel. Video footage of this experiment is provided in the ESI† (V2). The valve setup in this video relates to valve width screening experiments, which were outside the relevant range as the soft PDMS lid starts bending into the wider channels, effectively reversing the expected effect. As such, this experiment is not discussed here other than as an example of valve sealing.
As shown in Fig. 3(e–g), the off valve could also be embedded into a dividing main channel to turn off the two branches simultaneously. The geometry was symmetrical to guarantee similar filling speeds into both branches.
During these experiments, it was observed that by rounding the shape of the branching off valve, the edge-flow could be reduced, and thus the quality of the seal improved. We suggest that this results from the radius of the walls: the surface tension counteracts the capillary force that usually keeps the liquid at the edge, thus minimising edge flow. From these results, optimised designs (ESI,† Fig. S5(a) and Movie V1/V2) can be derived. The second design (ESI,† Fig. S5(b)) shows an improvement to stabilise the meniscus at the large opening. The concept of increasing the contact angle above 180° is based on previous literature.16 This is useful when there is a need for the meniscus to be pinned for a prolonged period or if the liquid has a low surface tension. This design was used in the sequential release setup described later.
To visualise the flow behaviour inside the switching valve and channels, the supply channel was filled with yellow dye and the main channel with blue dye. The two colours were chosen to yield a large contrast so that even the faintest mixing would be visible. As shown in Fig. 4(c–d), triggering induced a flow that almost completely overtook the flow from the blue dye reservoir. The triggering of all trigger valves occurred almost instantaneously (at ∼0.04–0.08 s in this example) after the meniscus reached the first valve. This speed in triggering can be explained by the flow resistance from the (yellow) supply channel being negligible in comparison with the narrower trigger channel. Without the additional closing valve in the trigger channel, a very low residual backflow through the trigger channel remained visible even for large resistors. By introducing an off valve into the trigger channel, the latter could be sealed after ∼1–3 s, preventing any further backflow. The valve showed almost complete inhibition of backflow, as shown by the presence of blue dye in the trigger channel even after 45 s (end of experiment). Once triggered, the connecting on-valve acts as a bridge between channels, meaning mixing between the two is enabled. Flow ratios thus depend on the resistance or flow rates in the main and supply channel. Video footage of this experiment is provided in the ESI† (V4).
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Fig. 5 Experimental demonstration of flow resistance reduction and trigger timing. (a) Simplified circuit diagram for demonstration setup. Resistor R1 represents the resistance from a longer circuit (e.g., mixers, reaction pads and other structures). R2 is used to tune the timing of the trigger event, while the evaluation loop (R3) is used to measure flow rates. (b) Top-down photograph of the fabricated demonstration platform. Each chip contains three circuits with different-sized resistors. All draw liquid from the same reservoir through a wide channel to maximise comparability. The main and supply channels were milled with a round bottom tool to 200 μm in both width and depth. The trigger channels were rectangular, 100 μm wide and 150 μm deep. The trigger valves in the switching valve were 100 μm wide and deep. (c) Plot of the liquid volumes of trigger channel R2 over time (correlates with meniscus position). (d) Plot of the liquid volume of evaluation resistor R3. The triggering event is marked in (a) and (b) by the blue bars connecting the diagrams. Graphs at higher experiment times continue to show the behaviour of classic capillary flow.2,26 Time t = 0 was defined as the time at which water entered the trigger channel. |
In this setup, the primary resistor (R1) resembled the resistance of a longer capillary circuit. The main channel passed the switching valve and led to the inlet of a trigger channel, which contained a resistor (R2) for timing and to reduce backflow to a minimum. Resistor R3 was only used to monitor the filling volume and thus the flow rates. The supply channel on the switching valve was directly attached to the main inlet and had much lower flow resistance than R1. This resulted in bridging of R1 when the switching valve was activated.
The results displayed in Fig. 5(c–d) demonstrate how timing is affected by trigger channel length. Each measurement was obtained from a single experiment. Graphs show the meniscus progression represented by the filling volume. Because surface properties vary slightly over time, the slope of each graph varied; however, the same general effect was observed across several experiments. When the liquid entered trigger channel R2, the flow behaviour in the trigger channel was similar to regular capillary flow in a straight capillary until shortly before the triggering event (see Fig. 5(c)). This type of capillary flow has been described previously2,26 by the formula:
In comparison, the flow in the evaluation resistor was strongly reduced during filling of the timing resistor. As illustrated in Fig. 5(d), liquid was drained into the significantly smaller trigger channel, reducing the flow in R3 to almost zero. With increasing filling of R2, the flow resistance increased and allowed liquid to be pulled into R3. Through the triggering event, the liquid in the evaluation resistor showed normal capillary flow behaviour, as described above.
Another observation from these experiments was a slowing in meniscus speed immediately prior to the triggering event which can be seen as the dip in the curves at the marked areas (Fig. 5). This behaviour was observed in all experiments with on-valves. Although the exact mechanism is yet unknown, we propose this might be caused by electrostatic repulsion of the contact lines due to the surface layer of surfactant that is contained in the dye, or by similar effects.27
Changes in the preset flow resistance caused by changes in the length of R1 resulted in a significant increase in the flow rate throughout the triggering event (ESI,† Fig. S7). The maximum and end flow rates were comparable, as the flow resistance was dominated by the low resistance through the switching valve. Differences in maximum flow rate mainly resulted from the higher volume in R3 at the point of the triggering event and noise arising from the binarization of the footage (noise correlates with the size of the black and white border). The latter did not increase with time, but was dependent on the filling volume (the black area on the binarized video). Trigger timing was influenced by the preset flow resistance (R1), as suggested by the blue markers in (ESI,† Fig. S7(a) and (b)). The filling of the trigger channel (R2) slowed, and the effect appeared to decrease with increasing preset resistance R1. Video footage is provided in the ESI† (V6 and V7). These results demonstrate how on-valves enable control of timing and flow resistances, which is necessary to ensure short experiment times in point-of-care diagnostics and for industrial application of microfluidics.
The design featured the combination of a connecting valve with self-sealing trigger channel and an off valve that closed the primary channel. By repeating this arrangement, any number of channels could be addressed. Each dye entered the chamber and was rinsed with water as the dye travelled through the system with the liquid front. Trigger channels were attached to the capillary pump (long channel) in distinct locations so that they triggered the switch between channels after the dye had passed and had been rinsed out of the chamber. When the trigger channels fill, the meniscus in the main channel is slowed down as the liquid is drained. With continued filling, this effect ceases and meniscus progression in the trigger channels slows down uncontrollably. The off valves contribute to that as the meniscus widens in them. Therefore, the main channel is widened just after the trigger channel inlets to temporarily decrease capillary pressure and thus drainage into the main channel. Because the device shown here was not fully optimised, some mixing occurred during the triggering events, and timing of the triggering events was not implemented. Benefits of this setup over others are thought to be the ease of prediction for triggering events, the versatility for different sample states (dry or liquid), simple volume and flow rate definition and simple fabrication and thus rapid prototyping. Video footage of this experiment is provided in the ESI† (V8).
While not shown here, we suggest that incubation times can be tuned by adjusting the flow rates through small volume flow resistors in front of each pump, as well as an arrangement of releasing switching valves to address each flow resistor individually if needed. In future designs, this setup could be used to deliver analyte and antibody solutions to a reaction pad with precise incubation timing to conduct immunosorbent assays, which is an advance on previously reported devices.5,6,8,9 As such a device would only require the input of analyte and water, it would be ideal for point-of-care diagnostics.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0lc00811g |
This journal is © The Royal Society of Chemistry 2021 |