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Method Article
We present protocols for simple actin filament microfluidic assays, in combination with fluorescence microscopy, that allow one to accurately monitor individual actin filaments in real-time while sequentially exposing them to different protein solutions.
In order to decipher the complex molecular mechanisms that regulate the assembly and disassembly of actin filaments, it is a great asset to monitor individual reactions live in well-controlled conditions. To do so, live single-filament experiments have emerged over the past 20 years, mostly using total internal reflection fluorescence (TIRF) microscopy, and have provided a trove of key results. In 2011, in order to further expand the possibilities of these experiments and to avoid recurring problematic artifacts, we introduced simple microfluidics in these assays. This study details our basic protocol, where individual actin filaments are anchored by one end to the passivated coverslip surface, align with the flow, and can be successively exposed to different protein solutions. We also present the protocols for specific applications and explain how controlled mechanical forces can be applied, thanks to the viscous drag of the flowing solution. We highlight the technical caveats of these experiments and briefly present possible developments based on this technique. These protocols and explanations, along with today's availability of easy-to-use microfluidics equipment, should allow non-specialists to implement this assay in their labs.
The assembly and disassembly of actin filaments and actin filament networks are controlled by several biochemical reactions and depend on the mechanical context. In order to gain insight into these complex mechanisms, it is invaluable to be able to observe individual reactions on individual filaments (in sufficiently large numbers). Over the past decades, the observation of dynamic actin filaments in real-time, mostly using total internal reflection fluorescence (TIRF) microscopy, has emerged as a key technique and has provided an impressive list of results that could not have been obtained with bulk solution biochemical assays1.
To achieve this, one needs to maintain fluorescently labeled actin filaments close to the surface of the microscope coverslip while exposing them to solutions of actin-binding proteins (ABPs), which can also be fluorescently labeled. Doing so provides a means to monitor events taking place on individual filaments in well-controlled biochemical conditions, and thus quantify reaction rates. However, a number of specific limitations should be considered. Artificially maintaining filaments close to the surface, often thanks to multiple anchoring points or by using a crowding agent such as methylcellulose, can alter their behavior (e.g., causing pauses in their polymerization and depolymerization2). Tracking the contour of each filament can be challenging, particularly if new filaments or filament fragments accumulate in the field of view over time. The reactions take place in a finite volume where the concentration of actin monomers and ABPs can vary over time, potentially making it difficult to derive accurate rate constants. Finally, renewing or changing the solution of ABPs is difficult to achieve in less than 30 s and will often lead to inhomogeneous protein content in the sample.
A bit over 10 years ago, inspired by what was already done to study individual Deoxyribonucleic Acid (DNA) strands3, we introduced a new technique based on microfluidics to observe and manipulate individual actin filaments4. It allows one to circumvent the aforementioned limitations of classical single-filament techniques. In these microfluidics assays, actin filaments are grown from spectrin-actin seeds adsorbed on the coverslip. Filaments are thus anchored by one end only to the bottom of the microfluidic chamber and fluctuate above the surface without sticking. Filaments align with the flow of incoming solutions, thereby easing the monitoring of their contour length and maintaining them in a shallow region above the coverslip where TIRF can be used. Different solutions are simultaneously flowed into the chamber without mixing, and the filaments can be exposed to them sequentially and rapidly.
Here, we propose a series of basic protocols to set up single-actin-filament microfluidics assays in the lab. Coverslips and microfluidics chambers can be prepared in advance (in half a day), and the experiment itself, where several biochemical conditions can be tested, is done in less than a day.
1. Microfluidic chamber preparation
2. Glass coverslip cleaning
NOTE: Here, a standard coverslip cleaning procedure, based on a series of sonication steps, is detailed. Other glass coverslip-cleaning procedures have been described in many other publications that can achieve similar satisfying results6,7,8,9.
3. PDMS chamber assembly
4. [OPTIONAL] Direct passivation and functionalization
NOTE: Depending on the application, chambers can be passivated and functionalized either once connected to the microfluidic controlling device (see Table of Materials) or by manually injecting solutions directly into the chamber with a pipette prior to its connection to the microfluidic device. The latter offers the advantage of consuming less reagent and avoiding potential contamination by flowing the solution through the polyether ether ketone (PEEK) tubing of the microfluidic device. In all the following steps, solutions are injected by directly sticking the pipette tip into the outlet. In order to avoid creating bubbles inside the chamber, make sure to have a tiny droplet sticking out of the pipette tip when plugging the tip into the outlet of the PDMS chamber. Likewise, remove the pipette tip before the entire volume has been injected.
5. Connect microfluidic device
NOTE: Use a pressure-based microfluidic system with up to four channels to control flows in the microfluidic chamber (Figure 1A, see Table of Materials). To avoid bubbles forming in the microfluidic tubing and perturbing flow stability, degas all solutions. Place 5 mL of dH20 and 10 mL of F-buffer stock in a vacuum desiccator connected to a vacuum pump (ultimate vacuum <250 mbar) and degas for at least 1 h at RT.
Figure 1: Injecting solutions through a microfluidic chamber. (A) Standard microfluidic setup for single actin filaments experiments. Protein solutions, placed in reservoirs 1-3, are pushed into the chamber by adjusting the pressure in the gas phase. The generated flow rates are measured by flow meters. Inside the microfluidic chambers, solutions do not mix and occupy space depending on the relative pressures applied (here, equal pressure on all inlets). Typical dimensions: reservoir tubes contain up to 2 mL of solution. PEEK tubing (0.25 mm inner diameter) connects the reservoirs to the flow meters (after 10 cm of tubing) and then to the PDMS chamber (after another 70 cm). Silicon tubing and stainless steel tubing couplers are used to connect the PEEK tubing to the PDMS inlets. The main microfluidic channel is 20-60 µm high, around 1 mm wide and 1 cm long. (B,C) Flow profiles inside the microfluidic chamber. (B) The fluid generates a parabolic profile across the chamber height: v(z) = 6z(h-z)R/h3w, where h and w are the chamber height and width, and R is the total flow rate. Bottom: Single actin filament polymerized from surface-anchored spectrin-actin seeds. (C) When the chamber width is considerably larger than its height, the flow is nearly uniform across the chamber, except at the PDMS surfaces, where it goes to zero. Please click here to view a larger version of this figure.
6. Configuring the setup with standard flow rates
NOTE: The computer-controlled pressure system allows easy and precise adjustment of the pressures of all inlets/outlet connected to the PDMS chamber, therefore the control of incoming and outcoming flow rates. Preset configurations can be saved and turned on/off with a single mouse click. Below are the recommended configurations (unless otherwise stated, outlet pressure is set to 0 mbar). See Table 3 for expected flow rates for these preset configurations. The pressures indicated here must be adjusted depending on the chamber geometry and system configuration.
Figure 2: The pressure applied to each reservoir controls the partition/spatial distribution of solutions inside the microfluidic chamber. (A) With equal pressure applied to the reservoirs, each solution occupies one-third of the chamber. (B) When changing a reservoir tube (here reservoir 3), the effective pressure drops down to zero, creating a backward flow. (C,D) Increasing the relative pressure on one of the reservoirs allows exposure of the glass surface to a single solution. The field of view in the middle of the chamber can be sequentially exposed to solutions 1 and 2 by alternating between configuration Mid Flow 1 (C) and Mid Flow 2 (D). Please click here to view a larger version of this figure.
7. Changing solution 'x'
NOTE: As shown in Figure 3A-C, it is important to keep in mind that solutions take minutes to flow from a reservoir tube to the main channel of the chamber. This minimal 'dead' time is imposed by the liquid volume contained in the tubing and the flow profile within the tubing (Figure 3A-C).
Figure 3: Delayed arrival of solutions from the reservoirs to the PDMS chamber and rapid change of biochemical conditions. (A-C) Delayed arrival of solutions from the reservoirs to the PDMS chamber. (A) Depending on the chamber geometry, the tube length, and the applied pressure at the inlet(s), the replacement of one solution by another is not instantaneous. After changing the reservoir tube to one containing a fluorescent solution (0 min), the solution progressively fills in the tubing (0.4 min) and the PDMS chamber (1-2 min). Indicative timing is given for a 150 mbar applied pressure, 80 cm PEEK tubing, and a 1600 µm wide, 20 µm high PDMS chamber. (B) The parabolic flow profile inside the PEEK tubing generates an effective gradient of fluorescence along the tubing radial profile and inside the chamber (see also Figure 1B). (C) Delayed arrival of solutions can be quantified by measuring the background epifluorescence signal in the chamber as a function of time. Experimental conditions: 0.5 µM 10% Alexa-568-labeled G-actin is injected with 150 mbar through a flow meter and 80 cm PEEK tubing. (D,E) Rapid change of biochemical conditions. (D) Pattern of incoming solutions in two Mid Flow conditions. (E) Increase in background fluorescence as a readout of actin concentration. Time t = 0 is set as the onset of fluorescence increase. Solution 1: 0.5 µM 10% Alexa-488-labeled G-actin, solution 2: F-buffer. (C,E) PDMS chamber: 20 µm high and 1600 µm wide. The epifluorescence intensity, ~2 µm above the surface, was quantified by averaging the signal over the full field of view, normalized to 0 in the absence of fluorophore and 1 at maximum intensity. Please click here to view a larger version of this figure.
8. Basic single filament experiment: Adenosine diphosphate (ADP)-actin barbed end depolymerization
NOTE: This section assumes a non-functionalized chamber (section 5 only). If the chamber has been directly functionalized (section 4), start at step 8.4.
9. Other single-filament experiments
10. Fascin-induced filament bundle formation and disassembly by ADF/cofilin
NOTE: To form actin filament bundles, make sure to have a sufficiently high filament seed density at the surface of the chamber. When exposed to fascin protein, neighboring filaments that fluctuate laterally will be dynamically cross-linked by fascin proteins. As fascin quickly unbinds from the filament side19, fascin has to be constantly present in the main flowing solution in order to maintain filament bundling.
11. Microfluidic device cleaning procedure
NOTE: To avoid any contamination from one experiment to another, it is critical to extensively clean and completely dry all the tubings and flow meters after each experiment.
12. Image analysis
NOTE: While this manuscript focuses on the method to assemble, manipulate, and visualize single actin filaments in microfluidics, a brief method to analyze acquired movies is provided here. The analysis is performed on 16-bit images, using ImageJ, following section 8.
For all the experiments described above, fluorescently labeled actin filaments should be clearly visible, with good contrast, indicative of low background fluorescence from the surface (Figure 4, see Supplementary File 1 for troubleshooting of common issues). Actin filaments should also not stick to the surface: when the dominant flow rate is low, the actin filaments' lateral fluctuations should be perceptible when observing them live and allow one to clearly determine t...
Compared to standard single-filament methods where actin filaments are anchored to the surface by multiple points along their length or maintained close to it by a crowding agent such as methylcellulose, microfluidics offers a number of advantages. As interactions with the surface are minimal, the artificial pauses these interactions can induce during both elongation and depolymerization are avoided. The filaments are aligned by the flow, parallel to each other, easing their monitoring and the measurement of their length...
The authors declare no conflicts of interest.
We are grateful to the B. Ladoux and R.-M. Mège lab for the use of their UV-cleaner equipment, and J. Heuvingh and 0. du Roure for the initial training we received on preparing molds on silicon wafers and providing tips on microfluidics. We acknowledge funding from European Research Council Grant StG-679116 (to A.J.) and Agence Nationale de la Recherche Grants Muscactin and Conformin (to G.R.-L.).
Name | Company | Catalog Number | Comments |
β-Casein | Merck | C6905 | Used at 8 mg/mL |
Biopsy punch (with plunger) | Ted Pella | 15115-2 | ID 0.75 mm, OD 1.07 mm |
Biotin-BSA | Merck | A8549 | Used at 1 mg/mL |
BSA | Merck | A8022 | Used at 50 mg/mL |
Coverslip Mini-Rack Teflon holder | Invitrogen | C14784 | for 8 coverslips |
Coverslips 22x40mm Thickness #1.5 | Menzel Gläser | 631-1370 | |
DABCO | Merck | D27802 | component in f-buffer |
DTT | Euromedex | EU0006-D | component in f-buffer |
Ester NHS Alexa Fluor 488 | Invitrogen | A20000 | Fluorophore for actin labeling on Lys328. |
EZ-Link Sulfo-NHS-Biotin | Thermo Scientific | 21338 | To biotinylate actin on Lys328 |
Hellmanex III | Hellma | 9-307-011-4-507 | Glass cleaning detergent |
ImageJ | NIH | N/A | open source software |
Laboport | KNF | 811kn.18 | vacuum pump (ultimate vacuum: 240 mbar) |
Magic invisible tape | Scotch | 7100024666 | standard transparent office tape |
Micrewtube | Simport | T341-6T | 2 mL microfluidic reservoir tubes |
Microfluidic device Part 1: Flow Unit S | Fluigent | FLU-S-D-PCKB | Flowmeter |
Microfluidic device Part 2: Fluiwell-4C-2 mL | Fluigent | 14002001PCK | Reservoir holder |
Microfluidic device Part 3: MFCS-EZ | Fluigent | EZ-11000001 EZ-00345001 | Pressure controller |
Model 42 - UVO-Cleaner | Jelight Inc. | 42-220 | Ultraviolet cleaner |
N6-(6-Aminohexyl)-ATP-ATTO-488 | Jena Bioscience | NU-805-488 | ATP-ATTO used to label actin |
neutravidin | Thermo Scientific | 31000 | |
PLL-PEG | SuSoS | PLL(20)-g[3.5]- PEG(2) | Use at 1 mg/mL in PBS. |
Polydimethylsiloxane (PDMS) Sylgard 184 Silicon Elastomer | Dow Corning | 1673921 | Contains PDMS base and curing agent |
Polyetheretherketone (PEEK) tubing | Merck | Z226661 | “Blue” : I.D. = 0.25 mm |
Safety blow gun | Coilhose Pneumatics | 700-S | filtered air |
Silicon tubing | VWR | 228-0701P | connect PEEK to coupler |
Stainless steel catheter coupler | Prime Bioscience | SC22/15 | Inserted into PDMS inlets and outlet to connect to PEEK tubing |
Thermoplastic film | Sigma Aldrich | PM996 | Standard "parafilm" |
Ultrapure ethanol | VWR | 64-17-5 | |
Ultrasonic cleaning bath | VWR | USC200TH | To accomodate 1 L beakers |
Vacuum dessicator | SP Bel-Art | F42022-0000 | to degas the PDMS or solutions |
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