An innovative microfluidic design (ChipX3) is described for simple biomacromolecule crystallization by counter-diffusion, allowing semi-automated structural analysis by serial crystallography at room temperature. The functionalities of ChipX3 are demonstrated using case studies leading to high-resolution structures of four proteins and an RNA.
Keywords: macromolecule, crystallization, counter-diffusion, microfluidics, seeding, ligand soaking, trace fluorescent labeling, serial crystallography, room temperature, protein structure, ChipX3
Abstract
Determining optimal conditions for the production of well diffracting crystals is a key step in every biocrystallography project. Here, a microfluidic device is described that enables the production of crystals by counter-diffusion and their direct on-chip analysis by serial crystallography at room temperature. Nine ‘non-model’ and diverse biomacromolecules, including seven soluble proteins, a membrane protein and an RNA duplex, were crystallized and treated on-chip with a variety of standard techniques including micro-seeding, crystal soaking with ligands and crystal detection by fluorescence. Furthermore, the crystal structures of four proteins and an RNA were determined based on serial data collected on four synchrotron beamlines, demonstrating the general applicability of this multipurpose chip concept.
1. Introduction
Crystallography plays a central role in contemporary biology because it enables the visualization of the 3D architecture of biological macromolecules, which provides insights into their cellular functions and partnerships on the atomic scale (Giegé & Sauter, 2010 ▸; Jaskolski et al., 2014 ▸). Over the past two decades, the advent of structural genomics and associated high-throughput (HTP) technologies (Vincentelli et al., 2003 ▸; Pusey et al., 2005 ▸), together with dramatic improvements in experimental setups and the computational environment at synchrotron facilities (Terwilliger et al., 2009 ▸; Owen et al., 2016 ▸), have revolutionized the field and led to a torrent of new crystal structures. This productivity boost is clear from the number of structures deposited in the Protein Data Bank (PDB), which recently exceeded 150 000 entries.
In spite of such advances, the time-consuming and costly mapping of reagents and phase space to identify conditions that yield diffraction-quality crystals from a limited amount of the macromolecule remains a bottleneck in crystallographic studies (McPherson & Gavira, 2014 ▸; Luft et al., 2014 ▸; Giegé, 2017 ▸). This process generally involves a trial-and-error sampling of chemical and physical space by screening hundreds of different cocktails composed of buffers at different pH values, various crystallants (salts, alcohols and polymers) and temperature to find at least one appropriate solvent and the right supersaturation conditions. The miniaturization of crystallization assays in microplates with drop volumes of 0.1–1 µl (typically containing 1–10 µg of the macromolecule) and automation of the screening procedure have made this task considerably more efficient, making it possible to successfully conduct a project with only a few milligrams of pure sample (Sauter et al., 2012 ▸).
With the introduction of the first microfluidic systems dedicated to HTP screening 15 years ago, the sample volume required for a single experiment was reduced by another order of magnitude, down to a few nanolitres (Hansen et al., 2002 ▸; Zheng et al., 2003 ▸). Indeed, microfluidics was immediately regarded as a major breakthrough, especially for biochemists dealing with samples that are difficult to purify in large quantities, such as macromolecules from higher eukaryotes, large biological assemblies and membrane proteins (Hansen & Quake, 2003 ▸; van der Woerd et al., 2003 ▸). However, despite their potential, microfluidic technologies have not yet been massively adopted by the global community for crystal growth, as illustrated by the limited number of PDB entries (only about 30 as of March 2019) that specifically cite the use of microfluidic systems. This can be partly explained by the cost of these microsystems and their associated equipment, but also by the difficulty in successfully extracting fragile crystals from the chips or the requirement to reproduce them using conventional crystallization methods before they can be subjected to crystallographic analysis.
To expand the functionality and attractiveness of microchips beyond crystallization and HTP screening, several teams have explored the possibility of analyzing crystals directly in their microfluidic environment (Yadav et al., 2005 ▸; Ng et al., 2008 ▸; Sauter et al., 2007 ▸; Dhouib et al., 2009 ▸; Emamzadah et al., 2009 ▸; Hansen et al., 2006 ▸; Stojanoff et al., 2011 ▸). Various geometries and materials have been tested and have led to promising results in terms of data collection, anomalous phasing or time-resolved applications (Pinker et al., 2013 ▸; Khvostichenko et al., 2014 ▸; Perry et al., 2013 ▸, 2014 ▸). The difficulty of cryopreserving crystals to protect them from radiation damage inside chips, owing to the wide flat surfaces of the device causing vapor condensation and ice formation in the cryojet, was first perceived as an obstacle. However, the recent revival of multi-crystal data-collection techniques at room temperature by the X-ray free-electron laser (XFEL) community has changed the paradigm and popularized serial crystallography (Chapman et al., 2011 ▸; Stellato et al., 2014 ▸; Ayyer et al., 2015 ▸). In this context, microfluidic systems provide promising solutions to prepare, handle and analyze crystals at both synchrotron beamlines and XFELs (Heymann et al., 2014 ▸; Sui et al., 2016 ▸).
In this report, we describe a versatile and low-cost microfluidic chip for crystal production and characterization. This chip was initially designed to miniaturize and facilitate the identification of crystal-growth conditions using the counter-diffusion method and its efficient self-optimizing process (Dhouib et al., 2009 ▸; Pinker et al., 2013 ▸). The latest version of the chip design, called ChipX3, incorporates several improvements in terms of sample injection, reservoir loading and design to allow low-cost manufacturing by injection molding. With ChipX3, we demonstrate that crystals can (i) be easily produced by seeding, (ii) be soaked in situ with ligands or (iii) be visualized by fluorescence imaging. In addition, the chip provides a stable platform for crystal storage, handling, shipment and in situ analysis by serial crystallography. We illustrate a range of applications for ChipX3 by the crystallization of seven soluble proteins, a membrane protein and an RNA duplex, as well as the structure determination of five ‘non-model’ macromolecules at room temperature using data collected on four beamlines at three different synchrotron sites. This lab-on-a-chip approach simplifies and efficiently miniaturizes the crystallographic structure-determination process, from the sample to its 3D structure, in a single device. It offers a user-friendly, cost-effective solution for routine biocrystallographic investigations at room temperature.
2. Materials and methods
2.1. Biomacromolecules, biochemicals and chemicals
The recombinant proteins used in this work include protease 1 from Pyrococcus horikoshii (PhP1), the llama nanobody PorM_02 (Nb02), a lipase from Thermomyces lanuginosus (Lip; provided by Macrocrystal Oy, Finland), the CCA-adding enzyme from the psychrophilic bacterium Planococcus halocryophilus (CCA), the TonB-dependent heme/hemoglobin outer membrane transporter (OMT) ShuA from the pathogen Shigella dysenteriae (OMT ShuA), the human mitochondrial aspartyl-tRNA synthetase (hmDRS) and aspartyl-tRNA synthetase 1 from the bacterium Thermus thermophilus (ttDRS), which were purified as described previously (Engilberge et al., 2018 ▸; Duhoo et al., 2017 ▸; Ernst et al., 2018 ▸; Brillet et al., 2009 ▸; Sauter et al., 2015 ▸; Zhu et al., 2001 ▸). Horse hemoglobin was purchased from Sigma. The nine-base-pair RNA duplex [r(CGUGAUCG)dC]2 was prepared as described by Masquida et al. (1999 ▸). Stock concentrations and storage buffers are indicated in Table 1 ▸.
Table 1. Biomolecules and crystallization conditions.
Biological source | No. of residues/molecular mass (kDa) | Biomolecule concentration (mg ml−1) | Biomolecule buffer solution | Crystallant solution | |
---|---|---|---|---|---|
CCA-adding enzyme | Planococcus halocryophilus | 420/48.5 | 5.5 | 50 mM Tris–HCl pH 7.5, 200 mM NaCl, 5 mM MgCl2 | 30%(m/v) PEG 3350, 200 mM sodium formate pH 6.6 |
Nanobody 02 | Llama | 129/14.5 | 13.8 | 10 mM HEPES–NaOH pH 7.25, 150 mM NaCl | 20%(m/v) PEG 3000, 0.1 M trisodium citrate pH 5.5 |
Protease 1 | Pyrococcus horikoshii | 6 × 166/111.6 | 7.4 | 20 mM Tris–HCl pH 7.5, 10 mM Xo4 | 3.4 M malonate pH 7.5 |
Lipase | Thermomyces lanuginosus | 269/29.3 | 30 | 25 mM HEPES–NaOH pH 7.5 | 0.3 M sodium/potasssium phosphate, 50 mM sodium acetate pH 4.5 |
Aspartyl-tRNA synthetase 1 | Thermus thermophilus | 2 × 580/132 | 19 | 50 mM Tris–HCl pH 7.2, 1 mM EDTA, 1 mM DTT | 10%(m/v) PEG 8000 |
Mitochondrial aspartyl-tRNA synthetase | Homo sapiens | 2 × 630/140 | 30 | 50 mM HEPES–NaOH pH 7.5, 150 mM NaCl, 10% glycerol, 1 mM DTT | 100 mM Tris–HCl pH 7.0, 40%(m/v) PEG 3350, .2 M sodium thiocyanate |
OMT ShuA | Shigella dysenteriae | 632/69.5 | 20 | 10 mM Tris–HCl pH 8.0, 1.4% β-D-octyl-glucoside | 0.1 M sodium acetate, 20%(m/v) PEG 400, 15%(m/v) PEG 4000, 10%(m/v) PEG 8000 pH 5.0 |
RNA duplex | Synthetic | 2 × 9/5.8 | 10 | 10 mM sodium cacodylate pH 6.0, 5 mM MgCl2 | 2.6 M ammonium sulfate, 50 mM sodium cacodylate pH 6.0, 5 mM MgSO4, 1 mM spermine |
Hemoglobin | Equus caballus | 574/62 | 20 | 50 mM potassium phosphate pH 7.5 | 3.3 M ammonium sulfate, 50 mM potassium phosphate pH 7.5 |
To facilitate the detection of CCA crystals by trace fluorescent labeling (TFL; Pusey et al., 2015 ▸), the protein was fluorescently labeled with carboxyrhodamine-succinimidyl ester (Invitrogen, catalog No. C6157) as described by de Wijn et al. (2018 ▸). The labeled protein solution was stored at 277 K and mixed with the protein stock solution just before preparing crystallization assays as a fraction corresponding to less than 1% of the total protein stock. This solution will be referred to as ‘CCA-TFL’.
The nonhydrolyzable analog of cytidyl triphosphate (CTP) that was soaked into the CCA crystals, cytidine-5′-[(α,β)-methyleno]triphosphate (CMPcPP), was purchased from Jena Bioscience (catalog No. NU-438). The lanthanide complex Tb-Xo4 (commercial name Crystallophore) used to crystallize PhP1 was synthesized as described by Engilberge et al. (2017 ▸).
2.2. ChipX3 manufacturing
ChipX3 devices were designed at IBMC, Strasbourg, France in collaboration with Synchrotron SOLEIL, Saint-Aubin, France and were manufactured by MicroLIQUID, Arraste, Spain. The fluidic layer (thickness 1 mm) was produced in cyclic olefin copolymer (COC; TOPAS 5013F-04) by injection molding. Channels and reservoirs were sealed with a second layer of COC (thickness 100 µm). The bonding process was carried out at 398 K and a pressure of 500 kPa. The straight section of the microfluidic channels is 4 cm long with a cross-section of 80 × 80 µm, to give a volume of 260 nl. The reservoir at their extremity has a volume of 10 µl (Fig. 1 ▸).
2.3. Sample loading and crystallization
Crystallization experiments in the ChipX3 were set up in three steps with a conventional 10 µl micropipet (Gilson) and regular tips (StarLab). Firstly, 4–6 µl of macromolecule solution was injected into the sample inlet connecting all channels to fill the entire arborescence up to the reservoirs. Secondly, 1 µl of paraffin oil (Fluka) was injected into the sample inlet to isolate the channels from each other and the inlet was sealed with CrystalClear tape (Hampton Research) to prevent evaporation and solution movements. The third and last step consisted of filling the reservoirs with 5 µl crystallization solution before sealing them with CrystalClear tape. The solutions used to set up the chips are listed in Table 1 ▸. All experiments were incubated at 293 K, except for the RNA duplex, which was crystallized at 310 K.
2.4. Crystallization by seeding
The condition producing the best CCA crystals (de Wijn et al., 2018 ▸) was found using the microseed matrix screening (MMS) method described by D’Arcy et al. (2007 ▸, 2014 ▸). Small crystals grown by the hanging-drop method using a reservoir consisting of 1 M diammonium hydrogen phosphate, 100 mM sodium acetate pH 4.5 (condition E8 from the commercial screen JCSG++ from Jena Biosciences) were recovered, vigorously resuspended, vortexed and diluted in 50 µl of the same crystallant solution. This suspension was stored at 277 K and is referred to as the ‘seed stock’. Protein crystallization solutions were prepared by mixing 6 µl enzyme solution (5.5 mg ml−1), 1.5 µl seed stock (either the original or diluted solution) and 1 µl CCA-TFL and were immediately injected into the chip channels. Crystallization of the ttDRS enzyme in the ChipX3 was also performed using seeds. The ‘seed stock’ suspension was prepared as described for the CCA enzyme by crushing crystals grown by vapor diffusion in hanging drops with a reservoir consisting of 7%(m/v) PEG 8000, 10 mM MgCl2. ttDRS crystallization solutions were prepared as a mixture consisting of 6.5 µl enzyme solution (19 mg ml−1) and 1.5 µl seed stock, either the original or diluted solution, and were immediately injected into the chip channels.
2.5. Crystal soaking with substrate
To soak CCA crystals grown in the ChipX3, the tape covering the reservoirs was removed and 3 µl of 10 mM CMPcPP solution was added to selected reservoirs (final concentration of 3.75 mM) before sealing them again. This step was performed a week before data collection to ensure good diffusion along the microfluidic channels and in an attempt to maximize site occupancy in the crystals.
2.6. X-ray data collection and analysis
Diffraction data were collected either (i) on beamline PXII (Fuchs et al., 2014 ▸) equipped with a PILATUS 6M detector or beamline PXIII (Bingel-Erlenmeyer et al., 2011 ▸) equipped with a MAR CCD or a PILATUS 2M-F detector at the Swiss Light Source (SLS), Villigen, Switzerland, (ii) on the PROXIMA-2A (PX2A) beamline (Duran et al., 2013 ▸) equipped with an EIGER X 9M detector at SOLEIL, Saint-Aubin, France or (iii) on beamline ID30B (McCarthy et al., 2018 ▸) equipped with a PILATUS3 6M detector at the ESRF, Grenoble, France.
All serial data collections were performed at room temperature (T = 293–298 K) on crystals inside ChipX3, owing to the reduced scattering background of the chip (Pinker et al., 2013 ▸). In most cases a dedicated 3D-printed holder mounted on a standard goniometer (see Fig. 5 and Supplementary Fig. S2) was used for data collections. To collect the widest possible rotation angle for each crystal in ChipX3, the channel containing the crystal was aligned with the rotation axis of the goniometer. Crystal alignment was performed either by standard low-dose grid screening at SLS and SOLEIL, or by a one-click procedure at ESRF as described by McCarthy et al. (2018 ▸). To avoid collisions with the surrounding equipment (beamstop and collimator), we typically collected 30° rotations per crystal or crystal sector between goniometer positions −30° and +30° (where 0° corresponding to the channels being perpendicular to the X-ray beam). Two data-collection strategies were used to obtain complete data: either merging several partial data sets (sweeps) from the same crystal (one orientation and a wide rotation range) or merging several data sets from different crystals (several orientations and a smaller rotation range per crystal). Table 2 ▸ provides details of data collection and processing.
Table 2. Data-collection and refinement statistics.
CCA-adding enzyme | CCA-adding enzyme + CMPcPP | Nanobody 02 | Protease 1 | Lipase | RNA duplex | |
---|---|---|---|---|---|---|
X-ray beamline | PXIII, SLS | PXII, SLS | PX2A, SOLEIL | PXIII, SLS | ID30B, ESRF | PXIII, SLS |
Wavelength (Å) | 1.000 | 1.000 | 0.826 | 1.240 | 0.976 | 0.826 |
Temperature (K) | 293 | 293 | 293 | 293 | 293 | 293 |
Detector | PILATUS 2M-F | PILATUS 6M | EIGER | PILATUS 2M-F | PILATUS3 6M | MAR CCD |
Crystal-to-detector distance (mm) | 300 | 400 | 154 | 150/200 | 502 | 200 |
Crystals collected | 6 | 14 | 9 | 1/11 | 14 | 3 |
Crystals selected | 5 | 5 | 1 | 8 | 2 | 3 |
Rotation range per image (°) | 0.1 | 0.2 | 0.1 | 0.2 | 0.1 | 2–3 |
No. of images selected | 1000 | 540 | 500 | 1300 | 600 | 80 |
Total rotation range (°) | 100 | 108 | 50 | 260 | 60 | 155 |
Exposure time per image (s) | 0.1 | 0.1 | 0.1 | 0.1 | 0.02 | 1–2 |
Space group | P43212 | P43212 | P43212 | P41212 | P61 | R3 |
a, c (Å) | 71.5, 293.8 | 71.4, 293.6 | 66.7, 91.8 | 125.6, 133.9 | 142.6, 80.7 | 40.0, 69.1 |
Solvent content (%) | 68.3 | 67.8 | 65.0 | 74.0 | 68.6 | 54.7 |
Mean mosaicity (°) | 0.04 | 0.04 | 0.07 | 0.04 | 0.03 | 0.15 |
Resolution range (Å) | 46–2.54 (2.60–2.54) | 48–2.30 (2.40–2.30) | 50–2.10 (2.18–2.10) | 50–2.15 (2.21–2.15) | 49.06–2.50 (2.60–2.50) | 23–1.55 (1.59–1.55) |
Total No. of reflections | 176105 (9374) | 232642 (32937) | 45307 (4574) | 1095436 (85346) | 102820 (11312) | 21681 (605) |
No. of unique reflections | 23922 (1598) | 34862 (4066) | 12281 (1196) | 57690 (4522) | 31982 (3668) | 5485 (304) |
Completeness (%) | 90.6 (84.6) | 99.5 (100.0) | 97.2 (98.3) | 98.5 (99.6) | 98.5 (98.9) | 91.5 (69.7) |
Multiplicity | 7.5 (6.0) | 6.7 (8.1) | 3.7 (3.8) | 19.0 (18.9) | 3.2 (3.1) | 3.9 (2.0) |
〈I/σ(I)〉 | 8.1 (1.3) | 6.9 (0.7) | 11.3 (1.8) | 12.0 (1.4) | 6.3 (0.8) | 6.1 (1.8) |
R meas (%) | 18.9 (126.0) | 18.0 (231.2) | 7.5 (84.7) | 17.4 (206.4) | 8.6 (86.8) | 17.9 (45.6) |
CC1/2 (%) | 98.7 (55.0) | 98.7 (46.9) | 99.7 (73.5) | 99.7 (69.4) | 99.4 (49.4) | 98.8 (75.5) |
B factor from Wilson plot (Å2) | 57.4 | 60.6 | 45.2 | 50.8 | 63.3 | 23.6 |
Reflections in working/test sets | 23583/1180 | 34840/3405 | 11053/1228 | 57659/5758 | 31516/1573 | 5484/382 |
Final R work/R free (%) | 18.8/21.4 | 20.0/22.9 | 16.9/21.1 | 16.2/18.4 | 17.2/19.9 | 19.2/22.3 |
No. of non-H atoms | ||||||
Total | 2998 | 3028 | 970 | 4017 | 4446 | 390 |
Protein | 2989 | 2989 | 947 | 3921 | 4404 | 342 |
Solvent | 9 | 10 | 23 | 96 | 47 | 43 |
Ligand | 0 | 29 | 0 | 0 | 33 | 0 |
Ion | 0 | 0 | 0 | 0 | 2 | 5 |
R.m.s.d., bonds (Å) | 0.009 | 0.010 | 0.008 | 0.012 | 0.004 | 0.004 |
R.m.s.d., angles (°) | 1.23 | 1.22 | 0.897 | 1.43 | 1.08 | 0.680 |
Average B factors (Å2) | ||||||
Overall | 60.1 | 62.6 | 53.8 | 57.1 | 83.8 | 17.8 |
Biomolecule | 60.1 | 60.1 | 53.8 | 57.1 | 82.9 | 17.6 |
Solvent | 52.7 | 55.5 | 50.9 | 56.1 | 62.6 | 15.1 |
Ramachandran plot regions (%) | ||||||
Most favored | 98.1 | 97.2 | 95.8 | 98.4 | 96.6 | |
Allowed | 1.9 | 2.8 | 4.2 | 1.6 | 3.2 | |
PDB code | 6ibp | 6q52 | 6gzp | 6q3t | 6hw1 | 6ibq |
PDB code at 100 K† | 6qy6 | 6qxn | 5lmw | 6hf6 | 4zgb | 485d |
R.m.s. distance (Å2)/ΔV c (%)† | 0.79/5.0 | 0.83/3.8 | 0.79/6.6 | 0.47/4.3 | 1.0/3.9 | 0.40/2.7 |
Structures solved at room temperature (this work) are compared with equivalent structures determined at cryogenic temperatures (100 K). R.m.s. distances are calculated taking into account all biomolecule atoms and ΔV c quantifies the increase in the unit-cell volume (V c) at room temperature.
Partial data sets were individually processed with XDS (Kabsch, 2010 ▸). When their number did not exceed ten, they were manually merged with XSCALE to find the best combination and determine the appropriate resolution range. In the case of the PhP1 enzyme, ccCluster (Santoni et al., 2017 ▸) was used to determine the best partial data sets to merge among the 35 available. For all remaining steps, the PHENIX package was used (Adams et al., 2010 ▸). Phases were determined by molecular replacement using the following structures: PDB entries 1miv (Li et al., 2002 ▸) for CCA, 5lmw (Duhoo et al., 2017 ▸) for Nb02, 1g2i (Du et al., 2000 ▸) for PhP1, 4gwl (P. K. Shukla, M. Sinha, J. Mukherjee, M. N. Gupta, P. Kaur, S. Sharma & T. P. Singh, unpublished work) for Lip and 485d (Masquida et al., 1999 ▸) for the RNA. The latter crystals (space group H3) presented translational pseudo-symmetry owing to the intrinsic symmetry of the duplex and merohedral twinning (twin fraction 0.21–0.39). Hence, the structure was refined using the twin law h, −k − h, −l. All structures were built and refined with Coot and phenix.refine (Emsley & Cowtan, 2004 ▸; Adams et al., 2010 ▸).
3. Results and discussion
3.1. ChipX3 design and setup
ChipX3 was designed to perform counter-diffusion (CD) experiments and take advantage of convection-free conditions (a prerequisite of CD) in channels of small cross-section (width 80 µm, depth 80 µm) to enable the creation of crystallant concentration gradients by pure diffusion [Fig. 1 ▸(a)]. The channels, with a length of 4 cm, allow a broad screening of supersaturation states, as does conventional CD in microcapillaries (García-Ruiz et al., 2001 ▸; Otálora et al., 2009 ▸).
The geometry of the sample inlet was adapted to fit standard P2/P10 micropipet tips for chip loading using standard laboratory materials. No extra equipment (such as a pump) is required. The standard micropipet is used to inject the solution into the fluidic system. The branching channel configuration [Fig. 1 ▸(b)] allows the simultaneous loading of the eight channels in a single manipulation, thus limiting the loading time and solution dead volumes. Note that in the case of membrane-protein samples containing a detergent (such as ShuA in this work), solutions enter and fill the channels spontaneously owing to capillary action and the native wettability of the COC material. Labels embossed along the channels facilitate crystal location and grid mapping on synchrotron beamlines [Fig. 1 ▸(c)].
Once the channels have been filled with the macromolecule solution and the inlet closed with tape, crystallant solutions are deposited in the reservoirs [Fig. 1 ▸(d)]. The setup is fully compatible with viscous solutions such as the PEG mixtures used in CD screens (González-Ramírez et al., 2017 ▸). The funnel-like channel shape has been optimized to facilitate the contact between the crystallization and macromolecule solutions and to avoid trapping air bubbles, which could prevent the diffusion process. 1 µl low-gelling temperature agarose solution at 1%(w/v) can optionally be deposited in the funnel prior to the crystallization cocktail to constitute a physical buffer at the entry to the channels that stabilizes the diffusion interface.
The loading procedure of ChipX3 is fast and straightforward. Setting up a chip with eight different conditions takes less than 5 min even for untrained experimenters, as attested by numerous assays performed in the five laboratories involved in this work and by the many participants of crystallization workshops [FEBS courses in 2014–2018 in Nové Hrady, Czech Republic; International School of Biological Crystallization (ISBC) 2015–2017 in Granada, Spain].
3.2. Crystallization in ChipX3
After a prototyping phase of small batches made by hot embossing (Pinker et al., 2013 ▸), a 3D mold was machined with the new ChipX3 specifications to produce a larger batch by injection molding. This enabled validation of the concept using real cases beyond classical model proteins such as lysozyme or thaumatin. We report here on eight proteins of different sizes and sources (from bacteria to human) and an RNA oligomer (Table 1 ▸) crystallized in ChipX3. Crystallization conditions were adapted from those initially used in vapor diffusion or batch crystallization: while the biomacromolecule concentration was kept unchanged, the crystallant concentration was increased by a factor of 1.5–2, as recommended by Otálora et al. (2009 ▸). Representative examples ranging from small microcrystals to large crystals filling a portion of the channel are shown in Fig. 2 ▸. Typical counter-diffusion patterns can be observed along the concentration gradient, with microcrystalline material close to the reservoirs where supersaturation is maximal and larger crystals towards the other extremity of the channels (see Supplementary Fig. S1).
Crystals appeared after a few hours or days and could be visualized under polarized light. To facilitate the detection of small crystals, we exploited different fluorescence approaches such as classical UV excitation (Meyer et al., 2015 ▸), the fluorescent lanthanide compound Tb-Xo4 developed by Engilberge et al. (2017 ▸) and trace fluorescent labeling (TFL) as developed by Pusey et al. (2015 ▸). All three approaches were compatible with ChipX3, but the Tb-Xo4 molecule and TFL gave a much brighter signal (Fig. 3 ▸). Fluorescence has the advantage of rapidly localizing samples in the channels and may be used in the future to automate and speed up serial analysis.
3.3. Advanced crystallogenesis strategies
In addition to providing an efficient screening of supersaturation conditions, the CD process has other practical benefits, including the possibility of diffusing anomalous scatterers into pregrown crystals for phasing, or cryoprotecting with compounds such as glycerol (Gavira et al., 2002 ▸; Ng et al., 2003 ▸). In a previous study, we demonstrated the feasibility of on-chip SAD phasing at room temperature using crystals soaked by CD with a lanthanide complex (Pinker et al., 2013 ▸). Along the same lines, CMPcPP, a nonhydrolyzable analog of CTP, which is a substrate of CCA-adding enzymes, was added to the reservoirs once CCA crystals had grown and one week before the synchrotron session. The resulting X-ray structures confirmed that the crystals were derivatized by smooth diffusion without any sign of damage (Figs. 4 ▸ and 6).
Microseeding can also be used together with CD crystallization (Bergfors, 2003 ▸; Gavira et al., 2011 ▸) to bypass the nucleation step and promote rapid crystal growth. Hence, CCA and ttDRS crystals were grown by a combination of CD and seeding. Microseeds were added to the protein solution just before it was injected into the chips and the first crystals appeared in the channels after a few days. Seeding proved to be an effective way to trigger rapid and abundant crystal production, which is of particular interest for serial analysis.
We also used a new nucleant called crystallophore or Xo4 (Engilberge et al., 2018 ▸) in the case of the protein PhP1, for which the crystallization conditions (Table 1 ▸) were determined only in the presence of this terbium complex. Tb-Xo4 was added to the protein solution before filling the channels. It triggered the nucleation and the growth of large PhP1 crystals, which completely filled the available volume. An added value for macromolecules crystallized in the presence of Xo4 is the strong luminescence when illuminated by UV light (see Fig. 3 ▸).
3.4. Serial crystal analysis inside ChipX3
The ChipX3 was designed for in situ characterization. Its overall thickness was optimized to give a good compromise between material rigidity and X-ray absorption/scattering (Pinker et al., 2013 ▸). The COC material produces a characteristic diffuse scattering ring [Fig. 5 ▸(c)] in the resolution range 4–6 Å (see also Fig. 4 in Dhouib et al., 2009 ▸ and Fig. 10.4 in Martiel et al., 2018 ▸), which hardly affects data processing and quality. During data collection, the chip is oriented with its thickest layer facing the direct beam and the thinnest face behind the crystal to minimize the attenuation of the diffraction signal (Fig. 5 ▸). Labels embossed along the channels enable the easy localization of crystals before analysis, with a view to future automation of the procedure on synchrotron beamlines. The chip can also be positioned in the beam using a plate gripper, as illustrated in Supplementary Fig. S3. To avoid intervention from beamline staff to mount/unmount the gripper, we developed a light chip holder that can be directly attached to a standard goniometer. This chip holder is manufactured by 3D printing (Fig. 5 ▸, Supplementary Fig. S2) and integrates a standard metal base (B5, SPINE-style; MiTeGen) that is in contact with the goniometer magnet. The holder can be used with any flat device of microscope-slide dimensions on synchrotron beamlines and laboratory-based instruments. The 3D description file for printing this device is provided as supporting information.
To illustrate the general applicability of on-chip serial crystallography at room temperature, we present the results of structure determination in the 1.5–2.5 Å resolution range of four proteins (CCA, Lip, Nb02 and PhP1) and an RNA (Table 2 ▸, Figs. 5 ▸ and 6 ▸). Hemoglobin crystals also yielded complete data to 2.8 Å resolution (data not shown), whereas the microcrystals of the aspartyl-tRNA synthetases and OMT ShuA only diffracted to low resolution and could not be used for structure determination without further optimization.
The data collections were carried out on series of crystals and their parameters were adapted for crystal size and sensitivity to radiation damage. When collecting several paths from the same crystal signs of radiation damage could clearly be seen [see Fig. 2 ▸(d)], accompanied by the formation of gas bubbles as described by Meents et al. (2010 ▸) and by the deterioration of data-collection statistics (data not shown).
Note that performing in situ analysis, i.e. without direct handling of the crystals, is a guarantee that their genuine diffraction properties have been preserved. Comparative tests on thaumatin or lipase crystals in ChipX3 sent by regular postal mail or carried to the synchrotron by experimenters did not show significant differences (results not shown), indicating that the chip is a stable and robust container for crystal storage and transport.
Final crystal structures were obtained either from a single large crystal and two wedges (Nb02) or from combining partial data sets from several individual crystals (RNA, CCA, Lip and PhP1). In the latter case, the use of ccCluster considerably facilitated the choice of partial data sets to be merged. The comparison of these structures with equivalent structures solved at cryogenic temperatures only showed small differences (see the r.m.s. distances in Table 2 ▸), although the unit-cell volumes were significantly larger (2.7–6.6%) at room temperature than at 100 K because of crystal shrinkage occurring during cryocooling.
The high sensitivity and low background of the latest hybrid pixel detectors (HPDs) compared with CCD detectors (Pinker et al., 2013 ▸), and the very short analysis time (seconds) of the largest wedge of reciprocal space from single crystals are crucial to outrun radiation damage for room-temperature data collection. The analysis in shutterless mode also limits systematic errors in crystal orientation and thus improves the data quality. For example, the highest apparent mosaicity of the RNA crystals (see Table 2 ▸), which were analyzed at an early stage of this work with a MAR CCD detector, is a direct symptom of the data-collection strategies used before the advent of HPDs. In the future, the widespread integration of HPD technology at synchrotron sites and on laboratory-based X-ray sources will undoubtedly facilitate the development of serial crystallography.
The concept of serial crystallography was introduced with XFEL sources and their extremely intense X-ray pulses that destroy the sample upon signal emission (a process called ‘diffraction before destruction’). As a consequence, large numbers (thousands) of micro/nanocrystals are necessary to obtain a complete data set from series of individual still images. The serial approach has been extended to room-temperature data collection using synchrotron radiation. However, with a lower beam intensity (compared with XFELs) crystals can be used to collect more than a single image and up to several degrees of rotation. With very stable crystals (see Nb02 in Table 2 ▸), a single crystal may even be sufficient to collect complete data with the help of high symmetry and rapid analysis using HPDs. More generally, the number of crystals that are required for structure determination will depend on their size, their symmetry and their sensitivity to radiation damage. Most of our structures were derived from rather small series of 6–14 crystals and the combination of best data sets (Table 2 ▸). With highly sensitive samples such as membrane proteins, in situ room-temperature serial crystallography can still be carried out successfully using several hundred crystals (Huang et al., 2015 ▸). In this context, ChipX3 provides a convenient means to produce batches of crystals distributed along chip channels and, in the future, automatic crystal detection and characterization should contribute to speeding up data collection and popularizing this kind of serial RT analysis.
4. Conclusion
Microfluidics has demonstrated its value in terms of miniaturization for macromolecular crystallization experiments and HTP screening. With ChipX3, we propose a versatile tool that integrates all of the steps of a crystallographic study on a single device with the size of a microscope slide. The same chip serves to produce crystals by counter-diffusion (including seeding techniques), to soak them with ligands (for substrate catalysis, ligand screening in fragment-based drug design or phasing purposes) and to perform their diffraction analysis by in situ serial crystallography. The latter step, which is carried out on-chip at room temperature, no longer requires any crystal handling: neither fishing, nor mounting nor cryocooling. This guarantees the preservation of the intrinsic crystal quality, with the chip being a safe means of sample storage and transportation. ChipX3 is easy to use with standard laboratory equipment for sample loading and crystal observation, making it cost-effective, with minimal training or expertise required. We show the general applicability of this lab-on-chip concept with several case studies. Sample fluorescent labeling, as exemplified in this work, may be exploited to detect and center individual crystals in the X-ray beam and to perform their characterization fully automatically. Such microfluidic devices show great promise in the future in the combination of serial analysis pipelines developed at advanced X-ray sources (XFELs and synchrotrons) for routine structure determination at temperatures close to physiological conditions (Martin-Garcia et al., 2016 ▸; Johansson et al., 2017 ▸).
Supplementary Material
Supplementary Figures. DOI: 10.1107/S2052252519003622/lz5024sup1.pdf
3D description of the chip holder to be used for 3D printing. DOI: 10.1107/S2052252519003622/lz5024sup2.txt
Acknowledgments
The authors thank the following synchrotron facilities and associated scientists for beamtime allocation to the project and for assistance during data collection: beamlines X06DA (PXIII) and X10SA (PXII) at the Swiss Light Source, Villigen, Switzerland, PROXIMA 2A at the SOLEIL synchrotron, Saint-Aubin, France and A. McCarthy for support on ID30B at the European Synchrotron Radiation Facility, Grenoble, France. They also acknowledge F. Riobé, O. Maury from Laboratoire de Chimie at ENS-Lyon and Polyvalan (Lyon, France) for providing Tb-Xo4, and V. Vanel and the team of the Shadok fablab (Strasbourg, France) for assistance with 3D printers, as well as the participants and organizers of crystallization schools at Nové Hrady in the Czech Republic (FEBS courses 2014–2018) and at Granada in Spain (ISBC 2013–2015) for their active participation in operational tests of ChipX3 and their technical feedback.
Funding Statement
This work was funded by Agence Nationale de la Recherche grants ANR-11-LABX-0057_MITOCROSS, ANR-10-LABX-0036_NETRN, and ANR-13-BS07-0007-01. Ministère des Affaires Etrangères grant PROCOPE Hubert Curien to Claude Sauter and Mario Mörl. Deutsche Forschungsgemeinschaft grant Mo 634/10-1 to Mario Mörl and Heike Betat. Université de Strasbourg grant Initiative d'excellence (IDEX) to Claude Sauter and Raphaël de Wijn. Centre National de la Recherche Scientifique grant MRCT-2012_PTI_UPR9002 to Claude Sauter.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Supplementary Figures. DOI: 10.1107/S2052252519003622/lz5024sup1.pdf
3D description of the chip holder to be used for 3D printing. DOI: 10.1107/S2052252519003622/lz5024sup2.txt