2.7. Crystallization, diffraction data collection and processing

MM Martin Malý
PK Petr Kolenko
JS Jan Stránský
Leona Švecová
JD Jarmila Dušková
TK Tomáš Koval’
TS Tereza Skálová
MT Mária Trundová
KA Kristýna Adámková
Jiří Černý
PB Paulína Božíková
JD Jan Dohnálek
ask Ask a question
Favorite

The optimal protein buffer for crystallization was selected according to screening using the nanoscale differential scanning fluorimetry method conducted on a Prometheus NT.48 (NanoTemper). The protein sample was transferred to buffer consisting of 20 mM bis-Tris, 50 mM NaCl pH 6.5 and concentrated to 10 mg ml−1 using a 3 kDa cutoff Nanosep centrifugal device (Pall Corporation). When searching for the optimal crystallization condition, we used several commercial crystallization screens, including our acidic screen (Fejfarová et al., 2016). 96-well crystallization plates were set up by a Gryphon crystallization robot (Art Robbins) using the sitting-drop vapour-diffusion method and were stored and monitored in an RI1000 protein crystallization imager (Formulatrix) at a temperature of 20°C; the protein:reservoir ratios were 2:1, 1:1 and 1:2 in a 0.3 µl drop. The initial crystallization hits from the MORPHEUS screen (Molecular Dimensions; Gorrec, 2009) were further optimized in hanging drops using the microseeding method and Additive Screen (Hampton Research). The final condition consisted of 12%(w/v) PEG 8000, 24%(v/v) ethylene glycol, 60 mM sodium nitrate, 60 mM disodium hydrogen phosphate, 60 mM ammonium sulfate, 100 mM MES–imidazole pH 6.5, 4% acetone; the protein:reservoir ratio was 2:1 in a 1.5 µl drop.

The crystals were harvested in LithoLoops (Molecular Dimensions) and vitrified in liquid nitrogen without cryoprotection owing to the presence of ethylene glycol at a sufficient concentration in the crystallization conditions. Diffraction data were collected on beamline 14.1 of the BESSY II synchrotron-radiation source (Helmholtz Zentrum Berlin, Germany; Mueller et al., 2015) using a mini-kappa goniometer and a PILATUS 6M detector (Dectris) under the control of MXCuBE (Oscarsson et al., 2019). The data set was processed in XDSGUI (Kabsch, 2010) and initially scaled in AIMLESS from the CCP4 suite (Evans & Murshudov, 2013; Agirre et al., 2023). A limited range of diffraction images (2400 images, corresponding to 240° of the total rotational angle) were processed due to an increase in R meas per image in the final stage of data collection. The diffraction data exhibited high anisotropy: the suggested diffraction limit according to the criterion of I/σ(I) being higher than 1.5 varied from 2.69 to 1.96 Å for different directions in reciprocal space, as reported in AIMLESS. After anisotropy correction with STARANISO (Tickle et al., 2018), the phase problem was solved with a combination of MoRDa (Vagin & Lebedev, 2015; Krissinel et al., 2018) and Phaser (McCoy et al., 2007) at 2.4 Å resolution. The crystal structure of AbsH3 (Clinger et al., 2021; PDB entry 6n04) was used as a template; its FAD-binding domain and substrate-binding domain were placed individually into the unit cell. The structure model was refined with REFMAC5 (Kovalevskiy et al., 2018) using restraints for FAD from AceDRG (Long et al., 2017) and manually edited as in Švecová et al. (2021); harmonic restraints were applied to several water molecules to avoid clashes. Manual modifications and real-space refinement were carried out in Coot (Emsley et al., 2010). The high-resolution diffraction limit (1.95 Å) was determined by the paired refinement protocol with PAIREF (Karplus & Diederichs, 2012; Malý et al., 2020, 2021). Regions in the model that were difficult to interpret due to a lack of signal were resolved using a combination of polder maps (Liebschner et al., 2017), composite omit maps (Terwilliger et al., 2008) and feature-enhanced maps (Afonine et al., 2015) from the Phenix package (Liebschner et al., 2019). The final structure was refined using all reflections and was validated with Coot, MolProbity (Williams et al., 2018) and the wwPDB validation service (Berman et al., 2003). Data-collection, processing and refinement statistics are shown in Table 1. The diffraction images are available from the Structural Biology Data Grid (https://data.sbgrid.org/) at https://doi.org/10.15785/SBGRID/956. The coordinates and structure-factor amplitudes were deposited in the PDB with accession code 8aq8. The presented structure alignments and calculations of root-mean-square deviation (r.m.s.d.) were carried out in PyMOL 2.5 (Schrödinger). The crystal structure and its similarity to other protein structures were investigated with ProFunc (Laskowski et al., 2005), PISA (Krissinel & Henrick, 2007), STRIDE (Heinig & Frishman, 2004), PDBsum (Laskowski et al., 2018), PDBeFold (Krissinel & Henrick, 2004), VAST (Madej et al., 2014) and DALI (Holm, 2020).

Values in parentheses are for the highest resolution shell.

We also attempted to solve the structure of SmTetX in complex with a tetracycline antibiotic using soaking and co-crystallization, without success.

Do you have any questions about this protocol?

Post your question to gather feedback from the community. We will also invite the authors of this article to respond.

post Post a Question
0 Q&A