| Literature DB >> 28861438 |
Huijong Han1, Petri Kursula1,2.
Abstract
We present datasets that can be used for the experimental phasing of crystal structures of two myelin proteins. The structures were recently described in the articles "Periaxin and AHNAK nucleoprotein 2 form intertwined homodimers through domain swapping" (H. Han, P. Kursula, 2014) [1] and "The olfactomedin domain from gliomedin is a β-propeller with unique structural properties" (H. Han, P. Kursula, 2015) [2]. Crystals of periaxin were derivatized with tungsten and xenon prior to data collection, and diffraction data for these crystals are reported at 3 and 1 wavelengths, respectively. Crystallographic data for two different pressurizing times for xenon are provided. Gliomedin was derivatized with platinum, and data for single-wavelength anomalous dispersion are included. The data can be used to repeat the phasing experiments, to analyze heavy atom binding sites in proteins, as well as to optimize future derivatization experiments of protein crystals with these and other heavy-atom compounds.Entities:
Keywords: Anomalous signal; Crystallography; Experimental phasing; Protein; Synchrotron
Year: 2017 PMID: 28861438 PMCID: PMC5567927 DOI: 10.1016/j.dib.2017.02.049
Source DB: PubMed Journal: Data Brief ISSN: 2352-3409
Crystallographic data processing statistics.
| Protein | Periaxin | Gliomedin | |||||
|---|---|---|---|---|---|---|---|
| Dataset | Native | Xe 2 min | Xe 8 min | W peak | W inflection | W remote | Pt |
| Wavelength (Å) | 0.918 | 1.700 | 1.700 | 1.2150 | 1.2155 | 1.2114 | 1.071 |
| Space group | P3221 | P21 | |||||
| Unit cell | |||||||
| 77.28 | 77.54 | 77.24 | 77.68 | 77.87 | 77.75 | 45.51 | |
| 77.28 | 77.54 | 77.24 | 77.68 | 77.87 | 77.75 | 100.65 | |
| 80.48 | 81.49 | 81.32 | 80.14 | 80.30 | 79.99 | 59.27 | |
| α (°) | 90 | 90 | 90 | 90 | 90 | 90 | 90 |
| β (°) | 90 | 90 | 90 | 90 | 90 | 90 | 90.050 |
| γ (°) | 120 | 120 | 120 | 120 | 120 | 120 | 90 |
| Resolution range (Å) | 50-3.20 (3.28-3.20) | 50-3.10 (3.30-3.10) | 50-3.30 (3.40-3.30) | 50-3.30 (3.40-3.30) | 50-3.50 (3.60-3.50) | 50-3.71 (3.8-3.71) | 50-2.01 (2.06-2.01) |
| Completeness (%) | 99.0 (100) | 100 (100) | 99.9 (99.9) | 99.8 (99.2) | 99.8 (99.0) | 99.9 (100) | 90.4 (89.5) |
| Redundancy | 5.7 (5.8) | 14.3 (14.2) | 13.8 (13.4) | 7.2 (7.5) | 14.5 (14.7) | 14.3 (14.2) | 1.5 (1.5) |
| <I/σI> | 15.1 (2.1) | 13.3 (1.1) | 11.4 (1.3) | 12.5 (1.4) | 14.7 (1.5) | 11.2 (0.6) | 10.4 (2.6) |
| Rmeas (%) | 10.0 (105.1) | 20.6 (273.5) | 20.5 (229.2) | 10.4 (157.6) | 13.8 (209.7) | 15.7 (592.9) | 6.0 (44.9) |
| CC1/2 (%) | 99.9 (60.2) | 99.9 (41.6) | 99.9 (48.0) | 99.9 (43.4) | 100 (44.3) | 100.0 (6.4) | 99.7 (82.7) |
Processing statistics were also reported in the original publications [1], [2], and they are shown to allow direct comparison to the datasets presented here. However, all the original datasets in the table are for the first time made public in this article.
Fig. 1Comparison of anomalous signals in the datasets. The resolution on the X-axis corresponds always to the high-resolution limit of the shell in question. A. Anomalous signal in the Xe-treated crystals. Native data, thin lines; 2-min derivatization, medium lines; 8-min derivatization, thick lines. The anomalous signal (black) and anomalous correlation (red) are as given by the XDS package. B. Anomalous signal in the W-derivatized crystal. From thickest to thinnest: peak wavelength, inflection point, remote energy, native data. C. Anomalous signal in the Pt derivative of gliomedin. D. Diffraction data intensity of all datasets. See inset for color code. For the Xe data, the 2-min (thin) and 8-min (thick) data are plotted. For the W data, line thicknesses are the same as in (B). (For interpretation of the references to color in this figure legend, the reader is referred to the web version of this article.)
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