9OER | pdb_00009oer

HalA with lysine, Fe(II), chloride, and a peroxyhemiketal intermediate


X-RAY DIFFRACTION

Starting Model(s)

Initial Refinement Model(s)
TypeSourceAccession CodeDetails
experimental modelPDB 7JSD 

Crystallization

Crystalization Experiments
IDMethodpHTemperatureDetails
1VAPOR DIFFUSION, HANGING DROP7298HalA crystals were obtained by the hanging drop vapor diffusion method by combining equal volumes of protein solution (HalA (5 mg/ml), lysine (50 mM, pH 7), and aKG (20 mM, pH 7)) and reservoir solution (potassium phosphate monobasic (40 mM), 20% (w/v) PEG 8000, 15% (v/v) glycerol). Crystals grew in three days and were transferred to an Eppendorf tube containing 250 uL of reservoir solution and vortexed for 30 seconds with 10 x 1 uM diameter zirconia/silica beads to produce a micro-seed solution. The seed solution was stored at -80C for future use. Subsequent crystals were prepared by micro-seeding equal volumes of protein solution (HalA (5 mg/ml), lysine (50 mM, pH 7), and aKG (20 mM, pH 7)) and reservoir solution (potassium phosphate monobasic (40 mM), 20% (w/v) PEG 8000, 15% (v/v) glycerol). Crystals grew after two weeks inside a Coy anaerobic chamber. Crystals were soaked with (NH4)2Fe(SO4)2 6H2O (1.42 mM) while NO accumulated in the well. To introduce NO, diethylamine NONOate was prepared by dissolving solid in 10 mM NaOH. The stock concentration was determined based on the published extinction coefficient of e250 = 6,500 M-1 cm-1 using a Nanodrop. NONOate was added to a final concentration of 26 mM in each well along with 150 mM HEPES pH 7.5 to trigger NONOate decomposition. The wells were quickly re-sealed and NO was allowed to accumulate for approximately 1 hour, after which the crystals were flash frozen in liquid nitrogen
Crystal Properties
Matthews coefficientSolvent content
2.5251.19

Crystal Data

Unit Cell
Length ( Å )Angle ( ˚ )
a = 147.3α = 90
b = 147.3β = 90
c = 287.87γ = 120
Symmetry
Space GroupH 3

Diffraction

Diffraction Experiment
ID #Crystal IDScattering TypeData Collection TemperatureDetectorDetector TypeDetailsCollection DateMonochromatorProtocol
11x-ray90PIXELDECTRIS PILATUS3 S 6M2022-12-22MSINGLE WAVELENGTH
Radiation Source
ID #SourceTypeWavelength ListSynchrotron SiteBeamline
1SYNCHROTRONALS BEAMLINE 8.3.11.11583ALS8.3.1

Data Collection

Overall
ID #Resolution (High)Resolution (Low)Percent Possible (Observed)R Merge I (Observed)Rrim I (All)Rpim I (All)CC (Half)Net I Over Average Sigma (I)RedundancyNumber Reflections (All)Number Reflections (Observed)Observed Criterion Sigma (F)Observed Criterion Sigma (I)B (Isotropic) From Wilson Plot
11.7295.9699.70.1810.1860.0410.99619.538.94246753
Highest Resolution Shell
ID #Resolution (High)Resolution (Low)Percent Possible (All)Percent Possible (Observed)R Merge I (Observed)Rrim I (All)Rpim I (All)CC (Half)Mean I Over Sigma (Observed)RedundancyNumber Unique Reflections (All)
11.721.78199.132.3762.4220.46430.6571.8426.67

Refinement

Statistics
Diffraction IDStructure Solution MethodCross Validation methodResolution (High)Resolution (Low)Cut-off Sigma (F)Number Reflections (Observed)Number Reflections (R-Free)Percent Reflections (Observed)R-Factor (Observed)R-Work (Depositor)R-Work (DCC)R-Free (Depositor)R-Free (DCC)Mean Isotropic B
X-RAY DIFFRACTIONMOLECULAR REPLACEMENTFREE R-VALUE1.7295.961.962467491254099.710.17840.16840.1710.20120.2034
Temperature Factor Modeling
Anisotropic B[1][1]Anisotropic B[1][2]Anisotropic B[1][3]Anisotropic B[2][2]Anisotropic B[2][3]Anisotropic B[3][3]
RMS Deviations
KeyRefinement Restraint Deviation
f_dihedral_angle_d12.391
f_angle_d0.678
f_chiral_restr0.042
f_bond_d0.011
f_plane_restr0.009
Non-Hydrogen Atoms Used in Refinement
Non-Hydrogen AtomsNumber
Protein Atoms15552
Nucleic Acid Atoms
Solvent Atoms697
Heterogen Atoms171

Software

Software
Software NamePurpose
PHENIXrefinement
XDSdata reduction
Aimlessdata scaling
PHASERphasing
PDB_EXTRACTdata extraction