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1 Turku Centre for Biotechnology, University of Turku and Åbo Akademi University, Turku, 20521, Finland
2 European Molecular Biology Laboratory (EMBL), Grenoble Outstation, Grenoble, Cedex 9, 38042, France
3 EMBL, Hamburg Outstation, c/o Deutsches Elektronen-Synchrotron (DESY), Hamburg, 22603, Germany
Reprint requests to: Anastassios C. Papageorgiou, Turku Centre for Biotechnology, BioCity, Tykistökatu 6, Turku 20521, Finland; e-mail: apapageo{at}btk.fi; fax: +358-2-333-8000.
(RECEIVED February 7, 2005; FINAL REVISION March 10, 2005; ACCEPTED March 10, 2005)
| Abstract |
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. Our data provide new insights into the enzymatic activation of pyridoxal-5'-phosphate and suggest that special care should be taken while using macromolecular crystallography to study details in strained active sites. Keywords: pyridoxal-5'-phosphate; Schiff base; phosphoserine aminotransferase; radiation damage
Abbreviations: AAT, aspartate aminotransferase BALC, Bacillus alcalophilus CD, circular dichroism PLP, pyridoxal-5'-phosphate PSAT, phosphoserine aminotransferase.
Article published online ahead of print. Article and publication date are at http://www.proteinscience.org/cgi/doi/10.1110/ps.051397905.
| Introduction |
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Phosphoserine aminotransferase (PSAT; EC 2.6.1.52
[EC]
) is a vitamin B6-dependent enzyme that catalyzes the reversible conversion of 3-phosphohydroxypyruvate to L-phosphoserine. The Schiff-base linkage between the cofactor, pyridoxal-5'-phosphate (PLP), and a protein Lys residue (the internal aldimine) (Fig. 1A
) is a conservative feature among all members of this protein family (Jansonius 1998; Schneider et al. 2000). In all PLP-dependent enzymes except glycogen phosphorylase, the internal aldimine is replaced by an external aldimine between PLP and the substrate amino group at the beginning of the catalytic cycle. The ionization state of the PLP-Lys Schiff base can be changed depending on the protonation of the imine nitrogen atom (Hayashi 1995). In the protonated Schiff base, the imine bond and the pyridine ring reside in the same plane (Fig. 1B
), while deprotonation is accompanied by disruption of planarity (Fig. 1C
) due to rotation around the C3-C4-C4'-NZ torsion angle (Mizuguchi et al. 2001). For a number of aminotransferases, including aspartate aminotransferase (Hayashi et al. 1998), aromatic amino acid aminotransferase (Islam et al. 2000), and histidinol phosphate aminotransferase, (Mizuguchi et al. 2003) presence of a chemical strain on the internal aldimine bond has been reported. This strain was proposed to distort the absolutely coplanar conformation of the protonated Schiff base (Fig. 1B
) by increasing the C3-C4-C4'-NZ torsion angle and, hence, to lower the imine pKa value by as much as 34 units (Hayashi et al. 2003; Mizuguchi et al. 2003).
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Here, using crystallographic data up to 1.3 Å resolution and single-crystal on-line spectroscopy, we analyze the X-ray-induced structural changes at the active site of B. alcalophilus PSAT. Remarkably, the Schiff base undergoes radiation damage within a relatively short total exposure time, both at second- and third-generation synchrotron beamlines. Analysis of the "early" crystal structure reveals a short NZ-C4' distance and close to zero C3-C4-C4'-NZ torsion angle of the internal aldimine. This conformation harbors a significant chemical strain on the Schiff base that leads to geometrical distortion of the cofactor. In the "late" structures after X-ray exposure, the active site strain is relaxed and the NZ-C4' distance and C3-C4-C4'-NZ torsion angle are increased.
| Results and Discussion |
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max=406408nm) (Fig. 2A
Structural changes induced by X-rays
Figure 3
shows the difference Fourier maps derived from the data sets AG. No significant structural changes were observed between the initial data set A and the data sets B and C, respectively (Fig. 3A, B
). However, further exposure leads to the loss of definition of the internal aldimine bond and several water molecules situated nearby (Fig. 3CF
). At the same time, the correlated appearance of positive and negative electron density peaks indicates a movement of the C2', C4', and O3' atoms of the cofactor. These results suggest that the conformation of the internal aldimine and the relative position of PLP molecule in the active site of BALC PSAT change in response to the X-ray exposure.
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With increased total absorbed dose, the refined bond distance of the internal aldimine (a double covalent bond) increases from 1.371.40 Å to 1.511.66 Å distance (Table 3
) that is more suitable for a single covalent bond. These results can be interpreted either as an X-ray-induced reduction of the internal aldimine, or as a disruption of the chemical bond in part of the molecules. In light of the available data, however, it is not possible to distinguish between the two possibilities. The first explanation seems to be more probable, as no electron density for the unbound conformation of the Lys196 was observed in any map. Nonetheless, in our previous crystallographic studies of the BALC PSAT at atomic resolution (Dubnovitsky et al. 2005), the bond distance NZ-C4' was even longer (1.73 ± 0.05 Å ), while it was restrained to 1.7 Å, since the electron density for the Schiff base in the final map was insufficient for unequivocal unrestrained refinement. If the restraint has been removed, the refined bond distance of 1.97 ± 0.05 Å was observed (data not shown). Such a large value suggests that in the structure obtained after ~20 h exposure at the EMBL/DESY beamline BW7A, the PLP in some protein molecules is not anymore covalently bound to the Lys196. In other words, the final model would represent the averaged coordinates for the disrupted and the chemically intact aldimine bond. These results therefore support the second explanation, e.g., X-rays induce disruption of the PLP-Lys Schiff base in the BALC PSAT crystals. In this case, however, it is still possible that reduction and disruption of the internal aldimine occur either simultaneously or consequently.
Interestingly, the two active sites of the BALC PSAT dimer show a certain degree of asymmetry. Indeed, such a difference between the theoretically identical and independent active sites has been previously reported for several PLP-containing enzymes (Eliot and Kirsch 2004, and references therein). The initial geometry of the Schiff base and the quantitative changes during the X-ray exposure do not match very well in subunits A and B (Table 3
). Analysis of the electron density maps in the active site of the monomer A suggests that Lys196 is partially disordered already in the initial structure (data not shown). For this reason, mainly subunit B was used in comparison. Although the two active sites seem to be differentially susceptible to the radiation damage, all structural changes described above coincide qualitatively in both subunits.
Due to the relatively low resolution of the data sets AG (1.681.77 Å ) (Table 1
), the mean coordinate error is relatively high (up to 0.12 Å ). The data-to-parameter ratio at such a resolution is pretty low for anisotropic refinement of atomic temperature factors. Thus, some degree of uncertainty could be introduced into the final models (DePristo et al. 2004). In order to describe the subtle structural changes in the BALC PSAT crystals under X-ray exposure more reliably, we collected two high-resolution data sets at the EMBL/DESY beamline BW7A (Table 2
). The mean coordinate errors assessed by a Luzzati plot or using Cruickshanks empirical formula for data sets H and I do not exceed 0.08 Å and 0.04 Å, respectively. Moreover, the number of observations at the resolution 1.3 Å is high enough to introduce a full anisotropic refinement of the model. Analysis of the difference Fourier maps (Fig. 5A
) and the final BALC PSAT structures refined against data sets H and I have shown X-ray induced structural changes similar to our previous findings at ~1.7 Å resolution. Strong positive and negative peaks in difference Fourier maps confirm the movement of the whole PLP molecule and suggest concomitant changes in the position of the Lys196, including both the side and the main chain (Fig. 5A
). The relative position of the PLP molecule in the active site, the torsion angle, and the bond length of the internal aldimine are changed even after a relatively short total exposure time (~90 min; unfortunately, no estimate of the flux and the dose could be given) at the second-generation synchrotron beamline (Table 3
). Further, comparison of the anisotropic displacement parameters of the active site residues shows an increased degree of disorder in the BALC PSAT structure after an X-ray exposure (Fig. 5B, C
). The mean equivalent isotropic temperature factor for all atoms in the residue Lys196 (subunit B) is increased from 13.6 Å2 in the model H to 20.1 Å2 in the model I. The corresponding values for the imine nitrogen (NZ) and the C4' atom of PLP are rising from 13.5 to 26.5 Å2 and from 13.6 to 20.4 Å2, respectively, while the other atoms of the cofactor are less affected. The average temperature factors for all protein atoms in models H and I are 16.4 Å and 15.9 Å2, respectively. Thus, the increase of the atomic temperature factors serves as additional evidence of the enhanced susceptibility of the BALC PSAT active site to radiation damage.
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-electron system of the pyridine ring and the internal aldimine. Such a distortion was confirmed by the CD spectroscopy of BALC PSAT at a different pH (Fig. 7
-
* transition (Kochendoerfer et al. 1996) and has been suggested to arise partially from the torsion angle of the Schiff base (Hayashi et al. 1998).
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-electron system of PLP and the internal aldimine in BALC PSAT are implemented in the catalytic mechanism. It was shown that the free PLP alone can catalyze slowly many of the possible reactions catalyzed by the PLP-dependent enzymes (Christen and Metzler 1985). This innate catalytic potential of the cofactor is enhanced upon binding to the protein apoenzyme (Eliot and Kirsch 2004). Since breakage of the PLP-Lys Schiff base is an early event of the catalytic cycle, the conformational strain on the internal aldimine may increase significantly the reactivity of this bond and, hence, may play a key role in the enzymatic activation of PLP in phosphoserine aminotransferase.
Conclusions
We have described the radiation damage of the Lys-PLP Schiff base in B. alcalophilus PSAT crystals during crystallographic data collection at 100 K. The active site geometry changes quickly in response to the X-ray exposure. Several previously reported crystal structures of other PLP-containing enzymes at 1.51.96 Å resolution (Krupka et al. 2000; Ura et al. 2001; Noland et al. 2002; Weyand et al. 2002) have revealed unexpected conformation of the internal aldimine that should be reinspected based on our results. Our data suggest that crystallographic mechanistic studies of enzymes with strained active sites, in general, and PLP-dependent enzymes, in particular, should be done with great care. Moreover, if our present findings are confirmed on any other PLP-containing enzyme, it should become a common practice in further crystallographic studies of the PLP enzymes to optimize the data-collection strategy in order to minimize the total absorbed dose as much as possible without a significant loss in resolution. The online monitoring of UV/VIS spectral changes in protein crystals could be of general use for finding the maximum allowed dose to avoid X-ray-induced structural changes in the active sites of chromatophore-containing enzymes.
| Materials and methods |
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Crystallographic data collection
A series of seven complete data sets (AG) were collected from a single crystal at 100 K on the undulator beamline ID14-4 at the ESRF using a Q4R ADSC CCD detector, with the synchrotron running in 16-bunch mode. A beam size of 50 x 250 µm2 was used at a wavelength of 0.939 Å. Each "composite" data set consists of 100 frames of 0.75°. Every 20 frames were collected from a fresh crystal location after a 60-µm translation (the crystal dimensions were 1.0 x 0.2 x 0.1 mm3). A similar technique was previously used for data collection from a single and from multiple crystals (Berglund et al. 2002; Adam et al. 2004). In order to minimize the total absorbed dose per data set, each frame was collected with a 2-sec exposure to a 19.2 x attenuated beam. As a result of the short exposure time, the resolution was limited to 1.681.77 Å, although the BALC PSAT crystals diffract to atomic resolution (Dubnovitsky et al. 2005). After the first data collection, the rotating crystal was "burnt" with an unattenuated beam for 5 sec, 10 sec, 1 min, 1 min, 2 min, and 3 min. After every "burning", the same 15° were collected. Finally, seven complete composite data sets with an increasing total absorbed dose were obtained (Table 1
). The total exposure time spent for each individual data-set collection was 40 sec with a 19.2 x attenuated beam that allowed us to minimize structural changes during data-collection course.
Data sets H and I (Table 2
)were collected to 1.3Å resolution from a single crystal at 100 K on the EMBL/DESY beamline BW7A equipped with a MarCCD 165-mm detector. A beam size of 100 x 200 µm2 was used at a wavelength of 0.921 Å. A composite data set H consists of seven subsets, including 20 frames each. The oscillation range was 0.5° per frame. Each subset was collected after ~150 µm translation of the crystal, which was 1.2 x 0.2 x 0.1 mm3 in size. Data were collected in the dose mode with the mean exposure time of ~8 sec per frame. Thus, the total exposure time for the data set H was ~160 sec. Data set I was collected from a single crystal location after it had been exposed to the X-rays for 60 min in total. Using an oscillation range of 0.3°, 187 frames were collected with the mean exposure time of ~10 sec. Thus, the total exposure time for data set I including a preliminary "burning" and data collection is ~90 min.
Data were processed with the HKL suite (Otwinowski and Minor 1997). The intensities were converted to amplitudes using the TRUNCATE program (Collaborative Computational Project Number 4 1994).
Structure refinement
Structures of the BALC PSAT were refined using the restrained conjugate least-squares method as implemented in SHELX-97 (Sheldrick and Schneider 1997). XtalView (McRee 1999) was used for manual modelling. The atomic resolution structure of the BALC PSAT (PDB accession code 1W23) was used as an initial model. Default effective standard deviations were used for all stereo-chemical restraints. No restraints were given for the torsion angle or the bond length of the internal aldimine, but pyridoxal-5'-phosphate was refined with stereo-chemical restraints applied. The PLP planarity restraint was released in the refinement against the 1.3 Å resolution data (data sets H and I). Models H and I were subjected to full anisotropic refinement and addition of hydrogen atoms at riding positions after the refinement converged. The final models were inspected with the PROCHECK program (Collaborative Computational Project Number 4 1994). In the Ramachandran plots, 91%92% of all nonglycine and nonproline residues were found in the most favored regions, and no residue was observed in the disallowed regions for all models. The refinement statistics for models AG and H and I are summarized in Tables 1
and 2
, respectively.
Absorbed dose calculation
The total absorbed doses for the data sets AG were calculated with the program RadDose (Murray et al. 2004) on the basis of measured crystal size (1.0 x 0.2 x 0.1 mm3), photon flux (about 3.7 x 1011 photons/sec in 50 x 250 µm2) and energy (13.2 keV), and calculated crystal absorption and density. Other input parameters used by RadDose were the number of amino-acids per molecule (360), number of molecules per unit cell (eight), number of Cys and Met residues in the protein (12), and non-C/H/N/O components of the mother liquor (200 mM MgCl2).
Spectroscopic analysis in solution
Absorption spectra of BALC PSAT in solution were recorded at room temperature in a 1-cm cuvette using Pharmacia Biotech Ultrospec 2000 spectrophotometer. The final protein concentration was 0.8 mg/mL. The CD spectra of BALC PSAT were recorded using a Jasco J-715 CD spectropolarimeter in a 0.2-cm cuvette at a protein concentration of 1.9 mg/mL. The averaged spectra of four scans were corrected for the buffer blank. Samples for absorption and CD spectroscopy were prepared by dilution of the concentrated protein solution (1020 mg/mL) in the appropriate buffers and were equilibrated before measurements for 1 h at room temperature.
Protein Data Bank accession codes
Atomic coordinates and structure factors have been deposited with the Protein Data Bank under identification codes 2BHX
[PDB]
, 2BI1, 2BI2, 2BI3, 2BI5, 2BI9, 2BIA, 2BIE, and 2BIG for the structures AI, respectively.
| Footnotes |
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| Acknowledgments |
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