Structural fluctuation observed in Z-DNA d(CGCGCG)2 in the absence of divalent metal cations and polyamines
In the present study, Z-DNA d(CGCGCG)2 was crystallized from a DNA solution in the absence of divalent metal cations and polyamines, and its X-ray structure was determined at 0.98 Å resolution. Comparison of this structure and previously reported Z-DNA structures, containing Mg2+ cations and/or polyamines, demonstrated that Z-DNA can have structural fluctuations with respect to phosphate groups and hydration in the minor groove. At the GpC steps, a two-state structural equilibrium between the ZI and ZII conformations was frequently observed. In contrast, at the CpG steps, the phosphate groups exhibited rotational fluctuation, which could induce distortion of sugar puckering. In addition, alternative positions of water molecules were found in the middle of the minor groove of the Z-DNA. These structural fluctuations were likely observable because of the absence of Mg2+ cations and polyamines. The results related to these phenomena were supported by those of other experimental methods, suggesting the possibility of these fluctuations occurring in biological conditions.
Z-DNA has a left-handed double helical structure, which is observably different from B-DNA. To date, associations have been found between Z-DNA and transcription (Schroth et al., 1992; Liu & Wang, 1987; Lipps et al., 1983), and Z-DNA binding proteins such as ADAR1 (Schwartz et al., 1999), ZALM1 (Schwartz et al., 2001) and DsrD (Mizuno et al., 2003) have been identified. Therefore, Z-DNA is now thought to play an important biological role (Rich & Zhang, 2003). The precise atomic structure of Z-DNA is applicable for understanding not only structural variety of DNA duplex but also interactions of Z-DNA with protein and DNA-binding drugs. The DNA hexamer d(CGCGCG) is the most common DNA oligomer used in the crystallographic study of Z-DNA. Since high-quality crystals of the DNA hexamer can be obtained, many comparative studies were carried out at the atomic level under different conditions.
One of the main topics for the structural study of Z-DNA is the relationship between negatively charged Z-DNA and cations. In previous crystallographic studies on Z-DNA, divalent metal cations and/or polyamines were used as counter ions to Z-DNA. The Mg2+ cation is the most commonly used divalent metal cation in crystallographic studies of Z-DNA, presumably because Mg2+ cations are the most prevalent divalent cations in cells. However, the majority of Mg2+ found in cells is complexed with cell components, and free cytosolic Mg2+ is estimated to be in the submillimolar range (Romani & Scarpa, 1992). Polyamines also bound to DNA in cells, and many complexes of Z-DNA and polyamines have been observed in crystallographic studies. A current concern is that examination of Z-DNA structure could be limited because of the presence of Mg2+ and polyamines. In the previous crystal structures of Z-DNA, Mg2+ ions were observed mainly at N7 amino groups of guanine base in the major groove and in the other parts such as the minor groove and phosphate groups (see Table 2 of Chatake & Sunami, 2013). However, the most abundant metal cations in cytosol and blood are not Mg2+ cations but K+ and Na+ cations; therefore, there was a concern about excessive structural restriction of Z-DNA due to Mg2+ cations. Polyamines also contribute to the stabilization of the Z-DNA structure. Polyamines such as spermine and spermidine are organic components which are present in cells at approximately millimolar concentrations. Recently, the 0.55 Å resolution crystal structure of the binary complex of Z-DNA d(CGCGCG)2 and spermine in the absence of divalent metal cations was reported [Protein Data Bank (PDB) ID 3p4j ; Brzezinski et al., 2011]. There was no disorder in the Z-DNA structure. Moreover, it was mentioned that a high degree of stability and excellent definition were observed in electron density maps, not only for the base pairs but also for potentially more flexible peripheral backbone elements. In the Z-DNA structure, a spermine molecule interacted with phosphate groups and bases in the major groove to contribute to the stability. Spermidine is another popular polyamine in organisms. The crystal structure of a complex of Z-DNA and spermidine demonstrated that a spermidine molecule located along the minor groove (2elg ; Ohishi et al., 2007), and that there was no disorder in the Z-DNA structure. These crystallographic studies suggested that both divalent metal cations and polyamines suppressed the structural flexibility of Z-DNA. Consequently, the three-dimensional structure of Z-DNA in the absence of divalent metal cations is essential to reveal the structural flexibility of Z-DNA. Moreover, this structure would be useful in studying the stabilization of Z-DNA structure by metal cations and polyamines. In the present study, we obtained a Z-DNA d(CGCGCG)2 crystal from solutions containing 40 mM Na+ monovalent cation in the absence of divalent metal cations and polyamines, and its structure was determined at 0.98 Å resolution.
Previous crystallographic analyses have reported two distinct conformations of phosphate groups at the GpC steps (ZI and ZII in Fig. 1; Wang et al., 1981). While the ZI conformation was the most prevalent conformation in the previously reported Z-DNA structures, all GpC steps within the Z-DNA structure exhibited ZII conformation in the presence of high concentrations of MgCl2 (1zna ; Drew & Dickerson, 1981; Drew et al., 1980; 4fs5 ; Chatake & Sunami, 2013). The coexistence of ZI and ZII at a GpC step has been occasionally observed in a few cases; for example, studies have reported that Z-DNA complexed with spermine (131d ; Bancroft et al., 1994; Egli et al., 1991) and Z-DNA in D2O solution show the coexistence of ZI and ZII only at a G8pC9 step (1woe : Chatake et al., 2005). These reports suggest that polyvalent cations have a strong effect on the selection of which conformation (ZI or ZII) is present. The Z-DNA structure that we report, which contained neither MgCl2 nor polyamine, showed behaviour different from that seen in previous studies with regard to the conformations of the phosphate groups at the GpC steps. Moreover, we also found alternative conformations at the CpG steps, which were of a different type from the two-state transition between ZI and ZII at the GpC steps. Structural fluctuation was also observed in the hydration structure.
Crude DNA hexamer d(CGCGCG) purchased from Operon Biotechnology KK was dissolved in water and desalted using the fast protein liquid chromatography system before crystallization. Salt contamination was assessed by conductivity monitoring. The content of salt in the purified solution was estimated to be lower than 0.1 mM, which is considered negligible. We used the temperature-control technique to crystallize the DNA hexamer (Chatake et al., 2010). A crystal was obtained from DNA solution containing 2.0 mM DNA hexamer, 20 mM sodium cacodylate buffer (pH 7.0), 30% 2-methyl-2,4-pentainediol and 20 mM NaCl; therefore, the crystallization aliquots contained Na+ (40 mM) as the cation. X-ray diffraction images were collected at 100 K at the BL38B1 station of SPring-8 (Okazaki et al., 2008), and they were integrated and merged up to 0.98 Å resolution by using the HKL2000 software (Otwinowski & Minor, 1997). Initial phases were determined by the molecular replacement method by using the coordinates of the Z-DNA hexamer of the P212121 crystal (1i0t ; Tereshko et al., 2001). The atomic models were rebuilt and refined using the COOT (Emsley et al., 2010) and PHENIX programs (Adams et al., 2010). The final model was determined with an R-factor (Rfree) of 0.156 (0.163). The statistical data for the X-ray experiment and structure determination are summarized in Table 1. Torsion angles and global helical parameters were calculated using the 3DNA program (Zheng et al., 2009; Lu & Olson, 2003). The figures provided in this paper were drawn using open-PyMOL.
In the structure reported here, no Na+ cation was found because of the small scattering factor of this cation, which was equivalent to the scattering factor of a water molecule. Nevertheless, the structure, with no Mg2+ ions or polyamines, had striking differences in comparison with previously reported structures of Z-DNA containing Mg2+ and/or polyamines. The global helical parameters of our structure were similar to those of the binary complex of Z-DNA and Mg2+ (1dcg ; Gessner et al., 1989) and the tertiary complex of Z-DNA, Mg2+ and spermine (2dcg ; Wang et al., 1979). Therefore, this DNA duplex maintained Z-form conformation without polyvalent cations. The phosphate backbone frequently exhibited alternative conformations at not only the GpC steps but also the CpG steps. The structural fluctuation of the GpC steps was observably different from that of the CpG steps. The two structural features of the GpC and CpG steps have been discussed separately in this study.
In the present Z-DNA structure, three (G2pC3, G4pC5, G8pC9) of the four GpC steps had ZI and ZII conformations; the exception was G10pC11. The ZI and ZII conformations can be defined by two torsion angles ζG and αC; the combinations of ζG/αC are approximately −65°/−150° for ZI and 70°/170° for ZII, respectively. As shown in Table 2, the two conformations coexisted in the Z-DNA structure. This coexistence of ZI and ZII conformations is different from that for previously reported Z-DNA structures. In almost all other crystal structures of Z-DNA d(CGCGCG), the GpC steps mainly had the ZI conformation. As for the Z-DNA hexamer, only two other crystal structures, which were obtained in the presence of high concentrations of alkaline earth cations (500 mM Mg2+ and 500 mM Ca2+), took the ZII conformation at all GpC steps, where coordination bonds of P—O—(Mg2+ or Ca2+)—O—P linked the DNA duplex to the neighbouring duplexes (Chatake & Sunami, 2013). The coexistence of ZI and ZII has been found occasionally at only one of the GpC steps (Bancroft et al., 1994; Egli et al., 1991; Chatake et al., 2005), and no Mg2+ cations were observed in such cases. These results suggest that the conformation of the GpC step is in equilibrium between the ZI and ZII forms and that certain species and concentrations of polyvalent cations strongly affect this equilibrium.
The ZI–ZII equilibrium has been proposed by other experimental methods since ZI and ZII conformations were observed in the first reported crystal structure of Z-DNA (Wang et al., 1981). Molecular dynamics simulations of Z-DNA d(5BrC-G-5BrC-G-5BrC-G)2 demonstrated structural fluctuations, including ZI and ZII of the GpC steps at 300 K under vacuum (Westhof et al., 1986). A molecular dynamics simulation of Z-DNA d(CGCGCG)2, with Na+ ions in solution, showed the transformation from ZI to ZII (Ohishi et al., 1997). Moreover, Fourier transform infrared spectroscopy demonstrated the interconversion of two conformers, which were related to the ZI and ZII conformations (Rauch et al., 2005). These results are consistent with the coexistence of ZI and ZII in the X-ray structures reported here.
We conclude that divalent cations have the following effects on determination of the ZI and ZII conformations of GpC steps: (i) at low Mg2+ concentration, phosphate groups of GpC steps are in equilibrium between ZI and ZII conformations; (ii) the equilibrium shifts to the ZI conformation in the presence of increased Mg2+; and (iii) excess Mg2+ forces the structure to convert to the ZII conformation.
Although alternative conformations of the phosphate backbone were also observed at the CpG steps, their structural fluctuation was different from the conformations at the GpC steps. As discussed in the previous subsection, structural fluctuation of the phosphate backbone at the GpC steps involved two-state equilibrium between the ZI and ZII conformations, whereas the phosphate backbone appeared to fluctuate continuously at the CpG steps. Alternative conformations were observed at four of the six CpG steps, that is, at the C1pG2, C3pG4, C5pG6 and C7pG8 steps (Fig. 2). Root-mean-square differences for O1P—P—O2P atoms between two conformations were, in ascending order, 0.60 Å for C1pG2, 0.97 Å for C7pG8, 1.27 Å for C5pG6 and 1.85 Å for C3pG4. When the CpG steps were superimposed, they appeared to vibrate rotationally, similarly to the motion of a windshield wiper. This structural fluctuation at CpG steps corresponds to another vibration mode of phosphate groups. The amplitude of the vibration seemed to be related to the puckering of the neighbouring sugars. The difference in pseudorotation between two conformers was larger than 15° at C3 (22.0°), C4 (15.7°), G6 (18.1°) and G8 (22.8°), and these residues were in the vicinity of CpG vibrations. In particular, at the C3pG4 step, the vibration of the phosphate group and CpG seemed to be connected to the fluctuation of puckering of sugar C3 (Fig. 2b). Consequently, in the absence of Mg2+, the phosphate groups exhibited rotational vibration, and the vibration would be related to distortion of sugar puckering.
Water molecules in the minor groove of Z-DNA are used as the main framework for Z-DNA folding and are tightly bound to Z-DNA (Wang et al., 1979). One of the hydration patterns specific to Z-DNA is the liner arrangement of water molecules, which Gessner et al. (1994) observed in the middle of the minor groove. These water molecules are usually located between two base pairs and interact with two O2 atoms in neighbouring cytosine bases. In an exception to this usual occurrence, Chatake et al. (2005) observed water molecules in a plane of a base pair; in this case, each water molecule interacted with an O2 atom of a cytosine. Fig. 3 shows the corresponding hydration structures in the minor groove observed in the present analysis. Unexpectedly, some water molecules in the minor groove were located in two alternative positions, which were between two base pairs and in a plane of a base pair (Fig. 3b). H2O(A) and H2O(B) were located in the conventional (between base pairs) (Fig. 3a) and unconventional (in a plane of a base pair) positions, respectively. Such alternative positions were observed at the C1G12 and G4C9 pairs. The distances between the two alternative positions were 2.25 Å and 1.75 Å for C1G12 and G4C9, respectively. H2O(A) interacted with each O2 atom of two cytosines to connect neighbouring base pairs by a hydrogen-bonding network. H2O(B) interacted with an O2 atom of one cytosine and interacted indirectly with phosphate groups via a water molecule [G10 in Fig. 3(b)]. The observed alternative positions of water molecules in the minor groove suggested that the hydration structure of the minor groove is more dynamic than the expected conventional structure discussed in previous crystallographic studies.
In the present study, we observed three types of structural fluctuations: (i) the equilibrium between ZI and ZII conformations at the GpC steps, (ii) continual fluctuation of phosphate groups at the CpG steps, and (iii) alternative positions of water molecules in the middle of the minor groove of Z-DNA. The equilibrium between the ZI and ZII conformations has been previously observed, but the frequency of this fluctuation was much higher than that of other reported structures. The continual fluctuation at the CpG steps was also frequent, and this fluctuation could be related to sugar puckering. The structural fluctuations reported here could have been suppressed by polyvalent cations, such as Mg2+ and polyamines; to our knowledge, these phenomena have been observed for the first time under the crystallization conditions used in this study, which did not include polyvalent cations. Since the concentrations of polyvalent cations in vitro are lower than those in crystallization solutions, it is reasonable to assume that the structural fluctuations observed would occur in biological conditions.
This work was supported by JSPS KAKENHI grant Nos. 18790030, 23770176. The synchrotron radiation experiments were performed at the BL38B1 beamline of SPring-8 with the approval of the Japan Synchrotron Radiation Research Institute (JASRI) [2007B1503].
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