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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2023 Aug 30;79(Pt 9):852–855. doi: 10.1107/S2056989023007405

Crystal structure of the nucleoside 2′-de­oxy­guanosine dimethyl sulfoxide disolvate

Bernhard Spingler a,*
Editor: A S Batsanovb
PMCID: PMC10483554  PMID: 37693671

The first high-quality crystal structure of unmodified 2′-de­oxy­guanosine is reported. The isolated crystals are the dimethyl sulfoxide disolvate.

Keywords: crystal structure, nucleoside, guanine, guanosine, purine

Abstract

The title com­pound, C10H13N5O4·2C2H6OS, which is of inter­est with respect to its biological activity, at 183 K has ortho­rhom­bic (P212121) crystal symmetry. The structure displays a network of inter­molecular N—H⋯N, N—H⋯O and O—H⋯O hydrogen bonds. 2′-De­oxy­guanosine mol­ecules are linked to each other and to the two dimethyl sulfoxide solvent mol­ecules by hydrogen bonding.

1. Chemical context

De­oxy­nucleosides are the building blocks of DNA, the storage place for the genetic information in most organisms. Understanding the properties of DNA is crucial for our knowledge of its reactivity in cellular processes of replication and transcription to yield transfer RNA (Stryer, 1995). Furthermore, mutagenic reagents can irreversibly alter the structure and function of DNA (Wang et al., 1998). In view of all this, it is of upmost importance to know the precise geometric parameters of all the nucleobases. These parameters are needed for techniques such as macromolecular X-ray crystallography in some cases and (NMR restrained) modelling of oligonucleotides (Clowney et al., 1996; Gelbin et al., 1996). Surprisingly, no high-quality crystal structure of unmodified 2′-de­oxy­guan­osine has been published to date. In the course of studying the inter­action of nucleobases with copper(II) (Santangelo et al., 2007), we obtained single crystals of 2′-de­oxy­guanosine as a solvate with two mol­ecules of dimethyl sulfoxide (DMSO), (I), and characterized it by X-ray diffraction. 1.

2. Structural commentary

Nucleobase (I) crystallized in the ortho­rhom­bic Sohnke space group P212121, with four formula units per unit cell and one per asymmetric unit (Fig. 1). The sugar conformation at the C3′ position (C13) is endo. The torsion angle χ (Alvarez et al., 2019; Schabert et al., 2021) of O14—C11—N9—C4 is −165.6 (1)° (Table 1). The freely refined H atoms of the exocyclic atom N2 were found to be in the plane of the latter and the adjacent six-membered aromatic ring, implying an sp 2 hybridization of N2. It is of inter­est to note that in the ligand database (Ligand Expo; Feng et al., 2004) of the Protein Database (Burley et al., 2023) an incorrect Lewis structure of 2′-de­oxy­guanosine (identifier GNG) is present (Fig. S1 in the supporting information).

Figure 1.

Figure 1

Displacement ellipsoid plot (50% probability) of (I).

Table 1. Sugar conformations in 2′-de­oxy­guanosine, its supra­molecular com­plexes and guanosine.

Compound Space group Sugar conformation χ (O4′—C1′—N1—C6) (°) Reference
2′-De­oxy­guanosine·2(DMSO) P212121 Envelope, C3′-endo −165.6 (1) This work
(Actinomycin D)·2(2′-de­oxy­guanosine)·12H2O P212121 Envelope, C3′-endo; Twisted, C1′-exo/C2′-endo −86.5; −90.6 Jain & Sobell (1972)
(7-Bromo­actinomycin D)·2(2′-de­oxy­guanosine)·11H2O P212121 Twisted, C2′-exo/C3′-endo; Twisted, C1′-exo/C2′-endo −86.5; −88.9 Jain & Sobell (1972)
(2′-De­oxy­guanosine)·(5-bromo-2′-de­oxy­cytidine) P21212 Envelope, C2′-endo 56.7 Haschemeyer et al. (1965)
(Guanosine)2·4H2O P21 Envelope, C2′-endo; Twisted, C1′-exo/C2′-endo −58.1; −137.2 Thewalt et al. (1970)

3. Supra­molecular features

The hydrogen bonds are listed in Table 2. The hydrogen bonding among the guanine nucleobases is a reverse Hoogsteen pairing (Johnson et al., 1992), generating an Inline graphic (9) graph set (Bernstein et al., 1995) (Fig. 2). A very similar hydrogen-bonding motif was found for guanine monohydrate (Thewalt et al., 1971) and guanosine dihydrate (Thewalt et al., 1970). Atom O21 of one DMSO mol­ecule is hydrogen bonded to the secondary alcohol group of 2′-de­oxy­guanosine, while atom O22 of the other DMSO mol­ecule is hydrogen bonded both to the exocyclic amino group of one 2′-de­oxy­guanosine mol­ecule and to the primary –OH group of another 2′-de­oxy­guanosine mol­ecule. Analysis of the fingerprint plots of the Hirshfeld surface around the 2′-de­oxy­guanosine mol­ecule calculated by CrystalExplorer (Spackman et al., 2021) (Fig. 3) indicates that H⋯H contacts account for 38.3% of the surface contacts, O⋯H/H⋯O contacts for 28.4%, N⋯H/H⋯N for 16.5% and C⋯H/H⋯C for 9.9%.

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C23—H23B⋯O6i 0.96 (3) 2.35 (3) 3.239 (3) 153 (2)
N1—H1⋯N7ii 0.87 (2) 2.09 (2) 2.962 (2) 173 (2)
N2—H2A⋯O22 0.83 (2) 2.09 (2) 2.902 (2) 168 (2)
N2—H2B⋯O6ii 0.83 (2) 2.24 (2) 3.012 (2) 155 (2)
O13—H13A⋯O21 0.87 (3) 1.88 (4) 2.738 (3) 169 (3)
O15—H15⋯O22iii 0.89 (3) 1.91 (3) 2.752 (2) 159 (3)

Symmetry codes: (i) Inline graphic ; (ii) Inline graphic ; (iii) Inline graphic .

Figure 2.

Figure 2

Hydrogen-bonding pattern of (I). Displacement ellipsoids are drawn at the 50% probability level.

Figure 3.

Figure 3

Fingerprint plots of (a) the entire Hirshfeld surface of 2′-de­oxy­guanosine within 2′-de­oxy­guanosine·2(DMSO), (b) H⋯H contacts, (c) O⋯H/H⋯O contacts, (d) N⋯H/H⋯N contacts and (e) C⋯H/H⋯C contacts.

4. Database survey

The search of the Cambridge Structural Database (CSD, Version 5.44, April 2023; Groom et al., 2016) was made with ConQuest (Version 2023.1.0; Bruno et al., 2002). The first structure containing 2′-de­oxy­guanosine (CSD refcode DGUBCY, a cocrystal with 5-bromo-2′-de­oxy­cytidine) was published by Haschemeyer et al. (1965). However, in the corresponding CSD entry, the Lewis diagram of the 2′-de­oxy­guanosine is wrong (Fig. S2), showing a 2-amino­pyrimidin-4-ol moiety, which should be redrawn as a 2-amino­pyrimidin-4(3H)-one. The cocrystal structures of (actinomycin D)·2(2′-de­oxy­guanosine)·12H2O (ACTDGU) and (7-bromo­ac­tino­mycin)·2(2′-de­oxy­guanosine)·11H2O (BRAXGU) at room temperature were also reported (Sobell et al., 1971; Jain & Sobell, 1972). In addition, the X-ray structures of four metal com­plexes containing 2′-de­oxy­guanosine are known (WEWKEO, UKISEM, WUNXIM and EWOBIN; Shionoya et al., 1994; Ito et al., 2002; Aoki & Salam, 2002; Baruah et al., 2004). Only one of them was recorded at low temperature (Baruah et al., 2004). Still, even for the latter structure, the average C—C bond distance was determined with a rather low precision of 0.009 Å. The present structure, (I), is the only purine nucleoside solvate in the CSD (Groom et al., 2016) with two DMSO mol­ecules per host mol­ecule.

5. Synthesis and crystallization

Single crystals of (I) were obtained upon slow evaporation of 2′-de­oxy­guanosine (product number D0052, TCI) from DMSO.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3. The structure was solved by direct methods with the program SIR97 (Altomare et al., 1999). All C-bonded H atoms were placed in ideal positions, with C—H bond lengths of 0.95 Å for aromatic, 1.00 Å for methine, 0.99 Å for methyl­ene and 0.98 Å for methyl C atoms, and refined as riding atoms, except those of methyl group C23H3 of one DMSO mol­ecule, which makes a relatively close contact to O6. The latter H atoms and those attached to non-C atoms were freely refined. The U iso(H) values were set at 1.2 times (for CH, NH, NH2 and CH2 units) or 1.5 times (for methyl and OH groups) the U eq value of the parent atom. The Flack parameter x was −0.00 (6) by classical fit to all intensities and 0.022 (14) by Parsons’ method (Parsons et al., 2013), from 2107 selected quotients.

Table 3. Experimental details.

Crystal data
Chemical formula C10H13N5O4·2C2H6OS
M r 423.51
Crystal system, space group Orthorhombic, P212121
Temperature (K) 183
a, b, c (Å) 9.7590 (1), 11.7951 (2), 16.7553 (2)
V3) 1928.68 (4)
Z 4
Radiation type Mo Kα
μ (mm−1) 0.32
Crystal size (mm) 0.44 × 0.24 × 0.17
 
Data collection
Diffractometer Oxford Diffraction Xcalibur Ruby
Absorption correction Multi-scan (CrysAlis RED; Oxford Diffraction, 2008)
T min, T max 0.909, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 19896, 5874, 5295
R int 0.024
(sin θ/λ)max−1) 0.714
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.030, 0.073, 1.01
No. of reflections 5874
No. of parameters 271
H-atom treatment H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.30, −0.27
Absolute structure Flack x determined using 2107 quotients [(I +) − (I )]/[(I +) + (I )] (Parsons et al., 2013)
Absolute structure parameter 0.022 (14)

Computer programs: CrysAlis CCD (Oxford Diffraction, 2008), CrysAlis RED (Oxford Diffraction, 2008), SIR97 (Altomare et al., 1999), SHELXL2018 (Sheldrick, 2015) and OLEX2 (Dolomanov et al., 2009).

7. Computational details

The sugar conformations (Table 1) were analysed with PLATON (Spek, 2020), using the published description of such conformations by Saenger (1984). For older structures, where the CSD does not contain H atoms, these were added using OLEX2 (Dolomanov et al., 2009) with default parameters.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S2056989023007405/zv2028sup1.cif

e-79-00852-sup1.cif (703.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989023007405/zv2028Isup2.hkl

e-79-00852-Isup2.hkl (467.2KB, hkl)

Figures S1 and S2. DOI: 10.1107/S2056989023007405/zv2028sup3.pdf

e-79-00852-sup3.pdf (119.8KB, pdf)

CCDC reference: 2290127

Additional supporting information: crystallographic information; 3D view; checkCIF report

supplementary crystallographic information

Crystal data

C10H13N5O4·2C2H6OS Dx = 1.459 Mg m3
Mr = 423.51 Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121 Cell parameters from 11856 reflections
a = 9.7590 (1) Å θ = 2.4–32.7°
b = 11.7951 (2) Å µ = 0.32 mm1
c = 16.7553 (2) Å T = 183 K
V = 1928.68 (4) Å3 Needle, colourless
Z = 4 0.44 × 0.24 × 0.17 mm
F(000) = 896

Data collection

Oxford Diffraction Xcalibur Ruby diffractometer 5874 independent reflections
Radiation source: Enhance (Mo) X-ray Source 5295 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.024
Detector resolution: 10.4498 pixels mm-1 θmax = 30.5°, θmin = 2.4°
ω scans h = −13→13
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008) k = −14→16
Tmin = 0.909, Tmax = 1.000 l = −22→23
19896 measured reflections

Refinement

Refinement on F2 Hydrogen site location: mixed
Least-squares matrix: full H atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.030 w = 1/[σ2(Fo2) + (0.045P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.073 (Δ/σ)max < 0.001
S = 1.01 Δρmax = 0.30 e Å3
5874 reflections Δρmin = −0.27 e Å3
271 parameters Absolute structure: Flack x determined using 2107 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
0 restraints Absolute structure parameter: 0.022 (14)
Primary atom site location: structure-invariant direct methods

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
C2 0.35188 (19) 0.60776 (14) 0.66640 (9) 0.0159 (3)
C4 0.31935 (18) 0.42499 (14) 0.64001 (9) 0.0157 (3)
C5 0.40248 (18) 0.38572 (15) 0.70072 (10) 0.0163 (3)
C6 0.47568 (18) 0.46616 (14) 0.74730 (10) 0.0183 (3)
C8 0.32641 (18) 0.23836 (15) 0.64098 (10) 0.0184 (3)
H8 0.308547 0.161923 0.626466 0.022*
C11 0.17747 (19) 0.33364 (15) 0.53323 (10) 0.0192 (3)
H11 0.101178 0.388127 0.543999 0.023*
C12 0.2513 (2) 0.36613 (16) 0.45639 (10) 0.0242 (4)
H12A 0.190773 0.410232 0.420577 0.029*
H12B 0.334890 0.410942 0.467733 0.029*
C13 0.2870 (2) 0.25191 (18) 0.42025 (10) 0.0243 (4)
H13 0.370902 0.219466 0.445824 0.029*
C14 0.16057 (19) 0.18386 (15) 0.44271 (11) 0.0212 (4)
H14 0.084806 0.204527 0.405249 0.025*
C15 0.1745 (2) 0.05766 (16) 0.44360 (13) 0.0296 (4)
H15A 0.088134 0.023128 0.462851 0.035*
H15B 0.191768 0.029894 0.388760 0.035*
C23 0.0397 (2) 0.63289 (18) 0.47584 (13) 0.0280 (4)
H23A 0.093 (3) 0.593 (2) 0.5123 (15) 0.042*
H23B 0.010 (3) 0.585 (2) 0.4328 (16) 0.042*
H23C −0.038 (3) 0.668 (2) 0.4972 (15) 0.042*
C24 0.2803 (3) 0.6683 (2) 0.40425 (16) 0.0438 (6)
H24A 0.248599 0.617530 0.361775 0.066*
H24B 0.319500 0.623323 0.447802 0.066*
H24C 0.350235 0.719659 0.382971 0.066*
N1 0.44138 (16) 0.57763 (13) 0.72580 (8) 0.0173 (3)
H1 0.483 (2) 0.6326 (19) 0.7512 (13) 0.021*
N2 0.32939 (19) 0.71824 (13) 0.65567 (9) 0.0218 (3)
H2A 0.281 (3) 0.737 (2) 0.6175 (13) 0.026*
H2B 0.367 (3) 0.771 (2) 0.6808 (13) 0.026*
N3 0.28910 (16) 0.53300 (12) 0.61976 (8) 0.0169 (3)
N7 0.40557 (16) 0.26752 (12) 0.70054 (8) 0.0187 (3)
N9 0.27173 (15) 0.33028 (12) 0.60156 (8) 0.0168 (3)
O6 0.56048 (15) 0.44860 (12) 0.80073 (7) 0.0270 (3)
O13 0.3041 (2) 0.26086 (16) 0.33678 (8) 0.0432 (4)
H13A 0.363 (4) 0.215 (3) 0.3158 (18) 0.065*
O14 0.12431 (14) 0.22319 (10) 0.52196 (7) 0.0219 (3)
O15 0.28382 (17) 0.02499 (13) 0.49400 (10) 0.0385 (4)
H15 0.275 (3) −0.048 (3) 0.5060 (16) 0.058*
O21 0.50822 (19) 0.11673 (15) 0.28913 (10) 0.0440 (4)
O22 0.19120 (17) 0.80671 (12) 0.51554 (8) 0.0318 (3)
S22 0.13986 (5) 0.74863 (4) 0.44083 (3) 0.02532 (11)
S21 0.53507 (5) 0.01236 (4) 0.24068 (3) 0.02556 (11)
C22 0.4129 (2) 0.0115 (2) 0.16179 (12) 0.0362 (5)
H22A 0.431974 0.074434 0.125214 0.054*
H22B 0.320604 0.020153 0.183990 0.054*
H22C 0.418952 −0.060392 0.132742 0.054*
C21 0.4665 (3) −0.1037 (2) 0.29503 (13) 0.0396 (5)
H21A 0.371508 −0.087110 0.309943 0.059*
H21B 0.521108 −0.116028 0.343349 0.059*
H21C 0.469085 −0.172052 0.261807 0.059*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C2 0.0194 (8) 0.0140 (8) 0.0144 (7) 0.0000 (6) 0.0000 (6) −0.0005 (6)
C4 0.0175 (8) 0.0146 (8) 0.0150 (7) −0.0013 (6) 0.0000 (6) −0.0009 (6)
C5 0.0184 (8) 0.0146 (8) 0.0158 (7) 0.0009 (6) −0.0004 (6) 0.0015 (6)
C6 0.0216 (8) 0.0172 (8) 0.0160 (7) 0.0014 (7) 0.0003 (7) 0.0009 (6)
C8 0.0208 (8) 0.0115 (8) 0.0231 (8) −0.0016 (7) 0.0007 (6) 0.0026 (6)
C11 0.0211 (9) 0.0129 (8) 0.0235 (8) 0.0001 (6) −0.0063 (7) −0.0033 (6)
C12 0.0327 (10) 0.0191 (9) 0.0207 (8) −0.0027 (8) −0.0048 (7) 0.0022 (7)
C13 0.0301 (9) 0.0238 (9) 0.0189 (7) 0.0038 (8) −0.0012 (7) 0.0018 (7)
C14 0.0247 (9) 0.0165 (9) 0.0224 (8) 0.0042 (7) −0.0097 (7) −0.0051 (7)
C15 0.0368 (11) 0.0169 (9) 0.0350 (10) 0.0027 (8) −0.0101 (9) −0.0059 (8)
C23 0.0255 (10) 0.0275 (11) 0.0310 (10) −0.0040 (9) 0.0012 (9) −0.0017 (8)
C24 0.0400 (13) 0.0350 (13) 0.0564 (14) −0.0071 (11) 0.0217 (11) −0.0083 (11)
N1 0.0228 (8) 0.0124 (7) 0.0166 (6) −0.0014 (6) −0.0055 (6) −0.0015 (5)
N2 0.0317 (9) 0.0118 (7) 0.0218 (7) −0.0004 (6) −0.0091 (7) −0.0011 (6)
N3 0.0208 (7) 0.0127 (7) 0.0171 (6) 0.0010 (6) −0.0035 (5) −0.0001 (5)
N7 0.0223 (7) 0.0125 (7) 0.0212 (7) 0.0005 (6) 0.0001 (6) 0.0032 (5)
N9 0.0191 (7) 0.0120 (7) 0.0195 (6) −0.0018 (6) −0.0031 (5) −0.0003 (5)
O6 0.0339 (8) 0.0236 (7) 0.0234 (6) 0.0003 (6) −0.0129 (6) 0.0019 (5)
O13 0.0663 (12) 0.0431 (10) 0.0201 (7) 0.0143 (9) 0.0066 (7) 0.0027 (7)
O14 0.0225 (6) 0.0156 (6) 0.0275 (6) −0.0048 (5) −0.0010 (5) −0.0059 (5)
O15 0.0365 (8) 0.0198 (8) 0.0592 (10) 0.0036 (7) −0.0145 (7) 0.0086 (7)
O21 0.0483 (11) 0.0361 (9) 0.0477 (10) 0.0013 (8) −0.0043 (8) −0.0179 (7)
O22 0.0463 (9) 0.0188 (7) 0.0302 (7) −0.0004 (7) −0.0144 (7) −0.0014 (5)
S22 0.0316 (2) 0.0205 (2) 0.0239 (2) −0.0008 (2) −0.00666 (18) 0.00218 (18)
S21 0.0255 (2) 0.0264 (3) 0.0248 (2) −0.00201 (19) −0.00031 (19) −0.00260 (17)
C22 0.0353 (11) 0.0424 (13) 0.0310 (10) −0.0071 (10) −0.0079 (9) 0.0039 (9)
C21 0.0464 (14) 0.0379 (13) 0.0345 (11) −0.0042 (11) 0.0051 (11) 0.0076 (9)

Geometric parameters (Å, º)

C2—N1 1.371 (2) C15—H15A 0.9900
C2—N2 1.334 (2) C15—H15B 0.9900
C2—N3 1.328 (2) C15—O15 1.414 (2)
C4—C5 1.381 (2) C23—H23A 0.93 (3)
C4—N3 1.351 (2) C23—H23B 0.96 (3)
C4—N9 1.371 (2) C23—H23C 0.94 (3)
C5—C6 1.421 (2) C23—S22 1.778 (2)
C5—N7 1.395 (2) C24—H24A 0.9800
C6—N1 1.404 (2) C24—H24B 0.9800
C6—O6 1.237 (2) C24—H24C 0.9800
C8—H8 0.9500 C24—S22 1.775 (2)
C8—N7 1.308 (2) N1—H1 0.87 (2)
C8—N9 1.377 (2) N2—H2A 0.83 (2)
C11—H11 1.0000 N2—H2B 0.83 (2)
C11—C12 1.525 (2) O13—H13A 0.87 (3)
C11—N9 1.469 (2) O15—H15 0.89 (3)
C11—O14 1.415 (2) O21—S21 1.4978 (17)
C12—H12A 0.9900 O22—S22 1.5124 (14)
C12—H12B 0.9900 S21—C22 1.780 (2)
C12—C13 1.518 (3) S21—C21 1.775 (2)
C13—H13 1.0000 C22—H22A 0.9800
C13—C14 1.520 (3) C22—H22B 0.9800
C13—O13 1.412 (2) C22—H22C 0.9800
C14—H14 1.0000 C21—H21A 0.9800
C14—C15 1.495 (3) C21—H21B 0.9800
C14—O14 1.450 (2) C21—H21C 0.9800
N2—C2—N1 117.13 (15) H23A—C23—H23B 111 (2)
N3—C2—N1 123.30 (15) H23A—C23—H23C 115 (2)
N3—C2—N2 119.57 (16) H23B—C23—H23C 108 (2)
N3—C4—C5 129.01 (15) S22—C23—H23A 107.2 (17)
N3—C4—N9 125.20 (15) S22—C23—H23B 111.7 (15)
N9—C4—C5 105.78 (15) S22—C23—H23C 103.7 (16)
C4—C5—C6 118.42 (16) H24A—C24—H24B 109.5
C4—C5—N7 110.26 (15) H24A—C24—H24C 109.5
N7—C5—C6 131.13 (16) H24B—C24—H24C 109.5
N1—C6—C5 111.38 (14) S22—C24—H24A 109.5
O6—C6—C5 128.47 (16) S22—C24—H24B 109.5
O6—C6—N1 120.15 (15) S22—C24—H24C 109.5
N7—C8—H8 123.6 C2—N1—C6 125.52 (14)
N7—C8—N9 112.82 (15) C2—N1—H1 117.2 (14)
N9—C8—H8 123.6 C6—N1—H1 117.3 (15)
C12—C11—H11 110.1 C2—N2—H2A 117.4 (17)
N9—C11—H11 110.1 C2—N2—H2B 125.9 (17)
N9—C11—C12 111.64 (15) H2A—N2—H2B 116 (2)
O14—C11—H11 110.1 C2—N3—C4 112.18 (14)
O14—C11—C12 106.99 (14) C8—N7—C5 104.58 (15)
O14—C11—N9 107.98 (14) C4—N9—C8 106.55 (13)
C11—C12—H12A 111.2 C4—N9—C11 123.81 (14)
C11—C12—H12B 111.2 C8—N9—C11 129.61 (14)
H12A—C12—H12B 109.1 C13—O13—H13A 116 (2)
C13—C12—C11 102.84 (15) C11—O14—C14 109.10 (14)
C13—C12—H12A 111.2 C15—O15—H15 109 (2)
C13—C12—H12B 111.2 C24—S22—C23 97.37 (11)
C12—C13—H13 110.9 O22—S22—C23 104.88 (9)
C12—C13—C14 100.59 (15) O22—S22—C24 105.77 (12)
C14—C13—H13 110.9 O21—S21—C22 106.85 (11)
O13—C13—C12 110.84 (16) O21—S21—C21 106.85 (11)
O13—C13—H13 110.9 C21—S21—C22 97.15 (12)
O13—C13—C14 112.36 (17) S21—C22—H22A 109.5
C13—C14—H14 108.4 S21—C22—H22B 109.5
C15—C14—C13 117.04 (17) S21—C22—H22C 109.5
C15—C14—H14 108.4 H22A—C22—H22B 109.5
O14—C14—C13 104.83 (14) H22A—C22—H22C 109.5
O14—C14—H14 108.4 H22B—C22—H22C 109.5
O14—C14—C15 109.36 (16) S21—C21—H21A 109.5
C14—C15—H15A 109.6 S21—C21—H21B 109.5
C14—C15—H15B 109.6 S21—C21—H21C 109.5
H15A—C15—H15B 108.1 H21A—C21—H21B 109.5
O15—C15—C14 110.24 (16) H21A—C21—H21C 109.5
O15—C15—H15A 109.6 H21B—C21—H21C 109.5
O15—C15—H15B 109.6
C4—C5—C6—N1 4.3 (2) N3—C4—C5—C6 −4.4 (3)
C4—C5—C6—O6 −175.47 (17) N3—C4—C5—N7 −179.94 (17)
C4—C5—N7—C8 0.2 (2) N3—C4—N9—C8 −179.89 (17)
C5—C4—N3—C2 0.6 (3) N3—C4—N9—C11 −1.5 (3)
C5—C4—N9—C8 0.69 (18) N7—C5—C6—N1 178.83 (18)
C5—C4—N9—C11 179.13 (15) N7—C5—C6—O6 −1.0 (3)
C5—C6—N1—C2 −1.6 (2) N7—C8—N9—C4 −0.6 (2)
C6—C5—N7—C8 −174.68 (18) N7—C8—N9—C11 −178.96 (16)
C11—C12—C13—C14 36.85 (17) N9—C4—C5—C6 175.04 (15)
C11—C12—C13—O13 155.88 (17) N9—C4—C5—N7 −0.55 (19)
C12—C11—N9—C4 77.0 (2) N9—C4—N3—C2 −178.67 (16)
C12—C11—N9—C8 −104.9 (2) N9—C8—N7—C5 0.3 (2)
C12—C11—O14—C14 0.18 (18) N9—C11—C12—C13 93.88 (17)
C12—C13—C14—C15 −159.00 (16) N9—C11—O14—C14 −120.12 (15)
C12—C13—C14—O14 −37.66 (16) O6—C6—N1—C2 178.24 (16)
C13—C14—C15—O15 55.1 (2) O13—C13—C14—C15 83.1 (2)
C13—C14—O14—C11 23.95 (18) O13—C13—C14—O14 −155.58 (16)
C15—C14—O14—C11 150.21 (15) O14—C11—C12—C13 −24.05 (18)
N1—C2—N3—C4 2.6 (2) O14—C11—N9—C4 −165.65 (15)
N2—C2—N1—C6 178.46 (17) O14—C11—N9—C8 12.4 (2)
N2—C2—N3—C4 −178.00 (16) O14—C14—C15—O15 −63.8 (2)
N3—C2—N1—C6 −2.1 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C23—H23B···O6i 0.96 (3) 2.35 (3) 3.239 (3) 153 (2)
N1—H1···N7ii 0.87 (2) 2.09 (2) 2.962 (2) 173 (2)
N2—H2A···O22 0.83 (2) 2.09 (2) 2.902 (2) 168 (2)
N2—H2B···O6ii 0.83 (2) 2.24 (2) 3.012 (2) 155 (2)
O13—H13A···O21 0.87 (3) 1.88 (4) 2.738 (3) 169 (3)
O15—H15···O22iii 0.89 (3) 1.91 (3) 2.752 (2) 159 (3)

Symmetry codes: (i) −x+1/2, −y+1, z−1/2; (ii) −x+1, y+1/2, −z+3/2; (iii) x, y−1, z.

Funding Statement

Funding for this research was provided by: University of Zurich.

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S2056989023007405/zv2028sup1.cif

e-79-00852-sup1.cif (703.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989023007405/zv2028Isup2.hkl

e-79-00852-Isup2.hkl (467.2KB, hkl)

Figures S1 and S2. DOI: 10.1107/S2056989023007405/zv2028sup3.pdf

e-79-00852-sup3.pdf (119.8KB, pdf)

CCDC reference: 2290127

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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