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In the crystal structure of the title complex, C6H6O2·C6H6N2O3, the mol­ecules are linked by intermolecular hydrogen bonds between the O—H and N—O groups. The O atom of the N-oxide group of 3-methyl-4-nitro­pyridine 1-oxide acts as an acceptor for hydrogen bonds from O—H groups of two symmetry-related hydro­quinone mol­ecules [O...O 2.732 (2) and 2.810 (2) Å]. The angles between the rings of the 3-methyl-4-nitro­pyridine 1-oxide and two hydro­quinone mol­ecules are 6.1 (3) and 0.6 (3)°. The crystal structure exhibits overlap between the aromatic rings of the mol­ecules in the [11\overline 1] direction.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680200819X/cf6173sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680200819X/cf6173Isup2.hkl
Contains datablock I

CCDC reference: 189375

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.043
  • wR factor = 0.127
  • Data-to-parameter ratio = 11.6

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Computing details top

Data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation, 1995); program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997) and ZORTEP (Zsolnai, 1995); software used to prepare material for publication: SHELXL97.

(I) top
Crystal data top
C6H6O2·C6H6N2O3Z = 2
Mr = 264.24F(000) = 276
Triclinic, P1Dx = 1.473 Mg m3
Hall symbol: -P 1Melting point: 384(1) K
a = 7.8593 (16) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.429 (3) ÅCell parameters from 25 reflections
c = 9.039 (3) Åθ = 8–20°
α = 84.39 (3)°µ = 0.12 mm1
β = 89.92 (2)°T = 293 K
γ = 88.91 (3)°Irregular_block, orange–red
V = 595.8 (3) Å30.20 × 0.14 × 0.14 mm
Data collection top
Rigaku AFC-7S
diffractometer
Rint = 0.015
Radiation source: fine-focus sealed tubeθmax = 25.0°, θmin = 2.3°
Graphite monochromatorh = 99
ω/2θ scansk = 100
2250 measured reflectionsl = 1010
2091 independent reflections3 standard reflections every 150 min
1848 reflections with I > 2σ(I) intensity decay: none
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.127 w = 1/[σ2(Fo2) + (0.077P)2 + 0.1509P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
2091 reflectionsΔρmax = 0.29 e Å3
181 parametersΔρmin = 0.22 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.034 (7)
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.3953 (2)0.55619 (19)0.68901 (18)0.0419 (4)
H10.46610.47110.66960.050*
C20.4149 (2)0.6282 (2)0.81648 (18)0.0421 (4)
H20.49730.59070.88560.051*
C30.3119 (2)0.75697 (19)0.84251 (17)0.0381 (4)
C40.1868 (2)0.81540 (18)0.74227 (18)0.0374 (4)
C50.1717 (2)0.73451 (19)0.61632 (18)0.0395 (4)
H50.08860.76830.54650.047*
C60.0674 (2)0.9538 (2)0.7568 (2)0.0536 (5)
H610.01630.95870.67920.064*
H620.13031.05090.74870.064*
H630.01190.94060.85170.064*
N10.27269 (17)0.60914 (15)0.59155 (14)0.0374 (3)
N20.3422 (2)0.82778 (19)0.98195 (17)0.0524 (4)
O10.25402 (17)0.53780 (15)0.46953 (13)0.0515 (4)
O20.2858 (3)0.9599 (2)0.99536 (19)0.0919 (6)
O30.4255 (3)0.7501 (2)1.07750 (17)0.0854 (6)
C70.1063 (2)0.6283 (2)0.02089 (19)0.0456 (4)
H70.17820.71460.03440.055*
C80.0043 (2)0.5704 (2)0.13225 (18)0.0428 (4)
C90.1105 (2)0.5577 (2)0.11172 (18)0.0447 (4)
H90.18510.59700.18680.054*
C100.4654 (2)0.11298 (18)0.59675 (17)0.0398 (4)
H100.44260.18910.66230.048*
C110.3716 (2)0.11380 (18)0.46727 (18)0.0386 (4)
C120.4074 (2)0.00009 (19)0.37064 (17)0.0409 (4)
H120.34530.00040.28320.049*
O40.0002 (2)0.64284 (19)0.26215 (16)0.0637 (4)
HO40.080 (4)0.605 (3)0.312 (3)0.087 (9)*
O50.24142 (17)0.22086 (16)0.43064 (16)0.0564 (4)
HO50.250 (3)0.306 (3)0.469 (3)0.063 (6)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0490 (9)0.0359 (8)0.0404 (9)0.0105 (7)0.0005 (7)0.0042 (7)
C20.0474 (9)0.0399 (9)0.0382 (8)0.0047 (7)0.0072 (7)0.0009 (7)
C30.0452 (9)0.0369 (8)0.0333 (8)0.0041 (7)0.0009 (6)0.0085 (6)
C40.0413 (8)0.0330 (8)0.0387 (8)0.0004 (6)0.0010 (6)0.0079 (6)
C50.0434 (9)0.0374 (8)0.0378 (8)0.0055 (7)0.0055 (7)0.0059 (7)
C60.0532 (11)0.0480 (10)0.0619 (11)0.0125 (8)0.0072 (9)0.0196 (8)
N10.0481 (8)0.0348 (7)0.0301 (7)0.0026 (6)0.0007 (5)0.0075 (5)
N20.0635 (10)0.0530 (9)0.0430 (8)0.0006 (7)0.0097 (7)0.0174 (7)
O10.0726 (9)0.0487 (7)0.0355 (6)0.0105 (6)0.0046 (6)0.0185 (5)
O20.1312 (16)0.0763 (11)0.0748 (11)0.0353 (10)0.0339 (10)0.0477 (9)
O30.1185 (14)0.0848 (11)0.0555 (9)0.0190 (10)0.0414 (9)0.0232 (8)
C70.0523 (10)0.0404 (9)0.0436 (9)0.0070 (7)0.0031 (7)0.0026 (7)
C80.0520 (10)0.0417 (9)0.0350 (8)0.0026 (7)0.0025 (7)0.0043 (7)
C90.0491 (9)0.0465 (10)0.0371 (9)0.0039 (7)0.0095 (7)0.0017 (7)
C100.0513 (9)0.0345 (8)0.0347 (8)0.0008 (7)0.0068 (7)0.0089 (6)
C110.0451 (9)0.0318 (8)0.0389 (8)0.0002 (6)0.0091 (7)0.0030 (6)
C120.0512 (9)0.0384 (9)0.0336 (8)0.0001 (7)0.0126 (7)0.0054 (6)
O40.0850 (11)0.0638 (9)0.0447 (8)0.0164 (8)0.0149 (7)0.0203 (6)
O50.0631 (8)0.0441 (7)0.0636 (8)0.0154 (6)0.0277 (6)0.0170 (6)
Geometric parameters (Å, º) top
C1—N11.346 (2)C7—C81.377 (3)
C1—C21.364 (2)C7—C91.390 (2)
C1—H10.930C7—H70.930
C2—C31.380 (2)C8—O41.375 (2)
C2—H20.930C8—C9i1.379 (3)
C3—C41.388 (2)C9—C8i1.379 (3)
C3—N21.468 (2)C9—H90.930
C4—C51.389 (2)C10—C12ii1.379 (2)
C4—C61.499 (2)C10—C111.384 (2)
C5—N11.346 (2)C10—H100.930
C5—H50.930C11—O51.370 (2)
C6—H610.960C11—C121.385 (2)
C6—H620.960C12—C10ii1.379 (2)
C6—H630.960C12—H120.930
N1—O11.3165 (17)O4—HO40.82 (3)
N2—O21.208 (2)O5—HO50.83 (2)
N2—O31.216 (2)
N1—C1—C2119.55 (14)O2—N2—O3123.45 (16)
N1—C1—H1120.2O2—N2—C3118.86 (16)
C2—C1—H1120.2O3—N2—C3117.68 (16)
C1—C2—C3119.77 (15)C8—C7—C9120.02 (17)
C1—C2—H2120.1C8—C7—H7120.0
C3—C2—H2120.1C9—C7—H7120.0
C2—C3—C4121.64 (15)O4—C8—C7117.43 (17)
C2—C3—N2116.19 (15)O4—C8—C9i122.79 (16)
C4—C3—N2122.18 (15)C7—C8—C9i119.76 (17)
C3—C4—C5115.54 (15)C8i—C9—C7120.22 (16)
C3—C4—C6126.99 (15)C8i—C9—H9119.9
C5—C4—C6117.47 (15)C7—C9—H9119.9
N1—C5—C4122.49 (15)C12ii—C10—C11120.49 (15)
N1—C5—H5118.8C12ii—C10—H10119.8
C4—C5—H5118.8C11—C10—H10119.8
C4—C6—H61109.5O5—C11—C10123.05 (15)
C4—C6—H62109.5O5—C11—C12117.85 (14)
H61—C6—H62109.5C10—C11—C12119.09 (15)
C4—C6—H63109.5C10ii—C12—C11120.42 (14)
H61—C6—H63109.5C10ii—C12—H12119.8
H62—C6—H63109.5C11—C12—H12119.8
O1—N1—C5120.00 (14)C8—O4—HO4106 (2)
O1—N1—C1119.01 (13)C11—O5—HO5113.9 (16)
C5—N1—C1120.98 (14)
N1—C1—C2—C31.6 (3)C2—C1—N1—C51.6 (2)
C1—C2—C3—C40.5 (3)C2—C3—N2—O2163.02 (19)
C1—C2—C3—N2179.68 (15)C4—C3—N2—O217.1 (3)
C2—C3—C4—C50.8 (2)C2—C3—N2—O316.0 (3)
N2—C3—C4—C5179.09 (14)C4—C3—N2—O3163.90 (18)
C2—C3—C4—C6179.82 (16)C9—C7—C8—O4178.64 (16)
N2—C3—C4—C60.3 (3)C9—C7—C8—C9i0.1 (3)
C3—C4—C5—N10.9 (2)C8—C7—C9—C8i0.1 (3)
C6—C4—C5—N1179.66 (15)C12ii—C10—C11—O5178.54 (15)
C4—C5—N1—O1179.30 (14)C12ii—C10—C11—C120.2 (3)
C4—C5—N1—C10.3 (2)O5—C11—C12—C10ii178.61 (15)
C2—C1—N1—O1179.41 (14)C10—C11—C12—C10ii0.2 (3)
Symmetry codes: (i) x, y+1, z; (ii) x+1, y, z+1.
 

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