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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jun 25;64(Pt 7):o1331. doi: 10.1107/S1600536808018527

2-(1H-Imidazo[4,5-f][1,10]phenanthrolin-2-yl)phenol monohydrate

Wen-Zhi Zhang a,*, Li Li a, Ying-Hui Xiao a
PMCID: PMC2961708  PMID: 21202955

Abstract

The asymmetric unit of the title compound, C19H12N4O·H2O, contains one organic molecule and one solvent water mol­ecule, which are connected by N—H⋯O and O—H⋯N hydrogen bonds. In addition, there is one intra­molecular O—H⋯N hydrogen bond. The organic mol­ecule is essentially planar (r.m.s. deviation for all non-H atoms = 0.028 Å).

Related literature

For related literature, see: Yin (2008). For a related structure, see: Sun et al. (2007).graphic file with name e-64-o1331-scheme1.jpg

Experimental

Crystal data

  • C19H12N4O·H2O

  • M r = 330.34

  • Monoclinic, Inline graphic

  • a = 4.5272 (9) Å

  • b = 19.822 (4) Å

  • c = 16.956 (3) Å

  • β = 94.15 (3)°

  • V = 1517.6 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 293 (2) K

  • 0.21 × 0.17 × 0.15 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.975, T max = 0.989

  • 14107 measured reflections

  • 3351 independent reflections

  • 1342 reflections with I > 2σ(I)

  • R int = 0.177

Refinement

  • R[F 2 > 2σ(F 2)] = 0.094

  • wR(F 2) = 0.205

  • S = 1.02

  • 3351 reflections

  • 232 parameters

  • 3 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: PROCESS-AUTO (Rigaku, 1998); cell refinement: PROCESS-AUTO; data reduction: PROCESS-AUTO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL-Plus (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808018527/bt2727sup1.cif

e-64-o1331-sup1.cif (17.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808018527/bt2727Isup2.hkl

e-64-o1331-Isup2.hkl (161KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1A⋯N3 0.82 1.83 2.569 (5) 149
N4—H4⋯O1W 0.86 1.90 2.744 (4) 169
O1W—HW12⋯N2i 0.863 (18) 1.91 (2) 2.715 (5) 155 (4)
O1W—HW12⋯N1i 0.863 (18) 2.62 (4) 3.255 (5) 131 (3)

Symmetry code: (i) Inline graphic.

Acknowledgments

This work was supported by the Program for Young Academic Backbone in Heilongjiang Provincial University (No. 1152 G053).

supplementary crystallographic information

Comment

1,10-Phenanthroline and its derivatives are commonly used as ligands in metal-organic coordination polymers (Sun et al., 2007; Yin, 2008). The title compound was synthesized from [4,5-f]1,10-phenanthroline. All bond lengths are within normal ranges. The H2O molecules links the 2-(1H-imidazo[4,5-f][1,10]phenanthrolin-2-yl)phenol molecules by hydrogen bonds to the nitrogen atoms of the imidazo-phenantholine ring systems.

Experimental

1,10-Phenanthroline-5,6-dione (1.5 mmol) and 2-hydroxybenzaldehyde (1.5 mmol) were dissolved in CH3COOHCH3COONH4 (1:1) solution (30 ml). The mixture was refluxed for 1.5 h under argon, after cooling, this mixture was diluted with water and neutralized with concentrated aqueous ammonia, immediately resulting a yellow precipitate, which was washed with water, acetone and diethyl ether respectively. Crystals of the title compound were obtained by recrystallization from dichloromethane.

Refinement

C- and N-bound H atoms were positioned geometrically (N-H = 0.86 Å and C-H = 0.93-0.96 Å) and refined as riding, with Uiso(H) = 1.2Ueq(carrier). The water H-atoms were located in a difference Fourier map, and were refined with distance restraints of O–H = 0.85±0.01 Å and HW11···HW12 = 1.35±0.01 Å and with Uiso(H) = 1.2Ueq(O).

Figures

Fig. 1.

Fig. 1.

A perspective view of the title compound, showing the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.

Crystal data

C19H12N4O·H2O F000 = 688
Mr = 330.34 Dx = 1.446 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 6908 reflections
a = 4.5272 (9) Å θ = 3.0–27.5º
b = 19.822 (4) Å µ = 0.10 mm1
c = 16.956 (3) Å T = 293 (2) K
β = 94.15 (3)º Block, pale yellow
V = 1517.6 (5) Å3 0.21 × 0.17 × 0.15 mm
Z = 4

Data collection

Rigaku R-AXIS RAPID diffractometer 3351 independent reflections
Radiation source: rotating anode 1342 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.177
Detector resolution: 10.0 pixels mm-1 θmax = 27.5º
T = 293(2) K θmin = 3.2º
ω scans h = −5→5
Absorption correction: multi-scan(ABSCOR; Higashi, 1995) k = −25→25
Tmin = 0.975, Tmax = 0.989 l = −21→21
14107 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.094 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.205   w = 1/[σ2(Fo2) + (0.0767P)2] where P = (Fo2 + 2Fc2)/3
S = 1.03 (Δ/σ)max = 0.006
3351 reflections Δρmax = 0.20 e Å3
232 parameters Δρmin = −0.21 e Å3
3 restraints Extinction correction: none
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.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2sigma(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

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

x y z Uiso*/Ueq
C1 0.8402 (11) 0.1329 (2) 1.0945 (2) 0.0583 (13)
H1 0.9502 0.1313 1.1429 0.070*
C2 0.6283 (11) 0.0844 (3) 1.0794 (2) 0.0632 (14)
H2 0.5933 0.0519 1.1172 0.076*
C3 0.4704 (10) 0.0846 (2) 1.0080 (2) 0.0568 (12)
H3 0.3234 0.0526 0.9964 0.068*
C4 0.5324 (9) 0.1337 (2) 0.9525 (2) 0.0454 (11)
C5 0.7451 (9) 0.1833 (2) 0.9742 (2) 0.0436 (10)
C6 0.8102 (9) 0.2370 (2) 0.9201 (2) 0.0434 (10)
C7 1.0598 (11) 0.3337 (2) 0.8980 (3) 0.0622 (13)
H7 1.1926 0.3669 0.9163 0.075*
C8 0.6649 (9) 0.2387 (2) 0.8427 (2) 0.0414 (10)
C9 0.3919 (9) 0.1377 (2) 0.8750 (2) 0.0419 (10)
C10 0.4603 (9) 0.1867 (2) 0.8232 (2) 0.0413 (10)
C11 0.1276 (9) 0.1180 (2) 0.7673 (2) 0.0421 (10)
C12 −0.0845 (9) 0.0871 (2) 0.7108 (2) 0.0467 (11)
C13 −0.2259 (10) 0.0279 (2) 0.7296 (3) 0.0544 (12)
C14 −0.4299 (11) −0.0019 (3) 0.6760 (3) 0.0685 (14)
H14 −0.5268 −0.0411 0.6895 0.082*
C15 −0.4894 (11) 0.0265 (3) 0.6030 (3) 0.0740 (16)
H15 −0.6268 0.0062 0.5671 0.089*
C16 −0.1476 (10) 0.1140 (2) 0.6352 (2) 0.0610 (13)
H16 −0.0506 0.1529 0.6205 0.073*
C17 −0.3502 (11) 0.0840 (3) 0.5825 (3) 0.0717 (15)
H17 −0.3924 0.1028 0.5327 0.086*
C18 0.9353 (10) 0.3391 (2) 0.8210 (2) 0.0587 (13)
H18 0.9871 0.3745 0.7887 0.070*
C19 0.7362 (10) 0.2917 (2) 0.7935 (2) 0.0486 (11)
H19 0.6485 0.2946 0.7423 0.058*
O1 −0.1730 (7) −0.00281 (16) 0.80052 (18) 0.0763 (11)
H1A −0.0499 0.0189 0.8278 0.114*
N1 1.0015 (8) 0.28440 (19) 0.94675 (19) 0.0546 (10)
N2 0.9002 (8) 0.18203 (19) 1.04526 (18) 0.0504 (10)
N3 0.1823 (7) 0.09440 (17) 0.84045 (18) 0.0449 (9)
N4 0.2873 (7) 0.17430 (17) 0.75510 (17) 0.0458 (9)
H4 0.2814 0.1979 0.7125 0.055*
O1W 0.3484 (8) 0.24505 (18) 0.61814 (17) 0.0688 (10)
HW12 0.195 (7) 0.257 (2) 0.588 (2) 0.083*
HW11 0.444 (9) 0.219 (2) 0.590 (2) 0.083*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.074 (4) 0.061 (3) 0.039 (2) 0.011 (3) −0.006 (2) 0.001 (2)
C2 0.075 (4) 0.071 (4) 0.044 (3) 0.008 (3) 0.004 (2) 0.013 (2)
C3 0.064 (3) 0.055 (3) 0.052 (3) 0.001 (3) 0.007 (2) 0.008 (2)
C4 0.049 (3) 0.048 (3) 0.039 (2) 0.007 (2) 0.0045 (19) 0.002 (2)
C5 0.046 (3) 0.044 (3) 0.041 (2) 0.008 (2) −0.0006 (19) −0.003 (2)
C6 0.045 (3) 0.039 (3) 0.046 (2) 0.005 (2) 0.002 (2) −0.005 (2)
C7 0.069 (4) 0.053 (3) 0.063 (3) −0.012 (3) −0.009 (2) −0.009 (3)
C8 0.043 (3) 0.040 (3) 0.041 (2) 0.007 (2) 0.0010 (19) 0.0004 (19)
C9 0.040 (3) 0.039 (3) 0.047 (2) 0.001 (2) 0.0010 (19) 0.000 (2)
C10 0.039 (3) 0.042 (3) 0.041 (2) 0.004 (2) −0.0061 (19) −0.001 (2)
C11 0.043 (3) 0.035 (2) 0.047 (2) 0.009 (2) 0.0010 (19) −0.003 (2)
C12 0.044 (3) 0.042 (3) 0.053 (3) 0.004 (2) −0.004 (2) −0.002 (2)
C13 0.055 (3) 0.046 (3) 0.062 (3) 0.006 (2) 0.002 (2) −0.006 (2)
C14 0.060 (4) 0.056 (3) 0.088 (4) −0.010 (3) 0.001 (3) −0.022 (3)
C15 0.066 (4) 0.078 (4) 0.075 (4) −0.003 (3) −0.016 (3) −0.022 (3)
C16 0.058 (3) 0.057 (3) 0.066 (3) −0.001 (3) −0.009 (2) −0.003 (3)
C17 0.072 (4) 0.071 (4) 0.069 (3) −0.001 (3) −0.019 (3) −0.007 (3)
C18 0.069 (4) 0.049 (3) 0.057 (3) −0.007 (2) 0.001 (2) 0.004 (2)
C19 0.054 (3) 0.046 (3) 0.046 (2) 0.001 (2) 0.000 (2) 0.002 (2)
O1 0.077 (2) 0.066 (2) 0.083 (2) −0.0178 (19) −0.0115 (18) 0.0141 (19)
N1 0.063 (3) 0.047 (2) 0.053 (2) −0.011 (2) −0.0019 (18) −0.0013 (19)
N2 0.059 (2) 0.052 (2) 0.0394 (19) 0.0082 (19) 0.0000 (17) 0.0002 (18)
N3 0.043 (2) 0.046 (2) 0.0449 (19) 0.0014 (18) 0.0012 (16) 0.0004 (17)
N4 0.046 (2) 0.044 (2) 0.0463 (19) 0.0008 (18) −0.0033 (16) 0.0060 (17)
O1W 0.077 (3) 0.071 (3) 0.0559 (19) 0.000 (2) −0.0092 (16) 0.0158 (17)

Geometric parameters (Å, °)

C1—N2 1.323 (5) C11—N3 1.332 (5)
C1—C2 1.370 (6) C11—N4 1.353 (5)
C1—H1 0.9300 C11—C12 1.443 (5)
C2—C3 1.360 (5) C12—C13 1.384 (6)
C2—H2 0.9300 C12—C16 1.400 (5)
C3—C4 1.397 (5) C13—O1 1.353 (5)
C3—H3 0.9300 C13—C14 1.380 (6)
C4—C5 1.407 (6) C14—C15 1.368 (6)
C4—C9 1.420 (5) C14—H14 0.9300
C5—N2 1.351 (4) C15—C17 1.360 (7)
C5—C6 1.449 (5) C15—H15 0.9300
C6—N1 1.334 (5) C16—C17 1.370 (6)
C6—C8 1.424 (5) C16—H16 0.9300
C7—N1 1.318 (5) C17—H17 0.9300
C7—C18 1.389 (5) C18—C19 1.361 (6)
C7—H7 0.9300 C18—H18 0.9300
C8—C19 1.393 (5) C19—H19 0.9300
C8—C10 1.410 (5) O1—H1A 0.8200
C9—C10 1.360 (5) N4—H4 0.8600
C9—N3 1.378 (5) O1W—HW12 0.863 (18)
C10—N4 1.370 (4) O1W—HW11 0.841 (18)
N2—C1—C2 124.9 (4) C13—C12—C16 117.8 (4)
N2—C1—H1 117.5 C13—C12—C11 120.3 (4)
C2—C1—H1 117.5 C16—C12—C11 121.8 (4)
C3—C2—C1 118.7 (4) O1—C13—C14 117.4 (4)
C3—C2—H2 120.7 O1—C13—C12 122.0 (4)
C1—C2—H2 120.7 C14—C13—C12 120.6 (4)
C2—C3—C4 118.9 (4) C15—C14—C13 119.9 (5)
C2—C3—H3 120.5 C15—C14—H14 120.1
C4—C3—H3 120.5 C13—C14—H14 120.1
C3—C4—C5 118.6 (4) C17—C15—C14 120.8 (5)
C3—C4—C9 124.4 (4) C17—C15—H15 119.6
C5—C4—C9 117.1 (4) C14—C15—H15 119.6
N2—C5—C4 121.4 (4) C17—C16—C12 121.0 (5)
N2—C5—C6 117.6 (4) C17—C16—H16 119.5
C4—C5—C6 121.0 (3) C12—C16—H16 119.5
N1—C6—C8 122.8 (4) C15—C17—C16 119.8 (5)
N1—C6—C5 117.3 (3) C15—C17—H17 120.1
C8—C6—C5 119.9 (4) C16—C17—H17 120.1
N1—C7—C18 124.1 (4) C19—C18—C7 118.8 (4)
N1—C7—H7 117.9 C19—C18—H18 120.6
C18—C7—H7 117.9 C7—C18—H18 120.6
C19—C8—C10 126.0 (3) C18—C19—C8 119.5 (4)
C19—C8—C6 117.2 (4) C18—C19—H19 120.3
C10—C8—C6 116.8 (4) C8—C19—H19 120.3
C10—C9—N3 110.6 (3) C13—O1—H1A 109.5
C10—C9—C4 122.0 (4) C7—N1—C6 117.6 (4)
N3—C9—C4 127.4 (4) C1—N2—C5 117.4 (4)
C9—C10—N4 105.8 (3) C11—N3—C9 104.6 (3)
C9—C10—C8 123.2 (3) C11—N4—C10 107.3 (3)
N4—C10—C8 130.9 (4) C11—N4—H4 126.3
N3—C11—N4 111.5 (3) C10—N4—H4 126.3
N3—C11—C12 122.5 (4) HW12—O1W—HW11 105 (3)
N4—C11—C12 125.9 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H1A···N3 0.82 1.83 2.569 (5) 149
N4—H4···O1W 0.86 1.90 2.744 (4) 169
O1W—HW12···N2i 0.863 (18) 1.91 (2) 2.715 (5) 155 (4)
O1W—HW12···N1i 0.863 (18) 2.62 (4) 3.255 (5) 131 (3)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2727).

References

  1. Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
  2. Rigaku (1998). PROCESS-AUTO Rigaku Corporation, Tokyo, Japan.
  3. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  4. Sun, M., Chen, G., Ling, B.-P. & Liu, Y.-X. (2007). Acta Cryst. E63, o1210–o1211.
  5. Yin, G.-Q. (2008). Acta Cryst. E64, o1236. [DOI] [PMC free article] [PubMed]

Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808018527/bt2727sup1.cif

e-64-o1331-sup1.cif (17.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808018527/bt2727Isup2.hkl

e-64-o1331-Isup2.hkl (161KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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