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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Nov 4;65(Pt 12):o2996. doi: 10.1107/S1600536809045620

4,4′-[Piperazine-1,4-diylbis(propyl­ene­nitrilo­methyl­idyne)]diphenol

Ruibo Xu a, Xingyou Xu b,*, Xujie Yang c, Yuping Huang a, Chunmei Xu a
PMCID: PMC2972058  PMID: 21578736

Abstract

In the title mol­ecule, C24H32N4O2, the piperazine ring adopts a chair conformation and the dihedral angle between the two benzene rings is 35.4 (1)°. In the crystal structure, inter­molecular O—H⋯N hydrogen bonds link mol­ecules into chains along [001].

Related literature

For the properties of piperazine derivatives, see: Keypour et al. (2008, 2009); Paital et al. (2009). For related structures, see: Thirumurugan et al. (1998); Yogavel et al. (2003).graphic file with name e-65-o2996-scheme1.jpg

Experimental

Crystal data

  • C24H32N4O2

  • M r = 408.54

  • Monoclinic, Inline graphic

  • a = 5.9701 (10) Å

  • b = 30.159 (3) Å

  • c = 12.8348 (18) Å

  • β = 97.558 (2)°

  • V = 2290.9 (6) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 298 K

  • 0.17 × 0.15 × 0.11 mm

Data collection

  • Siemens SMART CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.987, T max = 0.992

  • 5997 measured reflections

  • 2016 independent reflections

  • 1387 reflections with I > 2σ(I)

  • R int = 0.068

Refinement

  • R[F 2 > 2σ(F 2)] = 0.043

  • wR(F 2) = 0.103

  • S = 0.96

  • 2016 reflections

  • 271 parameters

  • 2 restraints

  • H-atom parameters constrained

  • Δρmax = 0.14 e Å−3

  • Δρmin = −0.19 e Å−3

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809045620/lh2937sup1.cif

e-65-o2996-sup1.cif (22.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809045620/lh2937Isup2.hkl

e-65-o2996-Isup2.hkl (99.2KB, 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
O2—H2⋯N1i 0.82 1.98 2.762 (4) 159
O1—H1⋯N2ii 0.82 2.00 2.780 (4) 159

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

Acknowledgments

This project was supported by the Key Project for Fundamental Research of the Jiangsu Provincial Educational Committee (07KJA150011), the Opened Funds of Jiangsu Key Laboratory of Marine Biotechnology of Huaihai Institute of Technology (2009HS06) and the QingLan Project of Jiangsu Province (2008).

supplementary crystallographic information

Comment

Piperazine derivatives possesses interesting structures and properties (Yogavel et al., 2003; Thirumurugan et al., 1998; Keypour et al., 2008,2009; Paital et al., 2009), therefore, our group have designed and prepared series of Schiff bases and complexes derived from substituted piperazines. As part of our work, the title compound (I) a potential hexadentate Schiff base ligand, was synthesized in our group and herein we report the crystal structure.

The molecular structure of (I) is shown in Fig. 1. In (I), the C8—N3 and C18—N4 double bond lengths are comparable to reported values (Yogavel et al., 2003; Thirumurugan et al., 1998). The dihedral angle between the two benzene rings (C9—C14 and C19—C24) is 35.4 (1) °. In the piperazine ring, atoms C1/C2/C3/C4 are essentially planar (the mean deviation from the plane is 0.0032 Å), and atoms N1 and N2 atom lie 0.6936 and 0.6693 Å either side of this plane. This four atom plane makes a dihedral angle of 50.9 (3)° with the plane of atoms C2/N2/C3 and 52.7 (3) ° with atoms C1/N1/C4, respectively, in accordance with the chair conformation of the piperazine ring. In the crystal structure, intermolecular O—H···N hydrogen bonds link molecules into one-dimensional chains along [001](Fig.2).

Experimental

A solution of N,N'-bis(N-aminopropyl)-piperazine (1.5 mmol in 10 ml anhydrous methanol) was added dropwise with constant stirring to a solution of parahydroxybenzaldehyde (3 mmol in 15 ml anhydrous methanol) at 325 K for 3 h. The resulting mixture was filtered. After cooling, the filtrate was evaporated at ambient environment. Several days later, pink crystals suitable for X-ray analysis were collected and washed with small amount of methanol and dried at room temperature.

Refinement

H atoms were placed in calculated positions with C—H = 0.97 Å(piperazinyl), 0.93 Å(benzene), 0.82 Å(hydroxyl) and 0.97 Å(methylene), and refined in riding mode with Uiso(H)= 1.5 Ueq(O) and Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (1). Displacement ellipsoids are drawn at the 30% probability level.

Fig. 2.

Fig. 2.

One-dimensional chain structure of (1) constructed by O—H···N intermolecular hydrogen bonds (dashed lines) along [001].

Crystal data

C24H32N4O2 F(000) = 880
Mr = 408.54 Dx = 1.185 Mg m3
Monoclinic, Cc Mo Kα radiation, λ = 0.71073 Å
Hall symbol: C -2yc Cell parameters from 1760 reflections
a = 5.9701 (10) Å θ = 2.7–24.9°
b = 30.159 (3) Å µ = 0.08 mm1
c = 12.8348 (18) Å T = 298 K
β = 97.558 (2)° Lamellate, pink
V = 2290.9 (6) Å3 0.17 × 0.15 × 0.11 mm
Z = 4

Data collection

Siemens SMART CCD diffractometer 2016 independent reflections
Radiation source: fine-focus sealed tube 1387 reflections with I > 2σ(I)
graphite Rint = 0.068
φ and ω scans θmax = 25.0°, θmin = 1.4°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −7→6
Tmin = 0.987, Tmax = 0.992 k = −30→35
5997 measured reflections l = −15→15

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103 H-atom parameters constrained
S = 0.96 w = 1/[σ2(Fo2) + (0.0507P)2] where P = (Fo2 + 2Fc2)/3
2016 reflections (Δ/σ)max < 0.001
271 parameters Δρmax = 0.14 e Å3
2 restraints Δρmin = −0.19 e Å3

Special details

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.
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 > σ(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
N1 0.6528 (5) 0.39796 (9) 0.5395 (2) 0.0440 (7)
N2 0.6327 (5) 0.34403 (9) 0.7270 (2) 0.0450 (7)
N3 0.6917 (7) 0.47133 (10) 0.2563 (2) 0.0619 (9)
N4 0.5753 (7) 0.26995 (10) 1.0120 (2) 0.0604 (9)
O1 1.0094 (5) 0.38009 (9) −0.1521 (2) 0.0684 (8)
H1 0.8981 0.3653 −0.1744 0.103*
O2 0.2701 (4) 0.37289 (8) 1.40788 (19) 0.0592 (7)
H2 0.3880 0.3735 1.4486 0.089*
C1 0.5611 (7) 0.41527 (12) 0.6330 (3) 0.0509 (10)
H1A 0.4439 0.4369 0.6113 0.061*
H1B 0.6804 0.4300 0.6789 0.061*
C2 0.4643 (7) 0.37801 (12) 0.6919 (3) 0.0524 (10)
H2A 0.4043 0.3901 0.7526 0.063*
H2B 0.3403 0.3644 0.6467 0.063*
C3 0.7284 (7) 0.32708 (12) 0.6338 (3) 0.0510 (10)
H3A 0.6111 0.3122 0.5871 0.061*
H3B 0.8464 0.3057 0.6560 0.061*
C4 0.8247 (6) 0.36472 (12) 0.5762 (3) 0.0504 (10)
H4A 0.9453 0.3788 0.6226 0.060*
H4B 0.8890 0.3530 0.5163 0.060*
C5 0.7518 (7) 0.43362 (13) 0.4807 (3) 0.0552 (10)
H5A 0.8202 0.4203 0.4237 0.066*
H5B 0.8712 0.4479 0.5273 0.066*
C6 0.5862 (8) 0.46839 (13) 0.4356 (3) 0.0628 (11)
H6A 0.5490 0.4873 0.4920 0.075*
H6B 0.4481 0.4540 0.4044 0.075*
C7 0.6779 (9) 0.49699 (13) 0.3524 (3) 0.0680 (12)
H7A 0.5796 0.5224 0.3361 0.082*
H7B 0.8268 0.5079 0.3798 0.082*
C8 0.8797 (8) 0.46994 (12) 0.2204 (3) 0.0555 (11)
H8 1.0022 0.4850 0.2563 0.067*
C9 0.9117 (7) 0.44553 (11) 0.1246 (3) 0.0479 (9)
C10 1.1116 (7) 0.44905 (13) 0.0817 (3) 0.0608 (10)
H10 1.2280 0.4664 0.1153 0.073*
C11 1.1427 (7) 0.42709 (14) −0.0112 (3) 0.0584 (10)
H11 1.2774 0.4304 −0.0395 0.070*
C12 0.9734 (6) 0.40044 (12) −0.0611 (3) 0.0471 (9)
C13 0.7736 (6) 0.39566 (12) −0.0171 (3) 0.0501 (10)
H13 0.6592 0.3775 −0.0497 0.060*
C14 0.7435 (6) 0.41775 (12) 0.0751 (3) 0.0472 (9)
H14 0.6100 0.4140 0.1041 0.057*
C15 0.5266 (7) 0.30844 (12) 0.7830 (3) 0.0566 (10)
H15A 0.4159 0.2933 0.7332 0.068*
H15B 0.4465 0.3219 0.8360 0.068*
C16 0.6907 (8) 0.27448 (12) 0.8355 (3) 0.0591 (11)
H16A 0.8220 0.2896 0.8713 0.071*
H16B 0.7411 0.2555 0.7821 0.071*
C17 0.5864 (9) 0.24597 (14) 0.9141 (3) 0.0703 (13)
H17A 0.4353 0.2372 0.8841 0.084*
H17B 0.6759 0.2193 0.9286 0.084*
C18 0.3869 (7) 0.28242 (12) 1.0347 (3) 0.0530 (10)
H18 0.2584 0.2760 0.9879 0.064*
C19 0.3598 (7) 0.30661 (11) 1.1315 (3) 0.0446 (9)
C20 0.5407 (7) 0.31283 (13) 1.2093 (3) 0.0563 (11)
H20 0.6820 0.3019 1.1994 0.068*
C21 0.5156 (7) 0.33506 (13) 1.3016 (3) 0.0566 (10)
H21 0.6392 0.3387 1.3530 0.068*
C22 0.3063 (6) 0.35184 (11) 1.3173 (3) 0.0462 (9)
C23 0.1256 (7) 0.34603 (12) 1.2404 (3) 0.0517 (9)
H23 −0.0150 0.3574 1.2501 0.062*
C24 0.1506 (7) 0.32352 (12) 1.1488 (3) 0.0545 (10)
H24 0.0260 0.3196 1.0980 0.065*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0460 (18) 0.0507 (17) 0.0371 (16) 0.0038 (15) 0.0126 (15) −0.0067 (14)
N2 0.0486 (18) 0.0493 (17) 0.0378 (16) 0.0054 (15) 0.0086 (14) −0.0041 (14)
N3 0.086 (3) 0.053 (2) 0.047 (2) −0.0058 (19) 0.0136 (19) −0.0030 (17)
N4 0.084 (3) 0.0542 (19) 0.045 (2) 0.0001 (19) 0.0140 (19) −0.0078 (16)
O1 0.0580 (18) 0.092 (2) 0.0577 (17) −0.0007 (15) 0.0161 (15) −0.0221 (16)
O2 0.0517 (17) 0.0707 (18) 0.0567 (17) 0.0012 (14) 0.0131 (14) −0.0143 (14)
C1 0.060 (2) 0.054 (2) 0.041 (2) 0.0106 (19) 0.0137 (19) −0.0060 (18)
C2 0.049 (2) 0.067 (2) 0.043 (2) 0.012 (2) 0.0145 (19) −0.0047 (19)
C3 0.057 (2) 0.054 (2) 0.043 (2) 0.0123 (19) 0.0086 (19) −0.0054 (18)
C4 0.045 (2) 0.065 (3) 0.042 (2) 0.0102 (18) 0.0110 (18) −0.0056 (19)
C5 0.063 (3) 0.058 (2) 0.046 (2) −0.007 (2) 0.014 (2) −0.0035 (19)
C6 0.083 (3) 0.052 (2) 0.056 (3) 0.003 (2) 0.019 (2) −0.002 (2)
C7 0.105 (4) 0.049 (2) 0.052 (2) −0.004 (2) 0.019 (2) −0.008 (2)
C8 0.070 (3) 0.049 (2) 0.047 (2) −0.005 (2) 0.004 (2) −0.0016 (18)
C9 0.055 (2) 0.043 (2) 0.044 (2) 0.0047 (18) 0.0010 (19) 0.0022 (17)
C10 0.054 (3) 0.069 (3) 0.057 (2) −0.009 (2) −0.001 (2) −0.007 (2)
C11 0.046 (2) 0.073 (3) 0.056 (2) 0.001 (2) 0.008 (2) −0.003 (2)
C12 0.047 (2) 0.051 (2) 0.042 (2) 0.0076 (18) 0.0023 (19) 0.0014 (19)
C13 0.052 (2) 0.049 (2) 0.049 (2) −0.0023 (18) 0.003 (2) −0.0043 (18)
C14 0.049 (2) 0.049 (2) 0.045 (2) 0.0014 (18) 0.0081 (18) 0.0016 (18)
C15 0.059 (2) 0.064 (2) 0.048 (2) −0.008 (2) 0.0096 (19) −0.005 (2)
C16 0.083 (3) 0.050 (2) 0.045 (2) 0.012 (2) 0.012 (2) −0.0052 (19)
C17 0.113 (4) 0.052 (2) 0.048 (2) 0.001 (3) 0.018 (3) −0.005 (2)
C18 0.066 (3) 0.049 (2) 0.042 (2) −0.011 (2) 0.001 (2) 0.0043 (18)
C19 0.055 (2) 0.045 (2) 0.0339 (19) −0.0059 (18) 0.0061 (17) 0.0028 (16)
C20 0.052 (2) 0.068 (3) 0.051 (2) 0.000 (2) 0.014 (2) −0.010 (2)
C21 0.047 (2) 0.077 (3) 0.046 (2) −0.006 (2) 0.005 (2) −0.016 (2)
C22 0.050 (2) 0.046 (2) 0.044 (2) −0.0031 (19) 0.010 (2) −0.0013 (18)
C23 0.047 (2) 0.055 (2) 0.053 (2) 0.0088 (19) 0.006 (2) 0.0049 (19)
C24 0.054 (2) 0.058 (2) 0.047 (2) 0.001 (2) −0.0086 (19) 0.0080 (19)

Geometric parameters (Å, °)

N1—C4 1.467 (5) C8—C9 1.466 (5)
N1—C1 1.478 (4) C8—H8 0.9300
N1—C5 1.481 (4) C9—C10 1.383 (5)
N2—C2 1.465 (5) C9—C14 1.395 (5)
N2—C15 1.479 (4) C10—C11 1.398 (5)
N2—C3 1.483 (4) C10—H10 0.9300
N3—C8 1.269 (5) C11—C12 1.381 (6)
N3—C7 1.467 (5) C11—H11 0.9300
N4—C18 1.256 (5) C12—C13 1.392 (5)
N4—C17 1.458 (5) C13—C14 1.390 (5)
O1—C12 1.361 (4) C13—H13 0.9300
O1—H1 0.8200 C14—H14 0.9300
O2—C22 1.367 (4) C15—C16 1.513 (6)
O2—H2 0.8200 C15—H15A 0.9700
C1—C2 1.511 (5) C15—H15B 0.9700
C1—H1A 0.9700 C16—C17 1.520 (5)
C1—H1B 0.9700 C16—H16A 0.9700
C2—H2A 0.9700 C16—H16B 0.9700
C2—H2B 0.9700 C17—H17A 0.9700
C3—C4 1.509 (5) C17—H17B 0.9700
C3—H3A 0.9700 C18—C19 1.468 (5)
C3—H3B 0.9700 C18—H18 0.9300
C4—H4A 0.9700 C19—C20 1.384 (5)
C4—H4B 0.9700 C19—C24 1.394 (5)
C5—C6 1.504 (6) C20—C21 1.386 (5)
C5—H5A 0.9700 C20—H20 0.9300
C5—H5B 0.9700 C21—C22 1.387 (5)
C6—C7 1.529 (6) C21—H21 0.9300
C6—H6A 0.9700 C22—C23 1.374 (5)
C6—H6B 0.9700 C23—C24 1.382 (5)
C7—H7A 0.9700 C23—H23 0.9300
C7—H7B 0.9700 C24—H24 0.9300
C4—N1—C1 107.4 (3) C10—C9—C8 120.7 (4)
C4—N1—C5 110.5 (3) C14—C9—C8 121.2 (4)
C1—N1—C5 111.9 (3) C9—C10—C11 121.5 (4)
C2—N2—C15 109.7 (3) C9—C10—H10 119.3
C2—N2—C3 108.3 (3) C11—C10—H10 119.3
C15—N2—C3 112.1 (3) C12—C11—C10 120.0 (4)
C8—N3—C7 118.2 (4) C12—C11—H11 120.0
C18—N4—C17 119.5 (4) C10—C11—H11 120.0
C12—O1—H1 109.5 O1—C12—C11 118.1 (3)
C22—O2—H2 109.5 O1—C12—C13 122.8 (3)
N1—C1—C2 110.5 (3) C11—C12—C13 119.1 (3)
N1—C1—H1A 109.5 C14—C13—C12 120.6 (3)
C2—C1—H1A 109.5 C14—C13—H13 119.7
N1—C1—H1B 109.5 C12—C13—H13 119.7
C2—C1—H1B 109.5 C13—C14—C9 120.7 (3)
H1A—C1—H1B 108.1 C13—C14—H14 119.7
N2—C2—C1 112.5 (3) C9—C14—H14 119.7
N2—C2—H2A 109.1 N2—C15—C16 114.4 (3)
C1—C2—H2A 109.1 N2—C15—H15A 108.7
N2—C2—H2B 109.1 C16—C15—H15A 108.7
C1—C2—H2B 109.1 N2—C15—H15B 108.7
H2A—C2—H2B 107.8 C16—C15—H15B 108.7
N2—C3—C4 110.4 (3) H15A—C15—H15B 107.6
N2—C3—H3A 109.6 C15—C16—C17 112.4 (4)
C4—C3—H3A 109.6 C15—C16—H16A 109.1
N2—C3—H3B 109.6 C17—C16—H16A 109.1
C4—C3—H3B 109.6 C15—C16—H16B 109.1
H3A—C3—H3B 108.1 C17—C16—H16B 109.1
N1—C4—C3 112.1 (3) H16A—C16—H16B 107.9
N1—C4—H4A 109.2 N4—C17—C16 111.1 (3)
C3—C4—H4A 109.2 N4—C17—H17A 109.4
N1—C4—H4B 109.2 C16—C17—H17A 109.4
C3—C4—H4B 109.2 N4—C17—H17B 109.4
H4A—C4—H4B 107.9 C16—C17—H17B 109.4
N1—C5—C6 114.6 (3) H17A—C17—H17B 108.0
N1—C5—H5A 108.6 N4—C18—C19 123.2 (4)
C6—C5—H5A 108.6 N4—C18—H18 118.4
N1—C5—H5B 108.6 C19—C18—H18 118.4
C6—C5—H5B 108.6 C20—C19—C24 117.8 (3)
H5A—C5—H5B 107.6 C20—C19—C18 121.0 (4)
C5—C6—C7 112.6 (4) C24—C19—C18 121.2 (4)
C5—C6—H6A 109.1 C19—C20—C21 121.3 (4)
C7—C6—H6A 109.1 C19—C20—H20 119.3
C5—C6—H6B 109.1 C21—C20—H20 119.3
C7—C6—H6B 109.1 C20—C21—C22 120.1 (4)
H6A—C6—H6B 107.8 C20—C21—H21 120.0
N3—C7—C6 110.8 (3) C22—C21—H21 120.0
N3—C7—H7A 109.5 O2—C22—C23 118.2 (3)
C6—C7—H7A 109.5 O2—C22—C21 122.6 (3)
N3—C7—H7B 109.5 C23—C22—C21 119.1 (3)
C6—C7—H7B 109.5 C22—C23—C24 120.7 (3)
H7A—C7—H7B 108.1 C22—C23—H23 119.6
N3—C8—C9 122.7 (4) C24—C23—H23 119.6
N3—C8—H8 118.6 C23—C24—C19 120.9 (4)
C9—C8—H8 118.6 C23—C24—H24 119.5
C10—C9—C14 118.1 (3) C19—C24—H24 119.5
C4—N1—C1—C2 −57.8 (4) O1—C12—C13—C14 −178.9 (3)
C5—N1—C1—C2 −179.3 (3) C11—C12—C13—C14 0.7 (6)
C15—N2—C2—C1 −179.4 (3) C12—C13—C14—C9 0.8 (5)
C3—N2—C2—C1 −56.8 (4) C10—C9—C14—C13 −2.5 (5)
N1—C1—C2—N2 59.2 (4) C8—C9—C14—C13 178.4 (3)
C2—N2—C3—C4 56.1 (4) C2—N2—C15—C16 −172.3 (3)
C15—N2—C3—C4 177.3 (3) C3—N2—C15—C16 67.3 (4)
C1—N1—C4—C3 59.4 (4) N2—C15—C16—C17 165.2 (3)
C5—N1—C4—C3 −178.3 (3) C18—N4—C17—C16 109.1 (5)
N2—C3—C4—N1 −60.0 (4) C15—C16—C17—N4 −77.3 (5)
C4—N1—C5—C6 177.5 (3) C17—N4—C18—C19 179.8 (3)
C1—N1—C5—C6 −62.9 (4) N4—C18—C19—C20 −7.1 (5)
N1—C5—C6—C7 −164.6 (3) N4—C18—C19—C24 173.7 (3)
C8—N3—C7—C6 −125.9 (4) C24—C19—C20—C21 0.1 (5)
C5—C6—C7—N3 70.6 (5) C18—C19—C20—C21 −179.0 (3)
C7—N3—C8—C9 −179.6 (3) C19—C20—C21—C22 −0.4 (6)
N3—C8—C9—C10 172.5 (4) C20—C21—C22—O2 178.0 (3)
N3—C8—C9—C14 −8.3 (5) C20—C21—C22—C23 0.1 (5)
C14—C9—C10—C11 2.7 (6) O2—C22—C23—C24 −177.6 (3)
C8—C9—C10—C11 −178.1 (3) C21—C22—C23—C24 0.4 (5)
C9—C10—C11—C12 −1.3 (6) C22—C23—C24—C19 −0.7 (5)
C10—C11—C12—O1 179.2 (3) C20—C19—C24—C23 0.4 (5)
C10—C11—C12—C13 −0.4 (6) C18—C19—C24—C23 179.6 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O2—H2···N1i 0.82 1.98 2.762 (4) 159
O1—H1···N2ii 0.82 2.00 2.780 (4) 159

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH2937).

References

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  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
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  8. Yogavel, M., Selvanayagam, S., Velmurugan, D., Shanmuga Sundara Raj, S., Fun, H.-K., Marappan, M. & Kandaswamy, M. (2003). Acta Cryst. E59, o83–o85.

Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809045620/lh2937sup1.cif

e-65-o2996-sup1.cif (22.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809045620/lh2937Isup2.hkl

e-65-o2996-Isup2.hkl (99.2KB, hkl)

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


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