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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Oct 3;65(Pt 11):o2627. doi: 10.1107/S160053680903921X

1-Dec­yloxy-4-nitro­benzene

Xi-Gui Yue a,*
PMCID: PMC2970962  PMID: 21578243

Abstract

The title compound, C16H25NO3, has a zigzag dec­yloxy chain para to the nitro group of the aromatic ring. There are two independent mol­ecules; the two rings are aligned at 48.15 (7)°. In the crystal, weak C—H⋯O hydrogen bonds lead to the formation of infinite chains.

Related literature

For structures of analogs of the title compound, see: McBurney et al. (2004).graphic file with name e-65-o2627-scheme1.jpg

Experimental

Crystal data

  • C16H25NO3

  • M r = 279.37

  • Triclinic, Inline graphic

  • a = 5.642 (3) Å

  • b = 16.065 (8) Å

  • c = 19.135 (7) Å

  • α = 107.410 (16)°

  • β = 90.610 (16)°

  • γ = 99.780 (18)°

  • V = 1627.4 (13) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 291 K

  • 0.20 × 0.19 × 0.17 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.984, T max = 0.987

  • 15990 measured reflections

  • 7274 independent reflections

  • 3970 reflections with I > 2σ(I)

  • R int = 0.030

Refinement

  • R[F 2 > 2σ(F 2)] = 0.052

  • wR(F 2) = 0.176

  • S = 0.97

  • 7274 reflections

  • 363 parameters

  • H-atom parameters constrained

  • Δρmax = 0.18 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: RAPID-AUTO (Rigaku, 1998); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053680903921X/ng2644sup1.cif

e-65-o2627-sup1.cif (25.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680903921X/ng2644Isup2.hkl

e-65-o2627-Isup2.hkl (355.9KB, 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
C6—H6⋯O2i 0.93 2.53 3.378 (3) 152
C7—H7B⋯O5ii 0.97 2.77 3.263 (3) 112
C18—H18⋯O4iii 0.93 2.60 3.379 (3) 141
C21—H21⋯O1iv 0.93 2.70 3.346 (3) 127
C22—H22⋯O1iv 0.93 2.79 3.381 (3) 123

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

supplementary crystallographic information

Comment

The hydroxy H atom of 4-nitropheno can be substituted by multifarious groups to form many ramifications(McBurney et al., 2004). We have synthesized the analogs using different alkyl as terminal groups and report here the molecular and crystal structures of the title compound, (I).

The title compound, (I), as shown in Fig. 1, crystallizes in space group P-1 and each asymmetric unit consists of two crystallographically independent 1-(decyloxy)-4-nitrobenzene. The angles of the two benzene rings (C1—C6 and C17—C22) in the same asymmetric unit is 48.15 (7) °. All nitryl oxygen atoms are engaged in C—H···O (2.53 (2), 2.60 (2), 2.70 (2), 2.77 (2), 2.79 (2) Å) hydrogen bonds. The weak C—H···O hydrogen bonds link the crystal into a two-dimensional network.

Experimental

1-(decyloxy)-4-nitrobenzene was prepared by adding 4-nitrophenol (0.14 g, 1 mmol), decyl iodide (0.27 g, 1 mmol) and acetone(15 ml) into 10 ml of 8% sodium hydroxide solution. The resultant mixture was heated for 2 h under reflux, then the solution was cooled to room temperaure in an ice bath with stirring. The colorless products were obtained by recrystallized the crude solid from 95% ethanol.

Refinement

The benzene H atoms were treated as riding on their parent atoms, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C). H atoms attached to methylene were treated as riding on their parent atoms with C—H = 0.97 Å and Uiso(H) = 1.2Ueq(C), instead with C—H = 0.96 Å and Uiso(H) = 1.5Ueq(C) for methyl.

Figures

Fig. 1.

Fig. 1.

The asymmetric of title compound, with the atom numbering. Displacement ellipsoids of non-H atoms are drawn at the 30% probalility level.

Crystal data

C16H25NO3 Z = 4
Mr = 279.37 F(000) = 608
Triclinic, P1 Dx = 1.140 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 5.642 (3) Å Cell parameters from 9752 reflections
b = 16.065 (8) Å θ = 3.2–27.5°
c = 19.135 (7) Å µ = 0.08 mm1
α = 107.410 (16)° T = 291 K
β = 90.610 (16)° Block, colorless
γ = 99.780 (18)° 0.20 × 0.19 × 0.17 mm
V = 1627.4 (13) Å3

Data collection

Rigaku R-AXIS RAPID diffractometer 7274 independent reflections
Radiation source: fine-focus sealed tube 3970 reflections with I > 2σ(I)
graphite Rint = 0.030
ω scans θmax = 27.5°, θmin = 3.2°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) h = −7→7
Tmin = 0.984, Tmax = 0.987 k = −20→20
15990 measured reflections l = −23→24

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)] = 0.052 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.176 H-atom parameters constrained
S = 0.97 w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3
7274 reflections (Δ/σ)max < 0.001
363 parameters Δρmax = 0.18 e Å3
0 restraints Δρmin = −0.17 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
C1 1.0435 (3) −0.10617 (12) 0.41928 (9) 0.0498 (4)
C2 0.8180 (4) −0.14170 (12) 0.38389 (10) 0.0552 (5)
H2 0.7414 −0.1982 0.3826 0.066*
C3 0.7089 (4) −0.09201 (13) 0.35064 (10) 0.0561 (5)
H3 0.5583 −0.1155 0.3258 0.067*
C4 0.8218 (3) −0.00675 (12) 0.35376 (9) 0.0492 (4)
C5 1.0481 (3) 0.02798 (12) 0.38982 (9) 0.0518 (4)
H5 1.1245 0.0848 0.3920 0.062*
C6 1.1591 (3) −0.02269 (13) 0.42251 (9) 0.0530 (5)
H6 1.3112 −0.0002 0.4465 0.064*
C7 0.7923 (4) 0.12696 (13) 0.32581 (11) 0.0622 (5)
H7A 0.9486 0.1313 0.3052 0.075*
H7B 0.8115 0.1628 0.3770 0.075*
C8 0.6180 (4) 0.15878 (14) 0.28437 (10) 0.0608 (5)
H8A 0.6685 0.2221 0.2934 0.073*
H8B 0.4603 0.1494 0.3033 0.073*
C9 0.5963 (4) 0.11315 (13) 0.20197 (9) 0.0557 (5)
H9A 0.7539 0.1221 0.1828 0.067*
H9B 0.5439 0.0499 0.1927 0.067*
C10 0.4209 (4) 0.14703 (13) 0.16135 (10) 0.0562 (5)
H10A 0.4705 0.2107 0.1724 0.067*
H10B 0.2627 0.1363 0.1797 0.067*
C11 0.4007 (4) 0.10524 (13) 0.07868 (10) 0.0575 (5)
H11A 0.3507 0.0416 0.0674 0.069*
H11B 0.5584 0.1161 0.0600 0.069*
C12 0.2237 (4) 0.14028 (13) 0.03955 (10) 0.0569 (5)
H12A 0.0659 0.1286 0.0579 0.068*
H12B 0.2724 0.2041 0.0519 0.068*
C13 0.2023 (4) 0.10103 (14) −0.04315 (10) 0.0611 (5)
H13A 0.1537 0.0372 −0.0557 0.073*
H13B 0.3595 0.1130 −0.0618 0.073*
C14 0.0239 (4) 0.13677 (14) −0.08081 (10) 0.0591 (5)
H14A −0.1333 0.1241 −0.0624 0.071*
H14B 0.0715 0.2007 −0.0673 0.071*
C15 0.0008 (4) 0.10000 (17) −0.16340 (11) 0.0763 (6)
H15A 0.1577 0.1128 −0.1820 0.092*
H15B −0.0471 0.0360 −0.1771 0.092*
C16 −0.1776 (5) 0.13638 (19) −0.19974 (12) 0.0838 (7)
H16A −0.3362 0.1198 −0.1849 0.126*
H16B −0.1757 0.1127 −0.2521 0.126*
H16C −0.1349 0.1999 −0.1854 0.126*
C17 1.6603 (3) 0.61062 (12) 0.48056 (9) 0.0483 (4)
C18 1.7118 (3) 0.52982 (12) 0.44104 (9) 0.0515 (4)
H18 1.8424 0.5094 0.4559 0.062*
C19 1.5682 (3) 0.47936 (12) 0.37915 (9) 0.0528 (5)
H19 1.6015 0.4246 0.3518 0.063*
C20 1.3741 (3) 0.51059 (12) 0.35782 (9) 0.0485 (4)
C21 1.3281 (4) 0.59306 (12) 0.39760 (10) 0.0550 (5)
H21 1.2002 0.6145 0.3824 0.066*
C22 1.4712 (3) 0.64329 (12) 0.45951 (10) 0.0549 (5)
H22 1.4402 0.6985 0.4867 0.066*
C23 1.2354 (4) 0.37683 (12) 0.25940 (10) 0.0599 (5)
H23A 1.2308 0.3412 0.2924 0.072*
H23B 1.3861 0.3757 0.2355 0.072*
C24 1.0252 (4) 0.34081 (13) 0.20304 (10) 0.0597 (5)
H24A 0.8776 0.3485 0.2278 0.072*
H24B 1.0193 0.2776 0.1810 0.072*
C25 1.0330 (4) 0.38395 (13) 0.14233 (9) 0.0577 (5)
H25A 1.0412 0.4473 0.1641 0.069*
H25B 1.1786 0.3752 0.1167 0.069*
C26 0.8174 (4) 0.34758 (13) 0.08732 (10) 0.0596 (5)
H26A 0.8071 0.2840 0.0667 0.072*
H26B 0.6725 0.3575 0.1130 0.072*
C27 0.8234 (4) 0.38781 (14) 0.02524 (10) 0.0636 (5)
H27A 0.9663 0.3766 −0.0012 0.076*
H27B 0.8377 0.4516 0.0459 0.076*
C28 0.6052 (4) 0.35306 (15) −0.02876 (11) 0.0664 (6)
H28A 0.5915 0.2893 −0.0495 0.080*
H28B 0.4625 0.3640 −0.0022 0.080*
C29 0.6087 (4) 0.39286 (17) −0.09064 (11) 0.0740 (6)
H29A 0.7486 0.3802 −0.1181 0.089*
H29B 0.6282 0.4568 −0.0699 0.089*
C30 0.3882 (4) 0.36084 (16) −0.14327 (11) 0.0727 (6)
H30A 0.3688 0.2969 −0.1639 0.087*
H30B 0.2485 0.3735 −0.1157 0.087*
C31 0.3896 (5) 0.3997 (2) −0.20473 (15) 0.1040 (10)
H31A 0.5228 0.3834 −0.2343 0.125*
H31B 0.4206 0.4638 −0.1842 0.125*
C32 0.1645 (5) 0.3727 (2) −0.25393 (14) 0.0943 (8)
H32A 0.1262 0.3092 −0.2727 0.141*
H32B 0.1884 0.3969 −0.2940 0.141*
H32C 0.0344 0.3947 −0.2267 0.141*
N1 1.1571 (3) −0.15848 (12) 0.45537 (9) 0.0611 (4)
N2 1.8046 (3) 0.66154 (12) 0.54848 (8) 0.0598 (4)
O1 1.0497 (3) −0.23246 (12) 0.45217 (11) 0.0953 (6)
O2 1.3531 (3) −0.12644 (11) 0.48909 (9) 0.0814 (5)
O3 0.6957 (2) 0.03615 (9) 0.31962 (7) 0.0598 (4)
O4 1.9796 (3) 0.63492 (11) 0.56572 (8) 0.0779 (5)
O5 1.7400 (3) 0.72868 (11) 0.58678 (8) 0.0860 (5)
O6 1.2164 (2) 0.46592 (9) 0.29918 (7) 0.0616 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0558 (11) 0.0542 (11) 0.0446 (9) 0.0219 (9) 0.0075 (8) 0.0163 (7)
C2 0.0593 (12) 0.0479 (11) 0.0608 (11) 0.0114 (9) 0.0059 (9) 0.0190 (8)
C3 0.0517 (11) 0.0557 (12) 0.0607 (11) 0.0080 (9) −0.0042 (9) 0.0188 (9)
C4 0.0543 (11) 0.0536 (11) 0.0428 (8) 0.0139 (8) 0.0003 (7) 0.0174 (7)
C5 0.0569 (11) 0.0500 (10) 0.0489 (9) 0.0059 (8) −0.0016 (8) 0.0181 (8)
C6 0.0529 (11) 0.0605 (12) 0.0462 (9) 0.0129 (9) −0.0013 (8) 0.0161 (8)
C7 0.0787 (14) 0.0553 (12) 0.0549 (10) 0.0099 (10) −0.0063 (10) 0.0218 (9)
C8 0.0753 (14) 0.0561 (12) 0.0580 (10) 0.0216 (10) 0.0011 (9) 0.0228 (9)
C9 0.0632 (12) 0.0560 (11) 0.0547 (10) 0.0197 (9) 0.0011 (9) 0.0223 (8)
C10 0.0613 (12) 0.0558 (11) 0.0577 (10) 0.0188 (9) 0.0021 (9) 0.0223 (9)
C11 0.0623 (12) 0.0578 (12) 0.0558 (10) 0.0153 (9) −0.0008 (9) 0.0204 (9)
C12 0.0581 (12) 0.0610 (12) 0.0553 (10) 0.0159 (9) −0.0011 (9) 0.0205 (9)
C13 0.0654 (13) 0.0649 (13) 0.0536 (10) 0.0150 (10) −0.0033 (9) 0.0171 (9)
C14 0.0568 (12) 0.0652 (13) 0.0553 (10) 0.0105 (10) −0.0005 (9) 0.0190 (9)
C15 0.0738 (15) 0.0979 (18) 0.0552 (11) 0.0226 (13) −0.0071 (10) 0.0168 (11)
C16 0.0803 (16) 0.113 (2) 0.0585 (12) 0.0234 (14) −0.0106 (11) 0.0247 (12)
C17 0.0491 (10) 0.0482 (10) 0.0461 (9) 0.0050 (8) 0.0005 (7) 0.0142 (7)
C18 0.0495 (10) 0.0560 (11) 0.0525 (10) 0.0140 (8) −0.0011 (8) 0.0198 (8)
C19 0.0611 (12) 0.0514 (11) 0.0466 (9) 0.0194 (9) 0.0010 (8) 0.0112 (8)
C20 0.0532 (11) 0.0513 (10) 0.0417 (8) 0.0115 (8) −0.0008 (7) 0.0144 (7)
C21 0.0553 (11) 0.0543 (11) 0.0569 (10) 0.0189 (9) −0.0033 (8) 0.0143 (8)
C22 0.0584 (11) 0.0458 (10) 0.0591 (10) 0.0156 (8) 0.0014 (9) 0.0106 (8)
C23 0.0765 (14) 0.0540 (11) 0.0481 (9) 0.0175 (10) −0.0059 (9) 0.0112 (8)
C24 0.0676 (13) 0.0561 (11) 0.0509 (10) 0.0060 (9) −0.0048 (9) 0.0130 (8)
C25 0.0613 (12) 0.0583 (12) 0.0503 (10) 0.0056 (9) −0.0032 (9) 0.0150 (8)
C26 0.0608 (12) 0.0626 (12) 0.0521 (10) 0.0029 (10) −0.0059 (9) 0.0173 (9)
C27 0.0603 (13) 0.0726 (14) 0.0571 (11) 0.0025 (10) −0.0061 (9) 0.0239 (10)
C28 0.0628 (13) 0.0753 (14) 0.0598 (11) −0.0001 (11) −0.0096 (10) 0.0261 (10)
C29 0.0664 (14) 0.0923 (17) 0.0672 (12) −0.0002 (12) −0.0090 (11) 0.0387 (11)
C30 0.0696 (14) 0.0848 (16) 0.0630 (12) 0.0045 (12) −0.0099 (10) 0.0272 (11)
C31 0.0847 (18) 0.150 (3) 0.0893 (17) −0.0053 (17) −0.0188 (14) 0.0705 (18)
C32 0.0967 (19) 0.118 (2) 0.0747 (15) 0.0257 (16) −0.0117 (14) 0.0354 (14)
N1 0.0681 (11) 0.0645 (11) 0.0604 (9) 0.0272 (9) 0.0088 (8) 0.0251 (8)
N2 0.0583 (10) 0.0597 (11) 0.0558 (9) 0.0045 (8) −0.0032 (8) 0.0128 (8)
O1 0.1013 (13) 0.0676 (11) 0.1324 (14) 0.0189 (9) −0.0091 (11) 0.0523 (10)
O2 0.0739 (11) 0.0946 (12) 0.0890 (11) 0.0244 (9) −0.0106 (9) 0.0433 (9)
O3 0.0613 (8) 0.0587 (8) 0.0645 (8) 0.0088 (6) −0.0112 (6) 0.0279 (6)
O4 0.0709 (10) 0.0857 (11) 0.0717 (9) 0.0151 (8) −0.0216 (8) 0.0163 (8)
O5 0.0878 (12) 0.0727 (11) 0.0754 (10) 0.0160 (9) −0.0120 (8) −0.0105 (8)
O6 0.0696 (9) 0.0574 (8) 0.0524 (7) 0.0203 (6) −0.0148 (6) 0.0047 (6)

Geometric parameters (Å, °)

C1—C6 1.371 (3) C17—N2 1.462 (2)
C1—C2 1.381 (3) C18—C19 1.378 (2)
C1—N1 1.454 (2) C18—H18 0.9300
C2—C3 1.372 (3) C19—C20 1.385 (3)
C2—H2 0.9300 C19—H19 0.9300
C3—C4 1.393 (3) C20—O6 1.359 (2)
C3—H3 0.9300 C20—C21 1.385 (3)
C4—O3 1.354 (2) C21—C22 1.375 (2)
C4—C5 1.388 (3) C21—H21 0.9300
C5—C6 1.384 (2) C22—H22 0.9300
C5—H5 0.9300 C23—O6 1.429 (2)
C6—H6 0.9300 C23—C24 1.507 (3)
C7—O3 1.437 (2) C23—H23A 0.9700
C7—C8 1.501 (3) C23—H23B 0.9700
C7—H7A 0.9700 C24—C25 1.518 (3)
C7—H7B 0.9700 C24—H24A 0.9700
C8—C9 1.521 (3) C24—H24B 0.9700
C8—H8A 0.9700 C25—C26 1.514 (2)
C8—H8B 0.9700 C25—H25A 0.9700
C9—C10 1.516 (2) C25—H25B 0.9700
C9—H9A 0.9700 C26—C27 1.511 (3)
C9—H9B 0.9700 C26—H26A 0.9700
C10—C11 1.517 (3) C26—H26B 0.9700
C10—H10A 0.9700 C27—C28 1.513 (3)
C10—H10B 0.9700 C27—H27A 0.9700
C11—C12 1.517 (3) C27—H27B 0.9700
C11—H11A 0.9700 C28—C29 1.504 (3)
C11—H11B 0.9700 C28—H28A 0.9700
C12—C13 1.513 (3) C28—H28B 0.9700
C12—H12A 0.9700 C29—C30 1.507 (3)
C12—H12B 0.9700 C29—H29A 0.9700
C13—C14 1.513 (3) C29—H29B 0.9700
C13—H13A 0.9700 C30—C31 1.487 (3)
C13—H13B 0.9700 C30—H30A 0.9700
C14—C15 1.508 (3) C30—H30B 0.9700
C14—H14A 0.9700 C31—C32 1.494 (3)
C14—H14B 0.9700 C31—H31A 0.9700
C15—C16 1.506 (3) C31—H31B 0.9700
C15—H15A 0.9700 C32—H32A 0.9600
C15—H15B 0.9700 C32—H32B 0.9600
C16—H16A 0.9600 C32—H32C 0.9600
C16—H16B 0.9600 N1—O1 1.222 (2)
C16—H16C 0.9600 N1—O2 1.223 (2)
C17—C22 1.373 (3) N2—O4 1.220 (2)
C17—C18 1.374 (3) N2—O5 1.225 (2)
C6—C1—C2 121.73 (17) C17—C18—H18 120.3
C6—C1—N1 119.66 (17) C19—C18—H18 120.3
C2—C1—N1 118.59 (18) C18—C19—C20 119.66 (18)
C3—C2—C1 118.74 (18) C18—C19—H19 120.2
C3—C2—H2 120.6 C20—C19—H19 120.2
C1—C2—H2 120.6 O6—C20—C19 124.99 (17)
C2—C3—C4 120.55 (18) O6—C20—C21 114.94 (16)
C2—C3—H3 119.7 C19—C20—C21 120.08 (16)
C4—C3—H3 119.7 C22—C21—C20 120.23 (17)
O3—C4—C5 124.92 (17) C22—C21—H21 119.9
O3—C4—C3 115.19 (16) C20—C21—H21 119.9
C5—C4—C3 119.89 (17) C17—C22—C21 118.89 (18)
C6—C5—C4 119.46 (17) C17—C22—H22 120.6
C6—C5—H5 120.3 C21—C22—H22 120.6
C4—C5—H5 120.3 O6—C23—C24 107.35 (16)
C1—C6—C5 119.62 (17) O6—C23—H23A 110.2
C1—C6—H6 120.2 C24—C23—H23A 110.2
C5—C6—H6 120.2 O6—C23—H23B 110.2
O3—C7—C8 107.42 (16) C24—C23—H23B 110.2
O3—C7—H7A 110.2 H23A—C23—H23B 108.5
C8—C7—H7A 110.2 C23—C24—C25 114.59 (17)
O3—C7—H7B 110.2 C23—C24—H24A 108.6
C8—C7—H7B 110.2 C25—C24—H24A 108.6
H7A—C7—H7B 108.5 C23—C24—H24B 108.6
C7—C8—C9 114.15 (17) C25—C24—H24B 108.6
C7—C8—H8A 108.7 H24A—C24—H24B 107.6
C9—C8—H8A 108.7 C26—C25—C24 113.38 (16)
C7—C8—H8B 108.7 C26—C25—H25A 108.9
C9—C8—H8B 108.7 C24—C25—H25A 108.9
H8A—C8—H8B 107.6 C26—C25—H25B 108.9
C10—C9—C8 113.08 (16) C24—C25—H25B 108.9
C10—C9—H9A 109.0 H25A—C25—H25B 107.7
C8—C9—H9A 109.0 C27—C26—C25 114.50 (16)
C10—C9—H9B 109.0 C27—C26—H26A 108.6
C8—C9—H9B 109.0 C25—C26—H26A 108.6
H9A—C9—H9B 107.8 C27—C26—H26B 108.6
C9—C10—C11 114.62 (16) C25—C26—H26B 108.6
C9—C10—H10A 108.6 H26A—C26—H26B 107.6
C11—C10—H10A 108.6 C26—C27—C28 114.52 (17)
C9—C10—H10B 108.6 C26—C27—H27A 108.6
C11—C10—H10B 108.6 C28—C27—H27A 108.6
H10A—C10—H10B 107.6 C26—C27—H27B 108.6
C10—C11—C12 113.45 (17) C28—C27—H27B 108.6
C10—C11—H11A 108.9 H27A—C27—H27B 107.6
C12—C11—H11A 108.9 C29—C28—C27 115.03 (17)
C10—C11—H11B 108.9 C29—C28—H28A 108.5
C12—C11—H11B 108.9 C27—C28—H28A 108.5
H11A—C11—H11B 107.7 C29—C28—H28B 108.5
C13—C12—C11 114.79 (17) C27—C28—H28B 108.5
C13—C12—H12A 108.6 H28A—C28—H28B 107.5
C11—C12—H12A 108.6 C28—C29—C30 115.36 (18)
C13—C12—H12B 108.6 C28—C29—H29A 108.4
C11—C12—H12B 108.6 C30—C29—H29A 108.4
H12A—C12—H12B 107.5 C28—C29—H29B 108.4
C12—C13—C14 113.73 (17) C30—C29—H29B 108.4
C12—C13—H13A 108.8 H29A—C29—H29B 107.5
C14—C13—H13A 108.8 C31—C30—C29 115.8 (2)
C12—C13—H13B 108.8 C31—C30—H30A 108.3
C14—C13—H13B 108.8 C29—C30—H30A 108.3
H13A—C13—H13B 107.7 C31—C30—H30B 108.3
C15—C14—C13 115.11 (18) C29—C30—H30B 108.3
C15—C14—H14A 108.5 H30A—C30—H30B 107.4
C13—C14—H14A 108.5 C30—C31—C32 115.9 (2)
C15—C14—H14B 108.5 C30—C31—H31A 108.3
C13—C14—H14B 108.5 C32—C31—H31A 108.3
H14A—C14—H14B 107.5 C30—C31—H31B 108.3
C16—C15—C14 114.2 (2) C32—C31—H31B 108.3
C16—C15—H15A 108.7 H31A—C31—H31B 107.4
C14—C15—H15A 108.7 C31—C32—H32A 109.5
C16—C15—H15B 108.7 C31—C32—H32B 109.5
C14—C15—H15B 108.7 H32A—C32—H32B 109.5
H15A—C15—H15B 107.6 C31—C32—H32C 109.5
C15—C16—H16A 109.5 H32A—C32—H32C 109.5
C15—C16—H16B 109.5 H32B—C32—H32C 109.5
H16A—C16—H16B 109.5 O1—N1—O2 122.39 (18)
C15—C16—H16C 109.5 O1—N1—C1 118.43 (18)
H16A—C16—H16C 109.5 O2—N1—C1 119.15 (18)
H16B—C16—H16C 109.5 O4—N2—O5 122.67 (17)
C22—C17—C18 121.79 (16) O4—N2—C17 119.36 (18)
C22—C17—N2 119.07 (17) O5—N2—C17 117.95 (17)
C18—C17—N2 119.10 (17) C4—O3—C7 118.14 (14)
C17—C18—C19 119.34 (17) C20—O6—C23 118.71 (14)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C6—H6···O2i 0.93 2.53 3.378 (3) 152
C7—H7B···O5ii 0.97 2.77 3.263 (3) 112
C18—H18···O4iii 0.93 2.60 3.379 (3) 141
C21—H21···O1iv 0.93 2.70 3.346 (3) 127
C22—H22···O1iv 0.93 2.79 3.381 (3) 123

Symmetry codes: (i) −x+3, −y, −z+1; (ii) −x+3, −y+1, −z+1; (iii) −x+4, −y+1, −z+1; (iv) x, y+1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2644).

References

  1. Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
  2. Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst.39, 453–457.
  3. McBurney, B., Foss, P. C. D., Reed, E. M., Shine, T. D., Glagovich, N. M., Westcott, B. L., Crundwell, G., Zeller, M. & Hunter, A. D. (2004). Acta Cryst. E60, o2179–o2180.
  4. Rigaku (1998). RAPID-AUTO Rigaku Corporation, Tokyo, Japan.
  5. Rigaku/MSC (2002). CrystalStructure Rigaku/MSC Inc., The Woodlands, Texas, USA.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [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/S160053680903921X/ng2644sup1.cif

e-65-o2627-sup1.cif (25.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680903921X/ng2644Isup2.hkl

e-65-o2627-Isup2.hkl (355.9KB, hkl)

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


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