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The synthesis, 1H and 13C NMR spectra, and X-ray structures are described for three di­alk­oxy ethynyl­nitro­benzenes that differ only in the length of the alk­oxy chain, namely 1-ethynyl-2-nitro-4,5-dipropoxybenzene, C14H17NO4, 1,2-di­but­oxy-4-ethynyl-5-nitro­benzene, C16H21NO4, and 1-ethynyl-2-nitro-4,5-dipentoxy­benzene, C18H25NO4. Despite the subtle changes in molecular structure, the crystal structures of the three compounds display great diversity. Thus, 1-ethynyl-2-nitro-4,5-dipropoxybenzene crystallizes in the trigonal crystal system in the space group R{\overline 3}, with Z = 18, 1,2-di­but­oxy-4-ethynyl-5-nitro­benzene crystallizes in the monoclinic crystal system in the space group P21/c, with Z = 4, and 1-ethynyl-2-nitro-4,5-dipentoxybenzene crystallizes in the tri­clinic crystal system in the space group P{\overline 1}, with Z = 2. The crystal structure of 1-ethynyl-2-nitro-4,5-dipropoxybenzene is dominated by planar hexamers formed by a bifurcated alkoxy sp-C—H...O,O′ interaction, while the structure of the di­but­oxy analogue is dominated by planar ribbons of molecules linked by a similar bifurcated alkoxy sp-C—H...O,O′ interaction. In contrast, the dipent­oxy analogue forms ribbons of molecules alternately connected by a self-complementary sp-C—H...O2N interaction and a self-complementary sp2-C—H...O2N interaction. Disordered solvent was included in the crystals of 1-ethynyl-2-nitro-4,5-dipropoxybenzene and its contribution was removed during refinement.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229617012761/fn3243sup1.cif
Contains datablocks 1, 2, 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229617012761/fn32431sup2.hkl
Contains datablock 1

cdx

Chemdraw file https://doi.org/10.1107/S2053229617012761/fn32431sup5.cdx
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229617012761/fn32431sup6.cml
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229617012761/fn32432sup3.hkl
Contains datablock 2

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229617012761/fn32432sup7.cml
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229617012761/fn32433sup4.hkl
Contains datablock 3

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229617012761/fn32433sup8.cml
Supplementary material

CCDC references: 1572979; 1572978; 1572977

Computing details top

For all structures, data collection: Bruker SMART; cell refinement: Bruker SMART; data reduction: Bruker SAINT; program(s) used to solve structure: SHELXT 2014/5 (Sheldrick, 2015); program(s) used to refine structure: SHELXL2017/1 (Sheldrick, 2015a); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: X-SEED (Barbour, 2001).

(1) top
Crystal data top
C14H17NO4Dx = 1.234 Mg m3
Mr = 263.29Mo Kα radiation, λ = 0.71073 Å
Trigonal, R3:HCell parameters from 5437 reflections
a = 26.6774 (16) Åθ = 2.6–27.1°
c = 10.3451 (6) ŵ = 0.09 mm1
V = 6376.1 (8) Å3T = 100 K
Z = 18Cut rectangular prism, colourless
F(000) = 25200.07 × 0.07 × 0.04 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
3172 independent reflections
Radiation source: fine-focus sealed tube2420 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
Detector resolution: 8.3660 pixels mm-1θmax = 27.2°, θmin = 1.5°
φ and ω scansh = 3434
Absorption correction: multi-scan
(SADABS Version 2014; Bruker AXS)
k = 3434
Tmin = 0.697, Tmax = 0.746l = 1313
28334 measured reflections
Refinement top
Refinement on F22 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.047H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.138 w = 1/[σ2(Fo2) + (0.0842P)2 + 1.9773P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.001
3172 reflectionsΔρmax = 0.43 e Å3
180 parametersΔρmin = 0.20 e Å3
Special details top

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. # SQUEEZE RESULTS # Note: Data are Listed for all Voids in the P1 Unit Cell # i.e. Centre of Gravity, Solvent Accessible Volume, # Recovered number of Electrons in the Void and # Details about the Squeezed Material loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 0.000 0.000 0.000 125 38 ' ' 2 0.333 0.667 0.667 115 38 ' ' 3 0.667 0.333 0.333 115 38 ' '

_platon_squeeze_details 'Reasonable that the squeezed solvent corresponds to dichloromethane (42 e)'

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.80137 (4)0.82653 (4)0.29721 (12)0.0429 (3)
N10.75096 (5)0.80819 (5)0.32978 (11)0.0256 (3)
C10.73231 (5)0.70715 (5)0.33025 (12)0.0206 (3)
O20.73202 (4)0.83983 (4)0.36150 (11)0.0375 (3)
C20.71127 (5)0.74567 (5)0.32948 (12)0.0212 (3)
O30.55388 (4)0.64527 (4)0.32599 (9)0.0261 (2)
C30.65221 (6)0.72722 (5)0.32879 (12)0.0212 (3)
O40.59014 (4)0.57189 (4)0.32933 (9)0.0244 (2)
C40.61230 (5)0.66862 (5)0.32747 (12)0.0209 (3)
C50.63200 (5)0.62827 (5)0.32965 (12)0.0209 (3)
C60.69061 (5)0.64767 (5)0.33122 (12)0.0205 (3)
H60.7032700.6201320.3330230.025*
C70.79185 (6)0.72157 (5)0.33451 (12)0.0232 (3)
C80.83787 (6)0.72495 (6)0.33970 (14)0.0286 (3)
C90.53135 (6)0.68428 (6)0.31049 (13)0.0252 (3)
H9A0.5435580.7044560.2262500.030*
H9B0.5460360.7136600.3801490.030*
C100.46645 (6)0.64833 (6)0.31691 (16)0.0336 (3)
H10A0.4547720.6299260.4030950.040*
H10B0.4525950.6172290.2512260.040*
C110.43856 (7)0.68527 (7)0.2930 (2)0.0480 (5)
H11A0.4536780.7171860.3554100.072*
H11B0.3965140.6614250.3032490.072*
H11C0.4475340.7009840.2050910.072*
C120.60887 (6)0.52969 (5)0.33039 (13)0.0239 (3)
H12A0.6303580.5332500.4110840.029*
H12B0.6349350.5363100.2562520.029*
C130.55624 (6)0.47007 (6)0.32152 (15)0.0290 (3)
H13A0.5347860.4667840.2409270.035*
H13B0.5302150.4637250.3955890.035*
C140.57451 (7)0.42451 (6)0.32240 (17)0.0374 (4)
H14A0.5985790.4296450.2464510.056*
H14B0.5400370.3858830.3202160.056*
H14C0.5966990.4286060.4010880.056*
H30.6402 (8)0.7547 (7)0.3249 (16)0.045*
H80.8740 (5)0.7274 (8)0.3423 (16)0.045*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0265 (6)0.0225 (5)0.0748 (8)0.0085 (4)0.0085 (5)0.0029 (5)
N10.0259 (6)0.0183 (6)0.0312 (6)0.0101 (5)0.0031 (5)0.0002 (4)
C10.0218 (6)0.0205 (6)0.0188 (6)0.0101 (5)0.0019 (5)0.0009 (5)
O20.0337 (6)0.0217 (5)0.0597 (7)0.0158 (4)0.0025 (5)0.0055 (5)
C20.0239 (6)0.0166 (6)0.0209 (6)0.0085 (5)0.0011 (5)0.0002 (5)
O30.0192 (5)0.0203 (5)0.0393 (6)0.0102 (4)0.0003 (4)0.0022 (4)
C30.0245 (6)0.0200 (6)0.0215 (6)0.0128 (5)0.0019 (5)0.0000 (5)
O40.0202 (5)0.0162 (4)0.0347 (5)0.0075 (4)0.0003 (4)0.0005 (4)
C40.0190 (6)0.0221 (6)0.0214 (6)0.0101 (5)0.0005 (5)0.0004 (5)
C50.0223 (6)0.0186 (6)0.0199 (6)0.0087 (5)0.0014 (5)0.0006 (5)
C60.0230 (6)0.0177 (6)0.0220 (6)0.0110 (5)0.0011 (5)0.0013 (5)
C70.0261 (7)0.0166 (6)0.0250 (6)0.0092 (5)0.0019 (5)0.0018 (5)
C80.0229 (7)0.0235 (7)0.0380 (8)0.0105 (6)0.0026 (6)0.0020 (6)
C90.0244 (7)0.0240 (6)0.0309 (7)0.0149 (6)0.0005 (5)0.0022 (5)
C100.0225 (7)0.0295 (7)0.0496 (9)0.0136 (6)0.0007 (6)0.0032 (6)
C110.0307 (8)0.0336 (8)0.0846 (13)0.0199 (7)0.0147 (8)0.0088 (8)
C120.0256 (7)0.0188 (6)0.0289 (7)0.0123 (5)0.0001 (5)0.0003 (5)
C130.0264 (7)0.0204 (7)0.0366 (7)0.0089 (6)0.0018 (6)0.0015 (6)
C140.0381 (8)0.0195 (7)0.0520 (10)0.0124 (6)0.0014 (7)0.0003 (6)
Geometric parameters (Å, º) top
O1—N11.2262 (14)C9—C101.5037 (18)
N1—O21.2255 (14)C9—H9A0.9900
N1—C21.4619 (16)C9—H9B0.9900
C1—C21.3955 (17)C10—C111.523 (2)
C1—C61.4108 (16)C10—H10A0.9900
C1—C71.4361 (18)C10—H10B0.9900
C2—C31.3963 (18)C11—H11A0.9800
O3—C41.3587 (14)C11—H11B0.9800
O3—C91.4476 (15)C11—H11C0.9800
C3—C41.3831 (17)C12—C131.5087 (17)
C3—H30.936 (14)C12—H12A0.9900
O4—C51.3527 (15)C12—H12B0.9900
O4—C121.4422 (14)C13—C141.5191 (19)
C4—C51.4148 (17)C13—H13A0.9900
C5—C61.3796 (17)C13—H13B0.9900
C6—H60.9500C14—H14A0.9800
C7—C81.1862 (19)C14—H14B0.9800
C8—H80.935 (9)C14—H14C0.9800
O2—N1—O1123.12 (11)C9—C10—C11111.07 (12)
O2—N1—C2118.26 (11)C9—C10—H10A109.4
O1—N1—C2118.62 (10)C11—C10—H10A109.4
C2—C1—C6116.55 (11)C9—C10—H10B109.4
C2—C1—C7126.96 (11)C11—C10—H10B109.4
C6—C1—C7116.46 (10)H10A—C10—H10B108.0
C1—C2—C3122.61 (11)C10—C11—H11A109.5
C1—C2—N1120.76 (11)C10—C11—H11B109.5
C3—C2—N1116.62 (11)H11A—C11—H11B109.5
C4—O3—C9117.71 (9)C10—C11—H11C109.5
C4—C3—C2119.58 (11)H11A—C11—H11C109.5
C4—C3—H3120.8 (11)H11B—C11—H11C109.5
C2—C3—H3119.5 (11)O4—C12—C13108.62 (10)
C5—O4—C12116.89 (10)O4—C12—H12A110.0
O3—C4—C3125.21 (11)C13—C12—H12A110.0
O3—C4—C5115.38 (10)O4—C12—H12B110.0
C3—C4—C5119.40 (11)C13—C12—H12B110.0
O4—C5—C6124.60 (11)H12A—C12—H12B108.3
O4—C5—C4115.58 (10)C12—C13—C14109.95 (12)
C6—C5—C4119.82 (11)C12—C13—H13A109.7
C5—C6—C1122.02 (11)C14—C13—H13A109.7
C5—C6—H6119.0C12—C13—H13B109.7
C1—C6—H6119.0C14—C13—H13B109.7
C8—C7—C1170.34 (13)H13A—C13—H13B108.2
C7—C8—H8179.0 (11)C13—C14—H14A109.5
O3—C9—C10107.23 (10)C13—C14—H14B109.5
O3—C9—H9A110.3H14A—C14—H14B109.5
C10—C9—H9A110.3C13—C14—H14C109.5
O3—C9—H9B110.3H14A—C14—H14C109.5
C10—C9—H9B110.3H14B—C14—H14C109.5
H9A—C9—H9B108.5
C3—C2—N1—O217.89 (17)C1—C2—N1—O118.77 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8···O3i0.94 (1)2.48 (1)3.4001 (16)167 (2)
C8—H8···O4i0.94 (1)2.62 (2)3.3267 (16)133 (1)
C3—H3···O2ii0.94 (1)2.61 (1)3.5459 (16)177 (2)
Symmetry codes: (i) y+1/3, x+y+2/3, z+2/3; (ii) x+4/3, y+5/3, z+2/3.
1,2-dibutoxy-4-ethynyl-5-nitrobenzene (2) top
Crystal data top
C16H21NO4F(000) = 624
Mr = 291.34Dx = 1.273 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.5209 (5) ÅCell parameters from 3448 reflections
b = 18.0914 (10) Åθ = 2.3–26.4°
c = 9.9579 (5) ŵ = 0.09 mm1
β = 97.967 (1)°T = 100 K
V = 1520.24 (14) Å3Irregular block, colourless
Z = 40.60 × 0.34 × 0.02 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
3370 independent reflections
Radiation source: fine-focus sealed tube2449 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.047
Detector resolution: 8.3660 pixels mm-1θmax = 27.2°, θmin = 2.3°
φ and ω scansh = 1010
Absorption correction: multi-scan
(SADABS Version 2014; Bruker AXS)
k = 2323
Tmin = 0.682, Tmax = 0.746l = 1212
19579 measured reflections
Refinement top
Refinement on F22 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.041H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.103 w = 1/[σ2(Fo2) + (0.0447P)2 + 0.5063P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
3370 reflectionsΔρmax = 0.25 e Å3
198 parametersΔρmin = 0.18 e Å3
Special details top

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) top
xyzUiso*/Ueq
O10.24462 (15)0.41330 (6)0.09599 (12)0.0331 (3)
N10.22644 (15)0.34657 (7)0.09358 (12)0.0194 (3)
C10.41750 (17)0.33670 (8)0.12054 (14)0.0153 (3)
O20.13376 (14)0.31327 (7)0.17849 (12)0.0335 (3)
C20.31940 (17)0.30296 (8)0.01366 (14)0.0153 (3)
O30.38628 (12)0.10631 (5)0.09739 (10)0.0170 (2)
C30.30591 (17)0.22633 (8)0.00230 (14)0.0156 (3)
H30.2381 (18)0.2081 (9)0.0705 (14)0.019*
H80.4862 (18)0.5273 (7)0.1967 (15)0.019*
O40.57880 (12)0.16462 (5)0.28966 (10)0.0169 (2)
C40.39137 (16)0.18124 (8)0.09726 (14)0.0146 (3)
C50.49571 (16)0.21339 (8)0.20434 (14)0.0145 (3)
C60.50568 (17)0.28947 (8)0.21533 (14)0.0150 (3)
H60.5739380.3105570.2888970.018*
C70.43705 (17)0.41478 (8)0.14269 (14)0.0183 (3)
C80.46506 (19)0.47713 (9)0.17401 (16)0.0227 (3)
C90.27503 (17)0.07150 (8)0.00558 (14)0.0168 (3)
H9A0.3070390.0799900.0961760.020*
H9B0.1679220.0925920.0050090.020*
C100.27354 (17)0.01003 (8)0.02436 (14)0.0167 (3)
H10A0.2367400.0178550.1133190.020*
H10B0.3827130.0296770.0301830.020*
C110.16582 (18)0.05231 (8)0.08441 (15)0.0190 (3)
H11A0.0572990.0317220.0920330.023*
H11B0.2044120.0456220.1729310.023*
C120.16069 (19)0.13435 (8)0.05226 (16)0.0231 (4)
H12A0.2668010.1555710.0502850.035*
H12B0.0869380.1592340.1221240.035*
H12C0.1250190.1411260.0363530.035*
C130.69850 (17)0.19390 (8)0.39333 (14)0.0161 (3)
H13A0.6484030.2244520.4581080.019*
H13B0.7738130.2252620.3516260.019*
C140.78460 (17)0.12937 (8)0.46602 (14)0.0175 (3)
H14A0.8448150.1027350.4028800.021*
H14B0.7064850.0946050.4956580.021*
C150.89834 (18)0.15516 (9)0.58933 (15)0.0200 (3)
H15A0.9745640.1909090.5597220.024*
H15B0.8375350.1808770.6531620.024*
C160.9892 (2)0.09090 (10)0.66219 (17)0.0288 (4)
H16A0.9140860.0554000.6917110.043*
H16B1.0591320.1095110.7413910.043*
H16C1.0527010.0664680.6003320.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0427 (8)0.0206 (7)0.0324 (7)0.0030 (5)0.0069 (6)0.0077 (5)
N10.0194 (7)0.0200 (7)0.0184 (7)0.0039 (5)0.0015 (5)0.0017 (5)
C10.0153 (7)0.0148 (7)0.0164 (7)0.0001 (6)0.0039 (6)0.0014 (6)
O20.0371 (7)0.0301 (7)0.0271 (6)0.0032 (5)0.0167 (5)0.0001 (5)
C20.0147 (7)0.0178 (8)0.0136 (7)0.0037 (6)0.0021 (6)0.0032 (6)
O30.0199 (5)0.0123 (5)0.0169 (5)0.0012 (4)0.0043 (4)0.0008 (4)
C30.0132 (7)0.0193 (8)0.0137 (7)0.0004 (6)0.0002 (6)0.0016 (6)
O40.0198 (5)0.0130 (5)0.0155 (5)0.0010 (4)0.0060 (4)0.0011 (4)
C40.0137 (7)0.0159 (7)0.0145 (7)0.0001 (6)0.0022 (5)0.0002 (6)
C50.0139 (7)0.0163 (7)0.0128 (7)0.0015 (6)0.0006 (5)0.0021 (6)
C60.0138 (7)0.0181 (8)0.0130 (7)0.0011 (6)0.0008 (5)0.0010 (6)
C70.0179 (8)0.0208 (8)0.0156 (7)0.0029 (6)0.0006 (6)0.0035 (6)
C80.0261 (9)0.0172 (8)0.0235 (8)0.0015 (7)0.0016 (6)0.0026 (7)
C90.0152 (7)0.0184 (8)0.0152 (7)0.0011 (6)0.0032 (6)0.0015 (6)
C100.0152 (7)0.0165 (8)0.0172 (7)0.0002 (6)0.0018 (6)0.0001 (6)
C110.0207 (8)0.0163 (8)0.0186 (7)0.0000 (6)0.0022 (6)0.0018 (6)
C120.0237 (8)0.0184 (8)0.0257 (8)0.0008 (6)0.0026 (7)0.0012 (7)
C130.0167 (7)0.0161 (7)0.0143 (7)0.0031 (6)0.0025 (6)0.0010 (6)
C140.0190 (8)0.0166 (8)0.0156 (7)0.0005 (6)0.0022 (6)0.0006 (6)
C150.0183 (7)0.0249 (9)0.0154 (7)0.0026 (6)0.0029 (6)0.0007 (6)
C160.0256 (9)0.0363 (10)0.0220 (8)0.0039 (7)0.0056 (7)0.0075 (7)
Geometric parameters (Å, º) top
O1—N11.2178 (16)C10—C111.5248 (19)
N1—O21.2314 (16)C10—H10A0.9900
N1—C21.4683 (18)C10—H10B0.9900
C1—C21.399 (2)C11—C121.520 (2)
C1—C61.4103 (19)C11—H11A0.9900
C1—C71.436 (2)C11—H11B0.9900
C2—C31.394 (2)C12—H12A0.9800
O3—C41.3564 (17)C12—H12B0.9800
O3—C91.4412 (16)C12—H12C0.9800
C3—C41.378 (2)C13—C141.509 (2)
C3—H30.923 (13)C13—H13A0.9900
O4—C51.3546 (16)C13—H13B0.9900
O4—C131.4473 (16)C14—C151.5281 (19)
C4—C51.4152 (19)C14—H14A0.9900
C5—C61.382 (2)C14—H14B0.9900
C6—H60.9500C15—C161.524 (2)
C7—C81.186 (2)C15—H15A0.9900
C8—H80.947 (13)C15—H15B0.9900
C9—C101.505 (2)C16—H16A0.9800
C9—H9A0.9900C16—H16B0.9800
C9—H9B0.9900C16—H16C0.9800
O1—N1—O2122.87 (13)C12—C11—C10111.85 (12)
O1—N1—C2119.33 (12)C12—C11—H11A109.2
O2—N1—C2117.80 (12)C10—C11—H11A109.2
C2—C1—C6116.84 (13)C12—C11—H11B109.2
C2—C1—C7126.19 (13)C10—C11—H11B109.2
C6—C1—C7116.97 (13)H11A—C11—H11B107.9
C3—C2—C1121.96 (13)C11—C12—H12A109.5
C3—C2—N1116.44 (13)C11—C12—H12B109.5
C1—C2—N1121.60 (13)H12A—C12—H12B109.5
C4—O3—C9117.00 (11)C11—C12—H12C109.5
C4—C3—C2120.21 (13)H12A—C12—H12C109.5
C4—C3—H3122.8 (10)H12B—C12—H12C109.5
C2—C3—H3117.0 (10)O4—C13—C14107.86 (11)
C5—O4—C13117.67 (11)O4—C13—H13A110.1
O3—C4—C3125.34 (13)C14—C13—H13A110.1
O3—C4—C5115.27 (12)O4—C13—H13B110.1
C3—C4—C5119.39 (13)C14—C13—H13B110.1
O4—C5—C6125.30 (13)H13A—C13—H13B108.4
O4—C5—C4115.09 (12)C13—C14—C15111.17 (12)
C6—C5—C4119.61 (13)C13—C14—H14A109.4
C5—C6—C1121.94 (13)C15—C14—H14A109.4
C5—C6—H6119.0C13—C14—H14B109.4
C1—C6—H6119.0C15—C14—H14B109.4
C8—C7—C1172.37 (16)H14A—C14—H14B108.0
C7—C8—H8178.5 (10)C16—C15—C14111.92 (13)
O3—C9—C10108.06 (11)C16—C15—H15A109.2
O3—C9—H9A110.1C14—C15—H15A109.2
C10—C9—H9A110.1C16—C15—H15B109.2
O3—C9—H9B110.1C14—C15—H15B109.2
C10—C9—H9B110.1H15A—C15—H15B107.9
H9A—C9—H9B108.4C15—C16—H16A109.5
C9—C10—C11111.82 (12)C15—C16—H16B109.5
C9—C10—H10A109.3H16A—C16—H16B109.5
C11—C10—H10A109.3C15—C16—H16C109.5
C9—C10—H10B109.3H16A—C16—H16C109.5
C11—C10—H10B109.3H16B—C16—H16C109.5
H10A—C10—H10B107.9
C1—C2—N1—O16.1 (2)C3—C2—N1—O26.1 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8···O3i0.95 (1)2.61 (1)3.3835 (19)139 (1)
C8—H8···O4i0.95 (1)2.55 (1)3.4371 (19)156 (1)
Symmetry code: (i) x+1, y+1/2, z+1/2.
(3) top
Crystal data top
C18H25NO4Z = 2
Mr = 319.39F(000) = 344
Triclinic, P1Dx = 1.181 Mg m3
a = 4.570 (4) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.415 (8) ÅCell parameters from 852 reflections
c = 20.968 (18) Åθ = 2.3–25.6°
α = 94.003 (12)°µ = 0.08 mm1
β = 90.758 (12)°T = 100 K
γ = 93.435 (11)°Square, colourless
V = 898.2 (14) Å30.46 × 0.14 × 0.14 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
2914 independent reflections
Radiation source: fine-focus sealed tube1604 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.055
Detector resolution: 8.3660 pixels mm-1θmax = 24.4°, θmin = 2.0°
φ and ω scansh = 55
Absorption correction: multi-scan
(SADABS Version 2014; Bruker AXS)
k = 1010
Tmin = 0.382, Tmax = 0.746l = 2423
5380 measured reflections
Refinement top
Refinement on F22 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.085H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.262 w = 1/[σ2(Fo2) + (0.1254P)2 + 0.8636P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
2914 reflectionsΔρmax = 0.36 e Å3
216 parametersΔρmin = 0.32 e Å3
Special details top

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) top
xyzUiso*/Ueq
O10.5970 (9)0.2146 (5)0.48201 (18)0.0588 (11)
N10.4403 (9)0.2986 (5)0.5092 (2)0.0370 (10)
C10.6541 (10)0.2513 (5)0.6159 (2)0.0315 (12)
O20.2526 (9)0.3609 (5)0.48100 (18)0.0590 (12)
C20.4709 (10)0.3307 (5)0.5786 (2)0.0295 (11)
O30.1873 (6)0.5814 (3)0.70199 (15)0.0326 (8)
C30.3139 (10)0.4410 (5)0.6053 (2)0.0298 (11)
O40.5189 (7)0.4440 (3)0.77303 (15)0.0345 (9)
C40.3319 (9)0.4762 (5)0.6707 (2)0.0266 (11)
C50.5148 (9)0.4001 (5)0.7095 (2)0.0290 (11)
C60.6704 (10)0.2917 (5)0.6818 (2)0.0310 (11)
H60.7936560.2421290.7083110.037*
C70.8201 (11)0.1340 (5)0.5926 (2)0.0363 (12)
C80.9653 (13)0.0361 (6)0.5791 (3)0.0473 (14)
C90.0258 (10)0.6727 (5)0.6633 (2)0.0330 (12)
H9A0.1226400.6150290.6362020.040*
H9B0.1607890.7243630.6350960.040*
C100.1205 (10)0.7763 (5)0.7078 (2)0.0345 (12)
H10A0.2490330.7218450.7363090.041*
H10B0.2474280.8332810.6822800.041*
C110.0872 (10)0.8788 (5)0.7493 (2)0.0379 (13)
H11A0.2243400.8226070.7726830.045*
H11B0.2045920.9394630.7212300.045*
C120.0696 (10)0.9732 (5)0.7969 (3)0.0406 (13)
H12A0.1848910.9123510.8252900.049*
H12B0.2089571.0281170.7735040.049*
C130.1374 (13)1.0785 (6)0.8384 (3)0.0603 (17)
H13A0.2752221.0251100.8620820.090*
H13B0.0218801.1351810.8685960.090*
H13C0.2465991.1419960.8108420.090*
C140.7373 (11)0.3898 (5)0.8135 (2)0.0354 (12)
H14A0.9362320.4189350.7991720.043*
H14B0.7165490.2842820.8114630.043*
C150.6920 (12)0.4506 (5)0.8810 (2)0.0420 (13)
H15A0.8286650.4076400.9100640.050*
H15B0.4898580.4229030.8937160.050*
C160.7393 (14)0.6118 (6)0.8896 (3)0.0523 (16)
H16A0.6061040.6553300.8599210.063*
H16B0.9432330.6399250.8782410.063*
C170.6833 (16)0.6703 (6)0.9585 (3)0.0654 (18)
H17A0.4799850.6408690.9697870.078*
H17B0.8172750.6266390.9879400.078*
C180.726 (2)0.8298 (8)0.9686 (3)0.111 (3)
H18A0.9281280.8599640.9585650.167*
H18B0.6875680.8593771.0133370.167*
H18C0.5901640.8741820.9406280.167*
H30.187 (15)0.483 (8)0.578 (3)0.133*
H81.065 (17)0.045 (6)0.564 (4)0.133*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.069 (3)0.063 (3)0.044 (2)0.018 (2)0.000 (2)0.006 (2)
N10.035 (2)0.031 (2)0.043 (3)0.010 (2)0.003 (2)0.003 (2)
C10.028 (3)0.029 (3)0.036 (3)0.012 (2)0.003 (2)0.002 (2)
O20.068 (3)0.067 (3)0.041 (2)0.005 (2)0.013 (2)0.002 (2)
C20.028 (3)0.026 (3)0.033 (3)0.013 (2)0.002 (2)0.003 (2)
O30.0285 (18)0.0289 (18)0.040 (2)0.0013 (14)0.0064 (14)0.0051 (15)
C30.024 (2)0.026 (3)0.038 (3)0.011 (2)0.004 (2)0.006 (2)
O40.0329 (18)0.037 (2)0.0327 (19)0.0043 (15)0.0057 (14)0.0033 (15)
C40.022 (2)0.020 (2)0.037 (3)0.0078 (19)0.002 (2)0.005 (2)
C50.023 (2)0.027 (3)0.036 (3)0.011 (2)0.002 (2)0.005 (2)
C60.025 (3)0.027 (3)0.040 (3)0.007 (2)0.004 (2)0.006 (2)
C70.037 (3)0.029 (3)0.041 (3)0.010 (2)0.001 (2)0.001 (2)
C80.061 (4)0.039 (3)0.041 (3)0.003 (3)0.002 (3)0.001 (3)
C90.023 (2)0.032 (3)0.044 (3)0.003 (2)0.003 (2)0.007 (2)
C100.025 (3)0.029 (3)0.050 (3)0.003 (2)0.002 (2)0.012 (2)
C110.030 (3)0.030 (3)0.054 (3)0.002 (2)0.000 (2)0.007 (2)
C120.032 (3)0.030 (3)0.060 (3)0.001 (2)0.002 (2)0.009 (2)
C130.053 (4)0.045 (4)0.080 (4)0.001 (3)0.010 (3)0.010 (3)
C140.037 (3)0.032 (3)0.037 (3)0.005 (2)0.007 (2)0.008 (2)
C150.048 (3)0.042 (3)0.035 (3)0.009 (2)0.005 (2)0.007 (2)
C160.069 (4)0.042 (3)0.044 (3)0.014 (3)0.007 (3)0.001 (3)
C170.096 (5)0.052 (4)0.047 (4)0.002 (4)0.008 (3)0.005 (3)
C180.210 (11)0.063 (5)0.057 (5)0.001 (6)0.002 (5)0.013 (4)
Geometric parameters (Å, º) top
O1—N11.215 (5)C11—C121.507 (7)
N1—O21.234 (5)C11—H11A0.9900
N1—C21.469 (6)C11—H11B0.9900
C1—C61.408 (6)C12—C131.542 (7)
C1—C21.418 (7)C12—H12A0.9900
C1—C71.438 (7)C12—H12B0.9900
C2—C31.388 (7)C13—H13A0.9800
O3—C41.359 (5)C13—H13B0.9800
O3—C91.449 (5)C13—H13C0.9800
C3—C41.388 (7)C14—C151.511 (7)
C3—H30.93 (2)C14—H14A0.9900
O4—C51.366 (5)C14—H14B0.9900
O4—C141.440 (6)C15—C161.518 (7)
C4—C51.417 (6)C15—H15A0.9900
C5—C61.379 (6)C15—H15B0.9900
C6—H60.9500C16—C171.540 (8)
C7—C81.188 (7)C16—H16A0.9900
C8—H80.95 (2)C16—H16B0.9900
C9—C101.496 (6)C17—C181.503 (9)
C9—H9A0.9900C17—H17A0.9900
C9—H9B0.9900C17—H17B0.9900
C10—C111.529 (6)C18—H18A0.9800
C10—H10A0.9900C18—H18B0.9800
C10—H10B0.9900C18—H18C0.9800
O1—N1—O2123.0 (4)C11—C12—C13113.8 (4)
O1—N1—C2120.1 (4)C11—C12—H12A108.8
O2—N1—C2116.9 (4)C13—C12—H12A108.8
C6—C1—C2116.1 (4)C11—C12—H12B108.8
C6—C1—C7117.8 (5)C13—C12—H12B108.8
C2—C1—C7126.1 (4)H12A—C12—H12B107.7
C3—C2—C1122.2 (4)C12—C13—H13A109.5
C3—C2—N1117.1 (4)C12—C13—H13B109.5
C1—C2—N1120.7 (4)H13A—C13—H13B109.5
C4—O3—C9117.2 (4)C12—C13—H13C109.5
C2—C3—C4120.0 (4)H13A—C13—H13C109.5
C2—C3—H3117 (5)H13B—C13—H13C109.5
C4—C3—H3123 (5)O4—C14—C15107.7 (4)
C5—O4—C14117.8 (4)O4—C14—H14A110.2
O3—C4—C3125.0 (4)C15—C14—H14A110.2
O3—C4—C5115.5 (4)O4—C14—H14B110.2
C3—C4—C5119.4 (4)C15—C14—H14B110.2
O4—C5—C6125.7 (4)H14A—C14—H14B108.5
O4—C5—C4114.8 (4)C14—C15—C16113.9 (4)
C6—C5—C4119.5 (4)C14—C15—H15A108.8
C5—C6—C1122.7 (5)C16—C15—H15A108.8
C5—C6—H6118.7C14—C15—H15B108.8
C1—C6—H6118.7C16—C15—H15B108.8
C8—C7—C1173.9 (6)H15A—C15—H15B107.7
C7—C8—H8173 (5)C15—C16—C17112.4 (5)
O3—C9—C10107.5 (4)C15—C16—H16A109.1
O3—C9—H9A110.2C17—C16—H16A109.1
C10—C9—H9A110.2C15—C16—H16B109.1
O3—C9—H9B110.2C17—C16—H16B109.1
C10—C9—H9B110.2H16A—C16—H16B107.8
H9A—C9—H9B108.5C18—C17—C16113.9 (6)
C9—C10—C11115.2 (4)C18—C17—H17A108.8
C9—C10—H10A108.5C16—C17—H17A108.8
C11—C10—H10A108.5C18—C17—H17B108.8
C9—C10—H10B108.5C16—C17—H17B108.8
C11—C10—H10B108.5H17A—C17—H17B107.7
H10A—C10—H10B107.5C17—C18—H18A109.5
C12—C11—C10113.3 (4)C17—C18—H18B109.5
C12—C11—H11A108.9H18A—C18—H18B109.5
C10—C11—H11A108.9C17—C18—H18C109.5
C12—C11—H11B108.9H18A—C18—H18C109.5
C10—C11—H11B108.9H18B—C18—H18C109.5
H11A—C11—H11B107.7
C1—C2—N1—O18.4 (6)C3—C2—N1—O28.0 (6)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O2i0.93 (2)2.88 (3)3.793 (7)167 (7)
C9—H9A···O2i0.992.553.254 (7)128
C8—H8···O1ii0.95 (2)2.45 (3)3.381 (8)167 (8)
Symmetry codes: (i) x, y+1, z+1; (ii) x+2, y, z+1.
 

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