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2,4-Di­nitro-N-(2-phenyl­ethyl)aniline, C14H13N3O4, (I), crystallizes with one independent mol­ecule in the asymmetric unit. The adjacent amine and nitro groups form an intra­molecular N—H...O hydrogen bond. The anti conformation about the ethyl C—C bond leads to the phenyl and aniline rings being essentially parallel. Mol­ecules are linked into dimers by inter­molecular N—H...O hydrogen bonds, such that each amine H atom participates in a three-centre inter­action with two nitro O atoms. Though the dimers pack so that the arene rings of adjacent mol­ecules are parallel, the rings are staggered and π–π inter­actions do not appear to be favoured. 4,6-Di­nitro-N,N′-bis­(2-phenyl­ethyl)benzene-1,3-di­amine, C22H22N4O4, (II), differs from (I) in the presence of a second 2-phenyl­ethyl­amine group on the substituted ring. Compound (II) also crystallizes with one unique mol­ecule in the asymmetric unit. Both amine groups are involved in intra­molecular N—H...O hydrogen bonds with adjacent nitro groups. Although one ethyl group adopts an anti conformation as in (I), the other is gauche, with the result that the pendant phenyl rings are not parallel. The amine group that is part of the gauche conformation participates in a three-centre N—H...O hydrogen bond with the nitro group of a neighbouring mol­ecule, leading to dimers as in (I). The other amine H atom does not form any inter­molecular hydrogen bonds. The packing leads to separations of ca 3.4 Å of the parallel anti phenyl and amino­benzene rings. 2-Cyano-4-nitro-N-(2-phenyl­ethyl)aniline, C15H13N3O2, (III), differs from (I) only in having a cyano group in place of the 2-nitro group. The absence of the adjacent nitro group eliminates the intra­molecular N—H...O hydrogen bond. Mol­ecules of (III) adopt the same anti conformation about the ethyl group as in (I), but crystallize in the higher-symmetry monoclinic space group P21/n. The mol­ecules are linked into dimers via N—H...N amine–cyano hydrogen bonds, while the nitro groups are not involved in any N—H...O inter­actions. Owing to the different symmetry, the mol­ecules pack in a herringbone pattern with fewer face-to-face inter­actions between the rings. The closest such inter­actions are about 3.5 Å between rings that are largely slipped past one another. 4-Methyl­sulfonyl-2-nitro-N-(2-phenyl­ethyl)aniline, C15H16N2O4S, (IV), differs from (I) in having a methyl­sulfonyl group in place of the 4-nitro group. The intra­molecular N—H...O hydrogen bond is present as in (I). However, unlike (I), the conformation about the ethyl group is gauche, so the two arene rings are nearly per­pen­dicular rather than parallel. The packing is significantly different from the other three structures in that there are no inter­molecular hydrogen bonds involving the N—H groups. The mol­ecules are arranged in tetra­gonal columns running along the c axis, with the aniline rings mostly parallel and separated by ca 3.7 Å. Taken together, these structures demonstrate that modest changes in functional groups cause significant differences in mol­ecular conformation, inter­molecular inter­actions and packing.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270113025869/cu3041sup1.cif
Contains datablocks C14H13N3O4, C22H22N4O4, C15H13N3O2, C15H16N2O4S, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025869/cu3041C14H13N3O4sup2.hkl
Contains datablock C14H13N3O4

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025869/cu3041C22H22N4O4sup3.hkl
Contains datablock C22H22N4O4

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025869/cu3041C15H13N3O2sup4.hkl
Contains datablock C15H13N3O2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025869/cu3041C15H16N2O4Ssup5.hkl
Contains datablock C15H16N2O4S

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025869/cu3041C14H13N3O4sup6.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025869/cu3041C22H22N4O4sup7.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025869/cu3041C15H13N3O2sup8.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025869/cu3041C15H16N2O4Ssup9.cml
Supplementary material

CCDC references: 961994; 961995; 961996; 961997

Computing details top

For all compounds, data collection: APEX2 (Bruker, 2005); cell refinement: APEX2 (Bruker, 2005); data reduction: APEX2 (Bruker, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: CrystalMaker (Palmer, 2013); software used to prepare material for publication: APEX2 (Bruker, 2005).

(C14H13N3O4) 2,4-Dinitro-N-(2-phenylethyl)aniline top
Crystal data top
C14H13N3O4Z = 2
Mr = 287.27F(000) = 300
Triclinic, P1Dx = 1.459 Mg m3
Hall symbol: -P 1Melting point: 425 K
a = 7.235 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.282 (2) ÅCell parameters from 11611 reflections
c = 13.512 (4) Åθ = 3.0–32.1°
α = 88.714 (5)°µ = 0.11 mm1
β = 85.131 (5)°T = 100 K
γ = 67.239 (5)°Plate, orange
V = 654.0 (4) Å30.20 × 0.10 × 0.02 mm
Data collection top
Bruker APEX DUO CCD area-detector
diffractometer
3158 independent reflections
Radiation source: sealed tube2288 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.027
ω scansθmax = 28.0°, θmin = 3.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 99
Tmin = 0.978, Tmax = 0.998k = 99
9039 measured reflectionsl = 1717
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.040Hydrogen site location: difference Fourier map
wR(F2) = 0.104All H-atom parameters refined
S = 1.03 w = 1/[σ2(Fo2) + (0.0523P)2 + 0.1059P]
where P = (Fo2 + 2Fc2)/3
3158 reflections(Δ/σ)max < 0.001
242 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = 0.26 e Å3
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.

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) top
xyzUiso*/Ueq
O210.47421 (16)0.19492 (14)0.46231 (7)0.0226 (3)
O220.30058 (15)0.48827 (14)0.40811 (8)0.0218 (2)
O410.35861 (18)0.39571 (17)0.04202 (8)0.0288 (3)
O420.17704 (17)0.61028 (16)0.07262 (8)0.0304 (3)
N10.69604 (18)0.09321 (17)0.33654 (9)0.0162 (3)
H10.654 (3)0.062 (3)0.3982 (14)0.032 (5)*
N20.41095 (17)0.31155 (16)0.39279 (8)0.0150 (3)
N40.31213 (19)0.44961 (18)0.04614 (9)0.0212 (3)
C10.61056 (19)0.04072 (19)0.26771 (10)0.0137 (3)
C20.46755 (19)0.23875 (19)0.29173 (10)0.0132 (3)
C30.3740 (2)0.3712 (2)0.21903 (10)0.0141 (3)
H30.280 (2)0.497 (2)0.2391 (11)0.018 (4)*
C40.4213 (2)0.3149 (2)0.12088 (10)0.0166 (3)
C50.5681 (2)0.1266 (2)0.09314 (11)0.0179 (3)
H50.599 (2)0.092 (2)0.0257 (13)0.021 (4)*
C60.6582 (2)0.0059 (2)0.16413 (11)0.0167 (3)
H60.756 (3)0.133 (3)0.1449 (13)0.027 (4)*
C70.8410 (2)0.2971 (2)0.31717 (12)0.0178 (3)
H7A0.932 (2)0.299 (2)0.2580 (12)0.018 (4)*
H7B0.920 (2)0.336 (2)0.3754 (12)0.021 (4)*
C80.7394 (2)0.4436 (2)0.30299 (12)0.0169 (3)
H8B0.641 (2)0.429 (2)0.3592 (12)0.015 (4)*
H8A0.662 (2)0.411 (2)0.2453 (12)0.014 (4)*
C90.8931 (2)0.65607 (19)0.29443 (10)0.0151 (3)
C100.9689 (2)0.7611 (2)0.37972 (11)0.0185 (3)
H100.917 (2)0.699 (2)0.4453 (13)0.025 (4)*
C111.1134 (2)0.9552 (2)0.37235 (13)0.0221 (3)
H111.161 (3)1.025 (3)0.4326 (14)0.034 (5)*
C121.1825 (2)1.0461 (2)0.27972 (13)0.0237 (3)
H121.277 (3)1.178 (3)0.2770 (12)0.026 (4)*
C131.1069 (2)0.9442 (2)0.19510 (12)0.0225 (3)
H131.155 (3)1.014 (3)0.1310 (14)0.031 (5)*
C140.9635 (2)0.7496 (2)0.20191 (11)0.0182 (3)
H140.914 (2)0.682 (2)0.1425 (13)0.025 (4)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O210.0317 (6)0.0159 (5)0.0157 (5)0.0043 (4)0.0026 (4)0.0024 (4)
O220.0234 (6)0.0124 (5)0.0224 (5)0.0007 (4)0.0012 (4)0.0048 (4)
O410.0441 (7)0.0303 (6)0.0144 (5)0.0161 (5)0.0063 (5)0.0025 (4)
O420.0346 (7)0.0196 (6)0.0282 (6)0.0002 (5)0.0069 (5)0.0043 (5)
N10.0168 (6)0.0101 (6)0.0190 (6)0.0023 (5)0.0014 (5)0.0008 (5)
N20.0154 (6)0.0131 (6)0.0154 (6)0.0046 (5)0.0004 (5)0.0009 (5)
N40.0282 (7)0.0195 (7)0.0180 (6)0.0109 (6)0.0052 (5)0.0036 (5)
C10.0113 (6)0.0122 (6)0.0191 (7)0.0061 (5)0.0008 (5)0.0012 (5)
C20.0140 (7)0.0112 (6)0.0143 (7)0.0050 (5)0.0010 (5)0.0027 (5)
C30.0129 (6)0.0108 (6)0.0186 (7)0.0047 (5)0.0002 (5)0.0014 (5)
C40.0182 (7)0.0151 (7)0.0180 (7)0.0080 (6)0.0021 (6)0.0020 (5)
C50.0217 (7)0.0183 (7)0.0155 (7)0.0104 (6)0.0029 (6)0.0045 (6)
C60.0152 (7)0.0127 (7)0.0214 (7)0.0049 (6)0.0028 (6)0.0047 (5)
C70.0135 (7)0.0108 (7)0.0263 (8)0.0011 (5)0.0042 (6)0.0003 (6)
C80.0130 (7)0.0121 (7)0.0235 (8)0.0024 (5)0.0018 (6)0.0014 (5)
C90.0119 (6)0.0126 (7)0.0214 (7)0.0055 (5)0.0002 (5)0.0017 (5)
C100.0188 (7)0.0167 (7)0.0203 (8)0.0077 (6)0.0003 (6)0.0010 (6)
C110.0190 (8)0.0156 (7)0.0326 (9)0.0073 (6)0.0052 (6)0.0062 (6)
C120.0138 (7)0.0110 (7)0.0451 (10)0.0040 (6)0.0009 (6)0.0032 (6)
C130.0172 (7)0.0196 (7)0.0311 (9)0.0088 (6)0.0068 (6)0.0120 (6)
C140.0177 (7)0.0188 (7)0.0200 (7)0.0091 (6)0.0007 (6)0.0021 (6)
Geometric parameters (Å, º) top
O21—N21.2448 (15)C7—C81.534 (2)
O22—N21.2350 (14)C7—H7A0.989 (16)
O41—N41.2398 (16)C7—H7B0.984 (16)
O42—N41.2356 (16)C8—C91.5161 (19)
N1—C11.3374 (18)C8—H8B0.974 (16)
N1—C71.4622 (17)C8—H8A0.967 (16)
N1—H10.867 (19)C9—C141.396 (2)
N2—C21.4433 (17)C9—C101.399 (2)
N4—C41.4482 (18)C10—C111.395 (2)
C1—C61.429 (2)C10—H100.980 (17)
C1—C21.4369 (18)C11—C121.389 (2)
C2—C31.3850 (19)C11—H110.966 (19)
C3—C41.372 (2)C12—C131.382 (2)
C3—H30.932 (16)C12—H120.938 (17)
C4—C51.406 (2)C13—C141.395 (2)
C5—C61.362 (2)C13—H130.979 (18)
C5—H50.937 (17)C14—H140.955 (17)
C6—H60.948 (17)
C1—N1—C7125.87 (13)C8—C7—H7A110.3 (9)
C1—N1—H1117.6 (12)N1—C7—H7B106.3 (9)
C7—N1—H1116.2 (12)C8—C7—H7B109.5 (9)
O22—N2—O21121.63 (11)H7A—C7—H7B108.7 (13)
O22—N2—C2119.07 (11)C9—C8—C7111.05 (11)
O21—N2—C2119.30 (11)C9—C8—H8B110.6 (9)
O42—N4—O41123.20 (12)C7—C8—H8B108.5 (9)
O42—N4—C4119.13 (12)C9—C8—H8A110.1 (9)
O41—N4—C4117.66 (12)C7—C8—H8A111.3 (9)
N1—C1—C6121.24 (12)H8B—C8—H8A105.1 (12)
N1—C1—C2123.14 (12)C14—C9—C10118.80 (13)
C6—C1—C2115.62 (12)C14—C9—C8120.97 (13)
C3—C2—C1121.89 (12)C10—C9—C8120.23 (13)
C3—C2—N2115.84 (11)C11—C10—C9120.58 (14)
C1—C2—N2122.28 (12)C11—C10—H10119.7 (10)
C4—C3—C2119.61 (12)C9—C10—H10119.7 (10)
C4—C3—H3122.3 (9)C12—C11—C10119.96 (15)
C2—C3—H3118.1 (9)C12—C11—H11121.3 (11)
C3—C4—C5120.74 (13)C10—C11—H11118.7 (11)
C3—C4—N4118.95 (12)C13—C12—C11119.87 (14)
C5—C4—N4120.27 (12)C13—C12—H12121.9 (11)
C6—C5—C4120.01 (13)C11—C12—H12118.2 (11)
C6—C5—H5120.6 (10)C12—C13—C14120.46 (14)
C4—C5—H5119.3 (10)C12—C13—H13118.1 (10)
C5—C6—C1122.00 (13)C14—C13—H13121.4 (10)
C5—C6—H6119.6 (10)C13—C14—C9120.33 (14)
C1—C6—H6118.4 (10)C13—C14—H14119.1 (10)
N1—C7—C8112.67 (12)C9—C14—H14120.6 (10)
N1—C7—H7A109.2 (9)
C7—N1—C1—C60.9 (2)C3—C4—C5—C63.2 (2)
C7—N1—C1—C2179.47 (12)N4—C4—C5—C6174.48 (13)
N1—C1—C2—C3176.80 (13)C4—C5—C6—C10.9 (2)
C6—C1—C2—C33.52 (19)N1—C1—C6—C5177.98 (13)
N1—C1—C2—N22.6 (2)C2—C1—C6—C52.33 (19)
C6—C1—C2—N2177.05 (12)C1—N1—C7—C885.52 (17)
O22—N2—C2—C36.70 (18)N1—C7—C8—C9173.75 (12)
O21—N2—C2—C3173.22 (12)C7—C8—C9—C1499.44 (16)
O22—N2—C2—C1173.85 (12)C7—C8—C9—C1079.65 (16)
O21—N2—C2—C16.24 (18)C14—C9—C10—C110.4 (2)
C1—C2—C3—C41.4 (2)C8—C9—C10—C11178.69 (13)
N2—C2—C3—C4179.12 (12)C9—C10—C11—C120.2 (2)
C2—C3—C4—C52.0 (2)C10—C11—C12—C130.4 (2)
C2—C3—C4—N4175.69 (12)C11—C12—C13—C140.9 (2)
O42—N4—C4—C31.2 (2)C12—C13—C14—C90.7 (2)
O41—N4—C4—C3179.53 (13)C10—C9—C14—C130.0 (2)
O42—N4—C4—C5176.52 (13)C8—C9—C14—C13179.15 (13)
O41—N4—C4—C52.7 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O210.867 (19)1.983 (19)2.6377 (16)131.5 (16)
N1—H1···O21i0.867 (19)2.381 (19)3.0823 (18)138.3 (16)
Symmetry code: (i) x+1, y, z+1.
(C22H22N4O4) 4,6-Dinitro-N,N'-bis(2-phenylethyl)benzene-1,3-diamine top
Crystal data top
C22H22N4O4Z = 2
Mr = 406.44F(000) = 428
Triclinic, P1Dx = 1.378 Mg m3
Hall symbol: -P 1Melting point: 408 K
a = 8.1121 (7) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.1819 (8) ÅCell parameters from 17364 reflections
c = 13.1018 (11) Åθ = 2.5–32.7°
α = 93.466 (1)°µ = 0.10 mm1
β = 106.595 (1)°T = 100 K
γ = 106.932 (1)°Parallelpiped, orange
V = 979.88 (14) Å30.20 × 0.10 × 0.05 mm
Data collection top
Bruker APEX DUO CCD area-detector
diffractometer
6868 independent reflections
Radiation source: sealed tube5289 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
ω scansθmax = 33.0°, θmin = 1.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1212
Tmin = 0.981, Tmax = 0.995k = 1515
17364 measured reflectionsl = 1919
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: difference Fourier map
wR(F2) = 0.121All H-atom parameters refined
S = 1.03 w = 1/[σ2(Fo2) + (0.0693P)2 + 0.148P]
where P = (Fo2 + 2Fc2)/3
6868 reflections(Δ/σ)max = 0.001
359 parametersΔρmax = 0.57 e Å3
0 restraintsΔρmin = 0.21 e Å3
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.

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) top
xyzUiso*/Ueq
O210.23044 (11)0.49365 (8)0.03714 (6)0.02254 (17)
O220.20579 (10)0.44974 (8)0.11874 (6)0.02074 (16)
O410.80203 (11)0.91022 (8)0.45448 (6)0.02101 (16)
O420.57135 (10)0.72779 (8)0.43962 (6)0.02098 (16)
N10.51043 (11)0.69381 (9)0.05088 (6)0.01446 (15)
H10.410 (2)0.6227 (15)0.0847 (12)0.029 (4)*
N20.28480 (11)0.52119 (8)0.06328 (7)0.01512 (16)
N40.67006 (11)0.80913 (9)0.39872 (6)0.01476 (16)
N50.86876 (11)1.00007 (8)0.28122 (7)0.01354 (15)
H50.905 (2)1.0156 (17)0.3538 (14)0.039 (4)*
C10.54668 (12)0.72552 (9)0.05682 (7)0.01225 (16)
C20.44289 (12)0.63957 (9)0.11528 (7)0.01285 (16)
C30.48939 (12)0.67177 (9)0.22604 (7)0.01303 (16)
H30.4177 (19)0.6132 (15)0.2631 (11)0.026 (4)*
C40.63377 (12)0.78684 (9)0.28394 (7)0.01247 (16)
C50.73706 (12)0.88063 (9)0.22938 (7)0.01228 (16)
C60.69047 (12)0.84309 (9)0.11745 (7)0.01281 (16)
H60.7613 (18)0.9005 (14)0.0809 (11)0.020 (3)*
C70.60110 (13)0.78288 (10)0.11463 (8)0.01417 (17)
H7A0.5825 (17)0.7264 (13)0.1818 (10)0.015 (3)*
H7B0.7300 (18)0.8193 (13)0.0770 (10)0.017 (3)*
C80.52363 (14)0.90188 (11)0.14096 (8)0.01701 (18)
H8B0.5228 (19)0.9459 (15)0.0728 (12)0.025 (4)*
H8A0.396 (2)0.8610 (15)0.1902 (12)0.027 (4)*
C90.63215 (12)1.00500 (10)0.19438 (7)0.01360 (17)
C100.59759 (13)0.98259 (10)0.30591 (8)0.01541 (17)
H100.501 (2)0.9015 (16)0.3492 (12)0.029 (4)*
C110.70127 (14)1.07599 (11)0.35487 (8)0.01895 (19)
H110.677 (2)1.0608 (16)0.4351 (13)0.032 (4)*
C120.84093 (14)1.19286 (11)0.29268 (9)0.0209 (2)
H120.915 (2)1.2594 (18)0.3244 (14)0.042 (4)*
C130.87739 (14)1.21631 (11)0.18180 (9)0.0208 (2)
H130.974 (2)1.2986 (18)0.1407 (14)0.039 (4)*
C140.77321 (14)1.12241 (10)0.13291 (8)0.01714 (18)
H140.796 (2)1.1411 (16)0.0549 (13)0.031 (4)*
C150.97367 (13)1.09930 (10)0.22897 (8)0.01359 (16)
H15A1.0524 (17)1.0589 (13)0.2021 (10)0.013 (3)*
H15B0.8901 (18)1.1204 (14)0.1646 (11)0.019 (3)*
C161.08512 (12)1.23457 (10)0.30761 (8)0.01436 (17)
H16B1.1659 (18)1.2924 (14)0.2730 (11)0.021 (3)*
H16A1.1643 (18)1.2117 (14)0.3725 (11)0.022 (3)*
C170.96790 (12)1.31233 (9)0.33662 (7)0.01351 (17)
C180.90244 (13)1.28766 (10)0.42395 (8)0.01619 (18)
H180.9416 (18)1.2227 (14)0.4720 (11)0.021 (3)*
C190.78662 (14)1.35502 (11)0.44617 (8)0.01860 (19)
H190.7421 (18)1.3349 (14)0.5078 (11)0.022 (3)*
C200.73618 (14)1.44989 (11)0.38173 (9)0.01931 (19)
H200.658 (2)1.4978 (15)0.4001 (12)0.028 (4)*
C210.80260 (14)1.47698 (10)0.29578 (8)0.01828 (19)
H210.7735 (19)1.5465 (15)0.2518 (12)0.024 (3)*
C220.91731 (13)1.40873 (10)0.27311 (8)0.01578 (18)
H220.9588 (18)1.4296 (14)0.2116 (11)0.019 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O210.0230 (4)0.0213 (4)0.0153 (3)0.0007 (3)0.0019 (3)0.0029 (3)
O220.0209 (4)0.0182 (3)0.0231 (4)0.0014 (3)0.0112 (3)0.0063 (3)
O410.0254 (4)0.0195 (3)0.0137 (3)0.0027 (3)0.0045 (3)0.0013 (3)
O420.0231 (4)0.0255 (4)0.0163 (3)0.0058 (3)0.0102 (3)0.0083 (3)
N10.0166 (4)0.0142 (3)0.0116 (3)0.0029 (3)0.0051 (3)0.0021 (3)
N20.0149 (4)0.0137 (3)0.0168 (4)0.0042 (3)0.0053 (3)0.0036 (3)
N40.0178 (4)0.0165 (4)0.0129 (3)0.0083 (3)0.0062 (3)0.0043 (3)
N50.0148 (4)0.0133 (3)0.0123 (3)0.0037 (3)0.0048 (3)0.0025 (3)
C10.0134 (4)0.0130 (4)0.0128 (4)0.0063 (3)0.0053 (3)0.0037 (3)
C20.0125 (4)0.0123 (4)0.0138 (4)0.0038 (3)0.0042 (3)0.0030 (3)
C30.0139 (4)0.0136 (4)0.0147 (4)0.0066 (3)0.0064 (3)0.0047 (3)
C40.0150 (4)0.0141 (4)0.0107 (4)0.0067 (3)0.0054 (3)0.0035 (3)
C50.0127 (4)0.0126 (4)0.0136 (4)0.0064 (3)0.0047 (3)0.0032 (3)
C60.0139 (4)0.0137 (4)0.0127 (4)0.0049 (3)0.0064 (3)0.0032 (3)
C70.0157 (4)0.0159 (4)0.0130 (4)0.0061 (3)0.0065 (3)0.0037 (3)
C80.0165 (4)0.0198 (4)0.0201 (4)0.0090 (4)0.0097 (4)0.0083 (4)
C90.0130 (4)0.0148 (4)0.0160 (4)0.0070 (3)0.0060 (3)0.0043 (3)
C100.0148 (4)0.0148 (4)0.0155 (4)0.0041 (3)0.0038 (3)0.0021 (3)
C110.0209 (5)0.0220 (5)0.0179 (4)0.0090 (4)0.0093 (4)0.0066 (4)
C120.0181 (4)0.0186 (4)0.0304 (5)0.0069 (4)0.0121 (4)0.0101 (4)
C130.0149 (4)0.0137 (4)0.0306 (5)0.0034 (3)0.0043 (4)0.0010 (4)
C140.0174 (4)0.0180 (4)0.0156 (4)0.0080 (4)0.0028 (3)0.0007 (3)
C150.0138 (4)0.0142 (4)0.0147 (4)0.0052 (3)0.0064 (3)0.0038 (3)
C160.0123 (4)0.0152 (4)0.0151 (4)0.0039 (3)0.0041 (3)0.0029 (3)
C170.0126 (4)0.0125 (4)0.0134 (4)0.0027 (3)0.0026 (3)0.0008 (3)
C180.0176 (4)0.0150 (4)0.0154 (4)0.0041 (3)0.0054 (3)0.0030 (3)
C190.0195 (4)0.0186 (4)0.0178 (4)0.0045 (4)0.0081 (4)0.0013 (3)
C200.0177 (4)0.0177 (4)0.0221 (5)0.0066 (4)0.0057 (4)0.0016 (4)
C210.0192 (4)0.0155 (4)0.0191 (4)0.0067 (4)0.0035 (4)0.0021 (3)
C220.0170 (4)0.0154 (4)0.0145 (4)0.0049 (3)0.0045 (3)0.0030 (3)
Geometric parameters (Å, º) top
O21—N21.2475 (11)C9—C101.3980 (13)
O22—N21.2354 (10)C10—C111.3925 (13)
O41—N41.2489 (11)C10—H100.966 (15)
O42—N41.2356 (10)C11—C121.3905 (15)
N1—C11.3544 (12)C11—H111.006 (16)
N1—C71.4543 (12)C12—C131.3880 (16)
N1—H10.891 (15)C12—H120.965 (17)
N2—C21.4363 (12)C13—C141.3968 (15)
N4—C41.4376 (12)C13—H130.963 (17)
N5—C51.3456 (12)C14—H140.980 (16)
N5—C151.4592 (12)C15—C161.5320 (13)
N5—H50.900 (17)C15—H15A0.983 (13)
C1—C61.4025 (13)C15—H15B0.999 (13)
C1—C21.4428 (12)C16—C171.5113 (13)
C2—C31.3832 (13)C16—H16B0.979 (14)
C3—C41.3805 (13)C16—H16A0.994 (14)
C3—H30.961 (14)C17—C181.3995 (13)
C4—C51.4434 (12)C17—C221.4009 (13)
C5—C61.4039 (13)C18—C191.3948 (14)
C6—H60.947 (14)C18—H180.996 (14)
C7—C81.5337 (14)C19—C201.3945 (15)
C7—H7A0.969 (13)C19—H190.983 (14)
C7—H7B0.965 (13)C20—C211.3900 (15)
C8—C91.5065 (13)C20—H200.974 (15)
C8—H8B0.977 (14)C21—C221.3952 (14)
C8—H8A1.000 (15)C21—H210.978 (14)
C9—C141.3956 (13)C22—H220.971 (13)
C1—N1—C7124.07 (8)C11—C10—C9120.67 (9)
C1—N1—H1115.8 (10)C11—C10—H10119.9 (9)
C7—N1—H1119.0 (10)C9—C10—H10119.4 (9)
O22—N2—O21121.71 (8)C12—C11—C10119.99 (9)
O22—N2—C2119.42 (8)C12—C11—H11118.8 (9)
O21—N2—C2118.88 (8)C10—C11—H11121.2 (9)
O42—N4—O41121.81 (8)C13—C12—C11120.05 (9)
O42—N4—C4119.44 (8)C13—C12—H12118.1 (10)
O41—N4—C4118.75 (8)C11—C12—H12121.8 (10)
C5—N5—C15124.42 (8)C12—C13—C14119.84 (9)
C5—N5—H5118.4 (10)C12—C13—H13118.5 (10)
C15—N5—H5116.8 (10)C14—C13—H13121.7 (10)
N1—C1—C6121.20 (8)C9—C14—C13120.72 (9)
N1—C1—C2122.14 (8)C9—C14—H14119.6 (9)
C6—C1—C2116.66 (8)C13—C14—H14119.6 (9)
C3—C2—N2116.57 (8)N5—C15—C16110.11 (8)
C3—C2—C1120.46 (8)N5—C15—H15A110.3 (7)
N2—C2—C1122.94 (8)C16—C15—H15A111.1 (7)
C4—C3—C2121.62 (8)N5—C15—H15B109.9 (8)
C4—C3—H3119.5 (8)C16—C15—H15B108.9 (8)
C2—C3—H3118.9 (9)H15A—C15—H15B106.3 (11)
C3—C4—N4116.64 (8)C17—C16—C15112.77 (8)
C3—C4—C5120.48 (8)C17—C16—H16B109.9 (8)
N4—C4—C5122.85 (8)C15—C16—H16B107.2 (8)
N5—C5—C6120.81 (8)C17—C16—H16A111.8 (8)
N5—C5—C4122.58 (8)C15—C16—H16A108.2 (8)
C6—C5—C4116.58 (8)H16B—C16—H16A106.7 (11)
C1—C6—C5124.07 (8)C18—C17—C22118.37 (9)
C1—C6—H6118.1 (8)C18—C17—C16121.76 (8)
C5—C6—H6117.8 (8)C22—C17—C16119.84 (8)
N1—C7—C8111.96 (8)C19—C18—C17121.00 (9)
N1—C7—H7A107.9 (7)C19—C18—H18119.6 (8)
C8—C7—H7A108.4 (8)C17—C18—H18119.4 (8)
N1—C7—H7B109.8 (8)C20—C19—C18120.00 (9)
C8—C7—H7B110.4 (8)C20—C19—H19121.0 (8)
H7A—C7—H7B108.2 (11)C18—C19—H19119.0 (8)
C9—C8—C7112.29 (8)C21—C20—C19119.56 (9)
C9—C8—H8B111.3 (8)C21—C20—H20121.8 (9)
C7—C8—H8B106.6 (8)C19—C20—H20118.6 (9)
C9—C8—H8A109.2 (8)C20—C21—C22120.38 (9)
C7—C8—H8A108.3 (8)C20—C21—H21120.7 (8)
H8B—C8—H8A109.0 (12)C22—C21—H21118.8 (8)
C14—C9—C10118.74 (9)C21—C22—C17120.68 (9)
C14—C9—C8120.54 (9)C21—C22—H22117.6 (8)
C10—C9—C8120.69 (9)C17—C22—H22121.7 (8)
C7—N1—C1—C66.57 (14)N5—C5—C6—C1175.36 (8)
C7—N1—C1—C2174.69 (8)C4—C5—C6—C13.10 (13)
O22—N2—C2—C34.46 (12)C1—N1—C7—C879.33 (11)
O21—N2—C2—C3175.24 (8)N1—C7—C8—C9172.60 (8)
O22—N2—C2—C1177.78 (8)C7—C8—C9—C1492.60 (11)
O21—N2—C2—C12.53 (13)C7—C8—C9—C1085.24 (11)
N1—C1—C2—C3176.93 (8)C14—C9—C10—C110.33 (14)
C6—C1—C2—C31.86 (13)C8—C9—C10—C11178.21 (9)
N1—C1—C2—N25.39 (14)C9—C10—C11—C120.07 (15)
C6—C1—C2—N2175.82 (8)C10—C11—C12—C130.16 (15)
N2—C2—C3—C4177.06 (8)C11—C12—C13—C140.14 (15)
C1—C2—C3—C40.76 (14)C10—C9—C14—C130.36 (14)
C2—C3—C4—N4179.52 (8)C8—C9—C14—C13178.24 (9)
C2—C3—C4—C52.36 (13)C12—C13—C14—C90.13 (15)
O42—N4—C4—C31.13 (12)C5—N5—C15—C16169.34 (8)
O41—N4—C4—C3178.37 (8)N5—C15—C16—C1766.94 (10)
O42—N4—C4—C5176.93 (8)C15—C16—C17—C1889.20 (11)
O41—N4—C4—C53.57 (13)C15—C16—C17—C2288.67 (10)
C15—N5—C5—C60.22 (13)C22—C17—C18—C191.31 (14)
C15—N5—C5—C4178.58 (8)C16—C17—C18—C19176.60 (9)
C3—C4—C5—N5174.25 (8)C17—C18—C19—C200.80 (15)
N4—C4—C5—N53.74 (13)C18—C19—C20—C210.24 (15)
C3—C4—C5—C64.17 (13)C19—C20—C21—C220.74 (15)
N4—C4—C5—C6177.83 (8)C20—C21—C22—C170.22 (15)
N1—C1—C6—C5178.97 (8)C18—C17—C22—C210.80 (14)
C2—C1—C6—C50.17 (13)C16—C17—C22—C21177.15 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O210.891 (15)1.935 (15)2.6318 (11)133.8 (13)
N5—H5···O410.900 (17)1.967 (16)2.6358 (11)129.8 (14)
N5—H5···O41i0.900 (17)2.800 (17)3.5877 (11)146.8 (13)
Symmetry code: (i) x+2, y+2, z+1.
(C15H13N3O2) 2-cyano-4-nitro-N-(2-phenylethyl)aniline top
Crystal data top
C15H13N3O2F(000) = 560
Mr = 267.28Dx = 1.348 Mg m3
Monoclinic, P21/nMelting point: 427 K
Hall symbol: -P 2ynMo Kα radiation, λ = 0.71073 Å
a = 7.4871 (5) ÅCell parameters from 23429 reflections
b = 16.270 (1) Åθ = 2.3–33.0°
c = 10.8432 (7) ŵ = 0.09 mm1
β = 94.384 (1)°T = 100 K
V = 1317.00 (15) Å3Parallelpiped, yellow
Z = 40.40 × 0.20 × 0.10 mm
Data collection top
Bruker APEX DUO CCD area-detector
diffractometer
4732 independent reflections
Radiation source: sealed tube4189 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
ω scansθmax = 32.9°, θmin = 2.3°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1111
Tmin = 0.964, Tmax = 0.991k = 2424
23007 measured reflectionsl = 1616
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038Hydrogen site location: difference Fourier map
wR(F2) = 0.113All H-atom parameters refined
S = 1.04 w = 1/[σ2(Fo2) + (0.0687P)2 + 0.3103P]
where P = (Fo2 + 2Fc2)/3
4732 reflections(Δ/σ)max = 0.001
233 parametersΔρmax = 0.56 e Å3
0 restraintsΔρmin = 0.20 e Å3
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.

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) top
xyzUiso*/Ueq
O410.28684 (9)0.12353 (4)0.29556 (6)0.02323 (14)
O420.10504 (8)0.03747 (4)0.37421 (6)0.02067 (13)
N10.65662 (8)0.09507 (4)0.83376 (6)0.01439 (12)
H10.6214 (19)0.0666 (9)0.8948 (14)0.033 (3)*
N20.33192 (10)0.05113 (4)0.89432 (7)0.02022 (14)
N40.23997 (8)0.08139 (4)0.38232 (6)0.01466 (13)
C10.55906 (9)0.09106 (4)0.72443 (6)0.01199 (13)
C20.40849 (9)0.03712 (4)0.70702 (6)0.01168 (13)
C30.30296 (9)0.03411 (4)0.59568 (7)0.01221 (13)
H30.2029 (15)0.0007 (7)0.5865 (11)0.019 (3)*
C40.34763 (9)0.08426 (4)0.49902 (6)0.01264 (13)
C50.49621 (10)0.13679 (5)0.51165 (7)0.01499 (14)
H50.5272 (16)0.1712 (8)0.4445 (11)0.021 (3)*
C60.59954 (10)0.13990 (5)0.62209 (7)0.01514 (14)
H60.6992 (17)0.1754 (8)0.6296 (12)0.024 (3)*
C70.80953 (9)0.14949 (5)0.86030 (7)0.01465 (14)
H7A0.7833 (16)0.2054 (7)0.8259 (11)0.020 (3)*
H7B0.8227 (16)0.1545 (8)0.9503 (12)0.022 (3)*
C80.98355 (10)0.11550 (5)0.81298 (8)0.01875 (15)
H8B0.9959 (18)0.0584 (8)0.8430 (13)0.029 (3)*
H8A0.9744 (18)0.1137 (8)0.7233 (13)0.030 (3)*
C91.14367 (9)0.16670 (5)0.85827 (7)0.01476 (14)
C101.22232 (10)0.15533 (5)0.97834 (7)0.01569 (14)
H101.1749 (18)0.1134 (8)1.0314 (13)0.027 (3)*
C111.36857 (10)0.20255 (5)1.02246 (7)0.01573 (14)
H111.4201 (18)0.1936 (8)1.1055 (12)0.026 (3)*
C121.43693 (10)0.26274 (5)0.94762 (7)0.01653 (14)
H121.5371 (18)0.2976 (8)0.9811 (13)0.030 (3)*
C131.36012 (10)0.27489 (5)0.82797 (7)0.01769 (15)
H131.4088 (18)0.3160 (8)0.7747 (13)0.028 (3)*
C141.21486 (10)0.22666 (5)0.78384 (7)0.01678 (14)
H141.1657 (16)0.2334 (8)0.6966 (12)0.024 (3)*
C150.36369 (9)0.01308 (4)0.80896 (7)0.01396 (13)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O410.0262 (3)0.0287 (3)0.0145 (3)0.0025 (2)0.0005 (2)0.0067 (2)
O420.0176 (3)0.0243 (3)0.0194 (3)0.0046 (2)0.0032 (2)0.0013 (2)
N10.0130 (3)0.0174 (3)0.0126 (3)0.0041 (2)0.0002 (2)0.0009 (2)
N20.0213 (3)0.0208 (3)0.0186 (3)0.0022 (2)0.0014 (2)0.0046 (2)
N40.0147 (3)0.0157 (3)0.0134 (3)0.0021 (2)0.0001 (2)0.0006 (2)
C10.0101 (3)0.0129 (3)0.0131 (3)0.0004 (2)0.0014 (2)0.0003 (2)
C20.0109 (3)0.0117 (3)0.0126 (3)0.0003 (2)0.0017 (2)0.0009 (2)
C30.0109 (3)0.0123 (3)0.0135 (3)0.0000 (2)0.0014 (2)0.0001 (2)
C40.0119 (3)0.0141 (3)0.0118 (3)0.0008 (2)0.0001 (2)0.0006 (2)
C50.0142 (3)0.0161 (3)0.0148 (3)0.0016 (2)0.0018 (2)0.0030 (2)
C60.0131 (3)0.0172 (3)0.0152 (3)0.0040 (2)0.0012 (2)0.0026 (2)
C70.0120 (3)0.0162 (3)0.0157 (3)0.0023 (2)0.0002 (2)0.0024 (2)
C80.0123 (3)0.0198 (3)0.0238 (4)0.0008 (2)0.0008 (3)0.0089 (3)
C90.0105 (3)0.0159 (3)0.0178 (3)0.0012 (2)0.0001 (2)0.0052 (2)
C100.0148 (3)0.0147 (3)0.0175 (3)0.0009 (2)0.0006 (2)0.0014 (2)
C110.0140 (3)0.0173 (3)0.0155 (3)0.0000 (2)0.0012 (2)0.0019 (2)
C120.0128 (3)0.0176 (3)0.0189 (3)0.0020 (2)0.0001 (2)0.0022 (3)
C130.0161 (3)0.0190 (3)0.0181 (3)0.0004 (2)0.0022 (3)0.0010 (3)
C140.0142 (3)0.0208 (3)0.0151 (3)0.0027 (2)0.0006 (2)0.0022 (3)
C150.0126 (3)0.0137 (3)0.0154 (3)0.0012 (2)0.0003 (2)0.0001 (2)
Geometric parameters (Å, º) top
O41—N41.2364 (9)C7—C81.5391 (11)
O42—N41.2351 (9)C7—H7A0.997 (12)
N1—C11.3456 (9)C7—H7B0.976 (13)
N1—C71.4585 (9)C8—C91.5107 (10)
N1—H10.866 (15)C8—H8B0.986 (14)
N2—C151.1534 (10)C8—H8A0.970 (14)
N4—C41.4481 (9)C9—C141.3975 (11)
C1—C61.4163 (10)C9—C101.3995 (11)
C1—C21.4298 (9)C10—C111.3921 (10)
C2—C31.3923 (10)C10—H100.977 (13)
C2—C151.4346 (10)C11—C121.3938 (11)
C3—C41.3892 (10)C11—H110.963 (13)
C3—H30.938 (12)C12—C131.3925 (11)
C4—C51.4013 (10)C12—H120.987 (14)
C5—C61.3761 (10)C13—C141.3957 (11)
C5—H50.961 (12)C13—H130.972 (14)
C6—H60.942 (13)C14—H140.994 (13)
C1—N1—C7124.63 (6)C8—C7—H7B109.9 (7)
C1—N1—H1118.1 (10)H7A—C7—H7B107.4 (10)
C7—N1—H1117.0 (10)C9—C8—C7111.37 (6)
O42—N4—O41123.01 (7)C9—C8—H8B111.1 (8)
O42—N4—C4118.59 (6)C7—C8—H8B106.8 (8)
O41—N4—C4118.40 (6)C9—C8—H8A109.7 (8)
N1—C1—C6121.93 (6)C7—C8—H8A110.4 (8)
N1—C1—C2121.03 (6)H8B—C8—H8A107.4 (11)
C6—C1—C2117.04 (6)C14—C9—C10118.53 (7)
C3—C2—C1121.71 (6)C14—C9—C8121.69 (7)
C3—C2—C15119.83 (6)C10—C9—C8119.77 (7)
C1—C2—C15118.43 (6)C11—C10—C9120.71 (7)
C4—C3—C2118.70 (6)C11—C10—H10119.6 (8)
C4—C3—H3120.7 (7)C9—C10—H10119.6 (8)
C2—C3—H3120.6 (7)C10—C11—C12120.12 (7)
C3—C4—C5121.31 (7)C10—C11—H11119.1 (8)
C3—C4—N4119.36 (6)C12—C11—H11120.8 (8)
C5—C4—N4119.32 (6)C13—C12—C11119.89 (7)
C6—C5—C4119.78 (7)C13—C12—H12120.6 (8)
C6—C5—H5119.1 (7)C11—C12—H12119.5 (8)
C4—C5—H5121.1 (7)C12—C13—C14119.67 (7)
C5—C6—C1121.44 (7)C12—C13—H13120.3 (8)
C5—C6—H6119.1 (8)C14—C13—H13120.0 (8)
C1—C6—H6119.5 (8)C13—C14—C9121.07 (7)
N1—C7—C8112.82 (6)C13—C14—H14119.1 (7)
N1—C7—H7A110.5 (7)C9—C14—H14119.8 (7)
C8—C7—H7A110.5 (7)N2—C15—C2177.02 (8)
N1—C7—H7B105.4 (7)
C7—N1—C1—C61.06 (11)C4—C5—C6—C10.14 (11)
C7—N1—C1—C2178.63 (6)N1—C1—C6—C5178.37 (7)
N1—C1—C2—C3178.00 (7)C2—C1—C6—C51.33 (11)
C6—C1—C2—C31.70 (10)C1—N1—C7—C881.27 (9)
N1—C1—C2—C150.18 (10)N1—C7—C8—C9171.53 (6)
C6—C1—C2—C15179.88 (6)C7—C8—C9—C1498.73 (8)
C1—C2—C3—C40.87 (10)C7—C8—C9—C1080.25 (9)
C15—C2—C3—C4179.03 (6)C14—C9—C10—C110.20 (11)
C2—C3—C4—C50.39 (11)C8—C9—C10—C11179.21 (7)
C2—C3—C4—N4179.54 (6)C9—C10—C11—C120.90 (11)
O42—N4—C4—C33.91 (10)C10—C11—C12—C130.82 (11)
O41—N4—C4—C3176.58 (7)C11—C12—C13—C140.06 (12)
O42—N4—C4—C5176.93 (7)C12—C13—C14—C90.65 (12)
O41—N4—C4—C52.58 (10)C10—C9—C14—C130.58 (11)
C3—C4—C5—C60.76 (11)C8—C9—C14—C13178.41 (7)
N4—C4—C5—C6179.91 (7)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···N2i0.866 (15)2.300 (15)3.0287 (10)141.9 (12)
Symmetry code: (i) x+1, y, z+2.
(C15H16N2O4S) 4-(methylsulfonyl)-2-nitro-N-(2-phenylethyl)aniline top
Crystal data top
C15H16N2O4SDx = 1.412 Mg m3
Mr = 320.36Melting point: 414 K
Tetragonal, I41/aMo Kα radiation, λ = 0.71073 Å
Hall symbol: -I 4adCell parameters from 53474 reflections
a = 20.4639 (13) Åθ = 2.6–32.9°
c = 14.3952 (14) ŵ = 0.24 mm1
V = 6028.3 (10) Å3T = 100 K
Z = 16Cuboid, yellow
F(000) = 26880.40 × 0.20 × 0.20 mm
Data collection top
Bruker APEX DUO CCD area-detector
diffractometer
5524 independent reflections
Radiation source: sealed tube5155 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
ω scansθmax = 32.9°, θmin = 1.7°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 3031
Tmin = 0.912, Tmax = 0.955k = 3130
52424 measured reflectionsl = 2121
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.029Hydrogen site location: difference Fourier map
wR(F2) = 0.086All H-atom parameters refined
S = 1.06 w = 1/[σ2(Fo2) + (0.0494P)2 + 3.0117P]
where P = (Fo2 + 2Fc2)/3
5524 reflections(Δ/σ)max = 0.002
263 parametersΔρmax = 0.51 e Å3
0 restraintsΔρmin = 0.31 e Å3
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.

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) top
xyzUiso*/Ueq
S10.918999 (8)0.384073 (8)0.115221 (13)0.01486 (5)
O210.72956 (3)0.62358 (3)0.13034 (5)0.02619 (14)
O220.83430 (3)0.61924 (3)0.15113 (5)0.02251 (12)
O410.91451 (3)0.33599 (3)0.04188 (4)0.02179 (12)
O420.96848 (3)0.43425 (3)0.10731 (5)0.02180 (12)
N10.66040 (3)0.51537 (3)0.11584 (5)0.01679 (12)
H10.6604 (7)0.5584 (8)0.1202 (10)0.038 (4)*
N20.78132 (3)0.59202 (3)0.13760 (5)0.01652 (11)
C10.71927 (3)0.48639 (3)0.12182 (5)0.01391 (12)
C20.77942 (3)0.52165 (3)0.13051 (5)0.01370 (12)
C30.84001 (3)0.49002 (3)0.13130 (5)0.01447 (12)
H30.8791 (7)0.5168 (6)0.1359 (9)0.026 (3)*
C40.84249 (3)0.42282 (3)0.12432 (5)0.01465 (12)
C50.78421 (4)0.38584 (4)0.11955 (5)0.01666 (13)
H50.7859 (6)0.3384 (6)0.1168 (8)0.023 (3)*
C60.72458 (4)0.41678 (4)0.11892 (5)0.01637 (13)
H60.6879 (6)0.3928 (6)0.1145 (9)0.023 (3)*
C70.59791 (4)0.48089 (4)0.11108 (5)0.01798 (13)
H7A0.5906 (5)0.4561 (5)0.1693 (8)0.015 (2)*
H7B0.5982 (6)0.4507 (6)0.0597 (8)0.018 (3)*
C80.54312 (4)0.53117 (4)0.09737 (5)0.01863 (13)
H8A0.5029 (6)0.5080 (6)0.0915 (9)0.021 (3)*
H8B0.5525 (6)0.5542 (6)0.0391 (9)0.025 (3)*
C90.53881 (3)0.57928 (4)0.17680 (5)0.01547 (12)
C100.56452 (4)0.64241 (4)0.17008 (5)0.01871 (13)
H100.5853 (6)0.6565 (7)0.1136 (9)0.026 (3)*
C110.56197 (4)0.68488 (4)0.24613 (6)0.02200 (15)
H110.5775 (6)0.7276 (7)0.2407 (10)0.029 (3)*
C120.53446 (4)0.66439 (4)0.32954 (6)0.02297 (15)
H120.5339 (7)0.6937 (7)0.3812 (10)0.034 (4)*
C130.50872 (4)0.60148 (4)0.33686 (5)0.02155 (14)
H130.4898 (7)0.5856 (7)0.3950 (10)0.031 (3)*
C140.51036 (4)0.55957 (4)0.26071 (5)0.01777 (13)
H140.4927 (6)0.5155 (6)0.2656 (9)0.022 (3)*
C150.92951 (4)0.34181 (4)0.22080 (6)0.02208 (14)
H15A0.9299 (6)0.3726 (7)0.2701 (10)0.031 (3)*
H15B0.8929 (7)0.3095 (7)0.2271 (10)0.034 (3)*
H15C0.9713 (7)0.3212 (7)0.2172 (10)0.037 (4)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.01361 (8)0.01350 (8)0.01747 (9)0.00014 (5)0.00355 (5)0.00138 (5)
O210.0209 (3)0.0141 (2)0.0435 (4)0.0033 (2)0.0035 (2)0.0016 (2)
O220.0192 (3)0.0156 (2)0.0328 (3)0.00497 (19)0.0030 (2)0.0024 (2)
O410.0247 (3)0.0191 (2)0.0216 (3)0.0014 (2)0.0052 (2)0.0065 (2)
O420.0150 (2)0.0172 (2)0.0332 (3)0.00241 (19)0.0043 (2)0.0003 (2)
N10.0135 (3)0.0149 (3)0.0220 (3)0.0003 (2)0.0005 (2)0.0027 (2)
N20.0184 (3)0.0123 (2)0.0188 (3)0.0008 (2)0.0017 (2)0.0005 (2)
C10.0138 (3)0.0140 (3)0.0140 (3)0.0006 (2)0.0006 (2)0.0017 (2)
C20.0149 (3)0.0105 (3)0.0156 (3)0.0010 (2)0.0010 (2)0.0012 (2)
C30.0142 (3)0.0135 (3)0.0157 (3)0.0011 (2)0.0011 (2)0.0015 (2)
C40.0138 (3)0.0128 (3)0.0173 (3)0.0002 (2)0.0014 (2)0.0016 (2)
C50.0159 (3)0.0131 (3)0.0210 (3)0.0010 (2)0.0007 (2)0.0022 (2)
C60.0148 (3)0.0133 (3)0.0210 (3)0.0019 (2)0.0006 (2)0.0024 (2)
C70.0140 (3)0.0191 (3)0.0209 (3)0.0016 (2)0.0003 (2)0.0048 (2)
C80.0142 (3)0.0259 (3)0.0159 (3)0.0013 (2)0.0016 (2)0.0044 (3)
C90.0116 (3)0.0203 (3)0.0145 (3)0.0027 (2)0.0010 (2)0.0006 (2)
C100.0176 (3)0.0209 (3)0.0176 (3)0.0014 (2)0.0006 (2)0.0027 (2)
C110.0242 (3)0.0178 (3)0.0240 (4)0.0021 (3)0.0030 (3)0.0002 (3)
C120.0270 (4)0.0221 (3)0.0198 (3)0.0072 (3)0.0021 (3)0.0044 (3)
C130.0225 (3)0.0256 (4)0.0166 (3)0.0053 (3)0.0033 (3)0.0006 (3)
C140.0155 (3)0.0202 (3)0.0175 (3)0.0018 (2)0.0020 (2)0.0002 (2)
C150.0201 (3)0.0257 (4)0.0205 (3)0.0041 (3)0.0026 (3)0.0032 (3)
Geometric parameters (Å, º) top
S1—O411.4462 (6)C7—H7A0.992 (11)
S1—O421.4467 (6)C7—H7B0.964 (12)
S1—C41.7599 (7)C8—C91.5114 (10)
S1—C151.7619 (8)C8—H8A0.954 (12)
O21—N21.2449 (9)C8—H8B0.982 (13)
O22—N21.2345 (9)C9—C101.3983 (11)
N1—C11.3454 (9)C9—C141.4002 (10)
N1—C71.4623 (10)C10—C111.3989 (11)
N1—H10.882 (16)C10—H100.962 (13)
N2—C21.4441 (9)C11—C121.3909 (12)
C1—C61.4293 (10)C11—H110.934 (13)
C1—C21.4322 (10)C12—C131.3949 (12)
C2—C31.3989 (10)C12—H120.955 (14)
C3—C41.3797 (10)C13—C141.3922 (11)
C3—H30.973 (14)C13—H130.977 (14)
C4—C51.4142 (10)C14—H140.974 (12)
C5—C61.3746 (10)C15—H15A0.949 (14)
C5—H50.972 (13)C15—H15B1.003 (14)
C6—H60.898 (13)C15—H15C0.955 (14)
C7—C81.5344 (11)
O41—S1—O42118.03 (4)N1—C7—H7B109.8 (7)
O41—S1—C4107.72 (4)C8—C7—H7B109.6 (7)
O42—S1—C4107.99 (3)H7A—C7—H7B108.8 (10)
O41—S1—C15107.66 (4)C9—C8—C7112.47 (6)
O42—S1—C15109.33 (4)C9—C8—H8A109.9 (7)
C4—S1—C15105.40 (4)C7—C8—H8A108.0 (7)
C1—N1—C7125.00 (6)C9—C8—H8B110.2 (8)
C1—N1—H1115.8 (10)C7—C8—H8B106.9 (7)
C7—N1—H1118.9 (10)H8A—C8—H8B109.3 (10)
O22—N2—O21121.76 (7)C10—C9—C14118.84 (7)
O22—N2—C2119.00 (6)C10—C9—C8121.84 (7)
O21—N2—C2119.24 (6)C14—C9—C8119.29 (7)
N1—C1—C6120.36 (7)C9—C10—C11120.39 (7)
N1—C1—C2123.58 (7)C9—C10—H10120.1 (8)
C6—C1—C2116.06 (6)C11—C10—H10119.4 (8)
C3—C2—C1121.96 (6)C12—C11—C10120.22 (8)
C3—C2—N2115.91 (6)C12—C11—H11119.5 (8)
C1—C2—N2122.12 (6)C10—C11—H11120.3 (9)
C4—C3—C2119.55 (6)C11—C12—C13119.76 (7)
C4—C3—H3122.5 (8)C11—C12—H12119.2 (9)
C2—C3—H3117.9 (8)C13—C12—H12121.0 (9)
C3—C4—C5120.39 (7)C14—C13—C12120.00 (7)
C3—C4—S1119.15 (5)C14—C13—H13118.6 (8)
C5—C4—S1120.37 (5)C12—C13—H13121.4 (8)
C6—C5—C4120.17 (7)C13—C14—C9120.78 (7)
C6—C5—H5119.5 (8)C13—C14—H14120.3 (7)
C4—C5—H5120.4 (8)C9—C14—H14118.9 (7)
C5—C6—C1121.75 (7)S1—C15—H15A108.7 (8)
C5—C6—H6119.4 (8)S1—C15—H15B108.1 (8)
C1—C6—H6118.9 (8)H15A—C15—H15B112.0 (11)
N1—C7—C8108.76 (6)S1—C15—H15C106.2 (9)
N1—C7—H7A109.9 (6)H15A—C15—H15C109.1 (12)
C8—C7—H7A110.0 (6)H15B—C15—H15C112.6 (12)
C7—N1—C1—C63.38 (11)C15—S1—C4—C572.35 (7)
C7—N1—C1—C2177.13 (7)C3—C4—C5—C62.03 (11)
N1—C1—C2—C3176.34 (7)S1—C4—C5—C6174.59 (6)
C6—C1—C2—C33.18 (10)C4—C5—C6—C10.80 (11)
N1—C1—C2—N22.73 (11)N1—C1—C6—C5176.24 (7)
C6—C1—C2—N2177.76 (6)C2—C1—C6—C53.29 (10)
O22—N2—C2—C35.65 (10)C1—N1—C7—C8175.70 (7)
O21—N2—C2—C3174.68 (7)N1—C7—C8—C961.20 (8)
O22—N2—C2—C1175.24 (7)C7—C8—C9—C10101.15 (8)
O21—N2—C2—C14.44 (10)C7—C8—C9—C1476.55 (8)
C1—C2—C3—C40.55 (10)C14—C9—C10—C110.21 (11)
N2—C2—C3—C4179.66 (6)C8—C9—C10—C11177.50 (7)
C2—C3—C4—C52.14 (10)C9—C10—C11—C120.74 (12)
C2—C3—C4—S1174.53 (5)C10—C11—C12—C130.70 (12)
O41—S1—C4—C3134.28 (6)C11—C12—C13—C140.30 (12)
O42—S1—C4—C35.78 (7)C12—C13—C14—C91.27 (12)
C15—S1—C4—C3110.98 (6)C10—C9—C14—C131.21 (11)
O41—S1—C4—C542.39 (7)C8—C9—C14—C13176.56 (7)
O42—S1—C4—C5170.88 (6)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O210.882 (16)1.951 (16)2.6364 (9)133.4 (14)
 

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