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The structures of reaction intermediates, arylnitrenes and their final products have been successfully analyzed by X-rays using acid–base complex formation. The acid–base complexes of 2-azidobenzoic acid (2a), 3-azidobenzoic acid (3a) and 4-azidobenzoic acid (4a) were made with dibenzylamine (db), N-benzyl-2-phenylethylamine (bp) and dicyclohexylamine (dc). For the complex crystals of (3a) and db (3a-db), and (4a) and db (4a-db) two forms of (I) and (II) were obtained. Eight types of complex crystals, (2a-db), (3a-db-I), (3a-db-II), (3a-dc), (4a-db-I), (4a-db-II), (4a-bp) and (4a-dc), suitable for X-ray analysis were obtained. When the crystals were irradiated with UV light at low temperatures, the reactions proceeded keeping the single-crystal form in the five crystals (2a-db), (3a-db-I), (3a-db-II), (3a-dc) and (4a-bp). Less than 25% of each azidobenzoic acids was transformed into an arylnitrene and dinitrogen. In three crystals the arylnitrenes produced gave new final products; 2,1-benzisoxazolone was observed for (2a-db) and trans-azobenzenes (i.e. dimerized nitrenes) were obtained for (3a-db-II) and (4a-bp). For (3a-db-I) and (3a-dc) the intermediate arylnitrenes were observed but did not transform to new products. All the structural changes were directly observed by X-ray analysis because the incomplete reactions occurred with retention crystallinity. The crystal environment, including the hydrogen bonding between the benzoic acid and the amine, places restrictions on the movement of the arylnitrene and influences the reaction pathway followed for conversion of the arylnitrene to its final product.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S010876811003661X/og5043sup1.cif
Contains datablocks 2a-db-i, 3a-db-I-i, 3a-db-II-i, 3a-dc-i, 4a-bp-i, 2a-db-f, 3a-db-I-f, 3a-db-II-f, 3a-dc-f, 4a-bp-f, 4a-db-I-i, 4a-db-II-i, 4a-dc-i, global

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50432a-db-isup2.fcf
Contains datablock 2a-db-i

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50433a-db-I-isup3.fcf
Contains datablock 3a-db-I-i

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50433a-db-II-isup4.fcf
Contains datablock 3a-db-II-i

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50433a-dc-isup5.fcf
Contains datablock 3a-dc-i

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50434a-bp-isup6.fcf
Contains datablock 4a-bp-i

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50432a-db-fsup7.fcf
Contains datablock 2a-db-f

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50433a-db-I-fsup8.fcf
Contains datablock 3a-db-I-f

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50433a-db-II-fsup9.fcf
Contains datablock 3a-db-II-f

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50433a-dc-fsup10.fcf
Contains datablock 3a-dc-f

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50434a-bp-fsup11.fcf
Contains datablock 4a-bp-f

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50434a-db-I-isup12.fcf
Contains datablock 4a-db-I-i

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50434a-db-II-isup13.fcf
Contains datablock 4a-db-II-i

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S010876811003661X/og50434a-dc-isup14.fcf
Contains datablock 4a-dc-i

CCDC references: 810870; 810871; 810872; 810873; 810874; 810875; 810876; 810877; 810878; 810879; 810880; 810881; 810882

Computing details top

Data collection: Siemens SMART for 2a-db-i, 3a-db-I-i, 3a-db-II-i, 3a-dc-i, 4a-bp-i, 2a-db-f, 3a-db-I-f, 3a-db-II-f, 3a-dc-f, 4a-bp-f, 4a-db-I-i, 4a-dc-i; PROCESS-AUTO (Rigaku, 1998) for 4a-db-II-i. Cell refinement: Siemens SMART for 2a-db-i, 3a-db-I-i, 3a-db-II-i, 3a-dc-i, 4a-bp-i, 2a-db-f, 3a-db-I-f, 3a-db-II-f, 3a-dc-f, 4a-bp-f, 4a-db-I-i, 4a-dc-i; PROCESS-AUTO (Rigaku, 1998) for 4a-db-II-i. Data reduction: SHELXS97 (Sheldrick, 1990) for 2a-db-i; Siemens SAINT & SADABS for 3a-db-I-i, 3a-dc-i, 4a-bp-i, 2a-db-f, 3a-db-I-f, 3a-db-II-f, 3a-dc-f, 4a-bp-f, 4a-db-I-i, 4a-dc-i; TEXSAN (Rigaku, 1999) for 4a-db-II-i. For all structures, program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997). Molecular graphics: ORTEP-3 for Window (Farrugia,1998) for 2a-db-i, 3a-db-I-i, 3a-dc-i, 4a-bp-i, 2a-db-f, 3a-db-I-f, 3a-db-II-f, 3a-dc-f, 4a-bp-f, 4a-db-I-i, 4a-dc-i; Siemens SAINT & SADABS for 3a-db-II-i; ORTEP-3 for Windows (Farrugia, 1998) for 4a-db-II-i. Software used to prepare material for publication: SHELXTL97 for 2a-db-i, 3a-db-I-i, 3a-db-II-i, 3a-dc-i, 4a-bp-i, 2a-db-f, 3a-db-I-f, 3a-db-II-f, 3a-dc-f, 4a-bp-f, 4a-db-I-i, 4a-dc-i; SHELXL97 (Sheldrick, 1997) for 4a-db-II-i.

Dibenzylammonium 2-azidebenzoate (2a-db-i) top
Crystal data top
C21H20N4O2F(000) = 760
Mr = 360.41Dx = 1.250 Mg m3
Monoclinic, CcMelting point: not measured K
a = 19.9575 (7) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.0329 (3) ÅCell parameters from 6026 reflections
c = 9.9849 (3) ŵ = 0.08 mm1
β = 106.640 (2)°T = 88 K
V = 1915.57 (11) Å3Block, pale-yellow
Z = 40.41 × 0.34 × 0.22 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
2788 independent reflections
Radiation source: rotating anode2668 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.035
ω scansθmax = 30.0°, θmin = 2.3°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 2828
Tmin = 0.967, Tmax = 0.982k = 1414
14815 measured reflectionsl = 1414
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.027Only H-atom coordinates refined
wR(F2) = 0.073 w = 1/[σ2(Fo2) + (0.0531P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max < 0.001
2788 reflectionsΔρmax = 0.21 e Å3
306 parametersΔρmin = 0.17 e Å3
2 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0 (10)
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
C70.52584 (6)0.28417 (11)0.17755 (12)0.0156 (2)
C10.51110 (6)0.07384 (11)0.31620 (12)0.0157 (2)
C20.53558 (7)0.05101 (12)0.37278 (12)0.0186 (2)
H20.5110 (11)0.1016 (19)0.427 (2)0.022*
C30.59777 (7)0.10205 (13)0.35731 (13)0.0210 (2)
H30.6127 (11)0.190 (2)0.393 (2)0.025*
C40.63557 (7)0.03052 (13)0.28332 (13)0.0215 (2)
H40.6789 (11)0.065 (2)0.269 (2)0.026*
C50.60980 (7)0.09231 (13)0.22353 (12)0.0187 (2)
H50.6341 (10)0.1426 (19)0.173 (2)0.022*
C60.54779 (6)0.14702 (11)0.23929 (11)0.0152 (2)
N10.44752 (6)0.12966 (11)0.33350 (12)0.0211 (2)
N20.42178 (6)0.06875 (12)0.41564 (12)0.0229 (2)
N30.39299 (7)0.02463 (15)0.48862 (15)0.0350 (3)
O10.49980 (5)0.36640 (9)0.24439 (9)0.02026 (18)
O20.53708 (5)0.30844 (9)0.06113 (9)0.02034 (18)
C80.41548 (6)0.43306 (12)0.49418 (13)0.0188 (2)
H810.4107 (10)0.4689 (19)0.583 (2)0.023*
H820.4000 (10)0.341 (2)0.487 (2)0.023*
C90.37123 (6)0.51203 (12)0.37163 (13)0.0199 (2)
C100.32648 (7)0.44712 (13)0.25664 (14)0.0225 (2)
H100.3267 (11)0.345 (2)0.257 (2)0.027*
C110.28343 (7)0.52001 (16)0.14560 (15)0.0270 (3)
H110.2533 (12)0.476 (2)0.065 (2)0.032*
C120.28549 (8)0.65867 (17)0.14707 (18)0.0313 (3)
H120.2539 (12)0.709 (2)0.073 (2)0.038*
C130.33064 (10)0.72386 (17)0.2590 (2)0.0421 (4)
H130.3304 (14)0.826 (3)0.269 (3)0.051*
C140.37258 (9)0.65203 (15)0.3726 (2)0.0369 (4)
H140.4055 (14)0.704 (2)0.456 (3)0.044*
C150.53440 (6)0.35001 (12)0.61997 (13)0.0177 (2)
H1510.5217 (10)0.262 (2)0.599 (2)0.021*
H1520.5219 (10)0.3775 (18)0.703 (2)0.021*
C160.61182 (6)0.36816 (11)0.63853 (12)0.0173 (2)
C170.64423 (7)0.30495 (13)0.54862 (13)0.0210 (2)
H170.6159 (10)0.242 (2)0.477 (2)0.025*
C180.71519 (7)0.32473 (14)0.56244 (14)0.0230 (2)
H180.7358 (11)0.283 (2)0.496 (2)0.028*
C190.75472 (7)0.40689 (15)0.66909 (17)0.0284 (3)
H190.8021 (13)0.424 (2)0.682 (2)0.034*
C200.72335 (8)0.46672 (18)0.76160 (19)0.0355 (3)
H200.7524 (13)0.520 (2)0.838 (3)0.043*
C210.65199 (7)0.44864 (15)0.74643 (16)0.0271 (3)
H210.6302 (12)0.496 (2)0.804 (2)0.032*
N40.49197 (5)0.43544 (10)0.50181 (11)0.01514 (18)
H010.5073 (9)0.5185 (19)0.5221 (19)0.018 (4)*
H020.4977 (9)0.4062 (18)0.420 (2)0.016 (4)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C70.0182 (5)0.0134 (5)0.0149 (5)0.0007 (4)0.0040 (4)0.0002 (4)
C10.0172 (5)0.0146 (5)0.0147 (5)0.0003 (4)0.0038 (4)0.0009 (4)
C20.0233 (6)0.0154 (5)0.0161 (5)0.0007 (4)0.0042 (4)0.0017 (4)
C30.0270 (6)0.0171 (5)0.0168 (5)0.0044 (4)0.0027 (4)0.0008 (4)
C40.0240 (6)0.0220 (6)0.0187 (5)0.0074 (4)0.0065 (4)0.0002 (4)
C50.0213 (5)0.0205 (5)0.0152 (5)0.0025 (4)0.0065 (4)0.0008 (4)
C60.0182 (5)0.0134 (5)0.0136 (5)0.0004 (4)0.0041 (4)0.0002 (4)
N10.0192 (5)0.0207 (5)0.0254 (5)0.0010 (4)0.0099 (4)0.0043 (4)
N20.0193 (5)0.0243 (5)0.0253 (5)0.0010 (4)0.0065 (4)0.0013 (4)
N30.0275 (6)0.0435 (8)0.0387 (7)0.0020 (5)0.0168 (5)0.0104 (6)
O10.0295 (5)0.0165 (4)0.0172 (4)0.0046 (3)0.0104 (3)0.0007 (3)
O20.0308 (5)0.0163 (4)0.0167 (4)0.0028 (3)0.0111 (3)0.0016 (3)
C80.0164 (5)0.0216 (5)0.0196 (6)0.0003 (4)0.0069 (4)0.0015 (4)
C90.0153 (5)0.0206 (5)0.0237 (6)0.0032 (4)0.0056 (4)0.0025 (4)
C100.0207 (5)0.0249 (6)0.0219 (6)0.0032 (5)0.0060 (4)0.0005 (5)
C110.0200 (6)0.0366 (7)0.0233 (6)0.0022 (5)0.0044 (5)0.0026 (6)
C120.0201 (6)0.0363 (7)0.0357 (7)0.0071 (5)0.0052 (5)0.0078 (6)
C130.0377 (8)0.0241 (7)0.0539 (11)0.0104 (6)0.0039 (7)0.0001 (7)
C140.0327 (8)0.0208 (6)0.0454 (9)0.0058 (6)0.0077 (7)0.0070 (6)
C150.0175 (5)0.0175 (5)0.0171 (5)0.0011 (4)0.0032 (4)0.0021 (4)
C160.0173 (5)0.0146 (5)0.0183 (5)0.0001 (4)0.0027 (4)0.0013 (4)
C170.0217 (6)0.0231 (6)0.0175 (5)0.0007 (4)0.0044 (4)0.0007 (4)
C180.0219 (6)0.0259 (6)0.0215 (6)0.0034 (4)0.0069 (5)0.0035 (5)
C190.0172 (6)0.0291 (7)0.0372 (8)0.0003 (5)0.0050 (5)0.0021 (6)
C200.0214 (6)0.0366 (8)0.0449 (9)0.0044 (5)0.0037 (6)0.0185 (7)
C210.0210 (6)0.0277 (6)0.0304 (7)0.0009 (5)0.0040 (5)0.0125 (5)
N40.0150 (4)0.0153 (4)0.0153 (4)0.0005 (3)0.0045 (3)0.0011 (3)
Geometric parameters (Å, º) top
C7—O11.2628 (14)C10—H101.03 (2)
C7—O21.2689 (14)C11—C121.392 (2)
C7—C61.5201 (16)C11—H110.96 (2)
C1—C21.4031 (16)C12—C131.383 (3)
C1—C61.4096 (15)C12—H120.97 (2)
C1—N11.4420 (15)C13—C141.401 (2)
C2—C31.3915 (18)C13—H131.03 (3)
C2—H20.97 (2)C14—H141.04 (3)
C3—C41.3962 (19)C15—N41.5072 (15)
C3—H30.96 (2)C15—C161.5136 (17)
C4—C51.4013 (17)C15—H1510.93 (2)
C4—H40.98 (2)C15—H1520.969 (19)
C5—C61.4032 (16)C16—C171.3997 (17)
C5—H50.94 (2)C16—C211.4003 (17)
N1—N21.2455 (15)C17—C181.3972 (18)
N1—O12.8379 (14)C17—H171.00 (2)
N1—O24.0733 (14)C18—C191.398 (2)
N1—N1i5.6297 (10)C18—H180.97 (2)
N2—N31.1389 (17)C19—C201.392 (2)
C8—N41.5067 (15)C19—H190.93 (2)
C8—C91.5120 (18)C20—C211.400 (2)
C8—H810.986 (19)C20—H200.97 (3)
C8—H820.97 (2)C21—H210.94 (2)
C9—C101.3974 (17)N4—H010.891 (19)
C9—C141.4048 (19)N4—H020.906 (19)
C10—C111.3988 (19)
O1—C7—O2124.48 (11)C9—C10—H10117.5 (12)
O1—C7—C6119.44 (10)C11—C10—H10121.8 (12)
O2—C7—C6116.06 (10)C12—C11—C10120.30 (14)
C2—C1—C6120.60 (11)C12—C11—H11118.4 (13)
C2—C1—N1121.02 (10)C10—C11—H11121.3 (13)
C6—C1—N1118.37 (10)C13—C12—C11119.46 (14)
C3—C2—C1120.17 (11)C13—C12—H12120.0 (14)
C3—C2—H2118.6 (12)C11—C12—H12120.4 (14)
C1—C2—H2121.2 (12)C12—C13—C14120.73 (15)
C2—C3—C4120.26 (11)C12—C13—H13121.9 (16)
C2—C3—H3118.9 (12)C14—C13—H13116.9 (16)
C4—C3—H3120.8 (12)C13—C14—C9120.21 (14)
C3—C4—C5119.30 (11)C13—C14—H14119.0 (14)
C3—C4—H4122.2 (12)C9—C14—H14120.8 (14)
C5—C4—H4118.4 (12)N4—C15—C16110.63 (9)
C4—C5—C6121.61 (11)N4—C15—H151108.2 (12)
C4—C5—H5121.2 (12)C16—C15—H151110.3 (12)
C6—C5—H5117.2 (12)N4—C15—H152106.3 (11)
C5—C6—C1118.02 (10)C16—C15—H152111.4 (12)
C5—C6—C7118.01 (10)H151—C15—H152110.0 (16)
C1—C6—C7123.93 (10)C17—C16—C21119.13 (11)
N2—N1—C1115.55 (10)C17—C16—C15120.67 (11)
N2—N1—O1151.06 (9)C21—C16—C15120.20 (11)
C1—N1—O182.67 (6)C18—C17—C16120.92 (12)
N2—N1—O2176.63 (9)C18—C17—H17120.7 (11)
C1—N1—O261.42 (6)C16—C17—H17118.3 (11)
O1—N1—O231.91 (2)C17—C18—C19119.59 (12)
N2—N1—N1i23.73 (7)C17—C18—H18119.0 (12)
C1—N1—N1i98.64 (7)C19—C18—H18121.4 (12)
O1—N1—N1i139.31 (4)C20—C19—C18119.80 (13)
O2—N1—N1i155.10 (2)C20—C19—H19117.5 (14)
N3—N2—N1172.25 (15)C18—C19—H19122.7 (14)
C7—O1—N182.11 (7)C19—C20—C21120.62 (13)
C7—O2—N122.69 (6)C19—C20—H20118.5 (15)
N4—C8—C9112.41 (10)C21—C20—H20120.9 (15)
N4—C8—H81107.9 (11)C20—C21—C16119.90 (13)
C9—C8—H81110.6 (11)C20—C21—H21120.1 (14)
N4—C8—H82108.4 (11)C16—C21—H21119.9 (14)
C9—C8—H82110.0 (11)C8—N4—C15111.38 (9)
H81—C8—H82107.4 (16)C8—N4—H01107.6 (12)
C10—C9—C14118.55 (12)C15—N4—H01106.0 (12)
C10—C9—C8120.57 (11)C8—N4—H02109.7 (11)
C14—C9—C8120.86 (12)C15—N4—H02109.5 (12)
C9—C10—C11120.70 (12)H01—N4—H02112.7 (16)
C6—C1—C2—C32.09 (18)O2—N1—O1—C714.31 (6)
N1—C1—C2—C3178.75 (11)N1i—N1—O1—C7125.53 (7)
C1—C2—C3—C41.13 (19)O1—C7—O2—N1114.4 (2)
C2—C3—C4—C50.75 (19)C6—C7—O2—N167.33 (14)
C3—C4—C5—C61.72 (19)N2—N1—O2—C7113.9 (16)
C4—C5—C6—C10.78 (18)C1—N1—O2—C787.69 (17)
C4—C5—C6—C7176.74 (11)O1—N1—O2—C739.18 (15)
C2—C1—C6—C51.13 (16)N1i—N1—O2—C747.79 (17)
N1—C1—C6—C5179.69 (11)N4—C8—C9—C10108.68 (13)
C2—C1—C6—C7178.49 (11)N4—C8—C9—C1473.22 (16)
N1—C1—C6—C72.33 (16)C14—C9—C10—C110.7 (2)
O1—C7—C6—C5140.53 (12)C8—C9—C10—C11177.45 (12)
O2—C7—C6—C537.78 (16)C9—C10—C11—C121.1 (2)
O1—C7—C6—C136.82 (17)C10—C11—C12—C130.2 (2)
O2—C7—C6—C1144.86 (11)C11—C12—C13—C142.0 (3)
C2—C1—N1—N28.94 (17)C12—C13—C14—C92.4 (3)
C6—C1—N1—N2171.88 (11)C10—C9—C14—C131.1 (3)
C2—C1—N1—O1165.35 (11)C8—C9—C14—C13179.21 (17)
C6—C1—N1—O115.47 (10)N4—C15—C16—C1778.18 (14)
C2—C1—N1—O2169.41 (12)N4—C15—C16—C21101.89 (14)
C6—C1—N1—O29.76 (8)C21—C16—C17—C182.14 (19)
C2—C1—N1—N1i26.44 (11)C15—C16—C17—C18177.93 (12)
C6—C1—N1—N1i154.38 (9)C16—C17—C18—C191.2 (2)
C1—N1—N2—N3173.7 (11)C17—C18—C19—C200.9 (2)
O1—N1—N2—N348.8 (12)C18—C19—C20—C211.9 (3)
O2—N1—N2—N3160.9 (11)C19—C20—C21—C160.9 (3)
N1i—N1—N2—N3126.0 (12)C17—C16—C21—C201.1 (2)
O2—C7—O1—N1149.41 (12)C15—C16—C21—C20178.97 (14)
C6—C7—O1—N132.42 (10)C9—C8—N4—C15176.89 (10)
N2—N1—O1—C7162.54 (19)C16—C15—N4—C8172.32 (9)
C1—N1—O1—C730.79 (9)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H01···O2ii0.891 (19)1.841 (19)2.7311 (13)178.7 (19)
N4—H01···O1ii0.891 (19)2.544 (18)3.1027 (14)121.4 (14)
N4—H02···O10.906 (19)1.810 (19)2.7094 (13)171.5 (17)
N4—H02···N10.906 (19)2.991 (18)3.4885 (15)116.3 (13)
Symmetry code: (ii) x, y+1, z+1/2.
Dibenzylammonium 3-azidebenzoate (3a-db-I-i) top
Crystal data top
C21H20N4O2Dx = 1.245 Mg m3
Mr = 360.41Melting point: not measured K
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
a = 8.9705 (1) ÅCell parameters from 8192 reflections
b = 14.4208 (1) ŵ = 0.08 mm1
c = 14.8689 (2) ÅT = 80 K
V = 1923.47 (4) Å3Needle, pale-yellow
Z = 40.40 × 0.20 × 0.15 mm
F(000) = 760
Data collection top
Bruker SMART CCD area detector system
diffractometer
3163 independent reflections
Radiation source: rotating anode2908 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
ω scansθmax = 30.0°, θmin = 2.0°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1212
Tmin = 0.968, Tmax = 0.988k = 2020
30731 measured reflectionsl = 2020
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.030Only H-atom coordinates refined
wR(F2) = 0.081 w = 1/[σ2(Fo2) + (0.0542P)2 + 0.0162P]
where P = (Fo2 + 2Fc2)/3
S = 1.17(Δ/σ)max < 0.001
3163 reflectionsΔρmax = 0.25 e Å3
324 parametersΔρmin = 0.17 e Å3
0 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0 (10)
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
C70.42563 (13)0.23810 (8)0.14946 (7)0.0175 (2)
C10.32640 (14)0.31922 (8)0.38437 (8)0.0214 (2)
C20.31631 (14)0.29550 (8)0.29364 (7)0.0187 (2)
H20.2235 (18)0.3030 (10)0.2611 (10)0.018 (4)*
C30.44015 (12)0.25957 (7)0.24902 (7)0.0168 (2)
C40.57361 (13)0.24659 (8)0.29573 (8)0.0201 (2)
H40.6589 (19)0.2247 (12)0.2638 (11)0.022 (4)*
C50.58356 (15)0.27224 (9)0.38620 (8)0.0239 (2)
H50.674 (2)0.2635 (13)0.4176 (11)0.030 (4)*
C60.46016 (16)0.30905 (9)0.43072 (8)0.0250 (2)
H60.470 (2)0.3279 (14)0.4913 (12)0.038 (5)*
N10.20195 (14)0.35639 (9)0.43364 (7)0.0293 (2)
N20.08173 (14)0.35293 (9)0.39244 (8)0.0308 (3)
N30.03312 (15)0.35272 (12)0.36100 (10)0.0438 (3)
O10.29982 (9)0.25381 (7)0.11410 (6)0.02326 (18)
O20.53704 (10)0.20693 (7)0.10808 (6)0.02380 (19)
C80.41324 (14)0.36028 (8)0.07267 (8)0.0206 (2)
H810.363 (2)0.4012 (13)0.0309 (12)0.028 (4)*
H820.517 (2)0.3485 (12)0.0540 (11)0.027 (4)*
C90.40358 (13)0.39821 (8)0.16715 (8)0.0179 (2)
C100.51563 (14)0.37881 (8)0.22938 (8)0.0217 (2)
H100.607 (2)0.3453 (13)0.2109 (11)0.028 (4)*
C110.50239 (16)0.40879 (10)0.31829 (9)0.0277 (3)
H110.581 (2)0.3955 (14)0.3619 (14)0.045 (5)*
C120.37921 (17)0.46022 (10)0.34463 (9)0.0305 (3)
H120.366 (2)0.4806 (14)0.4094 (12)0.035 (5)*
C130.26903 (16)0.48192 (9)0.28259 (11)0.0296 (3)
H130.190 (2)0.5175 (15)0.3003 (14)0.046 (6)*
C140.28009 (14)0.45043 (8)0.19401 (9)0.0235 (2)
H140.199 (2)0.4637 (12)0.1515 (12)0.034 (5)*
C150.40318 (13)0.19003 (8)0.11058 (8)0.0190 (2)
H1510.502 (2)0.1840 (12)0.0880 (11)0.028 (4)*
H1520.412 (2)0.2090 (14)0.1757 (13)0.035 (5)*
C160.31125 (13)0.10347 (8)0.09704 (8)0.0200 (2)
C170.31433 (15)0.05780 (8)0.01422 (9)0.0236 (2)
H170.377 (2)0.0794 (13)0.0359 (12)0.032 (5)*
C180.22703 (18)0.02091 (9)0.00042 (10)0.0317 (3)
H180.236 (2)0.0557 (14)0.0594 (14)0.044 (5)*
C190.13615 (17)0.05418 (10)0.06924 (13)0.0354 (3)
H190.074 (3)0.1077 (17)0.0620 (14)0.055 (6)*
C200.13448 (16)0.00994 (10)0.15191 (13)0.0344 (3)
H200.080 (3)0.0337 (18)0.2019 (15)0.057 (6)*
C210.22123 (15)0.06936 (9)0.16595 (10)0.0265 (3)
H210.227 (2)0.0995 (13)0.2226 (12)0.032 (4)*
N40.33057 (11)0.27002 (7)0.06358 (6)0.01650 (18)
H020.235 (2)0.2771 (14)0.0873 (12)0.032 (4)*
H010.324 (2)0.2539 (15)0.0004 (14)0.035 (5)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C70.0179 (5)0.0196 (5)0.0148 (4)0.0012 (4)0.0013 (4)0.0004 (4)
C10.0272 (6)0.0201 (5)0.0170 (5)0.0025 (4)0.0030 (5)0.0005 (4)
C20.0203 (5)0.0198 (5)0.0160 (5)0.0013 (4)0.0008 (4)0.0004 (4)
C30.0189 (5)0.0164 (5)0.0152 (4)0.0027 (4)0.0005 (4)0.0011 (4)
C40.0202 (5)0.0191 (5)0.0210 (5)0.0021 (4)0.0024 (4)0.0036 (4)
C50.0265 (6)0.0240 (5)0.0212 (5)0.0049 (5)0.0070 (5)0.0043 (4)
C60.0352 (7)0.0247 (6)0.0150 (5)0.0059 (5)0.0035 (5)0.0005 (4)
N10.0336 (6)0.0353 (6)0.0190 (5)0.0024 (5)0.0065 (4)0.0041 (4)
N20.0323 (6)0.0349 (6)0.0252 (5)0.0006 (5)0.0120 (5)0.0080 (5)
N30.0283 (6)0.0607 (9)0.0425 (7)0.0043 (6)0.0101 (6)0.0192 (7)
O10.0179 (4)0.0355 (5)0.0164 (3)0.0033 (4)0.0000 (3)0.0014 (3)
O20.0171 (4)0.0321 (5)0.0222 (4)0.0018 (3)0.0024 (3)0.0055 (4)
C80.0242 (5)0.0185 (5)0.0191 (5)0.0068 (4)0.0016 (4)0.0020 (4)
C90.0190 (5)0.0141 (4)0.0204 (5)0.0035 (4)0.0004 (4)0.0007 (4)
C100.0203 (5)0.0209 (5)0.0240 (5)0.0028 (4)0.0024 (4)0.0008 (4)
C110.0297 (7)0.0301 (6)0.0234 (6)0.0072 (5)0.0040 (5)0.0020 (5)
C120.0362 (7)0.0294 (6)0.0259 (6)0.0112 (6)0.0071 (5)0.0087 (5)
C130.0263 (6)0.0224 (6)0.0401 (7)0.0035 (5)0.0085 (6)0.0083 (5)
C140.0205 (5)0.0178 (5)0.0323 (6)0.0002 (4)0.0006 (5)0.0004 (5)
C150.0183 (5)0.0178 (5)0.0211 (5)0.0006 (4)0.0034 (4)0.0001 (4)
C160.0175 (5)0.0168 (5)0.0256 (5)0.0002 (4)0.0022 (4)0.0001 (4)
C170.0267 (6)0.0188 (5)0.0253 (6)0.0004 (5)0.0054 (5)0.0012 (4)
C180.0366 (7)0.0205 (6)0.0381 (7)0.0016 (5)0.0143 (6)0.0048 (5)
C190.0272 (6)0.0194 (6)0.0595 (10)0.0053 (5)0.0104 (7)0.0008 (6)
C200.0237 (6)0.0236 (6)0.0560 (10)0.0021 (5)0.0086 (6)0.0047 (6)
C210.0246 (6)0.0201 (5)0.0350 (7)0.0009 (5)0.0072 (5)0.0008 (5)
N40.0162 (4)0.0173 (4)0.0160 (4)0.0018 (3)0.0005 (3)0.0007 (3)
Geometric parameters (Å, º) top
C7—O21.2568 (14)C11—C121.387 (2)
C7—O11.2654 (14)C11—H110.97 (2)
C7—C31.5180 (15)C12—C131.388 (2)
C1—C61.3915 (18)C12—H121.014 (18)
C1—C21.3947 (16)C13—C141.397 (2)
C1—N11.4389 (16)C13—H130.92 (2)
C2—C31.3938 (16)C14—H140.985 (19)
C2—H20.968 (16)C15—N41.4977 (15)
C3—C41.3967 (16)C15—C161.5095 (16)
C4—C51.3980 (17)C15—H1510.954 (18)
C4—H40.955 (17)C15—H1521.010 (19)
C5—C61.395 (2)C16—C211.3943 (17)
C5—H50.943 (18)C16—C171.3967 (17)
C6—H60.944 (18)C17—C181.3942 (18)
N1—N21.2413 (18)C17—H170.981 (19)
N1—N1i5.7816 (16)C18—C191.393 (2)
N2—N31.1313 (19)C18—H181.02 (2)
C8—N41.5041 (15)C19—C201.385 (3)
C8—C91.5100 (16)C19—H190.96 (2)
C8—H810.966 (19)C20—C211.3990 (19)
C8—H820.986 (18)C20—H200.95 (2)
C9—C101.3944 (16)C21—H210.949 (19)
C9—C141.3978 (17)N4—H020.94 (2)
C10—C111.3961 (18)N4—H010.98 (2)
C10—H100.989 (18)
O2—C7—O1124.74 (10)C13—C12—C11120.02 (12)
O2—C7—C3118.83 (10)C13—C12—H12118.8 (11)
O1—C7—C3116.44 (10)C11—C12—H12121.1 (11)
C6—C1—C2120.61 (11)C12—C13—C14120.19 (12)
C6—C1—N1117.14 (11)C12—C13—H13119.2 (13)
C2—C1—N1122.24 (12)C14—C13—H13120.6 (13)
C1—C2—C3119.99 (11)C13—C14—C9120.05 (12)
C1—C2—H2120.7 (9)C13—C14—H14119.3 (11)
C3—C2—H2119.3 (9)C9—C14—H14120.6 (11)
C2—C3—C4119.76 (10)N4—C15—C16109.70 (9)
C2—C3—C7118.13 (10)N4—C15—H151108.1 (10)
C4—C3—C7122.09 (10)C16—C15—H151112.8 (10)
C5—C4—C3119.85 (11)N4—C15—H152105.8 (11)
C5—C4—H4121.0 (10)C16—C15—H152113.2 (11)
C3—C4—H4118.9 (10)H151—C15—H152106.9 (15)
C6—C5—C4120.44 (11)C21—C16—C17119.54 (11)
C6—C5—H5119.8 (10)C21—C16—C15120.67 (11)
C4—C5—H5119.7 (11)C17—C16—C15119.79 (11)
C1—C6—C5119.31 (11)C18—C17—C16120.17 (13)
C1—C6—H6121.3 (12)C18—C17—H17117.8 (11)
C5—C6—H6119.4 (12)C16—C17—H17122.1 (11)
N2—N1—C1114.07 (10)C19—C18—C17120.05 (13)
N2—N1—N1i145.20 (10)C19—C18—H18121.0 (12)
C1—N1—N1i51.26 (6)C17—C18—H18118.8 (12)
N3—N2—N1174.39 (13)C20—C19—C18119.97 (13)
N4—C8—C9111.64 (9)C20—C19—H19117.6 (13)
N4—C8—H81104.1 (11)C18—C19—H19122.4 (13)
C9—C8—H81110.5 (10)C19—C20—C21120.19 (14)
N4—C8—H82106.9 (10)C19—C20—H20122.2 (14)
C9—C8—H82112.3 (10)C21—C20—H20117.5 (14)
H81—C8—H82111.1 (14)C16—C21—C20120.06 (13)
C10—C9—C14119.33 (11)C16—C21—H21117.3 (11)
C10—C9—C8120.22 (11)C20—C21—H21122.5 (11)
C14—C9—C8120.42 (11)C15—N4—C8114.22 (9)
C11—C10—C9120.32 (11)C15—N4—H02107.9 (12)
C11—C10—H10119.0 (10)C8—N4—H02109.0 (12)
C9—C10—H10120.6 (10)C15—N4—H01107.1 (13)
C12—C11—C10120.04 (13)C8—N4—H01108.7 (12)
C12—C11—H11119.4 (12)H02—N4—H01109.8 (16)
C10—C11—H11120.6 (12)
C6—C1—C2—C31.25 (17)N4—C8—C9—C1483.88 (13)
N1—C1—C2—C3179.88 (11)C14—C9—C10—C111.98 (17)
C1—C2—C3—C40.64 (17)C8—C9—C10—C11175.91 (11)
C1—C2—C3—C7177.77 (10)C9—C10—C11—C121.68 (19)
O2—C7—C3—C2178.98 (11)C10—C11—C12—C130.0 (2)
O1—C7—C3—C20.69 (15)C11—C12—C13—C141.4 (2)
O2—C7—C3—C40.61 (16)C12—C13—C14—C91.08 (19)
O1—C7—C3—C4179.06 (11)C10—C9—C14—C130.60 (17)
C2—C3—C4—C51.88 (16)C8—C9—C14—C13177.28 (11)
C7—C3—C4—C5176.46 (10)N4—C15—C16—C21103.63 (13)
C3—C4—C5—C61.27 (17)N4—C15—C16—C1775.32 (13)
C2—C1—C6—C51.86 (18)C21—C16—C17—C180.51 (18)
N1—C1—C6—C5179.21 (11)C15—C16—C17—C18178.45 (11)
C4—C5—C6—C10.60 (18)C16—C17—C18—C190.1 (2)
C6—C1—N1—N2171.38 (12)C17—C18—C19—C201.1 (2)
C2—C1—N1—N29.72 (18)C18—C19—C20—C211.5 (2)
C6—C1—N1—N1i28.76 (8)C17—C16—C21—C200.15 (19)
C2—C1—N1—N1i152.34 (14)C15—C16—C21—C20178.80 (12)
C1—N1—N2—N3177 (100)C19—C20—C21—C160.8 (2)
N1i—N1—N2—N3121.1 (17)C16—C15—N4—C8179.97 (9)
N4—C8—C9—C1093.99 (13)C9—C8—N4—C1570.61 (13)
Symmetry code: (i) x+1/2, y+1/2, z+1.
Dibenzylammonium 3-azidebenzoate (3a-db-II-i) top
Crystal data top
C21H20N4O2F(000) = 760
Mr = 360.41Dx = 1.247 Mg m3
Monoclinic, P21/cMelting point: not measured K
a = 10.854 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.6662 (17) ÅCell parameters from 8192 reflections
c = 21.081 (4) ŵ = 0.08 mm1
β = 104.51 (3)°T = 78 K
V = 1919.7 (7) Å3Needle, pale-yellow
Z = 40.31 × 0.16 × 0.12 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
5594 independent reflections
Radiation source: rotating anode4774 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
ω scansθmax = 30.0°, θmin = 2.4°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1515
Tmin = 0.975, Tmax = 0.990k = 1212
29789 measured reflectionsl = 2929
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)] = 0.036Hydrogen site location: difference Fourier map
wR(F2) = 0.100Only H-atom coordinates refined
S = 1.05 w = 1/[σ2(Fo2) + (0.0556P)2 + 0.3146P]
where P = (Fo2 + 2Fc2)/3
5594 reflections(Δ/σ)max < 0.001
306 parametersΔρmax = 0.33 e Å3
0 restraintsΔρmin = 0.22 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
O10.13691 (6)0.29862 (7)0.23145 (3)0.02011 (13)
O20.05607 (6)0.07489 (7)0.18594 (3)0.01954 (13)
C70.11946 (7)0.19795 (9)0.18647 (4)0.01607 (15)
C10.19693 (8)0.15944 (9)0.02087 (4)0.01656 (15)
C20.14119 (7)0.13516 (9)0.07295 (4)0.01573 (15)
H20.0761 (11)0.0573 (13)0.0689 (5)0.019*
C30.17939 (7)0.22481 (9)0.12962 (4)0.01475 (15)
C40.27203 (8)0.33943 (10)0.13348 (4)0.01831 (16)
H40.3020 (11)0.4009 (14)0.1746 (6)0.022*
C50.32574 (8)0.36395 (10)0.08067 (4)0.02064 (17)
H50.3886 (12)0.4462 (14)0.0823 (6)0.025*
C60.28934 (8)0.27418 (10)0.02406 (4)0.01921 (16)
H60.3244 (11)0.2939 (14)0.0144 (6)0.023*
N10.15087 (8)0.06217 (10)0.03525 (4)0.02365 (16)
N20.21442 (8)0.06132 (9)0.07687 (4)0.02236 (16)
N30.26382 (10)0.04952 (10)0.11808 (4)0.0319 (2)
N40.07443 (6)0.60347 (8)0.22062 (3)0.01476 (13)
H020.0140 (13)0.5934 (16)0.2484 (7)0.034 (3)*
H010.1099 (12)0.5039 (16)0.2201 (6)0.029 (3)*
C80.17221 (8)0.71933 (9)0.25497 (4)0.01651 (15)
H810.1961 (11)0.6876 (13)0.3021 (6)0.020*
H820.1264 (11)0.8196 (13)0.2521 (6)0.020*
C90.28765 (7)0.72816 (9)0.22725 (4)0.01593 (15)
C100.28730 (8)0.82469 (10)0.17384 (4)0.01951 (16)
H100.2121 (12)0.8863 (14)0.1550 (6)0.023*
C110.39423 (9)0.83345 (11)0.14836 (5)0.02432 (18)
H110.3920 (12)0.9021 (15)0.1109 (6)0.029*
C120.50239 (9)0.74719 (11)0.17641 (5)0.02566 (19)
H120.5786 (13)0.7542 (15)0.1588 (6)0.031*
C130.50395 (8)0.65141 (11)0.22987 (5)0.02480 (19)
H130.5787 (12)0.5906 (15)0.2500 (6)0.030*
C140.39680 (8)0.64185 (10)0.25522 (4)0.02007 (16)
H140.3991 (11)0.5761 (14)0.2921 (6)0.024*
C150.00825 (8)0.65060 (10)0.15210 (4)0.01913 (16)
H1510.0736 (11)0.6551 (14)0.1268 (6)0.023*
H1520.0206 (11)0.7577 (14)0.1550 (6)0.023*
C160.09915 (8)0.54205 (10)0.12129 (4)0.01807 (16)
C170.08819 (9)0.44219 (11)0.07093 (4)0.02378 (18)
H170.0088 (12)0.4401 (15)0.0566 (6)0.029*
C180.18851 (11)0.34402 (11)0.04172 (5)0.0301 (2)
H180.1810 (13)0.2767 (16)0.0070 (7)0.036*
C190.30012 (10)0.34510 (12)0.06284 (5)0.0309 (2)
H190.3695 (13)0.2758 (17)0.0425 (7)0.037*
C200.31160 (9)0.44408 (12)0.11325 (5)0.02638 (19)
H200.3885 (13)0.4447 (15)0.1297 (6)0.032*
C210.21176 (8)0.54264 (11)0.14244 (4)0.02069 (17)
H210.2185 (11)0.6080 (15)0.1786 (6)0.025*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0276 (3)0.0162 (3)0.0176 (3)0.0018 (2)0.0077 (2)0.0014 (2)
O20.0230 (3)0.0166 (3)0.0223 (3)0.0014 (2)0.0118 (2)0.0007 (2)
C70.0172 (3)0.0153 (3)0.0166 (3)0.0037 (3)0.0057 (3)0.0015 (3)
C10.0174 (3)0.0173 (4)0.0150 (3)0.0007 (3)0.0041 (3)0.0007 (3)
C20.0158 (3)0.0150 (3)0.0170 (3)0.0007 (3)0.0053 (3)0.0010 (3)
C30.0148 (3)0.0142 (3)0.0156 (3)0.0018 (3)0.0044 (3)0.0015 (3)
C40.0177 (4)0.0183 (4)0.0180 (4)0.0018 (3)0.0029 (3)0.0005 (3)
C50.0176 (4)0.0225 (4)0.0215 (4)0.0057 (3)0.0042 (3)0.0013 (3)
C60.0179 (4)0.0225 (4)0.0178 (4)0.0027 (3)0.0056 (3)0.0038 (3)
N10.0284 (4)0.0274 (4)0.0179 (3)0.0087 (3)0.0108 (3)0.0054 (3)
N20.0299 (4)0.0198 (3)0.0191 (3)0.0027 (3)0.0094 (3)0.0009 (3)
N30.0457 (5)0.0285 (4)0.0279 (4)0.0059 (4)0.0210 (4)0.0045 (3)
N40.0154 (3)0.0140 (3)0.0155 (3)0.0007 (2)0.0050 (2)0.0007 (2)
C80.0178 (3)0.0155 (3)0.0169 (3)0.0027 (3)0.0055 (3)0.0023 (3)
C90.0160 (3)0.0138 (3)0.0184 (3)0.0022 (3)0.0051 (3)0.0024 (3)
C100.0193 (4)0.0166 (4)0.0239 (4)0.0003 (3)0.0077 (3)0.0018 (3)
C110.0251 (4)0.0222 (4)0.0292 (4)0.0034 (3)0.0135 (4)0.0029 (3)
C120.0196 (4)0.0254 (4)0.0354 (5)0.0033 (3)0.0131 (4)0.0025 (4)
C130.0158 (4)0.0259 (4)0.0321 (5)0.0007 (3)0.0047 (3)0.0013 (4)
C140.0181 (4)0.0199 (4)0.0212 (4)0.0008 (3)0.0031 (3)0.0005 (3)
C150.0181 (4)0.0209 (4)0.0176 (4)0.0019 (3)0.0031 (3)0.0043 (3)
C160.0170 (4)0.0181 (4)0.0174 (4)0.0007 (3)0.0013 (3)0.0030 (3)
C170.0249 (4)0.0231 (4)0.0216 (4)0.0068 (3)0.0025 (3)0.0011 (3)
C180.0380 (5)0.0203 (4)0.0262 (5)0.0048 (4)0.0030 (4)0.0035 (4)
C190.0300 (5)0.0222 (4)0.0321 (5)0.0057 (4)0.0079 (4)0.0033 (4)
C200.0193 (4)0.0282 (5)0.0284 (4)0.0040 (3)0.0001 (3)0.0078 (4)
C210.0176 (4)0.0230 (4)0.0204 (4)0.0000 (3)0.0027 (3)0.0031 (3)
Geometric parameters (Å, º) top
O1—C71.2672 (10)C9—C101.4019 (12)
O2—C71.2677 (10)C10—C111.3979 (12)
C7—C31.5180 (11)C10—H100.973 (12)
C1—C21.3959 (11)C11—C121.3925 (14)
C1—C61.4020 (11)C11—H110.985 (13)
C1—N11.4367 (11)C12—C131.3963 (14)
C2—C31.3980 (11)C12—H120.990 (13)
C2—H20.965 (11)C13—C141.3988 (13)
C3—C41.4012 (11)C13—H130.971 (13)
C4—C51.3964 (12)C14—H140.960 (12)
C4—H41.000 (12)C15—C161.5120 (12)
C5—C61.3962 (12)C15—H1510.989 (12)
C5—H50.981 (12)C15—H1520.987 (12)
C6—H60.993 (12)C16—C171.3978 (12)
N1—N21.2444 (11)C16—C211.4021 (12)
N2—N31.1342 (11)C17—C181.3974 (14)
N4—C151.4998 (11)C17—H170.982 (13)
N4—C81.5079 (11)C18—C191.3915 (17)
N4—H020.986 (13)C18—H180.956 (14)
N4—H010.946 (14)C19—C201.3955 (16)
C8—C91.5113 (12)C19—H190.975 (14)
C8—H811.001 (11)C20—C211.3959 (13)
C8—H820.995 (12)C20—H200.980 (13)
C9—C141.4002 (12)C21—H210.968 (13)
O1—C7—O2124.39 (8)C11—C10—C9120.38 (8)
O1—C7—C3118.16 (7)C11—C10—H10120.4 (7)
O2—C7—C3117.45 (7)C9—C10—H10119.2 (7)
C2—C1—C6121.01 (8)C12—C11—C10120.04 (8)
C2—C1—N1115.42 (7)C12—C11—H11120.9 (7)
C6—C1—N1123.55 (8)C10—C11—H11119.1 (7)
C1—C2—C3119.61 (7)C11—C12—C13120.02 (8)
C1—C2—H2119.1 (7)C11—C12—H12120.2 (8)
C3—C2—H2121.3 (7)C13—C12—H12119.8 (8)
C2—C3—C4119.89 (7)C12—C13—C14120.03 (9)
C2—C3—C7119.70 (7)C12—C13—H13120.9 (8)
C4—C3—C7120.41 (7)C14—C13—H13119.0 (8)
C5—C4—C3119.91 (8)C13—C14—C9120.28 (8)
C5—C4—H4120.0 (7)C13—C14—H14119.3 (7)
C3—C4—H4120.0 (7)C9—C14—H14120.4 (7)
C4—C5—C6120.76 (8)N4—C15—C16112.08 (7)
C4—C5—H5120.5 (7)N4—C15—H151107.2 (7)
C6—C5—H5118.7 (7)C16—C15—H151111.9 (7)
C5—C6—C1118.81 (8)N4—C15—H152106.3 (7)
C5—C6—H6121.1 (7)C16—C15—H152112.9 (7)
C1—C6—H6120.0 (7)H151—C15—H152106.1 (10)
N2—N1—C1116.36 (7)C17—C16—C21119.39 (8)
N2—N1—N1i153.58 (7)C17—C16—C15120.55 (8)
C1—N1—N1i90.02 (5)C21—C16—C15120.06 (8)
N3—N2—N1172.98 (10)C18—C17—C16120.43 (9)
C15—N4—C8113.00 (7)C18—C17—H17120.0 (7)
C15—N4—H02111.5 (8)C16—C17—H17119.5 (7)
C8—N4—H02105.5 (8)C19—C18—C17119.98 (9)
C15—N4—H01109.6 (8)C19—C18—H18119.8 (8)
C8—N4—H01111.9 (8)C17—C18—H18120.2 (8)
H02—N4—H01105.0 (11)C18—C19—C20119.93 (9)
N4—C8—C9113.58 (6)C18—C19—H19119.6 (8)
N4—C8—H81105.7 (7)C20—C19—H19120.5 (8)
C9—C8—H81111.4 (7)C19—C20—C21120.27 (9)
N4—C8—H82105.7 (7)C19—C20—H20121.2 (8)
C9—C8—H82112.5 (7)C21—C20—H20118.5 (8)
H81—C8—H82107.5 (9)C20—C21—C16120.00 (9)
C14—C9—C10119.25 (8)C20—C21—H21120.1 (7)
C14—C9—C8120.41 (7)C16—C21—H21119.8 (7)
C10—C9—C8120.33 (7)
C6—C1—C2—C31.03 (12)N4—C8—C9—C1494.60 (9)
N1—C1—C2—C3179.70 (7)N4—C8—C9—C1086.36 (9)
C1—C2—C3—C40.77 (12)C14—C9—C10—C110.67 (13)
C1—C2—C3—C7179.64 (7)C8—C9—C10—C11179.72 (8)
O1—C7—C3—C2166.55 (7)C9—C10—C11—C120.63 (14)
O2—C7—C3—C214.11 (11)C10—C11—C12—C130.24 (14)
O1—C7—C3—C413.04 (11)C11—C12—C13—C140.11 (14)
O2—C7—C3—C4166.31 (7)C12—C13—C14—C90.07 (14)
C2—C3—C4—C50.11 (12)C10—C9—C14—C130.32 (13)
C7—C3—C4—C5179.47 (7)C8—C9—C14—C13179.37 (8)
C3—C4—C5—C60.76 (13)C8—N4—C15—C16173.66 (7)
C4—C5—C6—C10.51 (13)N4—C15—C16—C17109.06 (9)
C2—C1—C6—C50.40 (13)N4—C15—C16—C2171.97 (10)
N1—C1—C6—C5178.95 (8)C21—C16—C17—C180.17 (13)
C2—C1—N1—N2167.14 (8)C15—C16—C17—C18178.81 (8)
C6—C1—N1—N214.23 (13)C16—C17—C18—C190.12 (14)
C2—C1—N1—N1i14.32 (8)C17—C18—C19—C200.11 (14)
C6—C1—N1—N1i164.30 (7)C18—C19—C20—C210.30 (14)
C1—N1—N2—N3177.0 (8)C19—C20—C21—C160.25 (13)
N1i—N1—N2—N36.3 (9)C17—C16—C21—C200.02 (13)
C15—N4—C8—C969.24 (9)C15—C16—C21—C20179.00 (8)
Symmetry code: (i) x, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H01···O10.946 (14)1.809 (14)2.7228 (10)161.5 (11)
N4—H02···O2ii0.986 (13)1.746 (14)2.7103 (11)164.8 (13)
Symmetry code: (ii) x, y+1/2, z+1/2.
Dicyclohexylammonium 3-azidebenzoate (3a-dc-i) top
Crystal data top
C19H28N4O2Z = 2
Mr = 344.45F(000) = 372
Triclinic, P1Dx = 1.259 Mg m3
a = 9.1925 (5) ÅMelting point: not measured K
b = 10.1813 (5) ÅMo Kα radiation, λ = 0.71073 Å
c = 11.3543 (6) ÅCell parameters from 6022 reflections
α = 110.816 (1)°µ = 0.08 mm1
β = 103.168 (2)°T = 82 K
γ = 103.370 (1)°Plate, pale-yellow
V = 908.51 (8) Å30.44 × 0.38 × 0.26 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
5259 independent reflections
Radiation source: rotating anode4561 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.023
ω scansθmax = 30.0°, θmin = 2.3°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1212
Tmin = 0.964, Tmax = 0.979k = 1414
14513 measured reflectionsl = 1515
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)] = 0.034Hydrogen site location: difference Fourier map
wR(F2) = 0.100Only H-atom coordinates refined
S = 1.06 w = 1/[σ2(Fo2) + (0.0603P)2 + 0.1086P]
where P = (Fo2 + 2Fc2)/3
5259 reflections(Δ/σ)max < 0.001
312 parametersΔρmax = 0.35 e Å3
0 restraintsΔρmin = 0.24 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
C70.70855 (8)0.21243 (8)0.35622 (7)0.01268 (14)
C10.32743 (9)0.12205 (8)0.23699 (8)0.01447 (15)
C20.45174 (9)0.01540 (8)0.31880 (7)0.01310 (14)
H20.4580 (13)0.0764 (12)0.4099 (11)0.016*
C30.57277 (8)0.06267 (8)0.27095 (7)0.01286 (14)
C40.56854 (9)0.02721 (9)0.14289 (8)0.01656 (15)
H40.6537 (14)0.0086 (13)0.1104 (11)0.020*
C50.44280 (10)0.16295 (9)0.06162 (8)0.01891 (16)
H50.4334 (14)0.2283 (13)0.0342 (12)0.023*
C60.32247 (10)0.21067 (9)0.10857 (8)0.01750 (15)
H60.2340 (14)0.3066 (13)0.0532 (11)0.021*
O10.70011 (7)0.29827 (6)0.46504 (6)0.01637 (12)
O20.81882 (7)0.23951 (7)0.30949 (6)0.01751 (13)
N10.19848 (8)0.18239 (8)0.27522 (7)0.01976 (15)
N20.19097 (8)0.10182 (8)0.38449 (7)0.01736 (14)
N30.16737 (9)0.04166 (8)0.48004 (8)0.02245 (16)
C80.19607 (8)0.33539 (8)0.51332 (7)0.01066 (13)
H80.1478 (13)0.2249 (12)0.4671 (10)0.013*
C90.37823 (8)0.38432 (8)0.56345 (7)0.01276 (14)
H910.4184 (13)0.4932 (12)0.5983 (10)0.015*
H920.4197 (13)0.3430 (12)0.4900 (11)0.015*
C100.43700 (9)0.33466 (9)0.67339 (8)0.01423 (14)
H1010.3959 (13)0.2232 (13)0.6352 (11)0.017*
H1020.5546 (13)0.3669 (12)0.7044 (11)0.017*
C110.37735 (10)0.39622 (9)0.79020 (8)0.01746 (15)
H1110.4231 (14)0.5096 (13)0.8321 (12)0.021*
H1120.4142 (14)0.3637 (13)0.8620 (11)0.021*
C120.19439 (10)0.34459 (10)0.73900 (8)0.01672 (15)
H1210.1516 (14)0.2336 (13)0.7038 (11)0.020*
H1220.1563 (14)0.3861 (13)0.8138 (11)0.020*
C130.13321 (9)0.39282 (8)0.62883 (7)0.01319 (14)
H1310.0127 (13)0.3532 (12)0.5901 (11)0.016*
H1320.1684 (13)0.5036 (12)0.6655 (11)0.016*
C140.18670 (8)0.35429 (8)0.29082 (7)0.01063 (13)
H140.3007 (13)0.4071 (12)0.3229 (10)0.013*
C150.09930 (9)0.41119 (8)0.19752 (7)0.01276 (14)
H1510.1219 (13)0.5200 (12)0.2462 (11)0.015*
H1520.0179 (13)0.3587 (12)0.1705 (11)0.015*
C160.14699 (9)0.37695 (9)0.07112 (7)0.01443 (14)
H1610.0811 (13)0.4088 (13)0.0098 (11)0.017*
H1620.2609 (14)0.4398 (13)0.0977 (11)0.017*
C170.12389 (10)0.21029 (9)0.00144 (8)0.01670 (15)
H1710.1639 (14)0.1907 (13)0.0790 (11)0.020*
H1720.0067 (14)0.1506 (13)0.0381 (12)0.020*
C180.20933 (10)0.15616 (9)0.09535 (8)0.01642 (15)
H1810.3260 (14)0.2096 (13)0.1283 (11)0.020*
H1820.1905 (14)0.0468 (13)0.0484 (11)0.020*
C190.15390 (9)0.18612 (8)0.21759 (7)0.01370 (14)
H1910.0384 (13)0.1314 (12)0.1899 (11)0.016*
H1920.2127 (13)0.1476 (12)0.2772 (11)0.016*
N40.13682 (7)0.39406 (7)0.41333 (6)0.01020 (12)
H1N0.0246 (14)0.3568 (13)0.3842 (11)0.021 (3)*
H2N0.1767 (15)0.4977 (14)0.4572 (12)0.024 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C70.0105 (3)0.0118 (3)0.0152 (3)0.0034 (2)0.0029 (2)0.0064 (3)
C10.0116 (3)0.0134 (3)0.0187 (3)0.0038 (3)0.0033 (3)0.0086 (3)
C20.0120 (3)0.0120 (3)0.0148 (3)0.0043 (3)0.0034 (2)0.0058 (3)
C30.0112 (3)0.0111 (3)0.0154 (3)0.0041 (2)0.0030 (2)0.0055 (3)
C40.0160 (3)0.0153 (3)0.0170 (3)0.0046 (3)0.0064 (3)0.0055 (3)
C50.0205 (4)0.0151 (3)0.0160 (3)0.0045 (3)0.0047 (3)0.0030 (3)
C60.0158 (3)0.0132 (3)0.0185 (4)0.0028 (3)0.0019 (3)0.0052 (3)
O10.0164 (3)0.0126 (2)0.0173 (3)0.0034 (2)0.0064 (2)0.0039 (2)
O20.0123 (3)0.0191 (3)0.0184 (3)0.0019 (2)0.0060 (2)0.0069 (2)
N10.0162 (3)0.0162 (3)0.0223 (3)0.0001 (2)0.0064 (3)0.0070 (3)
N20.0125 (3)0.0150 (3)0.0246 (3)0.0023 (2)0.0050 (2)0.0110 (3)
N30.0203 (3)0.0193 (3)0.0278 (4)0.0050 (3)0.0097 (3)0.0103 (3)
C80.0106 (3)0.0121 (3)0.0108 (3)0.0042 (2)0.0038 (2)0.0063 (2)
C90.0102 (3)0.0156 (3)0.0145 (3)0.0049 (3)0.0044 (2)0.0083 (3)
C100.0124 (3)0.0163 (3)0.0148 (3)0.0054 (3)0.0031 (3)0.0083 (3)
C110.0176 (3)0.0216 (4)0.0131 (3)0.0070 (3)0.0031 (3)0.0085 (3)
C120.0177 (3)0.0233 (4)0.0151 (3)0.0088 (3)0.0080 (3)0.0121 (3)
C130.0134 (3)0.0167 (3)0.0128 (3)0.0066 (3)0.0064 (3)0.0080 (3)
C140.0108 (3)0.0118 (3)0.0100 (3)0.0039 (2)0.0044 (2)0.0049 (2)
C150.0151 (3)0.0138 (3)0.0121 (3)0.0067 (3)0.0054 (2)0.0069 (3)
C160.0173 (3)0.0154 (3)0.0125 (3)0.0055 (3)0.0063 (3)0.0073 (3)
C170.0223 (4)0.0163 (3)0.0117 (3)0.0067 (3)0.0072 (3)0.0054 (3)
C180.0223 (4)0.0160 (3)0.0150 (3)0.0099 (3)0.0100 (3)0.0066 (3)
C190.0177 (3)0.0129 (3)0.0132 (3)0.0072 (3)0.0073 (3)0.0060 (3)
N40.0104 (3)0.0112 (3)0.0101 (3)0.0042 (2)0.0041 (2)0.0051 (2)
Geometric parameters (Å, º) top
C7—O11.2665 (9)C11—H1111.015 (12)
C7—O21.2668 (9)C11—H1121.003 (12)
C7—C31.5298 (10)C12—C131.5382 (10)
C1—C61.3993 (11)C12—H1210.997 (12)
C1—C21.4071 (10)C12—H1220.986 (11)
C1—N11.4346 (10)C13—H1311.014 (11)
C2—C31.4065 (10)C13—H1320.993 (11)
C2—H20.979 (11)C14—N41.5116 (9)
C3—C41.4019 (10)C14—C191.5327 (10)
C4—C51.4023 (11)C14—C151.5386 (10)
C4—H40.989 (12)C14—H140.973 (11)
C5—C61.3957 (12)C15—C161.5412 (10)
C5—H51.025 (11)C15—H1510.991 (11)
C6—H60.987 (12)C15—H1521.004 (11)
N1—N21.2486 (10)C16—C171.5372 (11)
N2—N31.1382 (11)C16—H1611.008 (11)
C8—N41.5143 (9)C16—H1621.003 (12)
C8—C131.5337 (10)C17—C181.5381 (11)
C8—C91.5344 (10)C17—H1711.003 (11)
C8—H80.991 (11)C17—H1721.008 (12)
C9—C101.5406 (10)C18—C191.5402 (10)
C9—H910.976 (11)C18—H1810.994 (12)
C9—H920.994 (11)C18—H1821.000 (11)
C10—C111.5337 (11)C19—H1910.994 (11)
C10—H1010.998 (11)C19—H1921.012 (11)
C10—H1020.990 (11)N4—H1N0.944 (12)
C11—C121.5399 (11)N4—H2N0.928 (13)
O1—C7—O2126.05 (7)C11—C12—H122110.0 (7)
O1—C7—C3117.77 (6)H121—C12—H122107.0 (9)
O2—C7—C3116.18 (7)C6—C13—C12111.18 (6)
C6—C1—C2120.65 (7)C6—C13—H131107.8 (6)
C6—C1—N1114.95 (7)C12—C13—H131111.6 (6)
C2—C1—N1124.40 (7)C6—C13—H132108.1 (6)
C3—C2—C1119.36 (7)C12—C13—H132110.5 (6)
C3—C2—H2119.4 (6)H131—C13—H132107.6 (9)
C1—C2—H2121.1 (6)N4—C14—C19112.60 (6)
C4—C3—C2119.87 (7)N4—C14—C15108.14 (5)
C4—C3—C7119.28 (7)C19—C14—C15111.00 (6)
C2—C3—C7120.84 (7)N4—C14—H14106.2 (6)
C3—C4—C5120.20 (7)C19—C14—H14108.9 (6)
C3—C4—H4118.7 (7)C15—C14—H14109.9 (6)
C5—C4—H4121.0 (7)C14—C15—C16111.01 (6)
C6—C5—C4120.22 (7)C14—C15—H151110.0 (6)
C6—C5—H5117.8 (7)C16—C15—H151110.6 (6)
C4—C5—H5121.9 (7)C14—C15—H152107.8 (6)
C5—C6—C1119.68 (7)C16—C15—H152109.3 (6)
C5—C6—H6121.2 (7)H151—C15—H152108.1 (9)
C1—C6—H6119.1 (7)C17—C16—C15111.83 (6)
N2—N1—C1117.16 (7)C17—C16—H161110.5 (6)
N3—N2—N1171.75 (8)C15—C16—H161108.4 (6)
N4—C8—C13107.56 (5)C17—C16—H162110.2 (6)
N4—C8—C9111.33 (6)C15—C16—H162108.8 (6)
C13—C8—C9111.57 (6)H161—C16—H162106.9 (9)
N4—C8—H8107.0 (6)C16—C17—C18110.97 (6)
C13—C8—H8108.5 (6)C16—C17—H171111.2 (7)
C9—C8—H8110.7 (6)C18—C17—H171109.5 (7)
C6—C9—C10110.60 (6)C16—C17—H172108.8 (7)
C6—C9—H91106.7 (6)C18—C17—H172108.7 (7)
C10—C9—H91110.9 (6)H171—C17—H172107.7 (9)
C6—C9—H92112.1 (6)C17—C18—C19111.51 (6)
C10—C9—H92108.8 (6)C17—C18—H181109.7 (7)
H91—C9—H92107.7 (9)C19—C18—H181108.2 (6)
C11—C10—C9111.16 (6)C17—C18—H182110.6 (7)
C11—C10—H101108.2 (6)C19—C18—H182109.4 (7)
C9—C10—H101109.4 (6)H181—C18—H182107.4 (9)
C11—C10—H102111.3 (6)C14—C19—C18109.03 (6)
C9—C10—H102109.5 (7)C14—C19—H191109.1 (6)
H101—C10—H102107.2 (9)C18—C19—H191111.1 (6)
C10—C11—C12110.10 (6)C14—C19—H192111.9 (6)
C10—C11—H111108.5 (7)C18—C19—H192108.2 (6)
C12—C11—H111109.6 (7)H191—C19—H192107.5 (9)
C10—C11—H112111.8 (6)C14—N4—C6117.34 (5)
C12—C11—H112109.5 (7)C14—N4—H1N108.1 (7)
H111—C11—H112107.3 (9)C6—N4—H1N106.9 (7)
C13—C12—C11111.07 (6)C14—N4—H2N105.4 (7)
C13—C12—H121110.3 (7)C6—N4—H2N107.6 (7)
C11—C12—H121108.5 (7)H1N—N4—H2N111.7 (10)
C13—C12—H122109.8 (7)
C6—C1—C2—C30.73 (11)C8—C9—C10—C1156.76 (8)
N1—C1—C2—C3179.46 (7)C9—C10—C11—C1257.53 (8)
C1—C2—C3—C40.06 (11)C10—C11—C12—C1356.87 (8)
C1—C2—C3—C7179.13 (6)N4—C8—C13—C12177.31 (6)
O1—C7—C3—C4172.53 (7)C9—C8—C13—C1254.94 (8)
O2—C7—C3—C46.57 (10)C11—C12—C13—C655.71 (8)
O1—C7—C3—C26.66 (10)N4—C14—C15—C16178.95 (6)
O2—C7—C3—C2174.24 (7)C19—C14—C15—C1657.08 (8)
C2—C3—C4—C50.96 (12)C14—C15—C16—C1753.71 (8)
C7—C3—C4—C5178.24 (7)C15—C16—C17—C1853.06 (8)
C3—C4—C5—C61.09 (12)C16—C17—C18—C1955.98 (9)
C4—C5—C6—C10.30 (12)N4—C14—C19—C18179.58 (6)
C2—C1—C6—C50.61 (12)C15—C14—C19—C1859.03 (8)
N1—C1—C6—C5179.57 (7)C17—C18—C19—C1458.68 (8)
C6—C1—N1—N2174.40 (7)C19—C14—N4—C851.17 (8)
C2—C1—N1—N25.42 (11)C15—C14—N4—C8174.17 (6)
C1—N1—N2—N3175.5 (5)C13—C6—N4—C14178.82 (6)
N4—C8—C9—C10175.39 (6)O2—C6—N4—C1456.30 (8)
C13—C8—C9—C1055.21 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H1N···O2i0.944 (12)1.797 (12)2.7194 (8)164.9 (11)
N4—H2N···O1ii0.928 (13)1.879 (13)2.7888 (8)166.3 (11)
Symmetry codes: (i) x1, y, z; (ii) x+1, y+1, z+1.
N-benzyl-2-phenylethylammonium 4-azidebenzoate (4a-bp-i) top
Crystal data top
C22H22N4O2Z = 2
Mr = 374.44F(000) = 396
Triclinic, P1Dx = 1.253 Mg m3
a = 8.0615 (2) ÅMelting point: not measured K
b = 10.3615 (2) ÅMo Kα radiation, λ = 0.71073 Å
c = 13.5356 (4) ÅCell parameters from 6018 reflections
α = 72.503 (1)°µ = 0.08 mm1
β = 72.933 (1)°T = 92 K
γ = 70.506 (1)°Plate, pale-yellow
V = 992.76 (4) Å30.31 × 0.12 × 0.08 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
5766 independent reflections
Radiation source: rotating anode4057 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.053
ω scansθmax = 30.0°, θmin = 1.6°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1111
Tmin = 0.975, Tmax = 0.993k = 1414
15962 measured reflectionsl = 1818
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)] = 0.050Hydrogen site location: difference Fourier map
wR(F2) = 0.148Only H-atom coordinates refined
S = 1.03 w = 1/[σ2(Fo2) + (0.0855P)2]
where P = (Fo2 + 2Fc2)/3
5766 reflections(Δ/σ)max < 0.001
319 parametersΔρmax = 0.40 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
C10.74869 (15)0.00293 (12)0.52514 (9)0.0230 (2)
C20.66148 (16)0.10149 (12)0.58242 (9)0.0245 (2)
H20.567 (2)0.1882 (15)0.5564 (11)0.029*
C30.70655 (16)0.08587 (12)0.67811 (9)0.0243 (2)
H30.650 (2)0.1543 (16)0.7150 (12)0.029*
C40.83763 (15)0.03191 (12)0.71663 (9)0.0230 (2)
C50.92501 (16)0.13450 (12)0.65719 (9)0.0241 (2)
H51.020 (2)0.2167 (15)0.6795 (12)0.029*
C60.87929 (16)0.12180 (12)0.56236 (9)0.0241 (2)
H60.939 (2)0.1914 (16)0.5195 (12)0.029*
C70.88465 (18)0.04706 (13)0.82082 (9)0.0282 (3)
N10.71091 (15)0.00314 (11)0.42634 (8)0.0287 (2)
N20.61219 (15)0.11711 (11)0.38672 (8)0.0293 (2)
N30.52390 (18)0.21433 (12)0.34259 (10)0.0391 (3)
O20.77098 (14)0.02808 (10)0.88220 (7)0.0383 (2)
O11.03312 (14)0.13148 (10)0.83829 (8)0.0389 (3)
N40.75323 (14)0.07712 (10)0.06816 (8)0.0262 (2)
H010.792 (2)0.0517 (15)0.0021 (12)0.031*
H020.844 (2)0.0990 (16)0.0848 (12)0.031*
C90.66866 (16)0.33067 (13)0.01742 (10)0.0288 (3)
C100.64991 (18)0.35859 (14)0.12205 (10)0.0343 (3)
H100.592 (2)0.2991 (17)0.1427 (13)0.041*
C110.7074 (2)0.46757 (16)0.19835 (12)0.0468 (4)
H110.696 (3)0.489 (2)0.2740 (16)0.056*
C120.7841 (2)0.54888 (17)0.17177 (16)0.0564 (5)
H120.825 (3)0.621 (2)0.2236 (17)0.068*
C130.8065 (2)0.52141 (16)0.06864 (18)0.0535 (5)
H130.862 (3)0.570 (2)0.0520 (17)0.064*
C140.74753 (19)0.41174 (15)0.00941 (13)0.0399 (3)
H140.766 (2)0.3941 (19)0.0821 (15)0.048*
C80.60335 (18)0.21146 (13)0.06385 (10)0.0316 (3)
H810.567 (2)0.2277 (17)0.1372 (13)0.038*
H820.495 (2)0.1929 (17)0.0431 (12)0.038*
C170.81127 (16)0.29394 (12)0.24357 (10)0.0281 (3)
C180.8430 (2)0.30448 (14)0.34206 (11)0.0358 (3)
H180.895 (2)0.2346 (18)0.3501 (13)0.043*
C190.8016 (2)0.41065 (17)0.42900 (13)0.0523 (5)
H190.822 (3)0.417 (2)0.4979 (17)0.063*
C200.7294 (2)0.50740 (18)0.41942 (19)0.0646 (6)
H200.700 (3)0.582 (2)0.4825 (18)0.078*
C210.6957 (2)0.49794 (18)0.3224 (2)0.0662 (6)
H210.649 (3)0.554 (2)0.3083 (18)0.079*
C220.7375 (2)0.39237 (16)0.23419 (16)0.0444 (4)
H220.717 (3)0.385 (2)0.1652 (16)0.053*
C150.69815 (18)0.04372 (13)0.15029 (10)0.0293 (3)
H1510.585 (2)0.0544 (16)0.1329 (12)0.035*
H1520.669 (2)0.0169 (16)0.2163 (13)0.035*
C160.85513 (18)0.17717 (13)0.15046 (10)0.0303 (3)
H1610.883 (2)0.2081 (16)0.0809 (13)0.036*
H1620.963 (2)0.1550 (16)0.1562 (12)0.036*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0226 (5)0.0246 (5)0.0209 (5)0.0098 (4)0.0045 (4)0.0001 (4)
C20.0215 (5)0.0216 (5)0.0255 (6)0.0042 (4)0.0057 (4)0.0007 (4)
C30.0244 (6)0.0211 (5)0.0228 (5)0.0045 (4)0.0026 (4)0.0026 (4)
C40.0227 (5)0.0219 (5)0.0200 (5)0.0064 (4)0.0032 (4)0.0007 (4)
C50.0220 (5)0.0206 (5)0.0248 (5)0.0044 (4)0.0056 (4)0.0009 (4)
C60.0242 (6)0.0214 (5)0.0243 (6)0.0055 (4)0.0040 (4)0.0036 (4)
C70.0357 (7)0.0236 (6)0.0209 (5)0.0057 (5)0.0082 (5)0.0009 (4)
N10.0320 (6)0.0281 (5)0.0259 (5)0.0076 (4)0.0114 (4)0.0014 (4)
N20.0349 (6)0.0298 (5)0.0265 (5)0.0153 (5)0.0114 (4)0.0011 (4)
N30.0501 (7)0.0320 (6)0.0376 (6)0.0148 (5)0.0228 (6)0.0058 (5)
O20.0447 (6)0.0398 (5)0.0234 (4)0.0029 (4)0.0062 (4)0.0079 (4)
O10.0459 (6)0.0335 (5)0.0330 (5)0.0041 (4)0.0219 (4)0.0048 (4)
N40.0259 (5)0.0245 (5)0.0178 (5)0.0002 (4)0.0026 (4)0.0005 (4)
C90.0233 (6)0.0240 (6)0.0252 (6)0.0047 (4)0.0041 (5)0.0009 (4)
C100.0295 (7)0.0316 (6)0.0258 (6)0.0044 (5)0.0053 (5)0.0013 (5)
C110.0377 (8)0.0379 (8)0.0320 (7)0.0070 (6)0.0021 (6)0.0104 (6)
C120.0310 (8)0.0315 (8)0.0684 (12)0.0031 (6)0.0046 (7)0.0153 (7)
C130.0285 (7)0.0268 (7)0.0977 (15)0.0002 (6)0.0153 (8)0.0103 (8)
C140.0323 (7)0.0282 (7)0.0520 (9)0.0066 (5)0.0165 (6)0.0078 (6)
C80.0295 (6)0.0259 (6)0.0236 (6)0.0035 (5)0.0020 (5)0.0010 (5)
C170.0228 (6)0.0193 (5)0.0326 (6)0.0004 (4)0.0015 (5)0.0035 (4)
C180.0395 (8)0.0262 (6)0.0296 (7)0.0016 (5)0.0019 (5)0.0025 (5)
C190.0480 (9)0.0371 (8)0.0366 (8)0.0059 (7)0.0039 (7)0.0097 (6)
C200.0380 (9)0.0334 (8)0.0794 (14)0.0006 (7)0.0051 (9)0.0213 (8)
C210.0365 (9)0.0282 (8)0.123 (2)0.0134 (7)0.0122 (10)0.0019 (10)
C220.0313 (7)0.0326 (7)0.0693 (11)0.0049 (6)0.0151 (7)0.0114 (7)
C150.0299 (6)0.0249 (6)0.0219 (6)0.0019 (5)0.0008 (5)0.0001 (4)
C160.0292 (7)0.0250 (6)0.0254 (6)0.0006 (5)0.0004 (5)0.0022 (5)
Geometric parameters (Å, º) top
C1—C21.3938 (17)C11—H111.005 (19)
C1—C61.3971 (16)C12—C131.392 (3)
C1—N11.4356 (15)C12—H120.93 (2)
C2—C31.3952 (17)C13—C141.406 (2)
C2—H21.010 (14)C13—H130.88 (2)
C3—C41.3992 (16)C14—H140.993 (18)
C3—H30.907 (15)C8—H810.998 (16)
C4—C51.3983 (17)C8—H821.079 (16)
C4—C71.5159 (16)C17—C221.392 (2)
C5—C61.3945 (17)C17—C181.396 (2)
C5—H50.976 (15)C17—C161.5114 (17)
C6—H60.972 (15)C18—C191.394 (2)
C7—O11.2636 (15)C18—H180.993 (17)
C7—O21.2657 (15)C19—C201.369 (3)
N1—N21.2482 (14)C19—H190.98 (2)
N2—N31.1346 (15)C20—C211.386 (3)
N4—C151.4983 (16)C20—H200.99 (2)
N4—C81.5069 (15)C21—C221.400 (3)
N4—H010.996 (15)C21—H210.88 (2)
N4—H020.938 (16)C22—H220.971 (19)
C9—C141.385 (2)C15—C161.5315 (17)
C9—C101.4009 (18)C15—H1511.054 (16)
C9—C81.5133 (18)C15—H1520.955 (16)
C10—C111.387 (2)C16—H1611.025 (16)
C10—H101.022 (17)C16—H1620.996 (16)
C11—C121.372 (3)
C2—C1—C6120.93 (10)C12—C13—H13120.7 (14)
C2—C1—N1123.11 (10)C14—C13—H13119.1 (14)
C6—C1—N1115.96 (10)C9—C14—C13119.47 (15)
C1—C2—C3118.96 (10)C9—C14—H14122.2 (10)
C1—C2—H2121.8 (8)C13—C14—H14118.4 (11)
C3—C2—H2119.2 (8)N4—C8—C9110.35 (10)
C2—C3—C4121.10 (11)N4—C8—H81105.1 (9)
C2—C3—H3118.8 (9)C9—C8—H81112.2 (9)
C4—C3—H3120.1 (9)N4—C8—H82107.0 (9)
C5—C4—C3118.95 (11)C9—C8—H82110.9 (8)
C5—C4—C7120.72 (10)H81—C8—H82111.0 (13)
C3—C4—C7120.33 (10)C22—C17—C18118.34 (13)
C6—C5—C4120.68 (10)C22—C17—C16121.45 (13)
C6—C5—H5117.4 (8)C18—C17—C16120.20 (12)
C4—C5—H5121.9 (8)C19—C18—C17120.93 (16)
C5—C6—C1119.35 (11)C19—C18—H18119.8 (10)
C5—C6—H6122.1 (9)C17—C18—H18119.3 (10)
C1—C6—H6118.5 (9)C20—C19—C18120.56 (18)
O1—C7—O2125.90 (11)C20—C19—H19118.9 (12)
O1—C7—C4117.71 (11)C18—C19—H19120.5 (12)
O2—C7—C4116.38 (11)C19—C20—C21119.30 (16)
N2—N1—C1115.54 (10)C19—C20—H20119.2 (13)
N3—N2—N1172.92 (13)C21—C20—H20121.5 (13)
C15—N4—C8112.72 (9)C20—C21—C22120.81 (18)
C15—N4—H01108.1 (9)C20—C21—H21126.2 (16)
C8—N4—H01109.5 (9)C22—C21—H21113.0 (16)
C15—N4—H02110.7 (9)C17—C22—C21120.06 (18)
C8—N4—H02103.8 (9)C17—C22—H22117.8 (11)
H01—N4—H02112.0 (13)C21—C22—H22122.2 (11)
C14—C9—C10119.50 (13)N4—C15—C16110.34 (10)
C14—C9—C8121.36 (12)N4—C15—H151107.1 (8)
C10—C9—C8119.15 (13)C16—C15—H151112.5 (9)
C11—C10—C9120.61 (15)N4—C15—H152104.9 (9)
C11—C10—H10119.3 (9)C16—C15—H152109.7 (9)
C9—C10—H10120.1 (9)H151—C15—H152112.0 (13)
C12—C11—C10120.03 (15)C17—C16—C15110.85 (10)
C12—C11—H11118.0 (11)C17—C16—H161110.0 (9)
C10—C11—H11122.0 (11)C15—C16—H161109.6 (9)
C11—C12—C13120.22 (15)C17—C16—H162109.1 (9)
C11—C12—H12119.7 (13)C15—C16—H162108.1 (9)
C13—C12—H12120.0 (13)H161—C16—H162109.2 (13)
C12—C13—C14120.17 (17)
C6—C1—C2—C30.04 (17)C10—C11—C12—C130.8 (2)
N1—C1—C2—C3179.60 (10)C11—C12—C13—C141.2 (2)
C1—C2—C3—C40.32 (18)C10—C9—C14—C130.42 (18)
C2—C3—C4—C50.48 (17)C8—C9—C14—C13179.94 (12)
C2—C3—C4—C7179.95 (11)C12—C13—C14—C90.6 (2)
C3—C4—C5—C61.65 (17)C15—N4—C8—C9177.89 (11)
C7—C4—C5—C6178.78 (11)C14—C9—C8—N488.51 (14)
C4—C5—C6—C12.01 (18)C10—C9—C8—N491.01 (14)
C2—C1—C6—C51.19 (17)C22—C17—C18—C190.1 (2)
N1—C1—C6—C5179.22 (10)C16—C17—C18—C19179.34 (12)
C5—C4—C7—O118.61 (17)C17—C18—C19—C200.2 (2)
C3—C4—C7—O1160.95 (12)C18—C19—C20—C210.7 (2)
C5—C4—C7—O2162.15 (12)C19—C20—C21—C221.1 (3)
C3—C4—C7—O218.29 (17)C18—C17—C22—C210.5 (2)
C2—C1—N1—N29.41 (17)C16—C17—C22—C21178.98 (13)
C6—C1—N1—N2171.01 (11)C20—C21—C22—C170.9 (2)
C1—N1—N2—N3178.3 (10)C8—N4—C15—C16179.62 (11)
C14—C9—C10—C110.83 (18)C22—C17—C16—C1593.70 (15)
C8—C9—C10—C11179.64 (11)C18—C17—C16—C1585.74 (15)
C9—C10—C11—C120.2 (2)N4—C15—C16—C17171.28 (11)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H01···O2i0.996 (15)1.720 (15)2.6689 (14)157.8 (13)
N4—H02···O1ii0.938 (16)1.792 (16)2.6914 (16)159.8 (14)
Symmetry codes: (i) x, y, z1; (ii) x+2, y, z+1.
Dibenzylammonium 2-azidebenzoate (2a-db-f) top
Crystal data top
C21H20N4O2F(000) = 760
Mr = 360.41Dx = 1.255 Mg m3
Monoclinic, CcMelting point: not measured K
a = 19.892 (7) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.966 (2) ÅCell parameters from 5377 reflections
c = 10.068 (2) ŵ = 0.08 mm1
β = 107.06 (4)°T = 88 K
V = 1908.1 (9) Å3Bloc, orange
Z = 40.41 × 0.34 × 0.22 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
2723 independent reflections
Radiation source: rotating anode2511 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.042
ω scansθmax = 30.0°, θmin = 2.3°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 2719
Tmin = 0.967, Tmax = 0.982k = 1312
7279 measured reflectionsl = 1414
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.046H-atom parameters constrained
wR(F2) = 0.139 w = 1/[σ2(Fo2) + (0.1113P)2 + 0.0483P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
2723 reflectionsΔρmax = 0.37 e Å3
210 parametersΔρmin = 0.31 e Å3
3 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: rigid modelAbsolute structure parameter: 0 (10)
Special details top

Experimental. 'photo-irradiated product 2,1-benzisoxazolone is observed

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*/UeqOcc. (<1)
C80.41483 (7)0.43225 (10)0.49159 (7)0.0248 (4)
H810.40840.46890.57850.030*
H820.39830.33800.48250.030*
C90.37055 (7)0.51239 (9)0.36955 (8)0.0255 (4)
C100.32592 (7)0.44757 (10)0.25409 (8)0.0277 (4)
H100.32480.35230.25070.033*
C110.28286 (7)0.52154 (13)0.14336 (9)0.0331 (5)
H110.25220.47620.06620.040*
C120.28482 (8)0.66108 (13)0.14581 (14)0.0390 (6)
H120.25550.71120.07080.047*
C130.32986 (8)0.72615 (10)0.25850 (17)0.0590 (10)
H130.33230.82140.25930.071*
C140.37182 (7)0.65333 (9)0.37140 (14)0.0525 (8)
H140.40130.69940.44960.063*
C150.53423 (7)0.34853 (10)0.61870 (9)0.0234 (4)
H1510.52160.25320.59780.028*
H1520.52310.37250.70530.028*
C160.61217 (7)0.36718 (9)0.63952 (10)0.0235 (4)
C170.64518 (7)0.30437 (10)0.55099 (12)0.0276 (4)
H170.61860.24720.47920.033*
C180.71656 (7)0.32468 (14)0.56682 (14)0.0318 (5)
H180.73820.28300.50500.038*
C190.75604 (7)0.40676 (13)0.67416 (17)0.0416 (6)
H190.80450.42190.68490.050*
C200.72407 (7)0.46625 (12)0.76517 (16)0.0509 (8)
H200.75120.52000.83960.061*
C210.65223 (7)0.44763 (12)0.74805 (12)0.0381 (6)
H210.63070.48950.81000.046*
N40.49180 (7)0.43511 (7)0.50132 (8)0.0201 (3)
H010.50710.51470.52260.023 (7)*
H020.49320.41500.42770.024 (7)*
C70.52571 (8)0.28504 (8)0.17894 (11)0.0200 (5)0.906 (6)
C10.51190 (8)0.07364 (7)0.31747 (11)0.0189 (4)0.906 (6)
C20.53695 (9)0.05179 (8)0.37418 (14)0.0225 (5)0.906 (6)
H20.51130.10200.42320.027*0.906 (6)
C30.59934 (9)0.10279 (9)0.35880 (16)0.0249 (5)0.906 (6)
H30.61650.18700.39880.030*0.906 (6)
C40.63682 (9)0.03081 (11)0.28489 (17)0.0245 (5)0.906 (6)
H40.67970.06510.27520.029*0.906 (6)
C50.61046 (8)0.09264 (10)0.22511 (14)0.0232 (5)0.906 (6)
H50.63530.14040.17270.028*0.906 (6)
C60.54822 (7)0.14741 (8)0.24074 (11)0.0189 (4)0.906 (6)
N10.44811 (8)0.12950 (9)0.33457 (13)0.0269 (5)0.906 (6)
N20.42273 (9)0.06817 (12)0.41648 (15)0.0281 (6)0.869 (8)
N30.39425 (10)0.02378 (14)0.48924 (18)0.0403 (7)0.869 (8)
O10.49965 (8)0.36791 (7)0.24507 (13)0.0240 (4)0.906 (6)
O20.53642 (9)0.30931 (11)0.06307 (12)0.0255 (5)0.906 (6)
C7P0.5354 (14)0.267 (3)0.145 (3)0.029 (3)*0.105 (5)
C1P0.5180 (8)0.1133 (16)0.2933 (18)0.029 (3)*0.105 (5)
C2P0.5290 (9)0.0033 (17)0.3724 (18)0.029 (3)*0.105 (5)
H2P0.49980.02330.42940.034*0.105 (5)
C3P0.5828 (10)0.0908 (15)0.368 (2)0.029 (3)*0.105 (5)
H3P0.59030.17050.42210.034*0.105 (5)
C4P0.6255 (9)0.0615 (17)0.285 (2)0.029 (3)*0.105 (5)
H4P0.66230.12120.28180.034*0.105 (5)
C5P0.6145 (9)0.0552 (19)0.2056 (19)0.029 (3)*0.105 (5)
H5P0.64370.07520.14860.034*0.105 (5)
C6P0.5607 (9)0.1426 (15)0.2099 (18)0.029 (3)*0.105 (5)
N1P0.4731 (18)0.223 (4)0.295 (4)0.062 (8)*0.105 (5)
N2P0.3828 (14)0.026 (3)0.527 (3)0.055 (6)*0.131 (8)
N3P0.392 (2)0.066 (4)0.569 (4)0.081 (10)*0.131 (8)
O1P0.4848 (12)0.308 (3)0.200 (2)0.044 (5)*0.105 (5)
O2P0.5521 (15)0.319 (3)0.054 (3)0.039 (6)*0.105 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C80.0214 (8)0.0259 (10)0.0275 (9)0.0010 (7)0.0079 (7)0.0026 (7)
C90.0192 (8)0.0255 (10)0.0315 (10)0.0032 (7)0.0068 (7)0.0034 (8)
C100.0258 (9)0.0284 (11)0.0280 (9)0.0031 (8)0.0063 (7)0.0010 (8)
C110.0247 (10)0.0421 (14)0.0309 (10)0.0019 (9)0.0055 (8)0.0039 (9)
C120.0259 (10)0.0419 (14)0.0453 (13)0.0086 (9)0.0043 (9)0.0094 (11)
C130.0546 (17)0.0287 (14)0.072 (2)0.0131 (13)0.0153 (15)0.0013 (14)
C140.0491 (16)0.0261 (13)0.0614 (18)0.0088 (11)0.0164 (13)0.0088 (12)
C150.0243 (8)0.0216 (9)0.0225 (8)0.0020 (7)0.0041 (6)0.0023 (7)
C160.0227 (8)0.0177 (9)0.0268 (9)0.0001 (6)0.0020 (7)0.0016 (7)
C170.0271 (10)0.0295 (11)0.0240 (9)0.0027 (8)0.0039 (7)0.0003 (7)
C180.0272 (10)0.0326 (12)0.0336 (11)0.0031 (8)0.0057 (8)0.0032 (8)
C190.0215 (10)0.0382 (14)0.0596 (17)0.0004 (9)0.0031 (10)0.0078 (12)
C200.0256 (11)0.0506 (17)0.0667 (19)0.0014 (11)0.0017 (11)0.0301 (15)
C210.0272 (11)0.0356 (13)0.0459 (13)0.0008 (9)0.0018 (9)0.0187 (10)
N40.0188 (7)0.0207 (8)0.0202 (7)0.0002 (6)0.0046 (5)0.0013 (6)
C70.0223 (10)0.0189 (11)0.0181 (10)0.0025 (7)0.0048 (7)0.0001 (8)
C10.0211 (9)0.0156 (10)0.0192 (9)0.0010 (7)0.0046 (7)0.0005 (7)
C20.0274 (10)0.0167 (11)0.0219 (9)0.0001 (8)0.0050 (7)0.0016 (8)
C30.0309 (13)0.0196 (11)0.0228 (10)0.0055 (8)0.0057 (8)0.0008 (8)
C40.0254 (11)0.0254 (12)0.0227 (9)0.0058 (9)0.0071 (8)0.0014 (9)
C50.0267 (10)0.0248 (11)0.0188 (9)0.0034 (8)0.0079 (7)0.0026 (8)
C60.0214 (9)0.0182 (10)0.0167 (9)0.0003 (7)0.0049 (7)0.0006 (7)
N10.0235 (9)0.0236 (10)0.0360 (11)0.0003 (7)0.0122 (8)0.0032 (8)
N20.0225 (10)0.0288 (12)0.0328 (11)0.0017 (8)0.0076 (8)0.0012 (8)
N30.0317 (12)0.0471 (17)0.0467 (15)0.0029 (11)0.0185 (10)0.0112 (13)
O10.0309 (8)0.0198 (8)0.0223 (7)0.0048 (6)0.0094 (6)0.0006 (6)
O20.0373 (12)0.0206 (9)0.0210 (8)0.0061 (8)0.0122 (8)0.0009 (6)
Geometric parameters (Å, º) top
C8—N41.5055C7—O11.2636
C8—C91.5128C7—O21.2691
C8—H810.9900C7—C61.5185
C8—H820.9900C1—C21.4035
C9—C101.3969C1—C61.4094
C9—C141.4048C1—N11.4414
C10—C111.3999C2—C31.3910
C10—H100.9500C2—H20.9500
C11—C121.3912C3—C41.3964
C11—H110.9500C3—H30.9500
C12—C131.3835C4—C51.4020
C12—H120.9500C4—H40.9500
C13—C141.3996C5—C61.4036
C13—H130.9500C5—H50.9500
C14—H140.9500N1—N21.2462
C15—N41.5061N2—N31.1387
C15—C161.5138C7P—O2P1.18 (4)
C15—H1510.9900C7P—O1P1.35 (3)
C15—H1520.9900C7P—C6P1.43 (3)
C16—C171.4003C1P—C2P1.3900
C16—C211.4004C1P—C6P1.3900
C17—C181.3963C1P—N1P1.42 (4)
C17—H170.9500C2P—C3P1.3900
C18—C191.3985C2P—H2P0.9500
C18—H180.9500C3P—C4P1.3900
C19—C201.3920C3P—H3P0.9500
C19—H190.9500C4P—C5P1.3900
C20—C211.4005C4P—H4P0.9500
C20—H200.9500C5P—C6P1.3900
C21—H210.9500C5P—H5P0.9500
N4—H010.8541N1P—O1P1.34 (4)
N4—H020.7767N2P—N3P1.00 (4)
N4—C8—C9112.4C15—N4—H01105.0
N4—C8—H81109.1C8—N4—H02104.7
C9—C8—H81109.1C15—N4—H02115.6
N4—C8—H82109.1H01—N4—H02111.6
C9—C8—H82109.1O1—C7—O2124.4
H81—C8—H82107.8O1—C7—C6119.4
C10—C9—C14118.6O2—C7—C6116.1
C10—C9—C8120.5C2—C1—C6120.6
C14—C9—C8120.9C2—C1—N1121.0
C9—C10—C11120.7C6—C1—N1118.3
C9—C10—H10119.7C3—C2—C1120.1
C11—C10—H10119.7C3—C2—H2119.9
C12—C11—C10120.3C1—C2—H2119.9
C12—C11—H11119.8C2—C3—C4120.3
C10—C11—H11119.8C2—C3—H3119.8
C13—C12—C11119.4C4—C3—H3119.8
C13—C12—H12120.3C3—C4—C5119.3
C11—C12—H12120.3C3—C4—H4120.4
C12—C13—C14120.8C5—C4—H4120.4
C12—C13—H13119.6C4—C5—C6121.6
C14—C13—H13119.6C4—C5—H5119.2
C13—C14—C9120.2C6—C5—H5119.2
C13—C14—H14119.9C5—C6—C1118.0
C9—C14—H14119.9C5—C6—C7118.0
N4—C15—C16110.7C1—C6—C7124.0
N4—C15—H151109.5N2—N1—C1115.6
C16—C15—H151109.5N3—N2—N1172.3
N4—C15—H152109.5O2P—C7P—O1P127 (3)
C16—C15—H152109.5O2P—C7P—C6P127 (3)
H151—C15—H152108.1O1P—C7P—C6P106 (2)
C17—C16—C21119.1C2P—C1P—C6P120.0
C17—C16—C15120.6C2P—C1P—N1P129.5 (17)
C21—C16—C15120.2C6P—C1P—N1P110.0 (17)
C18—C17—C16120.9C3P—C2P—C1P120.0
C18—C17—H17119.5C3P—C2P—H2P120.0
C16—C17—H17119.5C1P—C2P—H2P120.0
C17—C18—C19119.7C2P—C3P—C4P120.0
C17—C18—H18120.2C2P—C3P—H3P120.0
C19—C18—H18120.2C4P—C3P—H3P120.0
C20—C19—C18119.8C3P—C4P—C5P120.0
C20—C19—H19120.1C3P—C4P—H4P120.0
C18—C19—H19120.1C5P—C4P—H4P120.0
C19—C20—C21120.6C4P—C5P—C6P120.0
C19—C20—H20119.7C4P—C5P—H5P120.0
C21—C20—H20119.7C6P—C5P—H5P120.0
C16—C21—C20119.9C5P—C6P—C1P120.0
C16—C21—H21120.1C5P—C6P—C7P134.6 (14)
C20—C21—H21120.1C1P—C6P—C7P105.4 (14)
C8—N4—C15111.4O1P—N1P—C1P104 (2)
C8—N4—H01108.3N1P—O1P—C7P114 (3)
N4—C8—C9—C10108.7N1—C1—C6—C5179.7
N4—C8—C9—C1473.2C2—C1—C6—C7178.5
C14—C9—C10—C110.7N1—C1—C6—C72.3
C8—C9—C10—C11177.5O1—C7—C6—C5140.6
C9—C10—C11—C121.1O2—C7—C6—C537.8
C10—C11—C12—C130.2O1—C7—C6—C136.8
C11—C12—C13—C141.8O2—C7—C6—C1144.8
C12—C13—C14—C92.3C2—C1—N1—N28.9
C10—C9—C14—C131.0C6—C1—N1—N2171.9
C8—C9—C14—C13179.1C1—N1—N2—N3173.4
N4—C15—C16—C1778.2C6P—C1P—C2P—C3P0.0
N4—C15—C16—C21101.8N1P—C1P—C2P—C3P171 (3)
C21—C16—C17—C182.2C1P—C2P—C3P—C4P0.0
C15—C16—C17—C18177.9C2P—C3P—C4P—C5P0.0
C16—C17—C18—C191.3C3P—C4P—C5P—C6P0.0
C17—C18—C19—C200.7C4P—C5P—C6P—C1P0.0
C18—C19—C20—C211.7C4P—C5P—C6P—C7P180 (2)
C17—C16—C21—C201.2C2P—C1P—C6P—C5P0.0
C15—C16—C21—C20178.9N1P—C1P—C6P—C5P173 (2)
C19—C20—C21—C160.8C2P—C1P—C6P—C7P180.0 (18)
C9—C8—N4—C15176.9N1P—C1P—C6P—C7P7 (2)
C16—C15—N4—C8172.3O2P—C7P—C6P—C5P9 (4)
C6—C1—C2—C32.0O1P—C7P—C6P—C5P175.1 (18)
N1—C1—C2—C3178.8O2P—C7P—C6P—C1P171 (3)
C1—C2—C3—C41.1O1P—C7P—C6P—C1P5 (2)
C2—C3—C4—C50.7C2P—C1P—N1P—O1P178.6 (17)
C3—C4—C5—C61.7C6P—C1P—N1P—O1P7 (3)
C4—C5—C6—C10.8C1P—N1P—O1P—C7P4 (3)
C4—C5—C6—C7176.8O2P—C7P—O1P—N1P175 (3)
C2—C1—C6—C51.1C6P—C7P—O1P—N1P1 (3)
Dibenzylammonium 3-azidebenzoate (3a-db-I-f) top
Crystal data top
C21H20N4O2Dx = 1.235 Mg m3
Mr = 360.41Melting point: not measured K
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
a = 8.9378 (2) ÅCell parameters from 8192 reflections
b = 14.5133 (3) ŵ = 0.08 mm1
c = 14.9386 (3) ÅT = 80 K
V = 1937.79 (7) Å3Needle, orange
Z = 40.40 × 0.20 × 0.15 mm
F(000) = 760
Data collection top
Bruker SMART CCD area detector system
diffractometer
3183 independent reflections
Radiation source: rotating anode2575 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.050
ω scansθmax = 30.0°, θmin = 2.0°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1212
Tmin = 0.968, Tmax = 0.988k = 2020
30720 measured reflectionsl = 2121
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.059H-atom parameters constrained
wR(F2) = 0.181 w = 1/[σ2(Fo2) + (0.1067P)2 + 0.5646P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
3183 reflectionsΔρmax = 0.35 e Å3
183 parametersΔρmin = 0.24 e Å3
0 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0 (10)
Special details top

Experimental. 'photo-irradiated product 3-nitrenobenzoate is observed

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*/UeqOcc. (<1)
C80.41484 (15)0.35948 (6)0.07201 (7)0.0319 (5)
H810.52110.34970.05590.038*
H820.37250.40520.02990.038*
C90.40572 (11)0.39691 (6)0.16611 (7)0.0294 (5)
C100.51828 (12)0.37711 (7)0.22792 (8)0.0369 (6)
H100.60400.34330.20960.044*
C110.50563 (18)0.40671 (9)0.31642 (8)0.0480 (8)
H110.58150.39170.35850.058*
C120.3824 (2)0.45806 (9)0.34305 (8)0.0526 (9)
H120.37380.47810.40340.063*
C130.27178 (16)0.48010 (8)0.28149 (11)0.0520 (9)
H130.18860.51650.29940.062*
C140.28225 (13)0.44901 (6)0.19330 (10)0.0403 (7)
H140.20530.46330.15170.048*
C150.40374 (9)0.19026 (6)0.10927 (7)0.0316 (5)
H1510.50550.18050.08490.038*
H1520.41280.20360.17400.038*
C160.31095 (12)0.10449 (6)0.09564 (8)0.0372 (6)
C170.31346 (15)0.05934 (7)0.01311 (9)0.0426 (7)
H170.37550.08180.03370.051*
C180.22519 (18)0.01860 (7)0.00075 (11)0.0581 (10)
H180.22720.04920.05700.070*
C190.13409 (18)0.05166 (7)0.06783 (13)0.0654 (12)
H190.07280.10420.05810.078*
C200.13296 (19)0.00792 (7)0.15026 (12)0.0636 (12)
H200.07250.03130.19740.076*
C210.22067 (15)0.07061 (6)0.16433 (9)0.0510 (9)
H210.21870.10090.22070.061*
N40.33122 (12)0.27002 (6)0.06284 (6)0.0268 (4)
H010.32200.25620.00300.032*
H020.23640.27760.08560.032*
C70.42586 (10)0.23931 (8)0.14927 (6)0.0288 (5)
C10.32714 (14)0.31779 (9)0.38384 (6)0.0432 (7)
C20.31692 (10)0.29541 (7)0.29326 (6)0.0368 (6)
H20.22560.30480.26200.044*
C30.44051 (9)0.25927 (6)0.24851 (6)0.0293 (5)
C40.57416 (11)0.24472 (10)0.29508 (7)0.0348 (6)
H40.65780.21830.26540.042*
C50.58436 (14)0.26907 (13)0.38539 (7)0.0449 (7)
H50.67590.26040.41660.054*
C60.46110 (16)0.30600 (12)0.43001 (6)0.0485 (8)
H60.46850.32290.49130.058*
N10.20300 (17)0.35501 (13)0.43323 (8)0.0573 (8)
N20.08238 (15)0.35306 (14)0.39207 (10)0.0419 (15)0.75 (2)
N30.03288 (14)0.35417 (18)0.36061 (13)0.0544 (18)0.75 (2)
O10.30008 (11)0.25634 (10)0.11408 (6)0.0364 (4)
O20.53725 (12)0.20796 (9)0.10780 (7)0.0349 (4)
N2P0.054 (5)0.336 (4)0.378 (3)0.152 (10)*0.25 (2)
N3P0.056 (5)0.368 (3)0.329 (3)0.152 (10)*0.25 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C80.0309 (12)0.0273 (11)0.0375 (13)0.0103 (10)0.0007 (11)0.0032 (10)
C90.0248 (11)0.0238 (10)0.0396 (13)0.0059 (9)0.0031 (10)0.0015 (10)
C70.0314 (13)0.0374 (14)0.0417 (14)0.0051 (11)0.0004 (11)0.0027 (12)
C110.0501 (18)0.0504 (18)0.0433 (16)0.0130 (15)0.0080 (14)0.0039 (14)
C120.059 (2)0.0515 (18)0.0473 (17)0.0243 (17)0.0151 (16)0.0137 (15)
C130.0421 (17)0.0379 (16)0.076 (2)0.0087 (13)0.0143 (17)0.0193 (16)
C140.0308 (13)0.0313 (13)0.0589 (18)0.0002 (11)0.0006 (13)0.0064 (13)
C150.0250 (11)0.0290 (12)0.0408 (13)0.0003 (10)0.0009 (11)0.0010 (10)
C160.0249 (11)0.0268 (11)0.0599 (17)0.0012 (10)0.0004 (12)0.0003 (12)
C170.0428 (16)0.0287 (13)0.0564 (18)0.0013 (12)0.0142 (14)0.0024 (12)
C180.059 (2)0.0339 (15)0.082 (3)0.0021 (15)0.029 (2)0.0070 (16)
C190.0416 (18)0.0325 (15)0.122 (4)0.0107 (14)0.015 (2)0.002 (2)
C200.0364 (16)0.0380 (16)0.116 (4)0.0042 (14)0.019 (2)0.000 (2)
C210.0411 (16)0.0294 (13)0.083 (2)0.0013 (12)0.0210 (17)0.0042 (15)
N40.0205 (9)0.0248 (9)0.0351 (10)0.0040 (7)0.0018 (8)0.0017 (8)
C70.0228 (10)0.0315 (12)0.0321 (11)0.0018 (9)0.0014 (9)0.0044 (10)
C10.0480 (17)0.0440 (16)0.0377 (14)0.0045 (14)0.0078 (14)0.0030 (13)
C20.0342 (13)0.0401 (14)0.0362 (13)0.0023 (12)0.0049 (11)0.0035 (11)
C30.0272 (11)0.0295 (11)0.0310 (11)0.0053 (9)0.0015 (9)0.0047 (10)
C40.0288 (12)0.0358 (13)0.0399 (13)0.0049 (11)0.0016 (11)0.0088 (11)
C50.0445 (16)0.0487 (17)0.0414 (14)0.0145 (14)0.0099 (13)0.0124 (13)
C60.064 (2)0.0498 (18)0.0322 (13)0.0130 (17)0.0002 (14)0.0023 (13)
N10.0608 (19)0.071 (2)0.0398 (14)0.0012 (17)0.0144 (14)0.0042 (14)
N20.038 (2)0.051 (2)0.037 (2)0.0071 (16)0.0156 (16)0.0142 (16)
N30.028 (2)0.074 (3)0.061 (3)0.0027 (19)0.0145 (19)0.027 (2)
O10.0216 (8)0.0511 (12)0.0366 (9)0.0037 (8)0.0005 (7)0.0044 (9)
O20.0221 (8)0.0424 (11)0.0401 (10)0.0020 (8)0.0031 (8)0.0016 (9)
Geometric parameters (Å, º) top
C8—N41.5043C19—C201.3854
C8—C91.5093C19—H190.9500
C8—H810.9900C20—C211.3991
C8—H820.9900C20—H200.9500
C9—C101.3955C21—H210.9500
C9—C141.3980N4—H010.9200
C10—C111.3947N4—H020.9200
C10—H100.9500C7—O21.2578
C11—C121.3880C7—O11.2654
C11—H110.9500C7—C31.5162
C12—C131.3877C1—C61.3923
C12—H120.9500C1—C21.3945
C13—C141.3957C1—N11.4378
C13—H130.9500C2—C31.3937
C14—H140.9500C2—H20.9500
C15—N41.4971C3—C41.3983
C15—C161.5095C4—C51.3976
C15—H1510.9900C4—H40.9500
C15—H1520.9900C5—C61.3947
C16—C211.3949C5—H50.9500
C16—C171.3964C6—H60.9500
C17—C181.3946N1—N21.2415
C17—H170.9500N1—N1i5.766 (3)
C18—C191.3938N2—N31.1324
C18—H180.9500N2P—N3P1.32 (5)
N4—C8—C9111.6C20—C19—H19120.0
N4—C8—H81109.3C18—C19—H19120.0
C9—C8—H81109.3C19—C20—C21120.2
N4—C8—H82109.3C19—C20—H20119.9
C9—C8—H82109.3C21—C20—H20119.9
H81—C8—H82108.0C16—C21—C20120.0
C10—C9—C14119.2C16—C21—H21120.0
C10—C9—C8120.2C20—C21—H21120.0
C14—C9—C8120.5C15—N4—C8114.2
C11—C10—C9120.4C15—N4—H01108.7
C11—C10—H10119.8C8—N4—H01108.7
C9—C10—H10119.8C15—N4—H02108.7
C12—C11—C10120.1C8—N4—H02108.7
C12—C11—H11120.0H01—N4—H02107.6
C10—C11—H11120.0O2—C7—O1124.7
C13—C12—C11120.0O2—C7—C3118.8
C13—C12—H12120.0O1—C7—C3116.5
C11—C12—H12120.0C6—C1—C2120.6
C12—C13—C14120.2C6—C1—N1117.1
C12—C13—H13119.9C2—C1—N1122.3
C14—C13—H13119.9C3—C2—C1120.1
C13—C14—C9120.1C3—C2—H21120.0
C13—C14—H14119.9C1—C2—H21120.0
C9—C14—H14119.9C2—C3—C4119.7
N4—C15—C16109.7C2—C3—C7118.2
N4—C15—H151109.7C4—C3—C7122.1
C16—C15—H151109.7C5—C4—C3119.9
N4—C15—H152109.7C5—C4—H14120.1
C16—C15—H152109.7C3—C4—H14120.1
H151—C15—H152108.2C6—C5—C4120.5
C21—C16—C17119.6C6—C5—H151119.8
C21—C16—C15120.6C4—C5—H152119.8
C17—C16—C15119.8C1—C6—C5119.3
C18—C17—C16120.2C1—C6—H6120.3
C18—C17—H17119.9C5—C6—H6120.3
C16—C17—H17119.9N2—N1—C1114.0
C19—C18—C17120.0N2—N1—N1i146.35 (6)
C19—C18—H18120.0C1—N1—N1i51.7
C17—C18—H18120.0N3—N2—N1174.4
C20—C19—C18120.0
N4—C8—C9—C1093.9C9—C8—N4—C1570.6
N4—C8—C9—C1483.8C6—C1—C2—C31.2
C14—C9—C10—C111.8N1—C1—C2—C3179.8
C8—C9—C10—C11176.0C1—C2—C3—C40.6
C9—C10—C11—C121.6C1—C2—C3—C7177.8
C10—C11—C12—C130.1O2—C7—C3—C2179.0
C11—C12—C13—C141.5O1—C7—C3—C20.7
C12—C13—C14—C91.2O2—C7—C3—C40.6
C10—C9—C14—C130.5O1—C7—C3—C4179.1
C8—C9—C14—C13177.3C2—C3—C4—C51.9
N4—C15—C16—C21103.6C7—C3—C4—C5176.4
N4—C15—C16—C1775.3C3—C4—C5—C61.4
C21—C16—C17—C180.6C2—C1—C6—C51.8
C15—C16—C17—C18178.4N1—C1—C6—C5179.2
C16—C17—C18—C190.0C4—C5—C6—C10.5
C17—C18—C19—C201.0C6—C1—N1—N2171.4
C18—C19—C20—C211.4C2—C1—N1—N29.7
C17—C16—C21—C200.2C6—C1—N1—N1i27.36 (7)
C15—C16—C21—C20178.7C2—C1—N1—N1i153.66 (7)
C19—C20—C21—C160.8C1—N1—N2—N3177 (100)
C16—C15—N4—C8179.9N1i—N1—N2—N3120.9
Symmetry code: (i) x+1/2, y+1/2, z+1.
Dibenzylammonium 3-azidebenzoate (3a-db-II-f) top
Crystal data top
C21H20N4O2F(000) = 760
Mr = 360.41Dx = 1.216 Mg m3
Monoclinic, P21/cMelting point: not measured K
a = 10.908 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.7884 (18) ÅCell parameters from 7397 reflections
c = 21.240 (4) ŵ = 0.08 mm1
β = 104.87 (3)°T = 82 K
V = 1967.9 (7) Å3Needle, pale-yellow
Z = 40.31 × 0.16 × 0.12 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
5734 independent reflections
Radiation source: rotating anode4338 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.044
ω scansθmax = 30.0°, θmin = 2.0°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1515
Tmin = 0.975, Tmax = 0.990k = 1212
30460 measured reflectionsl = 2929
Refinement top
Refinement on F2Primary atom site location: rigid model
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.067Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.192H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0911P)2 + 1.2767P]
where P = (Fo2 + 2Fc2)/3
5734 reflections(Δ/σ)max < 0.001
206 parametersΔρmax = 0.57 e Å3
5 restraintsΔρmin = 0.56 e Å3
Special details top

Experimental. 'photo-irradiated product 3,3'-dicarboxy-trans-azobenzene is observed'

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*/UeqOcc. (<1)
C80.17213 (6)0.71400 (9)0.25544 (3)0.0255 (3)
H810.20050.68650.30210.031*
H820.13190.81560.25240.031*
C90.28668 (5)0.72342 (7)0.22800 (3)0.0240 (3)
C100.28565 (5)0.81927 (7)0.17506 (4)0.0288 (4)
H100.21240.87820.15630.035*
C110.39182 (6)0.82857 (10)0.14979 (4)0.0340 (4)
H110.39020.89290.11370.041*
C120.49992 (5)0.74350 (11)0.17758 (4)0.0359 (4)
H120.57210.75020.16050.043*
C130.50215 (4)0.64844 (9)0.23055 (5)0.0341 (4)
H130.57590.59060.24950.041*
C140.39578 (5)0.63839 (8)0.25569 (4)0.0290 (4)
H140.39760.57360.29170.035*
C150.00796 (4)0.64688 (6)0.15304 (3)0.0282 (4)
H1510.06980.64940.12610.034*
H1520.02630.75090.15390.034*
C160.09913 (5)0.53988 (7)0.12219 (3)0.0280 (4)
C170.08863 (6)0.44197 (9)0.07192 (3)0.0372 (4)
H170.01300.44130.05760.045*
C180.18871 (7)0.34511 (11)0.04265 (4)0.0473 (6)
H180.18100.27900.00850.057*
C190.29958 (6)0.34555 (10)0.06360 (5)0.0484 (6)
H190.36770.27990.04370.058*
C200.31059 (5)0.44258 (10)0.11390 (5)0.0418 (5)
H200.38620.44240.12830.050*
C210.21104 (5)0.53981 (9)0.14314 (4)0.0323 (4)
H210.21910.60590.17720.039*
N40.07458 (5)0.59982 (8)0.22107 (3)0.0236 (3)
H020.11380.50770.21960.028*
H010.01550.58680.24470.028*
C10.19678 (6)0.16036 (7)0.02177 (3)0.0267 (4)0.923 (4)
C20.14210 (6)0.13520 (7)0.07353 (3)0.0225 (4)0.923 (4)
H20.07980.05810.07050.027*0.923 (4)
C30.17957 (6)0.22403 (6)0.12982 (3)0.0196 (3)0.923 (4)
C40.27046 (8)0.33869 (9)0.13361 (3)0.0244 (4)0.923 (4)
H40.29620.39910.17180.029*0.923 (4)
C50.32313 (9)0.36409 (10)0.08115 (4)0.0284 (4)0.923 (4)
H50.38400.44280.08370.034*0.923 (4)
C60.28742 (8)0.27513 (9)0.02492 (3)0.0309 (4)0.923 (4)
H60.32390.29210.01060.037*0.923 (4)
C70.12082 (7)0.19626 (8)0.18627 (3)0.0212 (4)0.923 (4)
O10.13741 (9)0.29562 (10)0.23092 (3)0.0260 (3)0.923 (4)
O20.05916 (10)0.07375 (10)0.18578 (4)0.0259 (3)0.923 (4)
N10.15157 (9)0.06391 (10)0.03395 (3)0.0389 (5)0.923 (4)
N20.21439 (10)0.06437 (11)0.07524 (3)0.0322 (5)0.823 (4)
N30.26331 (12)0.05379 (13)0.11617 (4)0.0431 (6)0.823 (4)
C1P0.118 (2)0.148 (3)0.0376 (9)0.056 (4)*0.075 (4)
C2P0.099 (2)0.126 (2)0.0992 (10)0.056 (4)*0.075 (4)
H2P0.03870.05290.10540.067*0.075 (4)
C3P0.167 (2)0.212 (3)0.1516 (9)0.056 (4)*0.075 (4)
C4P0.254 (2)0.319 (3)0.1426 (10)0.056 (4)*0.075 (4)
H4P0.30080.37730.17840.067*0.075 (4)
C5P0.274 (2)0.341 (3)0.0810 (12)0.056 (4)*0.075 (4)
H5P0.33330.41420.07480.067*0.075 (4)
C6P0.205 (2)0.255 (3)0.0286 (9)0.056 (4)*0.075 (4)
H6P0.21860.27050.01350.067*0.075 (4)
C7P0.134 (2)0.201 (3)0.209 (2)0.056 (4)*0.075 (4)
O1P0.159 (3)0.318 (4)0.2516 (15)0.056 (4)*0.075 (4)
O2P0.073 (3)0.073 (3)0.2096 (15)0.056 (4)*0.075 (4)
N1P0.037 (3)0.049 (4)0.0078 (17)0.066 (9)*0.075 (4)
N2P0.395 (3)0.032 (4)0.0624 (15)0.136 (10)*0.177 (4)
N3P0.477 (2)0.019 (3)0.0176 (11)0.106 (7)*0.177 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C80.0274 (8)0.0198 (7)0.0315 (8)0.0031 (6)0.0117 (6)0.0039 (6)
C90.0242 (7)0.0181 (7)0.0309 (8)0.0033 (6)0.0090 (6)0.0043 (6)
C100.0271 (8)0.0213 (7)0.0399 (9)0.0001 (6)0.0122 (7)0.0022 (7)
C110.0339 (9)0.0285 (8)0.0438 (10)0.0038 (7)0.0175 (8)0.0043 (8)
C120.0262 (8)0.0340 (9)0.0515 (11)0.0060 (7)0.0173 (8)0.0034 (8)
C130.0224 (8)0.0334 (9)0.0452 (11)0.0003 (7)0.0064 (7)0.0027 (8)
C140.0270 (8)0.0265 (8)0.0327 (9)0.0023 (6)0.0062 (7)0.0010 (7)
C150.0246 (8)0.0275 (8)0.0321 (8)0.0016 (6)0.0064 (6)0.0050 (7)
C160.0248 (8)0.0254 (8)0.0317 (8)0.0026 (6)0.0033 (6)0.0044 (6)
C170.0333 (9)0.0365 (10)0.0384 (10)0.0084 (8)0.0030 (8)0.0013 (8)
C180.0525 (13)0.0334 (10)0.0461 (12)0.0078 (9)0.0053 (10)0.0072 (9)
C190.0407 (11)0.0358 (11)0.0555 (13)0.0088 (9)0.0114 (10)0.0046 (10)
C200.0297 (9)0.0423 (11)0.0487 (12)0.0056 (8)0.0014 (8)0.0099 (9)
C210.0269 (8)0.0326 (9)0.0353 (9)0.0003 (7)0.0043 (7)0.0048 (7)
N40.0228 (6)0.0188 (6)0.0315 (7)0.0003 (5)0.0113 (5)0.0007 (5)
C10.0284 (9)0.0272 (9)0.0252 (8)0.0026 (7)0.0082 (7)0.0026 (7)
C20.0238 (8)0.0207 (7)0.0252 (8)0.0023 (6)0.0102 (7)0.0001 (6)
C30.0189 (7)0.0176 (7)0.0233 (8)0.0019 (6)0.0073 (6)0.0023 (6)
C40.0236 (8)0.0221 (8)0.0270 (9)0.0036 (6)0.0057 (7)0.0019 (7)
C50.0213 (8)0.0305 (9)0.0331 (9)0.0073 (7)0.0064 (7)0.0029 (7)
C60.0294 (9)0.0376 (10)0.0276 (9)0.0038 (8)0.0106 (7)0.0028 (8)
C70.0223 (8)0.0190 (7)0.0240 (8)0.0046 (6)0.0089 (6)0.0010 (6)
O10.0344 (8)0.0198 (6)0.0258 (7)0.0019 (5)0.0113 (6)0.0030 (5)
O20.0332 (7)0.0200 (6)0.0292 (7)0.0014 (5)0.0165 (6)0.0023 (6)
N10.0454 (11)0.0437 (11)0.0318 (9)0.0146 (8)0.0175 (8)0.0099 (8)
N20.0435 (11)0.0260 (9)0.0307 (9)0.0050 (8)0.0157 (8)0.0027 (7)
N30.0656 (15)0.0348 (11)0.0390 (12)0.0099 (10)0.0317 (11)0.0074 (9)
Geometric parameters (Å, º) top
C8—N41.5077C1—C61.4020
C8—C91.5104C1—N11.4362
C8—H810.9900C2—C31.3983
C8—H820.9900C2—H20.9500
C9—C141.4005C3—C41.4013
C9—C101.4027C3—C71.5173
C10—C111.3981C4—C51.3964
C10—H100.9500C4—H40.9500
C11—C121.3930C5—C61.3967
C11—H110.9500C5—H50.9500
C12—C131.3966C6—H60.9500
C12—H120.9500C7—O11.2674
C13—C141.3989C7—O21.2681
C13—H130.9500N1—N21.2438
C14—H140.9500N2—N31.1346
C15—N41.4994C1P—C2P1.3900
C15—C161.5117C1P—C6P1.3900
C15—H1510.9900C1P—N1P1.42 (4)
C15—H1520.9900C2P—C3P1.3900
C16—C171.3987C2P—H2P0.9500
C16—C211.4024C3P—C7P1.35 (5)
C17—C181.3980C3P—C4P1.3900
C17—H170.9500C4P—C5P1.3900
C18—C191.3916C4P—H4P0.9500
C18—H180.9500C5P—C6P1.3900
C19—C201.3959C5P—H5P0.9500
C19—H190.9500C6P—H6P0.9500
C20—C211.3960C7P—O2P1.308 (19)
C20—H200.9500C7P—O1P1.35 (4)
C21—H360.9500N1P—N1Pi1.29 (7)
N4—H020.9200N2P—N3P1.13 (3)
N4—H010.9200N3P—N3Pii0.85 (4)
C1—C21.3962
N4—C8—C9113.6C8—N4—H02109.0
N4—C8—H81108.8C15—N4—H01109.0
C9—C8—H81108.8C8—N4—H01109.0
N4—C8—H82108.8H02—N4—H01107.8
C9—C8—H82108.8C2—C1—C6121.0
H81—C8—H82107.7C2—C1—N1115.4
C14—C9—C10119.2C6—C1—N1123.5
C14—C9—C8120.4C1—C2—C3119.6
C10—C9—C8120.3C1—C2—H2120.2
C11—C10—C9120.4C3—C2—H2120.2
C11—C10—H10119.8C2—C3—C4119.9
C9—C10—H10119.8C2—C3—C7119.7
C12—C11—C10120.0C4—C3—C7120.4
C12—C11—H11120.0C5—C4—C3119.9
C10—C11—H11120.0C5—C4—H4120.0
C11—C12—C13120.0C3—C4—H4120.0
C11—C12—H12120.0C4—C5—C6120.7
C13—C12—H12120.0C4—C5—H5119.6
C12—C13—C14120.0C6—C5—H5119.6
C12—C13—H13120.0C5—C6—C1118.8
C14—C13—H13120.0C5—C6—H6120.6
C13—C14—C9120.3C1—C6—H6120.6
C13—C14—H14119.8O1—C7—O2124.4
C9—C14—H14119.8O1—C7—C3118.2
N4—C15—C16112.1O2—C7—C3117.4
N4—C15—H151109.2N2—N1—C1116.4
C16—C15—H151109.2N3—N2—N1173.0
N4—C15—H152109.2C2P—C1P—C6P120.0
C16—C15—H152109.2C2P—C1P—N1P110 (2)
H151—C15—H152107.9C6P—C1P—N1P130 (2)
C17—C16—C21119.4C1P—C2P—C3P120.0
C17—C16—C15120.5C1P—C2P—H2P120.0
C21—C16—C15120.1C3P—C2P—H2P120.0
C18—C17—C16120.4C7P—C3P—C4P121.2 (8)
C18—C17—H17119.8C7P—C3P—C2P118.3 (8)
C16—C17—H17119.8C4P—C3P—C2P120.0
C19—C18—C17120.0C3P—C4P—C5P120.0
C19—C18—H18120.0C3P—C4P—H4P120.0
C17—C18—H18120.0C5P—C4P—H4P120.0
C18—C19—C20119.9C6P—C5P—C4P120.0
C18—C19—H19120.0C6P—C5P—H5P120.0
C20—C19—H19120.0C4P—C5P—H5P120.0
C19—C20—C21120.3C5P—C6P—C1P120.0
C19—C20—H20119.9C5P—C6P—H6P120.0
C21—C20—H20119.9C1P—C6P—H6P120.0
C20—C21—C16120.0O2P—C7P—O1P131 (4)
C20—C21—H36120.0O2P—C7P—C3P109 (3)
C16—C21—H36120.0O1P—C7P—C3P120 (2)
C15—N4—C8113.0N1Pi—N1P—C1P124 (4)
C15—N4—H02109.0N3Pii—N3P—N2P158 (5)
N4—C8—C9—C1494.6C3—C4—C5—C60.8
N4—C8—C9—C1086.4C4—C5—C6—C10.5
C14—C9—C10—C110.7C2—C1—C6—C50.4
C8—C9—C10—C11179.7N1—C1—C6—C5178.9
C9—C10—C11—C120.6C2—C3—C7—O1166.6
C10—C11—C12—C130.2C4—C3—C7—O113.0
C11—C12—C13—C140.1C2—C3—C7—O214.1
C12—C13—C14—C90.0C4—C3—C7—O2166.3
C10—C9—C14—C130.3C2—C1—N1—N2167.1
C8—C9—C14—C13179.4C6—C1—N1—N214.2
N4—C15—C16—C17109.1C1—N1—N2—N3177.1
N4—C15—C16—C2172.0C6P—C1P—C2P—C3P0.0
C21—C16—C17—C180.2N1P—C1P—C2P—C3P180 (3)
C15—C16—C17—C18178.8C1P—C2P—C3P—C7P171.9 (19)
C16—C17—C18—C190.1C1P—C2P—C3P—C4P0.0
C17—C18—C19—C200.1C7P—C3P—C4P—C5P171.6 (19)
C18—C19—C20—C210.3C2P—C3P—C4P—C5P0.0
C19—C20—C21—C160.3C3P—C4P—C5P—C6P0.0
C17—C16—C21—C200.0C4P—C5P—C6P—C1P0.0
C15—C16—C21—C20179.0C2P—C1P—C6P—C5P0.0
C16—C15—N4—C8173.7N1P—C1P—C6P—C5P179 (3)
C9—C8—N4—C1569.2C4P—C3P—C7P—O2P166.7 (19)
C6—C1—C2—C31.0C2P—C3P—C7P—O2P22 (2)
N1—C1—C2—C3179.7C4P—C3P—C7P—O1P18 (2)
C1—C2—C3—C40.8C2P—C3P—C7P—O1P154 (2)
C1—C2—C3—C7179.7C2P—C1P—N1P—N1Pi3 (6)
C2—C3—C4—C50.1C6P—C1P—N1P—N1Pi178 (4)
C7—C3—C4—C5179.5
Symmetry codes: (i) x, y, z; (ii) x+1, y, z.
Dicyclohexylammonium 3-azidebenzoate (3a-dc-f) top
Crystal data top
C19H28N4O2Z = 2
Mr = 344.45F(000) = 372
Triclinic, P1Dx = 1.244 Mg m3
a = 9.2356 (4) ÅMelting point: not measured K
b = 10.2844 (5) ÅMo Kα radiation, λ = 0.71073 Å
c = 11.3770 (6) ŵ = 0.08 mm1
α = 111.073 (2)°T = 82 K
β = 103.254 (2)°Plate, pale-yellow
γ = 103.553 (2)°0.44 × 0.38 × 0.26 mm
V = 919.86 (8) Å3
Data collection top
Bruker SMART CCD area detector system
diffractometer
5328 independent reflections
Radiation source: rotating anode4342 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.023
ω scansθmax = 30.0°, θmin = 2.0°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1212
Tmin = 0.965, Tmax = 0.979k = 1414
14760 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)] = 0.049Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.141H atoms treated by a mixture of independent and constrained refinement
S = 0.90 w = 1/[σ2(Fo2) + (0.0866P)2 + 0.4358P]
where P = (Fo2 + 2Fc2)/3
5328 reflections(Δ/σ)max < 0.001
171 parametersΔρmax = 0.40 e Å3
1 restraintΔρmin = 0.46 e Å3
Special details top

Experimental. 'photo-irradiated product 2,1-benzisoxazolone is observed

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*/UeqOcc. (<1)
C80.19633 (4)0.33724 (4)0.51373 (3)0.01734 (19)
H80.15060.22610.46880.021*
C90.37804 (4)0.38581 (6)0.56381 (3)0.0201 (2)
H910.42470.49530.60040.024*
H920.41340.34100.48780.024*
C100.43674 (6)0.33697 (7)0.67355 (4)0.0220 (2)
H1010.39770.22700.63460.026*
H1020.55420.37280.70720.026*
C110.37833 (6)0.39870 (7)0.79071 (4)0.0269 (2)
H1110.42360.50870.83410.032*
H1120.41470.36330.85850.032*
C120.19581 (6)0.34746 (7)0.73954 (4)0.0267 (2)
H1210.15100.23790.70310.032*
H1220.15960.39110.81530.032*
C130.13471 (6)0.39488 (7)0.62957 (4)0.0214 (2)
H1310.01720.35550.59470.026*
H1320.16990.50470.66860.026*
C140.18605 (4)0.35496 (4)0.29121 (3)0.01696 (19)
H140.30270.40820.32050.020*
C150.09899 (6)0.41111 (5)0.19818 (4)0.0194 (2)
H1510.12590.51980.24710.023*
H1520.01710.36300.17160.023*
C160.14561 (7)0.37646 (6)0.07154 (4)0.0214 (2)
H1610.08070.40520.00980.026*
H1620.25840.43640.09730.026*
C170.12131 (7)0.21073 (6)0.00159 (3)0.0242 (2)
H1710.16320.19470.07640.029*
H1720.00640.15170.04010.029*
C180.20644 (8)0.15734 (6)0.09495 (4)0.0241 (2)
H1810.32250.20900.12590.029*
H1820.18420.04930.04670.029*
C190.15208 (6)0.18773 (4)0.21741 (3)0.0205 (2)
H1910.03710.13240.18770.025*
H1920.20970.15380.27850.025*
N40.13726 (5)0.39508 (5)0.41397 (3)0.01682 (17)
H010.02810.36100.38540.020*
H020.17160.49710.45860.020*
C70.70870 (5)0.21398 (4)0.35477 (4)0.0208 (2)
C10.33130 (5)0.12219 (4)0.23526 (5)0.0268 (2)
C20.45416 (4)0.01587 (4)0.31703 (4)0.0226 (2)
H20.45580.07630.40350.027*
C30.57452 (4)0.06359 (4)0.26956 (4)0.0214 (2)
C40.57107 (6)0.02645 (5)0.14191 (4)0.0283 (2)
H40.65320.00500.11040.034*
C50.44676 (7)0.16284 (6)0.06067 (5)0.0332 (3)
H50.44400.22270.02640.040*
C60.32710 (6)0.21101 (5)0.10724 (5)0.0321 (3)
H60.24320.30360.05230.038*
O10.69944 (6)0.29962 (5)0.46306 (5)0.02617 (19)
O20.81857 (5)0.24170 (6)0.30853 (5)0.02648 (19)
N10.20316 (6)0.18301 (6)0.27312 (6)0.0354 (3)
N20.19491 (6)0.10253 (7)0.38192 (7)0.0244 (3)0.817 (4)
N30.17079 (8)0.04254 (9)0.47701 (8)0.0328 (4)0.817 (4)
N2P0.159 (2)0.0365 (19)0.4832 (17)0.092 (4)*0.183 (4)
N3P0.1175 (18)0.0435 (17)0.5514 (15)0.092 (4)*0.183 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C80.0159 (4)0.0218 (5)0.0144 (4)0.0063 (4)0.0058 (3)0.0080 (4)
C90.0165 (4)0.0248 (5)0.0192 (5)0.0066 (4)0.0062 (4)0.0101 (4)
C100.0184 (5)0.0264 (5)0.0200 (5)0.0075 (4)0.0044 (4)0.0104 (4)
C110.0269 (5)0.0350 (6)0.0174 (5)0.0113 (5)0.0052 (4)0.0112 (5)
C120.0272 (6)0.0397 (6)0.0201 (5)0.0143 (5)0.0116 (4)0.0165 (5)
C130.0200 (5)0.0298 (5)0.0174 (5)0.0104 (4)0.0093 (4)0.0107 (4)
C140.0164 (4)0.0204 (4)0.0139 (4)0.0060 (4)0.0070 (3)0.0065 (4)
C150.0210 (5)0.0220 (5)0.0166 (4)0.0084 (4)0.0073 (4)0.0087 (4)
C160.0244 (5)0.0237 (5)0.0166 (5)0.0074 (4)0.0085 (4)0.0091 (4)
C170.0314 (6)0.0244 (5)0.0153 (5)0.0085 (4)0.0097 (4)0.0070 (4)
C180.0316 (6)0.0239 (5)0.0202 (5)0.0127 (4)0.0135 (4)0.0085 (4)
C190.0249 (5)0.0216 (5)0.0171 (4)0.0098 (4)0.0098 (4)0.0082 (4)
N40.0155 (4)0.0202 (4)0.0140 (4)0.0061 (3)0.0057 (3)0.0064 (3)
C70.0167 (4)0.0210 (5)0.0215 (5)0.0055 (4)0.0050 (4)0.0075 (4)
C10.0205 (5)0.0272 (5)0.0332 (6)0.0076 (4)0.0061 (4)0.0159 (5)
C20.0199 (5)0.0226 (5)0.0240 (5)0.0075 (4)0.0060 (4)0.0098 (4)
C30.0177 (5)0.0205 (5)0.0227 (5)0.0066 (4)0.0047 (4)0.0074 (4)
C40.0256 (5)0.0257 (5)0.0268 (6)0.0060 (4)0.0099 (5)0.0057 (5)
C50.0341 (6)0.0252 (6)0.0277 (6)0.0063 (5)0.0077 (5)0.0024 (5)
C60.0257 (6)0.0243 (5)0.0369 (7)0.0042 (5)0.0015 (5)0.0119 (5)
O10.0246 (4)0.0224 (4)0.0249 (4)0.0054 (3)0.0095 (3)0.0044 (3)
O20.0181 (4)0.0294 (4)0.0255 (4)0.0037 (3)0.0079 (3)0.0077 (3)
N10.0304 (6)0.0309 (6)0.0361 (6)0.0013 (4)0.0077 (5)0.0135 (5)
N20.0192 (6)0.0221 (6)0.0292 (7)0.0035 (4)0.0060 (5)0.0122 (5)
N30.0282 (7)0.0289 (7)0.0377 (8)0.0058 (5)0.0119 (6)0.0131 (6)
Geometric parameters (Å, º) top
C8—N41.5143C17—C181.5382
C8—C131.5337C17—H1710.9900
C8—C91.5344C17—H1720.9900
C8—H81.0000C18—C191.5401
C9—C101.5406C18—H1810.9900
C9—H910.9900C18—H1820.9900
C9—H920.9900C19—H1910.9900
C10—C111.5337C19—H1920.9900
C10—H1010.9900N4—H010.9200
C10—H1020.9900N4—H020.9200
C11—C121.5399C7—O11.2665
C11—H1110.9900C7—O21.2668
C11—H1120.9900C7—C31.5298
C12—C131.5382C1—C61.3993
C12—H1210.9900C1—C21.4071
C12—H1220.9900C1—N11.4346
C13—H1310.9900C2—C31.4065
C13—H1320.9900C2—H20.9500
C14—N41.5116C3—C41.4019
C14—C191.5327C4—C51.4023
C14—C151.5386C4—H40.9500
C14—H141.0000C5—C61.3957
C15—C161.5412C5—H50.9500
C15—H1510.9900C6—H60.9500
C15—H1520.9900N1—N21.2486
C16—C171.5371N1—N1i5.8529 (11)
C16—H1610.9900N2—N31.1382
C16—H1620.9900N2P—N3P0.959 (14)
N4—C8—C13107.6C15—C16—H162109.2
N4—C8—C9111.3H161—C16—H162107.9
C13—C8—C9111.6C16—C17—C18111.0
N4—C8—H8108.8C16—C17—H171109.4
C13—C8—H8108.8C18—C17—H171109.4
C9—C8—H8108.8C16—C17—H172109.4
C8—C9—C10110.6C18—C17—H172109.4
C8—C9—H91109.5H171—C17—H172108.0
C10—C9—H91109.5C17—C18—C19111.5
C8—C9—H92109.5C17—C18—H181109.3
C10—C9—H92109.5C19—C18—H181109.3
H91—C9—H92108.1C17—C18—H182109.3
C11—C10—C9111.2C19—C18—H182109.3
C11—C10—H101109.4H181—C18—H182108.0
C9—C10—H101109.4C14—C19—C18109.0
C11—C10—H102109.4C14—C19—H191109.9
C9—C10—H102109.4C18—C19—H191109.9
H101—C10—H102108.0C14—C19—H192109.9
C10—C11—C12110.1C18—C19—H192109.9
C10—C11—H111109.6H191—C19—H192108.3
C12—C11—H111109.6C14—N4—C8117.3
C10—C11—H112109.6C14—N4—H01108.0
C12—C11—H112109.6C8—N4—H01108.0
H111—C11—H112108.2C14—N4—H02108.0
C13—C12—C11111.1C8—N4—H02108.0
C13—C12—H121109.4H01—N4—H02107.2
C11—C12—H121109.4O1—C7—O2126.0
C13—C12—H122109.4O1—C7—C3117.8
C11—C12—H122109.4O2—C7—C3116.2
H121—C12—H122108.0C6—C1—C2120.7
C8—C13—C12111.2C6—C1—N1114.9
C8—C13—H131109.4C2—C1—N1124.4
C12—C13—H131109.4C3—C2—C1119.4
C8—C13—H132109.4C3—C2—H2120.3
C12—C13—H132109.4C1—C2—H2120.3
H131—C13—H132108.0C4—C3—C2119.9
N4—C14—C19112.6C4—C3—C7119.3
N4—C14—C15108.1C2—C3—C7120.8
C19—C14—C15111.0C3—C4—C5120.2
N4—C14—H14108.3C3—C4—H4119.9
C19—C14—H14108.3C5—C4—H4119.9
C15—C14—H14108.3C6—C5—C4120.2
C14—C15—C16111.0C6—C5—H5119.9
C14—C15—H151109.4C4—C5—H5119.9
C16—C15—H151109.4C5—C6—C1119.7
C14—C15—H152109.4C5—C6—H6120.2
C16—C15—H152109.4C1—C6—H6120.2
H151—C15—H152108.0N2—N1—C1117.2
C17—C16—C15111.8N2—N1—N1i62.2
C17—C16—H161109.2C1—N1—N1i66.6
C15—C16—H161109.2N3—N2—N1171.7
C17—C16—H162109.2
N4—C8—C9—C10175.4C6—C1—C2—C30.7
C13—C8—C9—C1055.2N1—C1—C2—C3179.5
C8—C9—C10—C1156.8C1—C2—C3—C40.1
C9—C10—C11—C1257.5C1—C2—C3—C7179.1
C10—C11—C12—C1356.9O1—C7—C3—C4172.5
N4—C8—C13—C12177.3O2—C7—C3—C46.6
C9—C8—C13—C1254.9O1—C7—C3—C26.7
C11—C12—C13—C855.7O2—C7—C3—C2174.2
N4—C14—C15—C16179.0C2—C3—C4—C51.0
C19—C14—C15—C1657.1C7—C3—C4—C5178.2
C14—C15—C16—C1753.7C3—C4—C5—C61.1
C15—C16—C17—C1853.1C4—C5—C6—C10.3
C16—C17—C18—C1956.0C2—C1—C6—C50.6
N4—C14—C19—C18179.6N1—C1—C6—C5179.6
C15—C14—C19—C1859.0C6—C1—N1—N2174.4
C17—C18—C19—C1458.7C2—C1—N1—N25.4
C19—C14—N4—C851.2C6—C1—N1—N1i148.2
C15—C14—N4—C8174.2C2—C1—N1—N1i32.0
C13—C8—N4—C14178.8C1—N1—N2—N3175.5
C9—C8—N4—C1456.3N1i—N1—N2—N3145.4
Symmetry code: (i) x+1, y, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H01···O2ii0.921.832.7266 (11)164
N4—H02···O1iii0.921.892.7829 (10)162
Symmetry codes: (ii) x1, y, z; (iii) x+1, y+1, z+1.
N-benzyl-2-phenylethylammonium 4-azidebenzoate (4a-bp-f) top
Crystal data top
C22H22N4O2Z = 2
Mr = 374.44F(000) = 396
Triclinic, P1Dx = 1.238 Mg m3
a = 8.1100 (4) ÅMelting point: not measured K
b = 10.3363 (6) ÅMo Kα radiation, λ = 0.71073 Å
c = 13.6177 (7) ÅCell parameters from 3455 reflections
α = 72.377 (2)°µ = 0.08 mm1
β = 73.542 (2)°T = 92 K
γ = 70.583 (1)°Plate, orange
V = 1004.67 (9) Å30.31 × 0.12 × 0.08 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
5842 independent reflections
Radiation source: rotating anode2789 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.069
ω scansθmax = 30.0°, θmin = 1.6°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1111
Tmin = 0.975, Tmax = 0.994k = 1414
16229 measured reflectionsl = 1919
Refinement top
Refinement on F2Primary atom site location: rigid model
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.079Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.257H-atom parameters constrained
S = 0.99 w = 1/[σ2(Fo2) + (0.1379P)2]
where P = (Fo2 + 2Fc2)/3
5842 reflections(Δ/σ)max < 0.001
210 parametersΔρmax = 0.39 e Å3
9 restraintsΔρmin = 0.29 e Å3
Special details top

Experimental. 'photo-irradiated product 4,4'-dicarboxy-trans-azobenzene is observed'

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*/UeqOcc. (<1)
N40.75421 (9)0.07769 (7)0.06759 (6)0.0446 (5)
H020.78920.05540.00300.054*
H010.85080.09110.08190.054*
C90.66968 (12)0.33151 (8)0.01742 (8)0.0476 (6)
C100.64971 (17)0.35972 (10)0.12136 (8)0.0545 (7)
H100.59690.30350.14000.065*
C110.7063 (2)0.46901 (11)0.19729 (9)0.0777 (10)
H110.69180.48750.26750.093*
C120.78317 (17)0.55038 (10)0.17101 (11)0.0898 (13)
H120.82050.62590.22290.108*
C130.80663 (19)0.52264 (9)0.06854 (13)0.0897 (13)
H130.86190.57820.05100.108*
C140.74868 (18)0.41267 (8)0.00912 (10)0.0688 (9)
H140.76360.39420.07920.083*
C80.60626 (10)0.21285 (8)0.06255 (8)0.0512 (7)
H810.50400.20060.04360.061*
H820.56500.23590.13250.061*
C170.81189 (13)0.29432 (8)0.24343 (8)0.0491 (6)
C180.84528 (18)0.30497 (10)0.34111 (8)0.0571 (7)
H180.89640.23890.34860.069*
C190.8047 (2)0.41115 (11)0.42781 (9)0.0810 (11)
H190.82800.41650.49370.097*
C200.73165 (19)0.50784 (10)0.41883 (11)0.1056 (16)
H200.70530.58070.47790.127*
C210.69644 (19)0.49834 (10)0.32262 (13)0.1111 (17)
H210.64390.56430.31630.133*
C220.73734 (18)0.39272 (8)0.23467 (11)0.0762 (10)
H220.71420.38820.16890.091*
C150.69983 (9)0.04314 (8)0.14962 (7)0.0501 (6)
H1510.59610.05850.13470.060*
H1520.66370.02060.21960.060*
C160.85482 (11)0.17748 (7)0.15058 (7)0.0512 (6)
H1610.87860.20800.08450.061*
H1620.96390.15760.15430.061*
C10.75023 (14)0.00246 (10)0.52593 (7)0.0364 (6)0.861 (5)
C20.66111 (13)0.10162 (10)0.58257 (7)0.0365 (6)0.861 (5)
H20.57190.18160.55650.044*0.861 (5)
C30.70500 (15)0.08645 (12)0.67817 (8)0.0340 (6)0.861 (5)
H30.64440.15670.71740.041*0.861 (5)
C40.83668 (14)0.03042 (13)0.71721 (8)0.0322 (6)0.861 (5)
C50.92591 (17)0.13265 (13)0.65840 (10)0.0360 (6)0.861 (5)
H51.01770.21120.68330.043*0.861 (5)
C60.88150 (18)0.12042 (12)0.56367 (10)0.0392 (6)0.861 (5)
H60.94000.19160.52520.047*0.861 (5)
C70.88235 (19)0.04505 (17)0.82118 (8)0.0459 (8)0.861 (5)
O10.7680 (2)0.0291 (2)0.88169 (9)0.0561 (8)0.861 (5)
O21.0305 (2)0.1281 (2)0.83952 (11)0.0689 (9)0.861 (5)
N10.71382 (18)0.00314 (12)0.42732 (8)0.0490 (7)0.861 (5)
N20.61411 (19)0.11663 (13)0.38741 (8)0.0510 (7)0.912 (5)
N30.5251 (2)0.21343 (15)0.34306 (10)0.0612 (8)0.912 (5)
N1P0.584 (3)0.038 (2)0.4970 (17)0.093 (7)*0.149 (4)
C1P0.664 (3)0.020 (2)0.5724 (16)0.069 (3)*0.149 (4)
C2P0.5979 (17)0.0866 (14)0.6273 (10)0.069 (3)*0.149 (4)
H2P0.49830.16310.61000.083*0.149 (4)
C3P0.6762 (17)0.0823 (14)0.7072 (10)0.069 (3)*0.149 (4)
H3P0.62850.15450.74520.083*0.149 (4)
C4P0.8243 (17)0.0275 (14)0.7314 (10)0.069 (3)*0.149 (4)
C5P0.8941 (17)0.1331 (14)0.6758 (10)0.069 (3)*0.149 (4)
H5P0.99540.20820.69230.083*0.149 (4)
C6P0.8158 (17)0.1288 (14)0.5959 (10)0.069 (3)*0.149 (4)
H6P0.86550.20000.55700.083*0.149 (4)
C7P0.899 (3)0.049 (3)0.8276 (18)0.069 (3)*0.149 (4)
O1P0.817 (3)0.040 (2)0.8849 (15)0.069 (3)*0.149 (4)
O2P1.047 (2)0.142 (2)0.8341 (13)0.069 (3)*0.149 (4)
N2P0.636 (6)0.217 (4)0.318 (3)0.096*0.088 (5)
N3P0.569 (5)0.256 (4)0.409 (3)0.096*0.088 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N40.0427 (11)0.0379 (10)0.0376 (10)0.0104 (8)0.0154 (8)0.0034 (8)
C90.0371 (12)0.0355 (12)0.0514 (14)0.0134 (10)0.0158 (10)0.0026 (10)
C100.0454 (14)0.0448 (14)0.0497 (14)0.0107 (11)0.0159 (11)0.0030 (11)
C110.0565 (18)0.0593 (18)0.0638 (18)0.0174 (15)0.0041 (14)0.0175 (14)
C120.0455 (17)0.0444 (16)0.130 (3)0.0084 (13)0.0074 (19)0.0177 (18)
C130.0418 (16)0.0435 (17)0.177 (4)0.0116 (13)0.039 (2)0.025 (2)
C140.0516 (16)0.0442 (15)0.098 (2)0.0189 (13)0.0366 (16)0.0134 (15)
C80.0482 (14)0.0435 (13)0.0403 (12)0.0133 (11)0.0137 (11)0.0035 (10)
C170.0383 (12)0.0313 (11)0.0631 (16)0.0084 (10)0.0124 (11)0.0079 (11)
C180.0619 (17)0.0363 (13)0.0554 (15)0.0034 (12)0.0126 (13)0.0032 (11)
C190.073 (2)0.0522 (17)0.0685 (19)0.0131 (15)0.0046 (16)0.0139 (15)
C200.057 (2)0.0459 (18)0.153 (4)0.0039 (16)0.002 (2)0.026 (2)
C210.052 (2)0.0429 (18)0.221 (5)0.0114 (15)0.027 (3)0.007 (3)
C220.0476 (16)0.0539 (17)0.129 (3)0.0004 (14)0.0353 (18)0.0232 (19)
C150.0504 (14)0.0385 (12)0.0427 (13)0.0072 (11)0.0111 (11)0.0027 (10)
C160.0520 (14)0.0378 (13)0.0474 (13)0.0061 (11)0.0111 (11)0.0061 (10)
C10.0405 (15)0.0331 (12)0.0340 (13)0.0122 (11)0.0135 (11)0.0027 (10)
C20.0334 (13)0.0271 (12)0.0414 (14)0.0033 (10)0.0153 (11)0.0048 (10)
C30.0320 (12)0.0265 (11)0.0367 (13)0.0008 (9)0.0104 (10)0.0024 (10)
C40.0317 (12)0.0274 (11)0.0325 (12)0.0043 (9)0.0132 (10)0.0020 (9)
C50.0301 (12)0.0302 (12)0.0396 (14)0.0000 (10)0.0132 (10)0.0002 (10)
C60.0418 (15)0.0298 (12)0.0385 (14)0.0028 (11)0.0092 (11)0.0040 (10)
C70.0582 (19)0.0325 (13)0.0396 (15)0.0017 (13)0.0266 (13)0.0020 (11)
O10.0684 (19)0.0540 (14)0.0393 (11)0.0010 (13)0.0222 (11)0.0104 (10)
O20.0828 (18)0.0487 (14)0.0714 (16)0.0262 (12)0.0602 (14)0.0158 (11)
N10.0603 (16)0.0397 (13)0.0458 (14)0.0055 (11)0.0279 (12)0.0013 (10)
N20.0608 (15)0.0466 (14)0.0474 (14)0.0173 (12)0.0231 (11)0.0009 (11)
N30.077 (2)0.0483 (14)0.0594 (16)0.0210 (14)0.0386 (15)0.0137 (12)
Geometric parameters (Å, º) top
N4—C151.4981C16—H1620.9900
N4—C81.5068C1—C21.3943
N4—H020.9200C1—C61.3970
N4—H010.9200C1—N11.4353
C9—C141.3846C2—C31.3957
C9—C101.4012C2—H20.9500
C9—C81.4994C3—C41.3991
C10—C111.3873C3—H30.9500
C10—H100.9500C4—C51.3990
C11—C121.3716C4—C71.5149
C11—H110.9500C5—C61.3943
C12—C131.3920C5—H50.9500
C12—H120.9500C6—H60.9500
C13—C141.4060C7—O21.2641
C13—H130.9500C7—O11.2662
C14—H140.9500N1—N21.2481
C8—H810.9900N2—N31.1349
C8—H820.9900N1P—N1Pi1.33 (4)
C17—C221.3920N1P—C1P1.44 (3)
C17—C181.3965C1P—C2P1.39 (3)
C17—C161.5113C1P—C6P1.41 (3)
C18—C191.3935C2P—C3P1.3900
C18—H180.9500C2P—H2P0.9500
C19—C201.3690C3P—C4P1.3900
C19—H190.9500C3P—H3P0.9500
C20—C211.3868C4P—C5P1.3900
C20—H200.9500C4P—C7P1.52 (3)
C21—C221.4002C5P—C6P1.3900
C21—H210.9500C5P—H5P0.9500
C22—H220.9500C6P—H6P0.9500
C15—C161.5316C7P—O2P1.267 (16)
C15—H1510.9900C7P—O1P1.280 (16)
C15—H1520.9900N2P—N3P1.32 (5)
C16—H1610.9900
C15—N4—C8112.7C17—C16—C15110.9
C15—N4—H02109.0C17—C16—H161109.5
C8—N4—H02109.0C15—C16—H161109.5
C15—N4—H01109.0C17—C16—H162109.5
C8—N4—H01109.0C15—C16—H162109.5
H02—N4—H01107.8H161—C16—H162108.1
C14—C9—C10119.5C2—C1—C6120.9
C14—C9—C8121.4C2—C1—N1123.1
C10—C9—C8119.1C6—C1—N1116.0
C11—C10—C9120.6C1—C2—C3118.9
C11—C10—H10119.7C1—C2—H2120.5
C9—C10—H10119.7C3—C2—H2120.5
C12—C11—C10120.0C2—C3—C4121.1
C12—C11—H11120.0C2—C3—H3119.4
C10—C11—H11120.0C4—C3—H3119.4
C11—C12—C13120.2C5—C4—C3118.9
C11—C12—H12119.9C5—C4—C7120.7
C13—C12—H12119.9C3—C4—C7120.3
C12—C13—C14120.2C6—C5—C4120.7
C12—C13—H13119.9C6—C5—H5119.7
C14—C13—H13119.9C4—C5—H5119.7
C9—C14—C13119.5C5—C6—C1119.4
C9—C14—H14120.3C5—C6—H6120.3
C13—C14—H14120.3C1—C6—H6120.3
C9—C8—N4110.6O2—C7—O1125.8
C9—C8—H81109.5O2—C7—C4117.7
N4—C8—H81109.5O1—C7—C4116.4
C9—C8—H82109.5N2—N1—C1115.5
N4—C8—H82109.5N2—N1—N1i75.18 (8)
H81—C8—H82108.1C1—N1—N1i84.45 (5)
C22—C17—C18118.3N3—N2—N1172.9
C22—C17—C16121.5N1Pi—N1P—C1P111 (2)
C18—C17—C16120.2C2P—C1P—C6P118.8 (18)
C19—C18—C17120.9C2P—C1P—N1P126.8 (19)
C19—C18—H18119.5C6P—C1P—N1P114.2 (18)
C17—C18—H18119.5C3P—C2P—C1P120.7 (10)
C20—C19—C18120.5C3P—C2P—H2P119.6
C20—C19—H19119.7C1P—C2P—H2P119.6
C18—C19—H19119.7C4P—C3P—C2P120.0
C19—C20—C21119.3C4P—C3P—H3P120.0
C19—C20—H20120.3C2P—C3P—H3P120.0
C21—C20—H20120.3C5P—C4P—C3P120.0
C20—C21—C22120.8C5P—C4P—C7P117.2 (9)
C20—C21—H21119.6C3P—C4P—C7P122.2 (9)
C22—C21—H21119.6C4P—C5P—C6P120.0
C17—C22—C21120.1C4P—C5P—H5P120.0
C17—C22—H22120.0C6P—C5P—H5P120.0
C21—C22—H22120.0C5P—C6P—C1P120.4 (11)
N4—C15—C16110.3C5P—C6P—H6P119.8
N4—C15—H151109.6C1P—C6P—H6P119.8
C16—C15—H151109.6O2P—C7P—O1P128 (2)
N4—C15—H152109.6O2P—C7P—C4P115.9 (15)
C16—C15—H152109.6O1P—C7P—C4P115.7 (18)
H151—C15—H152108.1
C14—C9—C10—C110.8C4—C5—C6—C12.0
C8—C9—C10—C11179.8C2—C1—C6—C51.2
C9—C10—C11—C120.2N1—C1—C6—C5179.3
C10—C11—C12—C130.8C5—C4—C7—O218.6
C11—C12—C13—C141.2C3—C4—C7—O2161.0
C10—C9—C14—C130.4C5—C4—C7—O1162.1
C8—C9—C14—C13179.8C3—C4—C7—O118.3
C12—C13—C14—C90.6C2—C1—N1—N29.4
C14—C9—C8—N488.6C6—C1—N1—N2171.0
C10—C9—C8—N490.9C2—C1—N1—N1i61.23 (10)
C15—N4—C8—C9177.6C6—C1—N1—N1i118.35 (10)
C22—C17—C18—C190.1C1—N1—N2—N3178.2
C16—C17—C18—C19179.3N1i—N1—N2—N3101.95 (7)
C17—C18—C19—C200.2N1Pi—N1P—C1P—C2P15 (3)
C18—C19—C20—C210.7N1Pi—N1P—C1P—C6P160 (2)
C19—C20—C21—C221.0C6P—C1P—C2P—C3P2.8 (14)
C18—C17—C22—C210.5N1P—C1P—C2P—C3P172.1 (13)
C16—C17—C22—C21179.0C1P—C2P—C3P—C4P1.5 (7)
C20—C21—C22—C170.9C2P—C3P—C4P—C5P0.0
C8—N4—C15—C16179.6C2P—C3P—C4P—C7P171.2 (11)
C22—C17—C16—C1593.7C3P—C4P—C5P—C6P0.0
C18—C17—C16—C1585.7C7P—C4P—C5P—C6P171.6 (10)
N4—C15—C16—C17171.3C4P—C5P—C6P—C1P1.4 (7)
C6—C1—C2—C30.0C2P—C1P—C6P—C5P2.8 (14)
N1—C1—C2—C3179.6N1P—C1P—C6P—C5P172.8 (11)
C1—C2—C3—C40.3C5P—C4P—C7P—O2P17 (2)
C2—C3—C4—C50.5C3P—C4P—C7P—O2P172.0 (13)
C2—C3—C4—C7180.0C5P—C4P—C7P—O1P171.2 (15)
C3—C4—C5—C61.6C3P—C4P—C7P—O1P0 (2)
C7—C4—C5—C6178.8
Symmetry code: (i) x+1, y, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H02···O1ii0.921.822.6920 (14)158
N4—H01···O2iii0.921.812.678 (2)155
Symmetry codes: (ii) x, y, z1; (iii) x+2, y, z+1.
(Dibenzylammonium 4-azidebenzoate) 4-azidebenzoic acid clathrate (4a-db-I-i) top
Crystal data top
C28H25N7O4F(000) = 1096
Mr = 523.55Dx = 1.347 Mg m3
Monoclinic, P21/nMelting point: not measured K
a = 10.4763 (5) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.2909 (5) ÅCell parameters from 8192 reflections
c = 26.8857 (13) ŵ = 0.09 mm1
β = 99.468 (2)°T = 88 K
V = 2581.3 (2) Å3Block, pale-yellow
Z = 40.38 × 0.36 × 0.10 mm
Data collection top
Bruker SMART CCD area detector system
diffractometer
7514 independent reflections
Radiation source: rotating-anode6237 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.043
ω scansθmax = 30.0°, θmin = 1.5°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1414
Tmin = 0.965, Tmax = 0.991k = 1313
40617 measured reflectionsl = 3737
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)] = 0.035Hydrogen site location: difference Fourier map
wR(F2) = 0.105Only H-atom coordinates refined
S = 1.10 w = 1/[σ2(Fo2) + (0.0602P)2 + 0.2618P]
where P = (Fo2 + 2Fc2)/3
7514 reflections(Δ/σ)max = 0.001
428 parametersΔρmax = 0.35 e Å3
0 restraintsΔρmin = 0.27 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
C7A0.91063 (8)0.46223 (9)0.19194 (3)0.01394 (16)
C1A1.10690 (9)0.58437 (10)0.06960 (3)0.01712 (17)
C2A1.06942 (9)0.44159 (10)0.07395 (3)0.01835 (18)
H2A1.0847 (12)0.3665 (15)0.0488 (5)0.022*
C3A1.00551 (9)0.40244 (10)0.11346 (3)0.01661 (17)
H3A0.9783 (12)0.3030 (14)0.1158 (5)0.020*
C4A0.98124 (8)0.50317 (10)0.14931 (3)0.01424 (16)
C5A1.02282 (9)0.64470 (10)0.14501 (4)0.01730 (17)
H5A1.0096 (12)0.7167 (14)0.1699 (5)0.021*
C6A1.08359 (9)0.68633 (10)0.10507 (4)0.01887 (18)
H6A1.1082 (13)0.7868 (15)0.1012 (5)0.023*
N1A1.17086 (9)0.63625 (10)0.02999 (3)0.02252 (17)
N2A1.20732 (9)0.54155 (10)0.00269 (3)0.02396 (18)
N3A1.24501 (11)0.46644 (12)0.02456 (4)0.0358 (2)
O2A0.85798 (6)0.33725 (7)0.19006 (2)0.01610 (13)
O1A0.90660 (7)0.54922 (7)0.22693 (2)0.01814 (14)
C7B0.60372 (9)0.19720 (10)0.11843 (4)0.01812 (18)
C1B0.32340 (9)0.10927 (10)0.01213 (4)0.01995 (19)
C2B0.29438 (10)0.08144 (12)0.03577 (4)0.0246 (2)
H2B0.2112 (14)0.0394 (16)0.0396 (5)0.030*
C3B0.38688 (10)0.11122 (12)0.07777 (4)0.0238 (2)
H3B0.3691 (13)0.0908 (15)0.1112 (5)0.029*
C4B0.50712 (9)0.16822 (10)0.07230 (3)0.01788 (18)
C5B0.53386 (10)0.19668 (10)0.02400 (4)0.01860 (18)
H5B0.6190 (13)0.2338 (14)0.0201 (5)0.022*
C6B0.44223 (10)0.16719 (10)0.01823 (4)0.01978 (18)
H6B0.4618 (13)0.1807 (14)0.0525 (5)0.024*
N1B0.23633 (9)0.07975 (10)0.05782 (3)0.02518 (18)
N2B0.13687 (9)0.01086 (10)0.05374 (3)0.02553 (19)
N3B0.04313 (10)0.05135 (13)0.05600 (4)0.0361 (2)
O1B0.71772 (7)0.24175 (8)0.10853 (3)0.02112 (15)
O2B0.57967 (8)0.18208 (8)0.16103 (3)0.02374 (16)
H030.7653 (17)0.2723 (19)0.1373 (7)0.047 (5)*
C80.89352 (9)0.93862 (10)0.25916 (3)0.01663 (17)
H810.9117 (12)0.9182 (14)0.2947 (5)0.020*
H820.8463 (12)1.0286 (15)0.2534 (5)0.020*
C91.01782 (9)0.94611 (9)0.23779 (3)0.01529 (16)
C101.03023 (9)1.03984 (10)0.19847 (4)0.01833 (18)
H100.9559 (13)1.0958 (14)0.1825 (5)0.022*
C111.14928 (10)1.05688 (11)0.18230 (4)0.02173 (19)
H111.1572 (13)1.1247 (15)0.1547 (5)0.026*
C121.25692 (10)0.98118 (11)0.20575 (4)0.0229 (2)
H121.3408 (14)0.9970 (15)0.1948 (5)0.027*
C131.24458 (10)0.88448 (11)0.24428 (4)0.02218 (19)
H131.3206 (13)0.8313 (15)0.2605 (5)0.027*
C141.12543 (9)0.86654 (11)0.26017 (4)0.01892 (18)
H141.1171 (13)0.8029 (15)0.2880 (5)0.023*
C150.73730 (9)0.85791 (10)0.18389 (3)0.01673 (17)
H1510.8073 (12)0.8605 (14)0.1628 (5)0.020*
H1520.6986 (12)0.9539 (14)0.1842 (5)0.020*
C160.63326 (8)0.75101 (10)0.16403 (3)0.01482 (16)
C170.65232 (9)0.64938 (10)0.12780 (3)0.01572 (17)
H170.7369 (12)0.6470 (14)0.1153 (5)0.019*
C180.55284 (9)0.55533 (10)0.10825 (3)0.01768 (17)
H180.5686 (12)0.4851 (14)0.0824 (5)0.021*
C190.43450 (9)0.56155 (11)0.12530 (4)0.01989 (18)
H190.3654 (13)0.4947 (15)0.1123 (5)0.024*
C200.41478 (9)0.66225 (11)0.16165 (4)0.02147 (19)
H200.3313 (13)0.6628 (15)0.1733 (5)0.026*
C210.51389 (9)0.75676 (11)0.18081 (4)0.01876 (18)
H210.5023 (12)0.8293 (15)0.2062 (5)0.023*
N40.80110 (7)0.82311 (8)0.23663 (3)0.01398 (14)
H020.8400 (12)0.7338 (14)0.2377 (5)0.017*
H010.7379 (12)0.8174 (13)0.2588 (5)0.017*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C7A0.0122 (4)0.0158 (4)0.0134 (4)0.0033 (3)0.0009 (3)0.0002 (3)
C1A0.0147 (4)0.0219 (4)0.0150 (4)0.0006 (3)0.0032 (3)0.0008 (3)
C2A0.0194 (4)0.0204 (4)0.0161 (4)0.0012 (3)0.0054 (3)0.0028 (3)
C3A0.0182 (4)0.0157 (4)0.0163 (4)0.0007 (3)0.0040 (3)0.0016 (3)
C4A0.0131 (4)0.0165 (4)0.0131 (4)0.0015 (3)0.0017 (3)0.0009 (3)
C5A0.0170 (4)0.0172 (4)0.0179 (4)0.0003 (3)0.0039 (3)0.0030 (3)
C6A0.0187 (4)0.0177 (4)0.0207 (4)0.0021 (3)0.0047 (3)0.0013 (3)
N1A0.0251 (4)0.0249 (4)0.0194 (4)0.0011 (3)0.0092 (3)0.0004 (3)
N2A0.0234 (4)0.0295 (4)0.0207 (4)0.0016 (3)0.0089 (3)0.0040 (3)
N3A0.0434 (6)0.0393 (6)0.0300 (5)0.0088 (5)0.0215 (4)0.0027 (4)
O2A0.0169 (3)0.0162 (3)0.0154 (3)0.0005 (2)0.0030 (2)0.0009 (2)
O1A0.0211 (3)0.0182 (3)0.0156 (3)0.0019 (2)0.0044 (2)0.0029 (2)
C7B0.0212 (4)0.0149 (4)0.0176 (4)0.0013 (3)0.0013 (3)0.0002 (3)
C1B0.0209 (4)0.0182 (4)0.0191 (4)0.0021 (3)0.0017 (3)0.0009 (3)
C2B0.0192 (4)0.0319 (5)0.0226 (5)0.0034 (4)0.0035 (4)0.0032 (4)
C3B0.0223 (5)0.0316 (5)0.0180 (4)0.0022 (4)0.0052 (4)0.0021 (4)
C4B0.0195 (4)0.0171 (4)0.0163 (4)0.0013 (3)0.0008 (3)0.0011 (3)
C5B0.0214 (4)0.0155 (4)0.0183 (4)0.0010 (3)0.0016 (3)0.0019 (3)
C6B0.0247 (5)0.0166 (4)0.0169 (4)0.0000 (3)0.0003 (3)0.0027 (3)
N1B0.0247 (4)0.0270 (4)0.0214 (4)0.0036 (3)0.0037 (3)0.0004 (3)
N2B0.0235 (4)0.0285 (4)0.0226 (4)0.0012 (3)0.0021 (3)0.0045 (3)
N3B0.0262 (5)0.0469 (6)0.0336 (5)0.0074 (4)0.0001 (4)0.0089 (5)
O1B0.0200 (3)0.0252 (4)0.0174 (3)0.0019 (3)0.0009 (3)0.0041 (3)
O2B0.0291 (4)0.0257 (4)0.0161 (3)0.0027 (3)0.0026 (3)0.0012 (3)
C80.0158 (4)0.0176 (4)0.0171 (4)0.0034 (3)0.0045 (3)0.0060 (3)
C90.0153 (4)0.0149 (4)0.0161 (4)0.0013 (3)0.0039 (3)0.0044 (3)
C100.0168 (4)0.0161 (4)0.0225 (4)0.0023 (3)0.0046 (3)0.0006 (3)
C110.0212 (4)0.0194 (4)0.0263 (5)0.0019 (3)0.0091 (4)0.0045 (4)
C120.0185 (4)0.0232 (5)0.0289 (5)0.0025 (4)0.0095 (4)0.0017 (4)
C130.0177 (4)0.0241 (5)0.0247 (5)0.0050 (4)0.0034 (4)0.0024 (4)
C140.0196 (4)0.0201 (4)0.0172 (4)0.0014 (3)0.0035 (3)0.0007 (3)
C150.0183 (4)0.0180 (4)0.0133 (4)0.0010 (3)0.0007 (3)0.0016 (3)
C160.0151 (4)0.0159 (4)0.0127 (4)0.0019 (3)0.0000 (3)0.0021 (3)
C170.0166 (4)0.0175 (4)0.0132 (4)0.0021 (3)0.0026 (3)0.0021 (3)
C180.0215 (4)0.0166 (4)0.0139 (4)0.0015 (3)0.0003 (3)0.0010 (3)
C190.0174 (4)0.0213 (4)0.0191 (4)0.0019 (3)0.0026 (3)0.0023 (3)
C200.0135 (4)0.0287 (5)0.0218 (4)0.0025 (4)0.0018 (3)0.0018 (4)
C210.0160 (4)0.0231 (4)0.0168 (4)0.0047 (3)0.0017 (3)0.0012 (3)
N40.0146 (3)0.0149 (3)0.0123 (3)0.0004 (3)0.0019 (3)0.0011 (3)
Geometric parameters (Å, º) top
C7A—O1A1.2462 (11)C8—N41.5044 (11)
C7A—O2A1.2829 (11)C8—C91.5090 (12)
C7A—C4A1.5115 (12)C8—H810.961 (13)
C1A—C2A1.3938 (13)C8—H820.971 (13)
C1A—C6A1.3939 (13)C9—C101.3921 (13)
C1A—N1A1.4320 (12)C9—C141.3987 (13)
C2A—C3A1.3939 (13)C10—C111.3957 (13)
C2A—H2A1.003 (13)C10—H100.975 (13)
C3A—C4A1.3965 (12)C11—C121.3892 (14)
C3A—H3A0.972 (13)C11—H110.987 (14)
C4A—C5A1.3960 (13)C12—C131.3931 (14)
C5A—C6A1.3903 (13)C12—H120.983 (14)
C5A—H5A0.973 (13)C13—C141.3943 (14)
C6A—H6A0.979 (14)C13—H130.977 (14)
N1A—N2A1.2453 (12)C14—H140.969 (14)
N2A—N3A1.1291 (13)C15—N41.5000 (11)
C7B—O2B1.2209 (12)C15—C161.5060 (13)
C7B—O1B1.3315 (12)C15—H1510.999 (13)
C7B—C4B1.4905 (13)C15—H1520.980 (13)
C1B—C6B1.3905 (14)C16—C171.3944 (12)
C1B—C2B1.3951 (14)C16—C211.3986 (13)
C1B—N1B1.4310 (13)C17—C181.3949 (13)
C2B—C3B1.3897 (14)C17—H170.998 (13)
C2B—H2B0.976 (15)C18—C191.3919 (14)
C3B—C4B1.3964 (14)C18—H180.987 (13)
C3B—H3B0.967 (14)C19—C201.3927 (14)
C4B—C5B1.3982 (13)C19—H190.974 (14)
C5B—C6B1.3880 (13)C20—C211.3924 (14)
C5B—H5B0.978 (13)C20—H200.976 (14)
C6B—H6B0.986 (14)C21—H210.981 (14)
N1B—N2B1.2431 (13)N4—H020.923 (13)
N2B—N3B1.1325 (14)N4—H010.963 (13)
O1B—H030.895 (18)
O1A—C7A—O2A123.30 (8)C9—C8—H82110.4 (8)
O1A—C7A—C4A119.39 (8)H81—C8—H82109.9 (11)
O2A—C7A—C4A117.31 (8)C10—C9—C14119.21 (8)
C2A—C1A—C6A120.40 (8)C10—C9—C8120.81 (8)
C2A—C1A—N1A123.74 (8)C14—C9—C8119.79 (8)
C6A—C1A—N1A115.86 (8)C9—C10—C11120.48 (9)
C1A—C2A—C3A119.31 (8)C9—C10—H10120.0 (8)
C1A—C2A—H2A121.8 (8)C11—C10—H10119.5 (8)
C3A—C2A—H2A118.9 (8)C12—C11—C7A120.10 (9)
C2A—C3A—C4A121.06 (9)C12—C11—H11120.1 (8)
C2A—C3A—H3A118.8 (8)C10—C11—H11119.8 (8)
C4A—C3A—H3A120.2 (8)C11—C12—C13119.75 (9)
C5A—C4A—C3A118.64 (8)C11—C12—H12119.2 (8)
C5A—C4A—C7A119.88 (8)C13—C12—H12121.1 (8)
C3A—C4A—C7A121.48 (8)C12—C13—C14120.14 (9)
C6A—C5A—C4A120.98 (8)C12—C13—H13119.4 (8)
C6A—C5A—H5A118.4 (8)C14—C13—H13120.4 (8)
C4A—C5A—H5A120.6 (8)C13—C14—C9120.26 (9)
C5A—C6A—C1A119.56 (9)C13—C14—H14120.6 (8)
C5A—C6A—H6A120.6 (8)C9—C14—H14119.1 (8)
C1A—C6A—H6A119.8 (8)N4—C15—C16112.15 (7)
N2A—N1A—C1A115.27 (9)N4—C15—H151106.7 (7)
N3A—N2A—N1A173.20 (11)C16—C15—H151111.7 (7)
O2B—C7B—O1B123.62 (9)N4—C15—H152108.0 (8)
O2B—C7B—C4B122.90 (9)C16—C15—H152109.1 (8)
O1B—C7B—C4B113.48 (8)H151—C15—H152109.1 (11)
C6B—C1B—C2B121.06 (9)C17—C16—C21119.32 (8)
C6B—C1B—N1B115.44 (9)C17—C16—C15121.06 (8)
C2B—C1B—N1B123.50 (9)C21—C16—C15119.59 (8)
C3B—C2B—C1B118.98 (9)C16—C17—C18120.23 (8)
C3B—C2B—H2B120.6 (8)C16—C17—H17119.2 (7)
C1B—C2B—H2B120.4 (8)C18—C17—H17120.6 (7)
C2B—C3B—C4B120.70 (9)C19—C18—C17120.04 (9)
C2B—C3B—H3B120.1 (8)C19—C18—H18121.4 (8)
C4B—C3B—H3B119.2 (8)C17—C18—H18118.6 (8)
C3B—C4B—C5B119.44 (9)C18—C19—C20120.14 (9)
C3B—C4B—C7B118.80 (9)C18—C19—H19120.3 (8)
C5B—C4B—C7B121.76 (9)C20—C19—H19119.6 (8)
C6B—C5B—C4B120.34 (9)C21—C20—C19119.71 (9)
C6B—C5B—H5B120.1 (8)C21—C20—H20122.0 (8)
C4B—C5B—H5B119.5 (8)C19—C20—H20118.2 (8)
C5B—C6B—C1B119.47 (9)C20—C21—C16120.56 (9)
C5B—C6B—H6B121.2 (8)C20—C21—H21121.4 (8)
C1B—C6B—H6B119.2 (8)C16—C21—H21118.1 (8)
N2B—N1B—C1B116.62 (9)C15—N4—C8112.59 (7)
N3B—N2B—N1B171.96 (11)C15—N4—H02110.4 (8)
C7B—O1B—H03108.4 (11)C8—N4—H02112.2 (8)
N4—C8—C9114.71 (7)C15—N4—H01110.6 (8)
N4—C8—H81105.5 (8)C8—N4—H01104.7 (7)
C9—C8—H81110.2 (8)H02—N4—H01106.1 (11)
N4—C8—H82105.8 (8)
C6A—C1A—C2A—C3A1.55 (14)C4B—C5B—C6B—C1B0.10 (14)
N1A—C1A—C2A—C3A178.83 (9)C2B—C1B—C6B—C5B0.54 (15)
C1A—C2A—C3A—C4A1.50 (14)N1B—C1B—C6B—C5B178.75 (9)
C2A—C3A—C4A—C5A0.25 (13)C6B—C1B—N1B—N2B170.83 (9)
C2A—C3A—C4A—C7A179.27 (8)C2B—C1B—N1B—N2B8.44 (15)
O1A—C7A—C4A—C5A10.38 (12)C1B—N1B—N2B—N3B176.8 (8)
O2A—C7A—C4A—C5A169.99 (8)N4—C8—C9—C1094.46 (10)
O1A—C7A—C4A—C3A170.10 (8)N4—C8—C9—C1490.60 (10)
O2A—C7A—C4A—C3A9.53 (12)C14—C9—C10—C111.48 (14)
C3A—C4A—C5A—C6A1.99 (14)C8—C9—C10—C11173.49 (9)
C7A—C4A—C5A—C6A177.54 (8)C9—C10—C11—C120.63 (15)
C4A—C5A—C6A—C1A1.95 (14)C7A—C11—C12—C132.23 (16)
C2A—C1A—C6A—C5A0.15 (14)C11—C12—C13—C141.70 (16)
N1A—C1A—C6A—C5A179.50 (9)C12—C13—C14—C90.42 (15)
C2A—C1A—N1A—N2A9.23 (14)C10—C9—C14—C132.01 (14)
C6A—C1A—N1A—N2A170.40 (9)C8—C9—C14—C13173.02 (9)
C1A—N1A—N2A—N3A179 (100)N4—C15—C16—C17106.64 (9)
C6B—C1B—C2B—C3B0.62 (16)N4—C15—C16—C2175.63 (10)
N1B—C1B—C2B—C3B178.61 (10)C21—C16—C17—C180.53 (13)
C1B—C2B—C3B—C4B0.05 (17)C15—C16—C17—C18177.21 (8)
C2B—C3B—C4B—C5B0.58 (16)C16—C17—C18—C190.74 (13)
C2B—C3B—C4B—C7B179.46 (10)C17—C18—C19—C200.44 (14)
O2B—C7B—C4B—C3B4.87 (15)C18—C19—C20—C210.07 (14)
O1B—C7B—C4B—C3B175.53 (9)C19—C20—C21—C160.28 (15)
O2B—C7B—C4B—C5B175.09 (9)C17—C16—C21—C200.02 (14)
O1B—C7B—C4B—C5B4.50 (13)C15—C16—C21—C20177.75 (9)
C3B—C4B—C5B—C6B0.65 (15)C16—C15—N4—C8172.97 (7)
C7B—C4B—C5B—C6B179.38 (9)C9—C8—N4—C1572.50 (10)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1B—H03···O2A0.895 (18)1.692 (19)2.5869 (10)177.0 (17)
N4—H02···O1A0.923 (13)1.891 (13)2.8036 (10)169.3 (12)
N4—H01···O2Ai0.963 (13)1.840 (13)2.7856 (10)166.5 (11)
Symmetry code: (i) x+3/2, y+1/2, z+1/2.
Dibenzylammonium 4-azidebenzoate (4a-db-II-i) top
Crystal data top
C21H20N4O2Dx = 1.258 Mg m3
Mr = 360.41Melting point: not measured K
Orthorhombic, PbcaMo Kα radiation, λ = 0.71075 Å
a = 8.9331 (3) ÅCell parameters from 35949 reflections
b = 16.5714 (7) ŵ = 0.08 mm1
c = 25.7127 (9) ÅT = 78 K
V = 3806.4 (2) Å3Needle, pale-yellow
Z = 80.42 × 0.17 × 0.16 mm
F(000) = 1520
Data collection top
Rigaku RAXIS-RAPID IP area detector system
diffractometer
4248 independent reflections
Radiation source: rotating anode3698 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.054
Oscillation Photograph scansθmax = 27.5°, θmin = 3.0°
Absorption correction: empirical (using intensity measurements)
ABSCOR (Higashi, 1995)
h = 1110
Tmin = 0.966, Tmax = 0.987k = 2121
30191 measured reflectionsl = 3333
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)] = 0.054Hydrogen site location: difference Fourier map
wR(F2) = 0.121Only H-atom coordinates refined
S = 1.11 w = 1/[σ2(Fo2) + (0.0542P)2 + 1.6574P]
where P = (Fo2 + 2Fc2)/3
4248 reflections(Δ/σ)max = 0.001
306 parametersΔρmax = 0.25 e Å3
0 restraintsΔρmin = 0.28 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
N10.12430 (16)0.03020 (10)0.72512 (6)0.0383 (4)
N20.01742 (16)0.00766 (9)0.70645 (5)0.0332 (3)
N30.06905 (19)0.04387 (11)0.68456 (6)0.0458 (4)
O10.07559 (11)0.19827 (6)0.93805 (4)0.0235 (2)
O20.15512 (11)0.24885 (7)0.93047 (4)0.0242 (2)
C70.04879 (14)0.20548 (8)0.91504 (5)0.0188 (3)
C10.10044 (17)0.07095 (10)0.77354 (6)0.0261 (3)
C20.21055 (17)0.12507 (11)0.78865 (6)0.0298 (3)
H20.296 (2)0.1330 (12)0.7662 (7)0.036*
C30.19369 (16)0.16816 (10)0.83439 (6)0.0258 (3)
H30.270 (2)0.2065 (12)0.8443 (7)0.031*
C40.06708 (15)0.15822 (9)0.86524 (5)0.0197 (3)
C50.04116 (15)0.10289 (9)0.84970 (5)0.0226 (3)
H50.1291 (19)0.0960 (11)0.8702 (7)0.027*
C60.02439 (16)0.05822 (10)0.80451 (6)0.0246 (3)
H60.101 (2)0.0202 (12)0.7948 (7)0.030*
N40.44817 (12)0.24645 (7)0.96608 (4)0.0174 (2)
H020.354 (2)0.2461 (12)0.9510 (7)0.033 (5)*
H010.436 (2)0.2608 (13)1.0023 (8)0.039 (5)*
C80.51709 (16)0.16455 (9)0.96173 (6)0.0223 (3)
H810.610 (2)0.1673 (11)0.9804 (7)0.027*
H820.5374 (18)0.1534 (11)0.9237 (7)0.027*
C90.41222 (15)0.10255 (8)0.98438 (5)0.0204 (3)
C100.40941 (16)0.08806 (9)1.03768 (6)0.0235 (3)
H100.479 (2)0.1172 (11)1.0608 (7)0.028*
C110.30891 (17)0.03254 (10)1.05826 (6)0.0266 (3)
H110.3064 (19)0.0236 (11)1.0964 (7)0.032*
C120.21058 (16)0.00860 (10)1.02588 (7)0.0281 (3)
H120.142 (2)0.0484 (12)1.0398 (7)0.034*
C130.21268 (17)0.00630 (10)0.97291 (6)0.0284 (3)
H130.146 (2)0.0219 (12)0.9498 (7)0.034*
C140.31361 (16)0.06112 (9)0.95222 (6)0.0248 (3)
H140.3155 (19)0.0703 (11)0.9147 (7)0.030*
C150.54254 (16)0.31284 (9)0.94391 (5)0.0207 (3)
H1510.644 (2)0.3049 (11)0.9585 (6)0.025*
H1520.5000 (19)0.3633 (11)0.9574 (6)0.025*
C160.54500 (15)0.31313 (9)0.88554 (5)0.0210 (3)
C170.42758 (16)0.34675 (9)0.85731 (6)0.0241 (3)
H170.345 (2)0.3710 (11)0.8752 (7)0.029*
C180.42891 (19)0.34448 (11)0.80328 (6)0.0313 (4)
H180.344 (2)0.3694 (13)0.7845 (7)0.038*
C190.5472 (2)0.30913 (13)0.77727 (6)0.0408 (4)
H190.548 (2)0.3082 (13)0.7397 (9)0.049*
C200.6653 (2)0.27688 (13)0.80503 (7)0.0430 (5)
H200.752 (3)0.2542 (14)0.7870 (8)0.052*
C210.66453 (18)0.27884 (11)0.85895 (6)0.0326 (4)
H210.750 (2)0.2571 (12)0.8785 (7)0.039*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0317 (7)0.0480 (9)0.0354 (8)0.0120 (6)0.0099 (6)0.0181 (7)
N20.0354 (7)0.0375 (9)0.0267 (7)0.0042 (6)0.0048 (5)0.0079 (6)
N30.0476 (9)0.0546 (11)0.0351 (8)0.0123 (8)0.0022 (7)0.0150 (7)
O10.0204 (5)0.0280 (6)0.0222 (5)0.0029 (4)0.0007 (4)0.0020 (4)
O20.0186 (5)0.0245 (6)0.0296 (5)0.0009 (4)0.0031 (4)0.0039 (4)
C70.0183 (6)0.0180 (7)0.0202 (6)0.0016 (5)0.0038 (5)0.0033 (5)
C10.0272 (7)0.0278 (8)0.0232 (7)0.0011 (6)0.0020 (6)0.0041 (6)
C20.0240 (7)0.0333 (9)0.0322 (8)0.0063 (6)0.0091 (6)0.0042 (6)
C30.0219 (7)0.0257 (8)0.0298 (7)0.0058 (6)0.0028 (6)0.0028 (6)
C40.0186 (6)0.0197 (7)0.0207 (6)0.0012 (5)0.0017 (5)0.0027 (5)
C50.0187 (7)0.0272 (8)0.0217 (7)0.0022 (5)0.0003 (5)0.0021 (5)
C60.0208 (7)0.0276 (8)0.0253 (7)0.0042 (6)0.0023 (5)0.0013 (6)
N40.0156 (5)0.0159 (6)0.0206 (5)0.0004 (4)0.0002 (4)0.0004 (4)
C80.0198 (7)0.0156 (7)0.0314 (7)0.0012 (5)0.0032 (5)0.0004 (5)
C90.0169 (6)0.0145 (7)0.0299 (7)0.0031 (5)0.0009 (5)0.0007 (5)
C100.0209 (7)0.0195 (7)0.0301 (7)0.0019 (5)0.0014 (5)0.0008 (5)
C110.0260 (7)0.0232 (8)0.0306 (8)0.0041 (6)0.0027 (6)0.0052 (6)
C120.0220 (7)0.0178 (8)0.0444 (9)0.0009 (6)0.0049 (6)0.0062 (6)
C130.0238 (7)0.0214 (8)0.0401 (9)0.0038 (6)0.0052 (6)0.0005 (6)
C140.0244 (7)0.0207 (8)0.0292 (7)0.0001 (5)0.0014 (6)0.0001 (6)
C150.0220 (7)0.0171 (7)0.0230 (7)0.0037 (5)0.0008 (5)0.0008 (5)
C160.0209 (7)0.0182 (7)0.0238 (7)0.0044 (5)0.0005 (5)0.0028 (5)
C170.0224 (7)0.0218 (8)0.0281 (7)0.0012 (5)0.0013 (5)0.0026 (6)
C180.0343 (8)0.0317 (9)0.0278 (8)0.0024 (7)0.0072 (6)0.0071 (6)
C190.0492 (11)0.0518 (12)0.0213 (8)0.0005 (9)0.0022 (7)0.0043 (7)
C200.0393 (10)0.0578 (13)0.0318 (9)0.0094 (9)0.0116 (7)0.0013 (8)
C210.0245 (7)0.0424 (10)0.0307 (8)0.0063 (7)0.0017 (6)0.0051 (7)
Geometric parameters (Å, º) top
N1—N21.239 (2)C9—C101.392 (2)
N1—C11.4325 (19)C10—C111.390 (2)
N2—N31.128 (2)C10—H100.986 (18)
O1—C71.2645 (16)C11—C121.389 (2)
O2—C71.2554 (17)C11—H110.991 (18)
C7—C41.5099 (19)C12—C131.384 (2)
C1—C61.386 (2)C12—H120.97 (2)
C1—C21.387 (2)C13—C141.386 (2)
C2—C31.384 (2)C13—H130.964 (19)
C2—H20.968 (19)C14—H140.976 (18)
C3—C41.3912 (19)C15—C161.5010 (19)
C3—H30.969 (19)C15—H1510.991 (17)
C4—C51.3911 (19)C15—H1520.982 (18)
C5—C61.386 (2)C16—C211.389 (2)
C5—H50.953 (18)C16—C171.392 (2)
C6—H60.963 (19)C17—C181.390 (2)
N4—C81.4946 (18)C17—H170.960 (18)
N4—C151.4987 (17)C18—C191.381 (3)
N4—H020.93 (2)C18—H180.99 (2)
N4—H010.97 (2)C19—C201.381 (3)
C8—C91.5074 (19)C19—H190.97 (2)
C8—H810.960 (18)C20—C211.387 (2)
C8—H821.012 (17)C20—H200.98 (2)
C9—C141.390 (2)C21—H210.98 (2)
N2—N1—C1117.44 (13)C11—C10—H10120.2 (10)
N3—N2—N1171.81 (16)C9—C10—H10119.8 (11)
O2—C7—O1124.83 (13)C12—C11—C10120.35 (14)
O2—C7—C4118.89 (12)C12—C11—H11120.3 (11)
O1—C7—C4116.28 (12)C10—C11—H11119.3 (11)
C6—C1—C2120.54 (14)C13—C12—C11119.57 (14)
C6—C1—N1123.17 (14)C13—C12—H12119.5 (11)
C2—C1—N1116.29 (13)C11—C12—H12120.9 (11)
C3—C2—C1119.64 (14)C12—C13—C14120.23 (14)
C3—C2—H2121.5 (11)C12—C13—H13120.8 (11)
C1—C2—H2118.8 (11)C14—C13—H13119.0 (11)
C2—C3—C4120.78 (14)C13—C14—C9120.50 (14)
C2—C3—H3119.0 (11)C13—C14—H14119.5 (11)
C4—C3—H3120.2 (10)C9—C14—H14120.0 (11)
C5—C4—C3118.64 (13)N4—C15—C16113.01 (11)
C5—C4—C7120.68 (12)N4—C15—H151105.8 (10)
C3—C4—C7120.66 (13)C16—C15—H151111.5 (10)
C6—C5—C4121.18 (13)N4—C15—H152105.8 (10)
C6—C5—H5119.3 (11)C16—C15—H152110.9 (10)
C4—C5—H5119.5 (11)H151—C15—H152109.5 (15)
C5—C6—C1119.16 (14)C21—C16—C17119.09 (13)
C5—C6—H6119.3 (11)C21—C16—C15120.13 (13)
C1—C6—H6121.5 (11)C17—C16—C15120.77 (13)
C8—N4—C15113.98 (11)C18—C17—C16120.27 (14)
C8—N4—H02109.7 (12)C18—C17—H17119.9 (10)
C15—N4—H02110.8 (12)C16—C17—H17119.9 (10)
C8—N4—H01110.0 (12)C19—C18—C17120.13 (15)
C15—N4—H01104.5 (12)C19—C18—H18121.7 (11)
H02—N4—H01107.6 (16)C17—C18—H18118.1 (11)
N4—C8—C9109.51 (11)C20—C19—C18119.89 (15)
N4—C8—H81106.0 (11)C20—C19—H19120.4 (13)
C9—C8—H81112.1 (11)C18—C19—H19119.7 (13)
N4—C8—H82108.2 (10)C19—C20—C21120.24 (16)
C9—C8—H82111.2 (10)C19—C20—H20120.6 (13)
H81—C8—H82109.7 (14)C21—C20—H20119.2 (13)
C14—C9—C10119.30 (13)C20—C21—C16120.36 (15)
C14—C9—C8120.04 (13)C20—C21—H21120.0 (11)
C10—C9—C8120.62 (13)C16—C21—H21119.7 (11)
C11—C10—C9120.04 (14)
C1—N1—N2—N3176.3 (14)C14—C9—C10—C110.1 (2)
N2—N1—C1—C612.1 (3)C8—C9—C10—C11178.00 (13)
N2—N1—C1—C2168.04 (16)C9—C10—C11—C120.2 (2)
C6—C1—C2—C31.6 (3)C10—C11—C12—C130.3 (2)
N1—C1—C2—C3178.49 (16)C11—C12—C13—C140.9 (2)
C1—C2—C3—C40.4 (3)C12—C13—C14—C90.9 (2)
C2—C3—C4—C51.2 (2)C10—C9—C14—C130.4 (2)
C2—C3—C4—C7179.83 (14)C8—C9—C14—C13177.46 (13)
O2—C7—C4—C5173.03 (13)C8—N4—C15—C1673.63 (15)
O1—C7—C4—C57.41 (19)N4—C15—C16—C2198.90 (16)
O2—C7—C4—C35.9 (2)N4—C15—C16—C1780.42 (17)
O1—C7—C4—C3173.64 (13)C21—C16—C17—C181.3 (2)
C3—C4—C5—C60.0 (2)C15—C16—C17—C18178.04 (14)
C7—C4—C5—C6178.93 (13)C16—C17—C18—C190.3 (3)
C4—C5—C6—C12.0 (2)C17—C18—C19—C200.8 (3)
C2—C1—C6—C52.8 (2)C18—C19—C20—C210.9 (3)
N1—C1—C6—C5177.29 (15)C19—C20—C21—C160.1 (3)
C15—N4—C8—C9179.16 (11)C17—C16—C21—C201.2 (3)
N4—C8—C9—C1494.56 (15)C15—C16—C21—C20178.14 (17)
N4—C8—C9—C1083.30 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H01···O1i0.97 (2)1.68 (2)2.6384 (15)170.0 (19)
N4—H02···O20.93 (2)1.86 (2)2.7736 (15)171.5 (17)
Symmetry code: (i) x+1/2, y+1/2, z+2.
Dicyclohexylammonium 4-azidebenzoate (4a-dc-i) top
Crystal data top
C19H28N4O2Z = 2
Mr = 344.45F(000) = 372
Triclinic, p1Dx = 1.234 Mg m3
a = 9.0015 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.3009 (2) ÅCell parameters from 8192 reflections
c = 11.8819 (1) ŵ = 0.08 mm1
α = 107.909 (1)°T = 80 K
β = 100.454 (1)°Plate, pale-yellow
γ = 91.613 (1)°0.23 × 0.18 × 0.16 mm
V = 927.11 (3) Å3
Data collection top
Bruker SMART CCD area detector system
diffractometer
5369 independent reflections
Radiation source: rotating anode4476 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
ω scansθmax = 30.0°, θmin = 1.8°
Absorption correction: empirical (using intensity measurements)
Program SADABS was used.
h = 1212
Tmin = 0.981, Tmax = 0.987k = 1313
14876 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)] = 0.036Hydrogen site location: difference Fourier map
wR(F2) = 0.109H atoms treated by a mixture of independent and constrained refinement
S = 1.09 w = 1/[σ2(Fo2) + (0.0705P)2]
where P = (Fo2 + 2Fc2)/3
5369 reflections(Δ/σ)max < 0.001
306 parametersΔρmax = 0.43 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
C70.34728 (9)0.23018 (9)0.21129 (7)0.01336 (15)
C40.27903 (9)0.09543 (8)0.32075 (7)0.01275 (15)
C30.32593 (10)0.07436 (10)0.43020 (7)0.01852 (17)
H30.4041 (13)0.1445 (13)0.4340 (11)0.022*
C20.26616 (11)0.04998 (10)0.53101 (8)0.02156 (18)
H20.3003 (13)0.0659 (14)0.6067 (11)0.026*
C10.15619 (10)0.15322 (9)0.52292 (7)0.01729 (16)
C60.10717 (9)0.13356 (9)0.41448 (7)0.01653 (16)
H60.0270 (13)0.2037 (13)0.4082 (10)0.020*
C50.16986 (9)0.00971 (9)0.31390 (7)0.01507 (16)
H50.1354 (12)0.0026 (12)0.2382 (10)0.018*
N10.10055 (10)0.27766 (9)0.63098 (7)0.02580 (18)
N20.00167 (9)0.36899 (9)0.62448 (7)0.02437 (18)
N30.08790 (10)0.46096 (10)0.63058 (9)0.0354 (2)
O10.32736 (7)0.22575 (7)0.10966 (5)0.01705 (13)
O20.42010 (7)0.33600 (7)0.22984 (6)0.01876 (14)
C80.44971 (8)0.29984 (8)0.18519 (7)0.01120 (14)
H80.4349 (12)0.1877 (12)0.1484 (10)0.013*
C90.29221 (9)0.35908 (9)0.18393 (7)0.01391 (15)
H910.2323 (12)0.3301 (12)0.0999 (10)0.017*
H920.3026 (12)0.4755 (12)0.2132 (10)0.017*
C100.20808 (9)0.29855 (9)0.26378 (7)0.01592 (16)
H1010.1039 (13)0.3382 (13)0.2618 (10)0.019*
H1020.1903 (13)0.1838 (13)0.2295 (10)0.019*
C110.30000 (10)0.34268 (10)0.39316 (7)0.01749 (16)
H1110.2448 (13)0.3015 (13)0.4441 (11)0.021*
H1120.3116 (13)0.4565 (13)0.4299 (11)0.021*
C120.45846 (9)0.28592 (10)0.39391 (7)0.01726 (16)
H1210.4480 (12)0.1717 (13)0.3650 (10)0.021*
H1220.5167 (13)0.3181 (13)0.4755 (11)0.021*
C130.54395 (9)0.34401 (9)0.31363 (7)0.01437 (15)
H1310.5652 (12)0.4570 (13)0.3473 (10)0.017*
H1320.6433 (12)0.3005 (12)0.3144 (10)0.017*
C140.67994 (8)0.30815 (8)0.08581 (7)0.01092 (14)
H140.7508 (12)0.3448 (12)0.1652 (10)0.013*
C150.67317 (8)0.13498 (8)0.03705 (7)0.01300 (15)
H1510.5903 (12)0.0958 (12)0.0378 (10)0.016*
H1520.6472 (12)0.0881 (12)0.0954 (10)0.016*
C160.82612 (9)0.08478 (9)0.00644 (7)0.01521 (16)
H1610.90510.11570.08120.018*
H1620.81880.02720.02770.018*
C170.87218 (10)0.15505 (10)0.08433 (8)0.01899 (17)
H1710.9702 (13)0.1202 (13)0.1059 (11)0.023*
H1720.7954 (14)0.1184 (13)0.1600 (11)0.023*
C180.88202 (9)0.32790 (10)0.03397 (8)0.01720 (16)
H1810.9058 (13)0.3722 (13)0.0929 (11)0.021*
H1820.9633 (13)0.3644 (13)0.0399 (11)0.021*
C190.73172 (9)0.38297 (9)0.00087 (7)0.01373 (15)
H1910.6521 (12)0.3556 (12)0.0753 (10)0.016*
H1920.7395 (12)0.4920 (13)0.0339 (10)0.016*
N40.52640 (7)0.36044 (7)0.10448 (6)0.01064 (13)
H010.4593 (14)0.3316 (14)0.0283 (12)0.025 (3)*
H020.5355 (14)0.4614 (14)0.1341 (11)0.026 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C70.0140 (3)0.0112 (3)0.0129 (3)0.0016 (3)0.0004 (3)0.0023 (3)
C40.0152 (3)0.0107 (3)0.0111 (3)0.0007 (3)0.0006 (3)0.0028 (3)
C30.0242 (4)0.0171 (4)0.0136 (4)0.0048 (3)0.0036 (3)0.0046 (3)
C20.0297 (5)0.0212 (4)0.0119 (4)0.0040 (3)0.0060 (3)0.0020 (3)
C10.0201 (4)0.0150 (4)0.0121 (3)0.0006 (3)0.0002 (3)0.0004 (3)
C60.0163 (4)0.0149 (4)0.0159 (4)0.0025 (3)0.0029 (3)0.0018 (3)
C50.0158 (3)0.0151 (4)0.0128 (3)0.0004 (3)0.0034 (3)0.0021 (3)
N10.0304 (4)0.0228 (4)0.0158 (3)0.0068 (3)0.0036 (3)0.0044 (3)
N20.0207 (4)0.0212 (4)0.0199 (4)0.0004 (3)0.0010 (3)0.0076 (3)
N30.0269 (4)0.0282 (4)0.0355 (5)0.0097 (3)0.0072 (4)0.0116 (4)
O10.0199 (3)0.0176 (3)0.0108 (3)0.0017 (2)0.0011 (2)0.0019 (2)
O20.0246 (3)0.0116 (3)0.0180 (3)0.0034 (2)0.0028 (2)0.0029 (2)
C80.0121 (3)0.0111 (3)0.0109 (3)0.0001 (2)0.0034 (2)0.0035 (3)
C90.0121 (3)0.0168 (4)0.0133 (3)0.0021 (3)0.0032 (3)0.0051 (3)
C100.0134 (3)0.0189 (4)0.0151 (4)0.0001 (3)0.0053 (3)0.0035 (3)
C110.0189 (4)0.0205 (4)0.0134 (4)0.0012 (3)0.0062 (3)0.0045 (3)
C120.0176 (4)0.0215 (4)0.0142 (4)0.0012 (3)0.0027 (3)0.0085 (3)
C130.0134 (3)0.0180 (4)0.0121 (3)0.0015 (3)0.0012 (3)0.0063 (3)
C140.0100 (3)0.0109 (3)0.0116 (3)0.0008 (2)0.0027 (2)0.0029 (3)
C150.0129 (3)0.0106 (3)0.0153 (3)0.0007 (3)0.0027 (3)0.0039 (3)
C160.0159 (3)0.0133 (3)0.0177 (4)0.0041 (3)0.0060 (3)0.0049 (3)
C170.0217 (4)0.0197 (4)0.0194 (4)0.0079 (3)0.0109 (3)0.0074 (3)
C180.0153 (4)0.0191 (4)0.0213 (4)0.0025 (3)0.0080 (3)0.0098 (3)
C190.0142 (3)0.0127 (3)0.0162 (3)0.0015 (3)0.0051 (3)0.0061 (3)
N40.0112 (3)0.0103 (3)0.0104 (3)0.0007 (2)0.0027 (2)0.0030 (2)
Geometric parameters (Å, º) top
C7—O21.2635 (9)C11—H1111.000 (12)
C7—O11.2652 (10)C11—H1121.008 (12)
C7—C41.5179 (11)C12—C131.5341 (11)
C4—C51.3973 (11)C12—H1211.007 (11)
C4—C31.3983 (11)C12—H1220.966 (12)
C3—C21.3931 (12)C13—H1311.002 (11)
C3—H30.962 (11)C13—H1320.992 (11)
C2—C11.3961 (12)C14—N41.5095 (9)
C2—H20.973 (12)C14—C151.5301 (10)
C1—C61.3979 (12)C14—C191.5358 (10)
C1—N11.4349 (11)C14—H140.992 (11)
C6—C51.3948 (11)C15—C161.5360 (10)
C6—H60.987 (11)C15—H1511.012 (11)
C5—H50.979 (11)C15—H1520.982 (11)
N1—N21.2420 (11)C16—C171.5307 (11)
N2—N31.1352 (12)C16—H1610.9900
C8—N41.5048 (9)C16—H1620.9900
C8—C131.5305 (11)C17—C181.5270 (12)
C8—C91.5347 (10)C17—H1710.998 (12)
C8—H80.993 (11)C17—H1720.987 (12)
C9—C101.5349 (11)C18—C191.5348 (11)
C9—H910.996 (11)C18—H1810.966 (12)
C9—H921.026 (11)C18—H1820.995 (12)
C10—C111.5322 (11)C19—H1910.991 (11)
C10—H1011.016 (11)C19—H1920.966 (11)
C10—H1021.015 (11)N4—H010.949 (13)
C11—C121.5343 (12)N4—H020.892 (13)
O2—C7—O1125.91 (7)C13—C12—H122109.4 (7)
O2—C7—C4117.00 (7)H121—C12—H122107.1 (9)
O1—C7—C4117.09 (7)C8—C13—C12109.97 (6)
C5—C4—C3119.00 (7)C8—C13—H131109.8 (6)
C5—C4—C7120.91 (7)C12—C13—H131110.1 (6)
C3—C4—C7120.09 (7)C8—C13—H132111.1 (6)
C2—C3—C4120.82 (8)C12—C13—H132108.8 (6)
C2—C3—H3120.2 (7)H131—C13—H132107.1 (9)
C4—C3—H3118.9 (7)N4—C14—C15111.21 (6)
C3—C2—C1119.44 (8)N4—C14—C19107.16 (6)
C3—C2—H2120.9 (7)C15—C14—C19111.95 (6)
C1—C2—H2119.7 (7)N4—C14—H14107.7 (6)
C2—C1—C6120.56 (7)C15—C14—H14109.2 (6)
C2—C1—N1115.78 (8)C19—C14—H14109.5 (6)
C6—C1—N1123.66 (8)C14—C15—C16110.36 (6)
C5—C6—C1119.26 (7)C14—C15—H151109.6 (6)
C5—C6—H6119.3 (7)C16—C15—H151109.7 (6)
C1—C6—H6121.5 (7)C14—C15—H152111.5 (6)
C6—C5—C4120.91 (7)C16—C15—H152109.1 (6)
C6—C5—H5118.7 (6)H151—C15—H152106.4 (9)
C4—C5—H5120.4 (6)C17—C16—C15111.27 (6)
N2—N1—C1115.97 (8)C17—C16—H161109.4
N3—N2—N1172.81 (9)C15—C16—H161109.4
N4—C8—C13111.79 (6)C17—C16—H162109.4
N4—C8—C9108.21 (6)C15—C16—H162109.4
C13—C8—C9111.42 (6)H161—C16—H162108.0
N4—C8—H8107.0 (6)C18—C17—C16110.20 (7)
C13—C8—H8110.6 (6)C18—C17—H171110.8 (7)
C9—C8—H8107.6 (6)C16—C17—H171111.3 (7)
C8—C9—C10110.30 (6)C18—C17—H172110.1 (7)
C8—C9—H91110.6 (6)C16—C17—H172108.4 (7)
C10—C9—H91110.7 (6)H171—C17—H172106.0 (9)
C8—C9—H92109.9 (6)C17—C18—C19111.29 (6)
C10—C9—H92110.5 (6)C17—C18—H181110.2 (7)
H91—C9—H92104.7 (8)C19—C18—H181108.4 (7)
C11—C10—C9110.87 (6)C17—C18—H182109.7 (7)
C11—C10—H101111.3 (7)C19—C18—H182108.5 (7)
C9—C10—H101109.5 (6)H181—C18—H182108.7 (9)
C11—C10—H102109.1 (6)C18—C19—C14111.59 (6)
C9—C10—H102109.6 (6)C18—C19—H191109.0 (6)
H101—C10—H102106.4 (9)C14—C19—H191107.8 (6)
C10—C11—C12110.47 (7)C18—C19—H192111.1 (7)
C10—C11—H111110.2 (7)C14—C19—H192110.1 (7)
C12—C11—H111111.0 (7)H191—C19—H192107.0 (9)
C10—C11—H112109.5 (7)C8—N4—C14117.35 (6)
C12—C11—H112108.6 (6)C8—N4—H01106.3 (7)
H111—C11—H112107.0 (9)C14—N4—H01108.4 (7)
C11—C12—C13112.03 (7)C8—N4—H02108.0 (8)
C11—C12—H121108.9 (6)C14—N4—H02108.4 (8)
C13—C12—H121109.6 (7)H01—N4—H02108.0 (11)
C11—C12—H122109.7 (7)
O2—C7—C4—C5165.63 (7)C8—C9—C10—C1157.14 (9)
O1—C7—C4—C515.02 (11)C9—C10—C11—C1256.24 (9)
O2—C7—C4—C314.85 (11)C10—C11—C12—C1355.91 (9)
O1—C7—C4—C3164.50 (7)N4—C8—C13—C12177.54 (6)
C5—C4—C3—C20.53 (13)C9—C8—C13—C1256.33 (8)
C7—C4—C3—C2179.00 (8)C11—C12—C13—C855.67 (9)
C4—C3—C2—C11.11 (14)N4—C14—C15—C16174.20 (6)
C3—C2—C1—C60.70 (14)C19—C14—C15—C1654.36 (8)
C3—C2—C1—N1179.85 (8)C14—C15—C16—C1756.99 (8)
C2—C1—C6—C50.27 (13)C15—C16—C17—C1858.26 (9)
N1—C1—C6—C5179.13 (8)C16—C17—C18—C1956.65 (9)
C1—C6—C5—C40.86 (13)C17—C18—C19—C1454.45 (9)
C3—C4—C5—C60.46 (12)N4—C14—C19—C18175.65 (6)
C7—C4—C5—C6179.99 (7)C15—C14—C19—C1853.46 (8)
C2—C1—N1—N2179.36 (9)C13—C8—N4—C1460.74 (8)
C6—C1—N1—N21.21 (14)C9—C8—N4—C14176.20 (6)
C1—N1—N2—N3176.4 (8)C15—C14—N4—C856.33 (8)
N4—C8—C9—C10179.22 (6)C19—C14—N4—C8178.98 (6)
C13—C8—C9—C1057.50 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H01···O10.949 (13)1.817 (13)2.7409 (9)163.9 (11)
N4—H02···O2i0.892 (13)1.865 (13)2.7384 (9)166.0 (12)
Symmetry code: (i) x+1, y+1, z.
 

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