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A new photoactive monoclinic polymorph (γ-form) of 6-(2′,4′-dinitrobenzyl)-2,2′-bipyridine was obtained from an acetone–methanol solution. The crystal structure was compared with those of two polymorphs reported previously (photoactive orthorhombic α-form and photoinactive monoclinic β-form) and with structures of related nitrobenzylpyridines to explain the relation between the structure and photochromism. The comparison of the reaction cavities around the reactive pyridyl–benzyl–nitro fragment among the polymorphs and related nitrobenzylpyridines revealed that a crucial factor for photochromic activity is the rotational freedom of the ortho-nitro group in their crystals and its accessibility from the proton–donor and proton–acceptor sites. This is because the ortho-nitro group should rotate around the N—C bond to transfer a proton from the methylene group to the N atom of the pyridine ring.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768104005506/og0001sup1.cif
Contains datablocks alpha, gamma, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104005506/og0001alphasup2.hkl
Contains datablock alpha

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104005506/og0001gammasup3.hkl
Contains datablock gamma

CCDC references: 241471; 241472

Computing details top

For both compounds, data collection: SMART (Siemens, 1995); cell refinement: SMART (Siemens, 1995); data reduction: SAINT (Siemens, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-II (Johnson, 1976); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
(alpha) alpha form of 6-(2',4'-dinitrobenzyl)-2,2'-bipyridine top
Crystal data top
C17H12N4O4F(000) = 1392
Mr = 336.31Dx = 1.478 Mg m3
Orthorhombic, Pna21Mo Kα radiation, λ = 0.71073 Å
a = 14.0059 (1) ŵ = 0.11 mm1
b = 5.1399 (1) ÅT = 78 K
c = 41.9853 (6) ÅBlock, colorless
V = 3022.48 (8) Å30.35 × 0.10 × 0.05 mm
Z = 8
Data collection top
Siemens CCD
diffractometer
6678 independent reflections
Radiation source: fine-focus sealed tube4589 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.080
ω–scanθmax = 27.5°, θmin = 1.9°
Absorption correction: empirical
SADABS (Sheldrick, 1996)
h = 1518
Tmin = 0.674, Tmax = 1.000k = 66
19857 measured reflectionsl = 4754
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.064 w = 1/[σ2(Fo2) + (0.1P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.179(Δ/σ)max = 0.026
S = 1.03Δρmax = 1.13 e Å3
6678 reflectionsΔρmin = 0.27 e Å3
452 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
1 restraintExtinction coefficient: 0.0104 (11)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 1.0 (19)
Crystal data top
C17H12N4O4V = 3022.48 (8) Å3
Mr = 336.31Z = 8
Orthorhombic, Pna21Mo Kα radiation
a = 14.0059 (1) ŵ = 0.11 mm1
b = 5.1399 (1) ÅT = 78 K
c = 41.9853 (6) Å0.35 × 0.10 × 0.05 mm
Data collection top
Siemens CCD
diffractometer
6678 independent reflections
Absorption correction: empirical
SADABS (Sheldrick, 1996)
4589 reflections with I > 2σ(I)
Tmin = 0.674, Tmax = 1.000Rint = 0.080
19857 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.064H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.179Δρmax = 1.13 e Å3
S = 1.03Δρmin = 0.27 e Å3
6678 reflectionsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
452 parametersAbsolute structure parameter: 1.0 (19)
1 restraint
Special details top

Experimental. alpha form of 6-(2',4'-dinitrobenzyl)-2,2'-bipyridine

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
O10.3904 (3)0.4697 (7)0.76327 (8)0.0286 (8)
O20.4525 (2)0.0817 (7)0.75954 (9)0.0335 (9)
O30.3690 (3)0.5085 (7)0.84278 (9)0.0370 (9)
O40.2391 (3)0.4489 (8)0.87018 (8)0.0400 (10)
O50.3681 (2)0.9674 (7)0.96382 (8)0.0257 (7)
O60.3048 (2)0.5852 (7)0.96808 (9)0.0316 (9)
O70.3880 (3)0.0107 (7)0.88457 (8)0.0313 (9)
O80.5188 (3)0.0523 (7)0.85709 (9)0.0386 (9)
N10.2448 (3)0.1759 (9)0.71644 (9)0.0175 (8)
N20.3891 (4)0.2329 (8)0.76866 (15)0.0235 (13)
N30.2933 (3)0.3954 (8)0.84807 (10)0.0289 (10)
N40.3339 (3)0.0839 (7)0.64269 (9)0.0218 (8)
N50.5117 (3)0.6786 (9)1.01057 (9)0.0179 (8)
N60.3683 (4)0.7339 (8)0.95974 (13)0.0182 (12)
N70.4645 (3)0.1024 (7)0.87945 (10)0.0262 (9)
N80.4164 (3)0.4221 (7)1.08432 (9)0.0205 (8)
C10.2465 (3)0.1251 (8)0.68501 (10)0.0169 (9)
C20.1879 (4)0.2471 (8)0.66291 (16)0.0159 (15)
H20.19190.20810.64080.019*
C30.1224 (3)0.4303 (8)0.67458 (11)0.0204 (9)
H30.07950.51470.66040.025*
C40.1206 (3)0.4877 (8)0.70673 (11)0.0201 (9)
H40.07750.61440.71480.024*
C50.1821 (3)0.3584 (9)0.72688 (10)0.0177 (9)
C60.1849 (3)0.4290 (9)0.76193 (11)0.0225 (10)
H6A0.12020.48690.76830.027*
H6B0.22840.57920.76460.027*
C70.2166 (4)0.2147 (10)0.78485 (14)0.0189 (12)
C80.3100 (3)0.1193 (8)0.78638 (10)0.0161 (9)
C90.3353 (3)0.0801 (8)0.80682 (11)0.0207 (9)
H90.39910.14230.80760.025*
C100.2661 (4)0.1861 (11)0.82598 (12)0.0234 (10)
C110.1725 (4)0.1019 (10)0.82508 (11)0.0266 (11)
H110.12540.17730.83850.032*
C120.1491 (3)0.0973 (9)0.80387 (11)0.0248 (10)
H120.08460.15370.80250.030*
C130.3176 (3)0.0769 (8)0.67411 (10)0.0168 (9)
C140.3624 (4)0.2407 (8)0.69483 (15)0.0165 (15)
H140.34950.22630.71700.020*
C150.4258 (3)0.4260 (9)0.68438 (11)0.0195 (9)
H150.45620.54130.69890.023*
C160.4436 (3)0.4385 (9)0.65218 (11)0.0193 (9)
H160.48610.56450.64370.023*
C170.3977 (4)0.2628 (9)0.63272 (16)0.0197 (15)
H170.41220.26790.61060.024*
C180.5055 (3)0.6290 (8)1.04231 (10)0.0158 (9)
C190.5641 (5)0.7588 (9)1.06391 (18)0.0238 (17)
H190.55960.72011.08600.029*
C200.6286 (3)0.9427 (9)1.05353 (11)0.0228 (10)
H200.66851.03211.06820.027*
C210.6338 (3)0.9946 (9)1.02094 (10)0.0191 (9)
H210.67761.11901.01280.023*
C220.5722 (3)0.8570 (8)1.00065 (10)0.0168 (9)
C230.5727 (3)0.9305 (9)0.96536 (10)0.0199 (9)
H23A0.52991.08160.96220.024*
H23B0.63800.98490.95930.024*
C240.5419 (4)0.7169 (10)0.94392 (15)0.0182 (12)
C250.4484 (3)0.6180 (9)0.94088 (10)0.0180 (9)
C260.4212 (3)0.4185 (9)0.92063 (10)0.0196 (9)
H260.35730.35660.92000.023*
C270.4917 (4)0.3127 (11)0.90115 (11)0.0204 (10)
C280.5863 (4)0.3984 (10)0.90207 (11)0.0259 (10)
H280.63330.32590.88840.031*
C290.6093 (3)0.5941 (9)0.92376 (10)0.0216 (10)
H290.67400.64820.92510.026*
C300.4359 (3)0.4318 (8)1.05291 (9)0.0145 (9)
C310.3939 (4)0.2593 (8)1.02999 (17)0.0200 (15)
H310.40840.27091.00790.024*
C320.3298 (3)0.0713 (9)1.04196 (11)0.0214 (10)
H320.30010.04921.02790.026*
C330.3101 (3)0.0636 (9)1.07481 (12)0.0224 (10)
H330.26700.06121.08320.027*
C340.3552 (4)0.2427 (9)1.09487 (18)0.0233 (17)
H340.34170.23631.11700.028*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.036 (2)0.0223 (19)0.0270 (18)0.0014 (16)0.0015 (15)0.0025 (15)
O20.0202 (18)0.037 (2)0.043 (2)0.0075 (15)0.0023 (16)0.0013 (17)
O30.057 (3)0.025 (2)0.0285 (19)0.0065 (19)0.0099 (18)0.0057 (15)
O40.047 (2)0.045 (2)0.028 (2)0.0183 (19)0.0095 (17)0.0155 (17)
O50.0271 (18)0.0256 (19)0.0242 (18)0.0038 (15)0.0016 (14)0.0019 (14)
O60.0203 (18)0.037 (2)0.038 (2)0.0060 (16)0.0059 (16)0.0030 (17)
O70.050 (2)0.0214 (19)0.0228 (18)0.0073 (17)0.0091 (16)0.0000 (14)
O80.045 (2)0.040 (2)0.031 (2)0.0119 (18)0.0044 (17)0.0118 (18)
N10.0139 (19)0.0194 (18)0.019 (2)0.0037 (18)0.0001 (15)0.0020 (19)
N20.020 (2)0.026 (3)0.025 (3)0.0025 (16)0.000 (2)0.0022 (16)
N30.035 (2)0.026 (2)0.025 (2)0.004 (2)0.008 (2)0.0003 (18)
N40.021 (2)0.024 (2)0.020 (2)0.0008 (17)0.0016 (16)0.0018 (16)
N50.020 (2)0.0154 (18)0.018 (2)0.0031 (18)0.0033 (16)0.0012 (19)
N60.019 (2)0.023 (3)0.013 (2)0.0026 (15)0.0063 (19)0.0050 (14)
N70.040 (3)0.019 (2)0.020 (2)0.0074 (19)0.0108 (19)0.0002 (17)
N80.0188 (19)0.020 (2)0.023 (2)0.0033 (16)0.0033 (16)0.0013 (15)
C10.012 (2)0.017 (2)0.021 (2)0.0008 (17)0.0024 (16)0.0012 (17)
C20.020 (3)0.019 (4)0.009 (3)0.0025 (16)0.001 (2)0.0014 (14)
C30.018 (2)0.024 (2)0.019 (2)0.0010 (19)0.0046 (18)0.0055 (18)
C40.018 (2)0.019 (2)0.024 (2)0.0014 (18)0.0000 (18)0.0004 (18)
C50.016 (2)0.022 (3)0.016 (2)0.0023 (19)0.0026 (17)0.0025 (18)
C60.019 (2)0.020 (2)0.028 (3)0.0042 (18)0.0029 (19)0.0001 (19)
C70.024 (3)0.024 (2)0.008 (2)0.007 (2)0.0089 (19)0.0012 (19)
C80.013 (2)0.018 (2)0.017 (2)0.0003 (17)0.0005 (16)0.0047 (17)
C90.021 (2)0.014 (2)0.027 (2)0.0019 (19)0.0050 (19)0.0026 (18)
C100.033 (3)0.019 (2)0.018 (3)0.006 (2)0.009 (2)0.003 (2)
C110.024 (2)0.033 (3)0.023 (3)0.013 (2)0.0003 (19)0.0021 (19)
C120.019 (2)0.037 (3)0.019 (2)0.002 (2)0.0008 (18)0.005 (2)
C130.013 (2)0.017 (2)0.020 (2)0.0008 (17)0.0009 (17)0.0028 (17)
C140.015 (3)0.022 (4)0.013 (3)0.0030 (16)0.001 (2)0.0031 (15)
C150.020 (2)0.015 (2)0.023 (2)0.0030 (19)0.0049 (18)0.0042 (17)
C160.017 (2)0.016 (2)0.024 (2)0.0013 (17)0.0029 (18)0.0067 (18)
C170.021 (3)0.027 (4)0.012 (3)0.0040 (18)0.007 (2)0.0020 (16)
C180.0127 (19)0.019 (2)0.016 (2)0.0043 (17)0.0023 (16)0.0012 (17)
C190.024 (3)0.028 (5)0.020 (4)0.0004 (19)0.003 (3)0.0018 (18)
C200.018 (2)0.026 (2)0.025 (2)0.002 (2)0.0066 (19)0.0011 (19)
C210.012 (2)0.022 (2)0.023 (2)0.0043 (17)0.0002 (17)0.0015 (18)
C220.010 (2)0.018 (2)0.022 (2)0.0029 (17)0.0028 (17)0.0036 (18)
C230.021 (2)0.025 (2)0.013 (2)0.0080 (19)0.0000 (17)0.0031 (18)
C240.012 (2)0.025 (3)0.018 (3)0.0011 (19)0.0013 (19)0.012 (2)
C250.018 (2)0.022 (2)0.015 (2)0.0000 (18)0.0016 (17)0.0011 (17)
C260.021 (2)0.022 (2)0.016 (2)0.0034 (19)0.0056 (18)0.0046 (18)
C270.031 (3)0.015 (2)0.015 (2)0.003 (2)0.003 (2)0.000 (2)
C280.029 (3)0.028 (3)0.021 (3)0.003 (2)0.001 (2)0.0004 (18)
C290.018 (2)0.030 (3)0.017 (2)0.002 (2)0.0009 (17)0.0018 (19)
C300.017 (2)0.017 (2)0.010 (2)0.0059 (17)0.0036 (16)0.0028 (16)
C310.021 (3)0.017 (4)0.022 (3)0.0039 (17)0.000 (2)0.0015 (16)
C320.018 (2)0.021 (2)0.026 (2)0.0015 (19)0.0028 (19)0.0002 (19)
C330.021 (2)0.018 (2)0.028 (2)0.0011 (19)0.0030 (19)0.0067 (19)
C340.020 (3)0.026 (4)0.025 (4)0.0069 (18)0.007 (3)0.0032 (17)
Geometric parameters (Å, º) top
O1—N21.238 (5)C9—H90.9500
O1—C62.887 (6)C10—C111.382 (7)
O1—N13.210 (5)C11—C121.396 (7)
O2—N21.241 (6)C11—H110.9500
O3—N31.230 (5)C12—H120.9500
O4—N31.230 (6)C13—C141.364 (7)
O5—N61.212 (5)C14—C151.374 (7)
O5—C232.873 (6)C14—H140.9500
O5—N53.178 (5)C15—C161.376 (7)
O6—N61.224 (6)C15—H150.9500
O7—N71.238 (5)C16—C171.377 (8)
O8—N71.235 (6)C16—H160.9500
N1—C11.345 (6)C17—H170.9500
N1—C51.358 (6)C18—C191.393 (8)
N1—C62.459 (6)C18—C301.475 (6)
N2—C81.456 (7)C19—C201.378 (8)
N3—C101.470 (7)C19—H190.9500
N4—C131.340 (6)C20—C211.396 (7)
N4—C171.349 (6)C20—H200.9500
N5—C221.316 (6)C21—C221.403 (6)
N5—C181.360 (6)C21—H210.9500
N5—C232.451 (6)C22—C231.529 (6)
N6—C251.496 (7)C23—C241.484 (7)
N7—C271.464 (7)C23—H23A0.9900
N8—C341.334 (7)C23—H23B0.9900
N8—C301.348 (5)C24—C251.411 (7)
C1—C21.389 (7)C24—C291.417 (7)
C1—C131.509 (6)C25—C261.386 (6)
C2—C31.403 (7)C26—C271.393 (7)
C2—H20.9500C26—H260.9500
C3—C41.382 (6)C27—C281.396 (7)
C3—H30.9500C28—C291.395 (7)
C4—C51.378 (6)C28—H280.9500
C4—H40.9500C29—H290.9500
C5—C61.516 (6)C30—C311.435 (7)
C6—C71.529 (7)C31—C321.411 (7)
C6—H6A0.9900C31—H310.9500
C6—H6B0.9900C32—C331.407 (7)
C7—C121.377 (8)C32—H320.9500
C7—C81.399 (7)C33—C341.398 (8)
C8—C91.383 (6)C33—H330.9500
C9—C101.372 (7)C34—H340.9500
N2—O1—C685.3 (3)C11—C12—H12119.0
N2—O1—N168.9 (3)N4—C13—C14122.2 (4)
C6—O1—N147.20 (12)N4—C13—C1115.5 (4)
N6—O5—C2386.3 (3)C14—C13—C1122.4 (4)
N6—O5—N567.9 (3)C13—C14—C15121.5 (6)
C23—O5—N547.46 (12)C13—C14—H14119.3
C1—N1—C5117.5 (4)C15—C14—H14119.3
C1—N1—C6150.5 (3)C16—C15—C14117.6 (5)
C5—N1—C633.2 (2)C16—C15—H15121.2
C1—N1—O1132.9 (3)C14—C15—H15121.2
C5—N1—O183.6 (3)C15—C16—C17117.9 (4)
C6—N1—O159.49 (15)C15—C16—H16121.1
O1—N2—O2123.3 (5)C17—C16—H16121.1
O1—N2—C8119.9 (5)N4—C17—C16124.9 (6)
O2—N2—C8116.8 (4)N4—C17—H17117.6
O4—N3—O3124.2 (4)C16—C17—H17117.6
O4—N3—C10118.7 (4)N5—C18—C19120.7 (5)
O3—N3—C10117.1 (4)N5—C18—C30117.8 (4)
C13—N4—C17115.9 (4)C19—C18—C30121.5 (4)
C22—N5—C18118.8 (4)C20—C19—C18120.6 (6)
C22—N5—C2333.2 (2)C20—C19—H19119.7
C18—N5—C23151.7 (3)C18—C19—H19119.7
C22—N5—O583.5 (3)C19—C20—C21118.4 (5)
C18—N5—O5130.7 (3)C19—C20—H20120.8
C23—N5—O559.72 (15)C21—C20—H20120.8
O5—N6—O6125.1 (5)C20—C21—C22117.8 (4)
O5—N6—C25118.1 (5)C20—C21—H21121.1
O6—N6—C25116.6 (4)C22—C21—H21121.1
O8—N7—O7124.6 (4)N5—C22—C21123.7 (4)
O8—N7—C27117.8 (4)N5—C22—C23118.8 (4)
O7—N7—C27117.6 (4)C21—C22—C23117.5 (4)
C34—N8—C30118.8 (5)C24—C23—C22113.8 (4)
N1—C1—C2123.9 (4)C24—C23—N588.7 (3)
N1—C1—C13116.3 (4)C22—C23—N528.1 (2)
C2—C1—C13119.9 (4)C24—C23—O575.2 (3)
C1—C2—C3117.1 (5)C22—C23—O592.0 (3)
C1—C2—H2121.4N5—C23—O572.82 (16)
C3—C2—H2121.4C24—C23—H23A108.8
C4—C3—C2119.8 (5)C22—C23—H23A108.8
C4—C3—H3120.1N5—C23—H23A107.9
C2—C3—H3120.1O5—C23—H23A48.8
C5—C4—C3119.0 (4)C24—C23—H23B108.8
C5—C4—H4120.5C22—C23—H23B108.8
C3—C4—H4120.5N5—C23—H23B132.1
N1—C5—C4122.7 (4)O5—C23—H23B153.9
N1—C5—C6117.5 (4)H23A—C23—H23B107.7
C4—C5—C6119.7 (4)C25—C24—C29113.8 (5)
C5—C6—C7116.5 (4)C25—C24—C23126.3 (5)
C5—C6—N129.3 (2)C29—C24—C23119.9 (4)
C7—C6—N190.5 (3)C26—C25—C24125.3 (4)
C5—C6—O193.5 (3)C26—C25—N6114.4 (4)
C7—C6—O175.5 (3)C24—C25—N6120.3 (4)
N1—C6—O173.30 (16)C25—C26—C27117.0 (4)
C5—C6—H6A108.2C25—C26—H26121.5
C7—C6—H6A108.2C27—C26—H26121.5
N1—C6—H6A133.0C26—C27—C28122.2 (5)
O1—C6—H6A152.2C26—C27—N7118.0 (5)
C5—C6—H6B108.2C28—C27—N7119.8 (4)
C7—C6—H6B108.2C29—C28—C27117.7 (4)
N1—C6—H6B106.9C29—C28—H28121.2
O1—C6—H6B47.7C27—C28—H28121.2
H6A—C6—H6B107.3C28—C29—C24123.9 (5)
C12—C7—C8117.5 (5)C28—C29—H29118.1
C12—C7—C6118.8 (4)C24—C29—H29118.1
C8—C7—C6123.6 (5)N8—C30—C31123.3 (4)
C9—C8—C7121.8 (4)N8—C30—C18117.1 (4)
C9—C8—N2114.8 (4)C31—C30—C18119.6 (4)
C7—C8—N2123.2 (5)C32—C31—C30116.5 (6)
C10—C9—C8118.5 (4)C32—C31—H31121.8
C10—C9—H9120.7C30—C31—H31121.8
C8—C9—H9120.7C33—C32—C31119.5 (5)
C9—C10—C11122.0 (5)C33—C32—H32120.2
C9—C10—N3118.5 (5)C31—C32—H32120.2
C11—C10—N3119.4 (5)C34—C33—C32118.9 (5)
C10—C11—C12118.0 (5)C34—C33—H33120.5
C10—C11—H11121.0C32—C33—H33120.5
C12—C11—H11121.0N8—C34—C33123.0 (6)
C7—C12—C11122.0 (4)N8—C34—H34118.5
C7—C12—H12119.0C33—C34—H34118.5
(gamma) gamma form of 6-(2',4'-dinitrobenzyl)-2,2'-bipyridine top
Crystal data top
C17H12N4O4Z = 4
Mr = 336.31F(000) = 696
Monoclinic, P21/cDx = 1.489 Mg m3
a = 20.8360 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 5.2746 (1) ŵ = 0.11 mm1
c = 14.0971 (2) ÅT = 78 K
β = 104.457 (1)°Plate, colorless
V = 1500.23 (4) Å30.40 × 0.25 × 0.05 mm
Data collection top
Siemens CCD
diffractometer
3445 independent reflections
Radiation source: fine-focus sealed tube2934 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.048
ω–scanθmax = 27.6°, θmin = 1.0°
Absorption correction: empirical
SADABS (Sheldrick, 1996)
h = 2720
Tmin = 0.975, Tmax = 1.000k = 66
10094 measured reflectionsl = 1518
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) = 0.153H atoms treated by a mixture of independent and constrained refinement
S = 1.11 w = 1/[σ2(Fo2) + (0.1P)2]
where P = (Fo2 + 2Fc2)/3
3445 reflections(Δ/σ)max = 0.001
228 parametersΔρmax = 0.40 e Å3
0 restraintsΔρmin = 0.52 e Å3
Crystal data top
C17H12N4O4V = 1500.23 (4) Å3
Mr = 336.31Z = 4
Monoclinic, P21/cMo Kα radiation
a = 20.8360 (3) ŵ = 0.11 mm1
b = 5.2746 (1) ÅT = 78 K
c = 14.0971 (2) Å0.40 × 0.25 × 0.05 mm
β = 104.457 (1)°
Data collection top
Siemens CCD
diffractometer
3445 independent reflections
Absorption correction: empirical
SADABS (Sheldrick, 1996)
2934 reflections with I > 2σ(I)
Tmin = 0.975, Tmax = 1.000Rint = 0.048
10094 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.153H atoms treated by a mixture of independent and constrained refinement
S = 1.11Δρmax = 0.40 e Å3
3445 reflectionsΔρmin = 0.52 e Å3
228 parameters
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
O10.81007 (5)1.6028 (2)0.22845 (8)0.0218 (3)
O20.81247 (5)1.9763 (2)0.29337 (8)0.0234 (3)
O30.96491 (6)2.5705 (2)0.20348 (10)0.0318 (3)
O41.01989 (6)2.4242 (3)0.10337 (10)0.0408 (4)
N10.69744 (6)1.8705 (2)0.08211 (8)0.0146 (3)
N20.82012 (6)1.8321 (2)0.22873 (8)0.0161 (3)
N30.97264 (7)2.4211 (3)0.14122 (10)0.0254 (3)
N40.56525 (6)2.1212 (2)0.17702 (9)0.0187 (3)
C10.63491 (7)1.9080 (3)0.08969 (10)0.0143 (3)
C20.58149 (7)1.7649 (3)0.03705 (10)0.0176 (3)
H20.53781.79830.04260.021*
C30.59349 (7)1.5736 (3)0.02329 (11)0.0196 (3)
H30.55801.47240.05950.023*
C40.65760 (7)1.5307 (3)0.03051 (10)0.0178 (3)
H40.66701.39990.07140.021*
C50.70826 (7)1.6842 (3)0.02375 (10)0.0148 (3)
C60.77891 (7)1.6300 (3)0.01972 (11)0.0179 (3)
C70.82868 (7)1.8387 (3)0.05481 (10)0.0161 (3)
C80.84580 (6)1.9399 (3)0.14952 (10)0.0142 (3)
C90.89044 (7)2.1354 (3)0.17801 (10)0.0153 (3)
H90.89862.20710.24170.018*
C100.92269 (7)2.2221 (3)0.11014 (11)0.0189 (3)
C110.90986 (8)2.1284 (3)0.01600 (11)0.0255 (4)
H110.93342.18930.02900.031*
C120.86145 (7)1.9421 (3)0.01124 (11)0.0225 (3)
H120.85031.88340.07700.027*
C130.62558 (7)2.1097 (3)0.15857 (10)0.0146 (3)
C140.67691 (7)2.2751 (3)0.20159 (10)0.0165 (3)
H140.71892.26210.18690.020*
C150.66582 (7)2.4580 (3)0.26585 (11)0.0185 (3)
H150.69992.57320.29580.022*
C160.60399 (7)2.4704 (3)0.28583 (11)0.0197 (3)
H160.59492.59330.33000.024*
C170.55597 (7)2.2994 (3)0.23989 (11)0.0205 (3)
H170.51372.30900.25380.025*
H610.79351.47490.05550.028 (5)*
H620.77881.57990.04680.042 (6)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0242 (6)0.0199 (5)0.0247 (6)0.0020 (4)0.0126 (4)0.0049 (4)
O20.0306 (6)0.0296 (6)0.0143 (5)0.0049 (4)0.0138 (4)0.0018 (4)
O30.0247 (6)0.0194 (6)0.0464 (8)0.0002 (4)0.0002 (5)0.0049 (5)
O40.0328 (7)0.0639 (9)0.0285 (7)0.0261 (6)0.0128 (5)0.0033 (6)
N10.0163 (6)0.0164 (5)0.0139 (6)0.0007 (4)0.0091 (4)0.0006 (4)
N20.0158 (6)0.0220 (6)0.0130 (6)0.0018 (4)0.0086 (4)0.0021 (4)
N30.0225 (7)0.0266 (7)0.0247 (7)0.0065 (5)0.0017 (5)0.0076 (5)
N40.0175 (6)0.0199 (6)0.0229 (6)0.0010 (4)0.0129 (5)0.0003 (5)
C10.0156 (6)0.0156 (6)0.0143 (6)0.0001 (5)0.0085 (5)0.0034 (5)
C20.0157 (6)0.0210 (7)0.0180 (7)0.0020 (5)0.0081 (5)0.0027 (5)
C30.0191 (7)0.0222 (7)0.0177 (7)0.0051 (5)0.0052 (5)0.0006 (5)
C40.0221 (7)0.0180 (7)0.0152 (7)0.0028 (5)0.0083 (5)0.0011 (5)
C50.0176 (6)0.0167 (6)0.0128 (6)0.0010 (5)0.0089 (5)0.0009 (5)
C60.0188 (7)0.0201 (7)0.0183 (7)0.0015 (5)0.0110 (5)0.0063 (5)
C70.0153 (6)0.0198 (7)0.0162 (7)0.0001 (5)0.0097 (5)0.0027 (5)
C80.0158 (6)0.0178 (6)0.0124 (6)0.0024 (5)0.0100 (5)0.0023 (5)
C90.0165 (6)0.0159 (6)0.0143 (6)0.0021 (5)0.0054 (5)0.0002 (5)
C100.0167 (7)0.0201 (7)0.0202 (7)0.0035 (5)0.0052 (5)0.0026 (5)
C110.0232 (8)0.0381 (9)0.0190 (7)0.0085 (6)0.0124 (6)0.0027 (6)
C120.0220 (7)0.0354 (8)0.0139 (7)0.0057 (6)0.0117 (5)0.0042 (6)
C130.0160 (6)0.0155 (6)0.0152 (6)0.0009 (5)0.0093 (5)0.0039 (5)
C140.0173 (6)0.0181 (7)0.0171 (7)0.0001 (5)0.0100 (5)0.0027 (5)
C150.0194 (7)0.0192 (7)0.0192 (7)0.0004 (5)0.0089 (5)0.0007 (5)
C160.0245 (7)0.0196 (7)0.0188 (7)0.0038 (5)0.0125 (5)0.0003 (5)
C170.0193 (7)0.0220 (7)0.0252 (8)0.0024 (5)0.0151 (5)0.0013 (6)
Geometric parameters (Å, º) top
O1—N21.2275 (16)C6—H610.9691
O2—N21.2276 (16)C6—H620.9736
O3—N31.2197 (19)C7—C121.3956 (19)
O4—N31.231 (2)C7—C81.3989 (19)
N1—C51.3363 (17)C8—C91.3793 (19)
N1—C11.3482 (17)C9—C101.3775 (19)
N2—C81.4680 (16)C9—H90.9500
N3—C101.4660 (18)C10—C111.378 (2)
N4—C171.3386 (19)C11—C121.392 (2)
N4—C131.3471 (18)C11—H110.9500
C1—C21.3953 (19)C12—H120.9500
C1—C131.485 (2)C13—C141.3962 (19)
C2—C31.382 (2)C14—C151.3819 (19)
C2—H20.9500C14—H140.9500
C3—C41.383 (2)C15—C161.387 (2)
C3—H30.9500C15—H150.9500
C4—C51.3971 (18)C16—C171.382 (2)
C4—H40.9500C16—H160.9500
C5—C61.5145 (19)C17—H170.9500
C6—C71.5086 (19)
C5—N1—C1118.13 (12)C8—C7—C6125.59 (13)
O1—N2—O2124.01 (12)C9—C8—C7123.77 (13)
O1—N2—C8118.27 (11)C9—C8—N2114.54 (12)
O2—N2—C8117.66 (12)C7—C8—N2121.58 (12)
O3—N3—O4124.52 (14)C10—C9—C8117.15 (12)
O3—N3—C10117.78 (14)C10—C9—H9121.4
O4—N3—C10117.70 (14)C8—C9—H9121.4
C17—N4—C13117.11 (12)C9—C10—C11122.59 (13)
N1—C1—C2122.48 (13)C9—C10—N3117.60 (13)
N1—C1—C13116.34 (12)C11—C10—N3119.81 (13)
C2—C1—C13121.18 (13)C10—C11—C12118.15 (14)
C3—C2—C1118.65 (13)C10—C11—H11120.9
C3—C2—H2120.7C12—C11—H11120.9
C1—C2—H2120.7C11—C12—C7122.24 (13)
C2—C3—C4119.40 (13)C11—C12—H12118.9
C2—C3—H3120.3C7—C12—H12118.9
C4—C3—H3120.3N4—C13—C14122.57 (13)
C3—C4—C5118.45 (13)N4—C13—C1116.07 (12)
C3—C4—H4120.8C14—C13—C1121.36 (12)
C5—C4—H4120.8C15—C14—C13119.06 (13)
N1—C5—C4122.87 (13)C15—C14—H14120.5
N1—C5—C6118.47 (12)C13—C14—H14120.5
C4—C5—C6118.60 (12)C14—C15—C16118.80 (13)
C7—C6—C5116.42 (11)C14—C15—H15120.6
C7—C6—H61110.2C16—C15—H15120.6
C5—C6—H61108.7C17—C16—C15118.33 (13)
C7—C6—H62110.5C17—C16—H16120.8
C5—C6—H62108.5C15—C16—H16120.8
H61—C6—H62101.4N4—C17—C16124.12 (13)
C12—C7—C8115.90 (13)N4—C17—H17117.9
C12—C7—C6118.51 (12)C16—C17—H17117.9

Experimental details

(alpha)(gamma)
Crystal data
Chemical formulaC17H12N4O4C17H12N4O4
Mr336.31336.31
Crystal system, space groupOrthorhombic, Pna21Monoclinic, P21/c
Temperature (K)7878
a, b, c (Å)14.0059 (1), 5.1399 (1), 41.9853 (6)20.8360 (3), 5.2746 (1), 14.0971 (2)
α, β, γ (°)90, 90, 9090, 104.457 (1), 90
V3)3022.48 (8)1500.23 (4)
Z84
Radiation typeMo KαMo Kα
µ (mm1)0.110.11
Crystal size (mm)0.35 × 0.10 × 0.050.40 × 0.25 × 0.05
Data collection
DiffractometerSiemens CCD
diffractometer
Siemens CCD
diffractometer
Absorption correctionEmpirical
SADABS (Sheldrick, 1996)
Empirical
SADABS (Sheldrick, 1996)
Tmin, Tmax0.674, 1.0000.975, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
19857, 6678, 4589 10094, 3445, 2934
Rint0.0800.048
(sin θ/λ)max1)0.6490.652
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.064, 0.179, 1.03 0.049, 0.153, 1.11
No. of reflections66783445
No. of parameters452228
No. of restraints10
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)1.13, 0.270.40, 0.52
Absolute structureFlack H D (1983), Acta Cryst. A39, 876-881?
Absolute structure parameter1.0 (19)?

Computer programs: SMART (Siemens, 1995), SAINT (Siemens, 1995), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEP-II (Johnson, 1976).

 

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