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In the two title compounds, N-methyl­carba­zole-3,5-di­nitro­benzo­nitrile (1/1), C13H11N·C7H3N3O4, (I), and N-ethyl­carba­zole-3,5-di­nitro­benzo­nitrile (1/1), C14H13N·C7H3N3O4, (II), the donor and acceptor mol­ecules are stacked alternately to form one-dimensional columns. In (I), the N-methyl group of the donor is nearly eclipsed with respect to one of the nitro groups of the neighboring acceptor in a column, whereas the N-ethyl group is anti with respect to the cyano group of the neighboring acceptor in (II).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100003851/qa0230sup1.cif
Contains datablocks dncb, I, II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100003851/qa0230Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100003851/qa0230IIsup3.hkl
Contains datablock II

CCDC references: 144705; 144706

Comment top

Crystals of (I) underwent photoredox reactions initiated by the excited nitro group, leading to α-oxidation of the N-alkyl groups. However, no photoreaction was observed for (II) (Ito et al., 1998).

In (I), the N-methyl group of the donor is nearly eclipsed with respect to one of the nitro groups of the neighboring acceptor in a column, whereas the N-ethyl group is anti with respect to the cyano group of the neighboring acceptor in (II).

Experimental top

Equimolecular mixtures of N-alkylcarbazoles and 3,5-dinitrobenzonitrile were recrystallized from methylene chloride [for (I)] and ethyl acetate [for (II)].

Refinement top

All H-atom positional parameters were calculated geometrically and fixed with Uiso(H) = 1.2Ueq(parent atom).

Computing details top

For both compounds, data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation, 1999); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); software used to prepare material for publication: TEXSAN.

(I) top
Crystal data top
C13H11N·C7H3N3O4Dx = 1.382 Mg m3
Mr = 374.35Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 25 reflections
a = 8.339 (2) Åθ = 10.0–15.0°
b = 27.604 (4) ŵ = 0.10 mm1
c = 7.817 (2) ÅT = 293 K
V = 1799.4 (7) Å3Prism, red
Z = 40.55 × 0.3 × 0.2 mm
Data collection top
Rigaku AFC5
diffractometer
h = 010
ω scansk = 035
2384 measured reflectionsl = 010
2384 independent reflections3 standard reflections every 100 reflections
1034 reflections with I > 2σ(I) intensity decay: 1.1%
θmax = 27.5°, θmin = 2.0°
Refinement top
Refinement on F2H-atom parameters not refined
R[F2 > 2σ(F2)] = 0.063 w = 1/[σ2(Fo2) + (0.0604P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.162(Δ/σ)max = 0.001
S = 1.00Δρmax = 0.21 e Å3
2384 reflectionsΔρmin = 0.16 e Å3
253 parameters
Crystal data top
C13H11N·C7H3N3O4V = 1799.4 (7) Å3
Mr = 374.35Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 8.339 (2) ŵ = 0.10 mm1
b = 27.604 (4) ÅT = 293 K
c = 7.817 (2) Å0.55 × 0.3 × 0.2 mm
Data collection top
Rigaku AFC5
diffractometer
1034 reflections with I > 2σ(I)
2384 measured reflections3 standard reflections every 100 reflections
2384 independent reflections intensity decay: 1.1%
Refinement top
R[F2 > 2σ(F2)] = 0.063253 parameters
wR(F2) = 0.162H-atom parameters not refined
S = 1.00Δρmax = 0.21 e Å3
2384 reflectionsΔρmin = 0.16 e Å3
Special details top

Refinement. Refinement was based on F2 against all reflections. The weighted R-factor (wR) and goodness of fit (S) were based on F2, and conventional R-factor (R) was calculated on F, with F set to zero for negative F2. The threshold expression of I > 2σ(I) was used only for calculating R-factor(gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.0700 (7)0.3442 (2)1.0078 (7)0.125 (2)
O20.1186 (7)0.3062 (2)0.8773 (8)0.121 (2)
O30.2399 (6)0.3501 (2)0.2930 (6)0.100 (2)
O40.1621 (7)0.4184 (2)0.1971 (6)0.114 (2)
N50.0202 (8)0.3382 (2)0.8871 (8)0.085 (2)
N60.1671 (7)0.3876 (2)0.3075 (7)0.071 (1)
N70.2374 (8)0.5283 (2)0.6566 (9)0.113 (2)
N80.4414 (6)0.3313 (2)0.8117 (6)0.065 (1)
C90.1754 (7)0.4932 (2)0.6482 (9)0.074 (2)
C100.0869 (7)0.4477 (2)0.6324 (8)0.059 (2)
C110.0796 (7)0.4155 (2)0.7695 (6)0.066 (2)
C120.0086 (7)0.3742 (2)0.7454 (8)0.061 (2)
C130.0914 (6)0.3628 (2)0.5968 (8)0.059 (2)
C140.0796 (7)0.3966 (2)0.4685 (7)0.056 (1)
C150.0078 (7)0.4392 (2)0.4776 (6)0.056 (1)
C160.5011 (7)0.3748 (2)0.7579 (9)0.063 (2)
C170.5956 (8)0.4083 (3)0.8453 (6)0.092 (2)
C180.6378 (8)0.4503 (3)0.760 (1)0.113 (3)
C190.5899 (9)0.4592 (2)0.595 (1)0.096 (3)
C200.4951 (7)0.4265 (2)0.5055 (6)0.077 (2)
C210.4517 (6)0.3836 (2)0.5885 (8)0.054 (1)
C220.3520 (7)0.3429 (2)0.5402 (7)0.056 (1)
C230.2661 (8)0.3322 (2)0.3944 (6)0.069 (2)
C240.1792 (7)0.2896 (3)0.3903 (8)0.081 (2)
C250.1767 (7)0.2585 (2)0.530 (1)0.085 (2)
C260.2608 (8)0.2688 (2)0.6794 (7)0.069 (2)
C270.3481 (7)0.3117 (2)0.6822 (8)0.056 (1)
C280.4730 (5)0.3082 (2)0.9785 (6)0.100 (2)
H110.13510.42260.87580.0789*
H130.15360.33350.58400.0688*
H150.01020.46190.38190.0658*
H170.62700.40230.96240.1090*
H180.70250.47340.82220.1281*
H190.62470.48920.54390.1203*
H200.45820.43360.38930.0942*
H230.27300.35280.29480.0828*
H240.11170.28060.29480.0934*
H250.12060.22790.52290.0971*
H260.25540.24600.77200.0857*
H28A0.43630.32861.07140.1166*
H28B0.41850.27720.98780.1166*
H28C0.58680.30240.99430.1166*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.124 (5)0.171 (5)0.079 (3)0.024 (4)0.017 (4)0.033 (4)
O20.136 (5)0.101 (4)0.127 (5)0.011 (4)0.015 (5)0.037 (4)
O30.117 (4)0.076 (3)0.106 (4)0.022 (3)0.023 (4)0.012 (3)
O40.158 (5)0.105 (3)0.078 (3)0.032 (4)0.051 (4)0.021 (3)
N50.086 (5)0.098 (5)0.070 (4)0.027 (4)0.006 (4)0.021 (4)
N60.086 (4)0.061 (3)0.065 (3)0.001 (3)0.016 (4)0.001 (3)
N70.084 (4)0.106 (4)0.149 (6)0.024 (4)0.008 (5)0.038 (5)
N80.065 (3)0.083 (3)0.048 (3)0.008 (3)0.004 (3)0.000 (3)
C90.050 (4)0.081 (4)0.091 (5)0.002 (4)0.002 (4)0.027 (4)
C100.046 (3)0.065 (3)0.066 (4)0.010 (3)0.004 (3)0.012 (3)
C110.051 (4)0.092 (4)0.056 (4)0.012 (4)0.006 (3)0.014 (4)
C120.054 (3)0.077 (4)0.051 (3)0.024 (4)0.004 (3)0.008 (3)
C130.057 (4)0.054 (3)0.066 (4)0.014 (3)0.008 (3)0.004 (3)
C140.052 (4)0.062 (3)0.054 (3)0.011 (3)0.005 (3)0.006 (3)
C150.052 (4)0.062 (3)0.055 (4)0.004 (3)0.003 (3)0.007 (3)
C160.047 (3)0.064 (4)0.079 (4)0.011 (3)0.005 (3)0.018 (4)
C170.061 (4)0.091 (5)0.124 (6)0.011 (4)0.020 (5)0.052 (5)
C180.059 (5)0.083 (5)0.199 (10)0.004 (5)0.002 (7)0.065 (7)
C190.059 (5)0.068 (4)0.162 (8)0.003 (4)0.016 (6)0.001 (5)
C200.057 (4)0.066 (3)0.108 (5)0.018 (4)0.006 (5)0.006 (4)
C210.042 (3)0.050 (3)0.070 (4)0.009 (3)0.005 (3)0.000 (3)
C220.050 (3)0.060 (3)0.057 (3)0.013 (3)0.005 (3)0.004 (3)
C230.065 (4)0.082 (4)0.059 (4)0.011 (4)0.000 (4)0.003 (4)
C240.074 (5)0.090 (4)0.080 (4)0.020 (4)0.017 (4)0.022 (5)
C250.067 (5)0.067 (4)0.121 (6)0.005 (4)0.009 (5)0.033 (4)
C260.060 (4)0.053 (3)0.094 (5)0.003 (3)0.011 (4)0.006 (3)
C270.051 (4)0.059 (3)0.059 (3)0.011 (3)0.001 (3)0.003 (3)
C280.098 (6)0.142 (6)0.061 (4)0.009 (5)0.014 (5)0.007 (4)
Geometric parameters (Å, º) top
O1—N51.218 (9)C17—C181.38 (1)
O2—N51.209 (9)C17—H170.966
O3—N61.204 (7)C18—C191.37 (1)
O4—N61.212 (7)C18—H180.968
N5—C121.490 (9)C19—C201.389 (9)
N6—C141.476 (8)C19—H190.963
N7—C91.099 (9)C20—C211.397 (8)
N8—C161.365 (8)C20—H200.979
N8—C271.387 (7)C21—C221.449 (8)
N8—C281.475 (7)C22—C231.378 (8)
C9—C101.462 (9)C22—C271.405 (8)
C10—C111.393 (8)C23—C241.380 (9)
C10—C151.397 (8)C23—H230.966
C11—C121.371 (9)C24—C251.389 (10)
C11—H110.971C24—H240.968
C12—C131.388 (8)C25—C261.393 (10)
C13—C141.372 (8)C25—H250.968
C13—H130.967C26—C271.390 (8)
C14—C151.386 (7)C26—H260.961
C15—H150.977C28—H28A0.969
C16—C171.393 (9)C28—H28B0.971
C16—C211.409 (9)C28—H28C0.970
O1—N5—O2124.5 (7)C17—C18—H18116.8
O1—N5—C12116.4 (6)C19—C18—H18121.1
O2—N5—C12119.0 (6)C18—C19—C20121.4 (6)
O3—N6—O4123.5 (6)C18—C19—H19117.1
O3—N6—C14118.3 (5)C20—C19—H19121.5
O4—N6—C14118.2 (5)C19—C20—C21117.7 (5)
C16—N8—C27108.8 (5)C19—C20—H20121.0
C16—N8—C28126.0 (5)C21—C20—H20121.3
C27—N8—C28125.2 (5)C16—C21—C20120.5 (5)
N7—C9—C10177.3 (7)C16—C21—C22106.1 (5)
C9—C10—C11120.3 (5)C20—C21—C22133.3 (5)
C9—C10—C15117.2 (5)C21—C22—C23132.9 (5)
C11—C10—C15122.5 (5)C21—C22—C27106.4 (5)
C10—C11—C12116.6 (5)C23—C22—C27120.7 (5)
C10—C11—H11120.6C22—C23—C24118.4 (5)
C12—C11—H11122.7C22—C23—H23120.6
N5—C12—C11119.2 (5)C24—C23—H23120.9
N5—C12—C13116.0 (5)C23—C24—C25121.0 (5)
C11—C12—C13124.8 (5)C23—C24—H24122.9
C12—C13—C14115.0 (5)C25—C24—H24116.0
C12—C13—H13122.9C24—C25—C26121.7 (5)
C14—C13—H13122.1C24—C25—H25120.2
N6—C14—C13118.3 (5)C26—C25—H25118.0
N6—C14—C15116.5 (5)C25—C26—C27116.8 (5)
C13—C14—C15125.2 (5)C25—C26—H26118.3
C10—C15—C14115.8 (5)C27—C26—H26124.9
C10—C15—H15123.0N8—C27—C22109.0 (5)
C14—C15—H15121.1N8—C27—C26129.6 (5)
N8—C16—C17129.7 (6)C22—C27—C26121.4 (5)
N8—C16—C21109.6 (5)N8—C28—H28A110.8
C17—C16—C21120.7 (5)N8—C28—H28B111.3
C16—C17—C18117.6 (6)N8—C28—H28C111.0
C16—C17—H17120.3H28A—C28—H28B107.9
C18—C17—H17122.1H28A—C28—H28C108.0
C17—C18—C19122.0 (7)H28B—C28—H28C107.8
(II) top
Crystal data top
C14H13N·C7H3N3O4Dx = 1.368 Mg m3
Mr = 388.38Mo Kα radiation, λ = 0.71073 Å
Monoclinic, P21/aCell parameters from 25 reflections
a = 16.227 (2) Åθ = 10.0–15.0°
b = 6.982 (2) ŵ = 0.10 mm1
c = 17.435 (2) ÅT = 293 K
β = 107.30 (1)°Prism, orange
V = 1886.0 (6) Å30.5 × 0.35 × 0.3 mm
Z = 4
Data collection top
Rigaku AFC5
diffractometer
θmax = 27.5°, θmin = 2.0°
θ–2θ scansh = 021
4482 measured reflectionsk = 09
4322 independent reflectionsl = 2222
1585 reflections with I > 2σ(I)3 standard reflections every 100 reflections
Rint = 0.020 intensity decay: 2.8%
Refinement top
Refinement on F2 w = 1/[σ2(Fo2) + (0.0549P)2]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.064(Δ/σ)max = 0.001
wR(F2) = 0.160Δρmax = 0.13 e Å3
S = 0.97Δρmin = 0.13 e Å3
4322 reflectionsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
263 parametersExtinction coefficient: 0.0071 (10)
H-atom parameters not refined
Crystal data top
C14H13N·C7H3N3O4V = 1886.0 (6) Å3
Mr = 388.38Z = 4
Monoclinic, P21/aMo Kα radiation
a = 16.227 (2) ŵ = 0.10 mm1
b = 6.982 (2) ÅT = 293 K
c = 17.435 (2) Å0.5 × 0.35 × 0.3 mm
β = 107.30 (1)°
Data collection top
Rigaku AFC5
diffractometer
Rint = 0.020
4482 measured reflections3 standard reflections every 100 reflections
4322 independent reflections intensity decay: 2.8%
1585 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.064263 parameters
wR(F2) = 0.160H-atom parameters not refined
S = 0.97Δρmax = 0.13 e Å3
4322 reflectionsΔρmin = 0.13 e Å3
Special details top

Refinement. Refinement was based on F2 against all reflections. The weighted R-factor (wR) and goodness of fit (S) were based on F2, and conventional R-factor (R) was calculated on F, with F set to zero for negative F2. The threshold expression of I > 2σ(I) was used only for calculating R-factor(gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.5497 (2)0.8484 (4)0.9271 (2)0.0994 (9)
O20.5317 (2)0.8096 (4)0.8004 (2)0.0933 (9)
O30.2550 (2)0.9426 (4)0.6110 (1)0.1023 (10)
O40.1440 (2)0.9922 (4)0.6523 (2)0.1003 (9)
N50.5045 (2)0.8442 (4)0.8574 (2)0.0715 (8)
N60.2203 (2)0.9591 (4)0.6640 (2)0.0749 (9)
N70.2286 (2)0.9773 (6)1.0053 (2)0.126 (1)
N80.3681 (2)0.3832 (4)0.6538 (2)0.0662 (8)
C90.2554 (2)0.9581 (6)0.9534 (2)0.083 (1)
C100.2907 (2)0.9364 (5)0.8868 (2)0.0622 (9)
C110.3784 (2)0.9040 (5)0.9038 (2)0.0629 (9)
C120.4114 (2)0.8838 (4)0.8400 (2)0.0549 (8)
C130.3619 (2)0.8997 (4)0.7610 (2)0.0570 (8)
C140.2753 (2)0.9348 (4)0.7476 (2)0.0584 (8)
C150.2380 (2)0.9524 (5)0.8088 (2)0.0630 (9)
C160.4163 (2)0.3694 (4)0.7341 (2)0.0582 (8)
C170.5036 (2)0.3290 (5)0.7664 (2)0.0706 (10)
C180.5370 (2)0.3223 (5)0.8488 (2)0.080 (1)
C190.4841 (3)0.3556 (6)0.8974 (2)0.085 (1)
C200.3970 (3)0.3917 (5)0.8660 (2)0.074 (1)
C210.3621 (2)0.3992 (4)0.7823 (2)0.0593 (9)
C220.2774 (2)0.4341 (4)0.7289 (2)0.0625 (9)
C230.1964 (3)0.4741 (5)0.7397 (2)0.078 (1)
C240.1269 (2)0.5054 (6)0.6727 (3)0.092 (1)
C250.1347 (2)0.4988 (6)0.5953 (2)0.096 (1)
C260.2134 (3)0.4591 (6)0.5828 (2)0.085 (1)
C270.2836 (2)0.4260 (5)0.6504 (2)0.0645 (9)
C280.4035 (2)0.3946 (6)0.5860 (2)0.084 (1)
C290.4271 (2)0.5972 (6)0.5716 (2)0.105 (1)
H110.41620.89430.95910.0697*
H130.38710.88510.71650.0634*
H150.17570.96620.79680.0689*
H170.53940.30430.73160.0798*
H180.59830.29480.87270.0942*
H190.50970.35130.95600.0988*
H200.36010.41170.90050.0871*
H230.19050.47780.79350.0918*
H240.07160.53960.67990.1041*
H250.08360.52180.54890.1120*
H260.22080.45580.52900.1007*
H28A0.45430.31470.59610.0943*
H28B0.36110.34710.53790.0943*
H29A0.45010.60680.52740.1170*
H29B0.46920.64760.61950.1170*
H29C0.37610.67980.56090.1170*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.080 (2)0.117 (2)0.088 (2)0.009 (2)0.005 (2)0.003 (2)
O20.088 (2)0.101 (2)0.104 (2)0.009 (2)0.051 (2)0.004 (2)
O30.123 (2)0.123 (3)0.060 (2)0.007 (2)0.026 (2)0.005 (2)
O40.078 (2)0.109 (2)0.101 (2)0.002 (2)0.006 (2)0.004 (2)
N50.073 (2)0.061 (2)0.086 (2)0.001 (2)0.033 (2)0.006 (2)
N60.086 (2)0.067 (2)0.067 (2)0.006 (2)0.015 (2)0.007 (2)
N70.134 (3)0.167 (4)0.105 (3)0.024 (3)0.076 (2)0.021 (3)
N80.067 (2)0.074 (2)0.065 (2)0.002 (2)0.032 (1)0.012 (2)
C90.084 (3)0.098 (3)0.079 (3)0.006 (2)0.039 (2)0.003 (2)
C100.072 (2)0.057 (2)0.064 (2)0.004 (2)0.030 (2)0.000 (2)
C110.074 (2)0.060 (2)0.056 (2)0.002 (2)0.021 (2)0.008 (2)
C120.058 (2)0.047 (2)0.063 (2)0.002 (2)0.023 (2)0.000 (2)
C130.075 (2)0.042 (2)0.060 (2)0.007 (2)0.029 (2)0.005 (2)
C140.073 (2)0.047 (2)0.053 (2)0.007 (2)0.015 (2)0.003 (2)
C150.061 (2)0.059 (2)0.072 (2)0.007 (2)0.023 (2)0.001 (2)
C160.072 (2)0.046 (2)0.061 (2)0.005 (2)0.026 (2)0.005 (2)
C170.078 (3)0.058 (2)0.080 (3)0.006 (2)0.031 (2)0.003 (2)
C180.088 (3)0.064 (3)0.085 (3)0.005 (2)0.020 (2)0.011 (2)
C190.121 (3)0.064 (3)0.068 (2)0.004 (3)0.023 (2)0.014 (2)
C200.116 (3)0.050 (2)0.071 (2)0.001 (2)0.048 (2)0.007 (2)
C210.081 (3)0.040 (2)0.066 (2)0.009 (2)0.036 (2)0.004 (2)
C220.076 (2)0.042 (2)0.083 (2)0.010 (2)0.045 (2)0.006 (2)
C230.095 (3)0.053 (2)0.107 (3)0.003 (2)0.061 (3)0.002 (2)
C240.077 (3)0.074 (3)0.139 (4)0.002 (2)0.055 (3)0.007 (3)
C250.073 (3)0.091 (3)0.123 (4)0.005 (3)0.025 (3)0.004 (3)
C260.075 (3)0.092 (3)0.090 (3)0.008 (2)0.026 (2)0.005 (2)
C270.070 (2)0.055 (2)0.075 (2)0.009 (2)0.031 (2)0.011 (2)
C280.084 (3)0.112 (3)0.064 (2)0.006 (2)0.033 (2)0.016 (2)
C290.101 (3)0.131 (4)0.099 (3)0.003 (3)0.052 (3)0.026 (3)
Geometric parameters (Å, º) top
O1—N51.219 (4)C18—C191.395 (6)
O2—N51.225 (5)C18—H180.976
O3—N61.222 (5)C19—C201.379 (6)
O4—N61.216 (5)C19—H190.981
N5—C121.476 (4)C20—C211.400 (5)
N6—C141.475 (4)C20—H200.977
N7—C91.123 (6)C21—C221.434 (4)
N8—C161.390 (4)C22—C231.409 (6)
N8—C271.387 (5)C22—C271.403 (6)
N8—C281.463 (5)C23—C241.378 (5)
C9—C101.447 (6)C23—H230.972
C10—C111.383 (5)C24—C251.393 (7)
C10—C151.379 (4)C24—H240.972
C11—C121.378 (5)C25—C261.386 (6)
C11—H110.980C25—H250.985
C12—C131.376 (4)C26—C271.394 (4)
C13—C141.376 (5)C26—H260.980
C13—H130.984C28—C291.506 (6)
C14—C151.380 (5)C28—H28A0.966
C15—H150.976C28—H28B0.971
C16—C171.390 (5)C29—H29A0.953
C16—C211.401 (6)C29—H29B0.974
C17—C181.376 (5)C29—H29C0.979
C17—H170.971
O1—N5—O2123.9 (3)C18—C19—H19118.8
O1—N5—C12118.5 (3)C20—C19—H19119.1
O2—N5—C12117.6 (3)C19—C20—C21118.1 (4)
O3—N6—O4124.5 (3)C19—C20—H20121.6
O3—N6—C14117.2 (3)C21—C20—H20120.3
O4—N6—C14118.3 (3)C16—C21—C20119.2 (3)
C16—N8—C27108.1 (3)C16—C21—C22106.7 (3)
C16—N8—C28125.4 (3)C20—C21—C22134.1 (4)
C27—N8—C28125.1 (2)C21—C22—C23134.3 (3)
N7—C9—C10179.0 (4)C21—C22—C27107.1 (3)
C9—C10—C11118.2 (3)C23—C22—C27118.6 (3)
C9—C10—C15120.3 (3)C22—C23—C24118.6 (4)
C11—C10—C15121.4 (3)C22—C23—H23119.8
C10—C11—C12117.8 (3)C24—C23—H23121.6
C10—C11—H11121.6C23—C24—C25121.9 (4)
C12—C11—H11120.6C23—C24—H24118.9
N5—C12—C11118.2 (3)C25—C24—H24119.1
N5—C12—C13118.6 (3)C24—C25—C26120.8 (3)
C11—C12—C13123.2 (3)C24—C25—H25119.6
C12—C13—C14116.6 (3)C26—C25—H25119.6
C12—C13—H13121.6C25—C26—C27117.4 (4)
C14—C13—H13121.8C25—C26—H26122.4
N6—C14—C13118.4 (3)C27—C26—H26120.2
N6—C14—C15118.6 (3)N8—C27—C22109.0 (3)
C13—C14—C15123.0 (3)N8—C27—C26128.3 (4)
C10—C15—C14118.0 (3)C22—C27—C26122.7 (4)
C10—C15—H15121.3N8—C28—C29111.5 (3)
C14—C15—H15120.6N8—C28—H28A109.8
N8—C16—C17128.5 (3)N8—C28—H28B109.3
N8—C16—C21109.2 (3)C29—C28—H28A109.2
C17—C16—C21122.3 (3)C29—C28—H28B109.1
C16—C17—C18117.8 (4)H28A—C28—H28B108.0
C16—C17—H17120.7C28—C29—H29A112.3
C18—C17—H17121.5C28—C29—H29B110.2
C17—C18—C19120.5 (3)C28—C29—H29C110.0
C17—C18—H18119.1H29A—C29—H29B108.9
C19—C18—H18120.4H29A—C29—H29C108.4
C18—C19—C20122.1 (3)H29B—C29—H29C106.8

Experimental details

(I)(II)
Crystal data
Chemical formulaC13H11N·C7H3N3O4C14H13N·C7H3N3O4
Mr374.35388.38
Crystal system, space groupOrthorhombic, P212121Monoclinic, P21/a
Temperature (K)293293
a, b, c (Å)8.339 (2), 27.604 (4), 7.817 (2)16.227 (2), 6.982 (2), 17.435 (2)
α, β, γ (°)90, 90, 9090, 107.30 (1), 90
V3)1799.4 (7)1886.0 (6)
Z44
Radiation typeMo KαMo Kα
µ (mm1)0.100.10
Crystal size (mm)0.55 × 0.3 × 0.20.5 × 0.35 × 0.3
Data collection
DiffractometerRigaku AFC5
diffractometer
Rigaku AFC5
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
2384, 2384, 1034 4482, 4322, 1585
Rint?0.020
(sin θ/λ)max1)0.6500.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.063, 0.162, 1.00 0.064, 0.160, 0.97
No. of reflections23844322
No. of parameters253263
No. of restraints??
H-atom treatmentH-atom parameters not refinedH-atom parameters not refined
Δρmax, Δρmin (e Å3)0.21, 0.160.13, 0.13

Computer programs: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993), MSC/AFC Diffractometer Control Software, TEXSAN (Molecular Structure Corporation, 1999), SIR92 (Altomare et al., 1994), SHELXL97 (Sheldrick, 1997), TEXSAN.

Selected geometric parameters (Å, º) for (I) top
O1—N51.218 (9)N7—C91.099 (9)
O2—N51.209 (9)N8—C281.475 (7)
O3—N61.204 (7)C9—C101.462 (9)
O4—N61.212 (7)
O1—N5—O2124.5 (7)N7—C9—C10177.3 (7)
O3—N6—O4123.5 (6)
Selected geometric parameters (Å, º) for (II) top
O1—N51.219 (4)N7—C91.123 (6)
O2—N51.225 (5)N8—C281.463 (5)
O3—N61.222 (5)C9—C101.447 (6)
O4—N61.216 (5)C28—C291.506 (6)
O1—N5—O2123.9 (3)N7—C9—C10179.0 (4)
O3—N6—O4124.5 (3)N8—C28—C29111.5 (3)
 

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