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In the framework of a thorough study of the reactions of C-(2,4,6-tri­nitro­phenyl)­azo­methines with various nucleophiles, the crystal and molecular structures of three compounds, namely 2,4-dinitro-N-phenyl-6-(phenyl­azo)­benzamide, (I), N-(2-methoxy­phenyl)-2-(2-methoxy­phenylazo)-4,6-dinitro­benzamide, (II), and N-methyl-2,4-dinitro-N-phenyl-6-(phenylazo)­benzamide, (III), were determined from low-resolution laboratory powder diffraction data. The crystal structure determination of (I), starting from erroneous two-dimensional structures, produced the correct solution as a result of the use of a combination of a systematic grid search and bond-restrained Rietveld refinement. The obtained molecular structure of (I) was quite unexpected. Based on the correct molecular structure of (I), the crystal structures of (II) and (III) were routinely solved by the grid search technique.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0021889802014012/hw0101sup1.cif
Contains datablocks I, II, III

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889802014012/hw0101Isup2.rtv
Contains datablock I

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889802014012/hw0101IIsup3.rtv
Contains datablock II

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889802014012/hw0101IIIsup4.rtv
Contains datablock pattern_III

CCDC references: 199446; 199447; 199448

Computing details top

For all compounds, data collection: local program; cell refinement: LSPAID (Visser, 1986); program(s) used to solve structure: MRIA (Zlokazov & Chernyshev, 1992); program(s) used to refine structure: MRIA (Zlokazov & Chernyshev, 1992); molecular graphics: PLATON (Spek, 2001); software used to prepare material for publication: PARST (Nardelli, 1983).

Figures top
[Figure 1]
[Figure 2]
(I) 2,4-dinitro-N-phenyl-6-(phenyldiazenyl)-benzamide top
Crystal data top
C19H13N5O5Z = 2
Mr = 391.34F(000) = 404
Monoclinic, P21Dx = 1.474 Mg m3
a = 11.720 (6) ÅCu Kα radiation, λ = 1.5418 Å
b = 6.831 (4) ÅT = 295 K
c = 11.045 (6) ÅParticle morphology: needles
β = 94.38 (2)°yellow
V = 881.7 (8) Å3flat_sheet, 25 × 25 mm
Data collection top
DRON-3M
diffractometer (Burevestnik, Russia)
Data collection mode: reflection
Radiation source: X-ray sealed tubeScan method: step
Ni filtered monochromator2θmin = 6.00°, 2θmax = 70.0°, 2θstep = 0.02°
Specimen mounting: pressed as a thin layer in the specimen holder
Refinement top
Refinement on Inet138 parameters
Least-squares matrix: full with fixed elements per cycle51 restraints
Rp = 0.0651 constraint
Rwp = 0.083H-atom parameters not refined
Rexp = 0.021Weighting scheme based on measured s.u.'s
χ2 = 16.322(Δ/σ)max = 0.01
3201 data pointsBackground function: Chebyshev polynomial up to the 5th order
Profile function: split-type pseudo-Voigt (Toraya, 1986)Preferred orientation correction: Spherical harmonics expansion (Ahtee et al., 1989) up to the 6th order.
Crystal data top
C19H13N5O5β = 94.38 (2)°
Mr = 391.34V = 881.7 (8) Å3
Monoclinic, P21Z = 2
a = 11.720 (6) ÅCu Kα radiation, λ = 1.5418 Å
b = 6.831 (4) ÅT = 295 K
c = 11.045 (6) Åflat_sheet, 25 × 25 mm
Data collection top
DRON-3M
diffractometer (Burevestnik, Russia)
Scan method: step
Specimen mounting: pressed as a thin layer in the specimen holder2θmin = 6.00°, 2θmax = 70.0°, 2θstep = 0.02°
Data collection mode: reflection
Refinement top
Rp = 0.0653201 data points
Rwp = 0.083138 parameters
Rexp = 0.02151 restraints
χ2 = 16.322H-atom parameters not refined
Special details top

Experimental. specimen was rotated in its plane

Refinement. Hydrogen atoms were placed in calculated positions. The planarity of the aromatic rings and nitrogroups was restrained. The only common atomic displacement parameter was refined for all non-H atoms.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.5482 (8)0.04010.3273 (8)0.060 (2)*
C20.6418 (10)0.059 (5)0.2580 (8)0.060*
C30.7541 (8)0.033 (5)0.3112 (9)0.060*
C40.7654 (8)0.004 (5)0.4382 (8)0.060*
C50.6719 (8)0.021 (5)0.5098 (10)0.060*
C60.5622 (10)0.011 (5)0.4553 (8)0.060*
C70.4304 (10)0.068 (4)0.2728 (8)0.060*
N80.6246 (6)0.090 (4)0.1224 (7)0.060*
O90.5280 (6)0.110 (3)0.0801 (5)0.060*
O100.7054 (6)0.081 (3)0.0621 (6)0.060*
N110.8817 (6)0.019 (3)0.4993 (7)0.060*
O120.9648 (7)0.001 (3)0.4413 (6)0.060*
O130.8902 (6)0.068 (3)0.6054 (6)0.060*
N140.4620 (8)0.000 (5)0.5186 (8)0.060*
N150.4706 (7)0.053 (3)0.6259 (6)0.060*
C160.3748 (10)0.042 (5)0.6957 (8)0.060*
C170.3897 (8)0.022 (5)0.8243 (8)0.060*
C180.2933 (9)0.006 (5)0.8919 (8)0.060*
C190.1831 (8)0.015 (5)0.8357 (8)0.060*
C200.1675 (10)0.031 (5)0.7098 (8)0.060*
C210.2614 (8)0.047 (5)0.6407 (8)0.060*
N220.3707 (8)0.105 (3)0.2581 (7)0.060*
C230.2564 (8)0.109 (4)0.2098 (9)0.060*
C240.1849 (10)0.056 (5)0.2099 (10)0.060*
C250.0712 (10)0.042 (5)0.1622 (9)0.060*
C260.0271 (11)0.134 (4)0.1144 (10)0.060*
C270.0974 (11)0.297 (3)0.1132 (10)0.060*
C280.2100 (11)0.285 (4)0.1603 (11)0.060*
O290.4013 (7)0.236 (3)0.2419 (6)0.060*
H300.68610.03380.59360.051*
H310.81790.04610.26610.051*
H320.46280.01820.86180.051*
H330.30420.00420.97730.051*
H340.11890.00520.88200.051*
H350.09240.03690.67180.051*
H360.25180.05930.55580.051*
H370.40580.21580.27640.051*
H380.21330.17420.24270.051*
H390.02340.15320.16320.051*
H400.04930.14040.08040.051*
H410.06810.41790.08090.051*
H420.25800.39680.16160.051*
Geometric parameters (Å, º) top
C1—C21.39 (2)C17—C181.41 (1)
C1—C61.42 (1)C17—H320.92
C1—C71.48 (1)C18—C191.39 (1)
C2—C31.41 (2)C18—H330.94
C2—N81.51 (1)C19—C201.39 (1)
C3—C41.41 (1)C19—H340.94
C3—H310.93C20—C211.39 (2)
C4—C51.41 (2)C20—H350.95
C4—N111.48 (1)C21—H360.94
C5—C61.39 (2)N22—C231.40 (1)
C5—H300.93N22—H370.88
C6—N141.41 (2)C23—C241.41 (3)
C7—O291.24 (3)C23—C281.41 (3)
C7—N221.38 (3)C24—C251.40 (2)
N8—O91.20 (1)C24—H380.93
N8—O101.20 (1)C25—C261.40 (4)
N11—O121.21 (1)C25—H390.95
N11—O131.22 (1)C26—C271.39 (3)
N14—N151.24 (2)C26—H400.95
N15—C161.41 (1)C27—C281.38 (2)
C16—C211.42 (1)C27—H410.95
C16—C171.42 (1)C28—H420.95
C2—C1—C6121.5 (5)C16—C17—H32119.3
C2—C1—C7121.1 (8)C19—C18—C17121.1 (9)
C6—C1—C7117.1 (6)C19—C18—H33119.9
C1—C2—C3120.6 (9)C17—C18—H33118.9
C1—C2—N8120.5 (7)C18—C19—C20119.7 (9)
C3—C2—N8118.7 (8)C18—C19—H34120.5
C2—C3—C4116.4 (9)C20—C19—H34119.8
C2—C3—H31121.6C21—C20—C19120.3 (8)
C4—C3—H31121.7C21—C20—H35120.1
C5—C4—C3123.8 (9)C19—C20—H35119.5
C5—C4—N11117.4 (8)C20—C21—C16121 (1)
C3—C4—N11118.7 (8)C20—C21—H36121.0
C6—C5—C4118.1 (9)C16—C21—H36117.8
C6—C5—H30122.2C7—N22—C23121 (1)
C4—C5—H30118.8C7—N22—H37119.1
C5—C6—N14124 (1)C23—N22—H37119.4
C5—C6—C1118.9 (8)N22—C23—C24123 (1)
N14—C6—C1117.5 (7)N22—C23—C28119 (1)
O29—C7—N22130 (2)C24—C23—C28118 (2)
O29—C7—C1117 (1)C25—C24—C23120 (1)
N22—C7—C1113.0 (9)C25—C24—H38120.5
O9—N8—O10123.5 (8)C23—C24—H38119.9
O9—N8—C2116.9 (7)C26—C25—C24121 (1)
O10—N8—C2119.4 (7)C26—C25—H39119.7
O12—N11—O13122.0 (8)C24—C25—H39119.1
O12—N11—C4119.7 (8)C27—C26—C25119 (2)
O13—N11—C4118.2 (7)C27—C26—H40120.5
N15—N14—C6116.7 (8)C25—C26—H40120.0
N14—N15—C16119.8 (8)C28—C27—C26120 (1)
N15—C16—C21122 (1)C28—C27—H41119.9
N15—C16—C17120.5 (8)C26—C27—H41120.1
C21—C16—C17118.0 (8)C27—C28—C23122 (1)
C18—C17—C16119.7 (8)C27—C28—H42120.4
C18—C17—H32121.0C23—C28—H42118.0
(II) N-(2-methoxyphenyl-2-(methoxyphenyldiazenyl)-4,6-dinitrobenzamide top
Crystal data top
C21H17N5O7F(000) = 936
Mr = 451.40Dx = 1.461 Mg m3
Orthorhombic, P212121Cu Kα radiation, λ = 1.5418 Å
a = 22.788 (8) ÅT = 295 K
b = 13.018 (6) ÅParticle morphology: needles
c = 6.920 (3) Åyellow
V = 2052.8 (15) Å3flat_sheet, 25 × 25 mm
Z = 4
Data collection top
DRON-3M
diffractometer (Burevestnik, Russia)
Data collection mode: reflection
Radiation source: X-ray sealed tubeScan method: step
Ni filtered monochromator2θmin = 6.00°, 2θmax = 70.0°, 2θstep = 0.02°
Specimen mounting: pressed as a thin layer in the specimen holder
Refinement top
Refinement on Inet144 parameters
Least-squares matrix: full with fixed elements per cycle63 restraints
Rp = 0.0571 constraint
Rwp = 0.080H-atom parameters not refined
Rexp = 0.019Weighting scheme based on measured s.u.'s
χ2 = 17.140(Δ/σ)max = 0.01
3201 data pointsBackground function: Chebyshev polynomial up to the 5th order
Profile function: split-type pseudo-Voigt (Toraya, 1986)Preferred orientation correction: Spherical harmonics expansion (Ahtee et al., 1989) up to the 6th order.
Crystal data top
C21H17N5O7V = 2052.8 (15) Å3
Mr = 451.40Z = 4
Orthorhombic, P212121Cu Kα radiation, λ = 1.5418 Å
a = 22.788 (8) ÅT = 295 K
b = 13.018 (6) Åflat_sheet, 25 × 25 mm
c = 6.920 (3) Å
Data collection top
DRON-3M
diffractometer (Burevestnik, Russia)
Scan method: step
Specimen mounting: pressed as a thin layer in the specimen holder2θmin = 6.00°, 2θmax = 70.0°, 2θstep = 0.02°
Data collection mode: reflection
Refinement top
Rp = 0.0573201 data points
Rwp = 0.080144 parameters
Rexp = 0.01963 restraints
χ2 = 17.140H-atom parameters not refined
Special details top

Experimental. specimen was rotated in its plane

Refinement. Hydrogen atoms were placed in calculated positions. The planarity of the aromatic rings and nitrogroups was restrained. The only common atomic displacement parameter was refined for all non-H atoms.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.3077 (4)0.1227 (8)0.065 (3)0.035 (1)*
C20.3655 (4)0.1415 (9)0.067 (3)0.035*
C30.4090 (4)0.0624 (7)0.057 (3)0.035*
C40.3872 (4)0.0383 (7)0.041 (3)0.035*
C50.3268 (4)0.0607 (8)0.037 (3)0.035*
C60.2868 (4)0.0149 (8)0.047 (3)0.035*
C70.2573 (5)0.1913 (9)0.070 (3)0.035*
N80.3892 (4)0.2508 (8)0.083 (3)0.035*
O90.3527 (3)0.3163 (6)0.105 (2)0.035*
O100.4401 (3)0.2632 (5)0.059 (2)0.035*
N110.4282 (3)0.1255 (7)0.030 (3)0.035*
O120.4783 (2)0.1019 (6)0.042 (2)0.035*
O130.4114 (3)0.2128 (5)0.002 (2)0.035*
N140.2250 (4)0.0116 (8)0.045 (3)0.035*
N150.2009 (3)0.0681 (7)0.102 (3)0.035*
C160.1394 (3)0.0749 (8)0.074 (3)0.035*
C170.1130 (4)0.1735 (8)0.094 (3)0.035*
C180.0528 (4)0.1805 (7)0.066 (3)0.035*
C190.0194 (3)0.0946 (9)0.022 (3)0.035*
C200.0452 (4)0.0021 (7)0.005 (3)0.035*
C210.1050 (4)0.0117 (7)0.032 (3)0.035*
N220.2415 (4)0.2398 (6)0.098 (2)0.035*
C230.1927 (4)0.3052 (8)0.117 (3)0.035*
C240.1449 (4)0.2997 (8)0.012 (3)0.035*
C250.0962 (4)0.3634 (9)0.004 (3)0.035*
C260.0935 (4)0.4342 (9)0.153 (3)0.035*
C270.1390 (4)0.4398 (9)0.287 (3)0.035*
C280.1885 (4)0.3766 (9)0.271 (3)0.035*
O290.2347 (3)0.3838 (6)0.405 (2)0.035*
O300.1482 (3)0.2562 (5)0.136 (2)0.035*
C310.2186 (4)0.4368 (9)0.574 (3)0.035*
O320.2361 (3)0.2095 (6)0.2347 (17)0.035*
C330.1198 (5)0.352 (1)0.118 (3)0.035*
H340.31480.13020.02710.051*
H350.44880.07650.05990.051*
H360.03440.24430.07680.051*
H370.02090.10170.00530.051*
H380.02240.05950.02300.051*
H390.12280.07570.01990.051*
H400.26890.24320.18500.051*
H410.14750.25350.11420.051*
H420.06570.35790.08460.051*
H430.06050.47560.16640.051*
H440.13670.48670.38680.051*
H450.24980.43420.66630.051*
H460.21000.50720.54160.051*
H470.18380.40590.62810.051*
H480.14670.40590.15150.051*
H490.10720.36100.01360.051*
H500.08640.35410.20180.051*
Geometric parameters (Å, º) top
C1—C21.34 (1)C19—C201.39 (1)
C1—C71.46 (2)C19—H370.93
C1—C61.49 (2)C20—C211.38 (1)
C2—C31.43 (1)C20—H380.93
C2—N81.53 (1)C21—H390.93
C3—C41.41 (1)N22—C231.41 (1)
C3—H350.93N22—H400.87
C4—C51.41 (1)C23—C241.41 (2)
C4—N111.47 (1)C23—C281.42 (2)
C5—C61.34 (1)C24—C251.39 (1)
C5—H340.95C24—H410.93
C6—N141.41 (1)C25—C261.38 (2)
C7—O321.26 (2)C25—H420.93
C7—N221.37 (2)C26—C271.39 (2)
N8—O101.18 (1)C26—H430.93
N8—O91.20 (1)C27—C281.40 (1)
N11—O121.185 (9)C27—H440.93
N11—O131.22 (1)C28—O291.41 (2)
N14—N151.24 (2)O29—C311.41 (2)
N15—C161.42 (1)O30—C331.41 (1)
C16—C211.40 (1)C31—H450.96
C16—C171.42 (1)C31—H460.96
C17—O301.37 (1)C31—H470.96
C17—C181.39 (1)C33—H480.96
C18—C191.39 (1)C33—H490.96
C18—H360.93C33—H500.96
C2—C1—C7131.6 (9)C21—C20—C19119.1 (8)
C2—C1—C6119.2 (9)C21—C20—H38120.4
C7—C1—C6109.2 (9)C19—C20—H38120.5
C1—C2—C3123.3 (9)C20—C21—C16120.4 (8)
C1—C2—N8121.3 (9)C20—C21—H39120.0
C3—C2—N8115.4 (9)C16—C21—H39119.6
C4—C3—C2115.5 (9)C7—N22—C23124 (1)
C4—C3—H35122.2C7—N22—H40115.0
C2—C3—H35122.4C23—N22—H40118.2
C3—C4—C5122.7 (8)N22—C23—C24121.4 (9)
C3—C4—N11119.9 (8)N22—C23—C28121 (1)
C5—C4—N11117.4 (8)C24—C23—C28117 (1)
C6—C5—C4120.7 (9)C25—C24—C23122.4 (9)
C6—C5—H34120.5C25—C24—H41119.8
C4—C5—H34118.8C23—C24—H41117.7
C5—C6—N14130.9 (9)C26—C25—C24120 (1)
C5—C6—C1119 (1)C26—C25—H42120.6
N14—C6—C1110.5 (8)C24—C25—H42119.9
O32—C7—N22125 (2)C25—C26—C27120 (1)
O32—C7—C1116 (1)C25—C26—H43120.0
N22—C7—C1118 (1)C27—C26—H43120.2
O10—N8—O9126.9 (9)C26—C27—C28121.2 (9)
O10—N8—C2117.7 (9)C26—C27—H44119.4
O9—N8—C2115.2 (9)C28—C27—H44119.4
O12—N11—O13123.9 (8)C27—C28—O29121 (1)
O12—N11—C4114.1 (7)C27—C28—C23120 (1)
O13—N11—C4122.0 (8)O29—C28—C23119 (1)
N15—N14—C6117.7 (9)C31—O29—C28113 (1)
N14—N15—C16116.4 (8)C17—O30—C33113.9 (8)
C21—C16—N15122.1 (7)O29—C31—H45110.1
C21—C16—C17120.6 (9)O29—C31—H46109.0
N15—C16—C17117.4 (7)H45—C31—H46109.9
O30—C17—C18123.7 (8)O29—C31—H47109.4
O30—C17—C16118.7 (9)H45—C31—H47109.8
C18—C17—C16117.5 (8)H46—C31—H47108.7
C19—C18—C17121.3 (8)O30—C33—H48109.3
C19—C18—H36119.3O30—C33—H49109.3
C17—C18—H36119.4H48—C33—H49109.4
C18—C19—C20121 (1)O30—C33—H50109.5
C18—C19—H37119.3H48—C33—H50109.7
C20—C19—H37119.7H49—C33—H50109.5
(III) N-methyl-2,4-dinitro-N-phenyl-6-(phenyldiazenyl)-benzamide top
Crystal data top
C20H15N5O5Z = 4
Mr = 405.37F(000) = 840
Monoclinic, P21/cDx = 1.382 Mg m3
a = 8.676 (4) ÅCu Kα radiation, λ = 1.5418 Å
b = 18.560 (7) ÅT = 295 K
c = 12.098 (6) ÅParticle morphology: needles
β = 90.38 (2)°yellow
V = 1948.1 (15) Å3flat_sheet, 25 × 25 mm
Data collection top
DRON-3M
diffractometer (Burevestnik, Russia)
Data collection mode: reflection
Radiation source: X-ray sealed tubeScan method: step
Ni filtered monochromator2θmin = 8.00°, 2θmax = 72.0°, 2θstep = 0.02°
Specimen mounting: pressed as a thin layer in the specimen holder
Refinement top
Refinement on Inet142 parameters
Least-squares matrix: full with fixed elements per cycle53 restraints
Rp = 0.0501 constraint
Rwp = 0.066H-atom parameters not refined
Rexp = 0.022Weighting scheme based on measured s.u.'s
χ2 = 9.364(Δ/σ)max = 0.01
3201 data pointsBackground function: Chebyshev polynomial up to the 5th order
Profile function: split-type pseudo-Voigt (Toraya, 1986)Preferred orientation correction: Spherical harmonics expansion (Ahtee et al., 1989) up to the 6th order.
Crystal data top
C20H15N5O5β = 90.38 (2)°
Mr = 405.37V = 1948.1 (15) Å3
Monoclinic, P21/cZ = 4
a = 8.676 (4) ÅCu Kα radiation, λ = 1.5418 Å
b = 18.560 (7) ÅT = 295 K
c = 12.098 (6) Åflat_sheet, 25 × 25 mm
Data collection top
DRON-3M
diffractometer (Burevestnik, Russia)
Scan method: step
Specimen mounting: pressed as a thin layer in the specimen holder2θmin = 8.00°, 2θmax = 72.0°, 2θstep = 0.02°
Data collection mode: reflection
Refinement top
Rp = 0.0503201 data points
Rwp = 0.066142 parameters
Rexp = 0.02253 restraints
χ2 = 9.364H-atom parameters not refined
Special details top

Experimental. specimen was rotated in its plane

Refinement. Hydrogen atoms were placed in calculated positions. The planarity of the aromatic rings and nitrogroups was restrained. The only common atomic displacement parameter was refined for all non-H atoms.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.078 (2)0.4394 (6)0.3423 (8)0.073 (1)*
C20.038 (2)0.3678 (7)0.3334 (9)0.073*
C30.091 (2)0.3160 (6)0.4124 (9)0.073*
C40.1790 (18)0.3409 (6)0.5018 (9)0.073*
C50.2190 (19)0.4133 (6)0.5128 (9)0.073*
C60.167 (2)0.4635 (7)0.4352 (9)0.073*
C70.022 (2)0.4981 (6)0.2654 (8)0.073*
N80.2353 (19)0.2899 (7)0.5882 (10)0.073*
O90.2047 (14)0.2294 (4)0.5706 (6)0.073*
O100.2975 (17)0.3172 (6)0.6674 (8)0.073*
N110.0542 (18)0.3403 (6)0.2374 (8)0.073*
O120.0791 (17)0.2774 (5)0.2353 (7)0.073*
O130.0820 (14)0.3863 (4)0.1676 (6)0.073*
N140.2048 (14)0.5381 (5)0.4432 (6)0.073*
N150.2882 (14)0.5530 (5)0.5234 (6)0.073*
C160.3310 (18)0.6248 (6)0.5423 (9)0.073*
C170.434 (2)0.6415 (6)0.6296 (9)0.073*
C180.477 (2)0.7123 (6)0.6476 (9)0.073*
C190.419 (2)0.7671 (5)0.5785 (9)0.073*
C200.320 (2)0.7505 (6)0.4913 (9)0.073*
C210.2761 (18)0.6807 (6)0.4729 (9)0.073*
N220.1203 (16)0.5315 (5)0.1918 (7)0.073*
O230.1139 (13)0.5184 (4)0.2799 (5)0.073*
C240.2722 (19)0.5111 (6)0.1767 (8)0.073*
C250.393 (2)0.5578 (6)0.2091 (8)0.073*
C260.5455 (19)0.5371 (6)0.1916 (8)0.073*
C270.5776 (19)0.4707 (6)0.1437 (8)0.073*
C280.460 (2)0.4237 (6)0.1126 (8)0.073*
C290.3063 (19)0.4434 (6)0.1285 (8)0.073*
C300.070 (3)0.5933 (10)0.1248 (13)0.073*
H310.27910.42830.57320.051*
H320.06480.26810.40440.051*
H330.47280.60500.67460.051*
H340.54410.72380.70510.051*
H350.44690.81480.59120.051*
H360.28270.78700.44610.051*
H370.21020.66960.41440.051*
H380.37070.60310.23830.051*
H390.62540.56750.21260.051*
H400.67980.45720.13260.051*
H410.48310.37940.08060.051*
H420.22680.41280.10700.051*
H430.03600.60340.14050.051*
H440.08510.58370.04910.051*
H450.13220.63460.14740.051*
Geometric parameters (Å, º) top
C1—C21.38 (2)C18—C191.41 (2)
C1—C61.43 (2)C18—H340.93
C1—C71.51 (2)C19—C201.39 (2)
C2—C31.43 (2)C19—H350.93
C2—N111.50 (2)C20—C211.37 (2)
C3—C41.40 (2)C20—H360.93
C3—H320.92C21—H370.93
C4—C51.39 (2)N22—C241.38 (2)
C4—N81.49 (2)N22—C301.47 (2)
C5—C61.40 (2)C24—C251.41 (2)
C5—H310.94C24—C291.42 (2)
C6—N141.43 (2)C25—C261.40 (2)
C7—O231.25 (2)C25—H380.93
C7—N221.38 (2)C26—C271.39 (2)
N8—O91.17 (2)C26—H390.93
N8—O101.21 (2)C27—C281.39 (2)
N11—O121.19 (1)C27—H400.93
N11—O131.22 (1)C28—C291.39 (3)
N14—N151.24 (1)C28—H410.93
N15—C161.40 (1)C29—H420.93
C16—C171.41 (2)C30—H430.95
C16—C211.42 (2)C30—H440.94
C17—C181.38 (2)C30—H450.98
C17—H330.93
C2—C1—C6120 (1)C19—C18—H34120
C2—C1—C7125 (1)C20—C19—C18120 (1)
C6—C1—C7115 (1)C20—C19—H35120
C1—C2—C3121 (1)C18—C19—H35120
C1—C2—N11122 (1)C21—C20—C19120 (1)
C3—C2—N11117 (1)C21—C20—H36120
C4—C3—C2118 (1)C19—C20—H36120
C4—C3—H32122C20—C21—C16120 (1)
C2—C3—H32120C20—C21—H37120
C5—C4—C3122 (1)C16—C21—H37120
C5—C4—N8118 (1)C7—N22—C24124 (1)
C3—C4—N8121 (1)C7—N22—C30121 (1)
C4—C5—C6120 (1)C24—N22—C30115 (1)
C4—C5—H31120N22—C24—C25120 (1)
C6—C5—H31120N22—C24—C29120 (1)
C5—C6—N14122 (1)C25—C24—C29120 (1)
C5—C6—C1119 (1)C26—C25—C24119 (1)
N14—C6—C1119 (1)C26—C25—H38120
O23—C7—N22123 (1)C24—C25—H38120
O23—C7—C1115 (1)C27—C26—C25120 (1)
N22—C7—C1121.5 (9)C27—C26—H39120
O9—N8—O10130 (1)C25—C26—H39120
O9—N8—C4114 (1)C26—C27—C28121 (1)
O10—N8—C4116 (1)C26—C27—H40119
O12—N11—O13130 (1)C28—C27—H40119
O12—N11—C2117 (1)C27—C28—C29120 (1)
O13—N11—C2113.6 (9)C27—C28—H41120
N15—N14—C6113.9 (9)C29—C28—H41120
N14—N15—C16119.5 (9)C28—C29—C24119 (1)
N15—C16—C17120 (1)C28—C29—H42121
N15—C16—C21121 (1)C24—C29—H42120
C17—C16—C21119 (1)N22—C30—H43109
C18—C17—C16120 (1)N22—C30—H44110
C18—C17—H33120H43—C30—H44112
C16—C17—H33120N22—C30—H45107
C17—C18—C19120 (1)H43—C30—H45109
C17—C18—H34120H44—C30—H45110

Experimental details

(I)(II)(III)
Crystal data
Chemical formulaC19H13N5O5C21H17N5O7C20H15N5O5
Mr391.34451.40405.37
Crystal system, space groupMonoclinic, P21Orthorhombic, P212121Monoclinic, P21/c
Temperature (K)295295295
a, b, c (Å)11.720 (6), 6.831 (4), 11.045 (6)22.788 (8), 13.018 (6), 6.920 (3)8.676 (4), 18.560 (7), 12.098 (6)
α, β, γ (°)90, 94.38 (2), 9090, 90, 9090, 90.38 (2), 90
V3)881.7 (8)2052.8 (15)1948.1 (15)
Z244
Radiation typeCu Kα, λ = 1.5418 ÅCu Kα, λ = 1.5418 ÅCu Kα, λ = 1.5418 Å
Specimen shape, size (mm)Flat_sheet, 25 × 25Flat_sheet, 25 × 25Flat_sheet, 25 × 25
Data collection
DiffractometerDRON-3M
diffractometer (Burevestnik, Russia)
DRON-3M
diffractometer (Burevestnik, Russia)
DRON-3M
diffractometer (Burevestnik, Russia)
Specimen mountingPressed as a thin layer in the specimen holderPressed as a thin layer in the specimen holderPressed as a thin layer in the specimen holder
Data collection modeReflectionReflectionReflection
Scan methodStepStepStep
2θ values (°)2θmin = 6.00 2θmax = 70.0 2θstep = 0.022θmin = 6.00 2θmax = 70.0 2θstep = 0.022θmin = 8.00 2θmax = 72.0 2θstep = 0.02
Refinement
R factors and goodness of fitRp = 0.065, Rwp = 0.083, Rexp = 0.021, χ2 = 16.322Rp = 0.057, Rwp = 0.080, Rexp = 0.019, χ2 = 17.140Rp = 0.050, Rwp = 0.066, Rexp = 0.022, χ2 = 9.364
No. of data points320132013201
No. of parameters138144142
No. of restraints516353
H-atom treatmentH-atom parameters not refinedH-atom parameters not refinedH-atom parameters not refined

Computer programs: local program, LSPAID (Visser, 1986), MRIA (Zlokazov & Chernyshev, 1992), PLATON (Spek, 2001), PARST (Nardelli, 1983).

 

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