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The crystal structure of 3-nitrobenzonitrile, C7H4N2O2, was elucidated by low-temperature single-crystal X-ray diffraction. The compound crystallizes in the Sohncke space group P21 and features two mol­ecules in the unit cell. Aromatic π–π stacking leads to stacks of mol­ecules in the [100] direction. The absolute structure was established from anomalous dispersion.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2414314623008143/hb4451sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2414314623008143/hb4451Isup2.hkl
Contains datablock I

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2414314623008143/hb4451Isup3.cml
Supplementary material

CCDC reference: 2295676

Key indicators

Structure: I
  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.024
  • wR factor = 0.069
  • Data-to-parameter ratio = 11.7

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT089_ALERT_3_C Poor Data / Parameter Ratio (Zmax < 18) ........ 6.44 Note PLAT911_ALERT_3_C Missing FCF Refl Between Thmin & STh/L= 0.600 4 Report
Alert level G PLAT142_ALERT_4_G s.u. on b - Axis Small or Missing .............. 0.00005 Ang. PLAT143_ALERT_4_G s.u. on c - Axis Small or Missing .............. 0.00009 Ang. PLAT912_ALERT_4_G Missing # of FCF Reflections Above STh/L= 0.600 3 Note PLAT961_ALERT_5_G Dataset Contains no Negative Intensities ....... Please Check PLAT978_ALERT_2_G Number C-C Bonds with Positive Residual Density. 0 Info
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 2 ALERT level C = Check. Ensure it is not caused by an omission or oversight 5 ALERT level G = General information/check it is not something unexpected 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Computing details top

Data collection: CrysAlis PRO 1.171.42.92a (Rigaku OD, 2023); cell refinement: CrysAlis PRO 1.171.42.92a (Rigaku OD, 2023); data reduction: CrysAlis PRO 1.171.42.92a (Rigaku OD, 2023); program(s) used to solve structure: olex2.solve (Dolomanov et al., 2009); program(s) used to refine structure: SHELXL2019/3 (Sheldrick, 2015); molecular graphics: Olex2 1.5 (Dolomanov et al., 2009); software used to prepare material for publication: Olex2 1.5 (Dolomanov et al., 2009) and publCIF (Westrip, 2010).

3-Nitrobenzonitrile top
Crystal data top
C7H4N2O2F(000) = 152
Mr = 148.12Dx = 1.479 Mg m3
Monoclinic, P21Cu Kα radiation, λ = 1.54184 Å
a = 3.73339 (4) ÅCell parameters from 9014 reflections
b = 6.97307 (5) Åθ = 3.5–75.7°
c = 12.87327 (9) ŵ = 0.95 mm1
β = 97.1579 (8)°T = 100 K
V = 332.52 (1) Å3Needle, colourless
Z = 20.28 × 0.06 × 0.04 mm
Data collection top
XtaLAB Synergy-S, Dualflex, Eiger2 R CdTe 1M
diffractometer
1360 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source1353 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.025
Detector resolution: 13.3333 pixels mm-1θmax = 75.9°, θmin = 3.5°
ω scansh = 44
Absorption correction: gaussian
(CrysAlisPro; Rigaku OD, 2023)
k = 88
Tmin = 0.565, Tmax = 1.000l = 1616
10190 measured reflections
Refinement top
Refinement on F2Hydrogen site location: difference Fourier map
Least-squares matrix: fullAll H-atom parameters refined
R[F2 > 2σ(F2)] = 0.024 w = 1/[σ2(Fo2) + (0.0472P)2 + 0.0377P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.069(Δ/σ)max < 0.001
S = 1.09Δρmax = 0.17 e Å3
1360 reflectionsΔρmin = 0.17 e Å3
116 parametersAbsolute structure: Flack x determined using 611 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
1 restraintAbsolute structure parameter: 0.02 (5)
Primary atom site location: iterative
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.2952 (4)0.11413 (19)0.94632 (9)0.0316 (3)
O20.5449 (3)0.03136 (17)0.81028 (9)0.0294 (3)
N10.2525 (4)0.5665 (2)0.45848 (11)0.0323 (4)
N20.3724 (3)0.14375 (19)0.85792 (10)0.0199 (3)
C10.1823 (4)0.5195 (2)0.65436 (11)0.0192 (3)
C20.2895 (4)0.3452 (2)0.70086 (12)0.0179 (3)
C30.2551 (4)0.3250 (2)0.80620 (11)0.0171 (3)
C40.1192 (4)0.4678 (2)0.86529 (12)0.0195 (3)
C50.0164 (4)0.6403 (2)0.81697 (12)0.0215 (3)
C60.0461 (4)0.6674 (2)0.71128 (13)0.0218 (3)
C70.2185 (4)0.5471 (3)0.54475 (12)0.0236 (3)
H20.387 (6)0.249 (4)0.6661 (17)0.031 (6)*
H40.108 (5)0.445 (3)0.9361 (16)0.018 (5)*
H60.009 (5)0.790 (4)0.6782 (15)0.024 (5)*
H50.071 (6)0.738 (4)0.8528 (17)0.028 (5)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0389 (7)0.0334 (7)0.0230 (5)0.0024 (5)0.0053 (5)0.0092 (5)
O20.0321 (6)0.0201 (6)0.0368 (6)0.0076 (5)0.0073 (5)0.0018 (5)
N10.0338 (8)0.0387 (9)0.0252 (6)0.0019 (6)0.0064 (6)0.0066 (6)
N20.0181 (6)0.0192 (6)0.0220 (6)0.0006 (5)0.0014 (4)0.0019 (5)
C10.0167 (6)0.0217 (8)0.0192 (6)0.0029 (5)0.0016 (5)0.0008 (6)
C20.0151 (7)0.0184 (7)0.0206 (6)0.0003 (5)0.0034 (5)0.0018 (6)
C30.0148 (6)0.0165 (7)0.0199 (6)0.0017 (5)0.0018 (5)0.0006 (5)
C40.0165 (7)0.0231 (7)0.0190 (7)0.0010 (6)0.0021 (5)0.0023 (6)
C50.0183 (7)0.0202 (7)0.0258 (7)0.0016 (6)0.0020 (5)0.0070 (6)
C60.0181 (7)0.0190 (8)0.0275 (7)0.0005 (6)0.0004 (5)0.0013 (6)
C70.0214 (7)0.0246 (7)0.0247 (7)0.0022 (6)0.0027 (6)0.0029 (6)
Geometric parameters (Å, º) top
O1—N21.2258 (17)C2—H20.91 (3)
O2—N21.2262 (18)C3—C41.387 (2)
N1—C71.141 (2)C4—C51.386 (2)
N2—C31.4697 (19)C4—H40.93 (2)
C1—C21.392 (2)C5—C61.392 (2)
C1—C61.397 (2)C5—H50.91 (2)
C1—C71.447 (2)C6—H60.96 (2)
C2—C31.3851 (19)
O1—N2—O2123.75 (13)C4—C3—N2118.53 (12)
O1—N2—C3118.31 (12)C3—C4—H4118.7 (12)
O2—N2—C3117.93 (12)C5—C4—C3118.46 (13)
C2—C1—C6121.55 (14)C5—C4—H4122.8 (12)
C2—C1—C7118.61 (14)C4—C5—C6120.34 (14)
C6—C1—C7119.84 (14)C4—C5—H5121.5 (14)
C1—C2—H2123.1 (14)C6—C5—H5118.1 (14)
C3—C2—C1116.93 (13)C1—C6—H6119.6 (12)
C3—C2—H2119.9 (14)C5—C6—C1119.42 (14)
C2—C3—N2118.16 (12)C5—C6—H6120.9 (12)
C2—C3—C4123.30 (13)N1—C7—C1178.69 (17)
O1—N2—C3—C2169.59 (13)C2—C1—C6—C50.0 (2)
O1—N2—C3—C411.0 (2)C2—C3—C4—C50.8 (2)
O2—N2—C3—C211.01 (19)C3—C4—C5—C60.7 (2)
O2—N2—C3—C4168.36 (13)C4—C5—C6—C10.3 (2)
N2—C3—C4—C5178.55 (12)C6—C1—C2—C30.0 (2)
C1—C2—C3—N2178.92 (13)C7—C1—C2—C3179.18 (13)
C1—C2—C3—C40.4 (2)C7—C1—C6—C5179.21 (13)
 

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