Literature DB >> 25161573

2,3-Di-methyl-quinazolin-4(3H)-one.

Fozil E Saitkulov1, Azamat A Tashniyazov2, Azimjon A Mamadrahimov3, Kh M Shakhidoyatov4.   

Abstract

The non-H atoms of the title mol-ecule, C10H10N2O, are essentially coplanar, with a maximum deviation of 0.046 (4) Å for the O atom. In the crystal, mol-ecules are linked by weak C-H⋯O hydrogen bonds, forming chains along [010]. In addtion, weak C-H⋯π inter-actions and π-π stacking inter-actions between benzene and pyrimidine rings, with a centroid-centroid distance of 3.730 (3) Å, link the chains, forming a two-dimensional network parallel to (001).

Entities:  

Year:  2014        PMID: 25161573      PMCID: PMC4120575          DOI: 10.1107/S1600536814013749

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the synthesis of related compounds, see: Takeuchi & Eguchi (1989 ▶). For the crystal structure of a related compound, see: Makhloufi et al. (2013 ▶). For standard bond lengths, see: Allen et al. (1987 ▶).

Experimental

Crystal data

C10H10N2O M = 174.20 Orthorhombic, a = 4.826 (2) Å b = 7.919 (3) Å c = 23.060 (8) Å V = 881.3 (11) Å3 Z = 4 Cu Kα radiation μ = 0.71 mm−1 T = 293 K 0.40 × 0.10 × 0.08 mm

Data collection

Oxford Diffraction Xcalibur Ruby diffractometer Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009 ▶) T min = 0.041, T max = 1.000 2236 measured reflections 1585 independent reflections 821 reflections with I > 2σ(I) R int = 0.020

Refinement

R[F 2 > 2σ(F 2)] = 0.071 wR(F 2) = 0.230 S = 0.97 1585 reflections 121 parameters H-atom parameters constrained Δρmax = 0.20 e Å−3 Δρmin = −0.19 e Å−3 Absolute structure: Flack (1983 ▶), 507 Friedel pairs Absolute structure parameter: −0.3 (12) Data collection: CrysAlis PRO (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablock(s) I, GLOBAL. DOI: 10.1107/S1600536814013749/lh5714sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814013749/lh5714Isup2.hkl Click here for additional data file. Supporting information file. DOI: 10.1107/S1600536814013749/lh5714Isup3.cml CCDC reference: 1007927 Additional supporting information: crystallographic information; 3D view; checkCIF report
C10H10N2ODx = 1.313 Mg m3
Mr = 174.20Melting point: 491(2) K
Orthorhombic, P212121Cu Kα radiation, λ = 1.54184 Å
Hall symbol: P 2ac 2abCell parameters from 333 reflections
a = 4.826 (2) Åθ = 3.8–64.0°
b = 7.919 (3) ŵ = 0.71 mm1
c = 23.060 (8) ÅT = 293 K
V = 881.3 (11) Å3Needle, colourless
Z = 40.40 × 0.10 × 0.08 mm
F(000) = 368
Oxford Diffraction Xcalibur Ruby diffractometer1585 independent reflections
Radiation source: fine-focus sealed tube821 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.020
Detector resolution: 10.2576 pixels mm-1θmax = 75.9°, θmin = 3.8°
ω scansh = −5→5
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009)k = −5→9
Tmin = 0.041, Tmax = 1.000l = −28→28
2236 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.071H-atom parameters constrained
wR(F2) = 0.230w = 1/[σ2(Fo2) + (0.1116P)2] where P = (Fo2 + 2Fc2)/3
S = 0.97(Δ/σ)max < 0.001
1585 reflectionsΔρmax = 0.20 e Å3
121 parametersΔρmin = −0.19 e Å3
0 restraintsAbsolute structure: Flack (1983), 507 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: −0.3 (12)
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.
xyzUiso*/Ueq
N30.3333 (9)−0.1245 (5)0.17512 (17)0.0819 (12)
O10.4020 (9)0.1511 (4)0.19869 (17)0.1055 (13)
N10.5799 (9)−0.2643 (5)0.10074 (17)0.0846 (11)
C4A0.6580 (10)0.0357 (6)0.1199 (2)0.0773 (13)
C40.4620 (11)0.0295 (7)0.1667 (2)0.0807 (13)
C100.1309 (12)−0.1350 (7)0.2233 (2)0.1009 (17)
H10A0.2040−0.20590.25340.151*
H10B−0.0397−0.18190.20930.151*
H10C0.0975−0.02400.23860.151*
C80.8983 (11)−0.1088 (7)0.0431 (2)0.0912 (15)
H80.9313−0.20670.02190.109*
C20.4000 (11)−0.2650 (6)0.1422 (2)0.0816 (13)
C8A0.7099 (9)−0.1120 (6)0.0883 (2)0.0769 (12)
C71.0368 (13)0.0367 (8)0.0292 (2)0.1023 (16)
H71.16470.0374−0.00100.123*
C90.2541 (14)−0.4274 (7)0.1551 (3)0.109 (2)
H9A0.2779−0.45520.19540.164*
H9B0.3305−0.51580.13160.164*
H9C0.0603−0.41530.14680.164*
C60.9842 (12)0.1838 (7)0.0607 (3)0.1019 (18)
H61.07760.28280.05140.122*
C50.7965 (12)0.1837 (6)0.1051 (2)0.0923 (16)
H50.76150.28280.12550.111*
U11U22U33U12U13U23
N30.077 (2)0.080 (3)0.089 (3)0.004 (2)0.003 (2)0.002 (2)
O10.118 (3)0.083 (2)0.115 (3)0.008 (2)−0.002 (3)−0.024 (2)
N10.080 (2)0.080 (2)0.094 (3)−0.004 (2)0.002 (2)−0.005 (2)
C4A0.074 (3)0.072 (3)0.086 (3)−0.001 (2)−0.011 (3)−0.001 (3)
C40.083 (3)0.073 (3)0.086 (3)0.010 (3)−0.011 (3)−0.004 (3)
C100.100 (4)0.104 (4)0.098 (3)0.020 (4)0.012 (3)0.008 (3)
C80.085 (3)0.090 (3)0.099 (3)0.004 (3)0.003 (3)−0.012 (3)
C20.076 (3)0.066 (3)0.102 (3)0.004 (3)−0.006 (3)−0.002 (3)
C8A0.068 (3)0.071 (3)0.091 (3)−0.001 (3)−0.005 (3)0.003 (3)
C70.092 (4)0.117 (4)0.098 (3)−0.003 (4)0.006 (3)0.006 (4)
C90.103 (4)0.077 (3)0.147 (5)−0.002 (3)0.014 (4)0.002 (4)
C60.096 (4)0.092 (4)0.118 (4)−0.013 (3)−0.008 (4)0.022 (3)
C50.093 (4)0.076 (3)0.108 (4)0.003 (3)−0.009 (3)−0.002 (3)
N3—C41.382 (6)C8—C71.370 (7)
N3—C21.385 (6)C8—C8A1.383 (7)
N3—C101.482 (6)C8—H80.9300
O1—C41.248 (6)C2—C91.496 (7)
N1—C21.292 (6)C7—C61.397 (8)
N1—C8A1.390 (6)C7—H70.9300
C4A—C51.392 (7)C9—H9A0.9600
C4A—C8A1.400 (6)C9—H9B0.9600
C4A—C41.436 (7)C9—H9C0.9600
C10—H10A0.9600C6—C51.368 (7)
C10—H10B0.9600C6—H60.9300
C10—H10C0.9600C5—H50.9300
C4—N3—C2121.8 (4)N1—C2—C9117.9 (5)
C4—N3—C10116.8 (4)N3—C2—C9118.2 (5)
C2—N3—C10121.3 (5)C8—C8A—N1117.9 (5)
C2—N1—C8A117.4 (4)C8—C8A—C4A119.6 (5)
C5—C4A—C8A119.4 (5)N1—C8A—C4A122.4 (4)
C5—C4A—C4121.9 (5)C8—C7—C6119.4 (5)
C8A—C4A—C4118.7 (5)C8—C7—H7120.3
O1—C4—N3119.5 (5)C6—C7—H7120.3
O1—C4—C4A124.9 (5)C2—C9—H9A109.5
N3—C4—C4A115.6 (4)C2—C9—H9B109.5
N3—C10—H10A109.5H9A—C9—H9B109.5
N3—C10—H10B109.5C2—C9—H9C109.5
H10A—C10—H10B109.5H9A—C9—H9C109.5
N3—C10—H10C109.5H9B—C9—H9C109.5
H10A—C10—H10C109.5C5—C6—C7120.7 (5)
H10B—C10—H10C109.5C5—C6—H6119.7
C7—C8—C8A120.8 (5)C7—C6—H6119.7
C7—C8—H8119.6C6—C5—C4A120.1 (5)
C8A—C8—H8119.6C6—C5—H5120.0
N1—C2—N3124.0 (5)C4A—C5—H5120.0
D—H···AD—HH···AD···AD—H···A
C10—H10A···O1i0.962.473.345 (8)151
C10—H10B···Cgii0.962.803.608 (6)142
Table 1

Hydrogen-bond geometry (Å, °)

Cg is the centroid of the N1/C2/N3/C4/C4A/C8A ring.

D—H⋯A D—HH⋯A DA D—H⋯A
C10—H10A⋯O1i 0.962.473.345 (8)151
C10—H10BCg ii 0.962.803.608 (6)142

Symmetry codes: (i) ; (ii) .

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Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

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1.  Crystal structure and Hirshfeld surface analysis of 3-methyl-4-oxo-N-phenyl-3,4-di-hydro-quinazoline-2-carbo-thio-amide.

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