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The conformation of the N—H bond in the structure of the title compound, C11H14ClNO, is syn to the ortho-chloro substituent, similar to that in 2,2,2-trimethyl-N-(2-methyl­phen­yl)acetamide and the side-chain unsubstituted N-(2-chloro­phen­yl)acetamide, but in contrast with the anti conformation observed for N-(3-chloro­phen­yl)-2,2,2-trimethyl­acetamide. The bond parameters are also similar to those observed in related compounds and other acetanilides. The mol­ecules are linked into chains through N—H...O hydrogen bonding.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807029005/dn2190sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807029005/dn2190Isup2.hkl
Contains datablock I

CCDC reference: 655000

Key indicators

  • Single-crystal X-ray study
  • T = 302 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.049
  • wR factor = 0.136
  • Data-to-parameter ratio = 17.0

checkCIF/PLATON results

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Alert level B PLAT242_ALERT_2_B Check Low Ueq as Compared to Neighbors for C8
Alert level C PLAT153_ALERT_1_C The su's on the Cell Axes are Equal (x 100000) 100 Ang. PLAT180_ALERT_3_C Check Cell Rounding: # of Values Ending with 0 = 3 PLAT340_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 6
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 26.37 From the CIF: _reflns_number_total 2261 Count of symmetry unique reflns 1369 Completeness (_total/calc) 165.16% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 892 Fraction of Friedel pairs measured 0.652 Are heavy atom types Z>Si present yes PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 1 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 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The structure of N-(2-chlorophenyl)-2,2,2-trimethylacetamide (2CPTMA) has been determined as part of a study on the systematization of the crystal structures of N-aromatic amides (Gowda et al., 2007, 2007a,b). The conformation of the N—H bond in 2CPTMA is syn to the ortho-chloro substituent (Fig. 1), similar to that in N-(2-methylphenyl)-2,2,2-trimethylacetamide (2MPTMA) (Gowda et al., 2007a) and the side chain unsubstituted N-(2-chlorophenyl)-acetamide (2CPA), but in contrast to the anti conformation observed for the N-(3-chlorophenyl)-2,2,2-trimethylacetamide (3CPTMA) (Gowda et al., 2007). The geometric parameters of 2CPTMA are also similar to those of 2MPTMA, 2CPA, 3CPTMA and other acetanilides (Gowda et al., 2007, 2007a,b). The molecules in 2CPTMA are packed into chains in the direction of c axis through N—H···O hydrogen bonds (Fig. 2 & Table 1).

Related literature top

For related literature, see: Gowda et al. (2003, 2007, 2007a, 2007b).

Experimental top

The title compound was prepared according to the literature method (Gowda et al., 2003). The purity of the compound was checked by determining its melting point. It was characterized by recording its infrared and NMR spectra (Gowda et al., 2003). Single crystals of the title compound were obtained from an ethanolic solution and used for X-ray diffraction studies at room temperature.

Refinement top

All H atoms attached to C atoms were fixed geometrically and treated as riding with C—H = 0.93 Å (Caromatic) and 0.96 Å (Cmethyl) with Uiso(H) = 1.2Ueq(Caromatic) or Uiso(H) = 1.5Ueq(Cmethyl). H atom attached to N atom was located in difference Fourier maps and included in the subsequent refinement using restraint (N—H= 0.85 (1) Å) with Uiso(H) = 1.2Ueq(N).

Structure description top

The structure of N-(2-chlorophenyl)-2,2,2-trimethylacetamide (2CPTMA) has been determined as part of a study on the systematization of the crystal structures of N-aromatic amides (Gowda et al., 2007, 2007a,b). The conformation of the N—H bond in 2CPTMA is syn to the ortho-chloro substituent (Fig. 1), similar to that in N-(2-methylphenyl)-2,2,2-trimethylacetamide (2MPTMA) (Gowda et al., 2007a) and the side chain unsubstituted N-(2-chlorophenyl)-acetamide (2CPA), but in contrast to the anti conformation observed for the N-(3-chlorophenyl)-2,2,2-trimethylacetamide (3CPTMA) (Gowda et al., 2007). The geometric parameters of 2CPTMA are also similar to those of 2MPTMA, 2CPA, 3CPTMA and other acetanilides (Gowda et al., 2007, 2007a,b). The molecules in 2CPTMA are packed into chains in the direction of c axis through N—H···O hydrogen bonds (Fig. 2 & Table 1).

For related literature, see: Gowda et al. (2003, 2007, 2007a, 2007b).

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell refinement: CrysAlis RED (Oxford Diffraction, 2006); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003) and ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. Molecular structure of the title compound showing the atom labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are represented as small spheres of arbitrary radii.
[Figure 2] Fig. 2. Partial packing view showing the formation of the chain through N—H···O Hydrogen bonding. H atoms not involved in hydrogen bondings have been omitted for clarity. Hydrogen bonds are shown as dashed lines. [Symmetry code: (i) x - 1/2, 1/2 - y, 2 - z].
N-(2-Chlorophenyl)-2,2,2-trimethylacetamide top
Crystal data top
C11H14ClNOF(000) = 448
Mr = 211.68Dx = 1.220 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 1749 reflections
a = 10.159 (1) Åθ = 2.7–20.5°
b = 10.248 (1) ŵ = 0.30 mm1
c = 11.071 (1) ÅT = 302 K
V = 1152.6 (2) Å3Rod shape, colourless
Z = 40.60 × 0.16 × 0.14 mm
Data collection top
Oxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
2261 independent reflections
Radiation source: Enhance (Mo) X-ray Source1279 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.049
Detector resolution: 8.4012 pixels mm-1θmax = 26.4°, θmin = 2.7°
Rotation method data acquisition using ω and φ scansh = 129
Absorption correction: analytical
(CrysAlis RED; Oxford Diffraction, 2006) using a multifaceted crystal model (Clark & Reid, 1995)
k = 1112
Tmin = 0.840, Tmax = 0.959l = 1013
6499 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.049H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.136 w = 1/[σ2(Fo2) + (0.0688P)2 + 0.003P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.002
2261 reflectionsΔρmax = 0.37 e Å3
133 parametersΔρmin = 0.24 e Å3
1 restraintAbsolute structure: Flack (1983), with 892 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.07 (13)
Crystal data top
C11H14ClNOV = 1152.6 (2) Å3
Mr = 211.68Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 10.159 (1) ŵ = 0.30 mm1
b = 10.248 (1) ÅT = 302 K
c = 11.071 (1) Å0.60 × 0.16 × 0.14 mm
Data collection top
Oxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
2261 independent reflections
Absorption correction: analytical
(CrysAlis RED; Oxford Diffraction, 2006) using a multifaceted crystal model (Clark & Reid, 1995)
1279 reflections with I > 2σ(I)
Tmin = 0.840, Tmax = 0.959Rint = 0.049
6499 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.049H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.136Δρmax = 0.37 e Å3
S = 1.05Δρmin = 0.24 e Å3
2261 reflectionsAbsolute structure: Flack (1983), with 892 Friedel pairs
133 parametersAbsolute structure parameter: 0.07 (13)
1 restraint
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
C10.3757 (3)0.1032 (3)0.9165 (3)0.0485 (9)
C20.3373 (3)0.0764 (3)0.7973 (3)0.0529 (9)
C30.3577 (4)0.0442 (4)0.7466 (4)0.0701 (11)
H30.32900.06150.66840.084*
C40.4203 (4)0.1384 (4)0.8118 (4)0.0790 (12)
H40.43540.21970.77700.095*
C50.4610 (4)0.1155 (4)0.9273 (5)0.0776 (13)
H50.50420.18050.97050.093*
C60.4375 (4)0.0066 (3)0.9809 (4)0.0602 (10)
H60.46380.02191.06010.072*
C70.4429 (3)0.3056 (3)1.0162 (3)0.0451 (7)
C80.3943 (3)0.4347 (3)1.0682 (3)0.0533 (9)
C90.3016 (6)0.4088 (4)1.1719 (3)0.1125 (19)
H9A0.34640.35961.23310.169*
H9B0.22710.36021.14340.169*
H9C0.27230.49031.20520.169*
C100.3203 (5)0.5103 (4)0.9698 (4)0.0949 (15)
H10A0.29890.59590.99900.142*
H10B0.24070.46470.94940.142*
H10C0.37490.51760.89930.142*
C110.5068 (4)0.5190 (4)1.1055 (5)0.0958 (16)
H11A0.47370.60011.13670.144*
H11B0.56200.53591.03690.144*
H11C0.55700.47541.16690.144*
N10.3506 (3)0.2264 (3)0.9685 (3)0.0541 (7)
H10.2739 (15)0.253 (3)0.954 (3)0.065*
O10.5584 (2)0.2731 (2)1.0171 (3)0.0663 (7)
Cl10.26026 (11)0.19639 (10)0.71284 (8)0.0803 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.036 (2)0.0512 (19)0.058 (2)0.0058 (16)0.0068 (18)0.0057 (16)
C20.0393 (19)0.059 (2)0.061 (2)0.0091 (16)0.0096 (18)0.0019 (18)
C30.059 (2)0.075 (3)0.077 (3)0.008 (2)0.008 (2)0.022 (2)
C40.069 (3)0.063 (3)0.105 (4)0.003 (2)0.016 (3)0.031 (2)
C50.067 (3)0.050 (2)0.116 (4)0.0075 (19)0.001 (3)0.004 (2)
C60.053 (2)0.058 (2)0.071 (2)0.0044 (17)0.000 (2)0.002 (2)
C70.0353 (18)0.0538 (18)0.0463 (17)0.0028 (18)0.0013 (16)0.0029 (18)
C80.047 (2)0.0498 (19)0.063 (2)0.0012 (17)0.0005 (18)0.0107 (17)
C90.176 (5)0.088 (3)0.073 (3)0.005 (3)0.060 (3)0.015 (2)
C100.105 (3)0.066 (2)0.114 (3)0.022 (2)0.029 (3)0.008 (3)
C110.071 (3)0.074 (3)0.143 (4)0.004 (2)0.022 (3)0.034 (3)
N10.0377 (15)0.0533 (16)0.0713 (17)0.0076 (14)0.0047 (16)0.0130 (15)
O10.0377 (13)0.0658 (15)0.0955 (17)0.0029 (11)0.0005 (14)0.0217 (14)
Cl10.0859 (7)0.0839 (7)0.0712 (6)0.0095 (6)0.0137 (6)0.0169 (5)
Geometric parameters (Å, º) top
C1—C61.372 (5)C7—C81.526 (5)
C1—C21.404 (5)C8—C111.491 (5)
C1—N11.410 (4)C8—C91.508 (5)
C2—C31.374 (5)C8—C101.534 (5)
C2—Cl11.732 (3)C9—H9A0.9600
C3—C41.363 (6)C9—H9B0.9600
C3—H30.9300C9—H9C0.9600
C4—C51.365 (6)C10—H10A0.9600
C4—H40.9300C10—H10B0.9600
C5—C61.405 (5)C10—H10C0.9600
C5—H50.9300C11—H11A0.9600
C6—H60.9300C11—H11B0.9600
C7—O11.219 (4)C11—H11C0.9600
C7—N11.348 (4)N1—H10.841 (10)
C6—C1—C2118.3 (3)C11—C8—C10106.2 (3)
C6—C1—N1121.1 (3)C9—C8—C10108.9 (3)
C2—C1—N1120.6 (3)C7—C8—C10109.2 (3)
C3—C2—C1121.2 (3)C8—C9—H9A109.5
C3—C2—Cl1119.1 (3)C8—C9—H9B109.5
C1—C2—Cl1119.6 (2)H9A—C9—H9B109.5
C4—C3—C2119.4 (4)C8—C9—H9C109.5
C4—C3—H3120.3H9A—C9—H9C109.5
C2—C3—H3120.3H9B—C9—H9C109.5
C3—C4—C5121.0 (4)C8—C10—H10A109.5
C3—C4—H4119.5C8—C10—H10B109.5
C5—C4—H4119.5H10A—C10—H10B109.5
C4—C5—C6119.9 (4)C8—C10—H10C109.5
C4—C5—H5120.1H10A—C10—H10C109.5
C6—C5—H5120.1H10B—C10—H10C109.5
C1—C6—C5120.1 (4)C8—C11—H11A109.5
C1—C6—H6120.0C8—C11—H11B109.5
C5—C6—H6120.0H11A—C11—H11B109.5
O1—C7—N1120.5 (3)C8—C11—H11C109.5
O1—C7—C8123.1 (3)H11A—C11—H11C109.5
N1—C7—C8116.4 (3)H11B—C11—H11C109.5
C11—C8—C9111.7 (4)C7—N1—C1125.0 (3)
C11—C8—C7111.0 (3)C7—N1—H1122 (2)
C9—C8—C7109.7 (3)C1—N1—H1112 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.84 (1)2.23 (2)2.973 (3)148 (3)
Symmetry code: (i) x1/2, y+1/2, z+2.

Experimental details

Crystal data
Chemical formulaC11H14ClNO
Mr211.68
Crystal system, space groupOrthorhombic, P212121
Temperature (K)302
a, b, c (Å)10.159 (1), 10.248 (1), 11.071 (1)
V3)1152.6 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.30
Crystal size (mm)0.60 × 0.16 × 0.14
Data collection
DiffractometerOxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
Absorption correctionAnalytical
(CrysAlis RED; Oxford Diffraction, 2006) using a multifaceted crystal model (Clark & Reid, 1995)
Tmin, Tmax0.840, 0.959
No. of measured, independent and
observed [I > 2σ(I)] reflections
6499, 2261, 1279
Rint0.049
(sin θ/λ)max1)0.625
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.136, 1.05
No. of reflections2261
No. of parameters133
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.37, 0.24
Absolute structureFlack (1983), with 892 Friedel pairs
Absolute structure parameter0.07 (13)

Computer programs: CrysAlis CCD (Oxford Diffraction, 2006), CrysAlis RED (Oxford Diffraction, 2006), CrysAlis RED, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003) and ORTEP-3 (Farrugia, 1997), SHELXL97.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.841 (10)2.23 (2)2.973 (3)148 (3)
Symmetry code: (i) x1/2, y+1/2, z+2.
 

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