Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807029005/dn2190sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807029005/dn2190Isup2.hkl |
CCDC reference: 655000
Key indicators
- Single-crystal X-ray study
- T = 302 K
- Mean (C-C) = 0.005 Å
- R factor = 0.049
- wR factor = 0.136
- Data-to-parameter ratio = 17.0
checkCIF/PLATON results
No syntax errors found
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
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.
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).
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).
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.
C11H14ClNO | F(000) = 448 |
Mr = 211.68 | Dx = 1.220 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 1749 reflections |
a = 10.159 (1) Å | θ = 2.7–20.5° |
b = 10.248 (1) Å | µ = 0.30 mm−1 |
c = 11.071 (1) Å | T = 302 K |
V = 1152.6 (2) Å3 | Rod shape, colourless |
Z = 4 | 0.60 × 0.16 × 0.14 mm |
Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector | 2261 independent reflections |
Radiation source: Enhance (Mo) X-ray Source | 1279 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.049 |
Detector resolution: 8.4012 pixels mm-1 | θmax = 26.4°, θmin = 2.7° |
Rotation method data acquisition using ω and φ scans | h = −12→9 |
Absorption correction: analytical (CrysAlis RED; Oxford Diffraction, 2006) using a multifaceted crystal model (Clark & Reid, 1995) | k = −11→12 |
Tmin = 0.840, Tmax = 0.959 | l = −10→13 |
6499 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.049 | H 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 reflections | Δρmax = 0.37 e Å−3 |
133 parameters | Δρmin = −0.24 e Å−3 |
1 restraint | Absolute structure: Flack (1983), with 892 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.07 (13) |
C11H14ClNO | V = 1152.6 (2) Å3 |
Mr = 211.68 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 10.159 (1) Å | µ = 0.30 mm−1 |
b = 10.248 (1) Å | T = 302 K |
c = 11.071 (1) Å | 0.60 × 0.16 × 0.14 mm |
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 = 0.959 | Rint = 0.049 |
6499 measured reflections |
R[F2 > 2σ(F2)] = 0.049 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.136 | Δρmax = 0.37 e Å−3 |
S = 1.05 | Δρmin = −0.24 e Å−3 |
2261 reflections | Absolute structure: Flack (1983), with 892 Friedel pairs |
133 parameters | Absolute structure parameter: −0.07 (13) |
1 restraint |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.3757 (3) | 0.1032 (3) | 0.9165 (3) | 0.0485 (9) | |
C2 | 0.3373 (3) | 0.0764 (3) | 0.7973 (3) | 0.0529 (9) | |
C3 | 0.3577 (4) | −0.0442 (4) | 0.7466 (4) | 0.0701 (11) | |
H3 | 0.3290 | −0.0615 | 0.6684 | 0.084* | |
C4 | 0.4203 (4) | −0.1384 (4) | 0.8118 (4) | 0.0790 (12) | |
H4 | 0.4354 | −0.2197 | 0.7770 | 0.095* | |
C5 | 0.4610 (4) | −0.1155 (4) | 0.9273 (5) | 0.0776 (13) | |
H5 | 0.5042 | −0.1805 | 0.9705 | 0.093* | |
C6 | 0.4375 (4) | 0.0066 (3) | 0.9809 (4) | 0.0602 (10) | |
H6 | 0.4638 | 0.0219 | 1.0601 | 0.072* | |
C7 | 0.4429 (3) | 0.3056 (3) | 1.0162 (3) | 0.0451 (7) | |
C8 | 0.3943 (3) | 0.4347 (3) | 1.0682 (3) | 0.0533 (9) | |
C9 | 0.3016 (6) | 0.4088 (4) | 1.1719 (3) | 0.1125 (19) | |
H9A | 0.3464 | 0.3596 | 1.2331 | 0.169* | |
H9B | 0.2271 | 0.3602 | 1.1434 | 0.169* | |
H9C | 0.2723 | 0.4903 | 1.2052 | 0.169* | |
C10 | 0.3203 (5) | 0.5103 (4) | 0.9698 (4) | 0.0949 (15) | |
H10A | 0.2989 | 0.5959 | 0.9990 | 0.142* | |
H10B | 0.2407 | 0.4647 | 0.9494 | 0.142* | |
H10C | 0.3749 | 0.5176 | 0.8993 | 0.142* | |
C11 | 0.5068 (4) | 0.5190 (4) | 1.1055 (5) | 0.0958 (16) | |
H11A | 0.4737 | 0.6001 | 1.1367 | 0.144* | |
H11B | 0.5620 | 0.5359 | 1.0369 | 0.144* | |
H11C | 0.5570 | 0.4754 | 1.1669 | 0.144* | |
N1 | 0.3506 (3) | 0.2264 (3) | 0.9685 (3) | 0.0541 (7) | |
H1 | 0.2739 (15) | 0.253 (3) | 0.954 (3) | 0.065* | |
O1 | 0.5584 (2) | 0.2731 (2) | 1.0171 (3) | 0.0663 (7) | |
Cl1 | 0.26026 (11) | 0.19639 (10) | 0.71284 (8) | 0.0803 (4) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.036 (2) | 0.0512 (19) | 0.058 (2) | −0.0058 (16) | 0.0068 (18) | −0.0057 (16) |
C2 | 0.0393 (19) | 0.059 (2) | 0.061 (2) | −0.0091 (16) | 0.0096 (18) | −0.0019 (18) |
C3 | 0.059 (2) | 0.075 (3) | 0.077 (3) | −0.008 (2) | 0.008 (2) | −0.022 (2) |
C4 | 0.069 (3) | 0.063 (3) | 0.105 (4) | −0.003 (2) | 0.016 (3) | −0.031 (2) |
C5 | 0.067 (3) | 0.050 (2) | 0.116 (4) | 0.0075 (19) | 0.001 (3) | 0.004 (2) |
C6 | 0.053 (2) | 0.058 (2) | 0.071 (2) | 0.0044 (17) | 0.000 (2) | 0.002 (2) |
C7 | 0.0353 (18) | 0.0538 (18) | 0.0463 (17) | −0.0028 (18) | 0.0013 (16) | −0.0029 (18) |
C8 | 0.047 (2) | 0.0498 (19) | 0.063 (2) | −0.0012 (17) | −0.0005 (18) | −0.0107 (17) |
C9 | 0.176 (5) | 0.088 (3) | 0.073 (3) | −0.005 (3) | 0.060 (3) | −0.015 (2) |
C10 | 0.105 (3) | 0.066 (2) | 0.114 (3) | 0.022 (2) | −0.029 (3) | −0.008 (3) |
C11 | 0.071 (3) | 0.074 (3) | 0.143 (4) | 0.004 (2) | −0.022 (3) | −0.034 (3) |
N1 | 0.0377 (15) | 0.0533 (16) | 0.0713 (17) | 0.0076 (14) | −0.0047 (16) | −0.0130 (15) |
O1 | 0.0377 (13) | 0.0658 (15) | 0.0955 (17) | 0.0029 (11) | −0.0005 (14) | −0.0217 (14) |
Cl1 | 0.0859 (7) | 0.0839 (7) | 0.0712 (6) | −0.0095 (6) | −0.0137 (6) | 0.0169 (5) |
C1—C6 | 1.372 (5) | C7—C8 | 1.526 (5) |
C1—C2 | 1.404 (5) | C8—C11 | 1.491 (5) |
C1—N1 | 1.410 (4) | C8—C9 | 1.508 (5) |
C2—C3 | 1.374 (5) | C8—C10 | 1.534 (5) |
C2—Cl1 | 1.732 (3) | C9—H9A | 0.9600 |
C3—C4 | 1.363 (6) | C9—H9B | 0.9600 |
C3—H3 | 0.9300 | C9—H9C | 0.9600 |
C4—C5 | 1.365 (6) | C10—H10A | 0.9600 |
C4—H4 | 0.9300 | C10—H10B | 0.9600 |
C5—C6 | 1.405 (5) | C10—H10C | 0.9600 |
C5—H5 | 0.9300 | C11—H11A | 0.9600 |
C6—H6 | 0.9300 | C11—H11B | 0.9600 |
C7—O1 | 1.219 (4) | C11—H11C | 0.9600 |
C7—N1 | 1.348 (4) | N1—H1 | 0.841 (10) |
C6—C1—C2 | 118.3 (3) | C11—C8—C10 | 106.2 (3) |
C6—C1—N1 | 121.1 (3) | C9—C8—C10 | 108.9 (3) |
C2—C1—N1 | 120.6 (3) | C7—C8—C10 | 109.2 (3) |
C3—C2—C1 | 121.2 (3) | C8—C9—H9A | 109.5 |
C3—C2—Cl1 | 119.1 (3) | C8—C9—H9B | 109.5 |
C1—C2—Cl1 | 119.6 (2) | H9A—C9—H9B | 109.5 |
C4—C3—C2 | 119.4 (4) | C8—C9—H9C | 109.5 |
C4—C3—H3 | 120.3 | H9A—C9—H9C | 109.5 |
C2—C3—H3 | 120.3 | H9B—C9—H9C | 109.5 |
C3—C4—C5 | 121.0 (4) | C8—C10—H10A | 109.5 |
C3—C4—H4 | 119.5 | C8—C10—H10B | 109.5 |
C5—C4—H4 | 119.5 | H10A—C10—H10B | 109.5 |
C4—C5—C6 | 119.9 (4) | C8—C10—H10C | 109.5 |
C4—C5—H5 | 120.1 | H10A—C10—H10C | 109.5 |
C6—C5—H5 | 120.1 | H10B—C10—H10C | 109.5 |
C1—C6—C5 | 120.1 (4) | C8—C11—H11A | 109.5 |
C1—C6—H6 | 120.0 | C8—C11—H11B | 109.5 |
C5—C6—H6 | 120.0 | H11A—C11—H11B | 109.5 |
O1—C7—N1 | 120.5 (3) | C8—C11—H11C | 109.5 |
O1—C7—C8 | 123.1 (3) | H11A—C11—H11C | 109.5 |
N1—C7—C8 | 116.4 (3) | H11B—C11—H11C | 109.5 |
C11—C8—C9 | 111.7 (4) | C7—N1—C1 | 125.0 (3) |
C11—C8—C7 | 111.0 (3) | C7—N1—H1 | 122 (2) |
C9—C8—C7 | 109.7 (3) | C1—N1—H1 | 112 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.84 (1) | 2.23 (2) | 2.973 (3) | 148 (3) |
Symmetry code: (i) x−1/2, −y+1/2, −z+2. |
Experimental details
Crystal data | |
Chemical formula | C11H14ClNO |
Mr | 211.68 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 302 |
a, b, c (Å) | 10.159 (1), 10.248 (1), 11.071 (1) |
V (Å3) | 1152.6 (2) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.30 |
Crystal size (mm) | 0.60 × 0.16 × 0.14 |
Data collection | |
Diffractometer | Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector |
Absorption correction | Analytical (CrysAlis RED; Oxford Diffraction, 2006) using a multifaceted crystal model (Clark & Reid, 1995) |
Tmin, Tmax | 0.840, 0.959 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6499, 2261, 1279 |
Rint | 0.049 |
(sin θ/λ)max (Å−1) | 0.625 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.049, 0.136, 1.05 |
No. of reflections | 2261 |
No. of parameters | 133 |
No. of restraints | 1 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.37, −0.24 |
Absolute structure | Flack (1983), with 892 Friedel pairs |
Absolute structure parameter | −0.07 (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.
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.841 (10) | 2.23 (2) | 2.973 (3) | 148 (3) |
Symmetry code: (i) x−1/2, −y+1/2, −z+2. |
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).