N-(4-Chloro-phen-yl)-4-methyl-piperidine-1-carboxamide.

In the title compound, C(13)H(17)ClN(2)O, the piperidine ring adopts a chair conformation and the N atom in that ring is close to pyramidal (bond angle sum = 357.5°). In the crystal, mol-ecules are linked into C(4) chains propagating in [010] by N-H⋯O hydrogen bonds.

Related literature

For a related structure, see: Köhn et al. (2004 ▶).

Experimental

Crystal data

C13H17ClN2O

M = 252.74

Monoclinic,

a = 13.286 (3) Å

b = 9.1468 (18) Å

c = 10.957 (2) Å

β = 95.36 (3)°

V = 1325.7 (5) Å3

Z = 4

Mo Kα radiation

μ = 0.28 mm−1

T = 293 K

0.22 × 0.21 × 0.19 mm

Data collection

Bruker SMART CCD diffractometer

12608 measured reflections

3038 independent reflections

1999 reflections with I > 2σ(I)

R int = 0.037

Refinement

R[F 2 > 2σ(F 2)] = 0.045

wR(F 2) = 0.154

S = 1.13

3038 reflections

154 parameters

H-atom parameters constrained

Δρmax = 0.34 e Å−3

Δρmin = −0.37 e Å−3

Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAINT; 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: SHELXTL.

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811024123/hb5902sup1.cif

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811024123/hb5902Isup2.hkl

Supplementary material file. DOI: 10.1107/S1600536811024123/hb5902Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

C13H17ClN2O	F(000) = 536
Mr = 252.74	Dx = 1.266 Mg m−3
Monoclinic, P21/c	Mo Kα radiation, λ = 0.71073 Å
a = 13.286 (3) Å	Cell parameters from 1999 reflections
b = 9.1468 (18) Å	θ = 3.0–27.3°
c = 10.957 (2) Å	µ = 0.28 mm−1
β = 95.36 (3)°	T = 293 K
V = 1325.7 (5) Å3	Bar, colorless
Z = 4	0.22 × 0.21 × 0.19 mm

Bruker SMART CCD diffractometer	1999 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube	Rint = 0.037
graphite	θmax = 27.5°, θmin = 3.1°
φ and ω scans	h = −17→17
12608 measured reflections	k = −10→11
3038 independent reflections	l = −14→14

Refinement on F2	Primary atom site location: structure-invariant direct methods
Least-squares matrix: full	Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045	Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.154	H-atom parameters constrained
S = 1.13	w = 1/[σ2(Fo2) + (0.0806P)2 + 0.0785P] where P = (Fo2 + 2Fc2)/3
3038 reflections	(Δ/σ)max = 0.001
154 parameters	Δρmax = 0.34 e Å−3
0 restraints	Δρmin = −0.37 e Å−3

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.

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 > 2sigma(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
Cl1	0.83830 (4)	0.11364 (7)	0.42550 (6)	0.0690 (2)
O1	0.44390 (10)	0.14454 (13)	0.73592 (13)	0.0484 (4)
C8	0.57283 (13)	0.30099 (18)	0.59955 (16)	0.0379 (4)
N2	0.49079 (11)	0.36204 (15)	0.65583 (15)	0.0432 (4)
H2A	0.4793	0.4543	0.6491	0.052*
C12	0.63981 (15)	0.1297 (2)	0.46199 (18)	0.0452 (5)
H12A	0.6304	0.0526	0.4067	0.054*
C13	0.55876 (14)	0.1876 (2)	0.51610 (17)	0.0436 (4)
H13A	0.4943	0.1500	0.4963	0.052*
N1	0.35363 (11)	0.34976 (16)	0.77039 (16)	0.0447 (4)
C9	0.66864 (14)	0.35849 (19)	0.62681 (18)	0.0421 (4)
H9A	0.6783	0.4356	0.6820	0.051*
C11	0.73497 (14)	0.1877 (2)	0.49098 (17)	0.0436 (4)
C7	0.42888 (13)	0.27715 (18)	0.72121 (16)	0.0385 (4)
C10	0.75036 (14)	0.3019 (2)	0.57244 (17)	0.0447 (4)
H10A	0.8147	0.3406	0.5908	0.054*
C6	0.30658 (13)	0.48409 (19)	0.71993 (19)	0.0473 (5)
H6A	0.3479	0.5258	0.6603	0.057*
H6B	0.3021	0.5549	0.7851	0.057*
C2	0.29344 (15)	0.2735 (2)	0.85563 (19)	0.0485 (5)
H2B	0.2864	0.3352	0.9264	0.058*
H2C	0.3281	0.1847	0.8840	0.058*
C4	0.13554 (16)	0.3713 (3)	0.7433 (2)	0.0639 (6)
H4A	0.1244	0.4363	0.8119	0.077*
C5	0.20188 (15)	0.4518 (3)	0.6593 (2)	0.0567 (5)
H5A	0.2079	0.3931	0.5866	0.068*
H5B	0.1694	0.5431	0.6335	0.068*
C3	0.19038 (16)	0.2355 (3)	0.7956 (2)	0.0587 (6)
H3A	0.1508	0.1902	0.8554	0.070*
H3B	0.1971	0.1657	0.7302	0.070*
C1	0.0326 (2)	0.3348 (5)	0.6765 (4)	0.1222 (14)
H1A	0.0004	0.4231	0.6459	0.183*
H1B	−0.0088	0.2881	0.7323	0.183*
H1C	0.0415	0.2701	0.6094	0.183*

	U11	U22	U33	U12	U13	U23
Cl1	0.0609 (4)	0.0796 (5)	0.0696 (4)	0.0091 (3)	0.0222 (3)	−0.0124 (3)
O1	0.0568 (8)	0.0314 (6)	0.0577 (8)	0.0031 (6)	0.0080 (7)	0.0042 (6)
C8	0.0391 (9)	0.0341 (9)	0.0402 (9)	0.0000 (7)	0.0026 (7)	0.0040 (7)
N2	0.0428 (8)	0.0294 (7)	0.0585 (10)	0.0012 (6)	0.0104 (7)	0.0010 (7)
C12	0.0547 (11)	0.0415 (10)	0.0392 (10)	−0.0005 (8)	0.0029 (9)	−0.0049 (8)
C13	0.0443 (10)	0.0431 (10)	0.0418 (10)	−0.0047 (8)	−0.0034 (8)	−0.0020 (8)
N1	0.0400 (8)	0.0375 (8)	0.0575 (10)	0.0021 (6)	0.0089 (7)	0.0060 (7)
C9	0.0454 (10)	0.0371 (9)	0.0439 (10)	−0.0064 (8)	0.0044 (8)	−0.0028 (8)
C11	0.0473 (10)	0.0453 (10)	0.0389 (9)	0.0021 (8)	0.0082 (8)	0.0028 (8)
C7	0.0400 (9)	0.0340 (9)	0.0406 (9)	−0.0016 (7)	0.0002 (8)	−0.0005 (7)
C10	0.0406 (9)	0.0485 (11)	0.0453 (10)	−0.0060 (8)	0.0053 (8)	−0.0011 (8)
C6	0.0474 (10)	0.0351 (9)	0.0600 (12)	0.0049 (8)	0.0080 (9)	0.0012 (8)
C2	0.0516 (11)	0.0455 (10)	0.0496 (11)	−0.0007 (9)	0.0109 (9)	0.0035 (9)
C4	0.0430 (11)	0.0858 (17)	0.0633 (14)	−0.0028 (11)	0.0065 (10)	0.0013 (12)
C5	0.0482 (11)	0.0655 (13)	0.0561 (12)	0.0051 (10)	0.0030 (10)	0.0064 (11)
C3	0.0559 (12)	0.0610 (13)	0.0609 (13)	−0.0165 (10)	0.0141 (10)	0.0005 (10)
C1	0.0510 (15)	0.184 (4)	0.128 (3)	−0.027 (2)	−0.0114 (18)	0.031 (3)

Cl1—C11	1.7441 (19)	C6—C5	1.514 (3)
O1—C7	1.237 (2)	C6—H6A	0.9700
C8—C9	1.384 (2)	C6—H6B	0.9700
C8—C13	1.384 (2)	C2—C3	1.503 (3)
C8—N2	1.416 (2)	C2—H2B	0.9700
N2—C7	1.379 (2)	C2—H2C	0.9700
N2—H2A	0.8600	C4—C5	1.522 (3)
C12—C11	1.381 (3)	C4—C3	1.524 (3)
C12—C13	1.382 (3)	C4—C1	1.526 (3)
C12—H12A	0.9300	C4—H4A	0.9800
C13—H13A	0.9300	C5—H5A	0.9700
N1—C7	1.353 (2)	C5—H5B	0.9700
N1—C2	1.462 (2)	C3—H3A	0.9700
N1—C6	1.463 (2)	C3—H3B	0.9700
C9—C10	1.386 (3)	C1—H1A	0.9600
C9—H9A	0.9300	C1—H1B	0.9600
C11—C10	1.377 (3)	C1—H1C	0.9600
C10—H10A	0.9300
C9—C8—C13	119.49 (16)	H6A—C6—H6B	108.1
C9—C8—N2	119.08 (16)	N1—C2—C3	111.16 (17)
C13—C8—N2	121.42 (16)	N1—C2—H2B	109.4
C7—N2—C8	121.65 (14)	C3—C2—H2B	109.4
C7—N2—H2A	119.2	N1—C2—H2C	109.4
C8—N2—H2A	119.2	C3—C2—H2C	109.4
C11—C12—C13	119.19 (17)	H2B—C2—H2C	108.0
C11—C12—H12A	120.4	C5—C4—C3	109.76 (18)
C13—C12—H12A	120.4	C5—C4—C1	111.1 (2)
C12—C13—C8	120.52 (17)	C3—C4—C1	112.2 (2)
C12—C13—H13A	119.7	C5—C4—H4A	107.9
C8—C13—H13A	119.7	C3—C4—H4A	107.9
C7—N1—C2	119.25 (15)	C1—C4—H4A	107.9
C7—N1—C6	124.54 (16)	C6—C5—C4	112.92 (18)
C2—N1—C6	113.70 (15)	C6—C5—H5A	109.0
C8—C9—C10	120.46 (17)	C4—C5—H5A	109.0
C8—C9—H9A	119.8	C6—C5—H5B	109.0
C10—C9—H9A	119.8	C4—C5—H5B	109.0
C10—C11—C12	121.20 (17)	H5A—C5—H5B	107.8
C10—C11—Cl1	119.10 (15)	C2—C3—C4	111.12 (19)
C12—C11—Cl1	119.69 (14)	C2—C3—H3A	109.4
O1—C7—N1	123.05 (16)	C4—C3—H3A	109.4
O1—C7—N2	121.51 (16)	C2—C3—H3B	109.4
N1—C7—N2	115.41 (15)	C4—C3—H3B	109.4
C11—C10—C9	119.13 (17)	H3A—C3—H3B	108.0
C11—C10—H10A	120.4	C4—C1—H1A	109.5
C9—C10—H10A	120.4	C4—C1—H1B	109.5
N1—C6—C5	110.16 (16)	H1A—C1—H1B	109.5
N1—C6—H6A	109.6	C4—C1—H1C	109.5
C5—C6—H6A	109.6	H1A—C1—H1C	109.5
N1—C6—H6B	109.6	H1B—C1—H1C	109.5
C5—C6—H6B	109.6

D—H···A	D—H	H···A	D···A	D—H···A
N2—H2A···O1i	0.86	2.33	2.940 (2)	128

Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N2—H2A⋯O1i	0.86	2.33	2.940 (2)	128

Symmetry code: (i) .