N-Cyclo-hexyl-pyrrolidine-1-carbothio-amide.

In the title mol-ecule, C(11)H(20)N(2)S, the five-membered ring has an envelope conformation and the cyclo-hexane ring is in a chair conformation. The N-H group is not involved in any intra- or inter-molecular inter-actions.

Related literature

For the medicinal properties of pyrrolidine compounds, see: Yang et al. (1997 ▶). For related structures, see: Köhn et al. (2004 ▶); Li (2011 ▶).

Experimental

Crystal data

C11H20N2S

M = 212.35

Orthorhombic,

a = 9.3808 (19) Å

b = 10.925 (2) Å

c = 23.540 (5) Å

V = 2412.6 (8) Å3

Z = 8

Mo Kα radiation

μ = 0.24 mm−1

T = 293 K

0.22 × 0.20 × 0.18 mm

Data collection

Bruker SMART CCD diffractometer

22078 measured reflections

2766 independent reflections

1700 reflections with I > 2σ(I)

R int = 0.046

Refinement

R[F 2 > 2σ(F 2)] = 0.053

wR(F 2) = 0.190

S = 1.18

2766 reflections

127 parameters

H-atom parameters constrained

Δρmax = 0.25 e Å−3

Δρmin = −0.35 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/S1600536812012627/lh5439sup1.cif

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812012627/lh5439Isup2.hkl

Supplementary material file. DOI: 10.1107/S1600536812012627/lh5439Isup3.cml

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

C11H20N2S	F(000) = 928
Mr = 212.35	Dx = 1.169 Mg m−3
Orthorhombic, Pbca	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2ab	Cell parameters from 1700 reflections
a = 9.3808 (19) Å	θ = 3.4–27.5°
b = 10.925 (2) Å	µ = 0.24 mm−1
c = 23.540 (5) Å	T = 293 K
V = 2412.6 (8) Å3	Block, colorless
Z = 8	0.22 × 0.20 × 0.18 mm

Bruker SMART CCD diffractometer	1700 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube	Rint = 0.046
Graphite monochromator	θmax = 27.5°, θmin = 3.4°
φ and ω scans	h = −12→12
22078 measured reflections	k = −13→14
2766 independent reflections	l = −30→30

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)] = 0.053	Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.190	H-atom parameters constrained
S = 1.18	w = 1/[σ2(Fo2) + (0.1021P)2] where P = (Fo2 + 2Fc2)/3
2766 reflections	(Δ/σ)max < 0.001
127 parameters	Δρmax = 0.25 e Å−3
0 restraints	Δρmin = −0.35 e Å−3

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
S1	0.07717 (8)	0.34275 (5)	0.16033 (2)	0.0727 (3)
N2	0.1756 (2)	0.57053 (15)	0.14966 (7)	0.0649 (5)
H2A	0.2105	0.6354	0.1650	0.078*
N1	0.1569 (2)	0.49963 (16)	0.24023 (7)	0.0625 (5)
C5	0.1402 (2)	0.47798 (18)	0.18465 (8)	0.0533 (5)
C6	0.1600 (2)	0.57042 (18)	0.08782 (8)	0.0565 (6)
H6A	0.0941	0.5046	0.0773	0.068*
C7	0.3007 (3)	0.54772 (19)	0.05863 (8)	0.0604 (6)
H7A	0.3378	0.4686	0.0701	0.072*
H7B	0.3687	0.6098	0.0702	0.072*
C9	0.2197 (3)	0.6700 (2)	−0.02522 (9)	0.0637 (6)
H9A	0.2865	0.7359	−0.0179	0.076*
H9B	0.2032	0.6664	−0.0659	0.076*
C10	0.0817 (2)	0.6969 (2)	0.00449 (10)	0.0647 (6)
H10A	0.0103	0.6382	−0.0076	0.078*
H10B	0.0490	0.7778	−0.0064	0.078*
C11	0.0964 (2)	0.6912 (2)	0.06890 (10)	0.0657 (6)
H11A	0.1569	0.7578	0.0817	0.079*
H11B	0.0034	0.7015	0.0862	0.079*
C8	0.2838 (3)	0.5505 (2)	−0.00562 (8)	0.0655 (6)
H8A	0.3763	0.5396	−0.0233	0.079*
H8B	0.2230	0.4834	−0.0175	0.079*
C4	0.2130 (3)	0.6141 (2)	0.26409 (9)	0.0751 (7)
H4A	0.1503	0.6824	0.2557	0.090*
H4B	0.3073	0.6319	0.2493	0.090*
C3	0.2184 (4)	0.5887 (3)	0.32761 (10)	0.0947 (10)
H3A	0.3120	0.5596	0.3388	0.114*
H3B	0.1960	0.6619	0.3492	0.114*
C2	0.1095 (5)	0.4934 (3)	0.33665 (10)	0.1053 (11)
H2B	0.0163	0.5302	0.3418	0.126*
H2C	0.1320	0.4451	0.3700	0.126*
C1	0.1110 (4)	0.4151 (3)	0.28475 (9)	0.0917 (9)
H1A	0.1776	0.3477	0.2888	0.110*
H1B	0.0169	0.3826	0.2768	0.110*

	U11	U22	U33	U12	U13	U23
S1	0.1120 (6)	0.0526 (4)	0.0536 (4)	−0.0127 (3)	−0.0018 (3)	−0.0005 (2)
N2	0.0950 (14)	0.0592 (11)	0.0406 (9)	−0.0187 (10)	0.0007 (8)	−0.0041 (7)
N1	0.0922 (14)	0.0560 (10)	0.0393 (9)	0.0013 (9)	0.0052 (9)	−0.0024 (7)
C5	0.0651 (13)	0.0519 (11)	0.0429 (10)	0.0033 (9)	0.0023 (9)	−0.0004 (8)
C6	0.0732 (14)	0.0557 (12)	0.0408 (10)	−0.0137 (10)	−0.0010 (9)	−0.0014 (8)
C7	0.0765 (14)	0.0565 (12)	0.0482 (11)	0.0150 (10)	−0.0002 (10)	0.0070 (9)
C9	0.0625 (14)	0.0741 (14)	0.0545 (12)	−0.0005 (10)	−0.0019 (10)	0.0182 (10)
C10	0.0600 (14)	0.0720 (14)	0.0620 (13)	0.0034 (11)	−0.0089 (10)	0.0097 (11)
C11	0.0650 (14)	0.0706 (14)	0.0617 (13)	0.0093 (11)	0.0000 (10)	−0.0031 (11)
C8	0.0774 (15)	0.0722 (14)	0.0468 (11)	0.0104 (12)	0.0073 (10)	0.0057 (10)
C4	0.1016 (19)	0.0753 (14)	0.0484 (12)	−0.0030 (14)	−0.0013 (12)	−0.0143 (11)
C3	0.139 (3)	0.096 (2)	0.0492 (13)	0.0122 (19)	−0.0130 (15)	−0.0142 (12)
C2	0.155 (3)	0.119 (3)	0.0421 (14)	0.003 (2)	0.0090 (15)	0.0021 (14)
C1	0.156 (3)	0.0742 (17)	0.0452 (13)	−0.0016 (16)	0.0119 (14)	0.0066 (11)

S1—C5	1.691 (2)	C10—H10A	0.9700
N2—C5	1.346 (3)	C10—H10B	0.9700
N2—C6	1.463 (2)	C11—H11A	0.9700
N2—H2A	0.8600	C11—H11B	0.9700
N1—C5	1.339 (3)	C8—H8A	0.9700
N1—C1	1.462 (3)	C8—H8B	0.9700
N1—C4	1.469 (3)	C4—C3	1.522 (3)
C6—C7	1.509 (3)	C4—H4A	0.9700
C6—C11	1.515 (3)	C4—H4B	0.9700
C6—H6A	0.9800	C3—C2	1.475 (4)
C7—C8	1.521 (3)	C3—H3A	0.9700
C7—H7A	0.9700	C3—H3B	0.9700
C7—H7B	0.9700	C2—C1	1.491 (4)
C9—C10	1.500 (3)	C2—H2B	0.9700
C9—C8	1.510 (3)	C2—H2C	0.9700
C9—H9A	0.9700	C1—H1A	0.9700
C9—H9B	0.9700	C1—H1B	0.9700
C10—C11	1.524 (3)
C5—N2—C6	125.71 (17)	C10—C11—H11A	109.4
C5—N2—H2A	117.1	C6—C11—H11B	109.4
C6—N2—H2A	117.1	C10—C11—H11B	109.4
C5—N1—C1	123.67 (19)	H11A—C11—H11B	108.0
C5—N1—C4	124.49 (18)	C9—C8—C7	111.29 (18)
C1—N1—C4	111.69 (18)	C9—C8—H8A	109.4
N1—C5—N2	115.87 (18)	C7—C8—H8A	109.4
N1—C5—S1	121.75 (16)	C9—C8—H8B	109.4
N2—C5—S1	122.37 (15)	C7—C8—H8B	109.4
N2—C6—C7	111.45 (17)	H8A—C8—H8B	108.0
N2—C6—C11	109.34 (16)	N1—C4—C3	103.42 (19)
C7—C6—C11	110.72 (16)	N1—C4—H4A	111.1
N2—C6—H6A	108.4	C3—C4—H4A	111.1
C7—C6—H6A	108.4	N1—C4—H4B	111.1
C11—C6—H6A	108.4	C3—C4—H4B	111.1
C6—C7—C8	110.99 (18)	H4A—C4—H4B	109.0
C6—C7—H7A	109.4	C2—C3—C4	104.3 (2)
C8—C7—H7A	109.4	C2—C3—H3A	110.9
C6—C7—H7B	109.4	C4—C3—H3A	110.9
C8—C7—H7B	109.4	C2—C3—H3B	110.9
H7A—C7—H7B	108.0	C4—C3—H3B	110.9
C10—C9—C8	111.75 (18)	H3A—C3—H3B	108.9
C10—C9—H9A	109.3	C3—C2—C1	106.3 (2)
C8—C9—H9A	109.3	C3—C2—H2B	110.5
C10—C9—H9B	109.3	C1—C2—H2B	110.5
C8—C9—H9B	109.3	C3—C2—H2C	110.5
H9A—C9—H9B	107.9	C1—C2—H2C	110.5
C9—C10—C11	112.17 (18)	H2B—C2—H2C	108.7
C9—C10—H10A	109.2	N1—C1—C2	103.2 (2)
C11—C10—H10A	109.2	N1—C1—H1A	111.1
C9—C10—H10B	109.2	C2—C1—H1A	111.1
C11—C10—H10B	109.2	N1—C1—H1B	111.1
H10A—C10—H10B	107.9	C2—C1—H1B	111.1
C6—C11—C10	111.34 (18)	H1A—C1—H1B	109.1
C6—C11—H11A	109.4