Bis(benzyl-sulfan-yl)methane.

In the title compound, C(15)H(16)S(2), the structure of the dithioalkyl chain is a helix with an all-cis conformation. The dihedral angle between the mean planes of the terminal aromatic rings is 74.60 (4)°. In the crystal structure, weak C-H⋯π inter-actions contribute to the stabilization of the packing.

Related literature

For the synthesis of the title ligand, see: Cohen et al. (1980 ▶). For related structures, see: Li et al. (2005 ▶); Tanaka & Ajiki (2005 ▶).

Experimental

Crystal data

C15H16S2

M = 260.40

Monoclinic,

a = 5.5146 (1) Å

b = 12.2628 (3) Å

c = 20.0128 (5) Å

β = 101.156 (1)°

V = 1327.78 (5) Å3

Z = 4

Mo Kα radiation

μ = 0.38 mm−1

T = 173 K

0.22 × 0.15 × 0.15 mm

Data collection

Bruker APEXII CCD diffractometer

Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.922, T max = 0.946

12942 measured reflections

3335 independent reflections

2977 reflections with I > 2σ(I)

R int = 0.033

Refinement

R[F 2 > 2σ(F 2)] = 0.031

wR(F 2) = 0.082

S = 1.04

3335 reflections

155 parameters

H-atom parameters constrained

Δρmax = 0.30 e Å−3

Δρmin = −0.29 e Å−3

Data collection: APEX2 (Bruker, 2006 ▶); cell refinement: SAINT (Bruker, 2006 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL and DIAMOND (Brandenburg, 1998 ▶); software used to prepare material for publication: SHELXTL.

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810019641/sj5008sup1.cif

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810019641/sj5008Isup2.hkl

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

C15H16S2	F(000) = 552
Mr = 260.40	Dx = 1.303 Mg m−3
Monoclinic, P21/c	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc	Cell parameters from 7825 reflections
a = 5.5146 (1) Å	θ = 2.7–28.4°
b = 12.2628 (3) Å	µ = 0.38 mm−1
c = 20.0128 (5) Å	T = 173 K
β = 101.156 (1)°	Block, colourless
V = 1327.78 (5) Å3	0.22 × 0.15 × 0.15 mm
Z = 4

Bruker APEXII CCD diffractometer	3335 independent reflections
Radiation source: fine-focus sealed tube	2977 reflections with I > 2σ(I)
graphite	Rint = 0.033
Detector resolution: 10.0 pixels mm-1	θmax = 28.4°, θmin = 2.0°
φ and ω scans	h = −7→7
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)	k = −12→16
Tmin = 0.922, Tmax = 0.946	l = −24→26
12942 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)] = 0.031	H-atom parameters constrained
wR(F2) = 0.082	w = 1/[σ2(Fo2) + (0.0369P)2 + 0.4363P] where P = (Fo2 + 2Fc2)/3
S = 1.04	(Δ/σ)max < 0.001
3335 reflections	Δρmax = 0.30 e Å−3
155 parameters	Δρmin = −0.29 e Å−3
0 restraints	Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods	Extinction coefficient: 0.030 (2)

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 > 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	0.63212 (6)	0.46872 (3)	0.430321 (16)	0.03123 (10)
S2	0.80471 (6)	0.43167 (3)	0.294901 (16)	0.03327 (11)
C1	0.7958 (2)	0.73297 (11)	0.47700 (6)	0.0318 (3)
H1	0.6990	0.7130	0.5095	0.038*
C2	0.9857 (3)	0.80750 (11)	0.49456 (7)	0.0369 (3)
H2	1.0197	0.8377	0.5391	0.044*
C3	1.1262 (3)	0.83815 (11)	0.44745 (8)	0.0376 (3)
H3	1.2579	0.8887	0.4597	0.045*
C4	1.0740 (3)	0.79496 (11)	0.38253 (7)	0.0371 (3)
H4	1.1678	0.8170	0.3498	0.045*
C5	0.8848 (2)	0.71936 (11)	0.36495 (6)	0.0324 (3)
H5	0.8508	0.6897	0.3203	0.039*
C6	0.7447 (2)	0.68671 (10)	0.41215 (6)	0.0269 (2)
C7	0.5451 (2)	0.60237 (11)	0.39470 (7)	0.0319 (3)
H7A	0.4995	0.5959	0.3445	0.038*
H7B	0.3970	0.6276	0.4114	0.038*
C8	0.8761 (2)	0.43180 (11)	0.38662 (7)	0.0303 (3)
H8A	0.9344	0.3579	0.4019	0.036*
H8B	1.0158	0.4826	0.4014	0.036*
C9	0.5351 (2)	0.34398 (11)	0.27868 (6)	0.0320 (3)
H9A	0.3992	0.3808	0.2956	0.038*
H9B	0.4822	0.3351	0.2288	0.038*
C10	0.5717 (2)	0.23235 (10)	0.31064 (6)	0.0263 (2)
C11	0.7532 (2)	0.16136 (11)	0.29690 (6)	0.0309 (3)
H11	0.8598	0.1839	0.2675	0.037*
C12	0.7799 (2)	0.05829 (11)	0.32574 (7)	0.0327 (3)
H12	0.9041	0.0106	0.3158	0.039*
C13	0.6268 (2)	0.02439 (11)	0.36880 (7)	0.0324 (3)
H13	0.6452	−0.0463	0.3885	0.039*
C14	0.4464 (3)	0.09429 (11)	0.38292 (7)	0.0344 (3)
H14	0.3406	0.0716	0.4125	0.041*
C15	0.4196 (2)	0.19762 (11)	0.35389 (7)	0.0307 (3)
H15	0.2951	0.2451	0.3639	0.037*

	U11	U22	U33	U12	U13	U23
S1	0.03604 (18)	0.02830 (18)	0.03133 (17)	−0.00231 (12)	0.01147 (13)	−0.00010 (12)
S2	0.04070 (19)	0.02943 (18)	0.03283 (17)	−0.00462 (13)	0.01497 (13)	0.00064 (12)
C1	0.0353 (6)	0.0333 (7)	0.0270 (6)	−0.0013 (5)	0.0064 (5)	0.0029 (5)
C2	0.0422 (7)	0.0336 (7)	0.0322 (6)	−0.0033 (6)	0.0008 (5)	0.0007 (5)
C3	0.0336 (7)	0.0275 (7)	0.0505 (8)	−0.0018 (5)	0.0048 (6)	0.0079 (6)
C4	0.0395 (7)	0.0316 (7)	0.0445 (7)	0.0056 (6)	0.0185 (6)	0.0113 (6)
C5	0.0390 (7)	0.0293 (6)	0.0299 (6)	0.0089 (5)	0.0093 (5)	0.0039 (5)
C6	0.0270 (6)	0.0240 (6)	0.0285 (5)	0.0060 (5)	0.0026 (4)	0.0028 (4)
C7	0.0269 (6)	0.0302 (6)	0.0368 (6)	0.0046 (5)	0.0018 (5)	−0.0015 (5)
C8	0.0263 (6)	0.0291 (6)	0.0349 (6)	0.0019 (5)	0.0042 (5)	0.0005 (5)
C9	0.0345 (6)	0.0295 (6)	0.0302 (6)	−0.0001 (5)	0.0019 (5)	0.0020 (5)
C10	0.0264 (5)	0.0257 (6)	0.0251 (5)	−0.0019 (5)	0.0009 (4)	−0.0029 (4)
C11	0.0309 (6)	0.0340 (7)	0.0288 (6)	−0.0006 (5)	0.0085 (5)	−0.0032 (5)
C12	0.0320 (6)	0.0297 (6)	0.0359 (6)	0.0043 (5)	0.0051 (5)	−0.0072 (5)
C13	0.0355 (6)	0.0231 (6)	0.0364 (6)	−0.0019 (5)	0.0011 (5)	−0.0015 (5)
C14	0.0347 (7)	0.0305 (7)	0.0399 (7)	−0.0041 (5)	0.0120 (5)	0.0012 (5)
C15	0.0277 (6)	0.0281 (6)	0.0374 (6)	0.0011 (5)	0.0087 (5)	−0.0027 (5)

S1—C8	1.7988 (13)	C7—H7B	0.9900
S1—C7	1.8144 (14)	C8—H8A	0.9900
S2—C8	1.8013 (13)	C8—H8B	0.9900
S2—C9	1.8125 (14)	C9—C10	1.5079 (17)
C1—C2	1.3831 (19)	C9—H9A	0.9900
C1—C6	1.3942 (17)	C9—H9B	0.9900
C1—H1	0.9500	C10—C15	1.3841 (18)
C2—C3	1.383 (2)	C10—C11	1.3934 (18)
C2—H2	0.9500	C11—C12	1.3854 (19)
C3—C4	1.381 (2)	C11—H11	0.9500
C3—H3	0.9500	C12—C13	1.382 (2)
C4—C5	1.389 (2)	C12—H12	0.9500
C4—H4	0.9500	C13—C14	1.383 (2)
C5—C6	1.3898 (18)	C13—H13	0.9500
C5—H5	0.9500	C14—C15	1.3899 (19)
C6—C7	1.5016 (18)	C14—H14	0.9500
C7—H7A	0.9900	C15—H15	0.9500
C8—S1—C7	101.67 (6)	S2—C8—H8A	108.0
C8—S2—C9	101.13 (6)	S1—C8—H8B	108.0
C2—C1—C6	120.80 (12)	S2—C8—H8B	108.0
C2—C1—H1	119.6	H8A—C8—H8B	107.2
C6—C1—H1	119.6	C10—C9—S2	115.14 (9)
C1—C2—C3	120.19 (13)	C10—C9—H9A	108.5
C1—C2—H2	119.9	S2—C9—H9A	108.5
C3—C2—H2	119.9	C10—C9—H9B	108.5
C4—C3—C2	119.65 (13)	S2—C9—H9B	108.5
C4—C3—H3	120.2	H9A—C9—H9B	107.5
C2—C3—H3	120.2	C15—C10—C11	118.46 (12)
C3—C4—C5	120.26 (13)	C15—C10—C9	119.80 (11)
C3—C4—H4	119.9	C11—C10—C9	121.73 (11)
C5—C4—H4	119.9	C12—C11—C10	120.68 (12)
C4—C5—C6	120.61 (12)	C12—C11—H11	119.7
C4—C5—H5	119.7	C10—C11—H11	119.7
C6—C5—H5	119.7	C13—C12—C11	120.38 (12)
C5—C6—C1	118.46 (12)	C13—C12—H12	119.8
C5—C6—C7	121.28 (11)	C11—C12—H12	119.8
C1—C6—C7	120.25 (12)	C12—C13—C14	119.43 (12)
C6—C7—S1	113.86 (8)	C12—C13—H13	120.3
C6—C7—H7A	108.8	C14—C13—H13	120.3
S1—C7—H7A	108.8	C13—C14—C15	120.14 (13)
C6—C7—H7B	108.8	C13—C14—H14	119.9
S1—C7—H7B	108.8	C15—C14—H14	119.9
H7A—C7—H7B	107.7	C10—C15—C14	120.91 (12)
S1—C8—S2	117.33 (7)	C10—C15—H15	119.5
S1—C8—H8A	108.0	C14—C15—H15	119.5
C6—C1—C2—C3	0.7 (2)	C9—S2—C8—S1	−53.62 (9)
C1—C2—C3—C4	0.8 (2)	C8—S2—C9—C10	−55.87 (11)
C2—C3—C4—C5	−1.4 (2)	S2—C9—C10—C15	123.62 (11)
C3—C4—C5—C6	0.4 (2)	S2—C9—C10—C11	−57.57 (14)
C4—C5—C6—C1	1.09 (18)	C15—C10—C11—C12	0.22 (18)
C4—C5—C6—C7	−177.97 (12)	C9—C10—C11—C12	−178.61 (11)
C2—C1—C6—C5	−1.67 (19)	C10—C11—C12—C13	−0.15 (19)
C2—C1—C6—C7	177.40 (12)	C11—C12—C13—C14	0.00 (19)
C5—C6—C7—S1	103.14 (12)	C12—C13—C14—C15	0.1 (2)
C1—C6—C7—S1	−75.91 (14)	C11—C10—C15—C14	−0.12 (18)
C8—S1—C7—C6	−64.96 (10)	C9—C10—C15—C14	178.72 (12)
C7—S1—C8—S2	−56.40 (9)	C13—C14—C15—C10	0.0 (2)

Cg is the centroid of the C1–C6 ring.

D—H···A	D—H	H···A	D···A	D—H···A
C13—H13···Cgi	0.95	2.85	3.71	151

Table 1

Hydrogen-bond geometry (Å, °)

Cg is the centroid of the C1–C6 ring.

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
C13—H13⋯Cgi	0.95	2.85	3.71	151

Symmetry code: (i) .