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The title compound, C19H21NS, is the photoproduct obtained from N-iso­propyl-N-[(E)-2-phenyl­propenyl]­thio­benz­amide. Recrystallization showed a spontaneous resolution.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100004054/qa0254sup1.cif
Contains datablocks enamid5, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100004054/qa0254Isup2.hkl
Contains datablock I

CCDC reference: 144714

Experimental top

The title compound was prepared by one of the authors (HA) in a study on photocyclization of enamides and thioamides in the solid state (Aoyama, 2000). Crystals were grown from a hexane solution.

Refinement top

X-ray intensity data were measured for +h,+k,+l (θ < 30°) and for +h,-k,-l (θ < 15°). The chiral space group and Flack parameter of 0.1 (1) suggested a spontaneous resolution of the title compound. All H-atom positional parameters were calculated geometrically and fixed with Uiso(H) = 1.2Ueq(parent atom).

Computing details top

Data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation, 1999); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); software used to prepare material for publication: TEXSAN.

2-Isopropyl-4-methyl-4-phenyl-3,4-dihydro-2H-isoquinoline-1-thione top
Crystal data top
C19H21NSDx = 1.204 Mg m3
Mr = 295.44Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 25 reflections
a = 11.166 (1) Åθ = 14.0–14.8°
b = 13.423 (1) ŵ = 0.19 mm1
c = 10.878 (1) ÅT = 298 K
V = 1630.4 (2) Å3Prism, yellow
Z = 40.55 × 0.4 × 0.3 mm
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.006
θ–2θ scansθmax = 30.0°, θmin = 2.5°
Absorption correction: integration
(Coppens et al., 1965)
h = 016
Tmin = 0.928, Tmax = 0.947k = 1019
3090 measured reflectionsl = 816
2684 independent reflections3 standard reflections every 150 reflections
1963 reflections with I > 2σ(I) intensity decay: none
Refinement top
Refinement on F2 w = 1/[σ2(Fo2) + (0.0601P)2 + 0.1846P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.043(Δ/σ)max = 0.001
wR(F2) = 0.124Δρmax = 0.15 e Å3
S = 1.06Δρmin = 0.27 e Å3
2684 reflectionsAbsolute structure: Flack (1983), no Friedel pairs
190 parametersAbsolute structure parameter: 0.1 (1)
H-atom parameters not refined
Crystal data top
C19H21NSV = 1630.4 (2) Å3
Mr = 295.44Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 11.166 (1) ŵ = 0.19 mm1
b = 13.423 (1) ÅT = 298 K
c = 10.878 (1) Å0.55 × 0.4 × 0.3 mm
Data collection top
Rigaku AFC-7R
diffractometer
1963 reflections with I > 2σ(I)
Absorption correction: integration
(Coppens et al., 1965)
Rint = 0.006
Tmin = 0.928, Tmax = 0.9473 standard reflections every 150 reflections
3090 measured reflections intensity decay: none
2684 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.043H-atom parameters not refined
wR(F2) = 0.124Δρmax = 0.15 e Å3
S = 1.06Δρmin = 0.27 e Å3
2684 reflectionsAbsolute structure: Flack (1983), no Friedel pairs
190 parametersAbsolute structure parameter: 0.1 (1)
Special details top

Refinement. Refinement was based on F2 against all reflections. The weighted R-factor (wR) and goodness of fit (S) were based on F2, and conventional R-factor (R) was calculated on F, with F set to zero for negative F2. The threshold expression of I > 2σ(I) was used only for calculating R-factor(gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.53579 (9)0.13551 (6)0.08369 (7)0.0790 (3)
N20.6122 (2)0.0496 (2)0.1220 (2)0.0552 (5)
C30.5208 (3)0.0816 (2)0.0550 (2)0.0533 (6)
C40.3996 (2)0.0670 (2)0.1092 (2)0.0502 (5)
C50.3052 (3)0.1315 (2)0.0786 (3)0.0663 (8)
C60.1932 (3)0.1184 (2)0.1312 (3)0.0730 (9)
C70.1721 (3)0.0401 (3)0.2103 (3)0.0703 (8)
C80.2642 (2)0.0242 (2)0.2395 (3)0.0584 (6)
C90.3790 (2)0.0111 (2)0.1922 (2)0.0475 (5)
C100.7400 (3)0.0672 (3)0.0899 (3)0.0767 (9)
C110.8042 (4)0.0294 (3)0.0652 (4)0.106 (1)
C120.8002 (3)0.1288 (3)0.1885 (5)0.106 (1)
C130.5899 (2)0.0029 (2)0.2383 (2)0.0550 (6)
C140.4845 (2)0.0755 (2)0.2269 (2)0.0489 (5)
C150.4665 (3)0.1232 (3)0.3543 (3)0.0682 (7)
C160.5105 (2)0.1557 (2)0.1302 (2)0.0511 (5)
C170.5992 (3)0.2267 (2)0.1516 (4)0.0763 (9)
C180.6243 (3)0.2995 (2)0.0665 (5)0.092 (1)
C190.5647 (4)0.3018 (2)0.0447 (5)0.088 (1)
C200.4782 (3)0.2330 (2)0.0675 (4)0.0810 (9)
C210.4501 (3)0.1606 (2)0.0186 (3)0.0616 (7)
H50.32110.18530.02050.0813*
H60.12690.16380.11460.0900*
H70.09250.02920.24710.0834*
H80.24940.07990.29630.0707*
H100.74260.10660.01610.0901*
H11A0.88450.01850.04070.1286*
H11B0.76230.06510.00070.1286*
H11C0.80190.07130.13730.1286*
H12A0.75460.18970.20410.1244*
H12B0.87980.14450.17030.1244*
H12C0.79820.09130.26760.1244*
H13A0.57340.04600.30090.0686*
H13B0.66130.03900.26070.0686*
H15A0.53650.15850.37870.0843*
H15B0.39940.16970.35080.0843*
H15C0.44760.07290.41430.0843*
H170.64350.22370.22990.0910*
H180.68310.35050.08740.1151*
H190.58650.35220.10630.1028*
H200.43570.23450.14700.1000*
H210.38520.11370.00260.0760*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.1199 (7)0.0659 (4)0.0513 (3)0.0217 (5)0.0125 (4)0.0219 (3)
N20.058 (1)0.061 (1)0.046 (1)0.017 (1)0.0051 (10)0.0136 (10)
C30.079 (2)0.0371 (9)0.043 (1)0.011 (1)0.011 (1)0.0051 (8)
C40.063 (1)0.041 (1)0.047 (1)0.000 (1)0.016 (1)0.0056 (9)
C50.092 (2)0.045 (1)0.062 (1)0.007 (1)0.030 (2)0.012 (1)
C60.070 (2)0.069 (2)0.080 (2)0.021 (2)0.027 (2)0.029 (2)
C70.055 (1)0.079 (2)0.077 (2)0.010 (2)0.008 (1)0.028 (2)
C80.053 (1)0.061 (1)0.062 (1)0.001 (1)0.000 (1)0.007 (1)
C90.049 (1)0.048 (1)0.046 (1)0.000 (1)0.005 (1)0.004 (1)
C100.069 (2)0.090 (2)0.072 (2)0.022 (2)0.007 (2)0.030 (2)
C110.095 (3)0.115 (3)0.107 (3)0.005 (2)0.049 (2)0.000 (2)
C120.074 (2)0.101 (3)0.143 (4)0.038 (2)0.012 (2)0.007 (3)
C130.053 (1)0.068 (1)0.043 (1)0.008 (1)0.006 (1)0.016 (1)
C140.049 (1)0.054 (1)0.044 (1)0.004 (1)0.000 (1)0.0141 (10)
C150.063 (2)0.088 (2)0.054 (1)0.008 (2)0.000 (1)0.029 (1)
C160.049 (1)0.043 (1)0.062 (1)0.001 (1)0.006 (1)0.0158 (10)
C170.070 (2)0.066 (2)0.093 (2)0.019 (2)0.000 (2)0.025 (2)
C180.073 (2)0.058 (2)0.144 (4)0.024 (2)0.018 (2)0.015 (2)
C190.085 (2)0.051 (2)0.127 (3)0.009 (2)0.029 (2)0.011 (2)
C200.094 (2)0.061 (2)0.088 (2)0.012 (2)0.001 (2)0.019 (2)
C210.061 (2)0.053 (1)0.070 (2)0.013 (1)0.005 (1)0.005 (1)
Geometric parameters (Å, º) top
S1—C31.681 (2)C12—H12A0.98
N2—C31.326 (3)C12—H12B0.93
N2—C101.488 (4)C12—H12C1.00
N2—C131.470 (3)C13—C141.533 (4)
C3—C41.489 (4)C13—H13A0.96
C4—C51.405 (4)C13—H13B0.96
C4—C91.402 (3)C14—C151.539 (4)
C5—C61.387 (5)C14—C161.533 (3)
C5—H50.98C15—H15A0.95
C6—C71.378 (5)C15—H15B0.98
C6—H60.98C15—H15C0.96
C7—C81.380 (4)C16—C171.394 (4)
C7—H70.99C16—C211.390 (4)
C8—C91.393 (4)C17—C181.375 (6)
C8—H80.98C17—H170.99
C9—C141.510 (3)C18—C191.381 (7)
C10—C111.505 (6)C18—H180.98
C10—C121.512 (6)C19—C201.359 (5)
C10—H100.96C19—H190.98
C11—H11A0.95C20—C211.386 (4)
C11—H11B0.98C20—H200.99
C11—H11C0.97C21—H210.98
C3—N2—C10123.9 (2)H12A—C12—H12B110
C3—N2—C13119.9 (2)H12A—C12—H12C105
C10—N2—C13116.2 (2)H12B—C12—H12C109
S1—C3—N2123.8 (2)N2—C13—C14111.5 (2)
S1—C3—C4120.2 (2)N2—C13—H13A108
N2—C3—C4116.1 (2)N2—C13—H13B109
C3—C4—C5120.5 (2)C14—C13—H13A110
C3—C4—C9120.1 (2)C14—C13—H13B110
C5—C4—C9119.4 (2)H13A—C13—H13B109
C4—C5—C6120.0 (3)C9—C14—C13104.8 (2)
C4—C5—H5118C9—C14—C15111.2 (2)
C6—C5—H5122C9—C14—C16112.2 (2)
C5—C6—C7120.6 (3)C13—C14—C15107.0 (2)
C5—C6—H6122C13—C14—C16110.9 (2)
C7—C6—H6118C15—C14—C16110.6 (2)
C6—C7—C8119.6 (3)C14—C15—H15A111
C6—C7—H7121C14—C15—H15B109
C8—C7—H7119C14—C15—H15C110
C7—C8—C9121.4 (3)H15A—C15—H15B109
C7—C8—H8120H15A—C15—H15C110
C9—C8—H8119H15B—C15—H15C108
C4—C9—C8118.9 (2)C14—C16—C17120.0 (2)
C4—C9—C14117.5 (2)C14—C16—C21122.7 (2)
C8—C9—C14123.6 (2)C17—C16—C21117.3 (3)
N2—C10—C11111.2 (3)C16—C17—C18121.2 (3)
N2—C10—C12110.3 (3)C16—C17—H17118
N2—C10—H10108C18—C17—H17121
C11—C10—C12112.7 (3)C17—C18—C19120.5 (3)
C11—C10—H10108C17—C18—H18119
C12—C10—H10106C19—C18—H18121
C10—C11—H11A112C18—C19—C20119.1 (4)
C10—C11—H11B109C18—C19—H19120
C10—C11—H11C110C20—C19—H19121
H11A—C11—H11B109C19—C20—C21120.9 (4)
H11A—C11—H11C110C19—C20—H20119
H11B—C11—H11C107C21—C20—H20120
C10—C12—H12A110C16—C21—C20120.9 (3)
C10—C12—H12B113C16—C21—H21119
C10—C12—H12C109C20—C21—H21120

Experimental details

Crystal data
Chemical formulaC19H21NS
Mr295.44
Crystal system, space groupOrthorhombic, P212121
Temperature (K)298
a, b, c (Å)11.166 (1), 13.423 (1), 10.878 (1)
V3)1630.4 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.19
Crystal size (mm)0.55 × 0.4 × 0.3
Data collection
DiffractometerRigaku AFC-7R
diffractometer
Absorption correctionIntegration
(Coppens et al., 1965)
Tmin, Tmax0.928, 0.947
No. of measured, independent and
observed [I > 2σ(I)] reflections
3090, 2684, 1963
Rint0.006
(sin θ/λ)max1)0.703
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.124, 1.06
No. of reflections2684
No. of parameters190
No. of restraints?
H-atom treatmentH-atom parameters not refined
Δρmax, Δρmin (e Å3)0.15, 0.27
Absolute structureFlack (1983), no Friedel pairs
Absolute structure parameter0.1 (1)

Computer programs: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993), MSC/AFC Diffractometer Control Software, TEXSAN (Molecular Structure Corporation, 1999), SIR92 (Altomare et al., 1994), SHELXL97 (Sheldrick, 1997), TEXSAN.

Selected bond lengths (Å) top
S1—C31.681 (2)C9—C141.510 (3)
N2—C31.326 (3)C13—C141.533 (4)
N2—C131.470 (3)
 

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