supplementary materials


Acta Cryst. (2010). E66, o488    [ doi:10.1107/S1600536810003181 ]

5-Phenyl-3-(2-thienyl)-1,2,4-triazolo[3,4-a]isoquinoline

F. N. Khan, P. Manivel, K. Prabakaran, V. R. Hathwar and S. W. Ng

Abstract top

In the title molecule, C20H13N3S, the triazoloisoquinoline ring system is approximately planar, with an r.m.s. deviation of 0.045 Å and a maximum deviation of 0.090 (2) Å from the mean plane for the triazole ring C atom which is bonded to the thiophene ring. The phenyl ring is twisted by 52.0 (1)° with respect to the mean plane of the triazoloisoquinoline ring system. The thiophene ring is rotationally disordered by approximately 180° over two sites, the ratio of refined occupancies being 0.73 (1):0.27 (1).

Comment top

The molecular structure of the title compound is shown in Fig. 1.

Related literature top

For the synthesis and antihelmintic activity of triazolo compounds similar to the title compound, see: Nadkarni et al. (2001).

Experimental top

2-(3-Phenylisoquinolin-1-yl)hydrazine (1 mmol) was condensed with thienyl-2-carbaldehye (1.1 mmol) under refluxing conditions isopropanol (10 ml) solvent to give the corresponding 2-(3-phenylisoquinolin-1-yl)-1-(2-thienylmethylene)hydrazine in high yield. The compound was then oxidatively cyclized in nitrobenzene (10 ml) at 473 K. The product was recrystallized from dichlomethane to give block-shaped crystals.

Refinement top

Hydrogen atoms were placed in calculated positions (C–H 0.93 Å) and were included in the refinement in the riding model approximation, with U(H) set to 1.2U(C).

The thienyl ring is disordered over two positions. The temperature factors of the primed atoms were restrained to those of the unprimed ones, and the anisotropic temperature factors were restrained to be nearly isotropic. Pairs of distances of the primed atoms were restrained to within 0.01 Å of the umprimed ones.

Computing details top

Data collection: SMART (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. Thermal ellipsoid plot (Barbour, 2001) of C20H13N3S at the 50% probability level; hydrogen atoms are drawn as spheres of arbitrary radius. The disorder is not shown.
5-Phenyl-3-(2-thienyl)-1,2,4-triazolo[3,4-a]isoquinoline top
Crystal data top
C20H13N3SF(000) = 680
Mr = 327.39Dx = 1.348 Mg m3
Orthorhombic, P21212Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2 2abCell parameters from 1886 reflections
a = 19.7715 (17) Åθ = 2.4–20.1°
b = 8.7735 (7) ŵ = 0.21 mm1
c = 9.3027 (8) ÅT = 293 K
V = 1613.7 (2) Å3Block, yellow
Z = 40.32 × 0.30 × 0.24 mm
Data collection top
Bruker SMART area-detector
diffractometer
3670 independent reflections
Radiation source: fine-focus sealed tube2414 reflections with I > 2σ(I)
graphiteRint = 0.045
φ and ω scansθmax = 27.5°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2525
Tmin = 0.937, Tmax = 0.952k = 1110
10809 measured reflectionsl = 1012
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.057H-atom parameters constrained
wR(F2) = 0.128 w = 1/[σ2(Fo2) + (0.0577P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
3670 reflectionsΔρmax = 0.20 e Å3
230 parametersΔρmin = 0.21 e Å3
45 restraintsAbsolute structure: Flack (1983), 1631 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.05 (13)
Crystal data top
C20H13N3SV = 1613.7 (2) Å3
Mr = 327.39Z = 4
Orthorhombic, P21212Mo Kα radiation
a = 19.7715 (17) ŵ = 0.21 mm1
b = 8.7735 (7) ÅT = 293 K
c = 9.3027 (8) Å0.32 × 0.30 × 0.24 mm
Data collection top
Bruker SMART area-detector
diffractometer
3670 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2414 reflections with I > 2σ(I)
Tmin = 0.937, Tmax = 0.952Rint = 0.045
10809 measured reflectionsθmax = 27.5°
Refinement top
R[F2 > 2σ(F2)] = 0.057H-atom parameters constrained
wR(F2) = 0.128Δρmax = 0.20 e Å3
S = 1.03Δρmin = 0.21 e Å3
3670 reflectionsAbsolute structure: Flack (1983), 1631 Friedel pairs
230 parametersFlack parameter: 0.05 (13)
45 restraints
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
S10.59650 (8)0.46180 (17)0.63475 (18)0.0639 (5)0.731 (3)
S1'0.5970 (3)0.1599 (5)0.7573 (7)0.0639 (5)0.27
N10.50872 (10)0.2300 (3)0.3908 (2)0.0425 (6)
N20.41393 (12)0.1323 (3)0.4794 (3)0.0563 (7)
N30.45695 (12)0.1669 (3)0.5908 (3)0.0555 (7)
C10.55374 (13)0.2743 (3)0.2800 (3)0.0468 (7)
C20.52959 (14)0.2706 (4)0.1445 (3)0.0583 (8)
H20.55810.30160.07070.070*
C30.46266 (14)0.2218 (4)0.1071 (3)0.0563 (8)
C40.43864 (17)0.2247 (5)0.0345 (4)0.0718 (10)
H40.46650.26000.10780.086*
C50.37500 (18)0.1765 (4)0.0660 (4)0.0746 (11)
H50.35980.17840.16070.090*
C60.33259 (17)0.1246 (4)0.0419 (4)0.0715 (10)
H60.28910.09240.01930.086*
C70.35420 (15)0.1203 (4)0.1817 (4)0.0615 (9)
H70.32540.08580.25380.074*
C80.41991 (14)0.1682 (3)0.2156 (3)0.0483 (7)
C90.44535 (13)0.1724 (3)0.3605 (3)0.0449 (7)
C100.51257 (13)0.2250 (3)0.5399 (3)0.0448 (7)
C110.56696 (13)0.2788 (3)0.6329 (3)0.0492 (7)
C120.5985 (3)0.2087 (6)0.7424 (7)0.0665 (19)0.731 (3)
H120.58660.10840.76230.080*0.731 (3)
C130.6458 (4)0.2730 (7)0.8243 (11)0.0695 (18)0.731 (3)
H130.67110.22690.89650.083*0.731 (3)
C140.6491 (3)0.4187 (7)0.7808 (6)0.0649 (19)0.731 (3)
H140.67700.49060.82430.078*0.731 (3)
C12'0.5862 (10)0.4243 (14)0.659 (2)0.0665 (19)0.27
H12'0.56190.50620.62210.080*0.269 (3)
C13'0.6415 (10)0.447 (3)0.740 (2)0.0695 (18)0.27
H13'0.66970.53130.74630.083*0.269 (3)
C14'0.6445 (15)0.3135 (19)0.811 (3)0.0649 (19)0.27
H14B0.67290.30420.89030.078*0.269 (3)
C150.62471 (13)0.3176 (3)0.3121 (3)0.0460 (7)
C160.66749 (13)0.2237 (3)0.3895 (3)0.0491 (7)
H160.65190.13110.42510.059*
C170.73382 (14)0.2682 (4)0.4135 (3)0.0565 (8)
H170.76250.20510.46570.068*
C180.75759 (15)0.4039 (4)0.3615 (4)0.0634 (9)
H180.80190.43370.37970.076*
C190.71543 (15)0.4960 (4)0.2821 (4)0.0659 (9)
H190.73150.58750.24490.079*
C200.64940 (14)0.4525 (4)0.2576 (3)0.0569 (8)
H200.62120.51500.20360.068*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0616 (8)0.0510 (8)0.0790 (10)0.0019 (6)0.0066 (7)0.0081 (7)
S1'0.0616 (8)0.0510 (8)0.0790 (10)0.0019 (6)0.0066 (7)0.0081 (7)
N10.0383 (11)0.0443 (14)0.0448 (14)0.0009 (10)0.0050 (10)0.0028 (11)
N20.0483 (14)0.0649 (16)0.0557 (16)0.0058 (12)0.0043 (13)0.0079 (13)
N30.0510 (14)0.0667 (17)0.0489 (15)0.0028 (13)0.0059 (12)0.0061 (13)
C10.0424 (14)0.0469 (15)0.0511 (18)0.0034 (13)0.0072 (13)0.0010 (15)
C20.0534 (17)0.077 (2)0.0448 (18)0.0024 (16)0.0093 (14)0.0053 (17)
C30.0519 (17)0.067 (2)0.0497 (19)0.0066 (15)0.0018 (14)0.0057 (16)
C40.064 (2)0.100 (3)0.051 (2)0.009 (2)0.0022 (17)0.004 (2)
C50.067 (2)0.101 (3)0.056 (2)0.014 (2)0.0124 (18)0.015 (2)
C60.056 (2)0.078 (2)0.080 (3)0.0023 (18)0.018 (2)0.014 (2)
C70.0504 (18)0.067 (2)0.067 (2)0.0026 (16)0.0045 (15)0.0007 (17)
C80.0467 (16)0.0454 (16)0.0529 (18)0.0058 (13)0.0007 (14)0.0047 (14)
C90.0413 (14)0.0432 (16)0.0501 (17)0.0003 (12)0.0024 (14)0.0033 (14)
C100.0472 (15)0.0431 (16)0.0440 (17)0.0028 (13)0.0045 (13)0.0023 (14)
C110.0463 (15)0.0544 (17)0.0470 (17)0.0081 (13)0.0031 (13)0.0061 (15)
C120.073 (3)0.045 (3)0.082 (4)0.002 (3)0.012 (3)0.011 (3)
C130.054 (3)0.091 (4)0.064 (3)0.015 (4)0.004 (2)0.002 (4)
C140.063 (3)0.068 (4)0.063 (4)0.005 (3)0.019 (3)0.021 (3)
C12'0.073 (3)0.045 (3)0.082 (4)0.002 (3)0.012 (3)0.011 (3)
C13'0.054 (3)0.091 (4)0.064 (3)0.015 (4)0.004 (2)0.002 (4)
C14'0.063 (3)0.068 (4)0.063 (4)0.005 (3)0.019 (3)0.021 (3)
C150.0441 (14)0.0470 (17)0.0471 (17)0.0013 (13)0.0073 (13)0.0016 (13)
C160.0470 (15)0.0484 (16)0.0520 (18)0.0027 (14)0.0057 (14)0.0051 (14)
C170.0451 (15)0.069 (2)0.0555 (18)0.0142 (16)0.0029 (13)0.0004 (17)
C180.0441 (17)0.080 (2)0.066 (2)0.0092 (16)0.0086 (16)0.0034 (19)
C190.0613 (19)0.063 (2)0.074 (2)0.0157 (17)0.0121 (17)0.0096 (18)
C200.0518 (17)0.0544 (18)0.064 (2)0.0016 (15)0.0031 (15)0.0112 (16)
Geometric parameters (Å, °) top
S1—C111.708 (3)C10—C111.459 (4)
S1—C141.752 (4)C11—C121.344 (5)
S1'—C111.667 (5)C11—C12'1.355 (8)
S1'—C14'1.717 (9)C12—C131.331 (6)
N1—C91.380 (3)C12—H120.9300
N1—C101.389 (3)C13—C141.342 (6)
N1—C11.417 (3)C13—H130.9300
N2—C91.316 (4)C14—H140.9300
N2—N31.375 (3)C12'—C13'1.343 (8)
N3—C101.301 (3)C12'—H12'0.9300
C1—C21.348 (4)C13'—C14'1.342 (8)
C1—C151.484 (4)C13'—H13'0.9300
C2—C31.434 (4)C14'—H14B0.9300
C2—H20.9300C15—C201.377 (4)
C3—C81.398 (4)C15—C161.383 (4)
C3—C41.400 (4)C16—C171.387 (4)
C4—C51.359 (5)C16—H160.9300
C4—H40.9300C17—C181.368 (4)
C5—C61.385 (5)C17—H170.9300
C5—H50.9300C18—C191.376 (4)
C6—C71.369 (5)C18—H180.9300
C6—H60.9300C19—C201.379 (4)
C7—C81.402 (4)C19—H190.9300
C7—H70.9300C20—H200.9300
C8—C91.439 (4)
C11—S1—C1490.5 (2)C10—C11—S1'118.2 (3)
C11—S1'—C14'84.6 (8)C12—C11—S1105.3 (3)
C9—N1—C10104.0 (2)C10—C11—S1124.2 (2)
C9—N1—C1121.5 (2)S1'—C11—S1117.3 (2)
C10—N1—C1134.5 (2)C13—C12—C11124.5 (5)
C9—N2—N3106.4 (2)C13—C12—H12117.8
C10—N3—N2109.6 (2)C11—C12—H12117.8
C2—C1—N1116.8 (2)C12—C13—C14105.4 (6)
C2—C1—C15122.0 (3)C12—C13—H13127.3
N1—C1—C15121.2 (2)C14—C13—H13127.3
C1—C2—C3124.2 (3)C13—C14—S1114.2 (5)
C1—C2—H2117.9C13—C14—H14122.9
C3—C2—H2117.9S1—C14—H14122.9
C8—C3—C4118.7 (3)C13'—C12'—C11118.0 (17)
C8—C3—C2118.9 (3)C13'—C12'—H12'121.0
C4—C3—C2122.4 (3)C11—C12'—H12'121.0
C5—C4—C3120.8 (3)C14'—C13'—C12'100.6 (19)
C5—C4—H4119.6C14'—C13'—H13'129.7
C3—C4—H4119.6C12'—C13'—H13'129.7
C4—C5—C6120.4 (3)C13'—C14'—S1'121.1 (17)
C4—C5—H5119.8C13'—C14'—H14B119.4
C6—C5—H5119.8S1'—C14'—H14B119.4
C7—C6—C5120.6 (3)C20—C15—C16119.1 (3)
C7—C6—H6119.7C20—C15—C1118.8 (3)
C5—C6—H6119.7C16—C15—C1122.0 (3)
C6—C7—C8119.7 (3)C15—C16—C17119.6 (3)
C6—C7—H7120.2C15—C16—H16120.2
C8—C7—H7120.2C17—C16—H16120.2
C3—C8—C7119.9 (3)C18—C17—C16120.9 (3)
C3—C8—C9117.2 (2)C18—C17—H17119.6
C7—C8—C9122.8 (3)C16—C17—H17119.6
N2—C9—N1110.8 (3)C17—C18—C19119.5 (3)
N2—C9—C8127.9 (2)C17—C18—H18120.2
N1—C9—C8121.2 (3)C19—C18—H18120.2
N3—C10—N1109.2 (2)C18—C19—C20120.0 (3)
N3—C10—C11122.3 (2)C18—C19—H19120.0
N1—C10—C11128.5 (2)C20—C19—H19120.0
C12—C11—C12'99.4 (9)C19—C20—C15120.9 (3)
C12—C11—C10130.1 (3)C19—C20—H20119.6
C12'—C11—C10128.3 (9)C15—C20—H20119.6
C12'—C11—S1'111.4 (9)
C9—N2—N3—C100.4 (3)N1—C10—C11—C12'69.1 (13)
C9—N1—C1—C25.9 (4)N3—C10—C11—S1'53.0 (4)
C10—N1—C1—C2176.4 (3)N1—C10—C11—S1'129.4 (4)
C9—N1—C1—C15172.2 (2)N3—C10—C11—S1120.4 (3)
C10—N1—C1—C155.5 (5)N1—C10—C11—S157.2 (4)
N1—C1—C2—C31.5 (5)C14'—S1'—C11—C122(3)
C15—C1—C2—C3176.5 (3)C14'—S1'—C11—C12'10.5 (17)
C1—C2—C3—C82.8 (5)C14'—S1'—C11—C10175.0 (13)
C1—C2—C3—C4177.7 (4)C14'—S1'—C11—S11.1 (13)
C8—C3—C4—C50.0 (5)C14—S1—C11—C121.2 (5)
C2—C3—C4—C5179.6 (3)C14—S1—C11—C12'58 (5)
C3—C4—C5—C60.5 (6)C14—S1—C11—C10174.5 (3)
C4—C5—C6—C70.3 (6)C14—S1—C11—S1'1.0 (4)
C5—C6—C7—C80.3 (5)C12'—C11—C12—C1312.8 (12)
C4—C3—C8—C70.6 (5)C10—C11—C12—C13176.7 (7)
C2—C3—C8—C7179.8 (3)S1'—C11—C12—C13175 (3)
C4—C3—C8—C9177.6 (3)S1—C11—C12—C134.0 (9)
C2—C3—C8—C92.8 (4)C11—C12—C13—C144.9 (11)
C6—C7—C8—C30.8 (5)C12—C13—C14—S13.3 (8)
C6—C7—C8—C9177.6 (3)C11—S1—C14—C131.3 (5)
N3—N2—C9—N11.2 (3)C12—C11—C12'—C13'21 (2)
N3—N2—C9—C8175.8 (3)C10—C11—C12'—C13'174.8 (14)
C10—N1—C9—N21.4 (3)S1'—C11—C12'—C13'23 (2)
C1—N1—C9—N2176.9 (2)S1—C11—C12'—C13'104 (6)
C10—N1—C9—C8175.8 (3)C11—C12'—C13'—C14'22 (3)
C1—N1—C9—C85.9 (4)C12'—C13'—C14'—S1'13 (3)
C3—C8—C9—N2178.0 (3)C11—S1'—C14'—C13'2(3)
C7—C8—C9—N21.2 (5)C2—C1—C15—C2052.5 (4)
C3—C8—C9—N11.3 (4)N1—C1—C15—C20129.5 (3)
C7—C8—C9—N1175.5 (3)C2—C1—C15—C16124.6 (4)
N2—N3—C10—N10.5 (3)N1—C1—C15—C1653.4 (4)
N2—N3—C10—C11177.5 (3)C20—C15—C16—C171.4 (4)
C9—N1—C10—N31.2 (3)C1—C15—C16—C17178.5 (3)
C1—N1—C10—N3176.9 (3)C15—C16—C17—C180.1 (4)
C9—N1—C10—C11176.6 (3)C16—C17—C18—C191.2 (5)
C1—N1—C10—C115.3 (5)C17—C18—C19—C201.1 (5)
N3—C10—C11—C1251.1 (6)C18—C19—C20—C150.2 (5)
N1—C10—C11—C12131.3 (5)C16—C15—C20—C191.5 (4)
N3—C10—C11—C12'108.5 (13)C1—C15—C20—C19178.7 (3)
Acknowledgements top

We thank the Department of Science and Technology, India, for use of the diffraction facility at IISc under the IRHPA–DST program; FNK thanks the DST for Fast Track Proposal funding. We thank VIT University and the University of Malaya for supporting this study.

references
References top

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Bruker (2004). SAINT and SMART. Bruker AXS Inc., Madison, Wisconsin, USA.

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

Nadkarni, B. A., Kamat, V. R. & Khadse, B. G. (2001). Arzneim. Forsch. 51, 569–573.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Westrip, S. P. (2010). publCIF. In preparation.