Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536808015274/hg2397sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536808015274/hg2397Isup2.hkl |
CCDC reference: 696505
Key indicators
- Single-crystal X-ray study
- T = 298 K
- Mean (C-C) = 0.003 Å
- R factor = 0.044
- wR factor = 0.112
- Data-to-parameter ratio = 16.0
checkCIF/PLATON results
No syntax errors found
Alert level C REFLT03_ALERT_3_C Reflection count < 95% complete From the CIF: _diffrn_reflns_theta_max 28.27 From the CIF: _diffrn_reflns_theta_full 28.27 From the CIF: _reflns_number_total 1845 TEST2: Reflns within _diffrn_reflns_theta_max Count of symmetry unique reflns 1956 Completeness (_total/calc) 94.33% PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.96 PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ?
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
5-(2-Pyridyl)tetrazole, (3.0 g, 20.0 mmol) was dissolved in 25 ml of 2-butanone with stirring and to the solution 1,3-dibromopropane (2.0 g, 10.0 mmol) and K2CO3 (5.5 g, 40.0 mmol) were added. The reaction mixture was heated under reflux for 24 h. After cooling the inorganic materials were filtered off and the solvent was removed under reduced pressure to afford the mixture of isomers. These isomers were separated by column chromatography on silica gel (1:4–2:1 EtOAc/Petroleum ether(60-90°C). The pure compound (I) (334 mg, 1.0 mmol) was dissolved in the solvent (1:1 EtOAc/Petroleum ether), and recrystallized from EtOAc/Petroleum ether affording colorless crystals. .
Positional parameters of all H atoms were calculated geometrically and were allowed to ride on the C atoms to which they are bonded, with C-H distances in the range 0.93-0.97Å and Uiso(H) = 1.2Ueq(C).
Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); 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 (Sheldrick, 2008).
Fig. 1. The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level (Symmetry code(A): (-x+1,y,-z+1/2) |
C15H14N10 | F(000) = 696 |
Mr = 334.36 | Dx = 1.410 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 25 reflections |
a = 14.486 (2) Å | θ = 2.7–28.3° |
b = 9.1322 (13) Å | µ = 0.10 mm−1 |
c = 12.8032 (19) Å | T = 298 K |
β = 111.596 (2)° | Block, colourless |
V = 1574.8 (4) Å3 | 0.2 × 0.2 × 0.2 mm |
Z = 4 |
Rigaku Scxmini 1K CCD area-detector diffractometer | 1845 independent reflections |
Radiation source: fine-focus sealed tube | 1166 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.031 |
Detector resolution: 8.192 pixels mm-1 | θmax = 28.3°, θmin = 2.7° |
thin–slice ω scans | h = −15→18 |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −7→12 |
Tmin = 0.981, Tmax = 0.981 | l = −16→16 |
4930 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)] = 0.044 | H-atom parameters constrained |
wR(F2) = 0.112 | w = 1/[σ2(Fo2) + (0.0498P)2 + 0.113P] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max < 0.001 |
1845 reflections | Δρmax = 0.14 e Å−3 |
115 parameters | Δρmin = −0.14 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0018 (5) |
C15H14N10 | V = 1574.8 (4) Å3 |
Mr = 334.36 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 14.486 (2) Å | µ = 0.10 mm−1 |
b = 9.1322 (13) Å | T = 298 K |
c = 12.8032 (19) Å | 0.2 × 0.2 × 0.2 mm |
β = 111.596 (2)° |
Rigaku Scxmini 1K CCD area-detector diffractometer | 1845 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | 1166 reflections with I > 2σ(I) |
Tmin = 0.981, Tmax = 0.981 | Rint = 0.031 |
4930 measured reflections |
R[F2 > 2σ(F2)] = 0.044 | 0 restraints |
wR(F2) = 0.112 | H-atom parameters constrained |
S = 1.02 | Δρmax = 0.14 e Å−3 |
1845 reflections | Δρmin = −0.14 e Å−3 |
115 parameters |
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 | Occ. (<1) | |
C2 | 0.37119 (12) | 0.2927 (2) | −0.15496 (13) | 0.0542 (5) | |
H2A | 0.3811 | 0.2170 | −0.1982 | 0.065* | |
N2 | 0.39676 (9) | 0.07129 (14) | 0.09971 (10) | 0.0372 (3) | |
N3 | 0.40148 (11) | −0.07629 (15) | 0.10268 (13) | 0.0520 (4) | |
N4 | 0.38893 (11) | −0.11910 (16) | 0.00162 (14) | 0.0592 (4) | |
N5 | 0.37593 (11) | −0.00222 (17) | −0.06788 (12) | 0.0527 (4) | |
C1 | 0.36961 (10) | 0.26606 (18) | −0.04949 (12) | 0.0388 (4) | |
N1 | 0.35696 (10) | 0.37150 (15) | 0.01654 (10) | 0.0447 (4) | |
C3 | 0.34557 (13) | 0.50772 (19) | −0.02391 (15) | 0.0517 (5) | |
H3B | 0.3380 | 0.5826 | 0.0215 | 0.062* | |
C4 | 0.34441 (14) | 0.5440 (2) | −0.12819 (15) | 0.0579 (5) | |
H4B | 0.3349 | 0.6404 | −0.1533 | 0.069* | |
C5 | 0.35767 (15) | 0.4344 (2) | −0.19443 (15) | 0.0642 (6) | |
H5B | 0.3575 | 0.4556 | −0.2655 | 0.077* | |
C6 | 0.38094 (11) | 0.11518 (17) | −0.00589 (12) | 0.0382 (4) | |
C7 | 0.40529 (11) | 0.15178 (18) | 0.20192 (12) | 0.0411 (4) | |
H7A | 0.4022 | 0.0827 | 0.2581 | 0.049* | |
H7B | 0.3491 | 0.2177 | 0.1851 | 0.049* | |
C8 | 0.5000 | 0.2392 (2) | 0.2500 | 0.0418 (5) | |
H8B | 0.4950 | 0.3021 | 0.3087 | 0.063* | 0.50 |
H8A | 0.5050 | 0.3021 | 0.1913 | 0.063* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
C2 | 0.0685 (12) | 0.0581 (13) | 0.0403 (9) | 0.0009 (9) | 0.0250 (8) | −0.0008 (9) |
N2 | 0.0384 (7) | 0.0343 (8) | 0.0384 (7) | −0.0012 (6) | 0.0136 (5) | 0.0013 (6) |
N3 | 0.0556 (9) | 0.0364 (9) | 0.0627 (10) | −0.0013 (7) | 0.0203 (7) | 0.0003 (7) |
N4 | 0.0665 (10) | 0.0428 (9) | 0.0669 (11) | −0.0018 (7) | 0.0228 (8) | −0.0092 (8) |
N5 | 0.0594 (9) | 0.0484 (9) | 0.0490 (9) | −0.0014 (7) | 0.0188 (7) | −0.0109 (7) |
C1 | 0.0354 (8) | 0.0455 (10) | 0.0342 (8) | −0.0019 (7) | 0.0112 (6) | −0.0013 (7) |
N1 | 0.0554 (8) | 0.0395 (8) | 0.0404 (8) | 0.0038 (6) | 0.0192 (6) | 0.0028 (6) |
C3 | 0.0619 (11) | 0.0418 (10) | 0.0533 (10) | 0.0044 (8) | 0.0234 (9) | 0.0059 (9) |
C4 | 0.0646 (12) | 0.0524 (12) | 0.0590 (11) | 0.0033 (9) | 0.0256 (9) | 0.0179 (10) |
C5 | 0.0799 (14) | 0.0731 (15) | 0.0431 (10) | −0.0029 (11) | 0.0269 (9) | 0.0142 (10) |
C6 | 0.0369 (8) | 0.0412 (9) | 0.0353 (8) | −0.0003 (7) | 0.0119 (6) | −0.0043 (7) |
C7 | 0.0465 (9) | 0.0453 (10) | 0.0342 (8) | 0.0013 (7) | 0.0180 (7) | 0.0021 (7) |
C8 | 0.0472 (13) | 0.0396 (13) | 0.0357 (11) | 0.000 | 0.0120 (9) | 0.000 |
C2—C5 | 1.377 (2) | C3—C4 | 1.370 (2) |
C2—C1 | 1.381 (2) | C3—H3B | 0.9300 |
C2—H2A | 0.9300 | C4—C5 | 1.370 (3) |
N2—N3 | 1.3493 (18) | C4—H4B | 0.9300 |
N2—C6 | 1.3464 (18) | C5—H5B | 0.9300 |
N2—C7 | 1.4661 (19) | C7—C8 | 1.5091 (18) |
N3—N4 | 1.2988 (19) | C7—H7A | 0.9700 |
N4—N5 | 1.358 (2) | C7—H7B | 0.9700 |
N5—C6 | 1.3199 (19) | C8—C7i | 1.5091 (18) |
C1—N1 | 1.3378 (19) | C8—H8B | 0.9700 |
C1—C6 | 1.473 (2) | C8—H8A | 0.9700 |
N1—C3 | 1.334 (2) | ||
C5—C2—C1 | 118.27 (16) | C4—C5—C2 | 119.51 (16) |
C5—C2—H2A | 120.9 | C4—C5—H5B | 120.2 |
C1—C2—H2A | 120.9 | C2—C5—H5B | 120.2 |
N3—N2—C6 | 108.29 (13) | N5—C6—N2 | 108.26 (14) |
N3—N2—C7 | 119.27 (12) | N5—C6—C1 | 123.92 (14) |
C6—N2—C7 | 132.41 (13) | N2—C6—C1 | 127.81 (14) |
N4—N3—N2 | 106.59 (13) | N2—C7—C8 | 113.25 (11) |
N3—N4—N5 | 110.55 (14) | N2—C7—H7A | 108.9 |
C6—N5—N4 | 106.31 (13) | C8—C7—H7A | 108.9 |
N1—C1—C2 | 123.13 (15) | N2—C7—H7B | 108.9 |
N1—C1—C6 | 117.12 (13) | C8—C7—H7B | 108.9 |
C2—C1—C6 | 119.75 (15) | H7A—C7—H7B | 107.7 |
C3—N1—C1 | 116.87 (14) | C7—C8—C7i | 116.09 (19) |
N1—C3—C4 | 124.01 (17) | C7—C8—H8B | 108.3 |
N1—C3—H3B | 118.0 | C7i—C8—H8B | 108.3 |
C4—C3—H3B | 118.0 | C7—C8—H8A | 108.3 |
C5—C4—C3 | 118.19 (17) | C7i—C8—H8A | 108.3 |
C5—C4—H4B | 120.9 | H8B—C8—H8A | 107.4 |
C3—C4—H4B | 120.9 | ||
C6—N2—N3—N4 | 0.07 (16) | N4—N5—C6—C1 | −179.43 (14) |
C7—N2—N3—N4 | 178.05 (12) | N3—N2—C6—N5 | −0.06 (16) |
N2—N3—N4—N5 | −0.06 (17) | C7—N2—C6—N5 | −177.67 (14) |
N3—N4—N5—C6 | 0.02 (18) | N3—N2—C6—C1 | 179.36 (14) |
C5—C2—C1—N1 | −0.9 (2) | C7—N2—C6—C1 | 1.8 (2) |
C5—C2—C1—C6 | 178.24 (15) | N1—C1—C6—N5 | 167.21 (14) |
C2—C1—N1—C3 | 0.0 (2) | C2—C1—C6—N5 | −12.0 (2) |
C6—C1—N1—C3 | −179.23 (13) | N1—C1—C6—N2 | −12.1 (2) |
C1—N1—C3—C4 | 1.2 (2) | C2—C1—C6—N2 | 168.64 (14) |
N1—C3—C4—C5 | −1.3 (3) | N3—N2—C7—C8 | 111.61 (15) |
C3—C4—C5—C2 | 0.3 (3) | C6—N2—C7—C8 | −71.0 (2) |
C1—C2—C5—C4 | 0.8 (3) | N2—C7—C8—C7i | −67.96 (10) |
N4—N5—C6—N2 | 0.02 (17) |
Symmetry code: (i) −x+1, y, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C15H14N10 |
Mr | 334.36 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 298 |
a, b, c (Å) | 14.486 (2), 9.1322 (13), 12.8032 (19) |
β (°) | 111.596 (2) |
V (Å3) | 1574.8 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.10 |
Crystal size (mm) | 0.2 × 0.2 × 0.2 |
Data collection | |
Diffractometer | Rigaku Scxmini 1K CCD area-detector diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku, 2005) |
Tmin, Tmax | 0.981, 0.981 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4930, 1845, 1166 |
Rint | 0.031 |
(sin θ/λ)max (Å−1) | 0.666 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.044, 0.112, 1.02 |
No. of reflections | 1845 |
No. of parameters | 115 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.14, −0.14 |
Computer programs: CrystalClear (Rigaku, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
The tetrazolate anion is an ambident system in which alkylation can occur at the N-1 or N-2 position, the relative proportions of which depend upon the reaction conditions, the nature of the alkylating agent and the influence of the 5-substituent (Meyer et al., 1998; Bronisz, 2002). The crystal structure of one of the three regioisomers has already been published (Gallardo et al., 2004). In our case, no regioselectivity was observed and the three possible regioisomers were isolated in equal amounts.
The structure of the title compound (I) is similar to that observed in the paper (Gallardo et al., 2004) with bond lengths and angles in good agreement with expected values. The molecules of (I) are disposed about a crystallographic two-fold axis of symmetry with symmetrical 5-(2-pyridyl)- 2H-tetrazolyl units connected by a propylene bridge. The molecule is folded at the center of the bridge [C7-C8-C7i 116.1 (2)°; symmetry code (i) = (-x+1,y,-z+1/2)] giving a U-like conformation to the free ligand. The inter-ring dihedral angle Py/Tz is 12.00 (7)°.