






Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229618005272/ku3219sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S2053229618005272/ku3219Isup2.hkl |
![]() | Portable Document Format (PDF) file https://doi.org/10.1107/S2053229618005272/ku3219sup3.pdf |
![]() | Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229618005272/ku3219Isup4.cml |
CCDC reference: 1559416
Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: DIAMOND (Brandenburg & Putz, 1999); software used to prepare material for publication: SHELXL2014 (Sheldrick, 2015b).
C7H11N2O2+·Cl− | Dx = 1.347 Mg m−3 |
Mr = 190.63 | Melting point: 446.1 K |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 10.2225 (16) Å | Cell parameters from 4273 reflections |
b = 9.6736 (16) Å | θ = 3.0–26.2° |
c = 10.2678 (17) Å | µ = 0.37 mm−1 |
β = 112.165 (8)° | T = 294 K |
V = 940.3 (3) Å3 | Parallelepiped, colourless |
Z = 4 | 0.10 × 0.10 × 0.10 mm |
F(000) = 400 |
Bruker APEX CCD diffractometer | 1844 independent reflections |
Radiation source: fine-focus sealed tube | 1557 reflections with I > 2σ(I) |
Detector resolution: 8.33 pixels mm-1 | Rint = 0.031 |
ω scans | θmax = 26.0°, θmin = 3.0° |
Absorption correction: empirical (using intensity measurements) (Blessing, 1995) | h = −12→12 |
Tmin = 0.911, Tmax = 0.983 | k = −11→11 |
12035 measured reflections | l = −12→12 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.036 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.106 | w = 1/[σ2(Fo2) + (0.0564P)2 + 0.1633P] where P = (Fo2 + 2Fc2)/3 |
S = 1.10 | (Δ/σ)max < 0.001 |
1844 reflections | Δρmax = 0.23 e Å−3 |
112 parameters | Δρmin = −0.20 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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.13632 (17) | 0.67336 (15) | −0.00212 (17) | 0.0422 (4) | |
H1 | 0.0773 | 0.7390 | 0.0133 | 0.051* | |
C2 | 0.2695 (2) | 0.56244 (18) | −0.09152 (19) | 0.0528 (4) | |
H2A | 0.3172 | 0.5395 | −0.1498 | 0.063* | |
C3 | 0.2714 (2) | 0.49169 (18) | 0.0212 (2) | 0.0552 (5) | |
H3 | 0.3207 | 0.4104 | 0.0560 | 0.066* | |
C4 | 0.16677 (18) | 0.52539 (17) | 0.20420 (16) | 0.0448 (4) | |
H4B | 0.1726 | 0.4258 | 0.2162 | 0.054* | |
H4A | 0.0733 | 0.5543 | 0.1966 | 0.054* | |
C5 | 0.27599 (17) | 0.59300 (16) | 0.33095 (16) | 0.0425 (4) | |
C6 | 0.1495 (2) | 0.7779 (2) | −0.2195 (2) | 0.0571 (5) | |
H6A | 0.2362 | 0.8134 | −0.2245 | 0.069* | |
H6B | 0.0990 | 0.8548 | −0.1996 | 0.069* | |
C7 | 0.0606 (2) | 0.7146 (3) | −0.3581 (2) | 0.0749 (6) | |
H7A | 0.0397 | 0.7831 | −0.4308 | 0.112* | |
H7B | 0.1111 | 0.6394 | −0.3785 | 0.112* | |
H7C | −0.0259 | 0.6808 | −0.3537 | 0.112* | |
N1 | 0.18375 (14) | 0.67547 (12) | −0.10510 (14) | 0.0414 (3) | |
N2 | 0.18709 (14) | 0.56148 (13) | 0.07581 (13) | 0.0405 (3) | |
O1 | 0.35277 (13) | 0.68432 (12) | 0.32434 (13) | 0.0516 (3) | |
O2 | 0.27241 (16) | 0.54072 (15) | 0.44750 (13) | 0.0652 (4) | |
H2 | 0.338 (3) | 0.587 (3) | 0.528 (3) | 0.098* | |
Cl1 | 0.53307 (5) | 0.32422 (5) | 0.29617 (5) | 0.05769 (19) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0474 (9) | 0.0362 (8) | 0.0458 (9) | 0.0023 (6) | 0.0206 (7) | 0.0022 (7) |
C2 | 0.0682 (11) | 0.0491 (10) | 0.0482 (10) | 0.0122 (8) | 0.0299 (9) | 0.0008 (8) |
C3 | 0.0733 (12) | 0.0441 (9) | 0.0516 (11) | 0.0180 (8) | 0.0276 (9) | 0.0050 (8) |
C4 | 0.0548 (9) | 0.0410 (8) | 0.0400 (9) | −0.0083 (7) | 0.0195 (8) | 0.0006 (7) |
C5 | 0.0521 (9) | 0.0390 (8) | 0.0384 (9) | −0.0022 (7) | 0.0192 (8) | 0.0015 (6) |
C6 | 0.0629 (11) | 0.0543 (10) | 0.0619 (12) | 0.0082 (8) | 0.0322 (10) | 0.0213 (9) |
C7 | 0.0759 (14) | 0.1035 (17) | 0.0478 (12) | 0.0119 (12) | 0.0260 (11) | 0.0248 (11) |
N1 | 0.0469 (7) | 0.0385 (7) | 0.0402 (8) | 0.0017 (5) | 0.0179 (6) | 0.0032 (5) |
N2 | 0.0487 (7) | 0.0365 (7) | 0.0349 (7) | −0.0013 (5) | 0.0142 (6) | −0.0012 (5) |
O1 | 0.0616 (7) | 0.0491 (7) | 0.0443 (7) | −0.0149 (5) | 0.0201 (6) | −0.0002 (5) |
O2 | 0.0866 (10) | 0.0714 (9) | 0.0375 (7) | −0.0274 (7) | 0.0232 (7) | 0.0024 (6) |
Cl1 | 0.0604 (3) | 0.0721 (3) | 0.0408 (3) | −0.0079 (2) | 0.0194 (2) | 0.0024 (2) |
C1—N1 | 1.319 (2) | C4—H4A | 0.9700 |
C1—N2 | 1.330 (2) | C5—O1 | 1.2005 (19) |
C1—H1 | 0.9300 | C5—O2 | 1.3124 (19) |
C2—C3 | 1.339 (3) | C6—N1 | 1.474 (2) |
C2—N1 | 1.375 (2) | C6—C7 | 1.501 (3) |
C2—H2A | 0.9300 | C6—H6A | 0.9700 |
C3—N2 | 1.370 (2) | C6—H6B | 0.9700 |
C3—H3 | 0.9300 | C7—H7A | 0.9600 |
C4—N2 | 1.4524 (19) | C7—H7B | 0.9600 |
C4—C5 | 1.507 (2) | C7—H7C | 0.9600 |
C4—H4B | 0.9700 | O2—H2 | 0.96 (3) |
N1—C1—N2 | 108.48 (13) | N1—C6—H6A | 109.4 |
N1—C1—H1 | 125.8 | C7—C6—H6A | 109.4 |
N2—C1—H1 | 125.8 | N1—C6—H6B | 109.4 |
C3—C2—N1 | 107.16 (15) | C7—C6—H6B | 109.4 |
C3—C2—H2A | 126.4 | H6A—C6—H6B | 108.0 |
N1—C2—H2A | 126.4 | C6—C7—H7A | 109.5 |
C2—C3—N2 | 107.19 (15) | C6—C7—H7B | 109.5 |
C2—C3—H3 | 126.4 | H7A—C7—H7B | 109.5 |
N2—C3—H3 | 126.4 | C6—C7—H7C | 109.5 |
N2—C4—C5 | 111.49 (13) | H7A—C7—H7C | 109.5 |
N2—C4—H4B | 109.3 | H7B—C7—H7C | 109.5 |
C5—C4—H4B | 109.3 | C1—N1—C2 | 108.62 (13) |
N2—C4—H4A | 109.3 | C1—N1—C6 | 126.88 (14) |
C5—C4—H4A | 109.3 | C2—N1—C6 | 124.47 (14) |
H4B—C4—H4A | 108.0 | C1—N2—C3 | 108.54 (14) |
O1—C5—O2 | 125.37 (16) | C1—N2—C4 | 125.80 (13) |
O1—C5—C4 | 123.90 (14) | C3—N2—C4 | 125.46 (14) |
O2—C5—C4 | 110.71 (14) | C5—O2—H2 | 111.1 (16) |
N1—C6—C7 | 110.98 (16) | ||
N1—C2—C3—N2 | 0.0 (2) | C7—C6—N1—C2 | 67.4 (2) |
N2—C4—C5—O1 | 12.9 (2) | N1—C1—N2—C3 | 0.97 (19) |
N2—C4—C5—O2 | −168.70 (14) | N1—C1—N2—C4 | 176.09 (14) |
N2—C1—N1—C2 | −0.95 (19) | C2—C3—N2—C1 | −0.6 (2) |
N2—C1—N1—C6 | 177.42 (15) | C2—C3—N2—C4 | −175.75 (15) |
C3—C2—N1—C1 | 0.6 (2) | C5—C4—N2—C1 | −85.89 (19) |
C3—C2—N1—C6 | −177.86 (17) | C5—C4—N2—C3 | 88.4 (2) |
C7—C6—N1—C1 | −110.8 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···Cl1 | 0.93 | 2.73 | 3.472 (2) | 137 |
C1—H1···Cl1i | 0.93 | 2.73 | 3.5161 (19) | 143 |
C4—H4B···O1ii | 0.97 | 2.37 | 3.312 (2) | 164 |
O2—H2···Cl1iii | 0.96 (3) | 1.98 (3) | 2.9393 (15) | 176 (2) |
C1—H1···O1iv | 0.93 | 2.49 | 3.094 (2) | 122 |
C2—H2A···Cl1v | 0.93 | 2.84 | 3.590 (2) | 138 |
Symmetry codes: (i) −x+1/2, y+1/2, −z+1/2; (ii) −x+1/2, y−1/2, −z+1/2; (iii) −x+1, −y+1, −z+1; (iv) x−1/2, −y+3/2, z−1/2; (v) −x+1, −y+1, −z. |