Experimental
Crystal data
C12H16ClN3O Mr = 253.73 Orthorhombic, P b c n a = 24.920 (5) Å b = 9.5033 (19) Å c = 11.064 (2) Å V = 2620.3 (9) Å3 Z = 8 Mo Kα radiation μ = 0.28 mm−1 T = 293 K 0.22 × 0.20 × 0.18 mm
|
Data collection
Bruker SMART CCD diffractometer 23785 measured reflections 3006 independent reflections 2077 reflections with I > 2σ(I) Rint = 0.045
|
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A | N3—H3A⋯O1i | 0.86 | 2.26 | 3.001 (2) | 144 | Symmetry code: (i) . | |
Data collection: SMART (Bruker, 1997
); cell refinement: SAINT (Bruker, 1997
); data reduction: SAINT; 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.
Supporting information
A mixture of 1-methylpiperazine (0.1 mol), and (4-chlorophenyl)carbamic chloride (0.1 mol) was stirred in refluxing ethanol (20 ml) for 4 h to afford the title compound (0.079 mol, yield 79%). Colourless blocks of the title compound were obtained by recrystallization from ethanol at room temperature.
H atoms were fixed geometrically and allowed to ride on their attached atoms, with C—H distances = 0.93–0.97 Å; N—H = 0.86Å and with Uiso(H) = 1.2Ueq(C,N) or 1.5Ueq(Cmethyl).
Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); 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).
N-(4-Chlorophenyl)-4-methylpiperazine-1-carboxamide
top Crystal data top C12H16ClN3O | Dx = 1.286 Mg m−3 |
Mr = 253.73 | Mo Kα radiation, λ = 0.71073 Å |
Orthorhombic, Pbcn | Cell parameters from 2077 reflections |
a = 24.920 (5) Å | θ = 3.2–27.4° |
b = 9.5033 (19) Å | µ = 0.28 mm−1 |
c = 11.064 (2) Å | T = 293 K |
V = 2620.3 (9) Å3 | Block, colorless |
Z = 8 | 0.22 × 0.20 × 0.18 mm |
F(000) = 1072 | |
Data collection top Bruker SMART CCD diffractometer | 2077 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.045 |
Graphite monochromator | θmax = 27.5°, θmin = 3.3° |
ϕ and ω scans | h = −31→32 |
23785 measured reflections | k = −12→10 |
3006 independent reflections | l = −14→14 |
Refinement top Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.059 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.192 | H-atom parameters constrained |
S = 1.11 | w = 1/[σ2(Fo2) + (0.1054P)2 + 0.5647P] where P = (Fo2 + 2Fc2)/3 |
3006 reflections | (Δ/σ)max < 0.001 |
154 parameters | Δρmax = 0.25 e Å−3 |
0 restraints | Δρmin = −0.60 e Å−3 |
Crystal data top C12H16ClN3O | V = 2620.3 (9) Å3 |
Mr = 253.73 | Z = 8 |
Orthorhombic, Pbcn | Mo Kα radiation |
a = 24.920 (5) Å | µ = 0.28 mm−1 |
b = 9.5033 (19) Å | T = 293 K |
c = 11.064 (2) Å | 0.22 × 0.20 × 0.18 mm |
Data collection top Bruker SMART CCD diffractometer | 2077 reflections with I > 2σ(I) |
23785 measured reflections | Rint = 0.045 |
3006 independent reflections | |
Refinement top R[F2 > 2σ(F2)] = 0.059 | 0 restraints |
wR(F2) = 0.192 | H-atom parameters constrained |
S = 1.11 | Δρmax = 0.25 e Å−3 |
3006 reflections | Δρmin = −0.60 e Å−3 |
154 parameters | |
Special details top 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Cl1 | 0.07382 (3) | 0.14060 (8) | 0.66714 (8) | 0.0750 (3) | |
O1 | 0.28704 (6) | 0.11160 (14) | 1.01352 (17) | 0.0559 (5) | |
C6 | 0.28896 (7) | −0.0180 (2) | 1.0143 (2) | 0.0424 (5) | |
C7 | 0.21110 (7) | −0.0415 (2) | 0.88098 (19) | 0.0399 (5) | |
N3 | 0.25282 (6) | −0.09932 (17) | 0.95154 (18) | 0.0453 (5) | |
H3A | 0.2558 | −0.1894 | 0.9555 | 0.054* | |
C12 | 0.16012 (8) | −0.0996 (2) | 0.8900 (2) | 0.0479 (5) | |
H12A | 0.1541 | −0.1754 | 0.9415 | 0.058* | |
C11 | 0.11817 (8) | −0.0447 (3) | 0.8224 (2) | 0.0516 (6) | |
H11A | 0.0840 | −0.0836 | 0.8282 | 0.062* | |
C10 | 0.12738 (8) | 0.0675 (2) | 0.7469 (2) | 0.0501 (5) | |
C9 | 0.17805 (9) | 0.1239 (2) | 0.7340 (2) | 0.0522 (6) | |
H9A | 0.1840 | 0.1981 | 0.6809 | 0.063* | |
C8 | 0.21988 (8) | 0.0687 (2) | 0.8010 (2) | 0.0464 (5) | |
H8A | 0.2542 | 0.1057 | 0.7925 | 0.056* | |
N2 | 0.32650 (7) | −0.08928 (19) | 1.0782 (2) | 0.0558 (6) | |
N1 | 0.43172 (7) | −0.1934 (2) | 1.1165 (2) | 0.0605 (6) | |
C3 | 0.33749 (9) | −0.2391 (2) | 1.0715 (3) | 0.0593 (7) | |
H3B | 0.3139 | −0.2824 | 1.0126 | 0.071* | |
H3C | 0.3306 | −0.2822 | 1.1495 | 0.071* | |
C4 | 0.36406 (10) | −0.0151 (3) | 1.1554 (3) | 0.0681 (8) | |
H4A | 0.3592 | −0.0450 | 1.2385 | 0.082* | |
H4B | 0.3572 | 0.0852 | 1.1512 | 0.082* | |
C5 | 0.42085 (10) | −0.0446 (3) | 1.1162 (3) | 0.0719 (8) | |
H5A | 0.4265 | −0.0074 | 1.0356 | 0.086* | |
H5B | 0.4456 | 0.0025 | 1.1705 | 0.086* | |
C2 | 0.39479 (11) | −0.2641 (3) | 1.0361 (3) | 0.0647 (7) | |
H2A | 0.4021 | −0.3643 | 1.0372 | 0.078* | |
H2B | 0.4004 | −0.2305 | 0.9542 | 0.078* | |
C1 | 0.48742 (12) | −0.2234 (5) | 1.0819 (4) | 0.1134 (15) | |
H1A | 0.5114 | −0.1767 | 1.1367 | 0.170* | |
H1B | 0.4937 | −0.1902 | 1.0012 | 0.170* | |
H1C | 0.4936 | −0.3231 | 1.0851 | 0.170* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Cl1 | 0.0629 (4) | 0.0773 (5) | 0.0846 (6) | 0.0211 (3) | −0.0201 (3) | 0.0074 (4) |
O1 | 0.0555 (9) | 0.0286 (7) | 0.0836 (13) | 0.0032 (6) | −0.0119 (8) | −0.0023 (7) |
C6 | 0.0424 (10) | 0.0319 (9) | 0.0529 (13) | 0.0009 (7) | −0.0027 (8) | 0.0008 (8) |
C7 | 0.0433 (10) | 0.0341 (9) | 0.0422 (11) | 0.0036 (8) | −0.0015 (8) | 0.0007 (8) |
N3 | 0.0477 (9) | 0.0295 (8) | 0.0587 (12) | 0.0000 (7) | −0.0117 (8) | 0.0055 (7) |
C12 | 0.0493 (11) | 0.0431 (11) | 0.0514 (13) | −0.0051 (9) | −0.0025 (9) | 0.0047 (9) |
C11 | 0.0419 (10) | 0.0536 (13) | 0.0591 (15) | −0.0025 (9) | −0.0016 (9) | −0.0004 (11) |
C10 | 0.0499 (12) | 0.0490 (12) | 0.0514 (13) | 0.0120 (9) | −0.0052 (9) | −0.0021 (10) |
C9 | 0.0592 (13) | 0.0455 (11) | 0.0520 (14) | 0.0077 (9) | 0.0019 (10) | 0.0093 (10) |
C8 | 0.0433 (10) | 0.0436 (11) | 0.0523 (13) | 0.0014 (8) | 0.0018 (9) | 0.0060 (9) |
N2 | 0.0542 (11) | 0.0345 (9) | 0.0787 (15) | 0.0054 (8) | −0.0240 (10) | −0.0057 (9) |
N1 | 0.0428 (10) | 0.0548 (12) | 0.0838 (16) | 0.0033 (8) | −0.0014 (9) | −0.0012 (11) |
C3 | 0.0574 (13) | 0.0342 (11) | 0.0862 (19) | 0.0016 (9) | −0.0252 (12) | 0.0045 (11) |
C4 | 0.0611 (13) | 0.0508 (14) | 0.092 (2) | 0.0102 (11) | −0.0304 (13) | −0.0211 (14) |
C5 | 0.0595 (14) | 0.0533 (14) | 0.103 (2) | −0.0107 (11) | −0.0139 (14) | 0.0008 (15) |
C2 | 0.0767 (16) | 0.0486 (13) | 0.0689 (18) | 0.0123 (12) | −0.0063 (13) | −0.0065 (12) |
C1 | 0.0538 (18) | 0.113 (3) | 0.173 (4) | 0.0106 (17) | 0.023 (2) | −0.011 (3) |
Geometric parameters (Å, º) top Cl1—C10 | 1.745 (2) | N2—C3 | 1.452 (3) |
O1—C6 | 1.232 (2) | N1—C5 | 1.440 (3) |
C6—N2 | 1.355 (3) | N1—C2 | 1.446 (3) |
C6—N3 | 1.375 (3) | N1—C1 | 1.468 (3) |
C7—C8 | 1.388 (3) | C3—C2 | 1.500 (4) |
C7—C12 | 1.389 (3) | C3—H3B | 0.9700 |
C7—N3 | 1.411 (2) | C3—H3C | 0.9700 |
N3—H3A | 0.8600 | C4—C5 | 1.506 (4) |
C12—C11 | 1.388 (3) | C4—H4A | 0.9700 |
C12—H12A | 0.9300 | C4—H4B | 0.9700 |
C11—C10 | 1.374 (3) | C5—H5A | 0.9700 |
C11—H11A | 0.9300 | C5—H5B | 0.9700 |
C10—C9 | 1.379 (3) | C2—H2A | 0.9700 |
C9—C8 | 1.383 (3) | C2—H2B | 0.9700 |
C9—H9A | 0.9300 | C1—H1A | 0.9600 |
C8—H8A | 0.9300 | C1—H1B | 0.9600 |
N2—C4 | 1.450 (3) | C1—H1C | 0.9600 |
| | | |
O1—C6—N2 | 122.02 (19) | N2—C3—C2 | 110.4 (2) |
O1—C6—N3 | 122.22 (18) | N2—C3—H3B | 109.6 |
N2—C6—N3 | 115.75 (17) | C2—C3—H3B | 109.6 |
C8—C7—C12 | 119.35 (19) | N2—C3—H3C | 109.6 |
C8—C7—N3 | 122.00 (17) | C2—C3—H3C | 109.6 |
C12—C7—N3 | 118.63 (18) | H3B—C3—H3C | 108.1 |
C6—N3—C7 | 122.87 (16) | N2—C4—C5 | 110.3 (2) |
C6—N3—H3A | 118.6 | N2—C4—H4A | 109.6 |
C7—N3—H3A | 118.6 | C5—C4—H4A | 109.6 |
C11—C12—C7 | 120.0 (2) | N2—C4—H4B | 109.6 |
C11—C12—H12A | 120.0 | C5—C4—H4B | 109.6 |
C7—C12—H12A | 120.0 | H4A—C4—H4B | 108.1 |
C10—C11—C12 | 119.6 (2) | N1—C5—C4 | 111.0 (2) |
C10—C11—H11A | 120.2 | N1—C5—H5A | 109.4 |
C12—C11—H11A | 120.2 | C4—C5—H5A | 109.4 |
C11—C10—C9 | 121.2 (2) | N1—C5—H5B | 109.4 |
C11—C10—Cl1 | 119.27 (17) | C4—C5—H5B | 109.4 |
C9—C10—Cl1 | 119.57 (18) | H5A—C5—H5B | 108.0 |
C10—C9—C8 | 119.2 (2) | N1—C2—C3 | 111.8 (2) |
C10—C9—H9A | 120.4 | N1—C2—H2A | 109.3 |
C8—C9—H9A | 120.4 | C3—C2—H2A | 109.3 |
C9—C8—C7 | 120.6 (2) | N1—C2—H2B | 109.3 |
C9—C8—H8A | 119.7 | C3—C2—H2B | 109.3 |
C7—C8—H8A | 119.7 | H2A—C2—H2B | 107.9 |
C6—N2—C4 | 120.68 (18) | N1—C1—H1A | 109.5 |
C6—N2—C3 | 126.47 (18) | N1—C1—H1B | 109.5 |
C4—N2—C3 | 112.64 (17) | H1A—C1—H1B | 109.5 |
C5—N1—C2 | 109.6 (2) | N1—C1—H1C | 109.5 |
C5—N1—C1 | 111.6 (2) | H1A—C1—H1C | 109.5 |
C2—N1—C1 | 110.5 (3) | H1B—C1—H1C | 109.5 |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N3—H3A···O1i | 0.86 | 2.26 | 3.001 (2) | 144 |
Symmetry code: (i) −x+1/2, y−1/2, z. |
Experimental details
Crystal data |
Chemical formula | C12H16ClN3O |
Mr | 253.73 |
Crystal system, space group | Orthorhombic, Pbcn |
Temperature (K) | 293 |
a, b, c (Å) | 24.920 (5), 9.5033 (19), 11.064 (2) |
V (Å3) | 2620.3 (9) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 0.28 |
Crystal size (mm) | 0.22 × 0.20 × 0.18 |
|
Data collection |
Diffractometer | Bruker SMART CCD diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 23785, 3006, 2077 |
Rint | 0.045 |
(sin θ/λ)max (Å−1) | 0.649 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.059, 0.192, 1.11 |
No. of reflections | 3006 |
No. of parameters | 154 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.25, −0.60 |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N3—H3A···O1i | 0.86 | 2.26 | 3.001 (2) | 144 |
Symmetry code: (i) −x+1/2, y−1/2, z. |
References
Arrieta, A., Otaegui, D., Zubia, A., et al. (2007). J. Org. Chem. 72, 4313–4322. CrossRef CAS Google Scholar
Bruker (1997). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Li, Y.-F. (2011a). Acta Cryst. E67, o1796. Web of Science CSD CrossRef IUCr Journals Google Scholar
Li, Y.-F. (2011b). Acta Cryst. E67, o1792. Web of Science CSD CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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