Download citation
Download citation
link to html
In the crystal, mol­ecular pairs form dimers through N—H⋯O hydrogen bonds. These dimers are linked into ribbons parallel to the (100) plane by further N—H⋯O hydrogen bonds. In addition, π–π and C—Cl⋯π inter­actions between the ribbons form layers parallel to the (100) plane.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2056989024000835/nx2004sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2056989024000835/nx2004Isup2.hkl
Contains datablock I

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2056989024000835/nx2004Isup3.cml
Supplementary material

CCDC reference: 2327646

Computing details top

4-(2-Chloroethyl)-5-methyl-1,2-dihydropyrazol-3-one top
Crystal data top
C6H9ClN2OF(000) = 336
Mr = 160.60Dx = 1.405 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54184 Å
a = 9.8420 (2) ÅCell parameters from 4592 reflections
b = 6.9145 (2) Åθ = 4.5–77.6°
c = 11.1807 (2) ŵ = 3.92 mm1
β = 93.618 (2)°T = 100 K
V = 759.36 (3) Å3Prism, colourless
Z = 40.20 × 0.12 × 0.06 mm
Data collection top
XtaLAB Synergy, Dualflex, HyPix
diffractometer
1467 reflections with I > 2σ(I)
Radiation source: micro-focus sealed X-ray tubeRint = 0.027
ω scansθmax = 77.5°, θmin = 4.5°
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2022)
h = 1212
Tmin = 0.513, Tmax = 0.750k = 87
6642 measured reflectionsl = 148
1532 independent reflections
Refinement top
Refinement on F2Primary atom site location: difference Fourier map
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.036Hydrogen site location: difference Fourier map
wR(F2) = 0.097All H-atom parameters refined
S = 1.05 w = 1/[σ2(Fo2) + (0.0501P)2 + 0.606P]
where P = (Fo2 + 2Fc2)/3
1532 reflections(Δ/σ)max = 0.001
127 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = 0.41 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cl10.45324 (5)0.61848 (7)0.86496 (4)0.03447 (18)
O10.06705 (13)0.89161 (17)0.64445 (10)0.0231 (3)
N10.05777 (14)0.7905 (2)0.44644 (12)0.0197 (3)
H10.013 (3)0.890 (4)0.413 (2)0.040 (7)*
N20.11129 (14)0.6437 (2)0.38217 (12)0.0195 (3)
H20.096 (2)0.636 (3)0.300 (2)0.038 (6)*
C30.18687 (16)0.5302 (2)0.45765 (14)0.0189 (3)
C40.18362 (16)0.6035 (2)0.57245 (14)0.0181 (3)
C50.10154 (16)0.7717 (2)0.56311 (13)0.0188 (3)
C60.2560 (2)0.3553 (3)0.41307 (16)0.0254 (4)
H6A0.282 (3)0.372 (4)0.331 (3)0.058 (8)*
H6B0.338 (3)0.328 (5)0.458 (3)0.065 (9)*
H6C0.205 (3)0.250 (5)0.414 (3)0.066 (9)*
C70.25721 (17)0.5342 (2)0.68559 (14)0.0205 (3)
H7A0.194 (2)0.527 (3)0.7508 (18)0.021 (5)*
H7B0.295 (2)0.406 (3)0.676 (2)0.029 (5)*
C80.37260 (18)0.6724 (3)0.71941 (16)0.0254 (4)
H8A0.340 (2)0.807 (4)0.724 (2)0.031 (6)*
H8B0.443 (2)0.665 (4)0.664 (2)0.037 (6)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0401 (3)0.0366 (3)0.0249 (3)0.00431 (18)0.01242 (19)0.00157 (17)
O10.0374 (7)0.0209 (6)0.0110 (5)0.0082 (5)0.0007 (5)0.0010 (4)
N10.0297 (7)0.0180 (7)0.0114 (6)0.0045 (5)0.0008 (5)0.0006 (5)
N20.0278 (7)0.0194 (7)0.0115 (7)0.0026 (5)0.0013 (5)0.0028 (5)
C30.0237 (7)0.0179 (7)0.0153 (7)0.0011 (6)0.0027 (6)0.0008 (6)
C40.0238 (7)0.0177 (7)0.0128 (7)0.0008 (6)0.0024 (6)0.0017 (6)
C50.0273 (8)0.0183 (7)0.0110 (7)0.0002 (6)0.0023 (6)0.0003 (6)
C60.0333 (9)0.0233 (8)0.0198 (9)0.0057 (7)0.0033 (7)0.0036 (7)
C70.0280 (8)0.0192 (8)0.0144 (8)0.0036 (6)0.0015 (6)0.0016 (6)
C80.0264 (8)0.0315 (9)0.0180 (8)0.0006 (7)0.0019 (6)0.0029 (7)
Geometric parameters (Å, º) top
Cl1—C81.8040 (18)C4—C71.496 (2)
O1—C51.2920 (19)C6—H6A0.97 (3)
N1—C51.354 (2)C6—H6B0.95 (3)
N1—N21.3685 (19)C6—H6C0.88 (3)
N1—H10.88 (3)C7—C81.514 (2)
N2—C31.342 (2)C7—H7A0.99 (2)
N2—H20.92 (3)C7—H7B0.97 (2)
C3—C41.382 (2)C8—H8A0.99 (2)
C3—C61.489 (2)C8—H8B0.95 (2)
C4—C51.416 (2)
C5—N1—N2108.95 (13)H6A—C6—H6B105 (2)
C5—N1—H1126.8 (17)C3—C6—H6C113 (2)
N2—N1—H1123.6 (17)H6A—C6—H6C107 (3)
C3—N2—N1108.66 (13)H6B—C6—H6C107 (3)
C3—N2—H2129.9 (15)C4—C7—C8108.91 (14)
N1—N2—H2121.4 (15)C4—C7—H7A110.2 (12)
N2—C3—C4108.96 (14)C8—C7—H7A110.3 (12)
N2—C3—C6120.74 (15)C4—C7—H7B111.5 (13)
C4—C3—C6130.29 (15)C8—C7—H7B108.6 (13)
C3—C4—C5106.22 (14)H7A—C7—H7B107.3 (18)
C3—C4—C7128.97 (15)C7—C8—Cl1112.04 (12)
C5—C4—C7124.69 (14)C7—C8—H8A111.5 (13)
O1—C5—N1122.31 (15)Cl1—C8—H8A105.7 (13)
O1—C5—C4130.49 (14)C7—C8—H8B111.5 (15)
N1—C5—C4107.19 (13)Cl1—C8—H8B106.1 (15)
C3—C6—H6A111.6 (17)H8A—C8—H8B109.7 (19)
C3—C6—H6B111.9 (19)
C5—N1—N2—C30.98 (18)N2—N1—C5—C41.24 (18)
N1—N2—C3—C40.30 (18)C3—C4—C5—O1179.99 (17)
N1—N2—C3—C6178.79 (15)C7—C4—C5—O13.7 (3)
N2—C3—C4—C50.45 (18)C3—C4—C5—N11.04 (18)
C6—C3—C4—C5179.43 (17)C7—C4—C5—N1177.36 (15)
N2—C3—C4—C7176.56 (16)C3—C4—C7—C8105.67 (19)
C6—C3—C4—C74.5 (3)C5—C4—C7—C869.8 (2)
N2—N1—C5—O1179.70 (15)C4—C7—C8—Cl1172.38 (11)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.88 (3)1.81 (3)2.6861 (18)174 (2)
N2—H2···O1ii0.92 (3)1.75 (3)2.6772 (17)177 (2)
Symmetry codes: (i) x, y+2, z+1; (ii) x, y+3/2, z1/2.
Summary of short interatomic contacts (Å) in the title compound top
Cl1···H6B3.121 - x, 1/2 + y, 3/2 - z
Cl1···Cl13.511 - x, 1 - y, 2 - z
H1···O11.80-x, 2 - y, 1 - z
H6C···O12.89-x, 1 - y, 1 - z
O1···H21.76x, 1/2 - y, - 1/2 + z
H6A···H7B2.60x, 1/2 - y, - 1/2 + z
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds