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The crystal structure of the title compound, C23H18N2O2, contains an intra­molecular hydrogen bond that links the ketone and hydroxyl groups.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805039401/ww6392sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805039401/ww6392Isup2.hkl
Contains datablock I

CCDC reference: 296697

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.036
  • wR factor = 0.096
  • Data-to-parameter ratio = 13.3

checkCIF/PLATON results

No syntax errors found



Alert level C CELLV02_ALERT_1_C The supplied cell volume s.u. differs from that calculated from the cell parameter s.u.'s by > 2 Calculated cell volume su = 17.35 Cell volume su given = 21.00 PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ?
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 2 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 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

Pyrazol-5-one and its derivatives are widely used as biologically active compounds, metal extractants, dyes etc. (Ono et al., 1997). The tautomeric structures of these compounds have been extensively studied (Kataeva et al., 2002; Akama et al., 1996; Katritzky et al., 1964). For 4-acyl-substituted pyrazol-5-ones, two forms are stable in the solid state. These are the OH-form (A), stabilized by an intramolecular hydrogen bond, and the NH-form (B), stabilized by an intermolecular hydrogen bond (see scheme) (Kataeva et al., 2002). The X-ray crystal structure analysis of the title compound, (I), was undertaken in order to study its stereochemistry and crystal packing.

The present X-ray single-crystal study of compound (I) shows (Fig. 1) that it exists in the OH-tautomeric form.

Experimental top

The title compound was synthesized according to the method proposed by Jensen (1959) (yield 86%, m.p. 465–466 K). Analysis, required for C23H18N2O2: C 77.95, H 5.12, N 7.90%; found: C 77.62, H 5.34, N 7.92%. Plate-like single crystals of (I) were grown from a mixed solution of methanol and dichloromethane (Ratio?) by slow evaporation.

Refinement top

The H atom on atom O1 was located in a difference Fourier map. The O1—H1O distance was restrained to about 0.82 Å [0.898</span><span style=" font-weight:600;">(19) in CIF?] and the distance between atoms C7 and H1O was retrained to about 1.9(s.u.?) Å. The disorder for some H atoms on C23 was constrained by the instruction HFIX 123, which showed only 0.5 occupancy (H23A–H23F). The other H atoms were added by geometry, with C—H bond distances of 0.93 (aromatic) or 0.96 Å (for the CH3 group), and all H atoms were refined isotropically.

Computing details top

Data collection: XSCANS (Siemens, 1994); cell refinement: XSCANS; data reduction: SHELXTL (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. A view of the molecule of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. A packing diagram for (I), showing the dimers.
5-Hydroxy-4-(4-methylbenzoyl)-1,3-diphenyl-1H-pyrazole top
Crystal data top
C23H18N2O2Z = 2
Mr = 354.39F(000) = 372
Triclinic, P1Dx = 1.278 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.705 (1) ÅCell parameters from 28 reflections
b = 10.0821 (9) Åθ = 3.9–15.0°
c = 10.746 (1) ŵ = 0.08 mm1
α = 115.284 (8)°T = 294 K
β = 102.13 (1)°Plate, colourless
γ = 91.61 (1)°0.30 × 0.28 × 0.26 mm
V = 921.2 (2) Å3
Data collection top
Siemens P4
diffractometer
Rint = 0.009
Radiation source: normal-focus sealed tubeθmax = 25.3°, θmin = 2.2°
Graphite monochromatorh = 011
ω scansk = 1111
4049 measured reflectionsl = 1212
3307 independent reflections3 standard reflections every 97 reflections
2233 reflections with I > 2σ(I) intensity decay: 4.8%
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)] = 0.037H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.096 w = 1/[σ2(Fo2) + (0.0522P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.97(Δ/σ)max < 0.001
3307 reflectionsΔρmax = 0.16 e Å3
249 parametersΔρmin = 0.12 e Å3
2 restraintsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.045 (4)
Crystal data top
C23H18N2O2γ = 91.61 (1)°
Mr = 354.39V = 921.2 (2) Å3
Triclinic, P1Z = 2
a = 9.705 (1) ÅMo Kα radiation
b = 10.0821 (9) ŵ = 0.08 mm1
c = 10.746 (1) ÅT = 294 K
α = 115.284 (8)°0.30 × 0.28 × 0.26 mm
β = 102.13 (1)°
Data collection top
Siemens P4
diffractometer
Rint = 0.009
4049 measured reflections3 standard reflections every 97 reflections
3307 independent reflections intensity decay: 4.8%
2233 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0372 restraints
wR(F2) = 0.096H atoms treated by a mixture of independent and constrained refinement
S = 0.97Δρmax = 0.16 e Å3
3307 reflectionsΔρmin = 0.12 e Å3
249 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 > 2σ(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
xyzUiso*/UeqOcc. (<1)
O10.53443 (13)0.68831 (13)0.19927 (11)0.0623 (3)
O20.35647 (13)0.83941 (13)0.32274 (12)0.0708 (4)
N10.68695 (13)0.61547 (14)0.35100 (12)0.0520 (3)
N20.71040 (13)0.63278 (14)0.48968 (12)0.0528 (3)
C10.73782 (19)0.4586 (2)0.12434 (16)0.0664 (5)
H10.64240.44670.07890.080*
C20.8348 (2)0.3901 (2)0.04805 (18)0.0799 (6)
H20.80450.33290.04960.096*
C30.9750 (2)0.4057 (2)0.1150 (2)0.0844 (6)
H31.03950.35850.06320.101*
C41.0197 (2)0.4910 (2)0.2582 (2)0.0901 (7)
H41.11500.50160.30360.108*
C50.92513 (19)0.5617 (2)0.33635 (19)0.0746 (5)
H50.95610.62010.43380.090*
C60.78463 (17)0.54439 (17)0.26812 (15)0.0533 (4)
C70.57692 (16)0.68320 (16)0.32192 (14)0.0478 (4)
C80.51969 (15)0.74366 (15)0.44019 (14)0.0452 (4)
C90.61152 (16)0.70866 (16)0.54247 (14)0.0451 (4)
C100.61703 (14)0.75032 (16)0.69331 (14)0.0439 (4)
C110.62524 (16)0.64372 (18)0.74239 (16)0.0539 (4)
H110.62220.54510.67910.065*
C120.63783 (18)0.6819 (2)0.88412 (18)0.0654 (5)
H120.64220.60910.91570.079*
C130.64387 (18)0.8269 (2)0.97814 (17)0.0688 (5)
H130.65250.85291.07380.083*
C140.63716 (19)0.9340 (2)0.93079 (16)0.0659 (5)
H140.64261.03270.99500.079*
C150.62256 (17)0.89636 (18)0.78947 (16)0.0549 (4)
H150.61640.96950.75830.066*
C160.39436 (16)0.81483 (16)0.43021 (15)0.0497 (4)
C170.30364 (15)0.85520 (16)0.53170 (15)0.0476 (4)
C180.22801 (17)0.97470 (18)0.54930 (17)0.0582 (4)
H180.23981.03060.50140.070*
C190.13562 (19)1.0110 (2)0.63714 (19)0.0676 (5)
H190.08871.09340.65030.081*
C200.11181 (17)0.9268 (2)0.70582 (17)0.0654 (5)
C210.18616 (18)0.8073 (2)0.68691 (17)0.0625 (5)
H210.17150.74940.73230.075*
C220.28165 (16)0.77185 (18)0.60216 (15)0.0534 (4)
H220.33140.69190.59230.064*
C230.0065 (2)0.9634 (3)0.7970 (2)0.0995 (7)
H23A0.03441.04920.79770.119*0.50
H23B0.05430.98300.89210.119*0.50
H23C0.06730.88120.75920.119*0.50
H23D0.00280.89310.83490.119*0.50
H23E0.08590.95920.74050.119*0.50
H23F0.03571.06110.87350.119*0.50
H1O0.4642 (18)0.745 (2)0.2034 (16)0.113 (8)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0720 (8)0.0786 (8)0.0433 (6)0.0150 (7)0.0137 (5)0.0332 (6)
O20.0825 (9)0.0894 (9)0.0601 (7)0.0301 (7)0.0193 (6)0.0493 (7)
N10.0530 (8)0.0657 (9)0.0365 (7)0.0106 (7)0.0114 (6)0.0215 (6)
N20.0536 (8)0.0665 (9)0.0376 (7)0.0124 (7)0.0115 (6)0.0220 (6)
C10.0585 (11)0.0902 (13)0.0456 (9)0.0132 (10)0.0147 (8)0.0247 (9)
C20.0768 (14)0.1062 (16)0.0491 (10)0.0182 (12)0.0259 (10)0.0223 (10)
C30.0682 (14)0.1074 (16)0.0739 (13)0.0190 (12)0.0368 (11)0.0275 (12)
C40.0496 (11)0.1121 (17)0.0800 (14)0.0084 (11)0.0164 (10)0.0160 (12)
C50.0542 (11)0.0875 (13)0.0556 (10)0.0065 (10)0.0102 (9)0.0090 (9)
C60.0519 (10)0.0623 (10)0.0441 (9)0.0069 (8)0.0165 (7)0.0200 (8)
C70.0511 (9)0.0542 (9)0.0387 (8)0.0028 (7)0.0076 (7)0.0230 (7)
C80.0485 (9)0.0480 (9)0.0379 (8)0.0030 (7)0.0076 (7)0.0196 (7)
C90.0443 (9)0.0485 (9)0.0392 (8)0.0021 (7)0.0075 (7)0.0179 (7)
C100.0381 (8)0.0549 (9)0.0381 (8)0.0051 (7)0.0066 (6)0.0214 (7)
C110.0543 (10)0.0581 (10)0.0501 (9)0.0042 (8)0.0080 (7)0.0271 (8)
C120.0637 (11)0.0855 (13)0.0586 (11)0.0021 (10)0.0099 (9)0.0453 (10)
C130.0633 (11)0.0999 (15)0.0393 (9)0.0029 (10)0.0083 (8)0.0300 (10)
C140.0725 (12)0.0688 (12)0.0443 (9)0.0037 (9)0.0164 (8)0.0133 (9)
C150.0610 (10)0.0574 (10)0.0468 (9)0.0093 (8)0.0145 (8)0.0229 (8)
C160.0529 (10)0.0495 (9)0.0451 (8)0.0032 (7)0.0066 (7)0.0223 (7)
C170.0422 (9)0.0501 (9)0.0438 (8)0.0034 (7)0.0024 (7)0.0185 (7)
C180.0528 (10)0.0579 (10)0.0588 (10)0.0080 (8)0.0054 (8)0.0249 (8)
C190.0540 (11)0.0664 (11)0.0664 (11)0.0162 (9)0.0073 (9)0.0176 (9)
C200.0457 (10)0.0814 (13)0.0515 (10)0.0044 (9)0.0071 (8)0.0156 (9)
C210.0532 (10)0.0774 (12)0.0566 (10)0.0012 (9)0.0131 (8)0.0299 (9)
C220.0483 (9)0.0594 (10)0.0511 (9)0.0062 (8)0.0079 (7)0.0253 (8)
C230.0721 (14)0.1312 (19)0.0836 (14)0.0186 (13)0.0345 (12)0.0298 (14)
Geometric parameters (Å, º) top
O1—C71.3193 (16)C12—C131.367 (2)
O1—H1O0.898 (19)C12—H120.9300
O2—C161.2655 (17)C13—C141.374 (2)
N1—C71.3369 (19)C13—H130.9300
N1—N21.3915 (16)C14—C151.373 (2)
N1—C61.4330 (19)C14—H140.9300
N2—C91.3142 (18)C15—H150.9300
C1—C61.372 (2)C16—C171.475 (2)
C1—C21.383 (2)C17—C221.388 (2)
C1—H10.9300C17—C181.393 (2)
C2—C31.368 (3)C18—C191.381 (2)
C2—H20.9300C18—H180.9300
C3—C41.365 (3)C19—C201.384 (3)
C3—H30.9300C19—H190.9300
C4—C51.380 (2)C20—C211.384 (2)
C4—H40.9300C20—C231.508 (2)
C5—C61.373 (2)C21—C221.382 (2)
C5—H50.9300C21—H210.9300
C7—C81.3962 (19)C22—H220.9300
C8—C91.4366 (19)C23—H23A0.9600
C8—C161.437 (2)C23—H23B0.9600
C9—C101.4791 (18)C23—H23C0.9600
C10—C111.382 (2)C23—H23D0.9600
C10—C151.383 (2)C23—H23E0.9600
C11—C121.379 (2)C23—H23F0.9600
C11—H110.9300
C7—O1—H1O109.5 (9)C13—C14—H14119.7
C7—N1—N2110.47 (11)C14—C15—C10120.34 (15)
C7—N1—C6130.20 (12)C14—C15—H15119.8
N2—N1—C6119.06 (12)C10—C15—H15119.8
C9—N2—N1106.01 (12)O2—C16—C8117.03 (13)
C6—C1—C2118.97 (16)O2—C16—C17117.74 (13)
C6—C1—H1120.5C8—C16—C17125.17 (13)
C2—C1—H1120.5C22—C17—C18118.39 (15)
C3—C2—C1120.61 (17)C22—C17—C16122.59 (14)
C3—C2—H2119.7C18—C17—C16118.82 (14)
C1—C2—H2119.7C19—C18—C17120.69 (16)
C4—C3—C2119.67 (17)C19—C18—H18119.7
C4—C3—H3120.2C17—C18—H18119.7
C2—C3—H3120.2C18—C19—C20121.03 (16)
C3—C4—C5120.78 (18)C18—C19—H19119.5
C3—C4—H4119.6C20—C19—H19119.5
C5—C4—H4119.6C21—C20—C19118.04 (16)
C6—C5—C4119.00 (17)C21—C20—C23121.15 (19)
C6—C5—H5120.5C19—C20—C23120.80 (18)
C4—C5—H5120.5C22—C21—C20121.54 (17)
C1—C6—C5120.96 (15)C22—C21—H21119.2
C1—C6—N1120.57 (14)C20—C21—H21119.2
C5—C6—N1118.46 (14)C21—C22—C17120.27 (15)
O1—C7—N1123.18 (13)C21—C22—H22119.9
O1—C7—C8128.05 (14)C17—C22—H22119.9
N1—C7—C8108.77 (12)C20—C23—H23A109.5
C7—C8—C9103.31 (13)C20—C23—H23B109.5
C7—C8—C16118.56 (13)H23A—C23—H23B109.5
C9—C8—C16138.11 (13)C20—C23—H23C109.5
N2—C9—C8111.39 (12)H23A—C23—H23C109.5
N2—C9—C10117.21 (12)H23B—C23—H23C109.5
C8—C9—C10131.29 (13)C20—C23—H23D109.5
C11—C10—C15118.62 (13)H23A—C23—H23D141.1
C11—C10—C9120.08 (13)H23B—C23—H23D56.3
C15—C10—C9121.19 (13)H23C—C23—H23D56.3
C12—C11—C10120.79 (15)C20—C23—H23E109.5
C12—C11—H11119.6H23A—C23—H23E56.3
C10—C11—H11119.6H23B—C23—H23E141.1
C13—C12—C11119.95 (16)H23C—C23—H23E56.3
C13—C12—H12120.0H23D—C23—H23E109.5
C11—C12—H12120.0C20—C23—H23F109.5
C12—C13—C14119.78 (15)H23A—C23—H23F56.3
C12—C13—H13120.1H23B—C23—H23F56.3
C14—C13—H13120.1H23C—C23—H23F141.1
C15—C14—C13120.51 (16)H23D—C23—H23F109.5
C15—C14—H14119.7H23E—C23—H23F109.5
C7—N1—N2—C91.36 (17)C8—C9—C10—C11132.21 (16)
C6—N1—N2—C9176.03 (13)N2—C9—C10—C15124.20 (16)
C6—C1—C2—C30.9 (3)C8—C9—C10—C1551.6 (2)
C1—C2—C3—C40.7 (3)C15—C10—C11—C120.4 (2)
C2—C3—C4—C50.1 (4)C9—C10—C11—C12176.64 (14)
C3—C4—C5—C60.4 (3)C10—C11—C12—C130.7 (2)
C2—C1—C6—C50.5 (3)C11—C12—C13—C140.1 (3)
C2—C1—C6—N1179.15 (15)C12—C13—C14—C150.9 (3)
C4—C5—C6—C10.1 (3)C13—C14—C15—C101.2 (3)
C4—C5—C6—N1178.55 (17)C11—C10—C15—C140.6 (2)
C7—N1—C6—C140.2 (3)C9—C10—C15—C14175.65 (15)
N2—N1—C6—C1146.30 (15)C7—C8—C16—O211.0 (2)
C7—N1—C6—C5141.11 (18)C9—C8—C16—O2171.10 (16)
N2—N1—C6—C532.4 (2)C7—C8—C16—C17166.13 (14)
N2—N1—C7—O1177.74 (13)C9—C8—C16—C1711.7 (3)
C6—N1—C7—O13.8 (3)O2—C16—C17—C22143.95 (15)
N2—N1—C7—C82.25 (17)C8—C16—C17—C2233.2 (2)
C6—N1—C7—C8176.15 (14)O2—C16—C17—C1830.8 (2)
O1—C7—C8—C9177.86 (15)C8—C16—C17—C18152.03 (14)
N1—C7—C8—C92.12 (16)C22—C17—C18—C191.3 (2)
O1—C7—C8—C163.6 (2)C16—C17—C18—C19176.29 (14)
N1—C7—C8—C16176.40 (13)C17—C18—C19—C202.4 (2)
N1—N2—C9—C80.05 (16)C18—C19—C20—C211.7 (2)
N1—N2—C9—C10176.59 (12)C18—C19—C20—C23177.57 (16)
C7—C8—C9—N21.33 (16)C19—C20—C21—C220.0 (2)
C16—C8—C9—N2176.73 (17)C23—C20—C21—C22179.23 (16)
C7—C8—C9—C10174.70 (15)C20—C21—C22—C171.0 (2)
C16—C8—C9—C107.2 (3)C18—C17—C22—C210.3 (2)
N2—C9—C10—C1151.95 (19)C16—C17—C22—C21174.45 (14)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1O···O20.90 (2)1.79 (1)2.5394 (16)139 (1)
C15—H15···O2i0.932.463.378 (2)170
Symmetry code: (i) x+1, y+2, z+1.

Experimental details

Crystal data
Chemical formulaC23H18N2O2
Mr354.39
Crystal system, space groupTriclinic, P1
Temperature (K)294
a, b, c (Å)9.705 (1), 10.0821 (9), 10.746 (1)
α, β, γ (°)115.284 (8), 102.13 (1), 91.61 (1)
V3)921.2 (2)
Z2
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.30 × 0.28 × 0.26
Data collection
DiffractometerSiemens P4
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
4049, 3307, 2233
Rint0.009
(sin θ/λ)max1)0.600
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.037, 0.096, 0.97
No. of reflections3307
No. of parameters249
No. of restraints2
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.16, 0.12

Computer programs: XSCANS (Siemens, 1994), XSCANS, SHELXTL (Bruker, 1998), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL.

Selected geometric parameters (Å, º) top
O1—C71.3193 (16)N2—C91.3142 (18)
O2—C161.2655 (17)C7—C81.3962 (19)
N1—C71.3369 (19)C8—C91.4366 (19)
N1—N21.3915 (16)
C7—N1—N2110.47 (11)C7—C8—C9103.31 (13)
C9—N2—N1106.01 (12)C7—C8—C16118.56 (13)
O1—C7—N1123.18 (13)N2—C9—C8111.39 (12)
O1—C7—C8128.05 (14)O2—C16—C8117.03 (13)
N1—C7—C8108.77 (12)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1O···O20.898 (19)1.794 (14)2.5394 (16)138.7 (12)
C15—H15···O2i0.932.463.378 (2)170
Symmetry code: (i) x+1, y+2, z+1.
 

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