organic compounds
4-(Dimethylamino)phenyl phenyl ketone
aX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia
*Correspondence e-mail: hkfun@usm.my
In the 15H15NO, the two benzene rings are twisted from each other by a dihedral angle of 47.97 (4)°. The is stabilized by weak intermolecular C—H⋯O and C—H⋯π interactions, and π–π interactions with a centroid–centroid distance of 3.8493 (5) Å are observed.
of the title compound, CRelated literature
For related literature on non-linear optical properties of benzophenone, see: Arivanandhan et al. (2006); Szyrszyng et al. (2004); Vijayan et al. (2002) & Wang et al., (2007). For bond-length data see: Allen et al. (1987)
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2005); cell APEX2; data reduction: SAINT (Bruker, 2005); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2003).
Supporting information
10.1107/S1600536808020953/at2585sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808020953/at2585Isup2.hkl
4-(Dimethylamino)benzophenone was purchased from Aldrich and dissolved in ethanol. The solution was allowed to evaporate slowly. Colourless crystals were obtained after a month.
H atoms were positioned geometrically [C—H = 0.93Å and CH3=0.96 Å] and refined using a riding model, with Uiso(H) = 1.2 or 1.5Ueq(C). The rotating group model was considered for the methyl H atoms.
Data collection: APEX2 (Bruker, 2005); cell
APEX2 (Bruker, 2005); data reduction: SAINT (Bruker, 2005); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2003).C15H15NO | F(000) = 480 |
Mr = 225.28 | Dx = 1.275 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 8685 reflections |
a = 13.0575 (3) Å | θ = 3.1–38.7° |
b = 7.7456 (2) Å | µ = 0.08 mm−1 |
c = 12.4931 (3) Å | T = 100 K |
β = 111.717 (1)° | Block, colourless |
V = 1173.85 (5) Å3 | 0.60 × 0.43 × 0.28 mm |
Z = 4 |
Bruker SMART APEXII CCD area-detector diffractometer | 5156 independent reflections |
Radiation source: fine-focus sealed tube | 4138 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.028 |
ϕ and ω scans | θmax = 35.0°, θmin = 3.1° |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | h = −21→19 |
Tmin = 0.939, Tmax = 0.977 | k = −10→12 |
22302 measured reflections | l = −20→20 |
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)] = 0.047 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.138 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0744P)2 + 0.1876P] where P = (Fo2 + 2Fc2)/3 |
5156 reflections | (Δ/σ)max < 0.001 |
156 parameters | Δρmax = 0.42 e Å−3 |
0 restraints | Δρmin = −0.25 e Å−3 |
C15H15NO | V = 1173.85 (5) Å3 |
Mr = 225.28 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 13.0575 (3) Å | µ = 0.08 mm−1 |
b = 7.7456 (2) Å | T = 100 K |
c = 12.4931 (3) Å | 0.60 × 0.43 × 0.28 mm |
β = 111.717 (1)° |
Bruker SMART APEXII CCD area-detector diffractometer | 5156 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | 4138 reflections with I > 2σ(I) |
Tmin = 0.939, Tmax = 0.977 | Rint = 0.028 |
22302 measured reflections |
R[F2 > 2σ(F2)] = 0.047 | 0 restraints |
wR(F2) = 0.138 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.42 e Å−3 |
5156 reflections | Δρmin = −0.25 e Å−3 |
156 parameters |
Experimental. The data was collected with the Oxford Cyrosystem Cobra low-temperature attachment. |
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 | ||
O1 | 0.26958 (5) | 0.42158 (10) | 0.20400 (5) | 0.02533 (15) | |
N1 | −0.10640 (5) | 0.34279 (10) | 0.40740 (6) | 0.01934 (14) | |
C1 | 0.43352 (6) | 0.31796 (11) | 0.49440 (7) | 0.01861 (15) | |
H1 | 0.3933 | 0.3765 | 0.5308 | 0.022* | |
C2 | 0.53797 (7) | 0.25436 (12) | 0.55889 (7) | 0.02153 (16) | |
H2 | 0.5677 | 0.2714 | 0.6382 | 0.026* | |
C3 | 0.59761 (7) | 0.16567 (12) | 0.50493 (8) | 0.02318 (17) | |
H3 | 0.6668 | 0.1215 | 0.5484 | 0.028* | |
C4 | 0.55457 (7) | 0.14235 (12) | 0.38612 (8) | 0.02373 (17) | |
H4 | 0.5948 | 0.0833 | 0.3500 | 0.028* | |
C5 | 0.45115 (7) | 0.20786 (11) | 0.32186 (7) | 0.02078 (16) | |
H5 | 0.4228 | 0.1942 | 0.2423 | 0.025* | |
C6 | 0.38907 (6) | 0.29412 (10) | 0.37532 (7) | 0.01685 (14) | |
C7 | 0.27935 (6) | 0.36465 (10) | 0.29960 (7) | 0.01733 (14) | |
C8 | 0.18415 (6) | 0.36068 (10) | 0.33575 (6) | 0.01575 (14) | |
C9 | 0.08856 (6) | 0.44970 (10) | 0.26790 (7) | 0.01806 (15) | |
H9 | 0.0897 | 0.5141 | 0.2055 | 0.022* | |
C10 | −0.00688 (6) | 0.44473 (11) | 0.29074 (7) | 0.01847 (15) | |
H10 | −0.0687 | 0.5052 | 0.2436 | 0.022* | |
C11 | −0.01199 (6) | 0.34866 (10) | 0.38509 (6) | 0.01540 (14) | |
C12 | 0.08462 (6) | 0.25969 (10) | 0.45427 (6) | 0.01625 (14) | |
H12 | 0.0843 | 0.1963 | 0.5174 | 0.019* | |
C13 | 0.17938 (6) | 0.26547 (10) | 0.42967 (6) | 0.01610 (14) | |
H13 | 0.2414 | 0.2051 | 0.4763 | 0.019* | |
C14 | −0.11461 (7) | 0.24089 (12) | 0.50120 (7) | 0.02242 (16) | |
H14A | −0.0465 | 0.2479 | 0.5664 | 0.034* | |
H14B | −0.1292 | 0.1227 | 0.4773 | 0.034* | |
H14C | −0.1735 | 0.2846 | 0.5220 | 0.034* | |
C15 | −0.20773 (7) | 0.41652 (14) | 0.32699 (8) | 0.02666 (19) | |
H15A | −0.1986 | 0.5387 | 0.3213 | 0.040* | |
H15B | −0.2666 | 0.3950 | 0.3538 | 0.040* | |
H15C | −0.2250 | 0.3646 | 0.2526 | 0.040* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0234 (3) | 0.0354 (4) | 0.0184 (3) | −0.0007 (2) | 0.0091 (2) | 0.0074 (2) |
N1 | 0.0154 (3) | 0.0231 (3) | 0.0193 (3) | 0.0014 (2) | 0.0062 (2) | 0.0022 (2) |
C1 | 0.0176 (3) | 0.0211 (3) | 0.0172 (3) | −0.0011 (3) | 0.0065 (3) | −0.0014 (3) |
C2 | 0.0176 (3) | 0.0274 (4) | 0.0181 (3) | −0.0012 (3) | 0.0049 (3) | 0.0009 (3) |
C3 | 0.0168 (3) | 0.0271 (4) | 0.0261 (4) | 0.0013 (3) | 0.0086 (3) | 0.0050 (3) |
C4 | 0.0208 (3) | 0.0280 (4) | 0.0262 (4) | 0.0017 (3) | 0.0133 (3) | 0.0007 (3) |
C5 | 0.0204 (3) | 0.0254 (4) | 0.0190 (3) | −0.0013 (3) | 0.0102 (3) | −0.0012 (3) |
C6 | 0.0162 (3) | 0.0185 (3) | 0.0166 (3) | −0.0019 (2) | 0.0070 (2) | 0.0003 (2) |
C7 | 0.0183 (3) | 0.0180 (3) | 0.0156 (3) | −0.0021 (2) | 0.0062 (3) | 0.0002 (2) |
C8 | 0.0162 (3) | 0.0163 (3) | 0.0143 (3) | −0.0005 (2) | 0.0051 (2) | 0.0006 (2) |
C9 | 0.0195 (3) | 0.0184 (3) | 0.0152 (3) | 0.0006 (2) | 0.0052 (3) | 0.0031 (2) |
C10 | 0.0176 (3) | 0.0193 (3) | 0.0167 (3) | 0.0026 (2) | 0.0042 (3) | 0.0029 (3) |
C11 | 0.0154 (3) | 0.0149 (3) | 0.0148 (3) | −0.0003 (2) | 0.0043 (2) | −0.0019 (2) |
C12 | 0.0170 (3) | 0.0169 (3) | 0.0148 (3) | 0.0006 (2) | 0.0058 (2) | 0.0016 (2) |
C13 | 0.0158 (3) | 0.0164 (3) | 0.0154 (3) | 0.0013 (2) | 0.0049 (2) | 0.0016 (2) |
C14 | 0.0229 (3) | 0.0252 (4) | 0.0216 (4) | −0.0004 (3) | 0.0112 (3) | 0.0007 (3) |
C15 | 0.0158 (3) | 0.0350 (5) | 0.0267 (4) | 0.0032 (3) | 0.0049 (3) | 0.0048 (3) |
O1—C7 | 1.2346 (10) | C8—C9 | 1.4031 (10) |
N1—C11 | 1.3615 (10) | C8—C13 | 1.4066 (11) |
N1—C14 | 1.4494 (11) | C9—C10 | 1.3781 (11) |
N1—C15 | 1.4499 (11) | C9—H9 | 0.9300 |
C1—C2 | 1.3924 (11) | C10—C11 | 1.4163 (11) |
C1—C6 | 1.3947 (11) | C10—H10 | 0.9300 |
C1—H1 | 0.9300 | C11—C12 | 1.4165 (10) |
C2—C3 | 1.3862 (12) | C12—C13 | 1.3816 (11) |
C2—H2 | 0.9300 | C12—H12 | 0.9300 |
C3—C4 | 1.3907 (13) | C13—H13 | 0.9300 |
C3—H3 | 0.9300 | C14—H14A | 0.9600 |
C4—C5 | 1.3868 (12) | C14—H14B | 0.9600 |
C4—H4 | 0.9300 | C14—H14C | 0.9600 |
C5—C6 | 1.3965 (11) | C15—H15A | 0.9600 |
C5—H5 | 0.9300 | C15—H15B | 0.9600 |
C6—C7 | 1.4976 (11) | C15—H15C | 0.9600 |
C7—C8 | 1.4716 (11) | ||
C11—N1—C14 | 121.81 (7) | C10—C9—C8 | 122.12 (7) |
C11—N1—C15 | 120.55 (7) | C10—C9—H9 | 118.9 |
C14—N1—C15 | 116.94 (7) | C8—C9—H9 | 118.9 |
C2—C1—C6 | 120.15 (8) | C9—C10—C11 | 120.77 (7) |
C2—C1—H1 | 119.9 | C9—C10—H10 | 119.6 |
C6—C1—H1 | 119.9 | C11—C10—H10 | 119.6 |
C3—C2—C1 | 120.02 (8) | N1—C11—C10 | 120.86 (7) |
C3—C2—H2 | 120.0 | N1—C11—C12 | 121.89 (7) |
C1—C2—H2 | 120.0 | C10—C11—C12 | 117.25 (7) |
C2—C3—C4 | 120.36 (8) | C13—C12—C11 | 121.14 (7) |
C2—C3—H3 | 119.8 | C13—C12—H12 | 119.4 |
C4—C3—H3 | 119.8 | C11—C12—H12 | 119.4 |
C5—C4—C3 | 119.52 (8) | C12—C13—C8 | 121.49 (7) |
C5—C4—H4 | 120.2 | C12—C13—H13 | 119.3 |
C3—C4—H4 | 120.2 | C8—C13—H13 | 119.3 |
C4—C5—C6 | 120.76 (8) | N1—C14—H14A | 109.5 |
C4—C5—H5 | 119.6 | N1—C14—H14B | 109.5 |
C6—C5—H5 | 119.6 | H14A—C14—H14B | 109.5 |
C1—C6—C5 | 119.17 (7) | N1—C14—H14C | 109.5 |
C1—C6—C7 | 123.28 (7) | H14A—C14—H14C | 109.5 |
C5—C6—C7 | 117.47 (7) | H14B—C14—H14C | 109.5 |
O1—C7—C8 | 120.51 (7) | N1—C15—H15A | 109.5 |
O1—C7—C6 | 118.26 (7) | N1—C15—H15B | 109.5 |
C8—C7—C6 | 121.18 (7) | H15A—C15—H15B | 109.5 |
C9—C8—C13 | 117.23 (7) | N1—C15—H15C | 109.5 |
C9—C8—C7 | 117.90 (7) | H15A—C15—H15C | 109.5 |
C13—C8—C7 | 124.76 (7) | H15B—C15—H15C | 109.5 |
C6—C1—C2—C3 | −0.63 (13) | C6—C7—C8—C13 | −12.54 (12) |
C1—C2—C3—C4 | 1.18 (13) | C13—C8—C9—C10 | −0.33 (12) |
C2—C3—C4—C5 | −0.29 (14) | C7—C8—C9—C10 | 175.94 (7) |
C3—C4—C5—C6 | −1.15 (13) | C8—C9—C10—C11 | 0.20 (12) |
C2—C1—C6—C5 | −0.79 (12) | C14—N1—C11—C10 | 177.99 (7) |
C2—C1—C6—C7 | −177.50 (7) | C15—N1—C11—C10 | 7.82 (12) |
C4—C5—C6—C1 | 1.69 (12) | C14—N1—C11—C12 | −1.90 (12) |
C4—C5—C6—C7 | 178.59 (8) | C15—N1—C11—C12 | −172.07 (8) |
C1—C6—C7—O1 | 141.72 (9) | C9—C10—C11—N1 | −179.62 (7) |
C5—C6—C7—O1 | −35.04 (11) | C9—C10—C11—C12 | 0.27 (11) |
C1—C6—C7—C8 | −40.56 (11) | N1—C11—C12—C13 | 179.28 (7) |
C5—C6—C7—C8 | 142.68 (8) | C10—C11—C12—C13 | −0.61 (11) |
O1—C7—C8—C9 | −10.84 (12) | C11—C12—C13—C8 | 0.49 (12) |
C6—C7—C8—C9 | 171.49 (7) | C9—C8—C13—C12 | −0.02 (11) |
O1—C7—C8—C13 | 165.13 (8) | C7—C8—C13—C12 | −176.00 (7) |
D—H···A | D—H | H···A | D···A | D—H···A |
C4—H4···O1i | 0.93 | 2.46 | 3.3730 (12) | 168 |
C10—H10···Cg2ii | 0.93 | 2.98 | 3.6452 (9) | 130 |
Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) −x, y+1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C15H15NO |
Mr | 225.28 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 100 |
a, b, c (Å) | 13.0575 (3), 7.7456 (2), 12.4931 (3) |
β (°) | 111.717 (1) |
V (Å3) | 1173.85 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.08 |
Crystal size (mm) | 0.60 × 0.43 × 0.28 |
Data collection | |
Diffractometer | Bruker SMART APEXII CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2005) |
Tmin, Tmax | 0.939, 0.977 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 22302, 5156, 4138 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.807 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.047, 0.138, 1.06 |
No. of reflections | 5156 |
No. of parameters | 156 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.42, −0.25 |
Computer programs: APEX2 (Bruker, 2005), SAINT (Bruker, 2005), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2003).
D—H···A | D—H | H···A | D···A | D—H···A |
C4—H4···O1i | 0.93 | 2.46 | 3.3730 (12) | 168 |
C10—H10···Cg2ii | 0.93 | 2.98 | 3.6452 (9) | 130 |
Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) −x, y+1/2, −z+1/2. |
Footnotes
‡Permanent address: Department of Physics, Karunya University, Karunya Nagar, Coimbatore 641 114, India.
Acknowledgements
The authors thank the Malaysian Government and Universiti Sains Malaysia for the Science Fund grant No. 305/PFIZIK/613312. SRJ thanks Universiti Sains Malaysia for a post-doctoral research fellowship.
References
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Benzophenone and its derivatives exhibits non-linear optical properties (Wang et al., 2007; Vijayan et al., 2002 & Arivanandhan et al., 2006) and are good candidates for the non-linear optical applications (Szyrszyng et al., 2004). In view of the importance of the benzophenone derivatives, the crystal structure of the title compound (I) has been elucidated.
The asymmetric unit of (I) consists of one molecule of 4-(dimethylamino)benzophenone. Bond lengths and angles in the molecule are found to have normal values (Allen et al., 1987) The dihedral angle formed by the rings (C1–C6) and (C8–C13) is 47.97 (4)° indicating that the rings are twisted from each other. The crystal packing (Fig.2) is consolidated by intermolecular C—H···O hydrogen bonds and C—H···π interactions. π–π interactions with the centroid to centroid distance of 3.8493 (5)Å are observed.