organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

3-(m-Tol­yl­oxy)phthalo­nitrile

aDepartment of Chemistry, Hebei Normal University of Science and Technology, Qinhuangdao, Hebei Province 066004, People's Republic of China, and bDepartment of Chemistry, Beijing University of Chemical Technology, Beijing 100029, People's Republic of China
*Correspondence e-mail: zhangxianfu@tsinghua.org.cn

(Received 1 December 2007; accepted 22 December 2007; online 9 January 2008)

In the mol­ecule of the title compound, C15H10N2O, the dihedral angle between the two benzene rings is 65.49 (9)°.

Related literature

For the synthesis of a related compound, see: Sharman & van Lier (2003[Sharman, W. M. & van Lier, J. E. (2003). The Porphyrin Handbook, Vol. 15, edited by K. M. Kadish, K. M. Smith & G. Guilard, pp. 1-60. New York: Academic Press.]). For the crystal structure of an isomer of the title compound see: Ocak Ískeleli (2007[Ocak Ískeleli, N. (2007). Acta Cryst. E63, o997-o998.]). For related literature, see: Atalay et al. (2003[Atalay, Ş., Ağar, A., Akdemir, N. & Ağar, E. (2003). Acta Cryst. E59, o1111-o1112.], 2004[Atalay, Ş., Çoruh, U., Akdemir, N. & Ağar, E. (2004). Acta Cryst. E60, o303-o305.]); Cave et al. (1986[Cave, R. J., Siders, P. & Marcus, R. A. (1986). J. Phys. Chem. 90, 1436-1439.]); Koysal et al. (2004[Köysal, Y., Işık, Ş., Akdemir, N., Ağar, E. & Kantar, C. (2004). Acta Cryst. E60, o930-o931.]); Leznoff & Lever (1989–1996[Leznoff, C. C. & Lever, A. B. P. (1989-1996). Phthalocyanines: Properties and Applications , Vol. 1. pp. 1-20. Weinheim/New York: VCH Publishers Inc.]); McKeown (1998[McKeown, N. B. (1998). Phthalocyanine Materials: Synthesis, Structure and Function. pp. 12-30. Cambridge University Press.]); Ocak et al. (2003[Ocak, N., Ağar, A., Akdemir, N., Ağar, E., García-Granda, S. & Erdönmez, A. (2003). Acta Cryst. E59, o1000-o1001.]).

[Scheme 1]

Experimental

Crystal data
  • C15H10N2O

  • Mr = 234.25

  • Orthorhombic, P b c a

  • a = 25.514 (3) Å

  • b = 14.6064 (18) Å

  • c = 6.6109 (6) Å

  • V = 2463.7 (5) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 295 (2) K

  • 0.6 × 0.5 × 0.3 mm

Data collection
  • Bruker P4 diffractometer

  • Absorption correction: none

  • 3094 measured reflections

  • 2254 independent reflections

  • 1372 reflections with I > 2σ(I)

  • Rint = 0.041

  • 3 standard reflections every 97 reflections intensity decay: none

Refinement
  • R[F2 > 2σ(F2)] = 0.054

  • wR(F2) = 0.109

  • S = 1.04

  • 2254 reflections

  • 165 parameters

  • H-atom parameters constrained

  • Δρmax = 0.21 e Å−3

  • Δρmin = −0.23 e Å−3

Data collection: XSCANS (Bruker, 1997[Bruker. (1997). SHELXTL and XSCANS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: XSCANS; data reduction: XSCANS; program(s) used to solve structure: SHELXTL (Bruker, 1997[Bruker. (1997). SHELXTL and XSCANS. Bruker AXS Inc., Madison, Wisconsin, USA.]); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

Phthalonitriles are among the most important precusors of phthalocyanine materials (Leznoff, 1989–1986). Mono phenyloxyphthalonitriles have been used for preparing symetrical phthalocyanines and subphthalocyanines which have been applied in many areas, such as laser printing, photocopying, optical data storage, catalyst etc. (McKeown, 1998). The 3–(m–tolyloxy)phthalonitrile (I), which contains an electron–donating moiety and a strong electron–accepting fragment linked by an oxygen atom, is also a good model suitable for the study of photoinduced electron transfer between the short linked donor and acceptor. The rate of such electron transfer process and the lifetime of the resultant charge separation state, however, are highly dependent on the relative orientation between the donor and the acceptor (Cave, 1986). The crystal structure of the title compound, (I), can therefore provide very helpful information for it.

The triple bond lengths between C and N, both 1.140 (3)Å and 1.133 (3) Å, as shown in Fig. 1, agree with literature values (Ocak et al., 2003). The geometry around the O atoms is in good agreement with the literature (Atalay et al., 2003, 2004; Koysal et al., 2004). The dihedral angle between the two aromatic rings planes is 65.49 (9)°. The crystal structure of compound involves extensive intermolecular ππ interactions, as can be seen from the packing diagram (Fig. 2). Phthalonitrile moieties are packed shoulder by shoulder along the a–axis which is stablized by the intermolecular dipole–dipole interactions and partial face–to–face ππ overlaping along the c–axis, while the toluene moieties are arranged by face to face ππ stacking along the b–axis and shouler by shoulder along the c–axis within the distance 4.15–4.20 Å. It is worth noting that the structure of the isomeric 4–(m–tolyloxy)phthalonitrile is monoclinic (Ocak Ískeleli, 2007) while the title compound report herein is orthorhombic.

Related literature top

For the synthesis of a related compound, see: Sharman & van Lier (2003). For the crystal structure of an isomer of the title compound see: Ocak (2007). For related literature, see: Atalay et al. (2003, 2004); Cave et al. (1986); Koysal et al. (2004); Leznoff & Lever (1989–1996); McKeown (1998); Ocak et al. (2003).

Experimental top

The m–cresol (1.56 g, 14.4 mmol) and 3–nitrophthalonitrile (1.60 g, 9.3 mmol) were dissolved in dry DMF (30 ml) with stirring under N2. Dry fine–powdered potassium carbonate (2.5 g, 18.1 mmol) was added in portions evenly every 10 min. The reaction mixture was stirred for 48 h at room temperature and poured into iced water (150 g). The product was filtered off and washed with (10% w/w) NaOH solution and water until the filtrate was neutral. Recrystallization from ethanol gave a white product (yield 1.2 g, 55%). Single crystals were obtained from absolute ethanol at room temperature via slow evaporation (m.p. 374–375 K). IR data (νmax/cm-1): 3086 (Ar—H), 2980–2950 (CH3), 2229 (CN). 1H NMR data (p.p.m.): 2.34 (s,3H), 7.00–7.05 (d, 1H), 7.07 (s, 1H), 7.12–7.17 (d, 1H), 7.24–7.29 (dd, 1H), 7.35–7.42 (t, 1H), 7.81–7.84 (d, 1H), 7.84–7.85 (d, 1H).

Refinement top

All H atoms were positioned geometrically and refined using a riding model, with C—H = 0.96 Å (CH3) and C—H = 0.93 Å (CH) with Uiso(H) = 1.2Ueq (parent C) (for CH) or Uiso(H) = 1.5Ueq (parent C) (for CH3).

Computing details top

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

Figures top
[Figure 1] Fig. 1. The molecular structure of title compound with the atom numbering scheme. Displacement ellipsoids are drawn at 35% probability level. Hydrogen atoms are presented as spheres of arbitrary radius.
[Figure 2] Fig. 2. The packing of (I), viewed down the c–axis.
3-(m-Tolyloxy)phthalonitrile top
Crystal data top
C15H10N2ODx = 1.263 Mg m3
Mr = 234.25Melting point: 374 K
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 58 reflections
a = 25.514 (3) Åθ = 2.8–25.5°
b = 14.6064 (18) ŵ = 0.08 mm1
c = 6.6109 (6) ÅT = 295 K
V = 2463.7 (5) Å3Prism, colourless
Z = 80.6 × 0.5 × 0.3 mm
F(000) = 976
Data collection top
Bruker P4
diffractometer
Rint = 0.041
Radiation source: fine–focus sealed tubeθmax = 25.5°, θmin = 2.1°
Graphite monochromatorh = 301
ω scansk = 171
3094 measured reflectionsl = 18
2254 independent reflections3 standard reflections every 97 reflections
1372 reflections with I > 2σ(I) intensity decay: none
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)] = 0.054H-atom parameters constrained
wR(F2) = 0.109 w = 1/[σ2(Fo2) + (0.001P)2 + 2.2P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
2254 reflectionsΔρmax = 0.21 e Å3
165 parametersΔρmin = 0.23 e Å3
0 restraintsExtinction correction: SHELXTL (Bruker, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00028 (6)
Crystal data top
C15H10N2OV = 2463.7 (5) Å3
Mr = 234.25Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 25.514 (3) ŵ = 0.08 mm1
b = 14.6064 (18) ÅT = 295 K
c = 6.6109 (6) Å0.6 × 0.5 × 0.3 mm
Data collection top
Bruker P4
diffractometer
Rint = 0.041
3094 measured reflections3 standard reflections every 97 reflections
2254 independent reflections intensity decay: none
1372 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0540 restraints
wR(F2) = 0.109H-atom parameters constrained
S = 1.04Δρmax = 0.21 e Å3
2254 reflectionsΔρmin = 0.23 e Å3
165 parameters
Special details top

Geometry. All s.u.'s (except the s.u.'s in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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*/Ueq
O10.65134 (6)0.53717 (13)0.7428 (3)0.0755 (6)
N10.43352 (8)0.42711 (17)0.7588 (4)0.0682 (7)
N20.57804 (9)0.33811 (18)0.7422 (5)0.0842 (8)
C10.46678 (9)0.47844 (18)0.7550 (4)0.0532 (6)
C20.57161 (9)0.41537 (19)0.7437 (4)0.0570 (7)
C30.50933 (9)0.54397 (17)0.7508 (4)0.0510 (6)
C40.56143 (9)0.51093 (16)0.7447 (4)0.0499 (6)
C50.60184 (9)0.57428 (18)0.7405 (4)0.0568 (6)
C60.59127 (11)0.66675 (19)0.7441 (5)0.0678 (8)
H6A0.61870.70860.74290.081*
C70.54050 (11)0.69742 (19)0.7495 (5)0.0708 (8)
H7A0.53380.76000.75140.085*
C80.49907 (11)0.63599 (19)0.7523 (4)0.0634 (7)
H8A0.46470.65710.75510.076*
C90.69296 (10)0.58418 (18)0.6486 (5)0.0641 (8)
C100.74003 (9)0.58177 (18)0.7517 (5)0.0647 (7)
H10A0.74230.55520.87920.078*
C110.78408 (10)0.62010 (19)0.6599 (6)0.0757 (9)
C120.77921 (11)0.6595 (2)0.4711 (6)0.0835 (10)
H12A0.80850.68510.40960.100*
C130.73158 (12)0.6617 (2)0.3718 (6)0.0822 (10)
H13A0.72890.68910.24520.099*
C140.68779 (11)0.6230 (2)0.4610 (5)0.0725 (8)
H14A0.65560.62330.39510.087*
C150.83646 (11)0.6162 (2)0.7674 (7)0.1120 (16)
H15A0.85900.66320.71520.168*
H15B0.85230.55740.74550.168*
H15C0.83130.62550.90980.168*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0412 (9)0.0688 (12)0.1166 (18)0.0042 (8)0.0010 (11)0.0251 (12)
N10.0486 (12)0.0869 (17)0.0691 (16)0.0053 (12)0.0033 (12)0.0028 (14)
N20.0641 (15)0.0659 (16)0.123 (3)0.0005 (12)0.0043 (16)0.0054 (17)
C10.0453 (13)0.0675 (16)0.0469 (14)0.0045 (12)0.0021 (12)0.0014 (13)
C20.0411 (12)0.0611 (16)0.0688 (18)0.0028 (12)0.0024 (13)0.0046 (15)
C30.0461 (12)0.0618 (15)0.0452 (14)0.0005 (11)0.0002 (12)0.0005 (12)
C40.0433 (12)0.0564 (14)0.0500 (14)0.0003 (11)0.0015 (12)0.0024 (13)
C50.0447 (12)0.0627 (15)0.0630 (17)0.0007 (11)0.0008 (13)0.0029 (14)
C60.0603 (16)0.0609 (16)0.082 (2)0.0092 (13)0.0012 (16)0.0005 (16)
C70.0757 (18)0.0554 (15)0.081 (2)0.0070 (14)0.0064 (17)0.0022 (16)
C80.0555 (14)0.0682 (17)0.0665 (17)0.0106 (13)0.0057 (14)0.0006 (15)
C90.0456 (13)0.0553 (15)0.091 (2)0.0074 (12)0.0025 (15)0.0055 (16)
C100.0458 (13)0.0570 (15)0.091 (2)0.0012 (12)0.0044 (15)0.0047 (16)
C110.0420 (14)0.0559 (16)0.129 (3)0.0002 (12)0.0001 (17)0.0025 (19)
C120.0565 (17)0.0668 (19)0.127 (3)0.0029 (14)0.0243 (19)0.012 (2)
C130.075 (2)0.075 (2)0.097 (3)0.0020 (16)0.0121 (19)0.0110 (19)
C140.0572 (16)0.0723 (19)0.088 (2)0.0070 (14)0.0036 (16)0.0037 (18)
C150.0446 (15)0.090 (2)0.202 (5)0.0048 (15)0.022 (2)0.013 (3)
Geometric parameters (Å, º) top
O1—C51.375 (3)C9—C141.370 (4)
O1—C91.409 (3)C9—C101.381 (4)
N1—C11.133 (3)C10—C111.394 (4)
N2—C21.140 (3)C10—H10A0.9300
C1—C31.448 (3)C11—C121.380 (5)
C2—C41.420 (4)C11—C151.515 (4)
C3—C81.369 (4)C12—C131.382 (4)
C3—C41.415 (3)C12—H12A0.9300
C4—C51.386 (3)C13—C141.384 (4)
C5—C61.377 (4)C13—H13A0.9300
C6—C71.371 (4)C14—H14A0.9300
C6—H6A0.9300C15—H15A0.9600
C7—C81.387 (4)C15—H15B0.9600
C7—H7A0.9300C15—H15C0.9600
C8—H8A0.9300
C5—O1—C9119.7 (2)C10—C9—O1115.2 (3)
N1—C1—C3179.8 (3)C9—C10—C11118.4 (3)
N2—C2—C4177.7 (3)C9—C10—H10A120.8
C8—C3—C4121.0 (2)C11—C10—H10A120.8
C8—C3—C1120.4 (2)C12—C11—C10119.2 (3)
C4—C3—C1118.7 (2)C12—C11—C15121.3 (3)
C5—C4—C3118.2 (2)C10—C11—C15119.5 (3)
C5—C4—C2121.3 (2)C11—C12—C13121.2 (3)
C3—C4—C2120.5 (2)C11—C12—H12A119.4
O1—C5—C6124.5 (2)C13—C12—H12A119.4
O1—C5—C4114.8 (2)C12—C13—C14119.9 (3)
C6—C5—C4120.6 (2)C12—C13—H13A120.1
C7—C6—C5120.4 (2)C14—C13—H13A120.1
C7—C6—H6A119.8C9—C14—C13118.5 (3)
C5—C6—H6A119.8C9—C14—H14A120.8
C6—C7—C8120.6 (3)C13—C14—H14A120.8
C6—C7—H7A119.7C11—C15—H15A109.5
C8—C7—H7A119.7C11—C15—H15B109.5
C3—C8—C7119.3 (2)H15A—C15—H15B109.5
C3—C8—H8A120.4C11—C15—H15C109.5
C7—C8—H8A120.4H15A—C15—H15C109.5
C14—C9—C10122.7 (3)H15B—C15—H15C109.5
C14—C9—O1121.9 (3)

Experimental details

Crystal data
Chemical formulaC15H10N2O
Mr234.25
Crystal system, space groupOrthorhombic, Pbca
Temperature (K)295
a, b, c (Å)25.514 (3), 14.6064 (18), 6.6109 (6)
V3)2463.7 (5)
Z8
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.6 × 0.5 × 0.3
Data collection
DiffractometerBruker P4
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
3094, 2254, 1372
Rint0.041
(sin θ/λ)max1)0.606
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.054, 0.109, 1.04
No. of reflections2254
No. of parameters165
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.21, 0.23

Computer programs: XSCANS (Bruker, 1997), SHELXTL (Bruker, 1997).

 

Acknowledgements

The authors thank the HBUST for financial support.

References

First citationAtalay, Ş., Ağar, A., Akdemir, N. & Ağar, E. (2003). Acta Cryst. E59, o1111–o1112.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationAtalay, Ş., Çoruh, U., Akdemir, N. & Ağar, E. (2004). Acta Cryst. E60, o303–o305.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationBruker. (1997). SHELXTL and XSCANS. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationCave, R. J., Siders, P. & Marcus, R. A. (1986). J. Phys. Chem. 90, 1436–1439.  CrossRef CAS Web of Science Google Scholar
First citationKöysal, Y., Işık, Ş., Akdemir, N., Ağar, E. & Kantar, C. (2004). Acta Cryst. E60, o930–o931.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationLeznoff, C. C. & Lever, A. B. P. (1989–1996). Phthalocyanines: Properties and Applications , Vol. 1. pp. 1–20. Weinheim/New York: VCH Publishers Inc.  Google Scholar
First citationMcKeown, N. B. (1998). Phthalocyanine Materials: Synthesis, Structure and Function. pp. 12–30. Cambridge University Press.  Google Scholar
First citationOcak Ískeleli, N. (2007). Acta Cryst. E63, o997–o998.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationOcak, N., Ağar, A., Akdemir, N., Ağar, E., García-Granda, S. & Erdönmez, A. (2003). Acta Cryst. E59, o1000–o1001.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationSharman, W. M. & van Lier, J. E. (2003). The Porphyrin Handbook, Vol. 15, edited by K. M. Kadish, K. M. Smith & G. Guilard, pp. 1–60. New York: Academic Press.  Google Scholar

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