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In the title compound, C15H12N2, the geometric parameters are normal, within experimental error. The mol­ecules are arranged in pairs, with their hydrazone groups oriented towards one another.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803007694/su6023sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803007694/su6023Isup2.hkl
Contains datablock I

CCDC reference: 214615

Key indicators

  • Single-crystal X-ray study
  • T = 291 K, P = 0.0 kPa
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.052
  • wR factor = 0.140
  • Data-to-parameter ratio = 12.3

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_420 Alert C D-H Without Acceptor N2 - H2N2 ?
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

During our investigation of chemical and electrochemical properties of the azine grouping >CN—NC< (Riedl et al., 1996; Zuman & Ludv\'ιk, 2000), various azine and hydrazone derivatives were synthesized, including the title compound, (I), derived from anthracene-9-carbaldehyde.

In order to compare the distances in (I), a search of the Cambridge Structural Database (CSD, Version 5.21; Allen, 2002) was carried out and yielded 24 hits. The search considered structures containing anthracene, not involved in the π-bonding with a metal and with R factors < 0.09. The bond lengths within the anthracene ring of (I) are in accordance with those found in the search, except for slight deviations of the bond-lengths of the pairs C9—C11, C9—C13 and C10—C12, C10—C14 (Fig. 1), which are ~0.022 Å longer and 0.008 Å shorter, respectively, than in pure anthracene. The reason why the chemically equivalent bonds C9—C11, C9—C13 are longer than C10—C12, C10—C14 (Table 1) is probably due to the substituent on C9.

Neither atom N1 nor atom N2 lie in the plane of the central aromatic ring A (C9/C11/C12/C10/C14/C13). The dihedral angle between the plane through atoms N1, C15, C9 and plane A is 42.9 (2)°. The bond length N1—N2 of 1.387 (2) Å is significantly longer than the NN bond length in azo-compounds (~1.25 Å), as shown by a search of the CSD. [Compounds with a fragment C···C···N···N···C···C were searched while the coordination number on C was 3 and 2 on N. The value of ~1.25 Å corresponds to the maximum (more than 700 hits) in the distribution of N···N bond lengths.] On the other hand the N1—N2 bond length is shorter than that in hydrazine: the average N—N bond in hydrazinium(1+) is 1.435 (7) Å, according to 36 hits from the CSD.

This comparison shows that the N—N bond in (I) (Table 1) has a bond order close to one. The bond length between atoms C15 and N1 [1.272 (2) Å] corresponds, however, to a typical double bond, that is ~1.28 Å (Box \& Yu, 1997).

The hydrazone groups are oriented towards each other, ordering the molecules into hydrogen bonded pairs (Fig. 2). The geometry of the N2-H1N2···N1 contact points to a weak hydrogen bond (Table 2).

Experimental top

9-Anthraldehyde (1.4 g) was diluted in 30 ml of ethanol, and 0.34 ml of hydrazine hydrate was added under heating. After slow cooling the mixture was kept in a refrigerator overnight. The crystals formed were isolated, washed by ethanol and dried. The yield was 1 g of the title compound, whose identity and purity was checked by thin-layer chromatography and NMR spectra. If a half of the quantity of hydrazine hydrate was used and the mixture was refluxed for 5 h, the corresponding azine was produced. However, no suitable crystals could be obtained.

Computing details top

Data collection: COLLECT (Nonius BV, 1997-2000); cell refinement: HKL SCALEPACK (Otwinowski & Minor, 1997); data reduction: HKL DENZO (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2002); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. View of the title molecule with 40° probability displacement ellipsoids (PLATON; Spek, 2002).
[Figure 2] Fig. 2. Crystal packing view of the unit cell (PLATON; Spek, 2002).
1-(9-Anthrylmetylidene)hydrazine top
Crystal data top
C15H12N2F(000) = 464
Mr = 220.27Dx = 1.325 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 4704 reflections
a = 17.7211 (9) Åθ = 1.0–26.0°
b = 3.9082 (2) ŵ = 0.08 mm1
c = 16.4115 (9) ÅT = 291 K
β = 103.856 (3)°Plate, yellow
V = 1103.55 (10) Å30.3 × 0.2 × 0.08 mm
Z = 4
Data collection top
Nonius KappaCCD
diffractometer
1628 reflections with I > 2σ(I)
Radiation source: fine-focus sealed X-ray tubeRint = 0.000
Graphite monochromatorθmax = 26.0°, θmin = 2.6°
ω scansh = 021
2169 measured reflectionsk = 44
2169 independent reflectionsl = 2019
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.052H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.140 w = 1/[σ2(Fo2) + (0.0758P)2 + 0.0918P]
where P = (Fo2 + 2Fc2)/3
S = 1.10(Δ/σ)max < 0.001
2169 reflectionsΔρmax = 0.30 e Å3
177 parametersΔρmin = 0.24 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
27 constraintsExtinction coefficient: 0.107 (10)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H12N2V = 1103.55 (10) Å3
Mr = 220.27Z = 4
Monoclinic, P21/cMo Kα radiation
a = 17.7211 (9) ŵ = 0.08 mm1
b = 3.9082 (2) ÅT = 291 K
c = 16.4115 (9) Å0.3 × 0.2 × 0.08 mm
β = 103.856 (3)°
Data collection top
Nonius KappaCCD
diffractometer
1628 reflections with I > 2σ(I)
2169 measured reflectionsRint = 0.000
2169 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0520 restraints
wR(F2) = 0.140H atoms treated by a mixture of independent and constrained refinement
S = 1.10Δρmax = 0.30 e Å3
2169 reflectionsΔρmin = 0.24 e Å3
177 parameters
Special details top

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
xyzUiso*/Ueq
C10.18128 (9)0.7205 (4)0.47635 (10)0.0477 (4)
H10.22030.63820.52040.050 (4)*
C20.10649 (10)0.7134 (4)0.48320 (11)0.0559 (5)
H20.09520.62470.53150.069 (6)*
C30.04561 (10)0.8383 (5)0.41831 (12)0.0585 (5)
H30.00540.83090.42380.074 (6)*
C40.06163 (9)0.9688 (4)0.34813 (12)0.0537 (5)
H40.02121.05260.30580.068 (6)*
C50.37012 (10)1.0124 (4)0.30409 (10)0.0497 (4)
H50.41160.91620.34300.052 (5)*
C60.38282 (11)1.1584 (5)0.23336 (11)0.0586 (5)
H60.43301.16450.22530.068 (6)*
C70.32142 (12)1.3001 (4)0.17228 (11)0.0605 (5)
H70.33131.40360.12490.075 (6)*
C80.24828 (11)1.2864 (4)0.18225 (10)0.0544 (5)
H80.20791.37560.14070.074 (6)*
C90.27862 (8)0.8642 (3)0.39370 (9)0.0387 (4)
C100.15604 (10)1.1210 (4)0.26608 (10)0.0478 (4)
H100.11561.20660.22400.059 (5)*
C110.20133 (8)0.8516 (4)0.40300 (9)0.0404 (4)
C120.13899 (9)0.9813 (4)0.33731 (10)0.0439 (4)
C130.29429 (9)1.0040 (3)0.31968 (9)0.0406 (4)
C140.23133 (9)1.1372 (4)0.25553 (9)0.0445 (4)
C150.34009 (9)0.7253 (4)0.46235 (9)0.0421 (4)
N10.40544 (7)0.8693 (3)0.49051 (8)0.0455 (4)
N20.45402 (9)0.7240 (5)0.56097 (9)0.0580 (4)
H150.3280 (9)0.515 (5)0.4888 (11)0.054 (5)*
H1N20.5015 (13)0.765 (6)0.5600 (14)0.082 (7)*
H2N20.4443 (13)0.493 (7)0.5661 (16)0.100 (8)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0532 (9)0.0462 (9)0.0429 (9)0.0038 (7)0.0096 (7)0.0008 (7)
C20.0601 (11)0.0561 (10)0.0550 (11)0.0092 (8)0.0207 (9)0.0001 (8)
C30.0463 (10)0.0615 (11)0.0695 (12)0.0073 (8)0.0172 (8)0.0072 (9)
C40.0455 (9)0.0523 (10)0.0586 (11)0.0014 (7)0.0031 (8)0.0055 (8)
C50.0546 (10)0.0539 (10)0.0405 (9)0.0037 (7)0.0114 (7)0.0066 (7)
C60.0688 (12)0.0636 (11)0.0494 (10)0.0110 (9)0.0258 (9)0.0081 (8)
C70.0887 (14)0.0566 (10)0.0406 (9)0.0094 (9)0.0240 (9)0.0010 (8)
C80.0784 (12)0.0469 (9)0.0352 (8)0.0006 (8)0.0087 (8)0.0018 (7)
C90.0461 (8)0.0333 (7)0.0348 (8)0.0035 (6)0.0057 (6)0.0051 (6)
C100.0542 (9)0.0437 (8)0.0391 (9)0.0022 (7)0.0013 (7)0.0004 (7)
C110.0478 (9)0.0345 (7)0.0370 (8)0.0040 (6)0.0066 (6)0.0058 (6)
C120.0463 (9)0.0382 (8)0.0438 (9)0.0032 (6)0.0045 (7)0.0058 (6)
C130.0504 (9)0.0352 (8)0.0349 (8)0.0043 (6)0.0077 (6)0.0056 (6)
C140.0583 (10)0.0375 (8)0.0351 (8)0.0022 (7)0.0059 (7)0.0042 (6)
C150.0482 (9)0.0400 (8)0.0380 (8)0.0000 (7)0.0100 (7)0.0001 (6)
N10.0437 (7)0.0523 (7)0.0384 (7)0.0016 (6)0.0055 (6)0.0005 (6)
N20.0450 (9)0.0806 (12)0.0449 (8)0.0043 (8)0.0038 (6)0.0084 (8)
Geometric parameters (Å, º) top
C1—C21.357 (2)C8—C141.432 (2)
C1—C111.429 (2)C8—H80.9300
C1—H10.9300C9—C111.415 (2)
C2—C31.409 (2)C9—C131.419 (2)
C2—H20.9300C9—C151.471 (2)
C3—C41.350 (2)C10—C141.387 (2)
C3—H30.9300C10—C121.388 (2)
C4—C121.425 (2)C10—H100.9300
C4—H40.9300C11—C121.438 (2)
C5—C61.360 (2)C13—C141.436 (2)
C5—C131.427 (2)C15—N11.2709 (19)
C5—H50.9300C15—H150.977 (18)
C6—C71.405 (3)N1—N21.3870 (19)
C6—H60.9300N2—H1N20.86 (2)
C7—C81.346 (3)N2—H2N20.93 (3)
C7—H70.9300
C2—C1—C11121.45 (15)C11—C9—C15117.57 (13)
C2—C1—H1119.3C13—C9—C15122.50 (13)
C11—C1—H1119.3C14—C10—C12122.21 (14)
C1—C2—C3121.10 (16)C14—C10—H10118.9
C1—C2—H2119.4C12—C10—H10118.9
C3—C2—H2119.4C9—C11—C1123.08 (13)
C4—C3—C2119.74 (16)C9—C11—C12119.77 (14)
C4—C3—H3120.1C1—C11—C12117.14 (14)
C2—C3—H3120.1C10—C12—C4121.91 (15)
C3—C4—C12121.61 (16)C10—C12—C11119.14 (14)
C3—C4—H4119.2C4—C12—C11118.94 (15)
C12—C4—H4119.2C9—C13—C5123.23 (14)
C6—C5—C13121.21 (16)C9—C13—C14119.37 (14)
C6—C5—H5119.4C5—C13—C14117.38 (14)
C13—C5—H5119.4C10—C14—C8121.67 (14)
C5—C6—C7121.09 (17)C10—C14—C13119.57 (14)
C5—C6—H6119.5C8—C14—C13118.76 (15)
C7—C6—H6119.5N1—C15—C9123.94 (15)
C8—C7—C6120.10 (16)N1—C15—H15119.2 (10)
C8—C7—H7120.0C9—C15—H15116.8 (10)
C6—C7—H7120.0C15—N1—N2116.84 (15)
C7—C8—C14121.35 (16)N1—N2—H1N2108.9 (15)
C7—C8—H8119.3N1—N2—H2N2112.5 (15)
C14—C8—H8119.3H1N2—N2—H2N2112.7 (19)
C11—C9—C13119.92 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H1N2···N1i0.86 (2)2.47 (2)3.233 (2)147.9 (19)
Symmetry code: (i) x+1, y+2, z+1.

Experimental details

Crystal data
Chemical formulaC15H12N2
Mr220.27
Crystal system, space groupMonoclinic, P21/c
Temperature (K)291
a, b, c (Å)17.7211 (9), 3.9082 (2), 16.4115 (9)
β (°) 103.856 (3)
V3)1103.55 (10)
Z4
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.3 × 0.2 × 0.08
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
2169, 2169, 1628
Rint0.000
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.052, 0.140, 1.10
No. of reflections2169
No. of parameters177
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.30, 0.24

Computer programs: COLLECT (Nonius BV, 1997-2000), HKL SCALEPACK (Otwinowski & Minor, 1997), HKL DENZO (Otwinowski & Minor, 1997) and SCALEPACK, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2002), SHELXL97.

Selected geometric parameters (Å, º) top
C1—C21.357 (2)C9—C111.415 (2)
C1—C111.429 (2)C9—C131.419 (2)
C2—C31.409 (2)C9—C151.471 (2)
C3—C41.350 (2)C10—C141.387 (2)
C4—C121.425 (2)C10—C121.388 (2)
C5—C61.360 (2)C11—C121.438 (2)
C5—C131.427 (2)C13—C141.436 (2)
C6—C71.405 (3)C15—N11.2709 (19)
C7—C81.346 (3)N1—N21.3870 (19)
C8—C141.432 (2)
N1—C15—C9123.94 (15)C15—N1—N2116.84 (15)
N1—C15—H15119.2 (10)N1—N2—H1N2108.9 (15)
C9—C15—H15116.8 (10)N1—N2—H2N2112.5 (15)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H1N2···N1i0.86 (2)2.47 (2)3.233 (2)147.9 (19)
Symmetry code: (i) x+1, y+2, z+1.
 

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