Download citation
Download citation
link to html
The title compound, C16H28N6, was obtained from the reaction of o-phenyl­enediamine with N,N,N',N'-tetra­methyl­form­amidinium chloride. The two guanidyl groups are almost coplanar with the benzene ring. Both C-N bonds adjacent to the benzene ring were found to be double bonds, while the others were identified as single bonds, based on their bond distances.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806026365/ez2011sup1.cif
Contains datablocks I, TI03042C-6

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806026365/ez2011Isup2.hkl
Contains datablock I

CCDC reference: 618191

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C)= 0.002 Å
  • R factor = 0.047
  • wR factor = 0.137
  • Data-to-parameter ratio = 19.3

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

(I) top
Crystal data top
C16H28N6F(000) = 664
Mr = 304.44Dx = 1.144 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2861 reflections
a = 7.6337 (12) Åθ = 2.5–27.2°
b = 8.5800 (13) ŵ = 0.07 mm1
c = 27.199 (4) ÅT = 150 K
β = 97.000 (2)°Prism, colorless
V = 1768.2 (5) Å30.50 × 0.40 × 0.30 mm
Z = 4
Data collection top
Bruker SMART 1000 CCD area detector
diffractometer
3015 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.055
Graphite monochromatorθmax = 27.5°, θmin = 2.5°
φ and ω scansh = 99
10296 measured reflectionsk = 1011
3996 independent reflectionsl = 2634
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.137H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0671P)2 + 0.1667P]
where P = (Fo2 + 2Fc2)/3
3996 reflections(Δ/σ)max < 0.001
207 parametersΔρmax = 0.24 e Å3
0 restraintsΔρmin = 0.22 e Å3
Special details top

Experimental. 1H NMR (400 MHz, CDCl3): 2.67 (s, 24H), 6.49–6.53 (m, 2H), 6.71–6.75 (m, 2H); 13C NMR (100 MHz, CDCl3): 39.5 (CH3), 120.3 (CH), 121.9 (CH), 144.0 (C), 159.1 (C=N)

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.23274 (16)0.68186 (14)0.13970 (5)0.0246 (3)
C20.16967 (17)0.77484 (14)0.09827 (5)0.0242 (3)
C30.19594 (19)0.72384 (15)0.05104 (5)0.0298 (3)
C40.28004 (19)0.58354 (16)0.04379 (6)0.0336 (3)
C50.33775 (18)0.49135 (15)0.08417 (6)0.0329 (3)
C60.31210 (17)0.53948 (15)0.13133 (5)0.0293 (3)
C70.24667 (16)0.85403 (14)0.20772 (5)0.0248 (3)
C80.0071 (2)0.8366 (2)0.25257 (6)0.0465 (4)
C90.2565 (2)0.96686 (19)0.29065 (5)0.0422 (4)
C100.52725 (18)0.88165 (17)0.17281 (6)0.0353 (3)
C110.3720 (2)1.11413 (16)0.19474 (6)0.0368 (3)
C120.06544 (17)0.94950 (14)0.08343 (4)0.0235 (3)
C130.0170 (2)1.22317 (15)0.08569 (6)0.0353 (3)
C140.2921 (2)1.15529 (17)0.08286 (6)0.0376 (3)
C150.19606 (19)0.69007 (15)0.09159 (6)0.0337 (3)
C160.3026 (2)0.85247 (17)0.02032 (6)0.0390 (4)
N10.19831 (15)0.72093 (12)0.18765 (4)0.0270 (3)
N20.15726 (15)0.91146 (14)0.24502 (4)0.0316 (3)
N30.38589 (15)0.94542 (12)0.19744 (4)0.0283 (3)
N40.09075 (14)0.92062 (12)0.10542 (4)0.0258 (3)
N50.11661 (14)1.10351 (12)0.07491 (4)0.0270 (3)
N60.19425 (14)0.84153 (12)0.06781 (4)0.0275 (3)
H30.15540.78650.02320.036*
H40.29770.55130.01130.040*
H50.39500.39500.07960.039*
H60.34950.47380.15870.035*
H8A0.01770.73710.26970.056*
H8B0.07690.81770.22040.056*
H8C0.07360.90420.27270.056*
H9A0.36981.00960.28350.051*
H9B0.27770.88000.31400.051*
H9C0.18901.04830.30520.051*
H10A0.49750.89180.13690.042*
H10B0.54350.77130.18150.042*
H10C0.63670.93860.18330.042*
H11A0.26271.14740.20720.044*
H11B0.37031.14770.16020.044*
H11C0.47341.16110.21500.044*
H13A0.13011.18510.07690.042*
H13B0.02901.24830.12110.042*
H13C0.01801.31690.06640.042*
H14A0.29001.19320.11690.045*
H14B0.37491.06800.07740.045*
H14C0.32971.23960.05970.045*
H15A0.13200.69630.12500.040*
H15B0.13900.61320.07220.040*
H15C0.31830.65850.09360.040*
H16A0.27130.76820.00130.047*
H16B0.28240.95330.00500.047*
H16C0.42730.84330.02520.047*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0220 (6)0.0224 (6)0.0289 (7)0.0031 (5)0.0014 (5)0.0012 (5)
C20.0234 (6)0.0206 (6)0.0282 (7)0.0018 (5)0.0019 (5)0.0013 (5)
C30.0318 (7)0.0282 (7)0.0290 (7)0.0036 (5)0.0024 (5)0.0013 (5)
C40.0352 (8)0.0325 (7)0.0346 (8)0.0053 (6)0.0102 (6)0.0098 (6)
C50.0273 (7)0.0240 (6)0.0477 (9)0.0001 (5)0.0059 (6)0.0092 (6)
C60.0268 (7)0.0221 (6)0.0375 (8)0.0004 (5)0.0021 (6)0.0006 (5)
C70.0242 (6)0.0247 (6)0.0245 (7)0.0004 (5)0.0007 (5)0.0027 (5)
C80.0408 (9)0.0560 (10)0.0462 (10)0.0088 (7)0.0189 (7)0.0091 (8)
C90.0550 (10)0.0431 (8)0.0272 (8)0.0029 (7)0.0004 (7)0.0069 (6)
C100.0239 (7)0.0340 (7)0.0485 (9)0.0021 (6)0.0058 (6)0.0026 (6)
C110.0400 (8)0.0246 (7)0.0464 (9)0.0044 (6)0.0082 (7)0.0001 (6)
C120.0291 (7)0.0214 (6)0.0205 (6)0.0002 (5)0.0057 (5)0.0002 (5)
C130.0388 (8)0.0239 (7)0.0423 (9)0.0022 (6)0.0009 (6)0.0012 (6)
C140.0370 (8)0.0325 (7)0.0446 (9)0.0074 (6)0.0101 (6)0.0001 (6)
C150.0321 (8)0.0261 (7)0.0433 (9)0.0047 (5)0.0066 (6)0.0051 (6)
C160.0419 (9)0.0378 (8)0.0343 (8)0.0067 (6)0.0066 (6)0.0007 (6)
N10.0303 (6)0.0247 (5)0.0257 (6)0.0024 (4)0.0016 (4)0.0003 (4)
N20.0324 (6)0.0357 (6)0.0272 (6)0.0056 (5)0.0064 (5)0.0047 (5)
N30.0265 (6)0.0238 (5)0.0348 (6)0.0020 (4)0.0044 (5)0.0007 (5)
N40.0297 (6)0.0208 (5)0.0261 (6)0.0017 (4)0.0003 (4)0.0007 (4)
N50.0291 (6)0.0211 (5)0.0309 (6)0.0026 (4)0.0037 (5)0.0014 (4)
N60.0277 (6)0.0251 (5)0.0288 (6)0.0025 (4)0.0001 (4)0.0023 (4)
Geometric parameters (Å, º) top
C2—C11.4162 (18)C6—H60.9500
C2—C31.3947 (19)C8—H8A0.9800
C3—C41.3896 (19)C8—H8B0.9800
C5—C41.381 (2)C8—H8C0.9800
C6—C51.384 (2)C9—H9A0.9800
C6—C11.3945 (18)C9—H9B0.9800
N1—C11.4023 (17)C9—H9C0.9800
N1—C71.2996 (16)C10—H10A0.9800
N2—C71.3808 (18)C10—H10B0.9800
N2—C81.4467 (19)C10—H10C0.9800
N2—C91.4531 (17)C11—H11A0.9800
N3—C71.3765 (16)C11—H11B0.9800
N3—C101.4453 (18)C11—H11C0.9800
N3—C111.4526 (17)C13—H13A0.9800
N4—C21.4120 (16)C13—H13B0.9800
N4—C121.2910 (16)C13—H13C0.9800
N5—C121.3893 (15)C14—H14A0.9800
N5—C131.4515 (17)C14—H14B0.9800
N5—C141.4520 (18)C14—H14C0.9800
N6—C121.3798 (16)C15—H15A0.9800
N6—C151.4523 (17)C15—H15B0.9800
N6—C161.4495 (17)C15—H15C0.9800
C3—H30.9500C16—H16A0.9800
C4—H40.9500C16—H16B0.9800
C5—H50.9500C16—H16C0.9800
C3—C2—C1118.88 (12)N2—C9—H9C109.5
C3—C2—N4121.09 (11)N3—C10—H10A109.5
C3—C4—C5119.44 (13)N3—C10—H10B109.5
C4—C3—C2121.55 (13)N3—C10—H10C109.5
C5—C6—C1121.73 (12)N3—C11—H11A109.5
C6—C1—C2118.43 (12)N3—C11—H11B109.5
C6—C5—C4119.91 (13)N3—C11—H11C109.5
C7—N1—C1121.65 (11)N5—C13—H13A109.5
C7—N2—C8117.44 (11)N5—C13—H13B109.5
C7—N2—C9119.43 (12)N5—C13—H13C109.5
C7—N3—C10121.12 (11)N5—C14—H14A109.5
C7—N3—C11121.63 (11)N5—C14—H14B109.5
C8—N2—C9113.27 (13)N5—C14—H14C109.5
C11—N3—C10114.08 (11)N6—C15—H15A109.5
C12—N4—C2119.45 (10)N6—C15—H15B109.5
C12—N5—C13117.56 (11)N6—C15—H15C109.5
C12—N5—C14120.79 (11)N6—C16—H16A109.5
C12—N6—C15120.58 (11)N6—C16—H16B109.5
C12—N6—C16122.60 (11)N6—C16—H16C109.5
C13—N5—C14113.05 (11)H8A—C8—H8B109.5
C15—N6—C16114.80 (11)H8A—C8—H8C109.5
N1—C1—C2121.42 (11)H8B—C8—H8C109.5
N1—C1—C6119.71 (12)H9A—C9—H9B109.5
N1—C7—N2118.78 (12)H9A—C9—H9C109.5
N1—C7—N3127.03 (12)H9B—C9—H9C109.5
N2—C7—N3114.13 (11)H10A—C10—H10B109.5
N4—C2—C1119.93 (11)H10A—C10—H10C109.5
N4—C12—N5119.00 (11)H10B—C10—H10C109.5
N4—C12—N6126.66 (11)H11A—C11—H11B109.5
N5—C12—N6114.32 (11)H11A—C11—H11C109.5
C1—C6—H6119.1H11B—C11—H11C109.5
C2—C3—H3119.2H13A—C13—H13B109.5
C3—C4—H4120.3H13A—C13—H13C109.5
C4—C3—H3119.2H13B—C13—H13C109.5
C4—C5—H5120.0H14A—C14—H14B109.5
C5—C4—H4120.3H14A—C14—H14C109.5
C5—C6—H6119.1H14B—C14—H14C109.5
C6—C5—H5120.0H15A—C15—H15B109.5
N2—C8—H8A109.5H15A—C15—H15C109.5
N2—C8—H8B109.5H15B—C15—H15C109.5
N2—C8—H8C109.5H16A—C16—H16B109.5
N2—C9—H9A109.5H16A—C16—H16C109.5
N2—C9—H9B109.5H16B—C16—H16C109.5
C1—C2—C3—C40.9 (2)C10—N3—C7—N118.4 (2)
C1—C6—C5—C41.7 (2)C10—N3—C7—N2158.77 (12)
C1—N1—C7—N2155.99 (12)C11—N3—C7—N1140.33 (14)
C1—N1—C7—N327.01 (19)C11—N3—C7—N242.55 (17)
C2—C3—C4—C50.6 (2)C12—N4—C2—C358.28 (18)
C2—N4—C12—N5156.27 (11)C12—N4—C2—C1125.35 (13)
C2—N4—C12—N625.5 (2)C13—N5—C12—N47.64 (18)
C3—C2—C1—C62.70 (19)C13—N5—C12—N6173.90 (11)
C3—C2—C1—N1175.00 (11)C14—N5—C12—N4137.97 (14)
C5—C6—C1—C23.13 (19)C14—N5—C12—N640.50 (16)
C5—C6—C1—N1175.56 (12)C15—N6—C12—N425.5 (2)
C6—C5—C4—C30.3 (2)C15—N6—C12—N5152.84 (12)
C7—N1—C1—C258.19 (17)C16—N6—C12—N4137.47 (15)
C7—N1—C1—C6129.61 (13)C16—N6—C12—N544.20 (18)
C8—N2—C7—N112.47 (19)N4—C2—C1—C6179.15 (11)
C8—N2—C7—N3170.16 (12)N4—C2—C1—N18.55 (18)
C9—N2—C7—N1131.06 (13)N4—C2—C3—C4177.30 (12)
C9—N2—C7—N346.32 (17)
 

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