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The reaction of 1,10-phenanthroline-5,6-dione and diethyl­enetriamine unexpectedly yielded the title compound, C16H15N5, which is a non-planar and chiral fused-ring system composed of two pyridine rings and three non-aromatic rings. Crystal symmetry results in a racemic mixture of enanti­omers. Aromatic π–π stacking inter­actions exist between adjacent mol­ecules and weak bifurcated N—H...(N,N) hydrogen bonds lead to dimeric associations of mol­ecules, generated by inversion.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806030558/hb2108sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806030558/hb2108Isup2.hkl
Contains datablock I

CCDC reference: 621326

Key indicators

  • Single-crystal X-ray study
  • T = 273 K
  • Mean [sigma](C-C)= 0.002 Å
  • R factor = 0.038
  • wR factor = 0.117
  • Data-to-parameter ratio = 12.6

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1998); software used to prepare material for publication: SHELXTL.

(1R)-6,9,15,18,21-Pentaazapentacyclo[12.7.0.01,18.02,7.08,13]henicosa- 2,4,6,8(13),9,11,14-heptaene top
Crystal data top
C16H15N5F(000) = 584
Mr = 277.33Dx = 1.385 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 4400 reflections
a = 10.7254 (2) Åθ = 2.6–28.2°
b = 13.0587 (3) ŵ = 0.09 mm1
c = 10.2122 (2) ÅT = 273 K
β = 111.609 (1)°Block, yellow
V = 1329.79 (5) Å30.3 × 0.3 × 0.2 mm
Z = 4
Data collection top
Bruker SMART CCD
diffractometer
1963 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.021
Graphite monochromatorθmax = 25.2°, θmin = 2.0°
ω scansh = 1212
11156 measured reflectionsk = 1515
2402 independent reflectionsl = 1012
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)] = 0.038Hydrogen site location: difmap and geom
wR(F2) = 0.117H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0692P)2 + 0.1716P]
where P = (Fo2 + 2Fc2)/3
2402 reflections(Δ/σ)max < 0.001
190 parametersΔρmax = 0.17 e Å3
0 restraintsΔρmin = 0.16 e Å3
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 > 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
N10.41925 (12)0.01619 (9)0.74776 (12)0.0429 (3)
N20.55717 (11)0.14851 (10)0.95816 (13)0.0426 (3)
N30.02596 (12)0.13131 (10)0.81013 (13)0.0458 (3)
N40.17382 (12)0.18151 (10)1.10369 (13)0.0448 (3)
N50.24898 (11)0.01627 (9)1.09360 (12)0.0413 (3)
H50.32560.01621.09920.049*
C10.34671 (16)0.03749 (12)0.63435 (16)0.0496 (4)
H10.39130.06790.58170.060*
C20.21002 (16)0.05081 (13)0.59002 (16)0.0506 (4)
H20.16420.08890.50980.061*
C30.14281 (15)0.00651 (12)0.66698 (16)0.0452 (4)
H30.05050.01440.63980.054*
C40.21466 (13)0.05019 (10)0.78585 (14)0.0373 (3)
C50.35317 (13)0.05934 (10)0.82252 (14)0.0356 (3)
C60.43114 (13)0.12464 (10)0.94416 (14)0.0354 (3)
C70.37051 (13)0.16083 (10)1.03489 (14)0.0376 (3)
C80.44208 (16)0.22953 (12)1.13869 (16)0.0475 (4)
H80.40380.25721.19900.057*
C90.57037 (17)0.25655 (13)1.15188 (18)0.0536 (4)
H90.61940.30341.21990.064*
C100.62417 (15)0.21253 (13)1.06203 (17)0.0499 (4)
H100.71240.22831.07450.060*
C110.14718 (13)0.10318 (10)0.87070 (14)0.0379 (3)
C120.23465 (13)0.11806 (10)1.02534 (15)0.0379 (3)
C130.03535 (15)0.18784 (14)0.89479 (18)0.0548 (4)
H13A0.08240.14000.93290.066*
H13B0.10080.23550.83450.066*
C140.06562 (16)0.24626 (13)1.01435 (18)0.0522 (4)
H14A0.10320.30090.97600.063*
H14B0.02040.27731.07100.063*
C150.1405 (2)0.11580 (14)1.2012 (2)0.0631 (5)
H15A0.05150.08671.15750.076*
H15B0.14580.15281.28540.076*
C160.24701 (18)0.03467 (14)1.23358 (17)0.0548 (4)
H16A0.33290.05951.29820.066*
H16B0.22220.02641.27220.066*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0486 (7)0.0444 (7)0.0382 (7)0.0014 (5)0.0189 (6)0.0043 (6)
N20.0441 (6)0.0469 (7)0.0372 (7)0.0043 (5)0.0153 (5)0.0004 (6)
N30.0421 (6)0.0538 (8)0.0425 (7)0.0015 (5)0.0168 (6)0.0014 (6)
N40.0528 (7)0.0469 (7)0.0399 (7)0.0057 (5)0.0230 (6)0.0024 (6)
N50.0482 (7)0.0426 (7)0.0391 (7)0.0029 (5)0.0231 (5)0.0034 (5)
C10.0600 (9)0.0510 (9)0.0411 (9)0.0015 (7)0.0225 (7)0.0097 (7)
C20.0591 (9)0.0517 (9)0.0376 (9)0.0046 (7)0.0140 (7)0.0121 (7)
C30.0453 (8)0.0493 (9)0.0380 (8)0.0031 (6)0.0118 (6)0.0032 (7)
C40.0447 (7)0.0364 (7)0.0298 (7)0.0006 (5)0.0125 (6)0.0027 (6)
C50.0450 (7)0.0328 (7)0.0308 (7)0.0015 (5)0.0161 (6)0.0030 (6)
C60.0426 (7)0.0334 (7)0.0297 (7)0.0006 (5)0.0127 (6)0.0034 (6)
C70.0448 (7)0.0353 (7)0.0327 (7)0.0002 (6)0.0141 (6)0.0007 (6)
C80.0570 (9)0.0452 (9)0.0420 (9)0.0039 (7)0.0204 (7)0.0095 (7)
C90.0610 (10)0.0511 (9)0.0456 (9)0.0159 (7)0.0162 (8)0.0125 (8)
C100.0476 (8)0.0556 (10)0.0448 (9)0.0139 (7)0.0150 (7)0.0019 (8)
C110.0417 (7)0.0380 (7)0.0352 (8)0.0013 (6)0.0158 (6)0.0017 (6)
C120.0444 (7)0.0374 (7)0.0346 (8)0.0006 (6)0.0177 (6)0.0017 (6)
C130.0472 (8)0.0668 (11)0.0529 (10)0.0122 (7)0.0215 (8)0.0024 (8)
C140.0584 (9)0.0509 (9)0.0540 (10)0.0109 (7)0.0287 (8)0.0007 (8)
C150.0848 (12)0.0696 (12)0.0507 (10)0.0143 (9)0.0434 (10)0.0061 (9)
C160.0707 (10)0.0605 (10)0.0389 (9)0.0052 (8)0.0268 (8)0.0065 (8)
Geometric parameters (Å, º) top
N1—C11.3321 (19)C5—C61.4848 (19)
N1—C51.3422 (18)C6—C71.3960 (19)
N2—C101.334 (2)C7—C81.385 (2)
N2—C61.3425 (18)C7—C121.5298 (19)
N3—C111.2710 (18)C8—C91.378 (2)
N3—C131.464 (2)C8—H80.9300
N4—C141.454 (2)C9—C101.377 (2)
N4—C151.455 (2)C9—H90.9300
N4—C121.4618 (18)C10—H100.9300
N5—C161.4574 (19)C11—C121.523 (2)
N5—C121.4824 (18)C13—C141.507 (2)
N5—H50.9074C13—H13A0.9700
C1—C21.377 (2)C13—H13B0.9700
C1—H10.9300C14—H14A0.9700
C2—C31.375 (2)C14—H14B0.9700
C2—H20.9300C15—C161.503 (2)
C3—C41.388 (2)C15—H15A0.9700
C3—H30.9300C15—H15B0.9700
C4—C51.3970 (19)C16—H16A0.9700
C4—C111.4884 (19)C16—H16B0.9700
C1—N1—C5116.99 (12)N2—C10—C9123.81 (14)
C10—N2—C6117.17 (13)N2—C10—H10118.1
C11—N3—C13117.37 (13)C9—C10—H10118.1
C14—N4—C15115.57 (13)N3—C11—C4118.73 (12)
C14—N4—C12113.59 (11)N3—C11—C12126.63 (13)
C15—N4—C12108.18 (12)C4—C11—C12114.64 (11)
C16—N5—C12106.08 (12)N4—C12—N5103.93 (11)
C16—N5—H5110.8N4—C12—C11114.28 (11)
C12—N5—H5112.5N5—C12—C11106.90 (11)
N1—C1—C2124.24 (14)N4—C12—C7111.39 (11)
N1—C1—H1117.9N5—C12—C7111.47 (11)
C2—C1—H1117.9C11—C12—C7108.74 (11)
C3—C2—C1118.56 (14)N3—C13—C14112.87 (13)
C3—C2—H2120.7N3—C13—H13A109.0
C1—C2—H2120.7C14—C13—H13A109.0
C2—C3—C4119.03 (14)N3—C13—H13B109.0
C2—C3—H3120.5C14—C13—H13B109.0
C4—C3—H3120.5H13A—C13—H13B107.8
C3—C4—C5118.24 (13)N4—C14—C13112.54 (13)
C3—C4—C11121.65 (13)N4—C14—H14A109.1
C5—C4—C11120.08 (12)C13—C14—H14A109.1
N1—C5—C4122.94 (12)N4—C14—H14B109.1
N1—C5—C6117.66 (12)C13—C14—H14B109.1
C4—C5—C6119.29 (12)H14A—C14—H14B107.8
N2—C6—C7123.20 (13)N4—C15—C16102.00 (13)
N2—C6—C5117.21 (12)N4—C15—H15A111.4
C7—C6—C5119.55 (12)C16—C15—H15A111.4
C8—C7—C6117.70 (13)N4—C15—H15B111.4
C8—C7—C12122.13 (13)C16—C15—H15B111.4
C6—C7—C12119.98 (12)H15A—C15—H15B109.2
C9—C8—C7119.52 (15)N5—C16—C15100.64 (13)
C9—C8—H8120.2N5—C16—H16A111.6
C7—C8—H8120.2C15—C16—H16A111.6
C10—C9—C8118.45 (14)N5—C16—H16B111.6
C10—C9—H9120.8C15—C16—H16B111.6
C8—C9—H9120.8H16A—C16—H16B109.4
C5—N1—C1—C20.2 (2)C3—C4—C11—N327.4 (2)
C1—N1—C5—C40.2 (2)C3—C4—C11—C12152.69 (13)
C1—N1—C5—C6176.36 (12)C5—C4—C11—N3150.58 (14)
C10—N2—C6—C5175.77 (13)C5—C4—C11—C1229.30 (18)
C10—N2—C6—C72.1 (2)N1—C5—C6—N29.80 (18)
C6—N2—C10—C91.6 (2)N1—C5—C6—C7172.26 (12)
C13—N3—C11—C4176.95 (13)C4—C5—C6—N2166.52 (13)
C13—N3—C11—C122.9 (2)C4—C5—C6—C711.43 (19)
C11—N3—C13—C1427.2 (2)N2—C6—C7—C84.0 (2)
C14—N4—C12—N5136.08 (13)N2—C6—C7—C12171.07 (13)
C14—N4—C12—C7103.77 (14)C5—C6—C7—C8173.79 (13)
C14—N4—C12—C1119.95 (17)C5—C6—C7—C1211.12 (19)
C15—N4—C12—N56.34 (16)C6—C7—C8—C92.3 (2)
C15—N4—C12—C7126.49 (14)C12—C7—C8—C9172.70 (14)
C15—N4—C12—C11109.79 (14)C6—C7—C12—N4166.39 (12)
C12—N4—C14—C1349.36 (18)C6—C7—C12—N578.02 (16)
C15—N4—C14—C1376.54 (18)C6—C7—C12—C1139.58 (16)
C12—N4—C15—C1630.55 (17)C8—C7—C12—N418.74 (18)
C14—N4—C15—C16159.17 (14)C8—C7—C12—N596.85 (15)
C16—N5—C12—N421.52 (15)C8—C7—C12—C11145.55 (13)
C16—N5—C12—C798.58 (14)C7—C8—C9—C101.1 (2)
C16—N5—C12—C11142.72 (13)C8—C9—C10—N23.2 (3)
C12—N5—C16—C1539.80 (16)N3—C11—C12—N47.4 (2)
N1—C1—C2—C30.2 (2)N3—C11—C12—N5107.03 (16)
C1—C2—C3—C40.3 (2)N3—C11—C12—C7132.51 (15)
C2—C3—C4—C50.3 (2)C4—C11—C12—N4172.50 (11)
C2—C3—C4—C11177.76 (14)C4—C11—C12—N573.10 (15)
C3—C4—C5—N10.3 (2)C4—C11—C12—C747.36 (15)
C3—C4—C5—C6176.38 (13)N3—C13—C14—N454.03 (19)
C11—C4—C5—N1177.82 (12)N4—C15—C16—N542.54 (16)
C11—C4—C5—C61.70 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N5—H5···N1i0.912.603.3497 (18)140
N5—H5···N2i0.912.333.1689 (18)153
C8—H8···N40.932.502.836 (2)102
Symmetry code: (i) x+1, y, z+2.
 

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