Literature DB >> 21581995

N,N-Bis(2-pyridylmeth-yl)-tert-butyl-amine.

Allen Mambanda1, Deogratius Jaganyi, Kirsty Stewart.   

Abstract

In the title compound, C(16)H(21)N(3), the dihedral angle between the two pyridine rings is 88.11 (9)°. In the crystal, mol-ecules are linked through inter-molecular C-H⋯π inter-actions, forming a layer expanding parallel to the (10) plane.

Entities:  

Year:  2009        PMID: 21581995      PMCID: PMC2968317          DOI: 10.1107/S1600536809001366

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For related compounds, see: Mambanda et al. (2007 ▶); Foxon et al. (2007 ▶); Fujihara et al. (2004 ▶); Munro & Camp (2003 ▶). For metal complexes with the title compound as a ligand, see: Fujii et al. (2003 ▶); Lee & Lippard (2002 ▶); Mok et al. (1997 ▶). For the metal complex with N,N-bis­(2-pyridylmeth­yl)ethyl­amine as a ligand, see: Pal et al. (1992 ▶).

Experimental

Crystal data

C16H21N3 M = 255.36 Monoclinic, a = 6.1808 (3) Å b = 17.9502 (8) Å c = 13.7079 (6) Å β = 100.239 (4)° V = 1496.62 (12) Å3 Z = 4 Mo Kα radiation μ = 0.07 mm−1 T = 293 (2) K 0.50 × 0.50 × 0.30 mm

Data collection

Oxford Diffraction Xcalibur2 CCD diffractometer Absorption correction: multi-scan (; Oxford Diffraction, 2008 ▶) T min = 0.967, T max = 0.980 7475 measured reflections 2392 independent reflections 2024 reflections with I > 2σ(I) R int = 0.012

Refinement

R[F 2 > 2σ(F 2)] = 0.043 wR(F 2) = 0.119 S = 1.02 2392 reflections 175 parameters 2 restraints H-atom parameters constrained Δρmax = 0.21 e Å−3 Δρmin = −0.22 e Å−3 Data collection: CrysAlis CCD (Oxford Diffraction, 2008 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2008 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809001366/is2355sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809001366/is2355Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C16H21N3F(000) = 552
Mr = 255.36Dx = 1.133 Mg m3
Monoclinic, CcMo Kα radiation, λ = 0.71073 Å
Hall symbol: C -2ycCell parameters from 4672 reflections
a = 6.1808 (3) Åθ = 3.9–32.0°
b = 17.9502 (8) ŵ = 0.07 mm1
c = 13.7079 (6) ÅT = 293 K
β = 100.239 (4)°Plate, colourless
V = 1496.62 (12) Å30.50 × 0.50 × 0.30 mm
Z = 4
Oxford Diffraction Xcalibur2 CCD diffractometer2392 independent reflections
Radiation source: Enhance (Mo)X-Ray Source2024 reflections with I > 2σ(I)
graphiteRint = 0.012
Detector resolution: 8.4190 pixels mm-1θmax = 31.9°, θmin = 4.1°
ω–2θ scansh = −8→7
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008)k = −26→26
Tmin = 0.967, Tmax = 0.980l = −18→20
7475 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.119H-atom parameters constrained
S = 1.02w = 1/[σ2(Fo2) + (0.0873P)2 + 0.017P] where P = (Fo2 + 2Fc2)/3
2392 reflections(Δ/σ)max = 0.001
175 parametersΔρmax = 0.21 e Å3
2 restraintsΔρmin = −0.21 e Å3
0 constraints
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.
xyzUiso*/Ueq
C140.2251 (5)0.16330 (11)0.59751 (18)0.0645 (6)
H200.14520.18750.64250.097*
H210.23140.19550.54210.097*
H190.37160.15250.63110.097*
C150.2342 (5)0.05704 (14)0.48509 (17)0.0679 (6)
H180.37670.04090.51800.102*
H160.25080.09370.43590.102*
H170.15370.01520.45370.102*
C16−0.1269 (5)0.10773 (16)0.5103 (2)0.0739 (7)
H15−0.19400.06300.48060.111*
H14−0.12600.14490.46000.111*
H13−0.20900.12580.55860.111*
N30.1632 (2)0.14031 (8)0.88126 (11)0.0448 (3)
C90.2329 (2)0.09809 (8)0.81277 (11)0.0365 (3)
N10.1221 (2)0.03781 (7)0.64559 (9)0.0382 (3)
C30.1172 (3)−0.09657 (8)0.68278 (12)0.0384 (3)
C100.4530 (3)0.08012 (10)0.81845 (13)0.0434 (3)
H80.49820.05130.76940.052*
C10.1094 (3)0.09104 (10)0.56073 (13)0.0455 (4)
C20.0134 (3)−0.03384 (10)0.61861 (13)0.0452 (4)
H110.0200−0.04490.54990.054*
H12−0.1403−0.03000.62450.054*
N2−0.0196 (2)−0.14516 (8)0.71406 (13)0.0476 (3)
C80.0527 (3)0.06774 (11)0.73393 (12)0.0442 (4)
H9−0.02320.02870.76330.053*
H10−0.05270.10730.71370.053*
C120.5344 (3)0.14791 (10)0.96934 (14)0.0529 (4)
H60.63290.16521.02400.063*
C110.6047 (3)0.10564 (11)0.89812 (15)0.0501 (4)
H70.75300.09410.90310.060*
C40.3437 (3)−0.10609 (10)0.70322 (14)0.0466 (4)
H40.4352−0.07130.68090.056*
C130.3140 (4)0.16421 (10)0.95790 (14)0.0519 (4)
H50.26640.19351.00600.062*
C50.4322 (3)−0.16716 (12)0.75666 (16)0.0553 (5)
H30.5836−0.17430.77080.066*
C60.2920 (4)−0.21757 (11)0.78883 (17)0.0567 (5)
H20.3460−0.25940.82520.068*
C70.0701 (3)−0.20409 (10)0.76555 (17)0.0554 (5)
H1−0.0242−0.23830.78710.066*
U11U22U33U12U13U23
C140.0927 (17)0.0403 (9)0.0584 (12)−0.0074 (10)0.0077 (11)0.0060 (8)
C150.0990 (18)0.0620 (12)0.0486 (11)−0.0019 (12)0.0296 (11)0.0014 (9)
C160.0720 (14)0.0773 (16)0.0638 (13)0.0155 (12)−0.0114 (11)0.0176 (11)
N30.0476 (8)0.0460 (7)0.0408 (7)0.0030 (6)0.0075 (6)−0.0021 (5)
C90.0370 (7)0.0395 (7)0.0324 (6)−0.0014 (5)0.0047 (5)0.0033 (5)
N10.0426 (7)0.0397 (6)0.0307 (6)−0.0034 (5)0.0021 (5)0.0008 (4)
C30.0404 (8)0.0389 (7)0.0347 (7)−0.0029 (6)0.0033 (5)−0.0005 (5)
C100.0369 (7)0.0529 (9)0.0396 (7)0.0002 (6)0.0044 (6)−0.0019 (6)
C10.0559 (10)0.0416 (8)0.0371 (7)0.0006 (6)0.0034 (7)0.0054 (6)
C20.0446 (8)0.0451 (8)0.0409 (8)−0.0067 (6)−0.0060 (6)0.0039 (6)
N20.0412 (7)0.0437 (7)0.0568 (9)−0.0058 (6)0.0056 (6)0.0045 (6)
C80.0342 (7)0.0603 (10)0.0369 (7)−0.0018 (6)0.0031 (6)−0.0030 (6)
C120.0612 (11)0.0493 (9)0.0427 (9)−0.0136 (8)−0.0054 (8)0.0022 (7)
C110.0403 (8)0.0573 (10)0.0493 (9)−0.0036 (7)−0.0013 (7)0.0072 (7)
C40.0371 (8)0.0526 (9)0.0514 (9)−0.0026 (6)0.0114 (7)0.0003 (7)
C130.0678 (11)0.0456 (8)0.0413 (9)−0.0018 (8)0.0071 (8)−0.0066 (7)
C50.0433 (9)0.0576 (10)0.0637 (12)0.0114 (8)0.0061 (8)−0.0027 (9)
C60.0618 (11)0.0419 (8)0.0640 (11)0.0110 (7)0.0043 (9)0.0033 (8)
C70.0539 (10)0.0426 (9)0.0702 (12)−0.0057 (7)0.0127 (9)0.0088 (8)
C14—C11.523 (3)C3—C21.501 (2)
C14—H200.9600C10—C111.385 (2)
C14—H210.9600C10—H80.9300
C14—H190.9600C2—H110.9700
C15—C11.525 (3)C2—H120.9700
C15—H180.9600N2—C71.336 (2)
C15—H160.9600C8—H90.9700
C15—H170.9600C8—H100.9700
C16—C11.531 (3)C12—C111.367 (3)
C16—H150.9600C12—C131.375 (3)
C16—H140.9600C12—H60.9300
C16—H130.9600C11—H70.9300
N3—C91.336 (2)C4—C51.377 (3)
N3—C131.345 (2)C4—H40.9300
C9—C101.387 (2)C13—H50.9300
C9—C81.509 (2)C5—C61.378 (3)
N1—C81.457 (2)C5—H30.9300
N1—C21.468 (2)C6—C71.374 (3)
N1—C11.497 (2)C6—H20.9300
C3—N21.338 (2)C7—H10.9300
C3—C41.388 (2)
C1—C14—H20109.5C15—C1—C16109.18 (19)
C1—C14—H21109.5N1—C2—C3112.38 (12)
H20—C14—H21109.5N1—C2—H11109.1
C1—C14—H19109.5C3—C2—H11109.1
H20—C14—H19109.5N1—C2—H12109.1
H21—C14—H19109.5C3—C2—H12109.1
C1—C15—H18109.5H11—C2—H12107.9
C1—C15—H16109.5C7—N2—C3117.31 (16)
H18—C15—H16109.5N1—C8—C9116.05 (14)
C1—C15—H17109.5N1—C8—H9108.3
H18—C15—H17109.5C9—C8—H9108.3
H16—C15—H17109.5N1—C8—H10108.3
C1—C16—H15109.5C9—C8—H10108.3
C1—C16—H14109.5H9—C8—H10107.4
H15—C16—H14109.5C11—C12—C13118.10 (17)
C1—C16—H13109.5C11—C12—H6121.0
H15—C16—H13109.5C13—C12—H6121.0
H14—C16—H13109.5C12—C11—C10119.36 (17)
C9—N3—C13117.70 (16)C12—C11—H7120.3
N3—C9—C10121.88 (15)C10—C11—H7120.3
N3—C9—C8114.75 (14)C5—C4—C3119.78 (16)
C10—C9—C8123.24 (14)C5—C4—H4120.1
C8—N1—C2110.06 (14)C3—C4—H4120.1
C8—N1—C1115.35 (14)N3—C13—C12123.79 (17)
C2—N1—C1113.90 (12)N3—C13—H5118.1
N2—C3—C4121.83 (15)C12—C13—H5118.1
N2—C3—C2116.63 (15)C4—C5—C6118.68 (17)
C4—C3—C2121.42 (15)C4—C5—H3120.7
C11—C10—C9119.16 (17)C6—C5—H3120.7
C11—C10—H8120.4C7—C6—C5117.95 (18)
C9—C10—H8120.4C7—C6—H2121.0
N1—C1—C14109.25 (14)C5—C6—H2121.0
N1—C1—C15108.06 (15)N2—C7—C6124.45 (18)
C14—C1—C15107.53 (19)N2—C7—H1117.8
N1—C1—C16112.96 (17)C6—C7—H1117.8
C14—C1—C16109.70 (18)
C13—N3—C9—C10−1.1 (2)C2—C3—N2—C7175.54 (17)
C13—N3—C9—C8174.86 (16)C2—N1—C8—C9134.62 (15)
N3—C9—C10—C111.0 (2)C1—N1—C8—C9−94.82 (18)
C8—C9—C10—C11−174.62 (17)N3—C9—C8—N1165.09 (14)
C8—N1—C1—C1450.8 (2)C10—C9—C8—N1−19.0 (2)
C2—N1—C1—C14179.45 (17)C13—C12—C11—C10−0.8 (3)
C8—N1—C1—C15167.47 (17)C9—C10—C11—C120.0 (3)
C2—N1—C1—C15−63.8 (2)N2—C3—C4—C50.3 (3)
C8—N1—C1—C16−71.6 (2)C2—C3—C4—C5−175.51 (17)
C2—N1—C1—C1657.1 (2)C9—N3—C13—C120.3 (3)
C8—N1—C2—C3−77.86 (18)C11—C12—C13—N30.7 (3)
C1—N1—C2—C3150.82 (15)C3—C4—C5—C6−0.1 (3)
N2—C3—C2—N1137.29 (16)C4—C5—C6—C70.1 (3)
C4—C3—C2—N1−46.7 (2)C3—N2—C7—C60.5 (3)
C4—C3—N2—C7−0.5 (3)C5—C6—C7—N2−0.3 (3)
D—H···AD—HH···AD···AD—H···A
C7—H1···Cg2i0.932.973.819 (2)153
C15—H16···Cg1ii0.962.943.836 (2)156
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the N2/C3–C7and N3/C9–C13 rings, respectively.

D—H⋯AD—HH⋯ADAD—H⋯A
C7—H1⋯Cg2i0.932.973.819 (2)153
C15—H16⋯Cg1ii0.962.943.836 (2)156

Symmetry codes: (i) ; (ii) .

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