Literature DB >> 22719584

3-Phenyl-N,N,N',N'-tetra-methyl-1-ethyne-1-carboximidamidium bromide.

Ioannis Tiritiris, Willi Kantlehner.   

Abstract

The reaction of 3,3,3-tris-(dimethyl-amino)-1-phenyl-prop-1-yne with bromine in pentane yields the title compound, C(13)H(17)N(2) (+)·Br(-). The acetyl-enic bond distance [1.197 (2) Å] is consistent with a C C triple bond. The amidinium C=N bonds [1.325 (2) and 1.330 (2) Å] have double-bond character and the positive charge is delocalized between the two dimethyl-amino groups.

Entities:  

Year:  2012        PMID: 22719584      PMCID: PMC3379386          DOI: 10.1107/S1600536812021873

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


Related literature

For the synthesis of alkynyl orthoamides and acetyl­enic amidinium salts, see: Weingärtner et al. (2011 ▶). For the synthesis of vinyl­ogous guanidinium iodides and bromides, see: Kantlehner et al. (2012 ▶). For the crystal structure of N,N,N′,N′,N′′,N′′,N′′′,N′′′-octa­methyl-(but-2-yne)-bis­(amidinium)-bis­(tetra­fluoridoborate), see: Drandarov et al. (2012 ▶).

Experimental

Crystal data

C13H17N2Br M = 281.19 Monoclinic, a = 13.1009 (8) Å b = 10.6538 (6) Å c = 9.6611 (6) Å β = 100.276 (3)° V = 1326.81 (14) Å3 Z = 4 Mo Kα radiation μ = 3.08 mm−1 T = 100 K 0.28 × 0.20 × 0.15 mm

Data collection

Bruker Kappa APEXII DUO diffractometer Absorption correction: multi-scan (Blessing, 1995) ▶ T min = 0.483, T max = 0.630 27687 measured reflections 4075 independent reflections 3466 reflections with I > 2σ(I) R int = 0.032

Refinement

R[F 2 > 2σ(F 2)] = 0.021 wR(F 2) = 0.052 S = 1.07 4075 reflections 149 parameters H-atom parameters constrained Δρmax = 0.38 e Å−3 Δρmin = −0.43 e Å−3 Data collection: APEX2 (n class="Chemical">Bruker, 2008 ▶); cell refinement: SAINT (Bruker, 2008 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 2005 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812021873/kp2415sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812021873/kp2415Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C13H17N2+·BrF(000) = 576
Mr = 281.19Dx = 1.408 Mg m3
Monoclinic, P21/cMelting point: 441 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 13.1009 (8) ÅCell parameters from 4075 reflections
b = 10.6538 (6) Åθ = 2.5–30.6°
c = 9.6611 (6) ŵ = 3.08 mm1
β = 100.276 (3)°T = 100 K
V = 1326.81 (14) Å3Block, yellow
Z = 40.28 × 0.20 × 0.15 mm
Bruker Kappa APEXII DUO diffractometer4075 independent reflections
Radiation source: sealed tube3466 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.032
φ scans, and ω scansθmax = 30.6°, θmin = 2.5°
Absorption correction: multi-scan (Blessing, 1995)h = −18→18
Tmin = 0.483, Tmax = 0.630k = −15→15
27687 measured reflectionsl = −13→13
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.021Hydrogen site location: difference Fourier map
wR(F2) = 0.052H-atom parameters constrained
S = 1.07w = 1/[σ2(Fo2) + (0.024P)2 + 0.4023P] where P = (Fo2 + 2Fc2)/3
4075 reflections(Δ/σ)max < 0.001
149 parametersΔρmax = 0.38 e Å3
0 restraintsΔρmin = −0.43 e Å3
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
Br10.313905 (9)0.523031 (12)0.155779 (13)0.01703 (4)
C10.29358 (9)0.46256 (11)0.66879 (12)0.0128 (2)
N10.35589 (8)0.56042 (10)0.66379 (10)0.01344 (19)
N20.30756 (8)0.37987 (10)0.77285 (11)0.0147 (2)
C20.41450 (10)0.62002 (12)0.79005 (13)0.0164 (2)
H2A0.38820.59040.87310.025*
H2B0.40650.71130.78230.025*
H2C0.48810.59820.79920.025*
C30.35920 (11)0.62655 (13)0.53213 (13)0.0205 (3)
H3A0.31400.58380.45460.031*
H3B0.43050.62710.51430.031*
H3C0.33530.71310.53920.031*
C40.22431 (11)0.29642 (12)0.79900 (15)0.0207 (3)
H4A0.15800.32550.74510.031*
H4B0.22100.29700.89950.031*
H4C0.23820.21090.76990.031*
C50.40815 (10)0.35338 (13)0.86079 (14)0.0203 (3)
H5A0.46350.39000.81750.031*
H5B0.41810.26240.86950.031*
H5C0.41030.39000.95430.031*
C60.20698 (10)0.44506 (11)0.55744 (13)0.0153 (2)
C70.13169 (9)0.42701 (11)0.46956 (13)0.0148 (2)
C80.04099 (9)0.40275 (11)0.36723 (12)0.0133 (2)
C9−0.02930 (10)0.31159 (11)0.39520 (14)0.0170 (2)
H9A−0.01560.26510.48040.020*
C10−0.11893 (10)0.28928 (12)0.29838 (15)0.0204 (3)
H10A−0.16690.22740.31710.024*
C11−0.13845 (10)0.35719 (13)0.17439 (14)0.0203 (3)
H11A−0.20020.34200.10840.024*
C12−0.06867 (10)0.44725 (13)0.14572 (14)0.0195 (3)
H12A−0.08280.49350.06030.023*
C130.02160 (10)0.46995 (12)0.24136 (13)0.0167 (2)
H13A0.06990.53080.22130.020*
U11U22U33U12U13U23
Br10.01516 (6)0.01901 (6)0.01757 (7)0.00196 (5)0.00471 (4)−0.00012 (5)
C10.0109 (5)0.0140 (5)0.0139 (5)0.0021 (4)0.0035 (4)−0.0027 (4)
N10.0132 (5)0.0152 (4)0.0115 (4)−0.0012 (4)0.0012 (4)−0.0005 (4)
N20.0138 (5)0.0147 (5)0.0158 (5)0.0012 (4)0.0034 (4)0.0016 (4)
C20.0149 (6)0.0184 (6)0.0150 (6)−0.0022 (4)0.0001 (4)−0.0030 (4)
C30.0242 (7)0.0219 (6)0.0151 (6)−0.0052 (5)0.0028 (5)0.0034 (5)
C40.0224 (7)0.0158 (6)0.0258 (7)−0.0025 (5)0.0091 (5)0.0024 (5)
C50.0184 (6)0.0224 (6)0.0194 (6)0.0077 (5)0.0010 (5)0.0047 (5)
C60.0148 (6)0.0131 (5)0.0182 (6)0.0011 (4)0.0034 (4)−0.0018 (4)
C70.0140 (5)0.0130 (5)0.0179 (6)0.0008 (4)0.0045 (4)−0.0020 (4)
C80.0105 (5)0.0125 (5)0.0167 (6)0.0008 (4)0.0023 (4)−0.0039 (4)
C90.0162 (6)0.0141 (5)0.0216 (6)−0.0001 (4)0.0056 (5)−0.0007 (4)
C100.0131 (6)0.0171 (6)0.0323 (7)−0.0037 (5)0.0076 (5)−0.0081 (5)
C110.0105 (6)0.0252 (6)0.0246 (6)0.0019 (5)0.0010 (5)−0.0124 (5)
C120.0171 (6)0.0254 (6)0.0153 (6)0.0034 (5)0.0009 (5)−0.0022 (5)
C130.0140 (6)0.0169 (6)0.0191 (6)−0.0015 (4)0.0032 (5)−0.0005 (5)
C1—N21.3246 (15)C5—H5A0.9800
C1—N11.3304 (16)C5—H5B0.9800
C1—C61.4296 (17)C5—H5C0.9800
N1—C31.4615 (15)C6—C71.1966 (17)
N1—C21.4651 (15)C7—C81.4273 (17)
N2—C51.4625 (16)C8—C131.3949 (17)
N2—C41.4636 (16)C8—C91.3974 (17)
C2—H2A0.9800C9—C101.3851 (18)
C2—H2B0.9800C9—H9A0.9500
C2—H2C0.9800C10—C111.384 (2)
C3—H3A0.9800C10—H10A0.9500
C3—H3B0.9800C11—C121.3870 (19)
C3—H3C0.9800C11—H11A0.9500
C4—H4A0.9800C12—C131.3860 (18)
C4—H4B0.9800C12—H12A0.9500
C4—H4C0.9800C13—H13A0.9500
N2—C1—N1123.10 (11)N2—C5—H5A109.5
N2—C1—C6117.91 (11)N2—C5—H5B109.5
N1—C1—C6118.99 (11)H5A—C5—H5B109.5
C1—N1—C3121.53 (10)N2—C5—H5C109.5
C1—N1—C2122.91 (10)H5A—C5—H5C109.5
C3—N1—C2115.04 (10)H5B—C5—H5C109.5
C1—N2—C5123.89 (11)C7—C6—C1176.30 (13)
C1—N2—C4121.91 (11)C6—C7—C8178.36 (13)
C5—N2—C4113.86 (10)C13—C8—C9120.10 (11)
N1—C2—H2A109.5C13—C8—C7120.69 (11)
N1—C2—H2B109.5C9—C8—C7119.20 (11)
H2A—C2—H2B109.5C10—C9—C8119.81 (12)
N1—C2—H2C109.5C10—C9—H9A120.1
H2A—C2—H2C109.5C8—C9—H9A120.1
H2B—C2—H2C109.5C11—C10—C9119.90 (12)
N1—C3—H3A109.5C11—C10—H10A120.0
N1—C3—H3B109.5C9—C10—H10A120.0
H3A—C3—H3B109.5C10—C11—C12120.53 (12)
N1—C3—H3C109.5C10—C11—H11A119.7
H3A—C3—H3C109.5C12—C11—H11A119.7
H3B—C3—H3C109.5C13—C12—C11120.13 (12)
N2—C4—H4A109.5C13—C12—H12A119.9
N2—C4—H4B109.5C11—C12—H12A119.9
H4A—C4—H4B109.5C12—C13—C8119.51 (11)
N2—C4—H4C109.5C12—C13—H13A120.2
H4A—C4—H4C109.5C8—C13—H13A120.2
H4B—C4—H4C109.5
N2—C1—N1—C3160.73 (11)C13—C8—C9—C10−0.83 (18)
C6—C1—N1—C3−19.49 (17)C7—C8—C9—C10178.38 (11)
N2—C1—N1—C2−27.94 (18)C8—C9—C10—C110.07 (18)
C6—C1—N1—C2151.84 (11)C9—C10—C11—C120.32 (19)
N1—C1—N2—C5−25.57 (18)C10—C11—C12—C130.06 (19)
C6—C1—N2—C5154.65 (11)C11—C12—C13—C8−0.82 (19)
N1—C1—N2—C4161.57 (12)C9—C8—C13—C121.20 (18)
C6—C1—N2—C4−18.20 (17)C7—C8—C13—C12−178.00 (11)
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1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  An empirical correction for absorption anisotropy.

Authors:  R H Blessing
Journal:  Acta Crystallogr A       Date:  1995-01-01       Impact factor: 2.290

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Authors:  Konstantin Drandarov; Ioannis Tiritiris; Olga Wassiljew; Hans-Ullrich Siehl; Willi Kantlehner
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Authors:  Ioannis Tiritiris; Ralf Kress; Willi Kantlehner
Journal:  Acta Crystallogr E Crystallogr Commun       Date:  2015-12-16

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  2 in total

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