Literature DB >> 21201154

(S)-1,2-Dimethyl-1,1,2-triphenyl-2-(4-piperidiniometh-yl)disilane chloride.

Christian Däschlein1, Viktoria H Gessner, Carsten Strohmann.   

Abstract

The title compound, C(26)H(34)NSi(2) (+)·Cl(-), shows chirality at silicon. Because of its highly selective synthesis with an e.r. of >99:1 by means of a racemic resolution with mandelic acid, the free disilane is of great importance to the chemistry of highly enanti-omerically enriched lithio-silanes and their trapping products. N-H⋯Cl hydrogen bonding is present between the protonated nitro-gen atom of the piperidino group and the chloride counter-anion. The silicon-silicon distance as well as silicon-carbon and carbon-nitro-gen bond lengths are in the same ranges as in other quaternary, functionalized di- and tetra-silanes.

Entities:  

Year:  2008        PMID: 21201154      PMCID: PMC2959254          DOI: 10.1107/S1600536808028808

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


Related literature

For details of lithio­silanes, see: Lickiss & Smith (1995 ▶); Sekiguchi et al. (2000 ▶); Strohmann et al. (2001 ▶, 2006 ▶); Strohmann & Däschlein (2008a ▶,b ▶); Tamao & Kawachi (1995 ▶). For enanti­o­merically enriched lithio­silanes, see: Colomer & Corriu (1976 ▶); Oestreich et al. (2005 ▶); Omote et al. (2000 ▶); Sommer & Mason (1965 ▶); Strohmann et al. (2007 ▶). For the determination of the absolute configuration of the disilane as the mandelic acid adduct, see: Strohmann et al. (2002 ▶). For related literature on hydro­chlorides of amines, see: Farrugia et al. (2001 ▶).

Experimental

Crystal data

C26H34NSi2 +·Cl− M = 452.19 Orthorhombic, a = 10.120 (2) Å b = 13.289 (3) Å c = 18.598 (4) Å V = 2501.3 (9) Å3 Z = 4 Mo Kα radiation μ = 0.26 mm−1 T = 173 (2) K 0.30 × 0.30 × 0.20 mm

Data collection

Bruker SMART APEX CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 1999 ▶) T min = 0.926, T max = 0.950 45451 measured reflections 4911 independent reflections 4808 reflections with I > 2σ(I) R int = 0.077

Refinement

R[F 2 > 2σ(F 2)] = 0.055 wR(F 2) = 0.149 S = 1.05 4911 reflections 277 parameters H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.41 e Å−3 Δρmin = −0.34 e Å−3 Absolute structure: Flack (1983 ▶), 2128 Friedel pairs Flack parameter: 0.08 (10) Data collection: SMART (Bruker, 2001 ▶); cell refinement: SAINT-Plus (Bruker, 1999 ▶); data reduction: SAINT-Plus; 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: SHELXL97. Crystal structure: contains datablocks I, New_Global_Publ_Block. DOI: 10.1107/S1600536808028808/wm2191sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808028808/wm2191Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C26H34NSi2+·ClF(000) = 968
Mr = 452.19Dx = 1.201 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 999 reflections
a = 10.120 (2) Åθ = 1.9–26.0°
b = 13.289 (3) ŵ = 0.26 mm1
c = 18.598 (4) ÅT = 173 K
V = 2501.3 (9) Å3Block, colourless
Z = 40.30 × 0.30 × 0.20 mm
Bruker SMART APEX CCD diffractometer4911 independent reflections
Radiation source: fine-focus sealed tube4808 reflections with I > 2σ(I)
graphiteRint = 0.077
ω–scansθmax = 26.0°, θmin = 1.9°
Absorption correction: multi-scan (SADABS; Bruker, 1999)h = −12→12
Tmin = 0.926, Tmax = 0.950k = −16→16
45451 measured reflectionsl = −22→22
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.055H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.149w = 1/[σ2(Fo2) + (0.0402P)2 + 1.4067P] where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
4911 reflectionsΔρmax = 0.41 e Å3
277 parametersΔρmin = −0.34 e Å3
0 restraintsAbsolute structure: Flack (1983), 2128 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.08 (10)
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
Cl−0.09614 (10)0.04149 (6)0.25243 (5)0.0361 (2)
Si10.28622 (9)0.21087 (7)0.20801 (5)0.0249 (2)
Si20.40619 (9)0.23973 (7)0.10071 (5)0.0276 (2)
N10.0148 (3)0.2532 (2)0.25691 (15)0.0246 (5)
C3−0.2128 (4)0.2953 (3)0.2978 (2)0.0346 (8)
H3B−0.24110.22410.29610.042*
H3A−0.29090.33780.28760.042*
C170.4393 (5)0.0299 (3)−0.0646 (2)0.0433 (10)
H170.50600.0075−0.09680.052*
C80.3754 (3)0.2680 (3)0.28642 (17)0.0271 (7)
C2−0.1098 (3)0.3132 (3)0.24077 (19)0.0309 (7)
H2A−0.08810.38580.23870.037*
H2B−0.14520.29300.19330.037*
C160.4683 (4)0.1011 (3)−0.0121 (2)0.0374 (9)
H160.55590.1262−0.00820.045*
C60.0655 (3)0.2780 (3)0.32978 (17)0.0297 (7)
H6A0.09220.34960.33120.036*
H6B0.14460.23660.34000.036*
C10.1159 (3)0.2715 (2)0.19928 (16)0.0273 (7)
H1A0.12900.34520.19560.033*
H1B0.07730.24890.15310.033*
C110.4933 (4)0.3529 (4)0.4090 (2)0.0456 (10)
H110.53150.38120.45100.055*
C180.3126 (5)−0.0077 (3)−0.0696 (2)0.0435 (10)
H180.2926−0.0565−0.10540.052*
C190.2150 (5)0.0243 (3)−0.0237 (2)0.0466 (10)
H190.1282−0.0025−0.02730.056*
C100.4387 (4)0.4145 (3)0.3574 (2)0.0386 (9)
H100.44160.48550.36300.046*
C210.3634 (3)0.3622 (3)0.05534 (19)0.0302 (7)
C240.3080 (4)0.5453 (3)−0.0126 (2)0.0411 (9)
H240.28990.6077−0.03550.049*
C260.3724 (4)0.3723 (3)−0.0189 (2)0.0366 (8)
H260.39780.3157−0.04690.044*
C230.2970 (4)0.5373 (3)0.0615 (2)0.0420 (9)
H230.27080.59380.08940.050*
C90.3793 (4)0.3723 (3)0.29742 (19)0.0314 (7)
H90.34000.41540.26270.038*
C140.5853 (4)0.2419 (3)0.1259 (2)0.0397 (8)
H14C0.63920.24820.08230.060*
H14B0.60810.17940.15090.060*
H14A0.60240.29940.15760.060*
C70.2688 (4)0.0726 (3)0.2230 (2)0.0357 (8)
H7B0.35670.04200.22660.054*
H7C0.22090.04260.18250.054*
H7A0.21980.06070.26760.054*
C4−0.1613 (4)0.3193 (3)0.3725 (2)0.0394 (9)
H4A−0.14160.39200.37620.047*
H4B−0.22930.30240.40880.047*
C220.3244 (4)0.4466 (3)0.0945 (2)0.0363 (8)
H220.31660.44150.14520.044*
C120.4926 (4)0.2503 (4)0.3995 (2)0.0435 (9)
H120.53150.20800.43480.052*
C5−0.0374 (4)0.2590 (3)0.38669 (18)0.0334 (8)
H5A−0.00120.27740.43440.040*
H5B−0.05950.18640.38760.040*
C200.2446 (4)0.0968 (3)0.0282 (2)0.0368 (9)
H200.17700.11960.05960.044*
C150.3720 (4)0.1364 (3)0.03482 (18)0.0314 (8)
C130.4352 (4)0.2081 (3)0.33837 (18)0.0338 (8)
H130.43690.13720.33210.041*
C250.3450 (4)0.4636 (3)−0.0533 (2)0.0434 (9)
H250.35180.4690−0.10410.052*
H100−0.007 (5)0.180 (4)0.254 (3)0.050 (12)*
U11U22U33U12U13U23
Cl0.0441 (5)0.0229 (4)0.0413 (5)−0.0063 (4)−0.0004 (4)−0.0006 (3)
Si10.0270 (5)0.0232 (4)0.0246 (4)−0.0006 (4)0.0003 (4)−0.0014 (3)
Si20.0272 (5)0.0288 (4)0.0269 (4)0.0008 (4)0.0010 (4)−0.0027 (4)
N10.0219 (13)0.0218 (13)0.0300 (13)−0.0003 (11)−0.0012 (11)−0.0007 (11)
C30.0275 (17)0.0338 (18)0.0425 (19)0.0043 (15)−0.0010 (16)0.0033 (16)
C170.059 (3)0.040 (2)0.0312 (18)0.018 (2)0.0047 (17)−0.0007 (16)
C80.0232 (16)0.0319 (18)0.0263 (14)−0.0005 (13)0.0004 (13)−0.0045 (13)
C20.0268 (17)0.0288 (16)0.0370 (17)0.0046 (14)−0.0029 (15)0.0047 (14)
C160.044 (2)0.0319 (19)0.036 (2)0.0022 (16)0.0021 (17)0.0010 (15)
C60.0299 (18)0.0297 (17)0.0296 (15)−0.0014 (14)−0.0039 (13)0.0027 (14)
C10.0310 (17)0.0254 (16)0.0254 (15)−0.0010 (13)0.0006 (13)0.0002 (12)
C110.035 (2)0.067 (3)0.034 (2)0.003 (2)−0.0007 (17)−0.0203 (19)
C180.066 (3)0.037 (2)0.0277 (17)0.006 (2)−0.0085 (19)−0.0083 (15)
C190.046 (2)0.048 (2)0.046 (2)0.000 (2)−0.0119 (19)−0.0086 (18)
C100.030 (2)0.040 (2)0.046 (2)−0.0015 (16)0.0077 (16)−0.0142 (17)
C210.0263 (18)0.0330 (17)0.0314 (17)−0.0021 (14)0.0021 (14)0.0005 (14)
C240.038 (2)0.035 (2)0.051 (2)−0.0022 (17)−0.0056 (17)0.0141 (18)
C260.036 (2)0.039 (2)0.0353 (19)−0.0011 (16)−0.0011 (16)−0.0027 (16)
C230.044 (2)0.0252 (17)0.057 (2)−0.0022 (17)0.0085 (19)0.0011 (17)
C90.0306 (19)0.0304 (17)0.0333 (17)−0.0031 (14)−0.0030 (15)0.0015 (15)
C140.0336 (19)0.047 (2)0.0386 (19)0.0019 (18)−0.0008 (16)−0.0016 (17)
C70.046 (2)0.0242 (16)0.0369 (18)−0.0006 (16)0.0047 (16)0.0003 (14)
C40.035 (2)0.045 (2)0.0382 (19)0.0024 (17)0.0073 (16)−0.0065 (17)
C220.036 (2)0.0367 (19)0.0360 (18)−0.0055 (16)0.0053 (15)0.0010 (16)
C120.038 (2)0.061 (3)0.0323 (18)0.0150 (19)−0.0073 (16)0.0049 (19)
C50.0322 (18)0.0378 (19)0.0302 (17)−0.0004 (15)0.0056 (14)−0.0009 (15)
C200.036 (2)0.039 (2)0.0353 (19)0.0032 (16)0.0016 (16)−0.0080 (15)
C150.037 (2)0.0297 (17)0.0281 (17)0.0024 (15)−0.0028 (14)0.0009 (13)
C130.034 (2)0.0348 (18)0.0325 (17)0.0053 (16)−0.0001 (14)0.0002 (15)
C250.049 (2)0.044 (2)0.0368 (19)−0.0060 (19)−0.0076 (18)0.0085 (18)
Cl—H1002.05 (5)C18—H180.9500
Si1—C71.867 (4)C19—C201.397 (6)
Si1—C81.876 (3)C19—H190.9500
Si1—C11.910 (3)C10—C91.386 (5)
Si1—Si22.3672 (13)C10—H100.9500
Si2—C141.873 (4)C21—C261.390 (5)
Si2—C151.873 (4)C21—C221.393 (5)
Si2—C211.884 (4)C24—C251.375 (6)
N1—C61.486 (4)C24—C231.388 (6)
N1—C11.502 (4)C24—H240.9500
N1—C21.521 (4)C26—C251.400 (6)
N1—H1001.00 (5)C26—H260.9500
C3—C21.506 (5)C23—C221.381 (6)
C3—C41.518 (5)C23—H230.9500
C3—H3B0.9900C9—H90.9500
C3—H3A0.9900C14—H14C0.9800
C17—C181.379 (7)C14—H14B0.9800
C17—C161.392 (6)C14—H14A0.9800
C17—H170.9500C7—H7B0.9800
C8—C131.391 (5)C7—H7C0.9800
C8—C91.402 (5)C7—H7A0.9800
C2—H2A0.9900C4—C51.511 (5)
C2—H2B0.9900C4—H4A0.9900
C16—C151.389 (5)C4—H4B0.9900
C16—H160.9500C22—H220.9500
C6—C51.506 (5)C12—C131.395 (5)
C6—H6A0.9900C12—H120.9500
C6—H6B0.9900C5—H5A0.9900
C1—H1A0.9900C5—H5B0.9900
C1—H1B0.9900C20—C151.398 (5)
C11—C121.374 (7)C20—H200.9500
C11—C101.377 (6)C13—H130.9500
C11—H110.9500C25—H250.9500
C18—C191.374 (6)N1—Cl3.031 (3)
C7—Si1—C8109.16 (17)C11—C10—H10120.2
C7—Si1—C1110.05 (17)C9—C10—H10120.2
C8—Si1—C1109.24 (14)C26—C21—C22117.4 (3)
C7—Si1—Si2109.48 (13)C26—C21—Si2120.9 (3)
C8—Si1—Si2110.06 (11)C22—C21—Si2121.7 (3)
C1—Si1—Si2108.84 (10)C25—C24—C23120.5 (4)
C14—Si2—C15110.72 (17)C25—C24—H24119.7
C14—Si2—C21108.73 (17)C23—C24—H24119.7
C15—Si2—C21107.34 (15)C21—C26—C25121.6 (4)
C14—Si2—Si1106.77 (13)C21—C26—H26119.2
C15—Si2—Si1109.76 (12)C25—C26—H26119.2
C21—Si2—Si1113.55 (12)C22—C23—C24119.4 (4)
C6—N1—C1112.3 (2)C22—C23—H23120.3
C6—N1—C2110.5 (3)C24—C23—H23120.3
C1—N1—C2109.8 (2)C10—C9—C8122.0 (3)
C6—N1—H100110 (3)C10—C9—H9119.0
C1—N1—H100105 (3)C8—C9—H9119.0
C2—N1—H100109 (3)Si2—C14—H14C109.5
C2—C3—C4112.0 (3)Si2—C14—H14B109.5
C2—C3—H3B109.2H14C—C14—H14B109.5
C4—C3—H3B109.2Si2—C14—H14A109.5
C2—C3—H3A109.2H14C—C14—H14A109.5
C4—C3—H3A109.2H14B—C14—H14A109.5
H3B—C3—H3A107.9Si1—C7—H7B109.5
C18—C17—C16119.4 (4)Si1—C7—H7C109.5
C18—C17—H17120.3H7B—C7—H7C109.5
C16—C17—H17120.3Si1—C7—H7A109.5
C13—C8—C9116.9 (3)H7B—C7—H7A109.5
C13—C8—Si1121.2 (3)H7C—C7—H7A109.5
C9—C8—Si1121.8 (3)C5—C4—C3109.5 (3)
C3—C2—N1110.6 (3)C5—C4—H4A109.8
C3—C2—H2A109.5C3—C4—H4A109.8
N1—C2—H2A109.5C5—C4—H4B109.8
C3—C2—H2B109.5C3—C4—H4B109.8
N1—C2—H2B109.5H4A—C4—H4B108.2
H2A—C2—H2B108.1C23—C22—C21121.9 (4)
C15—C16—C17121.5 (4)C23—C22—H22119.1
C15—C16—H16119.3C21—C22—H22119.1
C17—C16—H16119.3C11—C12—C13120.4 (4)
N1—C6—C5111.4 (3)C11—C12—H12119.8
N1—C6—H6A109.3C13—C12—H12119.8
C5—C6—H6A109.3C6—C5—C4111.2 (3)
N1—C6—H6B109.3C6—C5—H5A109.4
C5—C6—H6B109.3C4—C5—H5A109.4
H6A—C6—H6B108.0C6—C5—H5B109.4
N1—C1—Si1119.1 (2)C4—C5—H5B109.4
N1—C1—H1A107.5H5A—C5—H5B108.0
Si1—C1—H1A107.5C19—C20—C15121.2 (4)
N1—C1—H1B107.5C19—C20—H20119.4
Si1—C1—H1B107.5C15—C20—H20119.4
H1A—C1—H1B107.0C16—C15—C20117.7 (3)
C12—C11—C10119.9 (4)C16—C15—Si2121.9 (3)
C12—C11—H11120.1C20—C15—Si2120.3 (3)
C10—C11—H11120.1C8—C13—C12121.1 (4)
C19—C18—C17121.0 (4)C8—C13—H13119.4
C19—C18—H18119.5C12—C13—H13119.4
C17—C18—H18119.5C24—C25—C26119.1 (4)
C18—C19—C20119.3 (4)C24—C25—H25120.4
C18—C19—H19120.4C26—C25—H25120.4
C20—C19—H19120.4N1—H100—Cl166.1 (41)
C11—C10—C9119.6 (4)
D—H···AD—HH···AD···AD—H···A
N1—H100···Cl1.00 (5)2.05 (5)3.031 (3)166 (4)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H100⋯Cl1.00 (5)2.05 (5)3.031 (3)166 (4)
  5 in total

1.  A highly enantiomerically enriched lithiosilane by selective cleavage of a silicon-phenyl bond with lithium.

Authors:  Carsten Strohmann; Christian Däschlein; Marco Kellert; Dominik Auer
Journal:  Angew Chem Int Ed Engl       Date:  2007       Impact factor: 15.336

2.  A short history of SHELX.

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

3.  Crystal structures of the chiral lithiosilanes [(Lis)-PhMe2SiLi x THF x (-)-sparteine] and [Ph2(NEt2)SiLi x (-)-sparteine].

Authors:  Carsten Strohmann; Christian Däschlein; Dominik Auer
Journal:  J Am Chem Soc       Date:  2006-01-25       Impact factor: 15.419

4.  Bent phenyl groups in lithiosilanes--crystal structures and interpretation of this unanticipated feature.

Authors:  Carsten Strohmann; Christian Däschlein
Journal:  Chem Commun (Camb)       Date:  2008-04-16       Impact factor: 6.222

5.  Synthesis of a highly enantiomerically enriched silyllithium compound.

Authors:  Carsten Strohmann; Jan Hörnig; Dominik Auer
Journal:  Chem Commun (Camb)       Date:  2002-04-07       Impact factor: 6.222

  5 in total

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