Download citation
Download citation
link to html
(±)-Pinenyllithium·TMEDA or (tetra­methyl­ethylenedi­amine-κ2N,N′)(η3-6,6-di­methyl-2-methylenebi­cyclo­[3.1.1]hept­yl)lithium, [Li(C10H15)(C6H16N2)], is readily pre­pared from β-pinene, butyl­lithium and TMEDA, and the racemic material pre­fer­entially crystallizes even from 96:4 (92% ee) mixtures of (−)- and (+)-β-pinene, respectively. The structure is monomeric, with the geminal-dimethyl bridge of the bicyclic structure shielding one face of the allyl system, restricting the lithium to the opposite face and preventing the Li–all­yl–Li aggregation observed with some other allyl­lithium systems. The symmetry of the allyl system, bond lengths, bond angles and out-of-plane deviations are com­pared to existing structures. In addition, a much older structure of this com­plex is compared to this very recent one.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229624004662/oj3017sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229624004662/oj3017Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229624004662/oj3017sup3.pdf
Complete tables of X-ray results

CCDC reference: 2323107

Computing details top

(Tetramethylethylenediamine-κ2N,N')(η3-2,6,6-\ trimethylbicyclo[3.1.1]heptyl)lithium top
Crystal data top
[Li(C10H15)(C6H16N2)]Z = 2
Mr = 258.37F(000) = 288
Triclinic, P1Dx = 1.047 Mg m3
a = 6.3160 (2) ÅCu Kα radiation, λ = 1.54184 Å
b = 9.6925 (2) ÅCell parameters from 17767 reflections
c = 13.7463 (2) Åθ = 3.3–77.9°
α = 97.336 (1)°µ = 0.44 mm1
β = 99.662 (2)°T = 120 K
γ = 93.520 (2)°Plate, translucent pale yellow
V = 819.83 (3) Å30.35 × 0.11 × 0.04 mm
Data collection top
Rigaku XtaLAB Synergy-S single source
diffractometer
3373 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet-S (Cu) X-ray Source3167 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.056
Detector resolution: 10.0000 pixels mm-1θmax = 77.9°, θmin = 3.3°
combination of ω and φ–scansh = 76
Absorption correction: gaussian
(CrysAlis PRO; Rigaku OD, 2021)
k = 1212
Tmin = 0.675, Tmax = 1.000l = 1716
20391 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: difference Fourier map
wR(F2) = 0.108All H-atom parameters refined
S = 1.09 w = 1/[σ2(Fo2) + (0.0589P)2 + 0.1668P]
where P = (Fo2 + 2Fc2)/3
3373 reflections(Δ/σ)max < 0.001
296 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = 0.22 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. All hydrogen atoms were found from difference Fourier maps and allowed to refine freely.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Li0.7333 (3)0.33286 (17)0.29985 (12)0.0238 (3)
C10.96126 (15)0.54977 (10)0.17707 (7)0.0192 (2)
H11.093 (2)0.5059 (13)0.1561 (9)0.025 (3)*
C20.92371 (15)0.51687 (9)0.27849 (7)0.0188 (2)
C30.73585 (15)0.56432 (10)0.30578 (7)0.0219 (2)
H30.710 (2)0.5586 (14)0.3725 (10)0.032 (3)*
C40.60919 (16)0.66118 (11)0.24454 (8)0.0248 (2)
H4A0.451 (2)0.6263 (14)0.2234 (10)0.034 (3)*
H4B0.614 (2)0.7578 (14)0.2846 (9)0.029 (3)*
C50.70154 (15)0.67625 (10)0.14985 (7)0.0224 (2)
H50.617 (2)0.7371 (14)0.1054 (10)0.030 (3)*
C60.95159 (14)0.71071 (10)0.17399 (7)0.0186 (2)
C70.74359 (16)0.52871 (11)0.10259 (7)0.0247 (2)
H7A0.762 (2)0.5245 (14)0.0308 (10)0.032 (3)*
H7B0.636 (2)0.4509 (14)0.1098 (10)0.032 (3)*
C81.04218 (16)0.75584 (11)0.08552 (7)0.0242 (2)
H8A0.990 (2)0.6944 (15)0.0226 (11)0.036 (3)*
H8B1.204 (2)0.7590 (14)0.0975 (10)0.035 (3)*
H8C1.000 (2)0.8539 (15)0.0756 (10)0.034 (3)*
C91.04919 (16)0.81089 (10)0.26738 (7)0.0220 (2)
H9A1.030 (2)0.9114 (15)0.2559 (10)0.037 (4)*
H9B0.980 (2)0.7952 (14)0.3236 (10)0.031 (3)*
H9C1.209 (2)0.8000 (14)0.2866 (10)0.031 (3)*
C101.06426 (16)0.43194 (10)0.32858 (7)0.0223 (2)
H10A1.200 (2)0.4133 (13)0.3047 (10)0.029 (3)*
H10B1.058 (2)0.4284 (14)0.3996 (10)0.029 (3)*
N10.57757 (12)0.16997 (8)0.19027 (6)0.01942 (19)
N20.64698 (13)0.21831 (8)0.40976 (6)0.02063 (19)
C110.48749 (16)0.11036 (10)0.34912 (7)0.0235 (2)
H11B0.465 (2)0.0293 (14)0.3874 (10)0.033 (3)*
H11A0.345 (2)0.1544 (14)0.3348 (10)0.033 (3)*
C120.55534 (17)0.05691 (10)0.25143 (7)0.0237 (2)
H12A0.703 (2)0.0165 (14)0.2645 (10)0.032 (3)*
H12B0.447 (2)0.0193 (14)0.2145 (10)0.031 (3)*
C130.54955 (19)0.29174 (12)0.48925 (8)0.0300 (2)
H13A0.659 (2)0.3632 (16)0.5323 (11)0.041 (4)*
H13B0.501 (2)0.2253 (16)0.5344 (11)0.045 (4)*
H13C0.423 (2)0.3379 (15)0.4594 (10)0.036 (3)*
C140.83887 (18)0.15574 (12)0.45485 (8)0.0297 (2)
H14A0.937 (2)0.2281 (14)0.4958 (10)0.032 (3)*
H14B0.913 (2)0.1087 (16)0.4018 (11)0.041 (4)*
H14C0.800 (2)0.0820 (15)0.4964 (11)0.041 (4)*
C150.36571 (16)0.19779 (11)0.13816 (8)0.0261 (2)
H15A0.379 (2)0.2717 (16)0.0963 (11)0.040 (4)*
H15B0.287 (2)0.1110 (15)0.0927 (11)0.038 (4)*
H15C0.273 (2)0.2299 (15)0.1865 (11)0.037 (3)*
C160.71351 (18)0.12824 (13)0.11672 (8)0.0306 (2)
H16A0.863 (3)0.1163 (16)0.1501 (11)0.044 (4)*
H16B0.655 (2)0.0380 (17)0.0737 (12)0.045 (4)*
H16C0.721 (2)0.2032 (16)0.0746 (12)0.044 (4)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Li0.0257 (8)0.0230 (8)0.0214 (8)0.0040 (6)0.0009 (6)0.0053 (6)
C10.0184 (4)0.0206 (4)0.0188 (4)0.0026 (3)0.0036 (3)0.0032 (3)
C20.0182 (4)0.0172 (4)0.0204 (4)0.0018 (3)0.0028 (3)0.0033 (3)
C30.0224 (5)0.0220 (5)0.0239 (5)0.0024 (4)0.0085 (4)0.0075 (4)
C40.0184 (5)0.0254 (5)0.0340 (5)0.0043 (4)0.0090 (4)0.0101 (4)
C50.0171 (4)0.0245 (5)0.0264 (5)0.0031 (4)0.0017 (4)0.0092 (4)
C60.0169 (4)0.0212 (4)0.0187 (4)0.0022 (3)0.0036 (3)0.0056 (3)
C70.0233 (5)0.0260 (5)0.0223 (5)0.0020 (4)0.0017 (4)0.0041 (4)
C80.0235 (5)0.0302 (5)0.0211 (5)0.0025 (4)0.0058 (4)0.0095 (4)
C90.0223 (5)0.0209 (5)0.0228 (5)0.0002 (3)0.0043 (4)0.0032 (4)
C100.0195 (5)0.0246 (5)0.0229 (5)0.0012 (4)0.0017 (4)0.0061 (4)
N10.0200 (4)0.0219 (4)0.0163 (4)0.0000 (3)0.0033 (3)0.0035 (3)
N20.0233 (4)0.0217 (4)0.0163 (4)0.0001 (3)0.0015 (3)0.0039 (3)
C110.0257 (5)0.0238 (5)0.0208 (5)0.0046 (4)0.0046 (4)0.0050 (4)
C120.0301 (5)0.0184 (4)0.0221 (5)0.0012 (4)0.0041 (4)0.0035 (4)
C130.0384 (6)0.0317 (5)0.0207 (5)0.0058 (5)0.0072 (4)0.0029 (4)
C140.0276 (5)0.0362 (6)0.0261 (5)0.0045 (5)0.0004 (4)0.0126 (4)
C150.0224 (5)0.0302 (5)0.0237 (5)0.0012 (4)0.0009 (4)0.0034 (4)
C160.0296 (6)0.0391 (6)0.0247 (5)0.0031 (5)0.0112 (4)0.0018 (4)
Geometric parameters (Å, º) top
Li—N12.1057 (18)C9—H9A1.017 (15)
Li—N22.1078 (18)C9—H9B0.973 (14)
Li—C22.1684 (18)C9—H9C1.018 (13)
Li—C32.2334 (19)C10—H10A0.989 (13)
Li—C102.1971 (19)C10—H10B0.988 (13)
Li—H32.311 (13)N1—C151.4657 (12)
Li—H10B2.334 (13)N1—C161.4673 (13)
C1—C21.5222 (12)N1—C121.4775 (12)
C1—C71.5555 (13)N2—C141.4680 (13)
C1—C61.5705 (13)N2—C131.4698 (13)
C1—H11.024 (13)N2—C111.4732 (12)
C2—C31.3902 (14)C11—C121.5160 (14)
C2—C101.4032 (13)C11—H11B1.015 (14)
C3—C41.5159 (13)C11—H11A1.019 (14)
C3—H30.966 (14)C12—H12A1.029 (14)
C4—C51.5326 (14)C12—H12B1.000 (14)
C4—H4A1.014 (14)C13—H13A1.004 (15)
C4—H4B1.019 (13)C13—H13B1.017 (16)
C5—C71.5508 (14)C13—H13C0.993 (14)
C5—C61.5643 (13)C14—H14A0.961 (14)
C5—H51.014 (13)C14—H14B1.007 (15)
C6—C91.5210 (13)C14—H14C1.013 (15)
C6—C81.5286 (12)C15—H15A0.983 (15)
C7—H7A1.009 (14)C15—H15B1.027 (14)
C7—H7B1.008 (14)C15—H15C0.990 (15)
C8—H8A0.980 (15)C16—H16A0.999 (16)
C8—H8B1.006 (14)C16—H16B1.003 (16)
C8—H8C1.021 (14)C16—H16C0.989 (16)
N1—Li—N288.76 (7)H8A—C8—H8B106.9 (11)
N1—Li—C2127.71 (9)C6—C8—H8C109.4 (8)
N2—Li—C2143.10 (9)H8A—C8—H8C107.7 (11)
N1—Li—C10131.22 (9)H8B—C8—H8C107.6 (11)
N2—Li—C10116.38 (8)C6—C9—H9A110.5 (8)
C2—Li—C1037.49 (4)C6—C9—H9B111.8 (8)
N1—Li—C3130.88 (8)H9A—C9—H9B106.9 (11)
N2—Li—C3125.26 (9)C6—C9—H9C110.5 (7)
C2—Li—C336.78 (4)H9A—C9—H9C108.5 (11)
C10—Li—C368.75 (6)H9B—C9—H9C108.4 (11)
N1—Li—H3144.2 (3)C2—C10—Li70.15 (7)
N2—Li—H3101.0 (4)C2—C10—H10A118.8 (7)
C2—Li—H354.2 (3)Li—C10—H10A136.4 (8)
C10—Li—H374.7 (3)C2—C10—H10B117.1 (8)
C3—Li—H324.5 (3)Li—C10—H10B85.3 (7)
N1—Li—H10B146.3 (3)H10A—C10—H10B118.6 (11)
N2—Li—H10B93.3 (3)C15—N1—C16109.20 (8)
C2—Li—H10B54.1 (3)C15—N1—C12110.40 (8)
C10—Li—H10B24.9 (3)C16—N1—C12109.29 (8)
C3—Li—H10B73.2 (3)C15—N1—Li115.05 (8)
H3—Li—H10B68.1 (5)C16—N1—Li111.74 (8)
C2—C1—C7109.50 (8)C12—N1—Li100.82 (7)
C2—C1—C6109.22 (7)C14—N2—C13109.09 (8)
C7—C1—C687.13 (7)C14—N2—C11110.86 (8)
C2—C1—H1112.5 (7)C13—N2—C11109.16 (8)
C7—C1—H1119.1 (7)C14—N2—Li108.18 (8)
C6—C1—H1116.8 (7)C13—N2—Li117.95 (8)
C3—C2—C10127.17 (9)C11—N2—Li101.34 (7)
C3—C2—C1114.19 (8)N2—C11—C12111.64 (8)
C10—C2—C1118.27 (8)N2—C11—H11B110.5 (8)
C3—C2—Li74.15 (7)C12—C11—H11B109.4 (8)
C10—C2—Li72.36 (7)N2—C11—H11A107.5 (7)
C1—C2—Li123.80 (7)C12—C11—H11A109.3 (8)
C2—C3—C4119.68 (8)H11B—C11—H11A108.3 (11)
C2—C3—Li69.07 (7)N1—C12—C11111.51 (8)
C4—C3—Li134.63 (8)N1—C12—H12A107.2 (7)
C2—C3—H3119.2 (8)C11—C12—H12A110.4 (7)
C4—C3—H3118.7 (8)N1—C12—H12B110.6 (8)
Li—C3—H382.2 (8)C11—C12—H12B108.8 (7)
C3—C4—C5110.65 (8)H12A—C12—H12B108.3 (10)
C3—C4—H4A112.3 (8)N2—C13—H13A109.5 (8)
C5—C4—H4A107.7 (8)N2—C13—H13B111.6 (9)
C3—C4—H4B110.8 (7)H13A—C13—H13B107.0 (12)
C5—C4—H4B108.5 (7)N2—C13—H13C109.7 (8)
H4A—C4—H4B106.7 (10)H13A—C13—H13C110.0 (12)
C4—C5—C7108.05 (8)H13B—C13—H13C109.0 (12)
C4—C5—C6111.37 (8)N2—C14—H14A108.9 (8)
C7—C5—C687.51 (7)N2—C14—H14B110.7 (8)
C4—C5—H5112.9 (7)H14A—C14—H14B108.9 (12)
C7—C5—H5118.0 (7)N2—C14—H14C111.6 (8)
C6—C5—H5116.4 (7)H14A—C14—H14C109.8 (11)
C9—C6—C8108.90 (8)H14B—C14—H14C107.0 (12)
C9—C6—C5118.81 (8)N1—C15—H15A111.1 (9)
C8—C6—C5112.52 (8)N1—C15—H15B112.2 (8)
C9—C6—C1118.35 (7)H15A—C15—H15B107.4 (12)
C8—C6—C1111.55 (8)N1—C15—H15C110.6 (8)
C5—C6—C185.08 (7)H15A—C15—H15C107.2 (12)
C5—C7—C186.05 (7)H15B—C15—H15C108.2 (11)
C5—C7—H7A113.1 (8)N1—C16—H16A111.0 (9)
C1—C7—H7A113.2 (8)N1—C16—H16B111.9 (9)
C5—C7—H7B115.2 (8)H16A—C16—H16B107.9 (12)
C1—C7—H7B117.4 (7)N1—C16—H16C108.2 (9)
H7A—C7—H7B110.2 (11)H16A—C16—H16C108.2 (12)
C6—C8—H8A113.8 (8)H16B—C16—H16C109.6 (12)
C6—C8—H8B111.3 (8)
C7—C1—C2—C339.93 (11)C7—C5—C6—C127.90 (7)
C6—C1—C2—C353.92 (10)C2—C1—C6—C938.36 (11)
C7—C1—C2—C10133.56 (9)C7—C1—C6—C9148.03 (8)
C6—C1—C2—C10132.58 (8)C2—C1—C6—C8165.86 (7)
C7—C1—C2—Li46.66 (11)C7—C1—C6—C884.47 (8)
C6—C1—C2—Li140.52 (8)C2—C1—C6—C581.85 (8)
C10—C2—C3—C4177.25 (9)C7—C1—C6—C527.82 (7)
C1—C2—C3—C49.94 (13)C4—C5—C7—C183.53 (8)
Li—C2—C3—C4130.37 (10)C6—C5—C7—C128.15 (7)
C10—C2—C3—Li52.38 (10)C2—C1—C7—C581.35 (8)
C1—C2—C3—Li120.43 (9)C6—C1—C7—C528.04 (7)
C2—C3—C4—C57.46 (13)C3—C2—C10—Li53.08 (10)
Li—C3—C4—C581.66 (12)C1—C2—C10—Li119.46 (9)
C3—C4—C5—C745.11 (10)C14—N2—C11—C1274.60 (10)
C3—C4—C5—C649.40 (11)C13—N2—C11—C12165.20 (8)
C4—C5—C6—C939.25 (11)Li—N2—C11—C1240.05 (10)
C7—C5—C6—C9147.68 (8)C15—N1—C12—C1180.01 (10)
C4—C5—C6—C8168.16 (8)C16—N1—C12—C11159.87 (8)
C7—C5—C6—C883.41 (9)Li—N1—C12—C1142.06 (10)
C4—C5—C6—C180.53 (8)N2—C11—C12—N160.64 (11)
Comparison of two crystal structures of racemic pinenyllithium.TMEDA top
1985 structure2023 structure
RadiationMo aα 0.71 ÅCu aα 1.54 Å
Temperature (K)295120
Detector typeserialarea
a (Å)6.3964 (11)6.3160 (2)
b (Å)9.8649 (18)9.6925 (2)
c (Å)13.8888 (21)13.7463 (2)
α (°)97.218 (13)97.336 (1)
β (°)99.090 (13)99.662 (2)
γ (°)94.141 (14)93.520 (2)
Volume (Å3)854.71 (25)819.83 (3)
No. reflections452220391
No, obs reflections11543167
Final R0.0470.0387
Li—C10 (Å)2.207 (6)2.1971 (19)
Li—C3 (Å)2.239 (6)2.2334 (19)
C10—C2—C3 (°)127.9 (3)127.17 (9)
oop* H3 (°)-17 (2)-6.4 (5)
oop* H10A (°)-5 (2)- .9 (9)
oop* H10B (°)-13 (2)-20.5 (9)
Note: (*) out of allyl plane, negative sign is away from the Li atom,
 

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