Aromaticity of Metallasilapentalynes Advisor Jun Zhu Reporter Xuerui Wang Outline Background Computational Method Results and Discussion Conclusion Background 1982 Thorn D L Hoffman R ID: 463329
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Slide1
Theoretical Study on the Aromaticity of Metallasilapentalynes
Advisor: Jun Zhu Reporter: Xuerui WangSlide2
Outline
Background Computational Method
Results and Discussion
Conclusion Slide3
Background
1982
Thorn ,D , L.; Hoffman, R.
Nouv . J. Chim
.
1979
,
3
, 39
.
1979
2001
G.P. Elliott, W.R. Roper, J. M. Waters,
J. Chem. Soc.
Chem.Commun
,
1982
, 811Tingbin Wen, Guochen Jia, Angew. Chem. Int. Ed, 2001, 40, 1951 Slide4
antiaromaticity
8e
distorted triple bond
extremely strained
116
destabilization
10e
aromaticity
129.5
reduce the ring strain significantly
Introduce a metal into the ring
X-ray molecular structureSlide5
C-C bond lengths 1.377-1.402Ǻ
Planar eight-membered metallabicycle
Benzene 1.396
Ǻ
The aromaticity of osmapentalyne
This feature suggests an aromatic
π
conjugation result from resonance structure
Down-field H chemical shifts
C NMR a lower field than osmabenzynes
silicon atom is reluctant to participate in
bonding
Kutzelnigg, W.
Angew. Chem., Int. Ed.
Engl.
1984, 23, 272.Slide6
Why M
δ--Siδ+
Frederick, P.; Arnold, J.
Organometallics
1999
,
18
, 4800.
σ-donation/weak
π
-back donation
Fischer carbene
,M
→L is limited.
Slide7
show high reactivities toward nucleophiles
Okazaki, M.; Tobita, H.; Ogino, H.
Dalton Trans
.
2003
, 493.Slide8
Computational Method
DFTPackage : Gaussian 03Method: B3LYPbasis sets : 6-311++G **
LanL2DZ:
Ru(ζ(f) = 1.235), Os(ζ(f) = 0.886) ,P(ζ(d) = 0.340), Cl(ζ(d) = 0.514), Si(ζ(d) = 0.262).
1
. Ehlers, A. W.; Böhme, M.; Dapprich, S.; Gobbi, A.; Höllwarth, A.; Jonas, V.; Köhler, K. F.; Stegmann, R.; Veldkamp, A.; G., F.
Chemical Physics Letters,
1993
,
208
, 111.
2. Check, C. E.; Faust, T. O.; Bailey, J. M.; Wright, B. J
. J. Phys. Chem. A 2001
, 105
, 8111.Slide9
Results and Discussion
Stability comparison which silicon in different positions of the ring
(kcal/mol)Slide10
HOMO (-5.67ev)
HOMO-1(-5.90ev)
HOMO-2 (-6.14ev)
HOMO-3 (-6.96ev)
HOMO-12(-9.96ev)
HOMO-8(-8.63ev)
Figure 1.optimized structure of osmasilapentalyne and the occupied
MOs together with their energies Slide11
Figure 2.optimized structure of ruthenasilapentalyne and the occupied
MOs together with their energies
HOMO(-5.82ev)
HOMO-1(-6.01ev)
HOMO-2(-6.24ev
)
HOMO-3(-7.10ev)
HOMO-8(-8.58ev)
HOMO-12(-9.98ev)Slide12
the nucleus-independent chemical shift (NICS) values for each ring by DFT calculations
Ring A;
NICS(0) = - 7.3
NICS(1) = - 9.8
NICS(2) = - 5.9
NICS(-1) = - 10.0
NICS(-2) = - 6.2
NICS(1)zz = - 19.8
Ring B:
NICS(0) = - 8.9
NICS(1) = - 8.8
NICS(2) = - 4.1
NICS(-1) = - 9.1NICS(-2) = - 4.2NICS(1)zz = - 16.2
Ring A;NICS(0) = - 5.0 NICS(1) = - 7.6NICS(2) = - 5.2
NICS(-1) = - 7.7NICS(-2) = -5.3NICS(1)zz = -15.3
Ring B:NICS(0) = - 7.5
NICS(1) = - 7.7NICS(2) = - 3.7NICS(-1) = -7.8NICS(-2) = -3.7
NICS(1)zz = -13.4
Figure 3. the NICS values of the each ring
A
BSlide13
Isomerization stabilization energies (kcal/mol) of metallasilapentalyne compare to metallapentalyne
Figure 4
.
Isomerization stabilization energies (kcal/mol) of metallasilapentalyne compare to metallapentalyne
. Slide14
Figure 5
. the transition of the osmasilapentalyne and (Si)-Cl -osmasilapentaleneSlide15
Conclusion
From the view of π molecular orbitals and negative NICS values compared to benzene both reveal aromaticity in osmasilapentalyne and ruthenasilapentalyne. And the large negative ISEs can also indicate aromaticity.
From the view of
thermodynamics, the Cl atom has the possiblity to migrate,
but from the figure 5 we can see there are high energy barrier to climb, so from the dynamics, the migration may be difficult.Slide16
16
Thank you