Home Ab initio study of mechanism of forming a spiro-Si-heterocyclic compound involving Ge from (CH3)2Ge=Si: and formaldehyde
Article Open Access

Ab initio study of mechanism of forming a spiro-Si-heterocyclic compound involving Ge from (CH3)2Ge=Si: and formaldehyde

  • Jingjing Ming , Junfeng Han and Xiuhui Lu EMAIL logo
Published/Copyright: June 24, 2014

Abstract

(CH3)2Ge=Si: and its derivatives (X2Ge=Si:, X=H, F, Cl, Br, Ph, Ar) are a new species. Their cycloaddition reaction is a new area for the study of silylene chemistry. The mechanism of the cycloaddition reaction between singlet (CH3)2Ge=Si: and formaldehyde was investigated with the CCSD(T)//MP2/6-31G* method. From the potential energy profile, it can be predicted that the reaction has one dominant pathway. The reaction rule presented is that the two reactants first form a four-membered Ge-heterocyclic silylene through the [2+2] cycloaddition reaction. Because of the 3p unoccupied orbital of Si: atom in the four-membered Ge-heterocyclic silylene and the π orbital of formaldehyde forming a π→p donor-acceptor bond, the four-membered Ge-heterocyclic silylene further combines with formaldehyde to form an intermediate product. The Si: atom in the intermediate product is sp3 hybridized after transition state, and this intermediate isomerizes to a spiro-Si-heterocyclic compound involving Ge via a transition state.

Introduction

Unsaturated silylenes are important active intermediates. Their cycloaddition reaction is considered to provide a convenient, short pathway for the synthesis of tensility cyclotella, silapolycyclic compounds, and to synthesize the compounds which are difficult to obtain by using general methods. The reaction is also regarded as an effective method in the synthesis of new bonds and heterocyclic compounds including derivatives of silicon. The silylene H2C=Si: is the simplest unsaturated species that was first observed experimentally by Leclercq and Dubois in 1979 [1]. Srinivas et al. [2] have used neutralization-reionization mass spectrometry to show that H2C=Si: is a viable molecule in the low-pressure gas phase. Theoretical studies indicate that the ground state of H2C=Si: is the singlet state.

The energy of H2C=Si: is by 84.0 kcal/mol lower than that of silaacetylide, and H2C=Si: is the lowest energy isomer [3]. We have performed preliminary studies on the cycloaddition reaction of unsaturated silylenes [4, 5], but these studies are limited to the cycloaddition reaction of H2C=Si: and its derivatives (X2C=Si:, X=Me, F, Cl, Br, Ph, Ar). There has been no published reports on the cycloaddition reaction of H2Ge=Si: and its derivatives (X2Ge=Si:, X=Me, F, Cl, Br, Ph, Ar) until now. It is fairly difficult to investigate mechanisms of the cycloaddition reaction directly by experimental methods due to the high activity of unsaturated silylenes; therefore, a theoretical study is more feasible. To explore the rules of cycloaddition reaction between H2Ge=Si: (including its derivatives) and the asymmetric π-bonded compounds, (CH3)2Ge=Si: and formaldehyde were selected as model molecules. The mechanism was investigated and analyzed theoretically. The results show that there are five possible pathways of the cycloaddition reaction (considering the hydrogen and methyl transfer simultaneously) as explained in Figure 1. The research results indicate the laws of cycloaddition reaction between X2Ge=Si: (X=H, Me, F, Cl, Br, Ph, Ar) and the asymmetric π-bonded compounds.

Figure 1 The reaction pathways 1–5. The major pathway 5 is explained in more detail by reaction 5′, where R1 is (CH3)2Ge=Si:, R2 is formaldehyde, INT4 denotes intermediate product 4, INT5 is intermediate product 5, TS5 is transition state 5, and P5 is product 5 (see also the text and Figures 2–9 for similar abbreviations).
Figure 1

The reaction pathways 1–5. The major pathway 5 is explained in more detail by reaction 5′, where R1 is (CH3)2Ge=Si:, R2 is formaldehyde, INT4 denotes intermediate product 4, INT5 is intermediate product 5, TS5 is transition state 5, and P5 is product 5 (see also the text and Figures 29 for similar abbreviations).

Calculation methods

MP2/6-31G* [6] implemented in the Gaussian 98 package [7] was employed to locate all the stationary points along the reaction pathways. Full optimization and vibrational analysis were done for the stationary points on the reaction profile. Zero point energy, CCSD(T) single point energy corrections [CCSD(T)//MP2/6-31G*] and basis set superposition error (BSSE) corrections were included in the energy calculations. To explicitly establish the relevant species, the intrinsic reaction coordinate (IRC) [8, 9] was also calculated for all transition states appearing on the cycloaddition energy surface profile.

Results and discussion

Reaction 1: the pathway to a three- membered ring product P1

Theoretical calculations show that the ground state of (CH3)2Ge=Si: is a singlet state. The geometrical parameters of the intermediate INT1, transition state TS1, and product P1 which appear in reaction 1 between (CH3)2Ge=Si: and formaldehyde are given in Figure 2. The energies are listed in Table 1, and the potential energy surface for the cycloaddition reaction is shown in Figure 3. According to Figure 3, reaction 1 consists of two steps: (i) the two reactants R1, R2 are transformed into an active intermediate INT1 in a barrier-free exothermic reaction of 28.7 kJ/mol; and (ii) intermediate INT1 isomerizes to a three-membered ring product P1 through transition state TS1 with an energy barrier of 56.0 kJ/mol.

Figure 2 Optimized MP2/6-31G* geometrical parameters and the atomic numbering for the species in cycloaddition reaction 1. Bond lengths (Å) and angles (°) are shown.
Figure 2

Optimized MP2/6-31G* geometrical parameters and the atomic numbering for the species in cycloaddition reaction 1. Bond lengths (Å) and angles (°) are shown.

Figure 3 The potential energy surface for the cycloaddition reactions between (CH3)2Ge=Si: and formaldehyde calculated by using CCSD (T)//MP2/6-31G*.
Figure 3

The potential energy surface for the cycloaddition reactions between (CH3)2Ge=Si: and formaldehyde calculated by using CCSD (T)//MP2/6-31G*.

Table 1

Zero point energy (ZPE, a.u.), total energies (ET, a.u.), and relative energies (ER, kJ/mol) for the species from various theoretical methods.

ReactionSpeciesZPEMP2/6-31G*CCSD(T)//MP2/6-31G*
ETaERETaER
(1)bR1+R20.10354-2555.804050.0-2555.900070.0
INT10.10645-2555.81912-39.6-2555.91102-28.7
TS1(INT1-P1)0.10524-2555.7949224.0-2555.8896827.3
P10.10770-2555.84203-99.7-2555.93076-80.6
(2)bR1+R20.10354-2555.804050.0-2555.900070.0
INT20.10690-2555.81707-34.2-2555.90872-22.7
TS2(INT2-P2)0.10648-2555.81618-31.8-2555.90782-20.3
P20.10888-2555.86910-170.8-2555.95753-150.9
TS2.1(P2-P2.1)0.10602-2555.81912-39.6-2555.90857-22.3
P2.10.10751-2555.84119-97.5-2555.92709-70.9
TS2.2(P2-P2.2)0.10364-2555.81235-21.8-2555.898763.4
P2.20.10461-2555.83412-78.9-2555.92295-60.1
(3)cP2+R20.13617-2670.042560.0-2670.153250.0
INT30.13920-2670.04685-11.3-2670.15557-6.1
TS3(INT3-P3)0.13898-2670.0157470.4-2670.1278866.6
P30.14116-2670.08715-117.1-2670.18803-91.3
(4)bR1+R20.10354-2555.804050.0-2555.900070.0
INT40.10692-2555.84005-94.5-2555.92842-74.4
TS40.10733-2555.83773-88.4-2555.92632-68.9
P40.10829-2555.85305-128.6-2555.93824-100.2
TS4.1(INT4-P4.1)0.10295-2555.83242-74.5-2555.92063-53.3
P4.10.10455-2555.84631-111.0-2555.93619-94.8
TS4.2(INT4-P4.2)0.10686-2555.82296-49.6-2555.90828-21.6
P4.20.10820-2555.83978-93.8-2555.92728-71.4
(5)dINT4+R20.13421-2670.011890.0-2670.122650.0
INT50.13856-2670.01339-3.9-2670.12346-2.1
TS5(INT5-P5)0.13799-2670.0074111.8-2670.1162816.7
P50.14033-2670.06875-149.3-2670.16958-123.2

aET=E(Species)+ZPE+BSSE, bER=ET-E(R1+R2), cER=ET-E(P2+R2), dER=ET-E(INT4+R2).

Reaction 2: the pathways to a four-membered Ge-heterocyclic silylene P2, CH3-transfer product P2.1 and H-transfer product P2.2

The geometrical parameters of transition states TS2, TS2.1, TS2.2 and products P2, P2.1, P2.2 which appear in reaction 2 between (CH3)2Ge=Si: and formaldehyde are given in Figure 4. The energies are listed in Table 1, and the potential energy surface for the cycloaddition reaction is shown in Figure 3. According to Figure 3, reaction 2 consists of four steps. In the first step, the two reactants R1, R2 form an intermediate INT2 in a barrier-free exothermic reaction of 22.7 kJ/mol. In the second step, the intermediate INT2 isomerizes to a four-membered Ge-heterocyclic ring silylene P2 via a transition state TS2 with an energy barrier of 2.4 kJ/mol. In the next two steps, product P2 undergoes a transfer of a CH3 group and a H atom via transition states TS2.1 and TS2.2 with energy barriers of 128.6 and 154.3 kJ/mol, respectively, resulting in the formation of products P2.1 and P2.2. Because the energies of P2.1 and P2.2 are by 80.0 and 90.8 kJ/mol higher than that of P2, thus the transfer reactions of P2→P2.1 and P2→P2.2 are thermodynamically prohibited at normal temperature and pressure, and reaction 2 ends with product P2. Comparing reaction 2 with reaction 1, the energy barrier of TS2 is by 53.6 kJ/mol lower than that of TS1, therefore reaction 2 is the dominant reaction pathway.

Figure 4 Optimized MP2/6-31G* geometrical parameters of TS2, TS2.1, TS2.2, P2, P2.1, P2.2 and the atomic numbering for cycloaddition reaction 2. Bond lengths (Å) and angles (°) are shown.
Figure 4

Optimized MP2/6-31G* geometrical parameters of TS2, TS2.1, TS2.2, P2, P2.1, P2.2 and the atomic numbering for cycloaddition reaction 2. Bond lengths (Å) and angles (°) are shown.

Reaction 3: the pathway to a Ge-spiro-Si-heterocyclic ring compound P3

In reaction 3, the four-membered Ge-heterocyclic ring silylene P2 further reacts with formaldehyde (R2) to form a spiro-Si-heterocyclic compound involving Ge (P3). The geometrical parameters of the intermediate product INT3, transition state TS3, and product P3 which appear in reaction 3 are given in Figure 5. The energies are listed in Table 1, and the potential energy surface for the cycloaddition reaction is shown in Figure 3. According to Figure 3, reaction 3 involves the generation of a four-membered Ge-heterocyclic silylene P2 from the reactants R1, R2, which is followed by the reaction of P2 with formaldehyde to form an intermediate INT3 in a barrier-free exothermic reaction of 6.1 kJ/mol. Then intermediate INT3 isomerizes to a Ge-spiro-Si-heterocyclic compound P3 via a transition state TS3 with an energy barrier of 72.7 kJ/mol.

Figure 5 Optimized MP2/6-31G* geometrical parameters of INT3, TS3, P3 and the atomic numbering for cycloaddition reaction 3. Bond lengths (Å) and angles (°) are shown.
Figure 5

Optimized MP2/6-31G* geometrical parameters of INT3, TS3, P3 and the atomic numbering for cycloaddition reaction 3. Bond lengths (Å) and angles (°) are shown.

Reaction 4: the pathways to a four- membered Ge-heterocyclic silylene INT4, its isomer P4, a H-transfer product P4.1, and a CH3-transfer product P4.2

The geometrical parameters of the four-membered Ge-heterocyclic silylene INT4, transition states TS4, TS4.1, TS4.2 and products P4, P4.1, P4.2 which appear in reaction 4 between (CH3)2Ge=Si: and formaldehyde are given in Figure 6. The energies are listed in Table 1, and the potential energy surface for the cycloaddition reaction is shown in Figure 3. According to Figure 3, reaction 4 consists of four steps: (i) the two reactants R1, R2 form a four-membered Ge-heterocyclic ring silylene INT4 in a barrier-free exothermic reaction of 74.4 kJ/mol; (ii) INT4 isomerizes to a distorted four-membered ring product P4 via the transition state TS4 with an energy barrier of 5.5 kJ/mol; (iii) INT4 undergoes hydrogen transfer via the transition state TS4.1 with an energy barrier of 21.1 kJ/mol, resulting in the formation of product P4.1; (iv) INT4 undergoes a transfer of a CH3 group via the transition state TS4.2 with an energy barrier of 52.8 kJ/mol, resulting in the formation of product P4.2. Because the energy of P4.2 is by 3.0 kJ/mol higher than that of INT4, the transformation INT4→P4.2 is thermodynamically prohibited at normal temperature and pressure. The energy barrier of TS4 is by 15.6 kJ/mol lower than that of TS4.1, therefore, INT4→P4 is the dominant reaction pathway of reaction 4.

Figure 6 Optimized MP2/6-31G* geometrical parameters of INT4, TS4, TS4.1, TS4.2, P4, P4.1, P4.2 and the atomic numbering for the species in cycloaddition reaction 4. Bond lengths (Å) and angles (°) are shown.
Figure 6

Optimized MP2/6-31G* geometrical parameters of INT4, TS4, TS4.1, TS4.2, P4, P4.1, P4.2 and the atomic numbering for the species in cycloaddition reaction 4. Bond lengths (Å) and angles (°) are shown.

According to Figures 3, 4, and 6 and thermodynamics formulas PT(i)=e-ΔGT(i)/RTie-ΔGT(i)/RT and ΔGT(i)=-RTlnKi, it can be suggested that INT2 and INT4 are isomeric, R1+R2→INT2 and R1+R2→INT4 are two parallel reactions, and the equilibrium distributions of INT2 and INT4 are PT(INT2)= K(INT2)/K(INT2)+K(INT4)≈0.0, PT(INT4)=K(INT4)/K(INT2)+K(INT4)≈1.0, respectively. Accordingly, INT4 is the main intermediate product.

Reaction 5: the pathway to a Ge-spiro-Si-heterocyclic compound P5

In reaction 5, the four-membered Ge-heterocyclic silylene INT4 further reacts with formaldehyde (R2) to form a Ge-spiro-Si-heterocyclic compound P5. The geometrical parameters of intermediate INT5, transition state TS5, and product P5 which appear in reaction 5 are given in Figure 7. The energies are listed in Table 1, and the potential energy surface for the cycloaddition reaction is shown in Figure 3. According to Figure 3, reaction 5 involves the formation of a four-membered Ge-heterocyclic silylene INT4 from the two reactants R1, R2, followed by a barrier-free exothermic reaction of 2.1 kJ/mol with formaldehyde (R2) to form an intermediate INT5. Then the intermediate INT5 isomerizes to a Ge-spiro-Si-heterocyclic compound P5 via a transition state TS5 with an energy barrier of 18.8 kJ/mol. In a comparison of reaction 5 with reaction 4, it can be concluded that the two reactions compete mutually due to scrambling for INT4. The intermediate product INT4 can react with R2, which can reduce the system energy of 2.1 kJ/mol. In reaction 4, the energy barrier of INT4→P4 is 5.5 kJ/mol, therefore reaction 5 will be the dominant reaction pathway.

Figure 7 Optimized MP2/6-31G* geometrical parameters of INT5, TS5, P5 and the atomic numbering for cycloaddition reaction 5. Bond lengths (Å) and angles (°) are shown.
Figure 7

Optimized MP2/6-31G* geometrical parameters of INT5, TS5, P5 and the atomic numbering for cycloaddition reaction 5. Bond lengths (Å) and angles (°) are shown.

Theoretical analysis and explanation of the dominant reaction pathway

According to the analysis above, reaction 5, additionally explained in Figure 1 by reaction 5′, should be the dominant reaction channel of the cycloaddition reaction between singlet (CH3)2Ge=Si: (R1) and formaldehyde (R2). The frontier molecular orbitals for R2 and INT4 of this reaction are shown in Figure 8. These frontier molecular orbitals can be expressed by a schematic diagram shown in Figure 9. The mechanism of this reaction can be explained by analysis of Figures 2, 6, 7, and 9. According to Figures 2 and 6, the molecule of (CH3)2Ge=Si: initially interacts with formaldehyde by the [2+2] cycloaddition of the bonding π-orbitals resulting in the formation of a four-membered Ge-heterocyclic silylene INT4. Because INT4 is an active intermediate, it can further react with formaldehyde (R2) to form a spiro-Si-heterocyclic compound P5 that contains Ge. The mechanism of this reaction can be explained with Figures 7 and 9. When INT4 interacts with formaldehyde (R2), the 3p unoccupied orbital of the Si atom in INT4 will insert the π-orbital of formaldehyde from the oxygen side. Then the shift of π-electrons to the p-unoccupied orbital gives a π→p donor-acceptor bond, leading to the formation of intermediate INT5. As the reaction progresses, the angle for O(2)SiGe (INT5: 108.1°, TS5: 123.8°, P5: 219.8°) increases gradually, the angle for C(4)O(2)Si (INT5: 135.3°, TS5: 113.2°, P5: 69.5°) decreases gradually, and the length of the C(4)-O(2) bond (INT5: 1.374 Å, TS5: 1.395 Å, P5: 1.505 Å) elongates gradually. Finally, the Si atom in INT5 undergoes hybridization to the sp3 hybrid orbital after the transition state TS5, forming the more stable spiro-Si-heterocyclic compound (P5) containing Ge.

Figure 8 The frontier molecular orbitals of formaldehyde R2 and the intermediate product INT4.
Figure 8

The frontier molecular orbitals of formaldehyde R2 and the intermediate product INT4.

Figure 9 A schematic interaction diagram for the frontier orbitals of INT4 and H2C=O (R2).
Figure 9

A schematic interaction diagram for the frontier orbitals of INT4 and H2C=O (R2).

Conclusion

On the basis of the potential energy profile of the cycloaddition reaction between singlet (CH3)2Ge=Si: and formaldehyde obtained with the CCSD(T)//MP2/6-31G* method, it is predicted that the dominant reaction pathway of the cycloaddition reaction is reaction 5. It consists of three steps. In the first step, a four-membered Ge-heterocyclic silylene INT4 in a barrier-free exothermic reaction of 74.4 kJ/mol is generated. In the second step, the intermediate product INT4 further reacts with formaldehyde (R2) by a barrier-free exothermic reaction of 2.1 kJ/mol to form another intermediate INT5. In the third step, the intermediate product INT5 isomerizes to a spiro-Si-heterocyclic compound P5 via a transition state TS5 with an energy barrier of 18.8 kJ/mol.


Corresponding author: Xiuhui Lu, School of Chemistry and Chemical Engineering, University of Jinan, Jiweilu 106, Jinan, Shandong 250022, P. R. China, e-mail:

References

[1] Leclercq, H.; Dubois, I. The absorption spectrum of the H2CSi radical. J. Mol. Spectrosc.1979, 76, 39–54.Search in Google Scholar

[2] Srinivas, R.; Sulzle, D.; Schwarz, H. Experimental evidence for the existence of SiCH, (x = 1–3) molecules in the gas phase. J. Am. Chem. Soc.1991, 113, 52–58.Search in Google Scholar

[3] Warren, W. H.; Kevin, W. W.; Dennis, J. C. Jet spectroscopy, structure, anomalous fluorescence, and molecular quantum beats of silylidene (H2C=Si), the simplest unsaturated silylene. J. Chem. Phys.1997, 107, 8829–8839.Search in Google Scholar

[4] Lu, X. H.; Yu, H. B.; Wu, W. R. A theoretical study on the mechanism of the cycloaddition reaction between dichloroalkylidene silylene and ethylene. New J. Chem.2005, 29, 332–335.Search in Google Scholar

[5] Lu, X. H.; Yu, H. B.; Xu, Y. H.; Xiang, P. P.; Che, X. Theoretical study of the mechanism of cycloaddition reaction between dichloromethylene silylene and formaldehyde. Mol. Phys.2007, 105, 1961–1969.Search in Google Scholar

[6] Curtis, L. A.; Raghavachari, K.; Pople, J. A. Gaussian-2 theory using reduced Møller-Plesset orders. J. Chem. Phys.1993, 98, 1293–1298.Search in Google Scholar

[7] Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.; Cheeseman, J. R.; Zakrzewski, V. G.; Montgomery, J. A.; Stratmann, R. E.; Burant, J. C.; et al. (1998) GAUSSIAN 98, Revision A.9. Gaussian Inc., Pittsburgh, PA.Search in Google Scholar

[8] Fukui, K. A formulation of the reaction coordinate. J. Phys. Chem.1970, 74, 4161–4163.Search in Google Scholar

[9] Ishida, K.; Morokuma, K.; Komornicki, A. The intrinsic reaction coordinate. An ab initio calculation for HNC to HCN and H-+CH4 to CH4+H-. J. Chem. Phys.1981, 66, 2153–2156.Search in Google Scholar

Received: 2014-4-20
Accepted: 2014-5-26
Published Online: 2014-6-24
Published in Print: 2014-8-1

©2014 by De Gruyter

This article is distributed under the terms of the Creative Commons Attribution Non-Commercial License, which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.

Downloaded on 23.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/hc-2014-0066/html
Scroll to top button