Theoretical Study of the Hydroalumination Reaction of Cyclopropane with Alane
Theoretical Study of the Hydroalumination Reaction of Cyclopropane with Alane
Journal of the Korean Chemical Society. 2013. Apr, 57(2): 216-220
Copyright © 2013, Korea Chemical Society
  • Received : November 05, 2012
  • Accepted : February 19, 2013
  • Published : April 20, 2013
Export by style
Cited by
About the Authors
Satya Prakash, Singh
Pompozhi Protasis, Thankachan

The hydroalumination of cyclopropane has been investigated using the B3LYP density functional method employing several split-valence basis sets. It is shown that the reaction proceeds via an intermediate weakly bound complex and a four-centered transition state. Calculations at higher levels of theory were also performed at the geometries optimized at the B3LYP level, but only slight changes in the barriers were observed. Structural parameters for the transition state are also reported.
Aluminium and boron belong to group III in the periodic table but there is large difference in their chemistry. 1 3 Only a few hydrides of aluminium are known along with monomer AlH 3 and dimer Al 2 H 6 while boron has a richer chemistry 4 5 in the inorganic as well as organic chemistry. Hydrides of aluminium are good reducing agents and used as reducing agent for functional groups, hydroalumination of alkenes, alkynes, allylic rearrangement in organic chemistry. 6
The addition of the Al–H bonds to the double or triple bonds of unsaturated organic compounds (hydroalumination) finds widespread application as a very powerful method for the reduction of specific substrates in organic synthesis. 7 15
The addition of an alkene or alkyne into the Al–H bond of an alkyl aluminium hydride is a key first step in the route to the formation of a new carbon–hydrogen bond via hydroalumination. For further understanding Bunden and Francl 16 used ab initio molecular orbital methods to probe the reaction path for the addition of carbon–carbon multiple bonds into Al–H bonds.
Several theoretical studies of the hydroalumination of ethylene and acetylene have appeared. It has been suggested that the reaction involve the formation of a symmetric π-complex intermediate leading to the formation of addition product via a four-centered transition state. Exploratory work by Egger supports these results. 17 The alternative π-complex transition state proposed by Eisch; 18 however, is inconsistent with both the theoretical studies and the experimental work of Egger and others. In 1981, Grophen and Haaland characterized the transition structure for the addition of acetylene into the Al–H bond of alane. 19 One year later, they have reported the transition structure for the parallel addition reaction of AlH 3 with ethylene. 20 Sakai described a push-pull two-stage mechanism for the similar reaction of AlH 3 with ethylene. 21 Sakai’s charge analysis on hydroalumination of ethylene suggested initial Al- C bond formation occurred which is found rapid than the breaking Al–H and the making of C–H bonds. Higashi et al. Investigated the reverse reaction of AlH 3 +C 2 H 4 in the context of its application to chemical vapor deposition. 22 They have reported a four-centered alane-ethylene transition structure using a more sophisticated theoretical model, although no substantial differences were found.
Houk et al. 23 24 have examined the reaction path for the analogous hydroboration reaction with a variety of substrates. The intermediates, and transition structures found in these studies are consistent with those for the hydroalumination pathway described earlier. Qualitatively, the energetics of these pathways compare well with those from the simple hydroalumination reaction studied earlier. Schleyer and Hommes 26 have examined the structure of the transition state for the reaction of dimethylborane and ethylene using correlated methods and suggest that the TS has a threecentered rather than four-centered structure. Chey et al. 27 have previously characterized the π-complex intermediates for hydroalumination of alkenes. In 1999 Bunden et al. 28 have studied the transition state for the carboalumination of alkene and alkynes at ab initio level of theory. They have shown that these reactions are essentially nucleo philic attacks by alkyl anions on the substrate activated by lewis acid substituents.
Togni and Grutzmacher 29 in 2001 have proposed metalcatalysed hydroalumination reactions of alkenes and alkynes and suggested that the catalytic hydroalumination of alkenes and alkynes is the potential tool for the functionalization of carbon–carbon multiple bonds. Among the different catalytic systems titanium (Ti), Zirconium (Zr) and Nickel (Ni) catalysts have found the widest application. Pankratyev et al. 30 has recently carried out a DFT study on the mechanism of olefin hydroalumination by XAlBu 2 i in the presence of Cp 2 ZrCl 2 catalyst for the mechanism of intermediate formation.
In the present paper, we have reported the results of our investigation of the reaction between cyclopropane and alane at DFT level of theory. Unlike hydroboration of cyclopropane 31 we found a four-centered transition state leading to the formation of n -propyl alane. A four-centered transition state occurs on the approach of AlH 3 moiety along the plane of cyclopropane ring and preceded by an intermediate complex.
- Computational Methods
All calculations have been performed on a PC running WINDOWS using the Gaussian 98 32 suite of programs. The B3LYP hybrid density functional was used for calculation at DFT 33 level using several split-valence basis sets. The geometries of the reactants (AlH 3 and C 3 H 6 ), intermediate complex ( LM1 ), transition state ( TS ) and the product ( LM2 ) were optimized at this level of theory using 6-31G ** , 6-31++G ** , 34 40 cc-pVDZ and aug-cc-pVTZ 41 45 basis sets. The nature of each stationary point was confirmed in each case by frequency calculations; all the minima were verified to have all positive frequencies and the transition state to have only one imaginary frequency. MP2 46 50 calculations were also performed using the chosen basis sets for comparison purposes. Single point (SP) calculations were as well performed at the geometries optimized at the B3LYP/6-31G ** level at the CCSD, CCSD(T), QCISD, QCISD(T) 51 55 and MP4SDQ levels to see if any significant change in the energetics is observed.
The geometries of the reactants (AlH 3 and C 3 H 6 ), the intermediate complex ( LM1 ), the transition state ( TS ) and product ( LM2 ) optimized at the B3LYP/6-31G ** level are shown in . 1 . The optimized geometrical parameters for these species are collected in 1 . Along the reaction path of cyclopropane and alane, three stationary points are located. The first is an intermediate complex ( LM1 ) between the reactants, which is found to be more stable than the reactants by 5.45 kcal mol −1 , the second a transition state ( TS ) and third the product ( LM2 ).
PPT Slide
Lager Image
B3LYP/6-31G** optimized geometries of the reactants (AlH3 and C3H6), complex (LM1), transition state (TS) and product (LM2). Energies are in kcal mol−1.
Optimized structural parameters (bond lengths in Å and angles in degree) for the reactants, complex (LM1, transition state (TS) and product (LM2)
PPT Slide
Lager Image
Optimized structural parameters (bond lengths in Å and angles in degree) for the reactants, complex (LM1, transition state (TS) and product (LM2)
The alane cyclopropane complex is found to be a stable intermediate along hydroalumination pathway. The carbon– carbon (C2–C3) bond length is not significantly affected by binding to the aluminium in the intermediate complex with cyclopropane while the considerable increase in the C2–C3 bond in the transition state has been noted.
The bond-making and bond breaking parameters for the cyclopropane and alane reaction, reactants (C 3 H 6 and AlH 3 ), intermediate complex, transition structure and addition product are collected in 1 . The results are parallel to earlier works on hydroalumination of other substructures. 20 We find the transition structure being best characterized four-centered structure unlike in the case of hydroboration of cyclopropane in which a three-centered transition structure has been reported recently. The formation of the product propylalane ( LM2 ) from the transition state ( TS ) involves H7, originally attached to the boron (B1) shifting closer to the C3 and the boron ( B1 ) moving towards C2, the bond between C2 and C3 lengthening and ultimately breaking. The cleavage of C2–C3 bond can be seen by the examining the molecular orbital picture for the transition structure of cyclopropane with alane. The molecular orbital plot in . 2 shows the cleavage of the C2–C3 π- system in the cyclopropane ring.
PPT Slide
Lager Image
HOMOs of complex (LM1) and transition state (TS) for the hydroalumination of cyclopropane at B3LYP/6-31G** level of calculation.
The energies relative to the sum of the reactants, C 3 H 6 and AlH 3 (in kcal mol −1 ) obtained are summarized in 2 . The aluminium trihydride and cyclopropane reactants are collapsed without the energy barrier to form weakly bound intermediate complex. This intermediate then has surmount a barrier of the order of 45.63 kcal mol −1 via a four-centered transition structure before forming the more stable (about 35.22 kcal mol −1 ) cyclopropane-alane addition product at B3LYP/6-31G ** level of theory and basis set.
Even though the geometry of the intermediate does not change substantially as larger basis sets are used for optimization, the energy of complexation changes considerably a variation of nearly 2 kcal mol −1 variation for the different theoretical models used. The larger basis set augcc- pVTZ gave calculated binding energy of the complex of −4.03 kcal mol −1 with −5.45 kcal mol −1 with the 6-31G ** basis with a B3LYP functional.
The computed barriers (E TS ) are much higher than the available experimental activation energy of about 4.9 kcal mol −1 reported in the case of diethyl aluminium hydride to ethylene. 56 Theoretically, Grophen and Haaland 19 20 reported the barriers of 14.0 and 11.9 kcal mol −1 for the hydroalumination of acetylene and ethylene respectively. The computed values for cyclopropane are higher than these too.
Relative energies (in kcal/mol) at different levels and basis sets
PPT Slide
Lager Image
aSingle point calculations on the B3LYP/6-31G** structures.
Calculated relative energies in kcal mol −1 of the stationary structure along the reaction pathway at DFT and MP2 levels using different basis sets are given in 2 . Single point energies computed at higher levels of theory for structures optimized at the B3LYP/6-31G ** level of theory and basis set are listed in 2 . While there are substantial variations in the barriers, the energies of the product are not very sensitive to the level of calculations.
IRC calculations have been performed and confirm that the transition structure ( TS ) does fall on the path between the complex ( LM1 ) and the product ( LM2 ). The IRC plot is displayed in . 3 shows the transition structure ( TS ) moving downhill towards the complex ( LM1 ) on one side and the product ( LM2 ) the other. Frequency calculations have been performed on all stationary structures. All positive frequencies are found for the stable species (AlH 3 , C 3 H 6 , LM1 and LM2) and one imaginary frequency (798 cm −1 ) is observed in the case of TS.
PPT Slide
Lager Image
IRC plot for the transition state at the B3LYP/6-31G** level.
The qualitative trends found parallel those found in the B3LYP/6-31G ** calculations, attesting to the essential validity of this DFT scheme in such studies. It may also be noted that the MP2 energies of the complex ( LM1 ) are somewhat lower than in the other cases and that the values show less variability with the basis set chosen. These results suggest an energy barrier less than 50.46 kcal mol −1 of energy barrier calculated at the MP2/6-31G ** level of theory and basis set, making the reaction viable; however, no experimental results are available for comparison.
In summary, we have studied the stationary structures involved in the hydroalumination of cyclopropane with alane. Our study posits a four-centered transition state for this reaction in contrast to the recent studies on the hydroboration of cyclopropane, in which three-centered transition state has been reported. It is also hoped that studies on reactions involving cyclopropane and its derivatives with other hydroalumination reagents will clarify the situation.
One of the authors (S.P.S.) is grateful to the Ministry of Human Resources and Development (MHRD), Government of India for the award of a fellowship. And the publication cost of this paper was supported by the Korean Chemical Society.
Aldridge S. , Downs A. J. 2001 Chem. Rev. 101 (11) 3305 - 3366    DOI : 10.1021/cr960151d
Rao B. K. et al. 2001 Phys. Rev. Lett. 86 (4) 692 -    DOI : 10.1103/PhysRevLett.86.692
Gámez J. A. 2008 Chemistry - A European Journal 14 (7) 2201 - 2208    DOI : 10.1002/chem.200701254
Greenwood N. N. 1992 Chem. Soc. Rev. 21 (1) 4957 -
Lipscomb W. N. 1977 Science 196 (4294) 1047 - 1055    DOI : 10.1126/science.196.4294.1047
Carey A. , Sundberg R. J. 2000 Advanced Organic Chemistry: Structure and Mechanisms Springer New York
Zweifel G. , Miller J. A. 1984 Org. React. 32 375 -
Winterfeldt E. 1975 Synthesis 1975 (10) 617 - 630    DOI : 10.1055/s-1975-23856
Marek I. , Normant J. F. 1996 Chem. Rev. 96 (8) 3241 - 3268    DOI : 10.1021/cr9600161
Eisch J. J. 1991 In Comprehensive Organic Synthesis; Brewster, J. H., Ed. Pergamon Press Oxford
Zweifel G. 1978 In Aspects of Mechanism and Organometallic Chemistry; Brewster, J. H., Ed. Plenum Press New York
Zweifel G. 1979 In Comprehensive Organic Chemistry; Barton, D. H. R.; Ollis, W. D., Eds. Pergamon Press Oxford
Negishi E. 1980 Organometallics in Organic Synthesis Wiley New York
Saito S. 2004 In Main Group Metals in Organic Synthesis; Yamamoto, H.; Oshima, K., Eds. Wiley-VCH Weinheim
Miller J. A. 1993 In Chemistry of Aluminum, Gallium, Indium and Thallium; Downs, A. J., Ed. Blackie Academic London
Bundens J. W. , Francl M. M. 1993 Organomet 12 (5) 1608 - 1615    DOI : 10.1021/om00029a019
Egger K. W. 1969 J. Am. Chem. Soc. 91 (11) 2867 - 2871    DOI : 10.1021/ja01039a007
Eisch J. J. 1982 In Comprehensive Organometallic Chemistry; Wilkinson, G.; Stone, F. G. A.; Abel, E. W., Eds., Chapter 6 Pergamon Press Oxford, U.K.
Gropen O. , Haaland A. 1981 Acta. Chem. Scand. Ser. A 35 305 -
Gropen O. , Haaland A. 1982 Acta. Chem. Scand. Ser. A 36 435 -
Sakai S. 1991 J. Phys. Chem. 95 (1) 175 - 178    DOI : 10.1021/j100154a035
Higashi G. S. , Raghavachari K. , Steigerwald M. L. 1990 J. Vac. Sci. Tech. B: Microelectronics and Nanometer Structures 8 (1) 103 - 105    DOI : 10.1116/1.584853
Dahlmann M. , Lautens M. 2001 In Metal-Catalysed Hydroalumination Reactions; Togni, A., Grüzmacher, H., Eds. Wiley-VCH Verlag GmbH
Pankratyev E. Y. 2009 Organomet 28 (4) 968 - 977    DOI : 10.1021/om800393j
Houk K. N. 1984 Tetrahedron 40 (12) 2257 - 2274    DOI : 10.1016/0040-4020(84)80009-5
Wang X. 1990 J. Org. Chem. 55 (9) 2601 - 2609    DOI : 10.1021/jo00296a013
Nagase S. , Ray N. K. , Morokuma K. 1980 J. Am. Chem. Soc. 102 (13) 4536 - 4537    DOI : 10.1021/ja00533a048
Van Eikema Hommes N. J. R. , Schleyer P. V. R. 1991 J. Org. Chem. 56 (12) 4074 - 4076    DOI : 10.1021/jo00012a057
Chey J. 1990 Organomet 9 2430 - 2436    DOI : 10.1021/om00159a009
Bundens J. W. , Yudenfreund J. , Francl M. M. 1999 Organomet 18 (19) 3913 - 3920    DOI : 10.1021/om990350y
Singh S. P. , Thankachan P. P. 2011 J. Mol. Model. 18 (2) 751 - 754
Frisch M. J. 1998 GAUSSIAN98, revision A.7 Gaussian, Inc. Pittsburgh, PA
Becke A. D. 1993 J. Chem. Phys. 98 5648 - 5652    DOI : 10.1063/1.464913
Gordon M. S. 1980 J. Am. Chem. Soc. 102 (25) 7419 - 7422    DOI : 10.1021/ja00545a002
Ditchfield R. , Hehre W. J. , Pople J. A. 1971 J. Chem. Phys. 54 (2) 724 - 728    DOI : 10.1063/1.1674902
Hehre W. J. , Ditchfield R. , Pople J. A. 1972 J. Chem. Phys. 56 (5) 2257 - 2261    DOI : 10.1063/1.1677527
Hariharan P. C. , Pople J. A. 1974 Mol. Phys.: An International Journal at the Interface between Chemistry and Physics 27 (1) 209 - 214
Hariharan P. C. , Pople J. A. 1973 Theoretical Chemistry Accounts: Theory, Computation, and Modeling Theoretica Chimica Acta 28 (3) 213 - 222    DOI : 10.1007/BF00533485
Clark T. 1983 J. Comp. Chem. 4 (3) 294 - 301    DOI : 10.1002/jcc.540040303
Frisch M. J. , Pople J. A. , Binkley J. S. 1984 J. Chem. Phys. 80 (7) 3265 - 3269    DOI : 10.1063/1.447079
Woon D. E. , Dunning J. T. H. 1993 J. Chem. Phys. 98 (2) 1358 - 1371    DOI : 10.1063/1.464303
Kendall R. A. , Dunning J. T. H. , Harrison R. J. 1992 J. Chem. Phys. 96 (9) 6796 - 6806    DOI : 10.1063/1.462569
Dunning J. T. H. 1989 J. Chem. Phys. 90 (2) 1007 - 1023    DOI : 10.1063/1.456153
Peterson K. A. , Woon D. E. , Dunning J. T. H. 1994 J. Chem. Phys. 100 (10) 7410 - 7415    DOI : 10.1063/1.466884
Wilson A. K. , van Mourik T. , Dunning T. H. 1996 J. Mol. Struct.: THEOCHEM 388 339 - 349    DOI : 10.1016/S0166-1280(96)80048-0
Head-Gordon M. , Pople J. A. , Frisch M. J. 1988 Chem. Phys. Lett. 153 (6) 503 - 506    DOI : 10.1016/0009-2614(88)85250-3
Frisch M. J. , Head-Gordon M. , Pople J. A. 1990 Chem. Phys. Lett. 166 (3) 275 - 280    DOI : 10.1016/0009-2614(90)80029-D
Frisch M. J. , Head-Gordon M. , Pople J. A. 1990 Chem. Phys. Lett. 166 (3) 281 - 289    DOI : 10.1016/0009-2614(90)80030-H
Head-Gordon M. , Head-Gordon T. 1994 Chem. Phys. Lett. 220 (1-2) 122 - 128    DOI : 10.1016/0009-2614(94)00116-2
Sæbø S. , Almlöf J. 1989 Chem. Phys. Lett. 154 (1) 83 - 89    DOI : 10.1016/0009-2614(89)87442-1
Cizek J. 1969 Adv. Chem. Phys. 14 35 -
Purvis G. D. , Bartlett R. J. 1982 J. Chem. Phys. 76 (4) 1910 - 1918    DOI : 10.1063/1.443164
Scuseria G. E. , Janssen C. L. , Schaefer H. F. 1988 J. Chem. Phys. 89 (12) 7382 - 7387    DOI : 10.1063/1.455269
Scuseria G. E. , Schaefer H. F. 1989 J. Chem. Phys. 90 (7) 3629 - 3636    DOI : 10.1063/1.455821
Pople J. A. , Gordon M. 1967 J. Am. Chem. Soc. 89 (17) 4253 - 4261    DOI : 10.1021/ja00993a001
Cocks A. T. , Egger K. W. 1972 J. Chem. Soc., Faraday Transactions 1: Physical Chemistry in Condensed Phases 68 423 - 428