Cyclization of 5-Hexenyl Radical: Thermodynamics vs. Kinetics Brandon Vittur University of Houston, Department of Chemistry Physical Chemistry II Presented to Dr. Bittner Spring 2007 Abstract Computations involving the cyclization of the 5-hexenyl radical to produce methylcyclopentane (81%), 1-hexene (17%), and cyclohexane (2%) as a result, proved that the reaction is kinetically rather than thermodynamically controlled. Specifically the stereoelectronic requirement of the addition of the radical center to the alkene in the transition state is the underlying factor of the difference in the ratios of the product and the rate of the reaction because the geometry in cyclized 5-hexenyl radical resembling methylcyclopentane meets the stereoelectronic requirements more readily than cyclized 5-hexenyl radical resembling cyclohexane. Introduction Gas phase radical processes received considerable attention for about thirty years after Moses Gomberg published a paper in 1900 titled “An Instance of Trivalent Carbon: Triphenylmethyl.”1 Though free radicals received this attention the possibility that free radical intermediates might be involved in organic reactions was not seriously considered until W. A. Waters, D. H. Hey, and M.S. Kharasch contributed to the development of free radical chemistry.1 Free-radical reactions are now considered useful for synthesizing aliphatic and alicyclic systems.1 In particular Kharasch explored virtually all of the elementary pathways available to free radicals which is shown in scheme 1:1 Scheme 1: A• + B• ↔ A-B (1) A• + B-D ↔ A-B + D• (2) A• + B=D ↔ A-B-D• (3) A• + e ↔ A⎯; A•-e ↔ A+ etc. (4) Most free radical reactions in use today can be rationalized by the four steps in scheme 1 or slight variations of them.1 Since the findings of these mechanistic pathways, only one completely new process has been found: pericyclic reactions of radicals and radical-ions.1 Much of the knowledge acquired about the factors that influence free radical reactions is derived from kinetic studies.1 Highly selective reactions are controlled by the rapid formation of one product over other much slower possible products.1 What affects the kinetic rates and ratios of product formation are the energies of transition complexes.1 In earlier studies it was thought that “radical reactions follow the most exothermic available pathway” and “radical reactions afford the most stable product.”1 This idea is based on the assumption that activation enthalpies reflect reaction enthalpy changes and lead one to conclude that the rates of related reactions can be estimated from the bond dissociation energies of the products formed.1 However, as we now know, thermodynamics is not the only driving force for product formation involving free radicals.1 The other factors include stereoelectronic, polar, steric and kinetic effects.1 The outcome of any particular reaction may involve one or a combination of these factors.1 Cyclization of 5-Hexynyl radical and the final products of this reaction are shown in scheme 2:2 Scheme 2: Bu3SnH AIBN BR Heat * i 17% ii * Rearrangement iii 81% iv 2% vi * v Most chemist will quickly recognize that six-membered rings are more stable than five membered rings (based on combustion data which suggest cyclohexane has a total ring strain of 0 kJ and cyclopentane has a total ring strain of 27 kJ) and 2º radicals are more stable than 1º radicals.3,4 This assumption is based on thermodynamics, however as was mentioned earlier this is not the only factor to consider when thinking about reaction pathways. As scheme 2 shows the overwhelming product formed is not the expected thermodynamic product cyclohexane it is however the less thermodynamically favored product methylcyclopentane. There are two possible explanations for the results of scheme 2: The reaction is thermodynamically controlled and theories on radical stability need to be revised or the reaction is kinetically controlled.2 This paper will attempt to show, based on computational chemistry calculations, that methylcyclopentane is indeed the desired mechanistic pathway for cyclization of 5-Hexynyl radical and give insight as to why this is the case. Experimental The calculations for all structures (figures 1-10 introduced in the results and discussion section) were made in the following order: Geometry optimization, molecular energy of the optimized geometry and finally (figures 5 & 8 only) transition state optimization of the optimized geometry. All calculations were made by a Gaussian program made available by Dr. Bittner and made accessible through the course website at http://minime.chem.uh.edu/pchem07/index.html and energy values were given in units of Hartree. Results The following figures give a three dimensional optimized geometrical representation of the radicals, transition states and the final products involved in the reaction shown in scheme 1 and the computations carried out: Figure 1: 1-hexene (ii) Figure 2: 5-hexenyl radical (i) Figure 6: cyclohexane (chair conformation) (vi) Figure 3: methylcyclopentane (iv) Figure 7: cyclohexyl radical (chair conformation) (v) Figure 4: methylcyclopentyl radical (iii) Figure 8: cyclized 5-hexenyl radical to resemble cyclohexane (chair type conformation) Figure 5: cyclized 5-hexenyl radical to resemble methylcyclopentane Figure 9: cyclized 5-hexenyl radical to resemble methylcyclopentane (bond angle and nuclear distance changed to mimic transition state) The following table summarizes the transition state energies obtained from Gaussian computations on figures 5 and 8: Table 2: Summary of Transition State Energy Structure Energy (kJ/mol) Figure 8 -609817.3982 Figure 5 -609850.2468 The following table gives the difference in energy for the calculations with which the proposed reasons for the results are based for figures 4, 5, 7, 8, 9, and 10: Figure 10: cyclized 5-hexenyl radical to resemble cyclohexane (bond angle and nuclear distance changed to mimic transition state) Table 3: Structural (fig. 4 & 7 and 9 &10) and Transition State (fig. 8 & 5)Energy Differences Structures Energy (kJ/Mol) Figures 4 and 7 24.29151 Figures 8 and 5 32.84799 Figures 9 and 10 218.1663 The following table presents various differences in transition state energies and their corresponding expected ratio of major : minor product formation based on calculations from the Boltzmann distribution: 2 Table 4: Differences In Transition State Energy and Expected Ratio Values of Products ∆E (kJ/mol) The following table summarizes the structural energy calculations obtained from Gaussian computations on figures 1-10: Table 1: Summary of Structural Energy Structure Energy (kJ/mol) Figure 1 -611431.2279 Figure 2 -609775.7153 Figure 3 -611503.3361 Figure 4 -609850.2676 Figure 5 -609850.2647 Figure 6 -611523.7638 Figure 7 -609874.5595 Figure 8 -609874.5591 Figure 9 -609423.3318 Figure 10 -609205.1655 Major : Minor (25˚C) 4 ~90:10 8 ~95:5 12 ~99:1 Discussion From the data in table 1, the original thought, based on thermodynamics about product formation, is justified because figure 6 is lower in energy than figure 3 by roughly 20 kJ/mol (see table 3). Also the 2º radical (figure 7) is more stable than the 1º radical (figure 4) by roughly 24 kJ/mol (see table 3). These results rule out the first possibility that theories on radical stability are incorrect and leave only that the reaction is kinetically controlled. Another expected thermodynamic outcome is that the structural energy, according to table 1, for the transition state structures for figure 8 is more stable than figure 5. All of the previous results mentioned combined suggest that there is something about how the geometry in figure 5 is oriented that affects the transition state in such a way that it forms the major product after the transition. From the data in table 2, the proposed theory that the reaction is kinetically controlled is strengthened significantly because figure 5 is lower in energy than figure 8. The difference in transition state energy of the two products in question is roughly 33 kJ/mol (see table 3). Furthermore based on calculations made by previous theoretical chemists (see table 4), the ratio of the products formed should also not be very surprising. For figure 8 there are two possible conformations: chair and boat. According to Wade4, cyclohexane is most stable in its chair confirmation which is why I chose to use this confirmation instead of the boat. Cyclopentane takes on only one stable conformation and that is the so called slightly puckered “envelope” conformation as shown in figures 3, 4, and 5.4 These conformations are formed in order to reduce eclipsing and lower torsional and angle strain.4 The figures 5 and 8 are both lower in energy than figure 2. This is most likely due to hyper conjugation (stabilization by electron density). It is possible that as the 1˚ radical moves closer to the double bond during cyclization it “feels” the π system in the chain and takes on a more 2˚ radical role and ultimately moves into a transition state for rearrangement. It has also been suggested that the conversion of a double bond to two single bonds provides the driving force for the reaction.3 Now widely accepted is that, the reason this reaction is kinetically controlled is due to stereoelectronic factors which play a dominant role in regiochemistry.1 In order to rationalize the results it is assumed that “…the strain engendered in accommodating the mandatory disposition of reactive centres within the transition structure for 1,6-ring closure outweighs those steric and thermochemical factors expected to favour the formation of the more stable possible product.”1 As noted earlier the total ring strain energy for cyclohexane is 0 kJ and 27 kJ for cyclopentane. In order for the transition state of figure 5 to be favored over figure 8, it must somehow overcome this energy difference to become a reasonable product. In fact in order for the transition to take place the orbital that the radical resides in must line up with the π* orbital of one of the carbon atoms in the double bond (terminal carbon for cyclohexane formation and α-carbon for methylcyclopentane formation).1 For this to happen the radical based carbon atom and one of the carbon atoms in the double bond must have an internuclear bond length of 2.4Å and form a bond angle of 106º (see figure 11).1 Figure 11: Transition state requirements for cyclized product formation at the reactive centers (pictorial reference only) The bond length in figure 8 is 1.562Ǻ with a bond length of 111º, therefore figure 8 must open up, which increases its ring strain, in order to create this required internuclear distance. Figure 8 must also change its conformation in order to achieve the required bond angle (see figure 10). The bond length for figure 5 is 1.551Ǻ with a bond angle of 114˚. Figure 5 must also open up and change its conformation resulting in increased ring strain. Although both molecules have to change their confirmation to match that of the transition state if you look at figures 9 and 10 and compare them with figures 5 and 8 you will notice that figure 8 must undergo more drastic changes than figure 5. Based on the visual geometry changes alone one would conclude that the transition state of figure 5 is significantly lower than figure 8. Based on calculations this is indeed the case and figure 8 is higher in energy by roughly 218 kJ/mol (see table 3). This was also the conclusion of Beckwith1, who found that the energy difference was 11kJ/mol greater for figure 8 than for figure 5. This difference is so great that cyclization of 5-hexynyl radical to figure 5 forms the major product which has an 81% yield compared with figure 8 which forms the minor product with only a 2% yield. An interesting point to make is that table 4 suggests that an energy difference of only 12kJ/mol will give a product ratio of 99:1. The energy difference for the reaction in scheme 2 is roughly 33 kJ/mol and yet cyclohexane makes up 2% of the total yield. This yield seems too high and further research on this reaction concerning this result must be conducted in order to find out why this is indeed the case. Possible reasons why may be factors or a combination of factors mentioned earlier: stereoelectronic, polar and steric effects, different conformations of the molecules or the actual temperature with which the reactions are experimentally carried out. Conclusion The ratio of products shown in scheme 1 give an interesting view into kinetic controlled reactions and help give insight into the actual mechanistic pathways involved in reactions in general. The cyclization of 5-hexynyl radical has become such an important kinetic reaction that it is used as a “Free-Radical Clock” for determining the rates of other reactions.5,6,7 Through free radical reactions chemist have learned that though thermodynamics is a powerful driving force for reactions it is not always the most powerful nor is it the only one worth considering. In addition to the thermodynamics of the system, one needs to consider the possible kinetic, stereoelectronic, polar, and steric effects on the system before making a conclusion about the final products. Notes Scheme 2 was made using ChemDraw Ultra 8.0. All tables were made using Microsoft Excel and the original units were converted to kJ/mol by multiplying the value in Hartree by 627.518 in order to convert to kcal/mol then dividing by 0.239019 in order to convert to kJ/mol. All figures were imported from the Gaussian results summary using Microsoft Paint. References 1 2 3 Beckwith, A. L. J. Chem. Soc. Rev. 1993, 22, 143. Ebgal, T. Quantum Chemistry & Spectroscopy 2006, Pearson Education Inc. Carroll, F.A. Perspectives On Structure and Mechanism In Organic Chemistry 1998 Brooks/Cole Publishing Company 4 5 6 7 8 9 Wade, L.G. Jr. Organic Chemistry 2003, 5th ed. Pearson Education Inc. Newcomb, M. Tetrahedron 1993, 49, 1151. Griller, D.; Ingold, K.U. Acc. Chem. Res. 1980, 13, 317. Lal, D.; Griller, D.; Mendenhall G. D.; Van Hoof W.; Ingold, K.U. 1974 J. Amer. Chem. Soc., in press. Van Der Heide, P. 2007 Chemistry 4272: Physical Chemistry Laboratory II. Garland, C. W.; Nibler, J. W.; Shoemaker, D. P. Experiments In Physical Chemistry 2003, 7th ed. McGraw-Hill Higher Education. Acknowledgements I would like to thank Dr. Bittner for the unlimited use of his Gaussian program, his help and advice throughout my project. Job NumbeJob Name Job DescripProgram Job User 389 C6H11 (5) Molecular Energy bmvittur 752 C6H12 (6) Geometry Optimizationbmvittur 739 C6H11(6) cTransition State Optim bmvittur 522 C6H11 (5) Transition State Optim bmvittur 736 C6H11(5) cMolecular Energy bmvittur bmvittur 936 C6H12 straMolecular Energy 474 C6H11 (6) Transition State Optim bmvittur 740 C6H11 straMolecular Energy bmvittur 778 C6H12 straGeometry Optimizationbmvittur 397 C6H11 (str Geometry Optimizationbmvittur 753 C6H12(5) mGeometry Optimizationbmvittur 756 C6H12(5) mMolecular Energy bmvittur 384 C6H11 (6) Geometry Optimizationbmvittur 755 C6H12(6) cMolecular Energy bmvittur 393 C6H11 (6) Molecular Energy bmvittur 729 C6H11(6) cGeometry Optimizationbmvittur 383 C6H11 Geometry Optimizationbmvittur 737 C6H11(6) cMolecular Energy bmvittur 738 C6H11(5) cTransition State Optim bmvittur 728 C6H11(5) cGeometry Optimizationbmvittur Job Date ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## ######## Route Stoichiome Symmetry #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H12 C1 #N HF/3-2 C6H11(2) C1 #N HF/6-3 C6H11(2) C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H12 C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H12 C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H12 C1 #N HF/3-2 C6H12 C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H12 C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H11(2) C1 #N HF/3-2 C6H11(2) C1 Basis 3-21G 3-21G 3-21G 6-31G(d) 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G 3-21G UHF EnergRotation A Rotation B Rotation C Dipole MomPCharge 1 -232.279500.210497420.101316190.07610869.1575 Deby -0.351311 0.143326020.143324580.08203957.0000 Deby -0.406543 -232.266980.149213000.137663260.08106319.4692 Deby -0.461118 -233.565590.176440810.114272540.09010134.2277 Deby -0.177077 -232.279500.210486970.101305570.07611156.1531 Deby -0.351394 0.436695050.041907060.04107925.3283 Deby -0.460849 -232.266980.149218210.137660230.08106524.4698 Deby -0.461172 -232.251100.448247550.043279580.04253172.1619 Deby -0.461849 0.436694970.041907050.04107924.3297 Deby -0.460798 -232.251120.448247610.043279580.04253173.1610 Deby -0.461804 0.161208340.113839830.09263916.0494 Deby -0.303834 0.161208370.113839830.09263917.0482 Deby -0.304051 -232.288760.150752870.143821610.08277861.1668 Deby -0.45687 0.143326030.143324620.08203957.0000 Deby -0.406531 -232.288750.150752890.143821610.08277861.1657 Deby -0.456909 -232.288760.150750950.143827150.08277886.1658 Deby -0.456851 -232.279500.210497390.101316170.07610868.1576 Deby -0.351304 -232.288750.150750950.143827110.08277884.1647 Deby -0.456891 -232.279490.210587750.101221760.07611284.1111 Deby -0.351788 -232.279500.210486920.101305550.07611155.1531 Deby -0.351384 PCharge 2 -0.379204 -0.406542 -0.159825 -0.328379 -0.37911 -0.202968 -0.159749 -0.383872 -0.203185 -0.383773 -0.388535 -0.388489 -0.155205 -0.40653 -0.155245 -0.15525 -0.379169 -0.15529 -0.378447 -0.379077 PCharge 3 -0.420986 -0.406547 -0.461144 -0.326755 -0.42095 -0.421559 -0.461133 -0.481668 -0.421494 -0.481331 -0.421248 -0.421182 -0.456869 -0.406535 -0.456908 -0.456839 -0.420954 -0.456878 -0.421148 -0.420918 PCharge 4 -0.42115 -0.406548 -0.408352 -0.320928 -0.421151 0.208543 -0.408496 -0.360421 0.208504 -0.36077 -0.421233 -0.421167 -0.400476 -0.406536 -0.400349 -0.400476 -0.421134 -0.400348 -0.421149 -0.421134 PCharge 5 -0.379005 -0.406544 -0.425245 -0.312728 -0.378974 0.20337 -0.425248 0.198327 0.203319 0.198385 -0.388544 -0.388499 -0.412219 -0.406532 -0.412206 -0.412265 -0.379001 -0.412251 -0.378446 -0.378969 PCharge 6 0.206064 -0.406543 -0.408481 0.16466 0.206061 0.21859 -0.408354 0.197559 0.218638 0.197622 0.207889 0.207916 -0.400476 -0.40653 -0.400349 -0.400483 0.206063 -0.400356 0.205643 0.20606 PCharge 7 0.209276 0.206301 0.211603 0.15607 0.209354 -0.389674 0.211556 0.21521 -0.389642 0.215181 0.205467 0.205413 0.207177 0.206286 0.207186 0.207169 0.209275 0.207178 0.210439 0.209353 PCharge 8 0.211082 0.200245 0.209849 0.160045 0.2111 -0.42487 0.209829 0.214651 -0.424853 0.214632 0.21141 0.211376 0.206057 0.200247 0.206021 0.206054 0.211073 0.206018 0.211102 0.211091 PCharge 9 0.211187 0.200244 0.213185 0.164382 0.211192 -0.5829 0.213183 0.205679 -0.582901 0.205648 0.210316 0.210313 0.200283 0.200246 0.200275 0.200288 0.211174 0.20028 0.211242 0.211179 PCharge 10PCharge 1 0.211452 0.211195 0.2063 0.200243 0.213347 0.211548 0.161378 0.165589 0.211413 0.211163 0.199091 0.200088 0.213346 0.211605 0.216592 -0.203173 0.199067 0.200087 0.216531 -0.203466 0.210316 0.211399 0.210313 0.211366 0.208452 0.207177 0.206286 0.200245 0.20842 0.207187 0.208453 0.20717 0.211438 0.211182 0.208421 0.207179 0.211242 0.211103 0.211398 0.21115 PCharge 12 0.21155 0.2063 0.209823 0.166332 0.211469 0.197992 0.209857 -0.421316 0.19798 -0.42074 0.207873 0.207899 0.206057 0.206285 0.206021 0.206066 0.211545 0.206029 0.210439 0.211464 PCharge 13PCharge 14PCharge 15PCharge 16PCharge 17Server CPU time Geometry SRHF Energ 0.205278 0.220356 -0.338578 0.192399 0.200396 matterhorn 14.4 sec 0.200244 0.2063 0.200244 0.2063 0.200246 matterhorn 72.1 sec TRUE -232.91690 0.21475 0.21284 0.199538 0.212934 0.214746 matterhorn 1694.2 sec TRUE 0.168162 0.172194 -0.344604 0.165905 0.165754 matterhorn 5241.2 sec TRUE 0.205259 0.220287 -0.33875 0.192408 0.200622 matterhorn 14.3 sec 0.204883 0.204282 0.202006 0.213 0.213994 matterhorn 5.6 sec -232.88166 0.214743 0.212929 0.199504 0.212842 0.214758 matterhorn 1898.3 sec TRUE 0.209164 0.203744 0.219268 0.217464 0.214642 matterhorn 11.3 sec 0.204887 0.204291 0.201999 0.213075 0.214029 matterhorn 522.7 sec TRUE -232.88166 0.209035 0.203624 0.219206 0.21742 0.214601 matterhorn 621.2 sec TRUE 0.205454 -0.555677 0.196631 0.196639 0.200941 matterhorn 69.7 sec TRUE -232.90912 0.2054 -0.555437 0.196661 0.196669 0.200902 matterhorn 5.7 sec -232.90912 0.213753 0.208483 0.20244 0.208484 0.213752 matterhorn 616.9 sec TRUE 0.200246 0.206286 0.200246 0.206285 0.200248 matterhorn 5.7 sec -232.91690 0.213747 0.20843 0.202502 0.20843 0.213746 matterhorn 14.7 sec 0.213754 0.208487 0.20249 0.208482 0.213751 matterhorn 493.7 sec TRUE 0.205269 0.220384 -0.338726 0.19245 0.200435 matterhorn 669.3 sec TRUE 0.213748 0.208434 0.202553 0.208428 0.213745 matterhorn 14.6 sec 0.205644 0.220154 -0.340708 0.192766 0.201912 matterhorn 597.5 sec TRUE 0.205251 0.220315 -0.338899 0.19246 0.200662 matterhorn 292.4 sec TRUE PCharge 18 0.206301 0.21698 0.216999 0.214736 0.214598 0.206287
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