Vinyl cation
View on WikipediaThe vinyl cation is a carbocation with the positive charge on an alkene carbon. Its empirical formula of the parent ion is C
2H+
3. Vinyl cation are invoked as reactive intermediates in solvolysis of vinyl halides,[1][2] as well as electrophilic addition to alkynes and allenes.[3]

History
[edit]Vinyl cations have long been poorly-understood[4] and were initially thought to be too high energy to form as reactive intermediates. Vinyl cations were first proposed in 1944 as a reactive intermediate for the acid-catalyzed hydrolysis of alkoxyacetylenes to give alkyl acetate.[5] In the first step of their facile hydration reaction, which was the rate limiting step, a vinyl cation reactive intermediate was proposed; the positive charge was believed to formally lie on a dicoordinate carbon. This is the first time such a transition state can be found in the literature.
In 1959, Grob and Cseh detected vinyl cations during solvolysis reactions of alpha-vinyl halides.[6] Indeed, for this contribution, Grob has been called “the father of the vinyl cation”.[7] The 1960s saw a flurry of vinyl cation-related research, with kinetics data driving the argument for the existence of the species. Noyce and coworkers, for example, reported the formation of a vinyl cation in acid-catalyzed hydration of phenylpropiolic acid.[8] The authors note that in the rate limiting step, a large positive charge develops on the benzylic carbon, indicating that the reaction proceeds through a vinyl cation transition state. Hyperconjugation and hydrogen bonding was evoked to explain the accessibility of the vinyl cation described by Noyce.
Generation
[edit]
Vinyl cations have been observed as reactive intermediates during solvolysis reactions. Consistent with SN1 chemistry, these reactions follow first order kinetics. Generally, vinylic halides are unreactive in solution: silver nitrate does not precipitate silver halides in the presence of vinyl halides,[10] and this fact was historically used to dispute the existence of the vinyl cation species.[4] The introduction of “super” leaving group in the 1970s first allowed for the generation of vinyl cation reactive intermediates with appreciable lifetimes.[11] These excellent leaving groups, such as triflate (trifluoromethanesulfonate) and nonaflate (nonafluorobutanesulfonate), are highly prone to SN1 reactivity. Utilization of these super leaving groups allowed researchers for the first time to move beyond speculation about the existence of such vinyl cations.

Other leaving groups, such as hypervalent iodine moities (which are 1 million fold better leaving groups than the classic triflates[13]), have been utilized to such end as well. Hinkle and coworkers synthesized a number of alkenyl(aryl)iodonium triflates from hypervalent phenyliodo precursors. In the scheme shown, the E- and Z-vinyl triflates form after heterolytic carbon-iodine bond cleavage and subsequent trapping of the cation by triflate. The presence of both E- and Z-vinyl triflate products offers support for the formation of a primary vinyl cation reactive intermediate; through SN2 chemistry, both only one isomer would form.[9]

Vinyl cation reactive intermediates have been generated in photochemical solvolysis reactions. The figure to the right depicts photochemical solvolysis of vinyl iodonium salt, through heterolytic carbon-iodine bond cleavage, to generate a vinyl carbocation and[14] iodobenzene. The reactive intermediate is prone to either nucleophilic attack by the solvent to yield E- and Z-enol ether isomers, or beta hydrogen elimination.
Generation of cyclic vinyl cations
[edit]The ease of generating cyclic vinyl cations depends on the size of the ring system, with vinyl cations residing on smaller rings being more difficult to produce. This trend is supported by calculations showing that the vinyl cation prefers a linear arrangement.[15] Due to the high degree of strain in 3-membered ring systems, the generation of the smallest cyclic vinyl cation, cycloprop-1-enyl cation, remains elusive.[16] The SN1 solvolysis chemistry used to produce other vinyl cations has not proven facile for the cycloprop-1-enyl cation. This is a chemical challenge that remains unsolved.
Structure
[edit]
2H+
3. Adapted from [17]

Two possible structures can be envisioned for C
2H+
3, the simplest vinyl cation: a classical linear or a non-classical bridged structure. Ab initio calculations favor the bridged structure vs the classical by 5.0 kcal/mol.[17] For substituted vinyl cations, however, the linear structure is supported by 13C and 1H NMR measurements.[18] NMR spectroscopy of β-silyl vinyl cations exhibited a single 29Si NMR signal which implies that the two Si are equivalent. The vinyl cation has an intense IR peak at 1987 cm−1 for the C=C+ stretching. The crystallography reveals the bond angles between the vinyl cation carbons and the first carbon of the alkyl substituted to be near 180o.[19]
Stability
[edit]
Initially it was believed that the existence of vinyl cations was questionable because of the large energy difference between it and its vinyl precursor. Once it was established that stable vinyl cation intermediates can be attained through the solvolysis of vinyl compounds with good leaving groups like triflate and nonaflate and stabilized by electron-donating groups, a significant amount of progress as taken place and produced a field of stable vinyl cations.
One of the earliest vinyl cations studied had aryl substituents with an electron-donating moiety. Arylvinyl compounds are stabilized by resonance. Upon the removal of the leaving group, the empty p-orbital is perpendicular to the conjugated system of the phenyl ring, so it can only achieve resonance stabilization in its transition state when the vinyl empty p-orbital is coplanar with the p system of the phenyl ring. Adding steric bulk to the ortho-positions improve conjugation as it makes the phenyl ring orthogonal to the vinyl carbons but coplanar with the empty p-orbital.



Like arylvinyl cations, dienyl and allenyl cations are also stabilized by conjugation. Once again, double bonds in the conjugated system must be coplanar to the empty p-orbital to achieve resonance stabilization. In allenyl cations, the positive charge is well-distributed across the whole structure.

Cyclopropylvinyl cations exhibit a non-classical approach to stabilization. When it is in its bisected structure, there is suitable overlap between its empty p-orbital and the cyclopropyl ring that stabilization is achieved. In its other form, the perpendicular structure, the empty p-orbital is perpendicular to the ring system. The stabilizing power of the cyclopropyl ring is so great that it has become a driving thermodynamic force in rearrangements like 1,2-hydride shifts in (E)- and (Z)-3-cyclopropyl-2-propenyl triflate solvolysis.[20]
Substituent effects on vinyl cation stability
| Substituent | Stabilization# | Electronic effect from α-substituent | ||
| Induction^ | π-donation | Hyperconjugation | ||
| -CH˭CH2 | + | - | +* | |
| -CH3 | + | + | ||
| -Cl | + | - | +* | |
| -Br | + | - | +* | |
| -I | + | - | +* | |
| -F | - | -* | + | |
| -NH2 | + | - | +* | |
| -OH | + | - | +* | |
| -SH | + | - | +* | |
| -C6H5 | + | +* | ||
| -CF3 | - | - | ||
| -CH2F | - | - | ||
| -NO2 | - | - | ||
| -C≡N | + | - | +* | |
| -CH2Y*** | + | - | +* | |
| -Si(CH3)3 | + | + | ||
| -C(O)H | - | +/-** | ||
| -COOH | - | +/-** | ||
| -C(CH3)2OH | + | - | ||
| -C≡CH | + | - | +* | |
Table 1: Electronic effects responsible for stabilization of vinyl cation at the α-position
^ ‘-’ electron-withdrawing, ‘+’ electron-donating
# ‘+’ indicates stabilization and ‘-‘ indicates destabilization of the substituted vinyl cation with respect to neutral alkene equivalent
*indicates the strongest factor responsible for (de)stabilization for substituents that exhibit more than one electronic effect
** the substituent is inductively withdrawing at the carbonyl carbon and also exhibits small electron delocalization from the carbonyl oxygen
*** Y = -F, -Cl, -Br, -I, -OH, -CN, -CF3

The presence of an empty p-orbital perpendicular to the p-bond imparts unwanted destabilization onto the vinyl cation. This inherent instability can be diminished through favorable interactions with a-substituents that reduce the charge at the carbocation. Ab initio computational methods have been used to show stabilizing or destabilizing effects of substituents by monitoring changes in the enthalpies, bond lengths, bond order, and charges in the structures.

There are three possible electronic effects that a substituent may exhibit to influence the stability of the vinyl cation. It may either destabilize the cation by drawing even more electron density from the carbon or stabilizing by contributing more electron density. The carbocation positive charge can be relieved by an unsaturated carbon-based or heteroatomic substituent through p-donation and/or C-H hyperconjugation by methylene/methyl substituents. In addition, inductive effects can either stabilize or destabilizing depending on whether the substituent is electron-donating or –withdrawing. Individual electronic effects are not isolable from the others as all three work together to influence the overall stability of the cation.

For vinyl cations, relative stabilities can be compared with respect to their neutral alkene analogs. To obtain the stabilization properties of a-substituents, the isodesmic reaction was used to calculate enthalpy differences between the substituted vinyl cation and its neutral alkene precursor by getting its reaction enthalpy. This method is advantageous as it can be benchmarked against experimentally-determined thermochemical values. Calculations are initialized from the bridged, nonclassical structure of vinyl cations as it is the global minimum.
In a preliminary work, 4 substituents (-CH=CH2, -F, -Cl, -CH3) were initially studied to investigate electronic effects on vinyl cation stability. The a-substituents induce structural changes in the vinyl cation when compared to its neutral alkene counterpart. These changes can be attributed to the electronic effects present. In vinyl cations, there is a marked decrease in the C-R and C=C bond lengths, indicative of electron donation or induction between Ca and R, and Cb and Ca. On the other hand, the increase in the Cb-H bond length implies a strong hyperconjugative effect that is inversely related to the thermodynamic stability of the cation. Stabilization is possible because of a good overlap between the C-H bond and the empty p-orbital at Ca. Hyperconjugation is evident in all structures because of the adjacent Cb-H bond and in the –CH3 substituent.
Enthalpy calculations obtained from the isodesmic reaction are fair accurate and shows good correlation with experimental data. Stabilization is ranked the order, -F < -Cl < -CH3 < -CH=CH2. All substituents impart stability except for fluorine which destabilized the vinyl cation by 7 kcal/mole. This phenomenon can be explained by comparing a-fluorine substituent effects on vinyl and ethyl cations. In ethyl cations, fluorine stabilizes the carbocation. The stark difference in the stabilizing capabilities of fluorine in the vinyl and ethyl cation is due to the difference in the hybridization of the a-carbons. Because the vinyl cation has a more electronegative sp-hybridized carbon, inductive effects will be more prominent. Having electronegative sp-hybridized carbon interact with fluorine significantly destabilizes the structure. This phenomenon is also apparent in a lesser extent when comparing –CH3 and –CH=CH2 substituents, where -CH=CH2 is less stabilizing.
Heteroatoms like fluorine and chlorine, can exhibit both inductive (electron-withdrawing) and p-donation electronic effects because of their high electronegativities and p-electrons. Stabilization then depends on the balance between the two electronic effects. For fluorine, destabilization via induction is dominant and resonance is significantly weaker. While for chlorine, resonance is sufficient to counteract induction so that overall the effect is stabilizing.
For inductively withdrawing/donating and p-donating substituents, some partial charges reside in the R group and Ca. Although the trend in charge magnitude in R and Ca for the four substituents are inversely related. It is also observed that there is an increase in the bond order of Cb=Ca and Ca-R, which is consistent with the corresponding changes in bond length.
In the small sample size of substituents, there was no observed correlation between bond order increase and charge distribution to R, and the stabilization due to the substituent. However, stabilization has exhibited a correlation to Cb-H bond elongation.
Based on the mechanisms provided above, a wide array of vinyl cation a-substituents can be classified according to the electronic effects they exhibit and the extent of stabilization would depend on the delicate balance between these effects.
Lone pair-containing substituents like –NH2, -OH, and –SH are stabilizing since p-donation overcomes inductively withdrawing effects. Conjugated systems like –CH=CH2 and –C6H5 are stabilizing due to strong p-donation. Highly destabilizing substituents like –CF3 and –NO2 only exhibit inductive electron withdrawal. Weakly destabilizing substituents like –CN has a weak p-donation effect that does not completely curb induction by electron withdrawal.
It is not entirely plausible to isolate the inductive effect of heteroatomic a-substituents because other electronic effects get in the way. However, one way inductive effects of functional groups can be investigated is by probing b-substituent effects where the heteroatom would be a methylene group away from the vinyl cation (-CH2Y). In –CH2Y groups that exhibit a very small or no p donation, there is only a very small difference in the hyperconjugative effect in the –CH2- groups of the substituents. Hence, the overall stability can be correlated to the b-substituent effect, now only driven by its inductive power. Comparing only purely inductively capabilities of functional groups the order is: CN > CF3 > F > Cl > Br > OH, with some destabilization energies comparable to a methyl group.
In most cases, substituents exhibit more than one electronic (de)stabilization effect. Usually, the inductive effect brought upon by multiple bonds to a heteroatom can be counterbalanced by p donation from the same heteroatom. For instance, based on absolute b-inductive power, -CN is more inductive than CF3, but since there can be p donation from the nitrogen of CN, its inductive capability is reduced. In common heteroatomic substituents like F, Cl, Br, and OH, the stabilization decreases with higher electron-withdrawing ability. However, p donation is still believed to take place because of C-R bond decrease.
Carbonyl substituents are mainly destabilizing because of the highly partially positive carbonyl carbon beside the vinyl cation and no p donation.
It is useful to compare substituent effects of vinyl cations and ethyl cations to investigate the hybridization effects of stabilization. In general, vinyl cations are more stabilized by substituents compared ethyl cations primarily because vinyl cations are inherently less stable to begin with. For strongly inductively electron-withdrawing groups like –F, -OH, and –NH2, inductive destabilization is more apparent in vinyl compared to ethyl cations because of the highly electronegative nature of vinyl cation sp hybrids compared to ethyl cation sp2 hybrids. In contrast, in the case of an α-Si(CH3)3 substituent, it is more stabilizing to vinyl cations because it has no p-electrons.
In terms of bond order, stabilizing substituents result in an increase in the C-R, Cα=Cβ, and Cβ-H bond orders. Small increases in bond orders are observed in –CF3, -CH2F, and –CH2X, where they are incapable of p donation, while large increases in bond orders are observed in substituents that can donate p or p electrons like –CH=CH2, -I, or –SH. [21][22]
Vinyl cation intermediates in chemical reactions
[edit]Electrophilic additions
[edit]

A vinyl cation intermediate is possibly formed when electrophilic moieties attack unsaturated carbons. This can be achieved in the reaction of electrophiles with alkynes or allenes. In these reactions, a positive electrophile attacks one of the unsaturated carbons that then forms a vinyl cation, which subsequently undergoes further reaction steps to form the final product.
In the acid-catalyzed hydration of arylacetylene derivatives, a proton initially attacks the triple bond to form a vinyl cation at the aryl substituted carbon. The intermediate experiences little resonance stabilization because of the orthogonality of the conjugated aryl orbital with the empty p-orbital of the vinyl cation. The reaction is first order with respect to both the acetylene and the proton and with the protonation of the acetylene as the rate-determining step. Monosubstituted aryl/alkoxyacetylenes exhibit faster kinetics in acidic hydrations compared to its methyl-substituted equivalents. In arylacetylenes, methyl groups appear to contribute less stabilization compared to hydrogens because of C-H hyperconjugation, reversing the stabilization trend observed in alkyl cations. C-H hyperconjugation is a significant factor because the C-H bond can significantly overlap with the vacant p-orbital. Another possible explanation is that smaller size of the hydrogen substituent allows solvation to take place more easily contributing more significant stabilization.
Aside from protons, other electrophilic groups can attack an acetylene moiety. When attacked by carboxylic acids, cis/trans alkene adducts may be formed. The reaction with hydrogen halides, which also has an initial protonation step, results in the formation of halo-substituted alkenes. Lastly, adamantyl ketones may be formed from an adamantyl cation attack on acetylene and subsequent hydration.[24]

In the hydrohalogenation of phenylpropene, two distinct alkene products are formed because of thermodynamic and kinetic effects. The linear sp-hybridized vinyl cation may be attacked by the halogen from two directions. When attacked from the less sterically hindered side (hydrogen), the E-alkene is produced, attack to the other side forms the Z-alkene. Over short time scales, the E-alkene is favored because the attack from the less bulky side is preferred, but over longer times, the more stable (bulky methyl and phenyl groups on opposite sides) Z-alkene is preferred. Though the E-alkene is initially formed, it isomerizes to the Z-alkene through a carbocation intermediate the stems from protonation and C-C rotation steps.[25]


Neighboring groups surround the alkyne can enhance reaction kinetics by interacting with the intermediate via nonclassical approaches like intramolecular interactions. An alkyne that is adjacent to a tertiary alcohol forms a four-membered cyclic vinyl cation intermediate in which the oxygen of the hydroxyl group bridges two carbons across two bonds. Likewise, a five-membered chloronium ring intermediate is formed from 5-chloro substituted 1-pentynes. An unusually shifted product is formed because the intermediate undergoes heterolysis at the C5-Cl position.[24]

In the electrophilic attack of allenes, it takes place in a manner that prefers to form a terminal adduct and the vinyl cation at the central carbon. The polarization of the allene group show that the terminal carbons have a higher electron density and tendency to under nucleophilic attack. However, if the terminal end is stabilized by a substituent, an allyl-like cation may form as the electrophile attacks the central carbon. Similar to phenyl rings adjacent to vinyl cations, there must be bond rotation to achieve complete resonance stabilization.[24]
Rearrangements
[edit]
Vinyl cations tend to rearrange. These rearrangements can be broadly categorized into two classes: migrations into double bonds and rearrangements via the double bonds. The first category involves 1,2-shifts that lead to the formation of an allyl cation, while the second type involves the formation of another vinyl cation isomer.


Vinyl cations undergo 1,2-hydride shifts to form an allyl-stabilized cation. 1,2-Hydride shifts are fairly common in alkyl cations and is fast in the NMR time scale. However, in vinyl cations, this rearrangement is uncommon even though the rearrangement product in thermodynamically stable. Much like the aryl-substituted vinyl cations, the interacting orbitals during the conversion of a linear vinyl cation to a non-linear allyl cation are orthogonal and passes through a non-planar transition state, which makes the rearrangement difficult. This is evident in the higher activation energies of 1,2-hydride shifts in vinyl cations compared to alkyl cations. Examples of reactions in which this is observed would be the protonation of dialkyl-substituted alkynes and in the solvolysis of ispropylvinyl trifluromethanesulfonate in trifluoroethanol.



1,2-Methyl shifts also occur in vinyl cations, and like 1,2-hydride shifts, they have higher activation barriers compared to their alkyl cation equivalents. In the protonation of alkynes, both 1,2-hydride and 1,2-methyl shifts may take place. The preference depends on the alkyl substituent since it will dictate the resulting allyl cation product. For t-butyl substituents, 1,2-methyl shifts are preferred, and for isopropyl substituents, 1,2-hydride shifts occur instead. Cyclic alkenes also exhibit 1,2-methyl shifts upon solvolysis.

In the solvolysis of spiro-vinyl triflate, the formation of a vinyl cation intermediate through a concerted process drives further rearrangements that involve the formation of a completely distinct cyclic structure. Ring expansion can also be achieved through the rearrangement of a vinyl cation.

The second class of rearrangements, the vinyl cation rearranges to form another vinyl cation isomer. The process is highly dependent on the solvent, nature of the nucleophile, and moieties in the compound. In primary vinyl cations, a 1,2-hydride is unlikely because of the low stability of the primary vinyl cation because of the low electron-donating capability of hydrogen. However, this is still observed in special cases like in 1-methyl-2-phenylvinyl triflate, where the resulting vinyl cation is resonance-stabilized.


Methyl shifts are observed in the addition of tert-butyl cation to but-2-yne. The pentaallyl cation that is formed could be the result of a single 1,3-methyl shift or two consecutive 1,2-methyl shifts. Rearrangement via the double bond could also change the size of a cyclic system. In the solvolysis of methyl-substituted cyclohexenyl triflate, the rearrangement and non-rearranged product are formed in almost equal amounts, with a small preference to the rearrangement product because of its linear structure. However, there is some strain in the methylenecyclopentane rearrangement product.
Lastly, halogens could also move into and stabilize a vinyl cation system. In the reaction of 5-chloropent-1-yne with trifluoroacetic acid, there is simultaneous protonation and 1,4-shift of chlorine that forms a bridged cyclic structure across four carbons. Trifluoroacetic acid subsequently attacks the intermediate from the terminal end to form 2-chloropent-4-enyl trifluoroacetate. This phenomenon is also observed in other halogens. For instance, fluoroalkynes can form a product with two adducts.[18]
Vinyl cations in pericyclic reactions
[edit]
Ketenes and allenes undergo [2+2] cycloadditions under thermal conditions in a concerted manner because they have pi orbitals that are orthogonal to each other. Vinyl cation intermediates undergo the same process in the same manner because it has 2 p orbitals that can simultaneously overlap with the orbitals of the dienophile. In the Smirnov-Zamkow reaction between 2-butyne and Cl2, a cycloaddition leads to the formation of dichlorocyclobutane. A similar reaction is also observed when allene is reacted with HCl. After the cycloaddition, a cationic cyclic intermediate is formed and then it is attacked by a nucleophile to form the final product.[26]
Vinyl cations in hydrohalogenation
[edit]There is debate on whether a vinyl cation intermediate forms with the addition of a halide (H-X) compound to a terminal alkyne for hydrohalogenation reactions. Alternatively, some believe that the addition of H and Br in this case is actually concerted.[citation needed]
References
[edit]- ^ Okuyama, T. (2002). "Solvolysis of Vinyl Iodonium Salts. New Insights into Vinyl Cation Intermediates". Acc. Chem. Res. 35 (1): 12–18. doi:10.1021/ar0100374. PMID 11790084.
- ^ Gronheid, R (2001). "Thermal and Photochemical Solvolysis of (E)- and (Z)-2-Phenyl-1-Propenyl(phenyl)iodonium Tetrafluoroborate: Benzenium and Primary Vinylic Cation Intermediates". J. Am. Chem. Soc. 123 (36): 8760–8765. Bibcode:2001JAChS.123.8760G. doi:10.1021/ja010861n. PMID 11535080.
- ^ Walkinshaw, Andrew J.; Xu, Wenshu; Suero, Marcos G.; Gaunt, Matthew J. (2013). "Copper-Catalyzed Carboarylation of Alkynes via Vinyl Cations". Journal of the American Chemical Society. 135 (34): 12532–12535. Bibcode:2013JAChS.13512532W. doi:10.1021/ja405972h. PMID 23947578.
- ^ a b Stang, P.J. (1979). Vinyl Cations. New York: Academic Press. p. 2.
- ^ Jacobs, Thomas L.; Searles, Scott (1944-05-01). "Acetylenic Ethers. IV.1 Hydration". Journal of the American Chemical Society. 66 (5): 686–689. Bibcode:1944JAChS..66..686J. doi:10.1021/ja01233a007. ISSN 0002-7863.
- ^ Grob, C.A. (1964). "Die Solvoltische Decarboxylierung von α,β-Ungesättigeten β-Halogensäuren Fragmentierungsreaktionen, 9. Miteilung". Helv. Chim. Acta. 47 (6): 1590. doi:10.1002/hlca.19640470621.
- ^ Miyamoto, K. (2009). "Facile Generation of a Strained Cyclic Vinyl Cation by Thermal Solvolysis of Cyclopent-1-Enyl-λ3-Bromanes". Angew. Chem. Int. Ed. 48 (47): 8931–4. doi:10.1002/anie.200903368. PMID 19830754.
- ^ Noyce, D. (1965). "Concerning the Acid-Catalyzed Hydration of Acetylenes". J. Am. Chem. Soc. 87 (10): 2295. Bibcode:1965JAChS..87.2295N. doi:10.1021/ja01088a042.
- ^ a b Hinkle, R.J. (1999). "Primary Vinyl Cations in Solution: Kinetics and Products of a,a-Disubstituted Alkenyl(aryl)iodonium Triflate Fragmentations". J. Am. Chem. Soc. 121 (32): 7437–7438. doi:10.1021/ja9916310.
- ^ Shriner, R.L. (1964). Systematic Identification of Organic Compounds. New York: Wiley.
- ^ Hanack, Michael (1970-07-01). "Vinyl cations in solvolysis reactions". Accounts of Chemical Research. 3 (7): 209–216. doi:10.1021/ar50031a001. ISSN 0001-4842.
- ^ Stang, P.J. (1979). Vinyl Cations. New York: Academic Press. p. 213.
- ^ Okuyama, Tadashi; Takino, Tomoki; Sueda, Takuya; Ochiai, Masahito (1995-03-01). "Solvolysis of Cyclohexenyliodonium Salt, a New Precursor for the Vinyl Cation: Remarkable Nucleofugality of the Phenyliodonio Group and Evidence for Internal Return from an Intimate Ion-Molecule Pair". Journal of the American Chemical Society. 117 (12): 3360–3367. Bibcode:1995JAChS.117.3360O. doi:10.1021/ja00117a006. ISSN 0002-7863.
- ^ a b Tidwell, Thomas T.; P.), Richard, J. P. (John (2003-01-01). Advances in physical organic chemistry. Vol. 37. Academic. ISBN 978-0120335374. OCLC 51840423.
{{cite book}}: CS1 maint: multiple names: authors list (link) - ^ Mayr, Herbert; Schneider, Reinhard; Wilhelm, Dieter; Schleyer, Paul V. R. (1981-12-01). "Vinyl cations. Comparison of gas-phase thermodynamic and solvolysis data with ab initio MO calculations" (PDF). The Journal of Organic Chemistry. 46 (26): 5336–5340. doi:10.1021/jo00339a015. ISSN 0022-3263.
- ^ Grob, C. A.; Csapilla, J.; Cseh, G. (1964-01-01). "Die solvoltische Decarboxylierung von α,β-ungesättigeten β-Halogensäuren Fragmentierungsreaktionen, 9. Miteilung". Helvetica Chimica Acta. 47 (6): 1590–1602. doi:10.1002/hlca.19640470621. ISSN 1522-2675.
- ^ a b c Pople, J.A. (1987). "The structure of the vinyl cation". Chemical Physics Letters. 137 (1): 10–12. Bibcode:1987CPL...137...10P. doi:10.1016/0009-2614(87)80294-4.
- ^ a b c d e f g h i j k l Shchegolev, A A; Kanishchev, M I (1981). "Rearrangements in Vinyl Cations". Russian Chemical Reviews. 50 (6): 553–564. Bibcode:1981RuCRv..50..553S. doi:10.1070/rc1981v050n06abeh002650.
- ^ Müller, Thomas; Juhasz, Mark; Reed, Christopher A. (2004-03-12). "The X-ray Structure of a Vinyl Cation" (PDF). Angewandte Chemie International Edition. 43 (12): 1543–1546. doi:10.1002/anie.200352986. ISSN 1521-3773. PMID 15022228.
- ^ a b c d e Hanack, Michael (1976-10-01). "Stabilized vinyl cations". Accounts of Chemical Research. 9 (10): 364–371. doi:10.1021/ar50106a004. ISSN 0001-4842.
- ^ van Alem, Kaj; Lodder, Gerrit; Zuilhof, Han (2000-03-01). "α-Substituted Vinyl Cations: Stabilities and Electronic Properties". The Journal of Physical Chemistry A. 104 (12): 2780–2787. Bibcode:2000JPCA..104.2780V. doi:10.1021/jp9935743. ISSN 1089-5639.
- ^ van Alem, Kaj; Lodder, Gerrit; Zuilhof, Han (2002-11-01). "Delocalization Does Not Always Stabilize: A Quantum Chemical Analysis of α-Substituent Effects on 54 Alkyl and Vinyl Cations". The Journal of Physical Chemistry A. 106 (44): 10681–10690. Bibcode:2002JPCA..10610681V. doi:10.1021/jp021766j. ISSN 1089-5639.
- ^ a b c Advances in Physical Organic Chemistry. Academic Press. 1971-12-31. p. 185. ISBN 9780080581484.
vinyl cation advances in physical organic chemistry modena.
- ^ a b c Modena, Giorgio (1971). "Vinyl cations". Advances in Physical Organic Chemistry. 9: 185–280.
- ^ a b Organic Chemistry (Second ed.). Oxford, New York: Oxford University Press. 2012-05-04. ISBN 9780199270293.
- ^ a b Fleming, Ian (2010). Molecular Orbitals and Organic Chemical Reactions, Reference Edition - Fleming - Wiley Online Library. doi:10.1002/9780470689493. ISBN 9780470689493.
Vinyl cation
View on GrokipediaDefinition and Structure
Molecular Geometry
The vinyl cation is a carbocation featuring the positive charge delocalized onto an sp-hybridized carbon atom within a vinyl (alkene) framework, with the parent ion denoted as C₂H₃⁺.[1] This sp hybridization at the cationic carbon imparts a linear geometry, characterized by a bond angle of approximately 180° around that center, distinguishing it from the trigonal planar arrangement typical of classical alkyl carbocations. In representative examples, such as β-silyl-substituted derivatives, X-ray crystallography reveals near-linear bond angles of 178.8° at the charged carbon, confirming the sp-hybridized configuration and a short C-C bond length of 1.22 Å.[6] Infrared spectroscopy further supports this geometry, showing a characteristic C=C⁺ stretching frequency at 1987 cm⁻¹ for stabilized vinyl cations, indicative of the strengthened double bond due to the linear arrangement.[6] Theoretical studies on the parent C₂H₃⁺ ion highlight a competition between linear (classical) and bridged (nonclassical) structures, with the bridged form calculated to be slightly more stable by approximately 3-5 kcal/mol at high levels of theory, featuring a C-C bond length of ~1.23 Å and reduced H-C-H angles of ~61°.[7] However, in substituted vinyl cations, particularly those stabilized by electron-donating groups, the linear geometry predominates, as evidenced by experimental structural data. The geometric implications arise from resonance between the classical linear form and the bridged nonclassical three-center bonded form, where the linear structure enhances p-orbital alignment for hyperconjugation and substituent effects in derivatives.[1]| Structure Type | Bond Angle at C⁺ (°) | C-C Bond Length (Å) | Key Evidence |
|---|---|---|---|
| Linear (Classical) | ~180 | ~1.22-1.28 | IR (1987 cm⁻¹), X-ray in derivatives (1.22 Å)[6] |
| Bridged (Nonclassical) | ~180 (C-C-C), ~61 (H-C-H) | ~1.23 | Theoretical calculations for parent ion[7] |
Electronic Structure
The electronic structure of the vinyl cation is characterized by sp hybridization at the cationic α-carbon, which adopts a linear configuration and features an empty p-orbital oriented perpendicular to the π-system formed by the Cα-Cβ bond. This hybridization arises from the trivalent nature of the α-carbon, bonded to the β-carbon and one substituent (or hydrogen in the parent ion), leaving the empty p-orbital available for interactions orthogonal to the molecular plane. A resonance description portrays the positive charge as delocalized between the α- and β-carbons, with the classical form (CH₂=CH⁺) contributing to partial double-bond character along the Cα-Cβ linkage, though the charge density remains predominantly at the α-carbon. This delocalization is evident in population analyses, where the β-carbon bears partial positive charge, influencing bond lengths and reactivity. Ab initio calculations on the parent vinyl cation predict a nonclassical bridged structure to be more stable than the linear classical form by approximately 3.1 kcal/mol, with the bridged isomer representing a minimum on the potential energy surface.[7] In contrast, experimental NMR studies of substituted vinyl cations, including ¹H and ¹³C spectra, support the linear structure, evidenced by deshielding effects consistent with partial positive charge at the β-carbon and sp hybridization at α. Stabilization of the vinyl cation involves the empty p-orbital at the α-carbon engaging in hyperconjugation with adjacent C-H or C-C σ-bonds, as well as potential π-conjugation with β-substituents that align with the orbital's plane, enhancing charge dispersal. This linear arrangement facilitates such orbital overlaps, distinguishing the vinyl cation from alkyl analogs. More recent calculations indicate the energy difference between bridged and linear forms for the parent ion is very small (~0.01 kcal/mol at MP2 level), with the bridged slightly favored, while substituted derivatives favor linear geometry.[8]Historical Development
Early Proposals
The concept of the vinyl cation as a reactive intermediate was first proposed in 1944 by Thomas L. Jacobs and Scott Searles to explain the acid-catalyzed hydration of acetylenic ethers (alkoxyacetylenes). In this mechanism, protonation of the triple bond generates a vinyl cation, which is subsequently attacked by water to yield an enol ether or, with further hydrolysis, an alkyl acetate. This suggestion marked an early recognition of vinyl cations in alkyne chemistry, though it remained speculative without direct evidence.[9] In the early 1950s, vinyl cations were invoked in mechanistic discussions of electrophilic additions to alkynes, such as hydrohalogenations and additions of hydrogen halides or other electrophiles. For instance, proposals suggested that the electrophile adds to the triple bond to form a vinyl cation intermediate, leading to trans addition products, in contrast to alternative pathways involving vinyl radicals or cyclic bridged ions that could account for stereochemical outcomes. These ideas gained traction in explaining regioselectivity and kinetics in reactions like the addition of HCl to acetylene derivatives, but they were debated due to the lack of experimental verification.[10] A key conceptual challenge to accepting vinyl cations was their perceived instability relative to classical alkyl cations. The sp-hybridized carbon in a vinyl cation places the empty p-orbital in an orbital with 50% s-character, increasing its energy and reducing hyperconjugative stabilization compared to the sp³-hybridized alkyl cations, which benefit from lower s-character and greater orbital overlap with adjacent C-H bonds. This theoretical hurdle, highlighted in early discussions, contributed to skepticism until later empirical support emerged.[10]Experimental Confirmation
The existence of vinyl cations was experimentally confirmed in 1964 through solvolysis studies conducted by Grob and Cseh, who observed significant rate enhancements in the solvolysis of α-vinyl halides compared to saturated analogs, along with stereospecific patterns that supported an SN1 mechanism involving a free vinylic carbocation intermediate. These findings provided the first indirect evidence for vinyl cations, as the reactions proceeded faster than expected for direct displacement and yielded products consistent with cationic rearrangement rather than concerted pathways.[11] In the 1960s, further kinetic studies solidified this evidence, particularly through solvolysis of vinyl sulfonates and nonaflates by Peterson and colleagues, which demonstrated anchimeric assistance from neighboring π-systems and the formation of specific rearrangement products, such as allylic isomers, that aligned with vinyl cation formation rates and selectivity. Similar investigations by Rappoport and others highlighted common-ion effects and salt dependencies in these reactions, confirming the intermediacy of vinyl cations via depressed solvolysis rates in the presence of added anions, thus distinguishing ion-pair mechanisms from free ions.[12][13] Direct spectroscopic evidence emerged from NMR studies of stabilized vinyl cation derivatives in superacid media, revealing characteristic deshielded vinylic protons at δ ≈ 5–6 ppm for the β-hydrogens adjacent to the cationic center, with the α-proton appearing further downfield due to the positive charge, confirming the sp-hybridized geometry and electronic delocalization.[14] More recently, persistent vinyl cations have been isolated as carborane salts, such as those with CHB11Cl11− counterions, exhibiting thermal stability up to 150 °C and enabling crystal growth from dichloromethane solutions for X-ray structural analysis, as reported in 2023 investigations of C3H5+ and C4H7+ derivatives.[15]Generation Methods
Solvolytic Generation
Solvolytic generation of vinyl cations primarily involves the heterolytic cleavage of vinyl halides or pseudohalides, such as triflates and nonaflates, in polar protic solvents, leading to the departure of the leaving group and formation of the cationic intermediate.[16] This process, often conducted in solvents like aqueous acetone or ethanol-water mixtures, proceeds via an SN1-like mechanism where the solvent acts as the nucleophile.[17] Triflates serve as particularly effective leaving groups due to their high reactivity, enabling generation at moderate temperatures, whereas halides like chlorides exhibit significantly slower rates, often necessitating elevated temperatures (up to 130°C) or superacidic conditions to achieve viable ionization.[1][17] The kinetics of these solvolyses follow an SN1-like mechanism with rate-limiting ionization of the C–X bond, influenced by common ion effects that suppress the rate through ion-pair return and recapture of the leaving group anion.[17][1] Early rate studies, such as those on β-substituted vinyl systems, confirmed this mechanism by demonstrating salt effects and isotope labeling consistent with carbocation intermediates, though detailed analysis resides in broader experimental confirmations.[17] A representative example is the solvolysis of 1-phenylvinyl triflate, which generates the 1-phenylvinyl cation intermediate, as indicated by product distributions including rearranged acetates and trapped solvent adducts.[18] This reaction highlights the role of aryl substitution in stabilizing the cation, allowing observation of characteristic rearrangements without excessive side reactions.[18]Photochemical and Other Methods
Photochemical methods offer a versatile route for generating vinyl cations under mild conditions, distinct from solvolytic processes by relying on light-induced heterolysis rather than thermal ionization. These approaches typically involve the photoexcitation of vinyl precursors, leading to cleavage of a leaving group and formation of the cation in solution or gas phase. The resulting vinyl cations exhibit high reactivity, often captured by nucleophiles or undergoing elimination, providing insights into their electronic structure and behavior without the need for strong acids.[1] One prominent technique is the photolysis of vinyl iodonium salts, where irradiation cleaves the vinylic C-I bond through a heterolytic S_N1 mechanism, directly affording the vinyl cation. This method is particularly effective for acyclic systems, as demonstrated by the photolysis of (E)-styryl(phenyl)iodonium tetrafluoroborate in methanol, which generates the styryl vinyl cation and yields substitution products with retention of configuration at the vinylic carbon. The process proceeds efficiently at 254 nm, with the phenyl group on iodine facilitating the departure and suppressing competing homolytic pathways. Vinyl diazonium compounds serve as another key precursor class, undergoing photolysis to expel N_2 and form singlet vinyl cations exclusively, enabling clean generation without triplet state interference.[19][20] Pseudohalide precursors, such as vinyl triflates, also respond to irradiation by ionizing to vinyl cations. A representative example is the photolysis of 1-phenylvinyl triflate, which dissociates to the 1-phenylvinyl cation and triflate anion:Cyclic Vinyl Cations
Cyclic vinyl cations present unique synthetic challenges due to the inherent ring strain in small carbocycles, which complicates their generation and stability. Efforts to produce the parent cyclopropenyl cation through solvolysis of suitable precursors, such as cyclopropenyl halides or tosylates, have proven elusive, primarily because the high ring strain in the three-membered unsaturated system—estimated at approximately 50 kcal/mol—renders such precursors unstable and prone to decomposition before ionization can occur.[24][1] Instead, the cyclopropenyl cation is typically accessed via alternative routes like hydride abstraction from cyclopropene derivatives. Larger cyclic vinyl cations, such as the cyclobutenyl cation, have been more successfully generated using adapted solvolytic techniques, including the ionization of 1-cyclobutenyl nonaflates in weakly nucleophilic solvents like trifluoroacetic acid or acetic acid. These reactions proceed with significant rate enhancements attributable to neighboring group participation or direct formation of the vinylic species, yielding products consistent with a stabilized four-membered ring vinyl cation intermediate. Although direct addition of electrophiles to alkynes can lead to cyclobutenyl-like structures in some cases, solvolysis remains the primary method for unambiguous generation in these systems.[1] In cyclopropyl systems, attempts to form direct cyclic vinyl cations often result in rapid rearrangement rather than stable intermediates. For instance, ionization of cyclopropyl-substituted vinyl derivatives typically triggers ring expansion via migration of the cyclopropyl bond to the adjacent cationic center, forming a cyclobutyl cation as shown:Stability and Substituent Effects
Factors Affecting Stability
Vinyl cations exhibit intrinsic instability relative to sp³-hybridized alkyl carbocations owing to the sp-hybridization at the cationic carbon, which imposes a linear geometry and diminishes hyperconjugative stabilization. In alkyl carbocations, the empty p-orbital aligns favorably with adjacent C-H σ-bonds for effective hyperconjugation, whereas in vinyl cations, the perpendicular orientation of the empty p-orbital to the adjacent π-system restricts such overlap, resulting in poorer delocalization of the positive charge. This structural difference renders unsubstituted vinyl cations approximately 20-30 kcal/mol less stable than analogous ethyl or isopropyl carbocations, as determined from solvolysis rate comparisons and computational analyses. Solvent effects significantly influence vinyl cation stability, with polar protic solvents providing notable stabilization through hydrogen bonding directly to the empty p-orbital and surrounding electron-deficient regions. These interactions, combined with ion-dipole solvation, lower the free energy of the cationic species relative to nonpolar or aprotic environments, facilitating their generation and persistence in solvolytic processes. The thermal stability of vinyl cations varies with the counterion and medium, but persistent species, particularly carborane salts, demonstrate remarkable resilience, remaining intact up to 150°C without decomposition or rearrangement. This temperature dependence underscores the role of weakly coordinating anions in minimizing ion-pairing interactions that could otherwise accelerate decay pathways.[27] Kinetic barriers to rearrangement further enhance the effective stability of vinyl cations by impeding rapid conversion to more thermodynamically favored isomers, such as allylic or alkyl species. Despite often exothermic rearrangements, activation energies exceeding 20 kcal/mol—arising from geometric distortions and orbital misalignment—allow these intermediates to maintain lifetimes on the order of microseconds to seconds under appropriate conditions, enabling their detection and utilization in reactions.[3]Substituent Classifications
Substituents attached to the α-carbon of vinyl cations are classified according to their capacity to stabilize or destabilize the positively charged center, with effects arising from resonance donation, hyperconjugation, or inductive withdrawal. These classifications are derived from empirical solvolysis rates and computational analyses at levels such as B3LYP/6-311+G(d,p) and CBS-Q, which quantify relative energies relative to the parent unsubstituted vinyl cation. Stabilizing substituents enhance the cation's lifetime and alter its reactivity, while destabilizing ones increase energy barriers for formation. Aryl substituents, exemplified by phenyl, strongly stabilize vinyl cations through resonance delocalization, where the empty p-orbital on the cationic carbon overlaps with the aromatic π-system; computational studies report a stabilization of approximately 15 kcal/mol for the phenyl-substituted case compared to alkyl analogs. Alkyl groups like methyl provide modest stabilization via hyperconjugation, involving donation from adjacent C-H σ-bonds to the vacant p-orbital, with an estimated contribution of +3 kcal/mol based on molecular orbital calculations. Similarly, the vinyl group (-CH=CH₂) offers stabilization through extended hyperconjugation and weak resonance, while amino groups (-NH₂) donate electrons via π-conjugation, further lowering the cation's energy. In contrast, electron-withdrawing substituents destabilize vinyl cations predominantly through inductive effects that deplete electron density from the electron-deficient center. Fluorine, despite its lone-pair donation potential, induces a net destabilization of -7 kcal/mol due to its strong electronegativity pulling electrons away via the high s-character α-C-F bond. The trifluoromethyl group (-CF₃) exacerbates this with a destabilization of about -10 kcal/mol, as the electronegative fluorines amplify inductive withdrawal without effective resonance compensation. Nitro groups (-NO₂) are highly destabilizing via both inductive and resonance electron withdrawal, rendering such cations extremely short-lived. Alkoxy groups (-OR) present an interesting case, where inductive withdrawal overrides any resonance donation from oxygen lone pairs, leading to overall destabilization. The following table summarizes representative substituent effects on vinyl cation stability, drawn from quantum chemical analyses:| Substituent | Relative Energy Effect (kcal/mol) | Primary Mechanism |
|---|---|---|
| -Ph | +15 | Resonance delocalization |
| -CH₃ | +3 | Hyperconjugation |
| -CH=CH₂ | + (ca. 5–8) | Hyperconjugation and resonance |
| -NH₂ | + (ca. 10–12) | π-electron donation |
| -OR | - (ca. 2–5) | Inductive withdrawal |
| -F | -7 | Inductive withdrawal |
| -CF₃ | -10 | Strong inductive withdrawal |
| -NO₂ | - (ca. 15–20) | Inductive and resonance withdrawal |