Elizabeth N.
Bess‡
a,
David M.
Guptill‡
b,
Huw M. L.
Davies
*b and
Matthew S.
Sigman
*a
aDepartment of Chemistry, University of Utah, 315 South 1400 East, Salt Lake City, UT 84112, USA. E-mail: sigman@chem.utah.edu
bDepartment of Chemistry, Emory University, 1515 Dickey Drive, Atlanta, GA 30322, USA. E-mail: hmdavie@emory.edu
First published on 18th March 2015
Achieving selective C–H functionalization is a significant challenge that requires discrimination between many similar C–H bonds. Yet, reaction systems employing Rh2(DOSP)4 and Rh2(BPCP)4 were recently demonstrated to afford high levels of selectivity in the C–H insertion of carbenes into toluene-derived substrates. Herein, we explore the origin of this selectivity through a systematic analysis of substrate and reagent features that alter levels of selectivity from 20:
1 to 1
:
610 for secondary (or tertiary)-to-primary benzylic C–H functionalization of toluene derivatives. Describing this variation using infrared vibrations and point charges, we have developed a mathematical model from which are identified features of the systems that determine levels of site-selectivity and are applied as predictive factors to describe the selectivity behavior of new substrate/reagent combinations.
An impressive example of site-selective C–H functionalization is the C–H insertion reaction of donor/acceptor rhodium-carbenes.3,4 This process is proposed to proceed through a hydride transfer-like event from the substrate to the carbene, with subsequent C–C bond formation.5 It is generally observed in these systems that more substituted (or activated) C–H bonds are electronically favored and primary C–H bonds are sterically preferred. With the most established catalyst, Rh2(S-DOSP)4, these effects are balanced so as to favor functionalization of secondary C–H bonds (Fig. 1).3 This tendency can be overcome to favor functionalization of primary C–H bonds when using a more sterically demanding catalyst, Rh2(R-BPCP)4 (Fig. 1).6,7 Nevertheless, the effect of the ester substituent7 and functionality on the donor group8 remain relatively unexplored as elements of control over site-selectivity. Understanding the origin of selectivity is thus a major goal in the design and development of new reagents and catalysts.6,7
![]() | ||
Fig. 1 Davies and colleagues' Rh-catalyzed C–H functionalization reaction, demonstrating site-selectivity sensitivity. Preferred C–H bond for functionalization under given conditions is highlighted. |
While there are many diverse means of exploring the molecular features at the origin of selectivity,9 the Sigman group has focused on a method that derives from linear free-energy relationship analysis. In short, mathematical relationships are developed that equate the differential transition state free energy between pathways affording isomeric products (ΔΔG‡) to numeric depictions of molecular features.10,11 Of the various parameters available, computationally measured infrared (IR) bond vibrations have recently emerged as particularly apt descriptors of the molecular characteristics that impact selectivity.10 The intrinsic ability of IR vibrations to accurately represent a molecule's multifaceted, fundamental structure has enabled the mathematical description of complex systems.12 However, the density of information manifested in an IR vibration can also make this descriptor difficult to interpret, clouding the origin of a vibration's importance for mathematically describing trends in selectivity.
Herein, we investigate a method of decoding the controlling elements of rhodium-catalyzed C–H insertion of donor/acceptor carbenes via free-energy mathematical models (Fig. 1).6 Using IR vibrations, we have developed quantitative relationships that describe a substantial range (20:
1 to 1
:
610) in ratios of secondary (or tertiary)-to-primary benzylic C–H functionalization of toluene derivatives. These relationships begin to inform the design of the optimum reagent/catalyst combination for reaction at a specific C–H bond and for the prediction of site-selective outcomes.
To systematically and efficiently assess combinations of these three variables, a face-centered cubic design matrix was implemented to define experimental evaluation of the reaction (Fig. 2b).14 The resulting suite of arene, ester, and substrate combinations was assessed in the Rh2(S-DOSP)4 and Rh2(R-BPCP)4 catalytic systems, affording an array of secondary (or tertiary)-to-primary benzylic C–H functionalization ratios that range from 20:
1 to 1
:
610, respectively (Tables 1 and 2). In the Rh2(S-DOSP)4-catalyzed reactions (Table 1), insertion into a secondary C–H bond preferentially occurs, as previously observed, but there is a considerable difference in the selectivity depending on the nature of the aryl substituent and the ester group. In the Rh2(R-BPCP)4-catalyzed reactions (Table 2), insertion into a primary C–H bond is strongly favored, although a range is also measured.
Entrya | R | R′ | Toluene Substrate | Meas. 3![]() ![]() |
Meas. ΔΔG‡ (kcal mol−1) | Pred. ΔΔG‡ (kcal mol−1) |
---|---|---|---|---|---|---|
a Entries 1–10, training set; entries 11–16, external validation set. | ||||||
1 | t-Bu | Me | 4-Ethyl | 20.0![]() ![]() |
1.92 | 1.90 |
2 | CF3 | Me | 4-Ethyl | 10.0![]() ![]() |
1.48 | 1.64 |
3 | Br | Me | 4-Isopropyl | 1.9![]() ![]() |
0.41 | 0.68 |
4 | Br | CH2CF3 | 4-Ethyl | 11.0![]() ![]() |
1.54 | 1.50 |
5 | t-Bu | CH2CF3 | 4-Isopropyl | 4.5![]() ![]() |
0.97 | 0.34 |
6 | Br | CH2CF3 | 4-Isopropyl | 1.8![]() ![]() |
0.38 | 0.31 |
7 | CF3 | CH2CF3 | 4-Isopropyl | 1.4![]() ![]() |
0.22 | 0.10 |
8 | t-Bu | CH2CCl3 | 4-Ethyl | 9.0![]() ![]() |
1.41 | 1.28 |
9 | CF3 | CH2CCl3 | 4-Ethyl | 4.8![]() ![]() |
1.01 | 1.05 |
10 | Br | CH2CCl3 | 4-Isopropyl | 1.0![]() ![]() |
−0.48 | 0.07 |
11 | Cl | Me | 4-Ethyl | 13.0![]() ![]() |
1.65 | 1.80 |
12 | Br | Et | 4-Ethyl | 12.3![]() ![]() |
1.61 | 1.80 |
13 | Br | CH2CBr3 | 4-Ethyl | 5.8![]() ![]() |
1.13 | 1.15 |
14 | OMe | Me | 4-Isopropyl | 4.7![]() ![]() |
0.99 | 0.73 |
15 | OMe | CH2CCl3 | 4-Isopropyl | 1.3![]() ![]() |
0.17 | −0.03 |
16 | Br | CH2CCl3 | 4-Ethyl | 6.6![]() ![]() |
1.21 | 1.26 |
Entrya | R | R′ | Toluene Substrate | Meas. 3![]() ![]() |
Meas. ΔΔG‡ (kcal mol−1) | Pred. ΔΔG‡ (kcal mol−1) |
---|---|---|---|---|---|---|
a Entries 1–10, training set; entries 11–19, external validation set. | ||||||
1 | t-Bu | Me | 4-Ethyl | 1.0![]() ![]() |
−0.81 | −0.68 |
2 | CF3 | Me | 4-Ethyl | 1.0![]() ![]() |
−1.03 | −0.99 |
3 | Br | Me | 4-Isopropyl | 1.0![]() ![]() |
−2.83 | −2.80 |
4 | Br | CH2CF3 | 4-Ethyl | 1.0![]() ![]() |
−1.01 | −1.15 |
5 | t-Bu | CH2CF3 | 4-Isopropyl | 1.0![]() ![]() |
−2.87 | −3.21 |
6 | Br | CH2CF3 | 4-Isopropyl | 1.0![]() ![]() |
−3.24 | −3.24 |
7 | CF3 | CH2CF3 | 4-Isopropyl | 1.0![]() ![]() |
−3.33 | −3.49 |
8 | t-Bu | CH2CCl3 | 4-Ethyl | 1.0![]() ![]() |
−1.43 | −1.41 |
9 | CF3 | CH2CCl3 | 4-Ethyl | 1.0![]() ![]() |
−1.64 | −1.69 |
10 | Br | CH2CCl3 | 4-Isopropyl | 1.0![]() ![]() |
−3.99 | −3.52 |
11 | Cl | Me | 4-Ethyl | 1.0![]() ![]() |
−0.83 | −0.80 |
12 | Br | Et | 4-Ethyl | 1.0![]() ![]() |
−0.92 | −0.79 |
13 | Br | CH2CBr3 | 4-Ethyl | 1.0![]() ![]() |
−1.64 | −1.57 |
14 | OMe | CH2CCl3 | 4-Isopropyl | 1.0![]() ![]() |
−2.49 | −3.65 |
15 | F | CH2CCl3 | 4-Isopropyl | 1.0![]() ![]() |
−3.78 | −3.76 |
16 | Br | CH2t-Bu | 4-Ethyl | 1.0![]() ![]() |
−1.24 | −1.05 |
17 | Br | CH2CCl3 | 4-Ethyl | 1.0![]() ![]() |
−1.50 | −1.44 |
18 | H | Me | 4-Ethyl | 1.0![]() ![]() |
−0.68 | −0.99 |
19 | Br | Me | 4-Ethyl | 1.0![]() ![]() |
−0.88 | −0.71 |
Reactions performed on 4-isobutyltoluene with Rh2(R-BPCP)4 lead to the detection of only primary C–H insertion products. Changing to Rh2(S-DOSP)4, insertion was favored at the primary site, but tertiary (rather than secondary, benzylic) insertion products were also observed. These results preclude the use of 4-isobutyltoluene in the remainder of these studies.
Due to the ease and fidelity with which computational IR measurements can be made and identical vibrational modes can be identified, IR frequencies and intensities were computed from energy-minimized diazo esters (M06-2X/TZVP, Fig. 3a).15 Although the diazo ester is not the active species that engages in C–H insertion, it likely shares significant structural similarities to the implicated rhodium-carbene. In analogy to the classical application of Hammett σ-parameters, we hypothesized that the rhodium-carbene's relative steric and electronic features would be conserved in its closely related precursor, a diazo ester. Additionally, performing computations on this simple, ground-state organic molecule is a facile exercise that obviates the greater computational load required for transition metal computation, especially when there is only one characterized example for this complex.16
As the goal of this study was not only to develop comprehensive models for prediction purposes but also to better understand the origin of site-selectivity, it was of interest to investigate what the NN diazo IR stretching frequency and intensity may represent in terms of classical physical organic parameters. Therefore, a MATLAB stepwise linear regression algorithm was used to find the optimal combinations of more simple parameters that describe the observed changes in νdiazo and idiazo.17 These parameters include Sterimol measures of substituents' steric effects (B1, minimum radial bulk; B5, maximum radial bulk; L, substituent length—Fig. 3b),18 molecular weight of R′, pKa of the corresponding R′ alcohol (R′–OH), and arene σ and σ+.
The results of these analyses are given in Fig. 4a. The effect of the ester substituent R′ on both νdiazo and idiazo is best related by the Sterimol length (LR′) and R′–OH pKa, which combine to effectively describe the observed trends in both IR measurements, although with different weights of importance. Of specific interest, groups with enhanced length increase the frequency whereas groups that are less able to stabilize negative charge result in decreased νdiazo. The opposite scenario is described by the idiazo model: vibrational intensity is decreased as the length increases but raised when R′ substituents bear higher pKa values. Arene influences on the diazo IR vibration were similarly assessed (Fig. 4b). A positive, nearly one-to-one correlation between νdiazo and σ+ is demonstrated, depicting a solely electronic contribution of para-substituted arenes on this IR frequency (Fig. 4b).19 Alternatively, an inverse correlation exists between idiazo and σ+, which is attenuated by mass at R, as described by Sterimol L.
![]() | ||
Fig. 4 Determination of which factors contribute to diazo IR stretching frequencies and intensities upon independent variation of the (a) ester and (b) arene moieties. |
Also represented in the idiazo term is the electronic influence of the diazo, which originates in both the ester (R′) and aryl (R) substituents. From the model in Fig. 4a, it is demonstrated that more electron-deficient esters (lower pKa) diminish idiazo and, correspondingly, erode the secondary (or tertiary)-to-primary product ratio (Fig. 5). Similarly, in the arene dimension (Fig. 4b), electron-withdrawing R substituents reduce idiazo (e.g., for R = CF3, σ+ = 0.61) and yield product ratios favoring insertion at primary C–H bonds. Taken together, these electronic effects can be explained by considering that electron-deficient groups will destabilize the electrophilic carbene, rendering it more reactive. As a result of its augmented reactivity, it proceeds with C–H insertion via the pathway leading to the kinetic product, i.e., the more easily accessible, albeit stronger, primary C–H bond.
Footnotes |
† Electronic supplementary information (ESI) available: Experimental procedures, tabulated descriptors, and model development MATLAB commands. See DOI: 10.1039/c5sc00357a |
‡ These authors contributed equally. |
This journal is © The Royal Society of Chemistry 2015 |