Organic Letters
Letter
Figure 1. (A) Visible light-driven borylation of heteroarenes in gel media under air conditions. (B) Examples of pharmaceutical agents containing
thiophene, furan, and pyrrole moieties.
furan, pyrrole, and selenophene halides. Thus, application of
this method may be extended beyond borylations to prepare
bioactive molecules (Figure 1A,B).
ditions involved lower reagent loading than reported else-
where15 (10 equiv of B2pin2 and 1.2 equiv of DIPEA), with
irradiation in the visible range at 410−700 nm with cold-white
LEDs in G1 medium for 2 h under aerobic conditions. The
result within the aerobic gel phase was gratifyingly comparable
to that obtained in solution in a strict inert atmosphere (Table
1, entry 2). The model reaction was also carried out under an
oxygen-free atmosphere instead of aerobic conditions (Table 1,
entries 4 versus 3), yielding a similar amount of 2aa. This
outcome reveals that the gel network offers an efficient
confinement effect for visible-light-induced radical reactions in
air.
Based on our previous work,15 we first screened the
photolysis of 2-acetyl-5-chlorothiophene (1a) with bis-
(pinacolato)diboron (B2pin2) and N,N-diisopropylethylamine
(DIPEA, Hunig’s base) in aerated MeCN/H2O (9/1 v/v)
̈
solution. The expected borylated thiophene 2aa was not
observed (Table 1, entry 1), confirming that the reaction was
a
Table 1. Optimization of Reaction Conditions
Varying the amount of each reactant did result in lower
yields of 2aa, although full conversion of 1a was observed in
some cases (Table 1, entries 5−7). The absence of DIPEA or
light in control experiments confirmed the key role of these
elements in the chemical transformation (Table 1, entry 8).
Additionally, employment of other bases did not offer better
This visible-light-driven thiophene borylation thus improved
considerably due to the gel network, which permitted the
process to occur in air. Full conversion of 1a and maximized
2aa yield were obtained with an optimal concentration of G1
(10 mg mL−1); reductions in yield were observed at G1
concentrations below 10 mg mL−1 (Table 1, entry 9). Perhaps
the oxygen diffusion rate through the gel phase is faster,
leading to the process being partially blocked. The diffusion of
reactants might decrease inside the solvent pools above the
optimal G1 concentration, also reducing yield (Table 1, entry
10). Moreover, the effect of light scattering could be
minimized by adjusting the solvent volume (see Table S1,
entries 11, 13, and 14). Thus, the lower the volume the higher
the process efficiency, i.e., 72% yield (1 mL), 64% yield (2
mL), and 53% yield (4 mL).
b
Entry
Deviations for the conditions shown
Yield (%)
0
56 (75)
1
2
3
4
5
6
7
8
without G1
purged N2/without G1
−
c
72 (100)
60 (73)
64 (100)
57 (92)
35 (46)
0 each
purged N2
0.04 mmol of 1a
5 equiv of B2pin2
1 equiv of DIPEA
no DIPEA, or dark reaction
d
9
10
11
G1 (8 mg mL−1
)
43 (70)
37 (59)
56 (86)
d
G1 (15 mg mL−1
)
)
d
G2 (10 mg mL−1
a
b
Optimal conditions. GC-FID yields of 2aa (1a conversion in
To check whether this reaction may be associated
specifically with gelator G1, the model reaction was performed
in the gel of G2 (N,N′-((1S,2S)-cyclohexane-1,2-diyl)-
didodecanamide,19 molecular structure in Table 1), which
assembles with a different matrix. A 56% yield of 2aa was
produced under optimal conditions (Table 1, entry 11);
therefore, G2 also offered a suitable microenvironment for the
investigated reaction. Note that the gelator can be easily
separated by filtration and reused in subsequent experiments
without detriment to its gelation properties (see SI).
The standardized conditions (Table 1, entry 3) were next
applied to a diverse set of heteroarene halides and various
diboron derivatives (Scheme 1). First, upon variation of both
starting materials, thiophene boronate esters (2aa―2fd)
were obtained in moderate-to-high yields (23−89%); these are
important scaffolds in pharmaceuticals20 and conjugated
parentheses) using internal 1-dodecanonitrile. Estimated error from
randomly duplicated experiments independently 3% (see Support-
in organic solvents is driven by hydrogen bonds and van der Waals
forces, leading to tangled fibrillar nanostructures over a wide
concentration range (2−21 g L−1 and 2−44 g L−1 for G1 and G2,
respectively).18,19
c
d
completely blocked by the dissolved molecular oxygen,
presumably shifting the reaction mechanism to other unwanted
pathways (vide infra). Conversely, the desired product 2aa was
formed in high yields when the physical gel formed by G1
(N,N′-bis(octadecyl)-L-boc-glutamic diamide, molecular struc-
ture in Table 1)18 was used as a confined medium under
otherwise identical conditions (Table 1, entry 3; the balance of
conversion was the dehalogenated product). Optimal con-
2321
Org. Lett. 2021, 23, 2320−2325