K. Gopaul and N. A. Koorbanally
second-order coupling. This second-order coupling was brought
about by the substituents on ring B, wherein lone pairs were
involved in shielding H-10. The data in Table 1 indicate that this
effect is largest when the substituents are in the ortho position
The carbon resonances were in the expected aromatic region of
the spectrum and were assigned with the aid of the HSQC
spectrum. For C-1′, an HMBC correlation to H-10 was used to
confirm its assignment. The carbon resonances on the
acetophenone ring where the substituents occurred were easy to
identify because these carbon resonances had characteristic
chemical shifts; the fluorinated carbon resonances appeared as
doublets at ~δ 163; the chlorinated carbon resonances appeared
at ~δ 139 and the methoxylated carbon resonances appeared at
~δ 160. The fluorinated carbon resonances also had a large
characteristic J value of ~δ 250Hz, which made it easier to identify.
However, if one is not aware of the C―F coupling, these
resonances can be mistaken for impurities.
(
(
5b and 5h). The largest effect is seen with the chlorine atom
5e) (Fig. 3) (with the largest atomic radius) at C-2′, where the
interaction is so pronounced that H-9 and H-10 coalesce into a
1
singlet with the outer peaks being absent in the H NMR
spectrum.
In many instances, the resonances of either H-9 or H-10 are found
to overlap with the aromatic proton resonances, making it difficult
to distinguish. However, the resonances can be identified because
their coupling constants are known and one can identify these
peaks in an overlapping set of resonances. This is illustrated in
Fig. S1 (Supporting Information) where H-9 and H-10 are
completely separate resonances (5j), or when either H-10 (5g) or
H-9 (5k) occur in the multiplet along with the aromatic resonances.
The fluorinated compounds (5b–5d)
The resonances of the proton and carbon atoms of the quinoline
moiety remain unaffected by the fluoro group as it is located away
from the quinoline ring, and thus has no influence on its chemical
shift. However, the proton and carbon atoms on the acetophenone
ring and the ketoethylenic group are affected. The carbon
resonances of the B-ring are split into doublets because of C―F
coupling with J decreasing as the carbon moves further away.
These coupling constants may be used to identify the carbon
resonances of the B-ring as well as distinguish them from the
remaining carbon resonances of the molecule. Once identified,
these carbon resonances can then be used to identify their
corresponding proton resonances using the HSQC spectrum.
For compounds 5b–d (the fluorinated quinoline chalcones), the
C-2′ (ipso) carbon resonates far downfield because of inductive
effects by the fluorine atom. This resonance appears as a doublet
with a large coupling constant, which may be mistaken for two
separate carbon resonances. In 5b, the ortho carbons, C-1′ and
C-3′ resonate upfield at δ 126.8 (J = 13.1 Hz) and 116.7 (J= 22.9 Hz)
whilst the meta carbons, C-4′ and C-6′ resonate downfield at 134.3
(J = 8.8 Hz) and 130.7 (J= 6.2 Hz) respectively (Fig. S2). The
difference between the chemical shifts of these carbon atoms is
because of resonance effects of the fluorine atom. Even the
carbonyl carbon, which is three bonds away from the fluoro group,
is split into a doublet with a coupling constant of 2.3Hz. C-10 and
C-5′ resonate as doublets at δ 131.0 (J = 2.6Hz) and δ 124.6
(J = 3.4Hz) respectively (Fig. S2).
The acetophenone ring
In the absence of substituents on the B-ring, as in 5a, the H-2′/6′
resonance lies downfield in a multiplet with H-4 at δH 8.07–8.12
whilst H-3′/5′ and H-4′ are well resolved and resonate upfield at δH
7.51 and 7.60 respectively. For the para substituted compounds
5g, 5j, 5m and 5o, a pair of doublets for H-2′/6′ and H-3′/5′ are
observed because of ortho coupling as expected, with H-3′/5′
occurring more upfield than H-2′/6′ because of resonance effects
of the substituent. However, the H-3′/5′ resonance for compound
5d appears as a triplet rather than a doublet which is because of
splitting by both the neighbouring hydrogen and fluorine atoms.
When the phenyl ring is substituted at the meta position (5f, 5i,
5l and 5n), expected splitting patterns are observed for H-2′, H-4′
and H-5′. H-2′ resonates downfield as a meta coupled triplet, whilst
H-4′ resonates upfield as a doublet of doublets because of ortho
and meta coupling. H-5′ is split equally by the ortho protons, H-4′
and H-6′ and results in a triplet. For compound 5i, H-6′ resonates
downfield as a doublet of doublets as expected, however, this
splitting pattern is not observed in 5f and 5n. The meta coupling
between H-6′ and H-2′/4′ is not seen and H-6′ resonates as a
doublet. For compound 5l, the doublet of doublets for H-7 and
H-6′ overlap resulting in a multiplet.
For compounds 5e, 5h and 5k, the ortho substituted chalcones,
H-3′ and H-6′ are expected to be split into doublet of doublets with
one large (ortho) and one small (meta) J value and H-4′ and H-5′ into
triplets of doublets. This is the case for 5e but not for 5h and 5k.
Meta coupling for H-3′ and H-5′ is not observed in 5h and 5k. H-3′
resonates as a doublet and H-5′ as a triplet; however, H-4′
undergoes meta coupling and resonates as a triplet of doublets
because it is coupled to two ortho protons and a meta proton.
H-6′ resonates downfield as a doublet of doublets for 5k as
expected, but was unable to be resolved for 5h as it overlaps with
other resonances.
Although some of the resonances coalesce in 5b, it is possible to
identify the ortho coupling between H-4′ and H-3′ (J = 7.2Hz), H-4′
and H-5′ (J = 7.2 Hz), the meta coupling between H-4′ and the
fluorine at C-2′ (J = 5.1Hz) and with the proton H-6′ (J = 1.8 Hz).
The proton of the α,β unsaturated bond, H-10, four bonds away
from fluorine, was also split into a dd at δ
(Fig. S3).
Interesting splitting patterns are observed in the H NMR spectra
H
7.89 (J = 15.8, 2.6 Hz)
1
1
for the fluorinated compounds. For example, in the H NMR spec-
trum of 5b, second order coupling and H-F splitting can be seen
for H-10 and H-F splitting can be seen for H-3′-6′ (Fig. S3). For com-
pound 5b, H-4′ resonates as a dddd initially split by H-3′ and H-5′
with the same J value (7.2Hz) resulting in a triplet (actually a dd),
which is further split into a td (actually a ddd) by F (5.1 Hz) and then
into a dddd by H-6′ (1.8Hz) (Fig. S4). A similar pattern occurs with
H-5′ of compound 5c, which resonates as a ddd, split initially by
H-4′ and H-6′ (J = 8.0Hz) resulting in a triplet (actually a dd), which
is split further into a td (actually a ddd) by the meta fluorine atom
(5.7Hz) (Fig. S4).
Figure 3. The structure of 5e showing the interaction of H-10 with the
2-chloro substituent.
wileyonlinelibrary.com/journal/mrc
Copyright © 2016 John Wiley & Sons, Ltd.
Magn. Reson. Chem. (2016)