5772
S. Tumminakatti et al. / Tetrahedron Letters 56 (2015) 5771–5775
employing two strategies. We investigated 4, the thioamide ana-
HL
N
Dag
O
R
R
O
C'lact
O
H
H
logue of 2. This is because the S atom is much larger than O; the
C@S bond is longer than C@O and due to similar electronegativities
of S and C there is greater mesomeric electron delocalization from
N to S in thioamide, than from N to O in amide (Fig. 3b)37–39 and S
is less electronegative than O. Due to these reasons, the thioamide
S in 4 is better placed than the amide O in 2, to donate its electronic
charge to the lactone C0. There is still only a slight upfield shift in
O
N
R
N
H
N
C5
C5
O
O
R
R
Oacyl
H
O
n
<2.5 A
O
Oacyl
O
O
o
o
C'lact
>3.2 A
(a)
(b)
(c)
(d)
Figure 1. (a) General structure of N-acyl homoserine lactones (AHLs).
(b) Oacylꢁ ꢁ ꢁC0lact interaction in AHLs. (c) Possible C5 H-bond in AHLs. (d) C5 H-bond
in 2.05 helical turn in oligo Dag.
13
the C signal of C0lact in 4. The C@Olact stretch band also remains
unchanged, denoting that the negative inductive effect of the acyl
motif is similar in 4 and 2. Second the peptide analogue 5 was
investigated because Ala is known to form intramolecular C7
constraint in the lactone motif, because the HL motif lacks the
a
Thorpe–Ingold effect at C , a unique characteristic of the gem
(
c
-turn) H-bonds (Fig. 3c), that would polarize the acyl C@O, favoring
the imidate tautomer where the acyl O is negatively charged. Here,
-turn H-bond formation is confirmed by the downfield shift of
acyl NH in 5 in the 1H NMR (
d ppm = 0.75) and red shift of its
stretch band in FT-IR (
cmꢀ1 = 9), compared to that in 2
di-substituents in Dag residues.30,31
Natural bond order (NBO) analysis of structures optimized by
density functional theory (DFT) calculations in vacuo at the
B3LYP/6311+G(2d,p) level of theory,32 using second-order pertur-
bation theory as implemented by NBO 5.9,33 have been prevalently
used to determine the energies of intramolecular non-covalent
interactions in molecules.34,35 Our NBO analyses further substanti-
ated the absence of C5 H-bonds in the minimum energy extended
conformations of 2, since the donor-acceptor distances are P3.2 Å
(Fig. 1c).29
c
D
D
m
(Fig. 5). There is again a slight upfield shift of the 13C signal (Fig. 3a)
of C0lact, compared to 3. In 6, where both these effects are opera-
tive29 there is more pronounced 13C upfield shift, further substan-
tiating that the eꢀs of Oacyl are felt by C0lact, but there is no evidence
for n ? p⁄ orbital overlap.
This weak 5-membered Oacylꢁ ꢁ ꢁC0lact interaction occurs in the
forward direction, between an N-terminal carbonyl O charge donor
and a C-terminal carbonyl C0 acceptor. In order to determine the
energy of this interaction, we reasoned that if a 5-membered
C0 Oacyl interaction is simultaneously present in the competing
reverse direction (C-terminal O donor to N-terminal acceptor) in
model compounds, then the forward interaction will perturb it
(Fig. 6b) and the extent of perturbation will represent the
Oacylꢁ ꢁ ꢁC0lact interaction energy.
Second, n ? p⁄ interactions are characterized by the down field
shift in 13C NMR signal (by ꢂ4–5 ppm) of the acceptor carbonyl
due to mixing of its paramagnetic component with the donor
13
orbitals.34 In 2, on the contrary, the C signal of C0lact is upfield
shifted by 1.8 ppm compared to that in 1. This is in agreement with
the shortening of C@Olact, and indicates decreased polarization
along this bond. The increased eꢀ density at C0lact clearly undermi-
nes the presence of an n ? p⁄ orbital overlap type Oacylꢁ ꢁ ꢁC0lact
interaction in 2, unlike suggested earlier (Fig. 4). On the other hand
a van der Waal’s proximity between n eꢀs of Oacyl and C0lact, by
which the electronic shielding at C0lact increases, could explain
the upfield shift of 13C NMR signal.
Reverse C0 Nacyl interactions, where N of imidate is the elec-
tron donor are known to selectively stabilize the cis Boc-Pro con-
formers (Fig. 6a).34 Here the equilibrium constant (Kc/t) value for
the trans to cis conformational isomerism at the Xaa-Pro peptide
bond acts as a direct reporter for the interaction energy. However,
Nacyl cannot donate its lone pair electrons simultaneously along
both of forward and reverse directions. The carbonyl O and S,
can. Thus we first investigated the selective cis Boc-Pro stabiliza-
tion by the reverse interactions in 7, 8 (donor is Oacyl or Sacyl).
The Kc/t value for Boc-Pro in 8 is 1.29 compared to 0.82 in 7.
There is 15 cmꢀ1 red shift in stretching frequency of Boc C@O in
8, compared to 7.29 There is concomitant down field shift
In the absence of spectral evidence for either n ? p⁄ orbital
overlap or C5 H-bond, the shortening of the lactone C@O and the
decrease in polarization towards Olact in 2, could arise from the
negative induction of electrons from the lactone C@O, by the
N-acyl group. In order to investigate the effect of countering this
negative inductive effect, we synthesized 3 where the tBu provides
strong positive induction of eꢀs. There is little change in the 13C
signal of C0lact, but the C@O stretching band red shifts from that
of 2, implying its lengthening due to this eꢀ donation. This is
consistent with the N-acyl group attenuating the lactone C@O
polarization and bond order through inductive effects. Similar
electron withdrawing effects of the N-acyl group are known to
increase polarization of their ring C–H bonds at Pro residues.36
Next in order to understand the nature of the OacylꢁꢁꢁC0lact inter-
actions, we improved the electronic charge of the acyl carbonyl
13
(1 ppm) in the C NMR signals of respective Boc C0 atoms. These
indicate that the C0Boc Sacyl
(
p⁄ n) interaction in the cis
Boc-Pro conformer, involving the larger sulfur atom of thioamide
in 8, is stronger than the C0Boc Oacyl interaction in 7, by
(a)
AHL
No.
(b)
13
b
Lactonea
C=O ν cm
C
ppm
δ
3.44
2.55
2.58
2.55
O
S
-1
-
H
N
C'lact
H
N
H
N
N
H
N
H
1
2
1772
1782
1778
1782
1783
1785
1786
1785
177.6
175.8
175.8
175.3
175.2
174.1
174.9
174.0
HN
R
3.04
3.04
X
O
O
O
O
S
O
(C)
O
O
O
O
O
O
tBu
3
2
3
5
6
R = CH3
R = tBu
X = O
X = S
4
1
4
γ-turn
H-bond
5
O
O
X = O, S
O
O
6
H
N
δ+
H
N
H
H
N
N
C7
N
C7
H
N
H
H
10
11
N
N
N
O
N
X
X
O
X
X
O
O
O
tBu
O
O
O
O
δ-
O
O
O
a = 10 mM, CHCl3, b = 60 mM, CDCl3.
tBu
X = O
X = S
7
X = O 10
11
9
8
X = S
Figure 3. (a) FT-IR stretching frequency and 13C chemical shift for lactone carbonyl
Figure 2.
(7–9).
c
-Butyrolactone (1), AHL analogues (2–6, 10, 11) and model compounds
of AHL. (b) Electronegativity difference between the amide and thioamides. (c) C7
(c-turn) H-bonding in 5 and 6.