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total free energy, such as nonionic hydrophobic ef-
fects driven by entropy, and specific interactions, in-
cluding H-bonds, van der Waals interactions, and p
stacking, and 2) the pure electrostatic (polyelectro-
lyte) contribution, DGoel, which reflects the ionic inter-
actions occurring between two groups of opposite
charge and is highly dependent on the salt concen-
tration. As expected, and in line with the Kd values,
we found that the interactions between all of the S–
amino acid conjugates and TAR RNA mainly involve
specific nonelectrostatic interactions because the
DGonel component represents 81–96% of the overall
free energy (DG8; Table 3), whereas the neomycin–
TAR interaction is clearly dominated by the electro-
static component (DGonel =33% and DGeol =67%). In-
terestingly, we also observed that an increase in am-
monium groups has no significant effect on the DGnoel
Table 2. Competition assays in the presence of tRNA and dsDNA.[a]
Entry
Ligand
Kd (TAR)
[mm]
K’d (TAR) with
tRNA[b] [mm]
K’d/Kd
K’’d (TAR) with
dsDNA[c] [mm]
K’’d/Kd
1
2
3
4
5
6
7
neomycin
1b
2b
17.2
7.5
78.5
10.4
26.2
18.10
0.69
0.35
45.5
4.6
1.4
10.7
1.1
2.9
3.2
25
n.b.
11.5
–
1.5
7.4
1.2
3.0
3.6
6.5
2.44
17.5
0.24
0.11
1.82
18.20
20.5
0.72
0.40
11.89
3b
13b
14b
15b
[a] Fluorescence measurements were performed in buffer A (20 mm HEPES, pH 7.4,
20 mm NaCl, 140 mm KCl, and 3 mm MgCl2). Kd values are given with an uncertainty
of Æ10%. [b] Measured in the presence of a 100-fold excess of a mixture of natural
tRNAs (tRNA mix). [c] Measured in the presence of a 100-fold excess of a 15-mer DNA.
n.b.: no binding.
the specificity of its analogue, 3b, bearing one amino acid (K’d/
Kd =1.1 and K’’d/Kd =1.2; Table 2, entry 4).
component because ligands 13b–15b, which contain twice as
many ammonium groups as 1b–6b, have very similar contri-
butions from the DGonel values to those obtained for 1b–6b
(1b/13b, 2b/14b,and 3b/15b; Table 3). This original mode of
binding could be ascribed to: 1) the high specific H-bonding
contribution of the S system and 2) the optimal position of the
amino acid, which allows additional specific interactions.[10b,15]
These results also showed that the overall free energy (DG8) is
driven by the enthalpy of the binding (DH8) and by the high
contribution of its nonelectrostatic component (DGonel; Table 3).
Finally, CD spectra were recorded in the absence and pres-
ence of ligands to show whether the involved interactions
affect the RNA structure. A typical example is shown for 13b,
which was selected for its high affinity (Figure 2). The CD spec-
trum of the TAR hairpin alone shows strong positive and nega-
tive peaks at 265 and 210 nm, respectively, and a weak nega-
tive signal at 240 nm, in accordance with the A form of RNA.
Addition of one equivalent of ligand 13b slightly affects the
signal at 210 nm. This indicates that the involved interactions
do not produce a significant change in the RNA structure, and
the contribution of the S system (H-bonding) does not abolish
the overall base stacking (kissing interaction). In a similar way,
when the ligand concentration was increased to 5 or 10 equiv-
alents (high excess), a similar
From these results, we can conclude that: 1) compared to
neomycin, the S-based ligands have higher TAR affinities and
better specificities and 2) S conjugates featuring one amino
acid have slightly lower TAR affinities but better specificities
than their S–diamino acid analogues. These results also illus-
trate how the binding affinity and specificity of S–amino acid
conjugates can be tuned by optimizing the linker length and
the nature and number of amino acid residues.
To get further insights on the ligand–TAR binding mode, the
thermodynamic parameters associated with the formation of
the complexes were determined. Nonelectrostatic (DGonel, DHnoel
,
and TDSonel) and electrostatic (DGeol, DHoel, and TDSeol) parameters
were obtained by plotting the Gibbs free energy (DG8) versus
the temperature and by examining the dependency of the dis-
sociation constants on the ionic strength of the solution
(Table 3). The enthalpy of binding (DH8) is independent of the
salt concentration, so only the contribution of the Gibbs
energy to the overall binding is discussed in this section.
Indeed, the DG8 value, which represents the total energy, can
be divided into two components: 1) the DGonel value, which re-
flects the contribution of nonelectrostatic interactions to the
decrease of signal intensity at
210 nm was observed, which is
Table 3. Thermodynamic parameters for ligand–TAR interactions.
mainly due to the phosphate
(TAR)–ammonium (residual ex-
[b]
o [c]
Ligand
DG8
DH8[a]
TDS8[a]
TDS8/DH8 DGonel
TDSonel
DG
el
[kJmolÀ1
]
[kJmolÀ1
]
[kJmolÀ1
]
[kJmolÀ1
]
[kJmolÀ1
]
[kJmolÀ1
]
cess of ligand) interactions.
Moreover, as attested by NMR,
fluorescence, and CD spectra of
13b, no self-structural organiza-
tion of this ligand was observed
at high concentrations, which
completely excluded the contri-
bution of 13b alone to the ob-
served CD variations at 210 nm.
The fact that the CD spectra
only indicated minimal alteration
of the base stacking clearly indi-
neomycin À26.7
À26.7Æ1.3
À38.1Æ1.5
À38.4Æ0.62
À49.0Æ3.1
À46.7Æ2.4
À38.7Æ1.9
À58.6Æ5.1
À0.025Æ0.01 0.00093
À9.26Æ1.5 0.24
À17.8 (67%)
À8.9Æ0.9
8.9Æ0.8
1b
2b
3b
À28.8
À31.5
À25.6
À37.1
À39.1
À32.2
À25.7 (89%) À12.4Æ1.1 À3.1Æ1.0
À28.6 (91%) À9.74Æ0.9 À2.9Æ1.1
À6.84Æ0.63 0.18
À23.4Æ3.2
À9.84Æ2.9
À0.317Æ0.1
À26.8Æ4.9
0.61
0.21
0.0082
0.46
À24.7 (96%)
À0.9Æ0.3 À0.9Æ0.4
13b
14b
15b
À30.1 (81%) À16.8Æ2.2 À7.0Æ1.1
À35.9 (92%) À3.52Æ1.2 À3.2Æ1.0
À30.2 (94%) À28.8Æ1.7 À2.0Æ0.7
[a] Determined by temperature effect experiments by using the equation DGoT =DHTor +DCP-
(TÀTr)ÀTDSoTrÀTDCPln(T/Tr). See the Supporting Information for definitions and further details. [b] Determined
by salt effect experiments by using the equation log(Kd)=log(Knel)ÀZYlog[KCl]. See the Supporting Information
for definitions and further details. The percentage of nonelectrostatic interactions (DGonel/DG8) is given in paren-
theses. [c] DGoel =DG8ÀDGonel =TDSeol.
Chem. Eur. J. 2014, 20, 2071 – 2079
2075
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