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mixture started a re-equilibration process at room temperature.
After 5.5 hours, the statistical distribution of 27/29/22/22% for
Kn1/A1/Kn2/A2 was obtained (Figure 1c), indicating a full recall
of the initial equilibrium state presented in Figure 1a (see
spectra of the initial equilibria and the five metal ion-driven
DCLs). The distributions of the constituents and the calculated
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standard Gibbs free energy ΔG in the equilibrium states before
and after the addition of the metal ions, are shown in Figure 3
(the yellow columns show the amount of hydrolysis products,
consisting of the two aldehydes quinoline-8-carbaldehyde and
4-methoxybenzaldehyde). Among them, Ag(I) gave a slight shift
of the equilibrium, while Fe(II) and Zn(II) triggered larger shifts,
revealing their stronger ability to bind the dynamic ligand A2.
For Cu(II), the integrals of Cu(II)-A2 complex could not be
precisely obtained due to the strong broadening of all peaks,
however the decrease of the compounds Kn1 and A1, and the
amplification of Kn2 gave evidence for the shift in equilibrium.
The addition of Li(I) led only to a small amount of hydrolysis
indicating that its binding was too weak to be effective.
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Figure S5 for the H NMR spectra of the re-equilibrium process,
recorded every 1 h). To confirm the stronger complexation
ability of neocuproine towards Cu(I) cations in competition with
A2, 0.5 eq. CuOTf was added into a mixture of neocuproine and
A2 (1 eq. each). The resulting 1H NMR spectrum (Figure 2e)
showed a two-constituent mixture of the 1:2 Cu(I)-neocuproine
complex and free A2 (see Figure 2b for the separately prepared
[Cu(A2)2]+ complex and Figure 2a for A2 alone). As expected,
the same mixture was obtained when 1 eq. neocuproine was
added into separately prepared 1 eq. [Cu(A2)2]+ complex (Fig-
ure 2f). These two competition reactions both demonstrate that
neocuproine presents much stronger binding ability towards Cu
(I) than the imine A2. In addition, one notes that whereas on
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To test the effect of increasing the complexity of the system,
0.25 eq. Ag(I) and 0.25 eq. Cu(I) were mixed and injected into
the initially equilibrated DCL. A mixture of 17% Kn1, 18% A1,
33% Kn2 and 32% M-A2 complex was obtained, which is a
distribution intermediate between those of the two DCLs
separately driven by 0.5 eq. Cu(I) (8%, 9%, 42%, 40%) and
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titration of neocuproine with Cu(I), the H NMR spectra display
the peaks of both the free ligand and the complex (Figure S3c),
in the case of A2 the ligand signals shift progressively from
those of the free ligand to those of the complex (Figure S3b).
These different behaviors indicate that ligand exchange is slow
in the first case and fast in the second one, a further
confirmation that the neocuproine complex is much stronger
than the Cu(I)-A2 complex. Thus, both these thermodynamic
and kinetic features demonstrate that neocuproine is a suitable
reagent for driving the backward process of the Cu(I) driven
constitutional adaptation.
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0.5 eq. Ag(I) (23%, 22%, 26%, 27%) (see Figure S6b for the H
NMR spectra after separate addition of 0.5 eq. Ag(I), 0.25 eq Ag
(I)+0.25 eq Cu(I) and 0.5 eq. Cu(I)). These results indicate that
Cu(I) is a much better driver of the system than Ag(I) and
dominates the equilibrium shift.
The fingerprint-like outputs caused by the different binding
ability of the metal ions to the ligand A2, have the potential to
discriminate between different effectors, indicating that the
information about the identity of the metal cations operating
Generation of specific dynamic DCL distribution patterns in
response to different metal cations. Besides Cu(I), some other
metal ions were also tested for their effect on the constituent
distributions in the present DCL. To this end, a 2.5 mL CD3CN
solution of the DCL was prepared and, after reaching thermody-
namic equilibrium, was distributed equally into five NMR tubes.
Then to the tubes was added separately 0.5 eq. CD3CN stock
solution of the different triflate salts of Ag(I), Fe(II), Zn(II), Cu(II)
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and Li(I) tetrafluoroborate. The H NMR spectra were followed
until the equilibrium was reached (see Figure S6a for the
Figure 3. Dynamic constitutional distribution patterns and table of their
normalized integrals (the integral of Cu(II)-A2 was considered as correspond-
ing to that of its agonist Kn2) at the equilibrium state and after the addition
of five different metal ions (from left to right). Every reaction was repeated
Figure 2. 1H NMR (500 MHz, 298 K, CD3CN) spectra of: a) A2; b) [Cu(A2)2]+
complex; c) neocuproine; d) Cu(I)-neocuproine complex; e) reaction mixture
10 min after adding 0.5 eq. Cu(I) triflate into 1 eq. A2 and 1 eq. neocuproine;
f) reaction mixture 10 min after adding 1 eq. neocuproine into 1 eq.
serparately prepared [Cu(A2)2]+ complex.
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three times. The corresponding standard Gibbs free energies ΔG (T=298 K)
are shown on the bottom. The % of the constituents have been obtained
from the integration of the signals in the 1H NMR spectra; error of about 1%
(see also SI).
Chem Asian J. 2020, 15, 1–6
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© 2020 Wiley-VCH GmbH
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