Surbhi Sharmaa,
Loic Toupetb,
Musheer Ahmadc and
Farukh Arjmand*a
aDepartment of Chemistry, Aligarh Muslim University, Aligarh 202002, India. E-mail: farukh_arjmand@yahoo.co.in; Tel: +91 5712703893
bInstitut de Physique de Rennes, UMR 625, Université de Rennes 1, Campus de Beaulieu Bat. 11 A, 263 av. Général Leclerc, 35042 Rennes Cedex, France
cDepartment of Applied Chemistry, Aligarh Muslim University, Aligarh 202002, India
First published on 10th August 2016
New ternary chiral Cu(II) complexes 1a and b derived from L- and D-phenylalanine and 1,10-phenanthroline were synthesized and characterized thoroughly by single crystal X-ray diffraction and other spectroscopic techniques viz. UV-vis, IR, EPR, ESI-MS and elemental analysis. The complexes crystallized in the monoclinic P21 space group, possessing the lattice parameters a = 5.74690(10) Å, b = 20.6365(2) Å, c = 9.28010(10) Å, α = γ = 90°, and β = 98.2040(10) in complex 1a and a = 5.728(5) Å, b = 20.587(5) Å, c = 9.252(5) Å, α = γ = 90°, and β = 98.308(5) in complex 1b per unit cell, respectively. Comparative in vitro RNA binding studies of the L- and D-enantiomeric complexes, 1a and b, were carried out by a variety of optical spectroscopy techniques viz. UV-vis, fluorescence, and circular dichroism. Because copper is a redox metal ion, cyclic voltammetry was employed to evaluate the enantioselective RNA binding of the complexes. The results demonstrated that the L-enantiomer of Cu(II) complex, 1a, binds more strongly to the t-RNA motif than the D-enantiomer, thereby underlining the differential disposition of the enantiomers and the site preference of RNA for the L-enantiomer over the D-enantiomer. Furthermore, the comparative Kb, K and Ksv values of the L- and D-complexes demonstrated significant increases for the L-enantiomer of the copper complex, 1a, in comparison to its D-enantiomeric form, 1b. SEM analysis divulged surface morphological alteration of complexes 1a and b, evidenced by the formation of hollow tubes and a concrete-like structure with the RNA condensate, which was less pronounced in SEM micrographs of the complex 1b condensate. Complexes 1a and b were evaluated by the agar well diffusion method and demonstrated significant antibacterial activity.
The in vivo structures of DNA and RNA are very different; whereas DNA typically remains in the helical double stranded form, RNA folds into diverse structures, adopting folds that are similar to proteins; this is responsible for its diverse functions in cells.15 The specific recognition of pockets available in RNA by suitable ligands, involving non-covalent binding usually based on van der Waals forces, electrostatic interactions and surface complementarity, is considered to be an important asset for RNA targeted therapeutics.16 Therefore, studies on RNA–metal complex interactions could be highly instrumental for envisaging drug design strategies.17
Antibiotic resistance, particularly multi-drug resistance (MDR) of pathogenic bacteria, is one of the most crucial problems facing modern health care. Hence, the focus of pharmaceutical R&D is to discover and develop new improved antibiotics/anti-infectives with specific biological targets, viz. Riboswitch RNAs18 and RNA secondary structures, such as bulges and helices.14,19 Previous literature reports reveal that most antibacterials exert their activity by modulating ribosome functions and RNA fragments/motifs by the binding of a suitable ligand framework, which acts as a pharmacophore. A combinatorial synthetic strategy involving several ligand fragments, in our case L- and D-phenylalanine (as a chiral centre and metal binding domain), 1,10-phenanthroline (as a recognition element that induces intercalation) and a redox active copper centre, is highly directed for specific interactions at RNA binding sites. Both the L- and D-enantiomers were proven to be good anti-bacterial agents against Gram-positive Bacillus subtilis [MTCC 121] and Staphylococcus aureus [NRRLB 767] as well as Gram-negative Escherichia coli [K12] and Pseudomonas aeruginosa. Because metal complexes (electropositive tendencies) attract bacterial membranes and other nucleic acid and protein targets, they are logical options for metal-based therapeutics which can perform dual antibacterial and antitumor functions.20 The metal centre acts as a scaffold, holding the 3D structure of the biological ligands firmly in place and tuning/synchronizing the drug entity to reach a specific site of action. Chiral molecules play a critical role in the exploitation of three-dimensional space at the target site and regulate stereoselectivity in a highly organized fashion.21 Furthermore, the use of ancillary chiral amino acid ligands provides insight into the mechanism of action, allowing discrimination between unspecific interactions which are common to both enantiomers and specific contacts that give rise to enantioselectivity. An amino acid with a side chain aromatic ring, e.g. phenylalanine, contributes mainly to the stabilization of proteins through hydrophobic interactions and the formation of hydrophilic environments.22 These ligands play a crucial role in modulating the hard/soft properties of the metal ions and the lipophilic/hydrophilic balance of the metal complexes, thereby controlling their solubility as well as their permeability to cross cell barriers.
Copper is a biological redox element and has efficacious biocidal properties. Because of its biological congruity, a large number of copper(II) complexes have been synthesized and their biological activities have been scrutinized.23–25 Among all these complexes, copper(II) complexes containing amino acids and 1,10-phenanthroline ligand have been receiving considerable interest due to their biological relevance, good nucleic acid binding, and antimicrobial and anticancer activities.26–28 Recently, J. R. Aldrich-Wright et al. reported a number of copper(II) analogs with different derivatives of 1,10-phenanthroline ligand. The antimicrobial properties of these complexes against bacterial strains of S. aureus, E. coli, P. aeruginosa, and yeast S. cerevisiae were characterized, as well as the activity of their phen-based intercalating ligands.29
In the continuation of our recent interest in RNA targeted chemotherapeutics,30–32 we have carried out the synthesis, single X-ray diffraction studies and in vitro t-RNA binding studies of enantiomeric Cu(II) complexes derived from L- and D-phenylalanine and the intercalating ligand 1,10-phenanthroline, which has proven antibacterial activity. Both complexes are highly soluble in most organic solvents and are readily soluble in water, which is a prerequisite condition for the design of novel therapeutics, as water soluble complexes show superior ability to cross biological membranes. The binding propensities of the L- and D-conformations with yeast t-RNA were studied by UV-vis absorption and emission, circular dichroism spectroscopy and cyclic voltammetry.
:
1
:
1 stoichiometric ratio under reflux conditions, as depicted in Scheme 1. A dark blue transparent solution was formed and maintained at room temperature. Crystals of complexes 1a and b suitable for single X-ray crystallography were obtained by slow evaporation of the reaction mixture. The synthesized complexes were found to be stable towards air and soluble in organic solvents, such as MeOH, DCM, DMF and DMSO. The molecular structures of both complexes were established by single X-ray diffraction studies, which corroborated well with the elemental analysis and other spectroscopic measurements. The syntheses were repeated several times and were found to be reproducible.
A single crystal X-ray structural study revealed that complexes 1a and b both crystallized in the monoclinic P21 space group, possessing the lattice parameters a = 5.74690(10) Å, b = 20.6365(2) Å, c = 9.28010(10) Å, α = γ = 90°, and β = 98.2040(10) and a = 5.728(5) Å, b = 20.587(5) Å, c = 9.252(5) Å, α = γ = 90°, and β = 98.308(5) per unit cell, respectively. An ellipsoid view of complexes 1a and b along with the atom numbering scheme is shown in Fig. 1. The packing diagram is depicted in Fig. S1,† and selected bond lengths and angles of complexes 1a and b are listed in Tables S1–S4,† respectively. The complexes are mononuclear, and the asymmetric units of complexes 1a and b contain one NO3− ion, one water molecule and a Cu(II) ion; they possess a distorted square pyramidal geometry in which L- and D-phenylalanine, respectively, coordinate through the amino nitrogen and the deprotonated carboxylato oxygen atom, i.e. the amino acid is N, O chelated, forming a five-membered ring with an “envelope” conformation. The ligands 1,10-phen [Cu(1)–N(1) = 2.029(3) Å, Cu(1)–N(2) = 2.004(3) Å] and L-phe [Cu(1)–O(2) = 1.941(2) Å, Cu(1)–N(3) = 1.993(3) Å] in complex 1a and 1,10-phen [Cu(1)–N(2) = 2.025(3) Å, Cu(1)–N(3) = 2.001(3) Å] and D-phe [Cu(1)–O(1) = 1.940(2) Å, Cu(1)–N(1) = 1.985(3) Å] in complex 1b form the square base, while the water molecule has a long axial coordination [Cu(1)–O(1) = 2.199(3) Å] and [Cu(1)–O(1) = 2.191(3) Å], respectively. The values of the C–O and C–N bonds are in agreement with those in the literature for similar geometries.33 The square base formed by the coordinated atom in complexes 1a and b is almost planar, with deviations of 0.063 Å and 0.066 Å, respectively; the Cu(1) atom is out of the plane of N1N2N3O2 by ca. 0.24 Å and 0.23 Å, respectively, towards the axial water molecule. Further, extensive hydrogen bonding (NH⋯O, O–H⋯O, C–H⋯O, O–H⋯N) interactions involving the amine nitrogen, carboxylato oxygen, distorted nitrato oxygen, and lattice water molecule stabilize the molecules in the crystal lattice.
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| Fig. 1 ORTEP view of (a) complex 1a and (b) complex 1b with partial numbering. Solid thermal ellipsoids are reported at the 50% probability level. Hydrogen atoms have been omitted for clarity. | ||
The IR spectra of complexes depicted diagnostic bands in the range of 3239 to 3131 cm−1, which were attributed to the coordinated NH2 group vibrations of L- and D-phenylalanine, and two broad bands at 3469 and 3467 cm−1, ascribed to the stretching vibration of the water molecule in complexes 1a and b, respectively. The IR spectra also facilitated prediction of the coordination mode of the carboxylate group. The characteristic bands of the carboxylate group were observed in the range of 1580 to 1630 cm−1 for the asymmetric stretch and 1358 to 1410 cm−1 for the symmetric stretch; the differences in the stretching frequencies of 1620 to 1369 cm−1 in both the complexes (Δν = νasym − νsym) suggested a value >200, which indicated the terminal (monodentate) coordination mode of the carboxylate group of L- or D-phenylalanine with the metal in both complexes.34 Strong bands at 912, 858, 765 and 705 cm−1 were identified as the aromatic hydrocarbons with the motion of the ring hydrogens in the complexes. In the far-IR region, the presence of medium intensity bands at 535 and 428 cm−1 correspond to Cu–N and Cu–O vibrations, respectively, in both complexes.32
The ESI-MS spectra of complexes 1a and b (Fig. S2 and S3†) displayed a prominent peak at m/z 487, corresponding to the molecular ion peak [C21H20CuN4O6]+. Other fragmentation peaks for complexes 1a and b were observed at m/z 425 and 407, which could be assigned to [C21H20CuN4O6–NO3]+ and [C21H20CuN4O6–NO3–H2O]+, respectively.
The solid state X-band EPR spectra of L- and D-Cu(II) complexes 1a and b were recorded in the solid state at room temperature (RT) on an X-band frequency of 9.1 GHz under a magnetic field strength of 3000 G (Fig. S4†). In the solid state, both complexes showed an isotropic band centered at g = 2.05.35 These values were in good agreement with the unpaired electrons mainly located in the dz2 orbital, i.e. (eg)4(a1g)2(b1g)2(b2g)1. This pattern is typical for copper complexes with square pyramidal environments.
The electronic spectra of complexes 1a and b were recorded for 1 × 10−4 molar solutions of the metal complexes in DMSO; they displayed peaks at 265 nm and 296 nm, attributed to π–π* and low energy n–π* ligand centered transitions, while in the visible region, a broad d–d transition band at 618 nm validated the pentacoordinated geometry around the central Cu(II) metal in both the complexes.36
Although there are subtle differences in the binding potentials of the different enantiomers, we can nevertheless discriminate between the two enantiomeric forms by observing their spectral titration profiles. The differences in binding of the enantiomeric L- and D-forms are quite discernible due to the alternate conformation, as there is greater hypochromism in the case of L-enantiomer 1a of 36% with a red shift of 6 nm, while D-enantiomer 1b exhibited hypochromism of 31% with a red shift of 4 nm.
In order to quantitatively compare the binding strengths of complexes 1a and b with the t-RNA intrinsic binding constant, Kb values were calculated using the Wolfe–Shimmer eqn (1).39
| [RNA]/εa − εf = [RNA]/εb − εf + 1/Kb|εb − εf| | (1) |
| Yeast t-RNA | λmax (nm) | Kb (M−1) | % hyperchromism |
|---|---|---|---|
| Complex 1a | 265 | 2.6 (±0.08) × 105 | 36 |
| Complex 1b | 265 | 1.5 (±0.08) × 105 | 31 |
Because DNA is a primary pharmacological target for many metal-based drugs, the comparative binding profiles for complexes 1a and b with CT-DNA were also studied; the results revealed a higher order of binding constants with t-RNA compared to CT-DNA (intrinsic binding constant, Kb = 2.73 (±0.05) × 104 M−1 and 1.97 (±0.05) × 104 M−1). H. Xu et al.40 carried out similar binding studies on a ruthenium(II) polypyridyl complex; these observations revealed that the complex exhibited better potential for enantioselective binding to yeast t-RNA than to CT-DNA. This is quantitatively validated by the values of Kb, which were found to be 2.21 × 106 M−1 and 8.53 × 105 M−1 for yeast t-RNA and CT-DNA, respectively. This experimental finding demonstrates strong binding propensity and specificity for yeast t-RNA. The rationale for the specific RNA binding of the complexes could be (i) the highly exposed base pairs of RNA, which are easy to access and (ii) the bulge region of yeast t-RNA (which is absent in CT-DNA), which provides greater overlap in RNA, thereby enhancing the binding affinity of the complexes.41
The binding of complexes 1a and b with t-RNA was further validated by another, more sensitive fluorescence spectroscopy method. Upon excitation at a wavelength of 260 nm (λex), the fluorescence spectra of complexes 1a and b exhibited appreciable fluorescence at ca. 380 nm (λem) and demonstrated a further increase upon concomitant addition of t-RNA (0–4.00 × 10−5 M) without any apparent shift in the emission maxima (Fig. S5†). This enhancement in the fluorescence intensity could be largely attributed to the penetration of complexes into the hydrophobic environment of the interior t-RNA helix, thereby reducing its accessibility to solvent molecules as well as restricting the mobility of the complexes at the binding site, which causes reduction of the vibrational modes and leads to higher emission intensity.42
The binding strengths of complexes 1a and b with t-RNA were ascertained by the binding constant (K) value derived from a Scatchard equation43 and were found to be 4.6 × 105 M−1 and 3.2 × 105 M−1, respectively. On the basis of the K values, we can evaluate the extent and mode of binding of the different enantiomers to underline the enantiospecific discrimination.
Competitive binding experiments were carried out on the EB–t-RNA system by varying the concentration of the complex to obtain further insight into the binding affinities of the complex–yeast t-RNA interactions. EB is a planar cationic dye that emits intense fluorescence in the presence of t-RNA at ca. 600 nm (λem) due to its strong intercalation between the adjacent base pairs. The enhanced fluorescence was quenched upon addition of the second molecule by replacing the bound EB or accepting the excited electron from EB.44
It was observed that upon concomitant addition of complexes 1a and b to the EB–t-RNA system [complex]/[t-RNA] = 1
:
1 to 8
:
1, the emission intensity decreased progressively, indicative of competition between EB and the complexes towards yeast t-RNA binding (Fig. S6†). The extent of reduction of the emission intensity gives a measure of the binding propensity of the complex to t-RNA. Quantitative assessment of the magnitude of interaction was further ascertained by the classical Stern–Volmer equation as
| I0/I = 1 + Ksvr | (2) |
Circular dichroic titrations were performed as a function of complex concentration to monitor the conformational changes in t-RNA and the binding modes of the complexes upon interaction with t-RNA. The CD spectrum of free t-RNA displayed four major peaks at 208 and 240 nm (negative) and 221 and 270 nm (positive), consistent with the conformation of t-RNA. Upon addition of complex 1a (r = [complex]/[t-RNA] = 1), a lower decrease in the molar ellipticity band at 208 and 270 nm was observed, while the positive band at 227 and the negative band at 240 nm demonstrated relatively greater amplification. Complex 1b presented an inverse CD spectrum in which the intensity of the positive band at 227 significantly increased, while the intensity of the other bands decreased (Fig. S7†). The enhancement in intensity of the band at 270 nm in the spectra of the complex–t-RNA systems along with the major intensity changes of the bands at 210 and 227 nm could be attributed to the formation of t-RNA aggregates upon complexation.45,46 From these CD assays, we could virtually discriminate the enantiopreferential binding of t-RNA with the L- and D-forms of the complexes; to the best of our knowledge, this is the first report of an enantiomeric binding profile of RNA in the literature.
The electrochemical profiles of complexes 1a and b were studied in H2O/DMSO (95
:
5) at room temperature at a scan rate of 0.2 V s−1 by cyclic voltammetry in the potential range from 0.8 to −1.0 V. Both complexes displayed well-defined cathodic waves; however, the corresponding anodic waves were drawn out, revealing that the very unstable CuI species are not discernible with the time scale of the CV experiments.47 The cyclic voltammogram of 1a exhibited a quasi-reversible one-e− redox process involving the CuII/CuI couple with a cathodic peak at Epc = −0.48 V and an oxidation peak at Epa = −0.12 V (Fig. S8(a)†). For this couple, the difference between the cathodic and anodic peak potential ΔEp and the ratio of the cathodic and anodic peak currents Ipa/Ipc are −0.36 and 1.0, respectively. The formal electrode potential E1/2, taken as an average of Epc and Epa, was −0.30 V in the absence of t-RNA. The CV of 1b (Fig. S8(b)†) featured reduction of the CuII/CuI form at a cathodic peak potential of Epc = −0.45 V. Reoxidation of the complex occurred at Epa = −0.11 V. The difference between the anodic and cathodic peak potential ΔEp = −0.34 V and the Ipa/Ipc ratio = 0.77, which indicated a quasi-reversible redox process.
Addition of yeast t-RNA to the complexes resulted in significant reduction in the cathodic and anodic peak currents due to the slow diffusion of an equilibrium mixture of the free and RNA-bound complexes to the electrode surface. The observed shifts in the E1/2 values suggested that the CuII and CuI forms of complexes 1a and b were bound to the t-RNA. However, the shifts observed in the ΔEp, E1/2 and Ipa/Ipc values were greater for complex 1a than for complex 1b, which further validated the greater binding affinity of the L-isomer of the complex towards t-RNA.
These results suggested the condensation of t-RNA by cationic molecules and that a major factor governing the condensation of t-RNA is specific interaction of the complexes with the base pairs of t-RNA, which correlates well with the in vitro t-RNA binding studies.
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| Fig. 5 Molecular docked model of complex 1a docked into the active pocket of the anticodon arm of yeast t-RNA (PDB ID: 6TNA) along with the possible hydrogen bonding interactions. Hydrogen atoms have been omitted for clarity. | ||
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| Fig. 6 Molecular docked model of complex 1b docked into the active pocket of the anticodon arm of yeast t-RNA (PDB ID: 6TNA) along with the possible hydrogen bonding interactions. Hydrogen atoms have been omitted for clarity. | ||
The resulting binding energies calculated for the best docked pose of complexes 1a and b with the yeast t-RNA target were found to be −275 and −256 kJ mol−1, respectively. The more negative binding energy value of complex 1a signifies the greater binding propensity of the L-form of the metal complex, which correlates well with the results of the in vitro t-RNA binding studies.
| Compound | Zone of inhibition (mm) | |||||||
|---|---|---|---|---|---|---|---|---|
| B. subtilis | S. aureus | E. coli | P. aeruginosa | |||||
| 100 μg | 200 μg | 100 μg | 200 μg | 100 μg | 200 μg | 100 μg | 200 μg | |
| 1a | 27 | 33 | 11 | 17 | 20 | 27 | — | 10 |
| 1b | 22 | 27 | 10 | 14 | 16 | 23 | — | — |
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| Fig. 7 Antibacterial activity of complex 1a (A) and b (B) against E. coli and B. subtilis at 100 μg (A1 and B1) and 200 μg (A2 and B2) concentrations. | ||
:
5) were employed for the cyclic voltammetry studies using 0.4 M KNO3 as the supporting electrolyte. A three electrode configuration was used, comprising a Pt disk working electrode, a Pt wire counter electrode and Ag/AgCl as the reference electrode.
:
1 was added to this reaction mixture, affording a dark blue clear solution. Dark blue crystals of complexes 1a and b suitable for single X-ray crystallography were obtained by slow evaporation of the reaction mixture.
:
MeOH solution (7
:
3) at room temperature. Single crystal X-ray structural studies of the complexes were performed on a CCD Oxford Diffraction X caliber Saphir 3 diffractometer employing graphite-monochromated Mo-Kα radiation generated from a fine-focus sealed tube (λ = 0.71073 Å) at 140(2) K. The data collection strategy was evaluated using Crys Alis Pro CCD software. The collections of data were observed by the standard ω scan techniques and were scaled and reduced using Crys Alis Pro RED software. The structure was solved by direct methods using SIR-97 (ref. 51) and refined by least-squares methods on F2 using SHELXL-97.52 The positions of all atoms were obtained by direct methods. Anisotropic thermal parameters were assigned to all non-hydrogen atoms, and the remaining hydrogen atoms were placed in geometrically constrained positions and refined as riding atoms with a common fixed isotropic thermal parameter. The drawing of the complex was realized with PLATON.53 A summary of selected crystallographic data for complexes 1a and 1b is given in Table 3.
| a GoF is defined as {∑[w(F02 − Fc2)]/(n − p)}1/2, where n is the number of data and p is the number of parameters.b R = {∑||F0| − |Fc||/∑|F0|, wR2 = {∑w(F02 − Fc2)2/∑w(F02)2}1/2. | ||
|---|---|---|
| Complex | 1a | 1b |
| Formula | C21H22CuN4O7 | C21H22CuN4O7 |
| Fw (g mol−1) | 505.96 | 505.97 |
| Crystal system | Monoclinic | Monoclinic |
| Space group | P21 | P21 |
| a (Å) | 5.74690(10) | 5.728(5) |
| b (Å) | 20.6365(2) | 20.587(5) |
| c (Å) | 9.28010(10) | 9.252(5) |
| α (deg) | 90 | 90 |
| β (deg) | 98.2040(10) | 98.308(5) |
| γ (deg) | 90 | 90 |
| U (Å3) | 1089.32(2) | 1079.6(11) |
| Z | 2 | 2 |
| ρcalc (mg cm−3) | 1.543 | 1.557 |
| μ (mm−1) | 1.871 | 1.064 |
| F(000) | 522 | 522 |
| Flack | 0.027(11) | −0.016(13) |
| Temp (K) | 150(2) K | 150(2) K |
| Measured reflns | 9949 | 12 893 |
| Indep reflns | 3741 | 3579 |
| GOFa | 1.080 | 1.056 |
| Rb[I > 2σ(I)] | 0.0253 | 0.0301 |
| wR2b (all data) | 0.0775 | 0.0684 |
:
50 mM) buffer at pH 7.2 and included absorption spectral traces, emission spectroscopy, viscosity measurements and CD, conforming to the standard methods and practices previously adopted by our laboratory.54–56 While measuring the absorption spectra, equal amounts of CT-DNA and t-RNA were added to both the compound solution and the reference solution to eliminate the absorbance of the t-RNA itself, and the absorbance of the Tris buffer was subtracted through base line correction.
Footnote |
| † Electronic supplementary information (ESI) available. CCDC 1405339 and 1472957. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c6ra14503e |
| This journal is © The Royal Society of Chemistry 2016 |