Short communication Complexation of the Silver Cation with Dibenzo-30-crown-10: Extraction and DFT Study Emanuel Makrllk,1'* Petr Toman2 and Petr Vanura3 1 Faculty of Environmental Sciences, Czech University of Life Sciences, Prague, Kamycka 129, 165 21 Prague 6, Czech Republic 2 Institute of Macromolecular Chemistry, Academy of Sciences of the Czech Republic, Heyrovskeho sq. 2, 162 06 Prague 6, Czech Republic 3 Department of Analytical Chemistry, Institute of Chemical Technology, Prague, Technicka 5, 166 28 Prague 6, Czech Republic * Corresponding author: E-mail: makrlik@centrum.cz Received: 15-02-2012 Abstract From extraction experiments and /-activity measurements, the exchange extraction constant corresponding to the equilibrium Ag+(aq) + 1-Cs+(nb) o 1-Ag+(nb) + Cs+(aq) taking place in the two-phase water-nitrobenzene system (1 = di-benzo-30-crown-10; aq = aqueous phase, nb = nitrobenzene phase) was determined as log Kex (Ag+, 1-Cs+) = -1.7 ± 0.1. Further, the stability constant of the complex 1-Ag+ in nitrobenzene saturated with water was calculated for a temperature of 25 °C: log Pnb (1-Ag+) = 6.0 ± 0.2. Finally, by using quantum mechanical DFT calculations, the most probable structure of the resulting complex 1-Ag+ was solved. Keywords: Silver cation, dibenzo-30-crown-10, complexation, extraction and stability constants, water-nitrobenzene system, DFT calculations, complex structure 1. Introduction In 1967, Pedersen published his first papers1'2 dealing with cyclic polyether compounds with oxyethylene groups -CH2-CH2-O-, that are called crowns owing to their structure. These electroneutral compounds form relatively stable complexes in nonaqueous solvents, especially with alkali and alkaline-earth metal cations, the cations being placed in the ligand cavities. The ratio of the size of the crown ligand cavity to the ion radius of the central cation is a decisive or at least an important factor in the stability of the complex compounds formed.3 It is the complexing properties of the crowns that are due to the rapid development of the chemistry of these cyclic polyet-hers that we have witnessed in recent decades. At this point it should be noted that several reviews have covered many aspects of their chemistry.3-6 The dicarbollylcobaltate anion (DCC-)7 and some of its halogen derivatives are very useful reagents for the extraction of various metal cations (especially Cs+, Sr2+, Ba2+, Eu3+ and Am3+) from aqueous solutions into a polar organic phase, both under laboratory conditions for purely theoretical or analytical purposes,8-21 and on the technological scale for the separation of some high-activity isotopes in the reprocessing of spent nuclear fuel and acidic radioactive waste.22-24 In the current work, the stability constant of the ca-tionic complex species 1*Ag+, where 1 denotes dibenzo-30-crown-10 (see Scheme 1), in nitrobenzene saturated Scheme 1. Structural formula of dibenzo-30-crown-10 (abbrev. 1). with water was evaluated. Moreover, applying quantum mechanical DFT calculations, the most probable structure of the mentioned complex species was predicted. 2. Experimental Dibenzo-30-crown-10 (abbrev. 1; see Scheme 1) was purchased from Fluka. Cesium dicarbollylcobaltate (CsDCC)7 was synthesized by means of the method published by Hawthorne et al.25 The other chemicals used (Lachema, Brno, Czech Republic) were of reagent grade purity. The radionuclide 137Cs+ was supplied by Techsna-veksport, Russia. The extraction experiments were carried out in 10 mL glass test-tubes with polyethylene stoppers: 2 mL of an aqueous solution of AgNO3 of a concentration in the range from 1 x 10-3 to 5 x 10-3 mol/L and microamounts of 137Cs+ were added to 2 mL of a nitrobenzene solution of 1 and CsDCC, whose initial concentrations also varied from 1 x 10-3 to 5 x 10-3 mol/L (in all experiments, the initial concentration of 1 in nitrobenzene, C1in,nb, was equal to the initial concentration of CsDCC in this medium, CiCns,nDbCC). The test-tubes filled with the solutions were shaken for 2 h at 25 ±1 °C, using a laboratory shaker. Then the phases were separated by centrifugation. Afterwards, 1 mL samples were taken from each phase and their /-activities were measured using a well-type NaI(Tl) scintillation detector connected to a /-analyzer NK 350 (Gamma, Budapest, Hungary). The equilibrium distribution ratios of cesium, DCs, were determined as the ratios of the measured radioactivities of 137Cs+ in the nitrobenzene and aqueous samples. 3. Results and Discussion Previous results26-32 indicated that the two-phase water-AgNO3-nitrobenzene-1 (dibenzo-30-crown-10) -cesium dicarbollylcobaltate (CsDCC) extraction system (see Experimental), chosen for determination of the stability constant of the complex 1.Ag+ in water-saturated nitrobenzene, can be characterized by the main chemical equilibrium Ag+ (aq) + 1.Cs+ (nb) « 1.Ag+ (nb) + Cs+ (aq); Kex (Ag+, 1.Cs+) (1) with the respective equilibrium extraction constant Ke, (Ag+, 1.Cs+): K. (Ag , 1 • Cs ) = •-------p- [Ag+U1-CV]nh (2) where the subscripts "aq" and "nb" denote the aqueous and nitrobenzene phases, respectively. It is necessary to emphasize that 1 is a considerably hydrophobic ligand, practically present in the nitrobenzene phase only, where it forms - with Ag+ and Cs+ - the very stable complexes 1.Ag+ and 1.Cs+. Taking into account the conditions of electroneutrality in the organic and aqueous phases of the system under study, the mass balances of the univalent cations studied at equal volumes of the nitrobenzene and aqueous phases, as well as the measured equilibrium distribution ratio of cesium, DCs = [1.Cs+]nb / [Cs+]aq, combined with Eq. (2), we obtain the final expression for Kex (Ag+, 1.Cs+) in the form 1 Kex ( Ag+,1 * GS*J) = — L' pin. Cs ( ' + DCs ) C AíaNO, ^ in.ub CsDCC (3) where CiAn,gaNqO is the initial concentration of AgNO3 in the aqueous phas3 e and CiCns,nDbCC denotes the initial concentration of CsDCC in the organic phase of the system under consideration. In this study, from the extraction experiments and /-activity measurements (see Experimental) by means of Eq. (3), the following value of the constant Kex (Ag+, 1.Cs+) was determined as log Kex(Ag+, 1.Cs+) = -1.7 ± 0.1. Furthermore, with respect to previous results,28-32 for the exchange extraction constant Kex (Ag+, Cs+) corresponding to the equilibrium Ag+(aq) + Cs+(nb) « Ag+(nb) + Cs+ (aq) and for the extraction constant Kex (Ag+, 1.Cs+) defined above, as well as for the stability constants of the complexes 1.Cs+ and 1.Ag+ in nitrobenzene saturated with water, denoted by pnb (1.Cs+) and pnb (1.Ag+), respectively, one gets log pnb(1.Ag+) = log pnb(1.Cs+) + log Kex(Ag+,1.Cs+) - log Kex(Ag+, Cs+) (4) Using the value log Kex (Ag+, Cs+) = -1.8 inferred from References 26 and 27, the constant log Kex (Ag+, 1.Cs+) given above, log pnb (1.Cs+) = 5.9 ± 0.1,33 and applying Eq. (4), we gain the stability constant of the 1.Ag+ complex in nitrobenzene saturated with water as log pnb (1.Ag+) = 6.0 ± 0.2. This means that in the mentioned nitrobenzene medium, the stability constants of the cationic complex species 1.Ag+ and 1.Cs+ are comparable. The quantum mechanical calculations were carried out at the density functional level of theory (DFT, B3LYP functional) using the Gaussian 03 suite of programs.34 The LanL2DZ basis set was used and the optimizations were unconstrained. In order to increase the numerical accuracy and to reduce oscillations during the molecular geometry optimization, two-electron integrals and their derivatives were calculated by using the pruned (99,590) integration grid, having 99 radial shells and 590 angular points per shell, which was requested by means of the Gaussian 03 keyword "Int = UltraFine". Although a possible influence of a polar solvent on the detailed structures of 1 and its complex with Ag+ could be imagined, our quantum mechanical calculations in similar cases, performed in an analogous way, showed very good agreement of experiment with theory.35-42 In the model calculations, we optimized the molecular geometries of the parent crown ligand 1 and the 1.Ag+ complex species. The optimized structure of the free ligand 1 with center symmetry is illustrated in Figure 1. Figure 1. Two projections of the DFT optimized structure of free ligand 1 (B3LYP/LanL2DZ). Figure 2. Two projections of the DFT optimized structure of the 1*Ag+ complex (B3LYP/LanL2DZ). In Figure 2, the structure obtained by the full DFT optimization of the 1.Ag+ complex having a tennis-ball-seam conformation is depicted, together with the lengths of the corresponding bonds (in A; 1 A = 0.1 nm). In the 1.Ag+ cationic complex species, which is most energetically favoured, the "central" cation Ag+ is bound by ten strong interactions to four (Ar-O-CH2) ethereal oxygens (2.84, 2.78, 3.79 and 3.71 A) and six (CH2-O-CH2) ethereal oxygen atoms (2.67, 2.94, 2.66, 2.83, 2.86 and 2.66 A) of the parent crown ligand 1. Finally, the interaction energy, E(int), of the 1.Ag+ complex [calculated as the difference between the pure electronic energies of the complex 1.Ag+ and isolated 1 and Ag+ species: E(int) = E(1.Ag+) - E(1) - E(Ag+)] was found to be -471.0 kJ/mol, which confirms the formation of the considered cationic complex 1.Ag+. 4. Acknowledgements This work was supported by the Grant Agency of Faculty of Environmental Sciences, Czech University of Life Sciences, Prague, Project No.: 42900/1312/3114 "Environ- mental Aspects of Sustainable Development of Society," by the Czech Ministry of Education, Youth and Sports (Project MSM 6046137307) and by the Czech Science Foundation (Project P 205/10/2280). The computer time at the Meta-Centrum (Project LM 2010005), as well as at the Institute of Physics (computer Luna/Apollo), Academy of Sciences of the Czech Republic, is gratefully acknowledged. 5. References 1. C. J. Pedersen, J. Am. Chem. Soc. 1967, 89, 2495-2496. 2. C. J. Pedersen, J. Am. Chem. Soc. 1967, 89, 7017-7036. 3. I. M. Kolthoff, Anal. Chem. 1979, 51, 1R-22R. 4. J. J. Christensen, D. J. Eatough, R. M. Izatt, Chem. Rev. 1974, 74, 351-384. 5. J. S. Bradshaw, R. M. Izatt, Acc. Chem. Res. 1997, 30, 338345. 6.R. M. Izatt, K. Pawlak, J. S. Bradshaw, R. L. Bruening, Chem. Rev. 1991, 91, 1721-2085. 7. E. Makrlik, P. Vanura, Talanta 1985, 32, 423-429. 8. E. Makrlik, P. Vanura, P. Selucky, J. Solution Chem. 2009, 38, 1129-1138. 9. E. Makrlik, P. Vanura, P. Selucky, V. A. Babain, I. V. Smir-nov, Acta Chim. Slov. 2009, 56, 718-722. 10. E. Makrlik, P. Vanura, P. Selucky, Acta Chim. Slov. 2010, 57, 470-474. 11. E. Makrlik, P. Vanura, P. Selucky, Acta Chim. Slov. 2010, 57, 485-490. 12. E. Makrlik, P. Vanura, P. Selucky, Acta Chim. Slov. 2010, 57, 922-926. 13. E. Makrlik, P. Toman, P. Vanura, R. Rathore, Acta Chim. Slov. 2010, 57, 948-952. 14. E. Makrlik, P. Vanura, P. Selucky, Acta Chim. Slov. 2011, 58, 176-180. 15. E. Makrlik, P. Vanura, P. Selucky, Z. Spichal, Acta Chim. Slov. 2011, 58, 600-604. 16. E. Makrlik, P. Toman, P. Vanura, R. Rathore, Acta Chim. Slov. 2011, 58, 611-615. 17. E. Makrlik, P. Vanura, P. Selucky, Z. Spichal, Acta Chim. Slov. 2011, 58, 860-865. 18. E. Makrlik, P. Vanura, P. Selucky, J. Radioanal. Nucl. Chem. 2009, 279, 137-142. 19. E. Makrlik, P. Vanura, Z. Sedläkovä, J. Radioanal. Nucl. Chem. 2009, 280, 607-611. 20. E. Makrlik, P. Vanura, P. Selucky, J. Radioanal. Nucl. Chem. 2010, 283, 571-575. 21. E. Makrlik, P. Vanura, P. Selucky, J. Radioanal. Nucl. Chem. 2010, 284, 137-142. 22. V. N. Romanovskiy, I.V. Smirnov, V. A. Babain, T. A. Todd, R. S. Herbst, J. D. Law, K. N. Brewer, Solvent Extr. Ion Exch. 2001, 19, 1-21. 23. J. D. Law, R. S. Herbst, T. A. Todd, V. N. Romanovskiy, V. A. Babain, V. M. Esimantovskiy, I. V. Smirnov, B. N. Zaitsev, Solvent Extr. Ion Exch. 2001, 19, 23-36. 24. R. S. Herbst, D. R. Peterman, R. D. Tillotson, L. H. Delmau, Solvent Extr. Ion Exch. 2008, 26, 163-174. 25. M. F. Hawthorne, D. C. Young, T. D. Andrews, D. V. Howe, R. L. Pilling, A. D. Pitts, M. Reintjes, L. F. Warren, P. A. Wegner, J. Am. Chem. Soc. 1968, 90, 879-896. 26. J. Rais, Collect. Czech. Chem. Commun. 1971, 36, 32533262. 27. E. Makrlik, F. Božek, Polish J. Chem. 1998, 72, 949-952. 28. E. Makrlik, J. Hälovä, M. Kyrs, Collect. Czech. Chem. Commun. 1984, 49, 39-44. 29. E. Makrlik, P. Vanura, J. Radioanal. Nucl. Chem. 1996, 214, 339-346. 30. M. Dankova, E. Makrlik, P. Vanuura, J. Radioanal. Nucl. Chem. 1997, 221, 251-253. 31. E. Makrlik, P. Vanura, M. Dankova, J. Radioanal. Nucl. Chem. 1999, 240, 579-583. 32. E. Makrlik, P. Vanura, Monatsh. Chem. 2006, 137, 157-161. 33. E. Makrlik, P. Vannura, Unpublished results. 34. M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, J. A. Montgomery, Jr., T. Vre-ven, K. N. Kudin, J. C. Burant, J. M. Millam, S. S. Iyengar, J. Tomasi, V. Barone, B. Mennucci, M. Cossi, G. Scalmani, N. Rega, G. A. Petersson, H. Nakatsuji, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda, O. Kitao, H. Nakai, M. Klene, X. Li, J. E. Knox, H. P. Hratchian, J. B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R. E. Stratmann, O. Yazyev, A. J. Austin, R. Cammi, C. Pomelli, J. W. Ochterski, P. Y. Ayala, K. Moroku-ma, G. A. Voth, P. Salvador, J. J. Dannenberg, V. G. Zakrzew-ski, S. Dapprich, A. D. Daniels, M. C. Strain, O. Farkas, D. K. Malick, A. D. Rabuck, K. Raghavachari, J. B. Foresman, J. V. Ortiz, Q. Cui, A. G. Baboul, S. Clifford, J. Cioslowski, B. B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I. Komaro-mi, R. L. Martin, D. J. Fox, T. Keith, M. A. Al-Laham, C. Y. Peng, A. Nanayakkara, M. Challacombe, P. M. W. Gill, B. Johnson, W. Chen, M. W. Wong, C. Gonzalez, J. A. Pople, Gaussian 03, Revision C.02, Gaussian, Inc., Wallingford, CT, 2004. 35. J. Kriz, J. Dybal, E. Makrlik, Biopolymers 2006, 82, 536-548. 36. J. Kriz, J. Dybal, E. Makrlik, P. Vanura, J. Lang, Supramol. Chem. 2007, 19, 419-424. 37. J. Kriz, J. Dybal, E. Makrlik, P. Vanura, Supramol. Chem. 2008, 20, 387-395. 38. J. Kriz, J. Dybal, E. Makrlik, J. Budka, P. Vanura, Supramol. Chem. 2008, 20, 487-494. 39. J. Kriz, J. Dybal, E. Makrlik, J. Budka, J. Phys. Chem. A 2008, 112, 10236-10243. 40. J. Kriz, J. Dybal, E. Makrlik, J. Budka, P. Vanura, J. Phys. Chem. A 2009, 113, 5896-5905. 41. J. Kriz, P. Toman, E. Makrlik, J. Budka, R. Shukla, R. Rathore, J. Phys. Chem. A 2010, 114, 5327-5334. 42. J. Kriz, J. Dybal, E. Makrlik, P. Varura, B. A. Moyer, J. Phys. Chem. B 2011, 115, 7578-7587. Povzetek S pomočjo ekstrakcijskih eksperimentov in meritev y-aktivnosti smo v dvofaznem sistemu voda-nitrobenzen določili konstanto ekstrakcije za ravnotežje Ag+(aq) + 1-Cs+(nb) o 1-Ag+ (nb) + Cs+(aq) (1 = dibenzo-30-crown-10; aq = vodna faza, nb = faza nitrobenzena); log Kex (Ag+, 1-Cs+) = -1.7 ± 0.1. Pri temperaturi 25 °C smo v izračunali tudi konstanto stabilnosti kompleksa, Pnb, za 1-Ag+ v vodni fazi, nasičeni z nitrobenzenom, ki znaša log Pnb (1-Ag+) = 6.0 ± 0.2. Najbolj verjetno strukturo kompleksa 1-Ag+ smo ocenili z uporabo kvantnomehanskih DFT računov