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Electrochemical synthesis and structural characterisation of transition metal complexes with 2,6-bis(1-salicyloylhydrazonoethyl)pyridine, H4daps

 

作者: Manuel R. Bermejo,  

 

期刊: Dalton Transactions  (RSC Available online 1999)
卷期: Volume 0, issue 13  

页码: 2211-2218

 

ISSN:1477-9226

 

年代: 1999

 

DOI:10.1039/a902018g

 

出版商: RSC

 

数据来源: RSC

 

摘要:

DALTON FULL PAPER J. Chem. Soc., Dalton Trans., 1999, 2211–2217 2211 Electrochemical synthesis and structural characterisation of transition metal complexes with 2,6-bis(1-salicyloylhydrazonoethyl) pyridine, H4daps Manuel R. Bermejo,*a Matilde Fondo,a Ana M. González,a Olga L. Hoyos,a Antonio Sousa,*a Charles A. McAuliVe,*b Wasif Hussain,b Robin Pritchard b and Vladimir M. Novotorsev c a Departamento de Química Inorgánica, Facultad de Química, Universidad de Santiago, E-15706 Santiago de Compostela, Spain.E-mail: qimb45@uscmail.usc.es; qiansoal@uscmail.usc.es b Department of Chemistry, University of Manchester Institute of Science and Technology, Manchester, UK M60 1QD c N.S. Kurnakov Institute of General and Inorganic Chemistry, 31 Leninsky prosp., 117907 Moscow, Russian Federation Received 15th March 1999, Accepted 11th May 1999 Neutral manganese, cobalt and nickel complexes of the pentadentate hydrazone 2,6-bis(1-salicyloylhydrazonoethyl) pyridine (H4daps) have been prepared by means of electrochemical syntheses.They have been characterised by elemental analyses, IR spectroscopy, fast atom bombardment mass spectrometry (FAB) and magnetic susceptibility measurements. The molecular structures of [Mn(H2daps)(py)2] 1, [Co(H2daps)(py)2] 2, [Ni2(H2daps)2]?CH2Cl2 3, and [Ni2(H2daps)2(py)2]?CH2Cl2 4 have been determined by X-ray diVraction. Depending on the nature of the metal ion, the dianionic [H2daps]22 ligand shows diVerent co-ordination modes in these complexes: 1 and 2 are mononuclear with the metal atom in a pentagonal bipyramidal environment, 3 and 4 are binuclear with a helicate structure in which the nickel atoms attain octahedral co-ordination.Introduction In the past few years the co-ordination properties of hydrazone ligands have extensively been investigated.1–9 The development of this co-ordination chemistry is, in part, the result of the interesting donor systems which could result.Many ligands, mainly containing nitrogen donors in heterocyclic rings, but also in hydrazones, have been investigated in an attempt to predict their behaviour upon co-ordination. The structural characterisation of the resultant mononuclear or polynuclear complexes has led to some emerging patterns and has improved the design of molecular threads which may be twisted, yielding helical molecular systems.6,7 Nevertheless many questions still remain and the predicted systems are not always obtained.The desire for an in depth understanding of the rules that lead to systems of diVerent nuclearity, together with their pharmacological activity,10–12 as well as their interesting electric and magnetic properties,13–15 make research on the co-ordination chemistry of hydrazone ligands even more attractive. Part of our research program is directed towards the synthesis and structural characterisation of transition metal complexes with SchiV bases.16 Many methods of synthesis have been tried in an attempt to obtain compounds of this kind.Recently we have turned our attention to electrochemical synthesis, as it has been found to be a convenient route for the preparation of neutral SchiV base metal complexes through the oxidation of a metal anode in a solution of a SchiV base bearing weakly acidic groups, e.g. salicylaldimines (phenol OH) or pyrrolaldimines (pyrrole NH).17 In this paper we apply this methodology to synthesize neutral complexes of Mn, Co and Ni containing 2,6-bis(1-salicyloylhydrazonoethyl)pyridine, H4daps with high purity and good yield.Results and discussion A series of neutral chelate complexes has been synthesized by electrochemical oxidation of the corresponding metal anode in the presence of the neutral ligand H4daps in an organic solvent. The electrochemical eYciency of the cell (Table 1) was close to 0.5 mol F21, which is compatible with Scheme 1. Cathode: H4daps 1 2e2 æÆ H2(g) 1 H2daps22 Anode: H2daps22 1 M æÆ M(H2daps) 1 2e2 Scheme 1 Elemental analyses (Table 2) show that all metals react with the ligand in molar ratio 1 : 1 to aVord solvated complexes of the bis-deprotonated ligand [H2daps]22 in high purity.These neutral metal complexes are obtained in high yields and appear to be stable in the solid state and in solution. Most of them are Table 1 Experimental conditions for the electrochemical syntheses (initial current 10.0 mA, electrolysis time 2.5 h) Metal Amount (mg) dissolved Voltage (V) Ef a/ mol F21 Mn Co Ni 30.4 30.2 25.1 17.5 4.2 3.3 0.59 0.55 0.52 a Electrochemical eYciency of the cell, defined as the amount of metal dissolved per Faraday of charge.2212 J.Chem. Soc., Dalton Trans., 1999, 2211–2217 Table 2 Analytical and some selected data for the complexes Analysis (%) a Complex C N H meff/mB FABb m/z Colour Mn(H2daps)(H2O)0.5 Co(H2daps)(H2O)1.5(CH3CN) Ni(H2daps)(H2O)1.5(CH3CN) Ni(H2daps)(CH2Cl2)0.5 56.0 (55.9) 54.3 (53.9) 53.6 (53.9) 53.5 (53.2) 14.4 (14.2) 14.9 (15.1) 15.4 (15.1) 13.3 (13.2) 3.6 (4.0) 4.4 (4.4) 4.6 (4.5) 3.9 (3.8) 5.7 4.0 2.9 2.9 485 489 488–491; 976* 488–491; 976* Dark orange Yellow-orange Yellow-brown Yellow-brown a Found (calculated). b Peaks corresponding to [ML]1 except * that correspond to [M2L2]1.Table 3 Selected bond lengths (Å) and angles (8) for complexes 1 and 2 with estimated standard deviations (e.s.d.s) in parentheses 1 2 Mn1–O2 Mn1–N1 Mn1–N2 Mn1–N6 O2–Mn1–O29 O2–Mn1–N1 O2–Mn1–N2 O2–Mn1–N29 O2–Mn1–N6 O2–Mn1–N69 N1–Mn1–N2 N1–Mn1–N29 N1–Mn1–N6 N2–Mn1–N29 N2–Mn1–N6 N2–Mn1–N69 N6–Mn1–N6 2.243(4) 2.380(6) 2.267(5) 2.297(4) 88.2(2) 135.9(1) 68.4(2) 156.1(2) 87.6(2) 86.6(1) 67.7(1) 67.7(1) 94.0(1) 135.3(3) 87.8(2) 95.2(2) 172.0(2) Co1–O2 Co1–O1 Co1–N1 Co1–N3 O2–Co1–O1 O2–Co1–N1 O2–Co1–N3 O2–Co1–N2 O2–Co1–N6 O2–Co1–N7 O1–Co1–N1 O1–Co1–N3 O1–Co1–N2 O1–Co1–N6 O1–Co1–N7 2.153(5) 2.171(5) 2.213(6) 2.181(6) 78.3(2) 140.2(2) 149.2(2) 70.6(2) 89.8(2) 87.6(2) 141.2(2) 70.9(2) 148.6(2) 88.1(2) 89.4(2) Co1–N2 Co1–N6 Co1–N7 N1–Co1–N3 N1–Co1–N2 N1–Co1–N6 N1–Co1–N7 N3–Co1–N2 N3–Co1–N6 N3–Co1–N7 N2–Co1–N6 N2–Co1–N7 N6–Co1–N7 2.210(6) 2.168(6) 2.193(6) 70.5(2) 70.1(2) 94.7(2) 88.6(2) 140.1(3) 88.9(2) 92.3(2) 88.3(2) 92.8(2) 176.7(2) insoluble or sparingly soluble in water and common organic solvents but soluble in polar co-ordinating solvents such as DMF, DMSO and pyridine.All the complexes melt above 300 8C.FAB mass and IR spectra All the FAB mass spectra show peaks (Table 2) due to the fragments [M(H2daps)]1. A peak at m/z 976 due to the fragment [Ni(H2daps)]2 1 is also observed for 3 and for Ni(H2daps)- (H2O)1.5(CH3CN). The IR spectra show that in all cases the Fig. 1 Molecular structure of [Mn(H2daps)(py)2] 1 showing the atomic numbering scheme. bands due to the amide I [n(CO)] and amide II [d(NH) 1 n(CN)] modes undergo negative shifts of 19–60 and 46–64 cm21, respectively.This behaviour is compatible with the participation of the oxygen atoms of both carbonyl CO groups in the co-ordination to the metal, in agreement with previous results.18 The spectra also show the absence of the n(N–H) bands, which for the “free” ligand appear at 3208 cm21. This is in accordance with the dianionic nature of the ligand. X-Ray studies Crystal structures of [Mn(H2daps)(py)2] 1 and [Co(H2daps)- (py)2] 2. The crystal structures of complexes 1 and 2 are shown in Figs. 1 and 2 and selected bond lengths and angles are given in Table 3. Both structures consist of discrete [M(H2daps)(py)2] molecules, with a crystallographic twofold axis bisecting the Fig. 2 Molecular structure of [Co(H2daps)(py)2] 2 showing the atomic numbering scheme.J. Chem. Soc., Dalton Trans., 1999, 2211–2217 2213 Table 4 Selected bond lengths (Å) and angles (8) for complexes 3 and 4 with estimated standard deviations (e.s.d.s) in parentheses 3 4 Ni1–N1 Ni1–N19 Ni1–N4 Ni1–N49 Ni1–O2 Ni1–O29 Ni1 ? ? ? Ni2 N4–Ni1–N49 N4–Ni1–O29 N4–Ni1–O2 N4–Ni1–N1 N4–Ni1–N19 N49–Ni1–O29 N49–Ni1–O2 N49–Ni1–N1 N49–Ni1–N19 O29–Ni1–O2 O29–Ni1–N1 O29–Ni1–N19 O2–Ni1–N1 O2–Ni1–N19 N1–Ni1–N19 Ni2–N1–Ni1 2.281(5) 2.430(4) 1.962(4) 1.965(4) 2.026(4) 2.010(3) 3.06(2) 174.34(18) 106.31(16) 79.35(16) 76.14(18) 100.53(16) 79.35(16) 99.86(16) 104.64(17) 73.81(16) 104.37(15) 84.49(15) 153.05(14) 155.14(15) 82.80(15) 99.88(15) 80.73(14) Ni2–N1 Ni2–N19 Ni2–N2 Ni2–N29 Ni2–O1 Ni2–O19 Ni2–N1–Ni1 N2–Ni2–O1 N2–Ni2–O19 N2–Ni2–N19 N29–Ni2–N2 N29–Ni2–O1 N29–Ni2–O19 N29–Ni2–N19 N1–Ni2–N2 N1–Ni2–N29 N1–Ni2–N19 N1–Ni2–O1 N1–Ni2–O19 O1–Ni2–O19 O1–Ni2–N19 O19–Ni2–N19 2.454(4) 2.300(4) 1.956(4) 1.953(4) 2.002(3) 2.019(4) 89.74(13) 79.10(17) 100.08(17) 104.37(17) 173.70(17) 107.14(16) 79.06(17) 75.80(17) 73.92(16) 99.80(16) 98.64(17) 152.73(17) 80.86(16) 108.04(15) 84.17(15) 154.41(15) Ni1–N1 Ni1–N2 Ni1–O1 Ni2–N4 Ni2–N5 Ni2–O3 Ni1 ? ? ? Ni2 N2–Ni1–N29 N2–Ni1–O1 N2–Ni1–O19 N2–Ni1–N19 N2–Ni1–N1 O1–Ni1–O19 O1–Ni1–N19 O1–Ni1–N1 N19–Ni1–N1 N4–Ni2–N49 N4–Ni2–N5 N4–Ni2–N59 N5–Ni2–N59 O3–Ni2–N5 O3–Ni2–N59 O39–Ni2–N49 2.175(11) 1.990(12) 2.120(10) 2.136(13) 2.148(12) 2.036(10) 4.51(9) 165.1(7) 76.9(4) 93.0(4) 76.7(5) 113.1(5) 95.1(5) 153.6(4) 87.5(4) 101.7(6) 87.9(7) 162.5(5) 85.0(4) 106.0(6) 76.5(4) 106.2(5) 87.4(5) O3–Ni2–N49 O3–Ni2–N4 O3–Ni2–O39 89.4(5) 87.4(5) 175(6) molecule in complex 1.The metal atom is in a distorted pentagonal bipyramidal environment [MN5O2] in both complexes.The equatorial plane of the bipyramid is occupied by the N3O2 donor set of the [H2daps]22 ligand, giving rise to four fivemembered chelate rings. Four of the five angles subtended at Mn by adjacent equatorial atoms are slightly smaller than the value of 728 for an ideal pentagonal bipyramidal arrangement, ranging from 67.7(1) to 68.4(2)8, while the fifth angle [O2–Mn1–O29] is 88.2(2)8. The pentagon is less distorted in the cobalt complex [four angles ranging from 70.1 to 70.98 and the fifth O2–Co1–O1 78.3(2)8].The deviations of the pentagon from planarity are also somewhat diVerent in the two cases. The five atoms of the donor set are planar within the experimental errors for the manganese complex (maximum deviation from the N3O2 least squares plane = 0.084 Å, with the manganese atom sitting on the plane) while the deviation from planarity is slightly higher for the cobalt compound (maximum = 0.098 Å, with the cobalt atom 0.004 Å below this plane).In both cases the apical positions are filled by two pyridine molecules, which come from the solvent of crystallisation. The interaxial angle is closer to the ideal value in the cobalt (176.7(2)8) than in the manganese complex (172.0(2)8). The structures of complexes 1 and 2 feature intramolecular hydrogen bonds between the phenol hydrogen atom and the hydrazide nitrogen atom, O (phenol) ? ? ? N (hydrazide) of ca. 2.5 Å for the manganese and cobalt complexes.This interaction resulted in O3–C14 acquiring some double bond character (1.323(8) Å for Mn and 1.331(9) Å for Co; ideal value for C–OH (phenol) = 1.36 Å). These data are in agreement with the bisdeprotonated nature of the ligands in 1 and 2. All the angles and bond distances are similar to the values found in related seven-co-ordinate complexes of Co and Mn containing acylhydrazones 19–23 and do not merit further discussion. Intermolecular interactions by p–p stacking between two very close capping pyridines and between two phenol rings are observed in 1 but not in 2.Crystal structure of [Ni2(H2daps)2]?CH2Cl2 3. The crystal structure of [Ni2(H2daps)2]?CH2Cl2 is shown in Fig. 3, together with the atom numbering scheme. Bond angles and distances are contained in Table 4. The compound is a binuclear nickel complex, with a helicate structure, solvated with one dichloromethane molecule. Each H4daps behaves as a dianionic ligand using five [ONNNO] donor atoms, viz.the pyridine nitrogen, both imine nitrogen and both carbonyl oxygen atoms, as in 1 and 2. However, the co-ordination mode of the ligand is found to diVer from that in 1 and 2. In 3 each ligand uses one imine nitrogen atom and one carbonyl oxygen atom to bind one metal centre. A rotation around the C–C bond adjacent to the pyridine ring allows the pyridine nitrogen atom to act as a bridge between the two nickel atoms. A further rotation about the symmetrical adjacent C–C bond leads to chelation of the remaining imine nitrogen and carbonyl oxygen atoms to a second metal centre, generating a double helical structure.This co-ordination mode produces four five-membered chelate rings around each nickel atom, which are in a distorted octahedral environment [NiN4O2]. The Ni ? ? ? Ni distance is 3.06(2) Å. This short distance is the result of the distortion of the central rhombus Ni1–N1–Ni2–N19, formed by both pyridine bridges and the two nickel atoms, with higher angles around each Ni atom (ca. 1008) and smaller than 908 around the pyridine nitrogen atoms. The Ni–N bond lengths are rather diVerent from one Fig. 3 An ORTEP24 view of the crystal structure of [Ni2- (H2daps)2]?CH2Cl2 3. Thermal ellipsoids are drawn at the 30% probability level. Lattice CH2Cl2 is not depicted. Hydrogen atoms, except those attached to oxygen atoms, are omitted for clarity.2214 J. Chem. Soc., Dalton Trans., 1999, 2211–2217 another; the Ni–N (imine) bonds (of ca. 1.96 Å) are shorter than the Ni–N (pyridine) bonds [ranging from 2.281(5) to 2.454(4) Å]. For each metal ion, one of the Ni–N (pyridine) bond lengths [Ni1–N1 2.281(5) and Ni2–N19 2.300(4) Å] is shorter than the other one [Ni1–N19 2.430(4) Å and Ni2–N1 2.454(4) Å]. The shorter distance corresponds to the interaction between the nickel atom and the pyridine ring in an equatorial plane and the longer one to the interaction with the pyridine group in an axial position.The Ni–O distances are similar for both metals (ca. 1.27 Å) and do not deserve further consideration. The four C–N (imine) bond distances are ca. 1.28 Å, typical of a double C]] N bond, and show the lack of electronic delocalisation as a consequence of the non-planar conformations of the ligands. The N (hydrazide) ? ? ? O (phenol) distances of ca. 2.5 Å, typical of intramolecular hydrogen bonds, indicate deprotonation of the hydrazide nitrogen atoms of the ligand.The most interesting feature of this compound lies in the octahedral environment around each metal centre and the double helical structure, as hydrazone ligands of this type usually lead to seven-co-ordinated complexes with a pentagonal bipyramidal geometry,1–4,11–15 as has also been found in 1 and 2. Helicates containing pyridine as a bridge have previously been described, mainly containing ligands with nitrogen donor atoms in heterocyclic rings or in acyclic imines,7 but few of them contain hydrazones. As far as we know, the most similar complex reported is [Ni(dapz)]2 25 [H2dapz = 2,6-diacetylpyridinebis( 19-phthalozinylhydrazone)] and a comparison between bond distances and angles for both complexes is shown below (see Table 5).Another important fact in relation with this structure is that it was thought that if a metal ion with a strong ligand fieldimposed preference for an octahedral geometry was selected, and a ligand with central pyridine and two other bidentate domains in each thread was used, a double helicate would result.7 The only diYculty would be to prevent the metal centres from adopting a pentagonal bipyramidal geometry.This could be avoided by introducing bulky substituents on the hydrazone. However these do not seem to be the unique reasons for obtaining a double helicate. The structure of a monomeric nickel compound [Ni(H4daps)(H2O)2]21, containing H4daps as a neutral ligand, has been described.26 The nickel atom is in a [NiN3O4] pentagonal bipyramidal environment, H4daps forming the equatorial plane and the water molecules filling the axial positions. The diVerent structures observed in 3 and in [Ni(H4daps)(H2O)2]21 cannot be attributed to the diVerent charge of the ligand (dianionic and neutral), as similar monomers have been found for manganese complexes containing dianionic and neutral H2dappc ligands (H2dappc = 2,6- diacetylpyridinebis(picolinylhydrazone)].20 In addition, reasons adducing diVerent nuclearity based on acidity of the reaction medium27 seem not to be valid in this case, as both compounds [Ni2(H2daps)2]?CH2Cl2 and [Ni(H4daps)(H2O)2][NO3]2 were obtained in a neutral medium.In an attempt to obtain the mononuclear neutral complex, 3 was treated with pyridine. This method has been previously reported to be successful for obtaining monomeric cobalt complexes with 2,29:69,20:60,2-:6-,2+-quinquepyridine ligands from binuclear complexes.28 However, in this case the experiment led to asymmetric cleavage of the pyridine bridges, yielding another helicate binuclear compound [Ni2(H2daps)2(py)2]? CH2Cl2, 4.Crystal structure of [Ni2(H2daps)2(py)2]?CH2Cl2 4. The molecular structure of [Ni2(H2daps)2(py)2]?CH2Cl2 4 is shown in Fig. 4, together with the atom numbering scheme and main bond distances and angles are given in Table 4. The compound is a binuclear nickel derivative, with the Ni atoms located on a crystallographic twofold axis.The [H2daps]22 ligand spans both metal atoms, and each nickel atom is in a distorted octahedral [NiN4O2] environment. However the nickel environments are diVerent. One arises from co-ordination of one nickel atom to the pyridine nitrogen, the imine nitrogen and one carbonyl oxygen atom of two [H2daps]22 ligands, the other from coordination of the nickel atom to one imine nitrogen and one carbonyl oxygen atom of two [H2daps]22 ligands and to the two nitrogen atoms of two pyridine molecules.Again, the Ni–N bond lengths are diVerent from one another and, as in complex 3, the Ni–N (imine) bonds are shorter than the Ni–N (pyridine) bonds. In addition, the Ni–N lengths corresponding to the isolated pyridine molecules are shorter than the one corresponding to the pyridine fragment of [H2daps]22. This is most probably due to steric hindrance. It should be noted that these distances are shorter than the corresponding distances in 3.This is a reflection of the pyridine in 3 acting as a bridging N donor rather than a terminal donor in 4. The cleavage of the pyridine bridges also leads to a longer Ni ? ? ? Ni distance in 4, 4.51(9) Å, than in 3, 3.06(2) Å. The C–O (phenol) distances of 1.27(2) and 1.34(2) Å are shorter than the ideal value. These data and the distances N (hydrazide) ? ? ? O (phenol) of ca. 2.5 Å suggest the presence of an intramolecular hydrogen bond between the phenol oxygen and the hydrazide nitrogen atoms, as a result of the bisdeprotonation of the ligand. It should be stressed that although the interaction of 3 with pyridine results is breaking of the pyridine bridges, the product of the reaction is not the expected mononuclear complex but a binuclear compound with both nickel atoms in diVerent environments.This behaviour contrasts with the symmetric breaking of the pyridine bridges in a binuclear complex containing quinquepyridine ligands, to yield mononuclear compounds.7,28 If we compare the binuclear compounds 3 and 4 with the related complexes [Ni2(dapz)2] and [Ni(H4daps)(H2O)2]21 (Table 5), some conclusions can be drawn.(1) The complexes [Ni2- (H2daps)2] and [Ni2(dapz)2] present very similar double helical structures, with both hydrazone ligands adopting the same conformation. The most remarkable diVerence is a more distorted Ni1–N1–Ni2–N19 central rhombus for 3, leading to a shorter Ni–Ni distance (3.06(2) Å in 3 and 3.125(2) Å in [Ni2(dapz)2]).All the other distances are quite similar and in the range of those expected for complexes containing hydrazone ligands. (2) The comparison of 3 and 4 with [Ni(H4daps)(H2O)2]21 is maybe more interesting and clearly shows a longer Ni–N (pyridine) distance in the binuclear complexes {ranging from 2.281(5) to 2.454(4) for 3, 2.175(11) for 4 and 2.028(6) Å for [Ni(H4daps)- Fig. 4 An ORTEP view of the crystal structure of [Ni2(H2daps)2- (py)2]?CH2Cl2 4.Lattice CH2Cl2 is not depicted. Thermal ellipsoids are drawn at the 30% probability level.J. Chem. Soc., Dalton Trans., 1999, 2211–2217 2215 Table 5 Comparison of bond lengths (Å) in 3, 4 and related complexes [Ni(H4daps)(H2O)]21a [Ni2(H2dapz)2] b [Ni2(H2daps)2] c [Ni2(H2daps)2(py)2] c Ni1–N (pyridine) Ni2–N (pyridine) Ni1–N (imine) Ni2–N (imine) Ni1–O (carbonyl) Ni2–O (carbonyl) Ni1 ? ? ? Ni2 C–N (pyridine) C (pyridine)–C (imine) C–N (imine) N (imine)–N (hydrazine) N (hydrazine)–C (carbonyl) C–O (carbonyl) C–O (phenol) N (hydrazine) ? ? ? O (phenol) 2.028(6) — 2.194(6); 2.081(6) — 2.628(6); 2.247(6) —— 1.347(10); 1.319(11) 1.490(11); 1.487(12) 1.288(10); 1.275(10) 1.342(10); 1.332(10) 1.371(11); 1.354(11) 1.221(10); 1.217(10) 1.377(9); 1.356(10) 2.62(1); 2.58(1) 2.347(7); 2.348(6) 2.313(7); 2.249(6) 1.985(7); 1.974(7) 1.975(7); 1.967(7) —— 3.125(2) 1.37(1); 1.36(1) 1.36(1); 1.36(1) 1.48(1); 1.39(1) 1.47(1); 1.45(1) 1.30(1); 1.30(1) 1.30(1); 1.28(1) 1.38(1); 1.36(1) 1.38(1); 1.36(1) — — — — 2.430(4); 2.281(5) 2.454(4); 2.300(4) 1.965(4); 1.962(4) 1.956(4); 1.953(4) 2.026(4); 2.010(3) 2.019(4); 2.002(3) 3.06(2) 1.357(7); 1.345(6) 1.364(7); 1.340(7) 1.481(8); 1.475(8) 1.466(8); 1.460(8) 1.284(6); 1.279(6) 1.288(7); 1.285(7) 1.377(6); 1.373(6) 1.375(6); 1.369(6) 1.342(7); 1.340(7) 1.340(7); 1.327(7) 1.276(6); 1.263(6) 1.277(6); 1.266(6) 1.346(7); 1.332(7) 1.351(8); 1.335(8) 2.56(2); 2.54(2) 2.175(11); 2.175(11) — 1.990(12); 1.990(12) 2.148(12); 2.148(12) 2.120(10); 2.120(10) 2.036(10); 2.036(10) 4.51(9) 1.36(2); 1.34(2) 1.36(2); 1.34(2) 1.50(2); 1.44(2) 1.50(2); 1.44(2) 1.30(2); 1.30(2) 1.30(2); 1.30(2) 1.39(2); 1.39(2) 1.39(2); 1.39(2) 1.35(2); 1.34(2) 1.35(2); 1.34(2) 1.28(2); 1.25(2) 1.28(2); 1.25(2) 1.34(2); 1.27(2) 1.34(2); 1.27(2) 2.56(2); 2.56(2) a Ref. 26. b Ref. 25. c This work. (H2O)2]21}, even when the pyridine ring is acting as a terminal donor (4). In contrast to this, the Ni–N (imine) and Ni–O (carbonyl) bonds are shorter in the binuclear complexes.The non-planar conformation of the ligands and the consequent lack of delocalisation is shown in all cases by the short C–N (imine) bonds (ca. 1.28 Å). The dianionic nature of the ligand in 3 and 4 is pointed out by the C–O (phenol) distances: these are slightly shorter for the binuclear compounds and reflect the intramolecular hydrogen bond between the phenol oxygen and the hydrazide nitrogen atoms.Magnetic measurements All the compounds show magnetic moment values per atom very close to that expected for their magnetically dilute metal(II) ions at room temperature. This confirms the oxidation state 1II of the metal centre and indicates the bis-deprotonation of H4daps. Magnetic measurements at variable temperature have been performed for the binuclear nickel compounds, 3 and 4. Magnetic susceptibility data for 3 were collected in the 78–289 K range, using a Faraday balance, and in the 5–300 K range for 4 in a SQUID at a small applied field of 5000 G.The magnetic behaviour of 3 and 4 is shown in Figs. 5 and 6, respectively, as plots of meff per Ni atom versus temperature. The eVective magnetic moments of complex 3 were calculated by formula (1). The value per Ni atom at room tempermeff = (8cMT)1/2 (1) Fig. 5 Plot of eVective magnetic moment versus T for complex 3, in the range 78–300 K; j represents the experimental data and the solid line the best fit of the data. ature is 2.88 mB and it decreases gradually with decreasing temperature, indicative of an antiferromagnetic exchange.The best fit of the values was obtained with the Heisenberg– Dirac–van Vleck (HDVV) theoretical model for two exchangecoupled nickel(II) ions in the absence of orbital degeneracy of the complex ground states. The spin Hamiltonian has the form (2) where J is the isotropic exchange coupling, g the isotropic g H = 22JS1S2 1 gbH(S1z 1 S2z) (2) factor and S are the spins of the exchange coupled ions (in this case S1 = S2 = 2). The calculation of the theoretical meff values and the least squares treatment were carried out as reported.29 The best fit values are 22J = 54 cm21, g = 2.2 which are within the usual range expected for binuclear nickel(II) complexes, showing antiferromagnetic exchange.The amount of paramagnetic impurity is negligible within experimental error. The eVective magnetic moments of complex 4 versus temperature are shown in Fig. 6. The temperature dependency first increases with decreasing temperature and then passes through a maximum at 19 K, clearly indicating the existence of ferromagnetic exchange between the Ni atoms. The experimental results were fitted using eqn. (3). The isotropic spin Hamiltonian c = (1 2 a)cdim 1 amon 1 Na (3) has the form (4) where a is the molar fraction of magnetic H = 22JS1S2 2 2zJMs ·SzÒ (4) Fig. 6 Plot of eVective magnetic moment versus T for complex 4, in the range 5–300 K.Details as in Fig. 5.2216 J. Chem. Soc., Dalton Trans., 1999, 2211–2217 Table 6 Crystal data and details of refinement for complexes 1–4 1 2 3 4 Formula M Crystal system Space group a/Å b/Å c/Å a/8 b/8 g/8 V/Å3 T/K Crystal size/mm Z m/cm21 Reflections collected No. unique reflections RR 9 C33H29MnN7O4 642.57 Monoclinic C2/c 18.528(1) 12.783(7) 14.274(1) — 112.36(5) — 3126.7(5) 296(2) 0.40 × 0.25 × 0.25 4 4.51 2982 2884 (Rint = 0.096) 0.061 0.050 C33H29CoN7O4 646.60 Monoclinic P21/n 14.315(8) 13.67(1) 16.126(5) — 106.82(3) — 3021(5) 296(2) 0.30 × 0.30 × 0.30 4 6.15 5810 5572 (Rint = 0.134) 0.043 0.043 C47H38Cl2N10Ni2O8 1059.19 Triclinic P1� 12.739(3) 14.266(3) 14.699(3) 77.00(3) 84.61(3) 63.04(3) 2139.9(9) 293(2) 0.40 × 0.22 × 0.10 2 9.93 3603 3391 (Rint = 0.0161) 0.036 0.036 C28.5H31ClN6NiO6 647.75 Monoclinic C2/c 20.993(4) 20.649(4) 16.821(3) — 122.32(2) — 6162(2) 293(2) 0.40 × 0.30 × 0.20 8 2.135 2791 2791 0.123 0.124 impurities, Na refers to the temperature-independent paramagnetism (250 × 1026 cm3 mol21 per NiII) and 2zJMs ·SzÒ describes the interbinuclear interaction;30 S are the spins of the exchange coupled ions (in this case S1 = S2 = 1 without zero- field splitting for the binuclear complex).The values of the parameters obtained from non-linear fits of the experimental data by eqn. (3) are 22J = 2.55 and g = 2.0, and agree fairly well with previous results for ferromagnetic exchange between nickel(II) ions.31 While antiferromagnetic interaction in binuclear nickel(II) complexes is often observed, the presence of a ferromagnetic exchange is quite unusual 31 and shows the very diVerent exchange mechanism between 3 and 4.This is in accordance with the very diVerent environments around the nickel atoms in the two cases. Conclusion The electrochemical synthetic methodology has been shown to be a new and simple way to prepare first row transition neutral metal(II) complexes of hydrazone ligands with high purity and good yield. The same reaction conditions lead to complexes of diVerent nuclearity (mononuclear and binuclear), suggesting that Ni has a low preference for a pentagonal bipyramidal geometry.It thus seems that the central ion plays a more important role in producing helicates than the ligand itself. Previous results seemed to indicate that the presence of a good donor solvent could break the pyridine bridges in a double helical complex to give rise to monomeric compounds with a co-ordination number of seven.The reaction mechanism must be more complicated as the presence of pyridine is not able to convert helicate 3 into the expected monomer. The addition of pyridine does indeed break the pyridine bridges, as predicted, but rather than producing the expected monomer it yields another binuclear compound. As a result, it appears that we must think about new reasons to explain which variables really favour the production of helicates and what are the reasons for retention of the helicate structure in some hydrazone complexes in the presence of strong donors.Experimental Chemicals All solvents, 2,6-diacetylpyridine and salicylhydrazide are commercially available and were used without further purifi- cation. Metals (Ega Chemie) were used as ca. 2 × 2 cm2 plates. Physical measurements Elemental analyses were performed on a Carlo Erba EA 1108 analyser.The NMR spectra were recorded on a Bruker WM- 250 spectrometer using DMSO-d6 as solvent, infrared spectra as KBr pellets on a Bio-Rad FTS 135 spectrophotometer in the range 4000–600 cm21 and fast atom bombardment (FAB) mass spectra on a Kratos MS-50 mass spectrometer, employing Xe atoms at 70 keV in m-nitrobenzyl alcohol as a matrix. Room-temperature magnetic susceptibilities were measured using a Digital Measurement system MSB-MKI, calibrated using tetrakis(isothiocyanato)cobaltate(II).Measurements of the binuclear nickel complexes were taken by the Faraday technique in the range 78–289 K for 3 and in a SQUID using an applied field of 5000 G in the range 5–300 K for 4. Ligand preparation The ligand H4daps was prepared as previously described.2 Its purity was checked by elemental analyses, 1H NMR and IR spectroscopy. The yield was almost quantitative (Found: C, 64.1; H, 4.8; N, 16.1. Calc. for C23H21N5O4: C, 64.0; H, 4.9; N, 16.2%). 1H NMR (DMSO-d6): d 2.50 (s, 6 H), 6.97–8.17 (m, 11 H), 11.51 (s, br, 2 H) and 11.80 (br, 2 H). Syntheses of the complexes The compounds were obtained using an electrochemical procedure. 17,32 An acetonitrile solution of the ligand containing about 10 mg of tetramethylammonium perchlorate, as supporting electrolyte, was electrolysed using a platinum wire as the cathode and a metal plate as the anode. The cell can be summarised as: Pt(2)|H4daps 1 MeCN|M(1), where M stands for the metal.The synthesis is typified by the preparation of Ni2(H2daps)2(H2O)1.5(CH3CN). A suspension (0.2 g, 0.464 mmol) of the ligand in acetonitrile (80 cm3), containing 10 mg of tetramethylammonium perchlorate, was electrolysed for 2.5 h using a current of 10 mA. Concentration of the resulting solution to a third of its initial volume yielded a yellow-brown solid that was washed with diethyl ether and dried under vacuum. Crystallisation from dichloromethane–hexane produced dark red crystals of [Ni2(H2daps)2]?CH2Cl2, suitable for X-ray diVraction.Slow evaporation of pyridine–dichloromethane solutions containing Mn(H2daps)(H2O)0.5, Co(H2daps)(H2O)1.5(CH3CN) and [Ni2(H2daps)2]?CH2Cl2 yielded crystals of [Mn(H2daps)- (py)2], [Co(H2daps)(py)2] and [Ni2(H2daps)2(py)2]?CH2Cl2, respectively, suitable for X-ray diVraction. Crystallographic measurements Crystal data and details of refinement are given in Table 6 for all the structures.J. Chem. Soc., Dalton Trans., 1999, 2211–2217 2217 [Mn(H2daps)(py)2] 1 and [Co(H2daps)(py)2] 2.Data were collected using an Enraf-Nonius CAD-4 diVractometer for complex 1 and a Rigaku AFC6S diVractometer for 2. The structures were solved by direct methods 33 and refined by fullmatrix least squares on F2. Lorentz-polarisation corrections were applied. Hydrogen atoms attached to oxygen ats were located in the Fourier map and isotropically refined. All calculations were performed using the TEXSAN crystallographic software package.34 [Ni2(H2daps)2]?CH2Cl2 3.Data were collected using a CAD-4 diVractometer. The structure was solved by direct methods and refined using Fourier techniques. Hydrogen atoms attached to oxygen atoms were located. Data processing and computation were carried out by using the SHELXL 97 program package.35 [Ni2(H2daps)2(py)2]?CH2Cl2 4. Data were collected using a Nicolet P-3 diVractometer. The crystals were extremely unstable under X-ray irradiation and we were unable to prevent decomposition (standards decay = 51%).This is the reason for the rather poor resolution of the structure. The structure was solved by direct methods33a and refined using Fourier techniques.36 CCDC reference number 186/1458. See http://www.rsc.org/suppdata/dt/1999/2211/ for crystallographic files in .cif format. 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