Nathalie
Boubals
b,
Michael G. B.
Drew
*a,
Clément
Hill
b,
Michael J.
Hudson
a,
Peter B.
Iveson
a,
Charles
Madic
b,
Mark L.
Russell
a and
Tristan G. A.
Youngs
a
aDepartment of Chemistry, University of Reading, Whiteknights, Reading, UK RG6 6AD. E-mail: m.g.b.drew@reading.ac.uk
bCommissariat à l'Energie Atomique, Valrhô, DEN/DRCP/SCPS/LCSE, Bât 399, B.P. 17171, 30207, Bagnols-sur-Cèze, Cedex, France
First published on 3rd December 2001
4-Amino-bis(2,6-(2-pyridyl))-1,3,5-triazine L4 and several, amide derivatives with hydrophobic alkyl substituents have been synthesised. Solvent extraction studies carried out on Am(III) and Eu(III) with L4 and its amide derivatives in synergistic combination with α-bromodecanoic acid, show that these ligands can selectively extract actinides with respect to lanthanides. The structures of [H2L4]·2Cl·2.5H2O and two amide derivatives have been determined and show respectively the trans, trans; cis, cis; and cis, trans conformations of the adjacent aromatic rings. These observed conformations are in agreement with the results of quantum mechanics calculations on L4 and its protonated derivatives. The structures of two Yb complexes with amide derivatives are also reported with stoichiometry [Yb(L)(NO3)(H2O)4]·2NO3·0.5H2O and [Yb(L)(NO3)3(H2O)]·2MeCN and show the metal in 9 coordinate environments.
For many years we have been designing and testing ligands for the co-extraction2,3 of lanthanides and actinides from nuclear waste and their subsequent separation.4,5 Oligoamines such as 2,2′:6′2″-terpyridine4–6 (L1) and 2,4,6-tris(2-pyridyl)-1,3,5-triazine5 (L2) have been shown to selectively extract actinides in preference to the lanthanides from nitric acid solutions into an organic phase. For extraction it proved necessary to use these ligands in synergistic combination with α-bromodecanoic acid. Separation factors for Am(III) relative to Eu(III) were found to be around 7 and 10 for L1 and L2 respectively.5 Although a separation factor of around 12 can be obtained with a more hydrophobic derivative of L2 (2,4,6-tris(4-tert-butyl-2-pyridyl)-1,3,5-triazine (L3), the synthesis is difficult and the ligand can only be prepared on a small scale. The promising solvent extraction results obtained with L2 and L3 led us to the synthesis of 4-amino-bis(2,6-(2-pyridyl))-1,3,5-triazine (L4). This ligand contains the same major binding cavity as L2 but is much more easily functionalised to prepare the appropriate hydrophobic derivatives. In this study, several new amide derivatives of L4 have been prepared containing either 2,2,4-trimethyl-1-pentyl (L5), 2,2-dimethyl-1-propyl (L6), cyclohexyl (L7), or heptyl (L8) as the hydrophobic alkyl substituent (Fig. 1). The Am(III)/Eu(III) separation–extraction performance of L4, L5, L7 and L8 was measured in combination with α-bromodecanoic acid. The structures of a bis hydrochloride salt of L4 and of the free ligands L5 3,5,5-trimethylhexanoylamino-bis(2,6-(2-pyridyl)-1,3,5-triazine) and L7 (4-cyclohexanoylamino-bis(2,6-(2-pyridyl))-1,3,5-triazine) together with the corresponding Yb(III) complexes of L6 and L7 were also determined.
Fig. 1 Structures of ligands. |
The distribution ratio DM for a metallic cation M is defined as the ratio of the concentration of the metallic species in the organic phase at equilibrium over its concentration in the aqueous phase at equilibrium. The error of the measure of DM (M = Am(III) or Eu(III)) was estimated to be within 5%. The separation factor SFM1/M2 for two metallic cations M1 and M2 is defined as the ratio of their distribution ratios. The error of the determination of SFAm/Eu was estimated to be 7%.
Compound | [H2L4]·2Cl·2.5H2O | L7 | L5·2H2O | [Yb(L7)(NO3)(H2O)4]·2NO3·0.5H2O | [Yb(L6)(NO3)3(H2O)]·2MeCN | |
Empirical formula | C13H17Cl2N6O2.5 | C20H20N6O | C22H29N6O3 | C20H29N9O14.5Yb | C24H28N11O10Yb | |
Formula weight | 368.23 | 360.42 | 425.51 | 800.56 | 803.61 | |
Temperature/K | 293(2) | 293(2) | 293(2) | 293(2) | 293(2) | |
Crystal system, space group | Triclinic, P | Monoclinic, P21/c | Monoclinic, P21/a | Monoclinic, C2/c | Monoclinic, C2/c | |
a/Å | 10.158(12) | 9.946(12) | 12.458(14) | 24.35(3) | 8.935(14) | |
b/Å | 13.890(15) | 17.15(2) | 14.997(17) | 16.760(18) | 12.887(14) | |
c/Å | 14.249(15) | 11.849(14) | 12.515(14) | 14.812(17) | 15.004(17) | |
α/° | 69.20(1) | (90) | (90) | (90) | 71.69(1) | |
β/° | 67.61(1) | 109.12(1) | 93.54(1) | 103.49(1) | 87.14(1) | |
γ/° | 71.60(1) | (90) | (90) | (90) | 78.96(1) | |
Volume/Å3 | 1699 | 1910 | 2334 | 5878 | 1610 | |
Z, Calculated density/Mg m−3 | 2, 1.439 | 4, 1.254 | 4, 1.211 | 4, 1.809 | 2, 1.658 | |
Absorption coefficient/mm−1 | 0.404 | 0.082 | 0.083 | 3.266 | 2.974 | |
F(000) | 764 | 760 | 908 | 3184 | 798 | |
Reflections collected | 5890 | 6387 | 7430 | 6980 | 5198 | |
Unique reflections/Rint | 5890 | 3383/0.0310 | 4416/0.0761 | 4420/0.0762 | 5198 | |
Data/restraints/parameters | 5890/15/457 | 3383/0/245 | 4416/4/297 | 4420/0/190 | 4198/2/428 | |
Final R indices [I > 2σ(I)] | R1 | 0.0479 | 0.0844 | 0.0920 | 0.1119 | 0.0296 |
wR2 | 0.1284 | 0.2336 | 0.2439 | 0.2809 | 0.0712 | |
R indices (all data) | R1 | 0.0722 | 0.1544 | 0.2214 | 0.2547 | 0.0367 |
wR2 | 0.1419 | 0.2846 | 0.3061 | 0.3363 | 0.0755 | |
Largest diff. peak and hole/e Å−3 | 0.260, −0.272 | 0.360, −0.233 | 0.697, −0.277 | 3.540, −1.922 | 0.997, −1.596 |
In the structure of the salt [H2L4]·2Cl·2.5H2O, there are two formula units in the asymmetric unit. All the hydrogen atoms on the water molecules were located in a difference Fourier map and included in the refinement with distance constraints. The structure of L7 contained no solvent. L5 contained two water molecules in the asymmetric unit but the hydrogen atoms on these solvent molecules were not located. For [Yb(L7)(NO3)(H2O)4]·2NO3·0.5H2O the hydrogen atoms on the water molecules were not located. The data were of poor quality and only the metal atom was refined anisotropically. For [Yb(L6)(NO3)3(H2O)]·2MeCN the hydrogen atoms on the water molecules were located and refined with distance constraints. All structures were refined on F2 till convergence using SHELXL.11
CCDC reference numbers 172878–172882.
See http://www.rsc.org/suppdata/dt/b1/b104181a/ for crystallographic data in CIF or other electronic format.
M3+ + 3αBrC10 + L ⇌ ML(αBrC10)3 + 3H+ |
We have studied the synergistic extraction of Am(III) and Eu(III) by combining ligands L4, L5, L7 or L8 with α-bromodecanoic acid, used here as a cationic exchanger. The replacement of nitrate anions by α-bromodecanoate anions enhances the extraction of [ML]3+ complexes in TPH. The results of these experiments are summarised in Table 2 together with the results related to ligands L2 and L3 and are also shown in Fig. 2 for ligands L4 and L5, and Fig. 3 for ligands L7 and L8, respectively.
Ligand | [HNO3]eq | D Eu(III) | D Am(III) | SFAm/Eu |
---|---|---|---|---|
a Organic solution: [αBrC10]initial = 1 M, [L]initial = 0.02 mol L−1, TPH. Aqueous solution: [HNO3]initial = variable, T = 22 °C. | ||||
L1 | 0.03 | 2.8 | 27 | 9.5 |
0.05 | 0.3 | 3.5 | 10 | |
0.08 | 0.09 | 0.8 | 9 | |
0.11 | 0.03 | 0.3 | 9 | |
L2 | 0.03 | 8.7 | 124 | 14 |
0.05 | 0.9 | 12 | 14 | |
0.08 | 0.2 | 2.1 | 11 | |
0.11 | 0.08 | 0.8 | 9 | |
L4 | 0.03 | 4.6 | 45 | 9.5 |
0.05 | 0.5 | 5.5 | 10 | |
0.08 | 0.08 | 0.7 | 9.5 | |
0.11 | 0.02 | 0.2 | 11.5 | |
L5 | 0.02 | 2.2 | 14 | 6.5 |
0.04 | 0.5 | 4.8 | 9.5 | |
0.06 | 0.12 | 1.1 | 9 | |
0.09 | 0.04 | 0.39 | 9 | |
0.13 | 0.02 | 0.21 | 9 | |
L7 | 0.03 | 2.2 | 24 | 11 |
0.05 | 0.24 | 2.8 | 12 | |
0.10 | 0.04 | 0.4 | 10 | |
L8 | 0.03 | 2.4 | 19 | 8 |
0.06 | 0.3 | 3.5 | 12 | |
0.10 | 0.03 | 0.4 | 12 |
Fig. 2 Am(III) and Eu(III) extraction by L4 and L5 in a synergistic mixture with α-bromodecanoic acid. Organic solution: [αBrC10]initial = 1 M, [L]initial = 0.02 mol L−1, TPH. Aqueous solution: [HNO3]initial = variable, T = 22 °C. The symbols denote each measurement of DM. The approximately horizontal lines represent calculated SF values. |
Fig. 3 Am(III) and Eu(III) extraction by L7 and L8 in a synergistic mixture with α-bromodecanoic acid. Organic solution: [αBrC10]initial = 1 M, [L]initial = 0.02 mol L−1, TPH. Aqueous solution: [HNO3]initial = variable, T = 22 °C. The symbols denote each measurement of DM. The approximately horizontal lines represent calculated SF values. |
Although not as efficient as ligand L2, ligands L4, L5, L7 and L8 appeared to be as efficient as ligand L1 when used in a synergistic mixture with α-bromodecanoic acid for the extraction of Am(III) and its separation from Eu(III). For the three rather hydrophobic substituted ligands L5, L7 and L8, the log–log plots of the experimental DM values vs. [HNO3]eq fitted well with a linear regression. The slope of which was close to −3, in agreement with the above proposed extraction equilibrium. However, for the non-substituted ligand L4, the log–log plots of the experimental DM values vs. [HNO3]eq were better fitted with a linear regression, the slope of which is close to −4, possibly because of the redistribution of this rather hydrophilic ligand in the aqueous acidic phase after protonation (i.e.: [HNO3]eq ≥ 0.08 M).
Symmetry elements. For [H2L4]·2Cl·2.5H2O: $1 x, y, 1 + z; $2 1 − x, 1 − y, −z; $3 −x − 1, 2 − y, −z; $4 −x − 1, 2 − y, 1 − z. For L7: $1 x, 0.5 − y, 0.5 + z. For L5·2H2O: $3 0.5 + x, 0.5 − y, z; $6 2.5 − x, 0.5 + y, 1 − z; $7 x + 0.5, 0.5 − y, z − 1. For [Yb(L7)(NO3)(H2O)4]·2NO3·0.5H2O: $1 x, 1 − y, z − .5; $2 0.5 − x, 0.5 − y, 1 − z; $4 1 − x, y, 0.5 − z; $5 1 − x, 1 − y, 1 − z; $6 x, 1 − y, 0.5 + z. For [Yb(L6)(NO3)3]·2MeCN: $4 1 − x, 1 − y, −z; $5 x + 1, y, z. | |||
---|---|---|---|
[H2L4]·2Cl·2.5H2O | |||
O(100)⋯Cl(1) | 3.15 | N(11B)⋯O(101)$3 | 2.69 |
O(100)⋯Cl(2)$2 | 3.11 | N(11B)⋯N(25B) | 2.70 |
O(101)⋯Cl(3) | 3.17 | N(27A)⋯O(100)$2 | 2.84 |
O(101)⋯Cl(4)$4 | 3.14 | N(27A)⋯Cl(1) | 3.26 |
O(102)⋯Cl(1) | 3.07 | N(27B)⋯Cl(3)$3 | 3.33 |
O(103)⋯Cl(3) | 3.21 | N(27B)⋯Cl(3) | 3.34 |
O(103)⋯Cl(4) | 3.21 | N(31A)⋯O(102) | 2.68 |
O(104)⋯Cl(4) | 3.13 | N(31A)⋯N(23A) | 2.72 |
O(104)⋯Cl(2)$1 | 3.11 | N(31B)⋯O(103) | 2.69 |
N(11A)⋯N(25A) | 2.71 | N(31B)⋯N(23B) | 2.69 |
N(11A)⋯Cl(2) | 3.09 | ||
L7 | |||
N(41)⋯N(11)$1 | 3.00 | ||
L5·2H2O | |||
N(11)⋯N(41)$3 | 2.94 | O(100)⋯O(200)$7 | 2.91 |
O(43)⋯O(200) | 2.79 | O(100)⋯O(200)$6 | 2.96 |
O(200)⋯N(31) | 2.84 | ||
[Yb(L7)(NO3)(H2O)4]·2NO3·0.5H2O | |||
O(100)⋯O(61)$4 | 2.79 | O(102)⋯O(64)$5 | 2.67 |
O(100)⋯O(62)$4 | 2.96 | O(102)⋯O(51)$1 | 2.86 |
O(101)⋯O(44)$6 | 2.97 | N(41)⋯O(54)$2 | 2.82 |
O(101)⋯O(61)$5 | 3.07 | ||
[Yb(L6)(NO3)3]·2MeCN | |||
O(100)⋯N(500)$5 | 2.76 | N(41)⋯N(400)$4 | 3.14 |
Fig. 4 The structure of the [H2L4]2+ cation A showing the hydrogen bond pattern (dotted lines). Ellipsoids at 30% probability. |
Fig. 5 The structure of the [H2L4]2+ cation B showing the hydrogen bond pattern (dotted lines). Ellipsoids at 30% probability. |
The structure of L7 is shown in Fig. 6. There is one strong hydrogen bond between N(41) and N(11) (x, 0.5 − y, 0.5 + z) with an N⋯N distance of 3.00 Å. The arrangement of the three nitrogen atoms is cis, cis (cc). On the other hand, the structure of L5·2H2O exhibits the ligand in the ct conformation as shown in Fig. 7. A water molecule O(200) forms donor hydrogen bonds to both N(31) at 2.84(1) and O(43) at 2.79(1) Å. The second water molecule in the asymmetric unit (not shown in the Figure) forms two hydrogen bonds to O(200) but not to L5. In addition N(11) forms an intermolecular hydrogen bond to N(41) (5 + x, 0.5 − y, z) at 2.94 Å.
Fig. 6 The structure of L7 with ellipsoids at 30% probability. |
Fig. 7 The structure of L5·2H2O with ellipsoids at 30% probability. One water molecule, present in the asymmetric unit, is not shown. |
The fact that L5 is in the ct conformation and L7 is in the cc conformation (and indeed that [H2L4]2+ is in the tt conformation) is particularly interesting. Our theoretical calculations on the parent amine (see below) show that there are only small energy differences between these three conformations, much lower than is found for ligands (e.g. 2,2′:6′2″-terpyridine (L1))6 with a central pyridine ring. The energy barrier between conformations is also likely to be much lower in these ligands containing a central triazine ring than in those containing a central pyridine ring where the ortho-hydrogen atoms on adjacent rings restrict rotation.
The structure of the [Yb(L7)(NO3)(H2O)4]2+ cation is shown in Fig. 8. There are two nitrate anions together with a disordered water molecule in the asymmetric unit. The structure of the cation shows the Yb to be in a 9-coordinate environment with the metal bond lengths shown in Table 4, together with the atomic numbering scheme. The water molecules show the shortest bonds although there is significant variation [2.29(2)–2.39(2) Å] but in addition, each of them forms two strong hydrogen bonds with adjacent non-coordinated nitrate anions. This formation of a doubly charged ionic complex containing a lanthanide with only one nitrate ion is unique and is not found in any of the 100 or so structures that we have determined of lanthanide nitrate complexes with terdentate nitrogen ligands.4,6,15 The bond to the central triazine nitrogen atom Yb(1)–N(21) is at 2.39(2) Å much shorter than the bonds to the outer pyridine nitrogen atoms (Yb(1)–N(31) 2.52(2), Yb(1)–N(11) 2.57(2) Å). The amide N–H group is hydrogen bonded to a nitrate oxygen atom (which is not bonded to the metal) from an adjacent molecule, viz (N(41)⋯O(54) (0.5 − x, 0.5 − y, 1 − z), 2.84 Å. There are many hydrogen bonds (Table 3) between the coordinated water molecules and nitrates in adjacent molecules.
[Yb(L7)(NO3)(H2O)4]·2NO3·0.5H2O | |||
Yb(1)–O(102) | 2.290(16) | Yb(1)–O(42) | 2.437(19) |
Yb(1)–O(101) | 2.313(15) | Yb(1)–N(31) | 2.52(2) |
Yb(1)–O(103) | 2.385(18) | Yb(1)–O(41) | 2.548(18) |
Yb(1)–N(21) | 2.39(2) | Yb(1)–N(11) | 2.57(2) |
Yb(1)–O(100) | 2.398(16) | ||
[Yb(L6)(NO3)3(H2O)]·2MeCN | |||
Yb(1)–O(41) | 2.277(4) | Yb(1)–N(21) | 2.419(4) |
Yb(1)–O(100) | 2.298(4) | Yb(1)–O(52) | 2.470(4) |
Yb(1)–O(51) | 2.362(4) | Yb(1)–N(11) | 2.489(5) |
Yb(1)–O(61) | 2.400(4) | Yb(1)–N(31) | 2.519(5) |
Yb(1)–O(62) | 2.404(4) |
Fig. 8 The structure of the [Yb(L7)(NO3)(H2O)4]2+ cation with the atomic numbering scheme. Ellipsoids at 30% probability. Hydrogen atoms on the water molecules could not be located and are not shown. |
This structural type, [Yb(L7)(NO3)(H2O)4]2+, is different from the two types obtained previously for Yb(III) and L4 as in [Yb(L4)(NO3)2(H2O)2], [NO3], Yb is coordinated to one tridentate L4 ligand, two bidentate nitrates and two water molecules and in [Yb(L4)(NO3)3(H2O)], Yb is coordinated to one L4, two bidentate nitrates, one monodentate nitrate and one water molecule.15 The latter structure is similar to that of [Yb(L6)(NO3)3(H2O)] which is shown in Fig. 9. This structure also contains two solvent acetonitrile groups in the asymmetric unit. This structure is also 9-coordinate as one of the nitrate anions is monodentate. As is usually the case, the shortest Yb–O bond is to the monodentate nitrate Yb(1)–O(41) 2.277(4) Å, followed by the bond to the water molecule Yb(1)–O(100) 2.298(4) Å. The next shortest bonds are those to the bidentate nitrate although the bond to O(52) at 2.470(4) Å is significantly longer than the other three (2.362(4), 2.400(4), 2.404(4) Å). As was found for [Yb(L7)(NO3)(H2O)4]·2NO3·0.5H2O, the bond to the triazine nitrogen atom is, at 2.419(4) Å, significantly shorter than the bonds to the other nitrogen atoms (2.489(5), 2.519(5) Å). The amide nitrogen atom in this case is hydrogen bonded to a solvent acetonitrile molecule (N(41)⋯N(400) (1 − x, 1 − y, −z) 3.14 Å).
Fig. 9 The structure of the [Yb(L6)(NO3)3(H2O)] complex with ellipsoids at 30% probability. One of the two solvent acetonitrile molecules is shown. |
We ascribe no particular significance to the difference in stoichiometry between the two metal complexes of Yb with L6 and L7. In previous work we have shown that there can be very different coordination geometries for specific metals with these planar terdentate ligands and it seems likely that the replacement of one bidentate and one monodentate nitrate by three water molecules is not unusual and that both structures together with others are likely to co-exist in solution. The only thing in common is that in both cases the metal cations are 9-coordinate as is usually found for ytterbium. It is likely that with these ligands the smaller lanthanides are 9-coordinate and have the form [ML(NO3)n(H2O)m]p+ with n = 1, 2 or 3; m = 6 − 2n + x, where x is the number of monodentate nitrates. General structural trends show that the number of monodentate nitrates will be either 1 or 0, and that at least one bidentate nitrate will be coordinated so that the charge p on the complex is 0, 1 or 2. It can also be considered that there are several different entities for the complexes in solution.
It is interesting to note that 2,6-bis(5,6-dipropyl-1,2,4-triazin-3-yl)pyridine which provides a separation ratio for An/Ln of greater than 100,16 when used without a synergist, forms the 1 ∶ 3 complex in the presence of nitrate with the smaller lanthanides (Sm–Lu)17 but not for the larger lanthanides (La–Sm).18 This suggests that ligands that always form 1 ∶ 1 complexes are not likely to give high separation ratios in the absence of a synergist. While we have only determined crystal structures with Yb and not the other lanthanides, all indications from previously obtained structural information2,4,15 is that when Yb forms 1 ∶ 1 complexes with particular ligands then so do the other lanthanides and therefore we conclude that these ligands do not form 1 ∶ 3 complexes with any lanthanide. Another factor that may lessen the usefulness of L4 and derivatives is that they always form hydrogen bonds with either solvent molecules or other metal complexes, a feature not present in the ML33+ complex of 2,6-bis(5,6-dipropyl-1,2,4-triazin-3-yl)pyridine, which has a hydrophobic exterior. The propensity for hydrogen bond formation as indicated by Table 3 is widespread in all the crystal structures for ligands and metal complexes alike and the aggregation of molecules may occur in solution to prevent efficient extraction.
Conformation | Protonated nitrogen | cc | ct | tt |
---|---|---|---|---|
L4 | 2.36 | 0.00 | 0.49 | |
L2 | 12.55 | 6.90 | 0.00 | |
[HL4]+ | N(11) | 9.77 | 14.67 | 14.55 |
N(31) | N(11) | 12.22 | N(11) | |
N(21) | 0.00 | 10.13 | 22.19 | |
N(25) | 28.98 | 27.07 | 14.55 | |
N(23) | N(25) | 14.05 | N(25) | |
N(27) | 51.10 | 46.15 | 44.38 | |
[H2L4]2+ | N(11), N(21) | 24.35 | 40.53 | 34.20 |
N(11), N(31) | 5.37 | 1.79 | 0.00 | |
N(11), N(25) | 33.99 | 39.75 | 45.83 | |
N(11), N(23) | 24.55 | 14.18 | 13.82 | |
N(11), N(27) | 41.70 | 44.15 | 45.70 | |
N(21), N(23) | N(21), N(25) | 34.00 | N(21), N(25) | |
N(21), N(25) | 37.82 | 50.57 | 49.71 | |
N(21), N(27) | 50.98 | 60.49 | 73.44 | |
N(21), N(31) | N(11), N(21) | 18.52 | N(11), N(21) | |
N(25), N(31) | N(11), N(23) | 26.33 | N(11), N(23) | |
N(23), N(25) | 69.04 | 51.03 | 35.82 | |
N(23), N(27) | N(25), N(27) | 91.29 | N(25), N(27) |
We then investigated the possible structures of [HL4]+ cations. Given that N(11) and N(31) are equivalent as indeed are N(25) and N(23) in cc and tt conformations we constructed 14 different structures, combinations of the nitrogen to be protonated and the three possible conformations. The cc conformation with N(21) protonated was ca. 10 kcal mol−1 lower in energy than all the others. The relative stability of this configuration is probably due to a combination of factors, N(21) is the preferred nitrogen to be protonated, and also it can form weak hydrogen bonds to the ortho nitrogen atoms in the terminal pyridine rings. In addition, there are no steric repulsions owing to adjacent ortho hydrogen atoms. The next most favourable configuration is the cc conformation with N(11) protonated but this only forms one weak intramolecular hydrogen bond. The ct conformation with N(21) protonated is disfavoured owing to repulsion between ortho hydrogen atoms on N(21) and C(33). It is interesting that in this case (and in others) the presence of two mutually ortho-hydrogen atoms leads to a twist in the rings of ca. 33–46° leading to a loss of conjugation. The highest energies (>44 kcal mol−1) occur with N(27) protonated even though this does not lead to increased steric repulsions so that these energies must be due to the unfavourable nature of protonation at that atom.
Results for [H2L4]2+ are less clear cut and show three configurations with comparable low energies within 5.4 kcal mol−1, all with N(11) and N(31) protonated. The lowest energy configuration has the tt conformation in which there are two weak hydrogen bonds formed between N(11)–H⋯N(25) and N(31)–H⋯N(23) and no ortho⋯ortho interactions. This is the structure found in the crystal structure of [H2L4]·2Cl·2.5H2O (Figs. 4 and 5) where the configuration is further stabilized by intermolecular hydrogen bonds. The other conformations ct and cc also have low energies. With a cis conformation the pyridine nitrogen atom N(11) and/or N(31) can form hydrogen bonds to the central nitrogen atom N(21) but again there are no undesirable ortho⋯ortho interactions. All other configurations have an energy of 13.8 kcal mol−1 greater than the minimum. There are several features that can be discerned from the energy distribution. Unlike in [HL4]+ protonation of N(21) is not favourable, because the second proton, wherever placed, always leads to ortho⋯ortho intramolecular interactions unless it is situated on N(27) which is an unfavourable site. Protonation on N(25) {or N(23)} is favourable in the trans conformation because it gives rise to N(25)–H⋯N(11) or {N(23)–H⋯N(31)} interactions but not in the cis conformation because of ortho⋯ortho interactions which lead to rotation of the rings. An intermediate situation arises in configurations such as the cis conformation with N(11) protonated where there is a weak hydrogen bond between N(11)–H and N(21). However, a repulsion between N(25)–H and C(13)–H, which is resolved via an intermediate rotation of 20° compared to the ca. 40°, found where there is no such hydrogen bond formation. We can draw the overall conclusion that the order of preference for protonation is N(11) > N(21) > N(25) > N(27) but that this order can be varied according to which other nitrogen atoms are protonated and the presence of solvent which can lead to intramolecular hydrogen bonds. The energy barrier to rotation between cis and trans in L4 with a central triazine ring is far less than that observed with a central pyridine ring as in terpy where ortho⋯ortho hydrogen interactions provide a high energy barrier.
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