Open Access Article
Edwin C.
Constable
*a,
Catherine E.
Housecroft
*a,
Srboljub
Vujovic
a,
Jennifer A.
Zampese
a,
Aurélien
Crochet
b and
Stuart R.
Batten
c
aDepartment of Chemistry, University of Basel, Spitalstrasse 51, CH-4056 Basel, Switzerland. E-mail: catherine.housecroft@unibas.ch; Fax: +41 61 267 1018; Tel: +41 61 267 1008
bDepartment of Physics, University of Fribourg, Chemin du Musée 3, CH-1700 Fribourg, Switzerland. E-mail: aurelien.crochet@unifr.ch
cSchool of Chemistry, Monash University, Victoria 3800, Australia. E-mail: stuart.batten@monash.edu
First published on 24th October 2013
The consequences for the structures of coordination polymers of introducing fluoro substituents into the terminal phenyl domain of 4′-(biphenyl-4-yl)-4,2′:6′,4′′-terpyridine (1) have been investigated. Reaction between Cu(OAc)2·H2O and 4′-(2′,3′,4′,5′,6′-pentafluorobiphenyl-4-yl)-4,2′:6′,4′′-terpyridine (2) yields the one-dimensional coordination polymer [Cu2(μ-OAc)4(2)]n which contains paddle-wheel {Cu2(OAc)4} nodes bridged by ligands 2. The compound is isostructural with [Cu2(μ-OAc)4(1)]n. When Cu(OAc)2·H2O reacts with a 1
:
1 mixture of 1 and 2, [Cu2(μ-OAc)4(1)]n and [Cu2(μ-OAc)4(2)]n co-crystallize with 1 and 2 disordered over one ligand site; the one-dimensional coordination polymer is isostructural with each of [Cu2(μ-OAc)4(1)]n and [Cu2(μ-OAc)4(2)]n indicating that replacing H by F substituents in the peripheral arene ring has no effect on the overall solid-state structure: tpy⋯tpy π-stacking is preserved, arene⋯arene πH⋯πH interactions are replaced by perfluoroarene⋯arene πF⋯πH interactions, and H⋯H contacts are replaced by H⋯F interactions. In stark contrast to the latter observations, the reaction of Zn(OAc)2·2H2O with perfluoro derivative 2 yields [Zn5(OAc)10(2)4·11H2O]n as the dominant one-dimensional polymer; minor amounts of the anticipated polymer [Zn2(μ-OAc)4(2)]n are also formed. The solid-state structure of [Zn5(OAc)10(2)4·11H2O]n consists of quadruple-stranded polymer chains assembled from {Zn5(2)4} subchains interconnected by {Zn5(OAc)10} units. Within each chain, πF⋯πF and πH⋯πH stacking interactions are dominant, while the observed assembly of chains into sheets and π-stacking between arene units in adjacent sheets mimic the dominant interactions in the single-stranded chains observed in [Zn2(μ-OAc)4(1)]n, [Zn2(μ-OAc)4(2)]n, [Cu2(μ-OAc)4(1)]n, [Cu2(μ-OAc)4(2)]n and [Cu2(μ-OAc)4(1)]n·[Cu2(μ-OAc)4(2)]n.
:
1 co-crystallized mixture. Both C6H62 and C6F63 exhibit edge-to-face CX⋯π interactions (X = H4–6 or F7), while the co-crystallized material has infinite columns of alternating C6D6 and C6F6 molecules which interact through π-stacking interactions.8,9 Molecular assembly directed by such arene⋯perfluoroarene interactions is now well recognized.10,11 A wider perspective has been taken by Hulliger and coworkers who have surveyed the roles played in crystal engineering by phenyl⋯perfluorophenyl (abbreviated as πH⋯πF), CF⋯H, F⋯F and CF⋯πF interactions; they concluded (in 2005) that ‘the role of fluorine in crystal engineering is not yet clear in detail’.12 An update of this picture appeared in 2011, adding CF⋯M+, CF⋯C
O and anion⋯πF contacts to packing interactions in fluorine-containing compounds.13 A study of the packing of partially fluorinated diphenylethynes underlines the importance of phenyl⋯perfluorophenyl stacking but questions the stabilizing effects of CH⋯F and CF⋯F contacts.14 Although πH⋯πF stacking has gained significant attention in crystal engineering and has been utilized to direct host–guest complex formation,15 the coexistence of arene and perfluoroarene rings does not necessarily result in such interactions. Competitive packing motifs may predominate, and hydrogen bonds in particular are favoured over πH⋯πF contacts.13 (The strength of the face-to-face πH⋯πF interaction is ca. 20 to 25 kJ mol−1.11) More subtle factors may also tip the balance. For example, the compounds shown in Scheme 1a crystallize with no face-to-face πH⋯πF interactions.16 In contrast, the molecules of a related 2,2′-bipyridine derivative with X = F (Scheme 1b) pack with πH(py)⋯πF interactions, while co-crystallization of the two compounds in Scheme 1b leads to a crystal lattice containing efficient πH⋯πF contacts.17
![]() | ||
| Scheme 1 (a) Examples of compounds that crystallize with no πH⋯πF stacking interactions and (b) related compounds which when co-crystallized exhibit πH⋯πF contacts. | ||
Surprisingly, the use of phenyl⋯perfluorophenyl interactions to direct the assembly of coordination polymers has received little attention. Two examples with related ligands present contrasting packing motifs, with the presence of an ethyne unit in the first example apparently playing a critical role. Reaction of 1,4-bis(4′-pyridylethynyl)tetrafluorobenzene (Scheme 1a, top) with zinc(II) nitrate results in the formation of a one-dimensional polymer in which zig-zag chains interact with each other through πalkyne⋯πF and πalkyne⋯πpyridine interactions; there is no πH⋯πF stacking.16 The related ligand 1,4-bis(4′-pyridylmethyl)tetrafluorobenzene reacts with Cd(NO3)2 and aniline to give a one-dimensional coordination polymer in which {Cd(NO3)2(C6H5NH2)2} nodes are connected by bridging ligands. In this case, adjacent chains interact through πH⋯πF stacking. However, replacing aniline by 4-bromoaniline turns off the inter-chain πH⋯πF interactions.18
We have recently reported the assembly of coordination polymers containing the functionalized 4,2′:6′,4′′-terpyridine 1 (Scheme 2) and have discussed the role that face-to-face π-stacking of pairs of biphenyl domains and pairs of tpy units plays in the organization of polymers formed in reactions of 1 with Zn(OAc)2·2H2O, Cu(OAc)2·H2O and Cd(OAc)2·2H2O.19 We now report the preparation of compound 2 and investigate the structural consequences of introducing the perfluorophenyl domain. The coordination behaviour of 2 with Cu(OAc)2 and Zn(OAc)2 is described, along with the effect of treating Cu(OAc)2 with a 1
:
1 mixture of ligands 1 and 2.
![]() | ||
| Scheme 2 Ligand structures and numbering for NMR spectroscopic assignments. | ||
2′,3′,4′,5′,6′-Pentafluorobiphenyl-4-carbaldehyde was prepared according to the literature.20
500), 268 (43
100). ESI MS (MeCN) m/z 476.1 [M + H]+ (calc. 476.1). Found: C 67.52, H 3.26, N 8.55; C27H14F5N3 requires C 68.21, H 2.97, N 8.84%.
280 reflections, 3453 unique, Rint = 0.0281. Refinement of 3414 reflections (316 parameters) with I > 2σ(I) converged at final R1 = 0.0293 (R1 all data = 0.0296), wR2 = 0.0777 (wR2 all data = 0.0782), gof = 1.061. CCDC 949634.
388 reflections, 3059 unique, Rint = 0.0417. Refinement of 2718 reflections (322 parameters) with I > 2σ(I) converged at final R1 = 0.0610 (R1 all data = 0.0672), wR2 = 0.1639 (wR2 all data = 0.1696), gof = 1.114. CCDC 949632.
871 reflections, 2950 unique, Rint = 0.0306. Refinement of 2663 reflections (245 parameters) with I > 2σ(I) converged at final R1 = 0.0502 (R1 all data = 0.0541), wR2 = 0.1518 (wR2 all data = 0.1560), gof = 1.125. CCDC 949633.
388 reflections, 20
471 unique, Rint = 0.0445. Refinement of 15
051 reflections (1879 parameters) with I > 2σ(I) converged at final R1 = 0.0683 (R1 all data = 0.0962), wR2 = 0.1802 (wR2 all data = 0.2057), gof = 1023. CCDC 949635.
![]() | ||
| Scheme 3 Synthetic route to compound 2. | ||
![]() | ||
| Fig. 1 Absorption spectra of EtOH solutions of compounds 1 and 2. | ||
Single crystals of 2 were grown from a CHCl3 solution layered with hexane. The compound crystallizes in the monoclinic space group Cc, and the structure is shown in Fig. 2; bond lengths and angles are unexceptional. The tpy domain is close to planar, and the pentafluorophenyl ring also lies approximately in this plane, with the phenylene ring showing a significant twist. Using the ring labelling in Scheme 2, the angles between ring planes are A/B = 9.6 and 6.3°, B/C = 34.9° and C/D = 32.5°; twisting of B/C and C/D pairs of rings minimizes repulsions between ortho substituents on adjacent rings, whether they be H or F atoms. In contrast to 2, compound 1 crystallizes in the space group P21/c with five independent molecules which possess significant differences in conformation.19 Crystal packing in 1 involves π-stacking and CH⋯N interactions. However, the conformational variation among independent molecules precludes a simple packing description. In contrast, slipped πH(py)⋯πF contacts between molecules of 2 result in the assembly of chains which run parallel to the c-axis (Fig. 3a). However, the π interaction is not optimal; the pentafluorophenyl ring lies between two pyridine rings with πF centroid⋯πH(py) centroid distances of 4.24 and 3.88 Å. Packing of adjacent chains involves weak πH(py)⋯πH(arene) and πH(arene)⋯πF contacts (Fig. 3b), but the interplane angles and centroid⋯centroid separations (14.6° with 4.21 Å and 16.3° with 4.63 Å) are outside the limits for efficient interactions. Additional CH⋯N and CH⋯F contacts contribute to the overall packing between the chains. We note that the structure of 4′-pentafluoro-2,2′:6′,2′′-terpyridine has been reported, but the packing has not been discussed.26 Inspection of the structure (CSD27 refcode NAZYOE) shows that the pentafluorophenyl unit is sandwiched between two tpy domains of adjacent molecules, with a stacking interaction with respect to each tpy similar to that in 2.
![]() | ||
| Fig. 2 ORTEP diagram of the structure of 2 (ellipsoids were plotted at the 40% probability level). | ||
![]() | ||
| Fig. 3 Packing interactions in 2: (a) chains following the c-axis with slipped intermolecular πH(py)⋯πF contacts and (b) relatively inefficient π-stacking (space-filling representation) along the a-axis. H and F atoms are shown in white and green, respectively. | ||
In the context of the coordination polymers discussed later in this work, it is significant that the solid-state structures of 1 and 2 differ. We investigated the co-crystallization of 1 and 2 from CH2Cl2/MeOH layered with hexane, but X-ray diffraction analysis of single crystals from these mixtures revealed the growth of separate crystals of 119 and 2, with structures identical to those previously determined.
![]() | ||
| Fig. 4 ORTEP representation of the repeat unit in [Cu2(μ-OAc)4(2)]n (ellipsoids were plotted at the 30% probability level, and H atoms were omitted for clarity). Only one occupancy site of each disordered acetato ligand is shown. Symmetry codes: i = 1 − x, y, 3/2 − z; ii = 1/2 − x, 7/2 − y, 2 − z. Selected bond lengths: Cu1–O1 = 1.799(6), Cu1–O3 = 1.955(6), Cu1–O2ii = 2.030(7), Cu1–O4ii = 2.039(6), Cu1–N1 = 2.186(2), Cu1–Cu1ii = 2.6358(8) Å. | ||
Packing of zig-zag chains in [Cu2(μ-OAc)4(2)]n involves the organization of chains into sheets and π-stacking interactions between arene domains in adjacent sheets. The left-hand part of Fig. 5a illustrates how the pentafluorophenyl unit slots into the V-shaped cavity of a tpy domain of the next chain with short CHmethyl⋯F (2.51 Å) and CHtpy⋯F contacts (2.42 and 2.54 Å). Although attractive in nature, these interactions are apparently not significant in terms of assisting assembly of the chains into sheets since CH⋯F interactions in [Cu2(μ-OAc)4(2)]n are replaced by CH⋯H contacts in [Cu2(μ-OAc)4(1)]n.19 Chains in adjacent sheets in [Cu2(μ-OAc)4(2)]n exhibit the same tpy⋯tpy π interactions (Fig. 5b) that are observed in a number of related structures containing functionalized 4,2′:6′,4′′-terpyridines and {Zn2(μ-OAc)4} or {Cu2(μ-OAc)4} nodes.19,28–30 Pyridine rings with N1 and N2 engage in face-to-face contacts with those containing N1iii and N2iii (symmetry code iii = 1 − x, 3 − y, 2 − z) at a separation of 3.48 Å. These are complemented by head-to-tail stacking of pentafluorobiphenyl domains giving πH⋯πF interactions (Fig. 5a, right-hand side). However, the twist angle of 31.5° between the bonded C6F5 and C6H4 rings reduces the efficiency of the interaction, with the angle between the stacked rings necessarily also being 31.5°.
![]() | ||
| Fig. 5 Packing motifs in [Cu2(μ-OAc)4(2)]n: (a) short CH⋯F contacts shown in red (left) and πH⋯πF interactions shown in space-filling representation (right); (b) tpy⋯tpy π interactions between zig-zag chains. | ||
:
1 mixture of ligands 1 and 2. Elemental analysis of the bulk sample was consistent with an overall stoichiometry of [Cu2(μ-OAc)4(1)]n·[Cu2(μ-OAc)4(2)]n. The product crystallized in the monoclinic C2/c space group with cell dimensions essentially the same as those of [Cu2(μ-OAc)4(1)]n and [Cu2(μ-OAc)4(2)]n. Structural analysis confirmed not only the formation of [Cu2(μ-OAc)4(1)]n·[Cu2(μ-OAc)4(2)]n but also the fact that the asymmetric unit contains the two ligands superimposed; the terminal phenyl/pentafluorophenyl ring is disordered and has been modelled with a 0.5/0.5 site occupancy of each of ligands 1 and 2. An ordered structure with alternating ligands 1 and 2 along the polymer chain would require a bigger unit cell resulting in more observable reflections, but no additional reflections were observed between the original intensities. This confirms that the only meaningful way to describe the structure is with a disordered model. The metrical parameters of the {Cu2(μ-OAc)4} unit in [Cu2(μ-OAc)4(1)]n·[Cu2(μ-OAc)4(2)] (Cu1–O1 = 1.9740(16), Cu1–O3 = 1.974(2), Cu1–O2ii = 1.9599(19), Cu1–O4ii = 1.962(2), Cu1–N1 = 2.1763(19), Cu1–Cu1ii = 2.6326(7) Å, symmetry code as in Fig. 4) are comparable with those in [Cu2(μ-OAc)4(1)]n. The disorder in [Cu2(μ-OAc)4(2)]n (see above) makes comparison less meaningful.
The powder diffraction pattern for the bulk sample was in accord with the pattern calculated from the single crystal diffraction data (Fig. S2†).
Reaction of 2 with two equivalents of Zn(OAc)2·2H2O yielded colourless blocks and plates in the same crystallization tube. Preliminary crystal data for the colourless blocks confirmed this to be the one-dimensional coordination polymer [Zn2(μ-OAc)4(2)]n which crystallizes in the monoclinic space group C2/c and possesses the same gross structure as [Zn2(μ-OAc)4(1)]n,19 [Cu2(μ-OAc)4(1)]n19 and [Cu2(μ-OAc)4(2)]n. Repeated attempts to obtain a good quality crystal were unsuccessful. X-Ray analysis of the colourless plates revealed the formation of [Zn5(OAc)10(2)4·11H2O]n with an unexpected one-dimensional polymer assembly in which four bridging ligands 2 are associated with five zinc atoms. The repeat unit (Fig. 6) contains five crystallographically independent zinc atoms; Zn1 and Zn5 are tetrahedrally sited, while Zn2, Zn3 and Zn4 are 6-coordinate (Table 1). The coordination environments of Zn1 and Zn5 are similar, each zinc(II) being bound by two monodentate (terminal) acetato ligands, one N donor of a bridging ligand 2 and one O donor of a bridging acetato ligand. The monodentate acetato ligands containing O1/O2 and O17/O18 are disordered, and each has been modelled over two sites of occupancies 0.51/0.49 and 0.54/0.46, respectively. The N2O4-coordination shell of each of Zn2, Zn3 and Zn4 contains trans-N donors, and the acetato ligands that connect them adopt either a μ-O,O′ or μ,κ3-O,O′:O′ mode. The Zn⋯Zn separations along the {Zn5(OAc)10} chain are listed in Table 1; we note the appreciably longer separations associated with the {Zn2(μ-O,O′-OAc)} versus {Zn2(μ-O,O′-OAc)(μ,κ3-O,O′:O′-OAc)} units. A search of the CSD27 (Conquest v. 1.15, CSD v. 5.34 with November 2012 updates)23 did not reveal any pentametal (M = any metal) building blocks that are structurally analogous to the {Zn5(OAc)10} unit in [Zn5(OAc)10(2)4·11H2O]n, although several examples of coordination polymers and networks containing {Zn3(μ-O,O′-O2CR)2(μ,κ3-O,O′:O′-O2CR)2},33–37 or {Zn3(μ-O,O′-O2CR)4(μ,κ3-O,O′:O′-O2CR)2},38–44 units have been reported.
![]() | ||
| Fig. 6 Repeat unit of the polymer [Zn5(OAc)10(2)4·11H2O]n. Symmetry codes: i = x, −y, 1/2 + z; ii = x, −y, −1/2 + z. | ||
| Bond | Bond distance/Å | Bond | Bond distance/Å |
|---|---|---|---|
| Zn1–O1 | 2.062(4) | Zn5–O15 | 1.981(2) |
| Zn1–O3 | 2.007(3) | Zn5–O17 | 1.996(4) |
| Zn1–O5 | 2.008(2) | Zn5–O19 | 1.9538(19) |
| Zn1–N3ii | 2.079(3) | Zn5–N10 | 2.048(3) |
| Zn2–O6 | 2.0450(13) | Zn3–O8 | 2.1288(17) |
| Zn2–O7 | 2.123(2) | Zn3–O10 | 2.1133(19) |
| Zn2–O8 | 2.2560(14) | Zn3–O11 | 2.0939(19) |
| Zn2–O9 | 1.990(2) | Zn3–O13 | 2.1280(17) |
| Zn2–N6ii | 2.224(3) | Zn3–N9ii | 2.100(3) |
| Zn2–N1 | 2.232(3) | Zn3–N4 | 2.122(3) |
| Zn4–O12 | 2.019(2) | Zn4–O13 | 2.2889(14) |
| Zn4–O16 | 2.0305(14) | Zn4–N7 | 2.181(2) |
| Zn4–O14 | 2.128(2) | Zn4–N12ii | 2.202(3) |
| Zn1⋯Zn2 | 4.4346(8) | Zn2⋯Zn3 | 3.8241(8) |
| Zn4⋯Zn5 | 4.6079(8) | Zn3⋯Zn4 | 3.8844 (8) |
Each ligand 2 coordinates only through the outer pyridine rings, as is typical for 4,2′:6′,4′′-terpyridines. Fig. 6 illustrates that Zn2, Zn3 and Zn4 are connected to two ligands 2, while each of Zn1 and Zn5 is bonded to only one. The connectivities are such that {Zn5(2)4} units (black arrow in Fig. 7a) are interconnected by {Zn5(OAc)10} units (red arrow in Fig. 7a) to generate infinite polymer chains that run parallel to the c-axis (Fig. 7a and b). Fig. 7b illustrates how the domains of four pentafluorobiphenyl units protrude from either side of the chain. The four ligands 2 present in the repeat unit shown in Fig. 6 engage in face-to-face stacking of tpy domains and of pentafluorobiphenyl domains, and the efficiencies of the interactions can be assessed from the parameters given in Table 2.
![]() | ||
| Fig. 7 Assembly of deep chains in [Zn5(OAc)10(2)4·11H2O]n. (a) The red and black arrows define the directionalities of the {Zn5(OAc)10} and {Zn5(2)4} units, respectively. (b) Chains run along the c-axis, and groups of four adjacent pentafluorobiphenyl domains engage in πF⋯πF and πH⋯πH stacking interactions. | ||
| Biphenyl units containing atoms | πF⋯πF centroid⋯centroid/Å | πF⋯πF angle between ring planes/deg | πH⋯πH centroid⋯centroid/Å | πH⋯πH angle between ring planes/deg |
|---|---|---|---|---|
| F3/F8 | 3.66 | 5.6 | 3.69 | 6.7 |
| F8/F13 | 3.55 | 4.5 | 3.69 | 2.5 |
| F13/F18 | 3.52 | 7.1 | 3.75 | 9.9 |
| tpy units containing atoms | πH⋯πH centroid⋯centroid/Å | πH⋯πH angle between ring planes/deg |
|---|---|---|
| N1/N4 | 3.88 | 12.0 |
| N2/N5 | 3.73 | 1.8 |
| N3/N6 | 3.80 | 11.1 |
| N4/N7 | 3.80 | 8.1 |
| N5/N8 | 3.74 | 0.9 |
| N6/N9 | 3.75 | 3.9 |
| N7/N10 | 3.94 | 16.3 |
| N8/N11 | 3.79 | 1.6 |
| N9/N12 | 3.92 | 8.1 |
When viewed through the π-stacked domains, the chains exhibit a similar zig-zag appearance to the single chains in [Zn2(μ-OAc)4(1)]n,19 [Zn2(μ-OAc)4(2)]n, [Cu2(μ-OAc)4(1)]n19 and [Cu2(μ-OAc)4(2)]n. As in [Cu2(μ-OAc)4(2)]n (described above), this involves assembly of chains into sheets and π-stacking between arene units in adjacent sheets. Fig. 8 illustrates the packing of two adjacent chains within one sheet (blue and green chains) and between two chains in adjacent sheets (red and blue chains). The latter is comparable to that shown in Fig. 5b. We cannot comment on the role played by the water molecules in [Zn5(OAc)10(2)4·11H2O]n. Hydrogen atoms on the water solvates could not be located reliably from the difference map and were not included in the model.
![]() | ||
| Fig. 8 Packing of adjacent chains in [Zn5(OAc)10(2)4·11H2O]n. The blue and green chains are in the same sheet (see text). | ||
In order to gain insight into the composition of the bulk crystalline material, all crystals (except for those used for single crystal X-ray diffraction) were collected and ground to a powder. The powder pattern for the bulk material is shown in Fig. S2.† When matched to patterns simulated from single crystal data for [Zn5(OAc)10(2)4·11H2O]n and [Zn2(μ-OAc)4(2)]n, the data reveal that [Zn5(OAc)10(2)4·11H2O]n is the dominant component. The sample contains residual Zn(OAc)2·H2O but no free ligand 2. The powder pattern also indicates the presence of an additional unknown component.
![]() | ||
| Scheme 4 Examples of {M(OAc)2}n motifs in coordination polymers of type [M(OAc)2(L)]n and [M2(OAc)4(L)]n where L is a bis(pyridine) donor. | ||
The results described in this and our earlier work19,28–30,32 illustrate both predictable and unpredictable, and in some cases competitive, structural diversity among {Mx(OAc)2x} nodes (x = 1, 2, 3, 5) leading to the formation of single-, double-, triple- or quadruple-stranded one-dimensional coordination polymers. Single-stranded coordination polymers containing {M2(OAc)4} paddle-wheel nodes predominate and form in reactions of Zn(OAc)2·2H2O with 4′-Ph-4,2′:6′,4′′-tpy,28 4′-(4-BrC6H4)-4,2′:6′,4′′-tpy,29 4′-(4-MeSC6H4)-4,2′:6′,4′′-tpy,29 4′-tBu-4,2′:6′,4′′-tpy30 and 119 and in reactions of Cu(OAc)2·2H2O with 1,192 and a 1
:
1 mixture of 1 and 2. In these reactions, single products are isolated and elemental analyses for bulk samples are consistent with the stoichiometries confirmed crystallographically. In the case of [Zn2(μ-OAc)4(4′-Ph-4,2′:6′,4′′-tpy)]n, we observe that crystallization over extended periods is accompanied by conversion of [Zn2(μ-OAc)4(4′-Ph-4,2′:6′,4′′-tpy)]n to [Zn(O-OAc)2(4′-Ph-4,2′:6′,4′′-tpy)]n.28
The outcome of the reaction of Zn(OAc)2·2H2O with 2 is unexpected and not readily explained. The anticipated single-stranded polymer [Zn2(μ-OAc)4(2)]n is indeed formed, but the dominant crystalline product is the quadruple-stranded [Zn5(OAc)10(2)4·11H2O]n. The remarkable feature of this polymer is the 5
:
4 ratio of zinc atoms
:
bridging ligands which leads to a deep (thick) chain constructed from interconnected, oblique {Zn5(2)4} subchains (Fig. 7a). This assembly is a highly unusual 1D net, and Scheme 5 compares it to more commonly cited examples.51,52 The net defined by all Zn atoms is shown in Scheme 5a, and the Schläfli symbol with all Zn atoms as nodes (which thus includes two 2-connecting nodes, Zn1 and Zn5, which are normally reduced to links) is (4)2(43·628)2(44·62). If Zn1 and Zn5 are treated simply as links and omitted from the topological description (which is topologically more rigorous, but perhaps less chemically sensible), then the topology is reduced to that shown in Scheme 5b and the Schläfli symbol becomes (32·4.52·6)2(32·42·52). This net is in stark contrast to other multiple-stranded chains supported by 4′-X-4,2′:6′,4′′-tpy bridging ligands. In both the double-stranded one-dimensional polymer [Cd2(OAc)4(1)2]n19 and the triple-stranded [Mn3(OAc)6(4′-(4-BrC6H4)-4,2′:6′,4′′-tpy)3]n,29 each Cd or Mn atom is connected to an N-donor of each of two 4,2′:6′,4′′-tpy linkers leading to strand multiplicity that matches the nuclearity of the {M(OAc)2}n node (Scheme 6a and b). Attempts to grow single crystals from the reaction of Cd(OAc)2·2H2O with 2 (see Experimental section) repeatedly produced poor quality crystals of [Cd2(μ-OAc)4(2)2]n. Preliminary data confirmed the formation of a coordination polymer that is structurally analogous to [Cd2(OAc)4(1)2]n,19i.e. {Cd2(μ,κ3-O,O′:O′-OAc)2(κ2-O,O′-OAc)2} nodes (Scheme 6a) supporting double-stranded chains. In the unique {Zn(OAc)2}5 node in [Zn5(OAc)10(2)4·11H2O]n (Scheme 6c), each of the terminal Zn atoms serendipitously binds only one N-donor.
![]() | ||
| Scheme 5 1D nets: (a) and (b) in [Zn5(OAc)10(2)4·11H2O]n (see text), and (c) more commonly cited examples. | ||
![]() | ||
| Scheme 6 {M(OAc)2}n motifs in coordination polymers containing 4′-X-4,2′:6′,4′′-tpy and M = Cd, Mn and Zn. | ||
Finally, whereas [Zn(OAc)2(4′-X-4,2′:6′,4′′-tpy)]n polymers are chiral by virtue of a helical twist along the chain,29,32 all of the polymers featuring {M(OAc)2}n nodes (n = 2, 3 or 5) are essentially flat ribbons with single-, double- or quadruple-stranded components. Irrespective of the internal assembly of each ribbon, the latter engage in similar inter-ribbon interactions ultimately giving π-stacked sheets.
:
1 mixture of 1 and 2, [Cu2(μ-OAc)4(1)]n and [Cu2(μ-OAc)4(2)]n co-crystallize with 1 and 2 disordered over one ligand site, the whole assembly being isostructural with polymers [Cu2(μ-OAc)4(1)]n and [Cu2(μ-OAc)4(2)]n. On going from [Cu2(μ-OAc)4(1)]n to [Cu2(μ-OAc)4(2)]n, tpy⋯tpy π-stacking is retained, head-to-tail biphenyl⋯biphenyl πH⋯πH interactions are replaced by πH⋯πF contacts, and H⋯H contacts within sheets are replaced by H⋯F interactions. Significantly, the replacement of H by F substituents makes no difference to the overall solid-state structure.
With Zn(OAc)2·2H2O, ligand 2 behaves unpredictably, forming [Zn5(OAc)10(2)4·11H2O]n and [Zn2(μ-OAc)4(2)]n as the dominant minor products, respectively. The latter is a one-dimensional polymer containing simple paddle-wheel nodes, while the former is constructed from {Zn5(2)4} subchains interconnected by {Zn5(OAc)10} units to generate infinite, quadruple-stranded polymer chains. These observations are surprising in the light of the predictable formation of [Zn2(μ-OAc)4(1)]n as (apparently) the only product in the reaction of Zn(OAc)2·H2O and 1.
In conclusion, our results based on reactions with copper(II) acetate suggest that perfluoroarene⋯arene and C–H⋯F interactions have little structural influence on 4,2′:6′,4′′-terpyridine-based coordination polymers. In the spirit of ‘one experiment too many’, observations from products of reactions of ligands 1 and 2 with zinc(II) acetate highlight once again53 the role of serendipity in directing the outcome of crystallization experiments.
Footnote |
| † Electronic supplementary information (ESI) available: Fig. S1–S3. Powder diffraction patterns for bulk samples. CCDC 949632–949635. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c3ce41384e |
| This journal is © The Royal Society of Chemistry 2013 |