Sonia
Bruña
ab,
Ana Mª
González-Vadillo
a,
Marta
Ferrández
a,
Josefina
Perles
c,
M. Merced
Montero-Campillo
d,
Otilia
Mó
bd and
Isabel
Cuadrado
*ab
aDepartamento de Química Inorgánica, Facultad de Ciencias, Universidad Autónoma de Madrid, Cantoblanco, 28049 Madrid, Spain. E-mail: isabel.cuadrado@uam.es
bInstitute for Advanced Research in Chemical Sciences (IAdChem), Universidad Autónoma de Madrid, Spain
cLaboratorio de Difracción de Rayos X de Monocristal, Servicio Interdepartamental de Investigación (SIDI), Universidad Autónoma de Madrid, Cantoblanco, 28049 Madrid, Spain
dDepartamento de Química, Facultad de Ciencias, Universidad Autónoma de Madrid, Cantoblanco, 28049 Madrid, Spain
First published on 24th July 2017
The formation of a family of silicon- and siloxane-bridged multiferrocenyl derivatives carrying different functional groups attached to silicon, including Fc2(CH3)3C(CH2)2SiCHCH2 (5), Fc2(CH2
CH–O)SiCH
CH2 (6), Fc2(OH)SiCH
CH2 (7), Fc2(CH2
CH–O)Si–O–Si(O–CH
CH2)Fc2 (8) and Fc2(CH2
CH–O)Si–O–SiFc3 (9) is described. Silyl vinyl ether molecules 6, 8 and 9 and the heteroleptic vinylsilane 5 resulted from the competing metathesis reaction of lithioferrocene (FcLi), CH2
CH–OLi or (CH3)3C(CH2)2Li with the corresponding multifunctional chlorosilane, Cl3SiCH
CH2 or Cl3Si–O–SiCl3. The last two organolithium species have been likely formed in situ by fragmentation of the tetrahydrofuran solvent. Diferrocenylvinyloxyvinylsilane 6 is noteworthy since it represents a rare example of a redox-active silyl mononomer in which two different C
C polymerisable groups are directly connected to silicon. The molecular structures of the silicon-containing multiferrocenyl species 5, 6, 8 and 9 have been investigated by single-crystal X-ray diffraction studies, demonstrating the capture and storage processes of two ring fragments resulting from the cleavage of cyclic THF in redox-active and stable crystalline organometallic compounds. From electrochemical studies we found that by changing the anion of the supporting electrolyte from [PF6]− to [B(C6F5)4]−, the redox behaviour of tetrametallic disiloxane 8 can be switched from a poorly resolved multistep redox process to four consecutive well-separated one-electron oxidations, corresponding to the sequential oxidation of the four ferrocenyl moieties.
Metal-induced cleavage reactions of ethers are rather complicated and, depending on the organometallic reagent and conditions, can take place in many different forms. Scheme 1 summarises an overview of the main described degradation processes of THF. Route A represents the principal pathway for decomposition of THF by strong organolithium bases RLi (R = Me, t-Bu, n-Bu) and involves the deprotonation of the α carbon, adjacent to oxygen, to generate a C–Li bond. Subsequently, the resultant 2-furyl anion undergoes a facile reverse [3 + 2] rearrangement to afford ethylene gas and the lithium enolate of acetaldehyde (CH2CH–OLi).3 In rare cases, for example using a t-BuLi/HMPA mixture (HMPA = hexamethylphosphoric triamide ((Me2N)3PO)) (Route B) ring opening occurs but a THF ring retains the five atoms forming lithium but-3-en-1-oxide.2 Using novel and more sophisticated synergic mixed-metal strategies, Mulvey and co-workers have observed remarkable unprecedented degradation pathways of THF. Thus, in the presence of a moderately reactive bimetallic Na/Zn base (TMEDA)Na(TMP)(CH2SiMe3)Zn(CH2SiMe3) (TMEDA = N,N,N′,N′-tetramethylethylenediamine; TMP = 2,2,6,6-tetramethylpiperidide) (Route C), α-metallation of THF occurs but the α deprotonated anion remains intact without any opening of the heterocyclic OC4 ring.5 In marked contrast to this, the more reactive heterometallic Na/Mg [(TMEDA)Na(TMP)(CH2SiMe3)Mg(TMP)] or Na/Mn [(TMEDA)Na(TMP)(CH2SiMe3)Mn(TMP)] bases promote a noteworthy cleavage of six bonds in the five-membered THF ring (Route D).6 The two anionic fragments of the THF deconstruction shown in Route D have been trapped in separated complexes, which have been crystallographically characterised.6
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Scheme 1 Summary of the main known fragmentation reactions that the THF ring can experiment in the presence of different organometallic bases. |
In a related context, deprotonative metallation has proved to be of particular importance in the chemistry of ferrocene since this synthetic transformation has been frequently applied for the derivatisation of the ferrocene backbone. The reagents classically used for this purpose are organolithiums such as n-BuLi and t-BuLi.7 Accordingly, both 1-lithioferrocene (FcLi)8 and dimetallated 1,1′-dilithioferrocene Fe(η5-C5H4Li)2, (fcLi2)9 have been prepared and often used as valuable intermediates in the synthesis of new ferrocene derivatives as they readily undergo transmetallation or nucleophilic substitution reactions. In addition, recent work by Mulvey and co-workers has shown that direct multimetallation of ferrocene with mixed bimetallic synergic bases is also possible.10 One of the most noteworthy examples of this chemistry is the 1,1′,3,3′-tetramagnesiation of ferrocene using the sodium tris(amido)magnesiate base NaMg(NiPr2)3.10b,c In addition to promoting unique polymetallation of ferrocene, some of these bimetallic reagents are particularly useful for the functionalisation of substituted ferrocenes bearing sensitive organic functional groups such as nitriles, esters or carboxylic acids.11–13
Over the years, our research interest concerns the chemistry of silicon-containing multiferrocenyl compounds.14,15 As contributions to this field, we have recently synthesised and studied Si-vinyl and Si–H functionalised triferrocenyl molecules Fc3SiCHCH2 (1)16 and Fc3SiH (2)17 (Fc = (η5-C5H4)Fe(η5-C5H5)). Triferrocenylvinylsilane 1 was prepared from 1-lithioferrocene, in turn generated by the transmetallation of 1-(tri-n-butylstannyl)ferrocene (FcSnBu3) with n-BuLi, followed by quenching with the electrophile trichlorovinylsilane. In contrast, the synthesis of homoleptic hydrosilane 2 was effected in a one-pot procedure, in which 1-lithioferrocene was directly generated in situ, by the reaction of ferrocene and t-BuLi, in a 1
:
1 mixture of THF and n-hexane.17 Over the course of this reaction we found that, in addition to the desired Si–H-functionalised triferrocenylsilane 2, diferrocenyl(3,3-dimethylbutyl)silane Fc2(CH3)3C(CH2)2SiH (3) was unexpectedly generated. The formation of heteroleptic silicon hydride 3 is proposed to occur via the competitive metathesis reaction of Cl3SiH with organolithium bases FcLi and (CH3)3C(CH2)2Li, which, in turn, has been formed in situ via the carbolithiation of ethene, generated by degradation of THF.
Herein we report on the formation of structurally new multiferrocenyl silanes and disiloxanes, namely Fc2(CH3)3C(CH2)2SiCHCH2 (5), Fc2(CH2
CH–O)SiCH
CH2 (6), Fc2(OH)SiCH
CH2 (7), Fc2(CH2
CH–O)Si–O–Si(O–CH
CH2)Fc2 (8) and Fc2(CH2
CH–O)Si–O–SiFc3 (9). These vinylsilyl compounds have been serendipitously generated from the reaction of ferrocene, t-BuLi and the corresponding multifunctional chlorosilane in the presence of a cyclic THF solvent. The formation of 6, 8 and 9, bearing the reactive silyl vinyl ether group (–Si–O–CH
CH2), is noteworthy since it not only provides new experimental proof about the fragmentation mechanism of cyclic THF, but also points to a new potentially useful synthetic way to functionalised ferrocenes. It is interesting to note that, among vinylsilanes, those bearing oxygen substituents at silicon are particularly useful, as these reagents consistently provide superior reactivity compared to their alkylsilyl counterparts.18
Accordingly, in our first attempt to prepare 1, with three ferrocenyl moieties attached to the vinylsilane functionality, we used a two-step synthetic procedure starting from FcSnBu3 as the monolithioferrocene precursor (Scheme 2, Route A).16 Subsequently, the transmetallation of FcSnBu3 was achieved by treatment with n-BuLi at −78 °C, followed by quenching with Cl3SiCHCH2. After removing the insoluble LiCl and subsequent purification via column chromatography, the target Si-vinyl-terminated 1 was isolated in high purity and reasonable yield (42%). During the purification of the reaction mixture, tetraferrocenyl disiloxane 4 was also obtained. Most likely, this initially unexpected tetrametallic compound 4 was formed under the used reaction conditions, as a result of the condensation reaction of a silanol-containing diferrocenyl molecule Fc2(OH)SiCH
CH2, in turn generated accidentally, either by partial hydrolysis of the starting trichlorovinylsilane or by hydrolysis of chlorodiferrocenylvinylsilane Fc2(Cl)SiCH
CH2, as it is shown in Scheme S1 (see the ESI†).16 Triferrocenyl compound 1 has proven to be a particularly reactive vinylsilane and has been successfully incorporated, via hydrosilylation chemistry, around the surface of polyhedral octasilsesquioxane cages (POSS) and linear and cyclic siloxane scaffolds.14c
With the aim to improve the yield of vinylsilane 1, to reduce the number of reaction steps, and mainly, to check whether new functionalised ferrocenes were formed, in an alternative approach 1-lithioferrocene was directly generated in situ in a single synthetic step, from the reaction between ferrocene and t-BuLi in a 1:
1 mixture of THF and n-hexane at −10 °C (Scheme 2, Route B). Subsequently, without isolation of the pyrophoric solid FcLi, a THF solution of trichlorovinylsilane was added dropwise to the reaction mixture cooled at −20 °C.
After the separation of the solid LiCl and appropriate workup of the crude product, the 1H NMR spectrum of the reaction mixture (see the ESI, Fig. S1†) exhibited the signals of targeted compound 1 and the apparition of new cyclopentadienyl resonances due to unknown monosubstituted ferrocenyl species. Thus, two complex multiplets centred at δ 1.00–1.50 ppm characteristic of linked CH2 groups, and a very intense singlet at δ 0.95 ppm, clearly attributable to the protons of decoupled methyl units were observed. In addition, informative resonances in the vinyl region also appeared. These key NMR spectroscopic data motivated us to isolate the unknown compounds and properly investigate their origins and molecular structures.
The purification of the crude reaction product by careful column chromatography on silica gel allowed us to separate a first band containing unreacted ferrocene, followed by other orange bands. The first one, eluted with n-hexane/CH2Cl2 (10:
1), contained a yellow-orange crystalline compound which was isolated in 6% yield, in high purity, and unequivocally identified as diferrocenyl(3,3-dimethylbutyl)vinylsilane (5). This heteroleptic silane supports the resonances observed at δ 1.00–1.50 and 0.95 ppm in the 1H NMR spectrum of the reaction mixture (see the ESI, Fig. S1†). The second band, eluted with n-hexane/CH2Cl2 (10
:
2) was found to contain a mixture of the expected compound 1 and a new mysterious vinylsilane 6. Unfortunately, both compounds have very similar physical properties and have been therefore particularly difficult to separate. Luckily after repeated column chromatographies and several recrystallization processes using different mixtures of n-hexane/CH2Cl2, we achieved the separation and isolation of pure samples of the targeted vinylsilane 1 (in 65% yield) and the new ferrocenyl species 6 (in 9% yield). On the basis of multinuclear NMR spectroscopy, mass spectrometry and X-ray studies (see below) the unknown compound was unequivocally identified as Fc2(CH2
CH–O)SiCH
CH2 (6), an interesting molecule bearing two ferrocenyl moieties and two types of C
C double bonds (one directly connected to silicon, and the other one to oxygen), thus explaining the striking 1H NMR resonances observed in the vinyl region in the spectrum of the reaction mixture.
The origin of the initially unexpected vinylsilanes Fc2(CH3)3C(CH2)2SiCHCH2 (5) and Fc2(CH2
CH–O)SiCH
CH2 (6) is certainly noteworthy and deserves an explanation. Their formation can be rationalised by the sequence of processes outlined in Scheme 3, and presumably involves the THF cleavage. As already mentioned in the introduction (Scheme 1), the main pathway for the THF degradation by RLi reagents first comprises the deprotonation at the carbon α to oxygen. Then, the resultant 2-furyl anion undergoes a reverse [3 + 2] cycloaddition to generate ethylene and the lithium enolate of acetaldehyde. Therefore, probably, compound 6 carrying both a vinyloxy and a vinyl group has been formed under the used reaction conditions, as a result of the competing salt-metathesis reaction of the organolithium reagents FcLi and CH2
CH–OLi with Cl3SiCH
CH2. Meanwhile, diferrocenyl compound 5 is likely formed as a result of the competing metathesis reaction of FcLi and (CH3)3C(CH2)2Li with Cl3SiCH
CH2. As observed during the formation of heteroleptic hydrosilane 3,17 the only plausible source of the lithiated reagent (CH3)3C(CH2)2Li is the intermolecular carbolithiation of ethylene arising from the decomposition of THF (Scheme 3).1–3
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Scheme 3 Pathway for the degradation of THF and reactions that presumably occur in the system THF/t-BuLi/FcLi/Cl3SiCH![]() |
When comparing the two synthetic procedures used to prepare 1 it can be concluded that Route B resulted more efficient and less complicated than the approach using FcSnBu3 as a starting material and that, in addition, newly interesting products, 5 and 6, have been formed. The reaction of FcLi with Cl3SiCHCH2 following Route B (Scheme 2) was repeatedly performed and in all the cases compounds 1, 5 and 6 were obtained. In addition, in some reactions, diferrocenylvinylsilanol (7) was also isolated. The formation of compound 7 provides significant evidence to affirm that disiloxane 4, obtained by Route A, was generated as a result of the condensation reaction of silanol-containing intermediates, as we previously proposed (see the ESI, Scheme S1†).16 Compound 7 was purified by column chromatography and was isolated as an air stable, yellow-orangish crystalline solid in 5% yield.
It must be emphasised that compounds 6 and 7 carry two different reactive and polymerisable groups, allowing them to participate in different chemical transformations. In addition, the polar vinyl ether reactive group present in 6 is an attractive functionalisation due to its versatile and rich reactivity.18
Once separated, the new multiferrocenyl vinylsilanes 5–7 were thoroughly characterised by elemental analysis, multinuclear NMR spectroscopy, IR and MALDI-TOF mass spectrometry. In addition to the ferrocenyl resonances, the 1H NMR spectra of 5–7 show three double doublets in the expected integrated ratios, which are consistent with the vinyl AMX system. Furthermore, the 1H NMR spectrum of 5 shows the peculiar pattern for the –(CH2)2C(CH3)3 group, a singlet at δ 0.94 ppm corresponding to the nine protons of the three decoupled methyl groups, and two complex multiplets centred at δ 1.02 and 1.44 ppm characteristic of the –CH2–CH2– unit. The –O–CHCH2 group of 6 appears as a double doublet at δ 6.59 and two doublets, one centred at δ 4.58 while the other one cannot be observed because it is overlapped with the C5H5 resonance at δ 4.16 ppm. This last signal could be identified performing a {1H–13C} HMQC experiment (see the ESI, Fig. S9†), as the carbon resonance of the –O–CH
CH2 unit correlates, not only with the multiplet at δ 4.58 ppm, but also with the other that is under the C5H5 resonance at δ 4.16 ppm. Meanwhile, the spectrum of compound 7 exhibits a singlet at δ 2.15 ppm, distinctive of the OH group.
Besides the characteristic carbon signals of the ferrocenyl units and of the vinyl groups (at 133 and 137 ppm), the 13C NMR spectrum of 5 shows the resonances of the 3,3-dimethylbutyl group. Thus, the CH2 carbons appear at δ 9.0 and 38.3 ppm, the CH3 at δ 28.9 ppm, and the ipso-carbon at δ 31.3 ppm. In the spectrum of compound 6 two resonances of the –O–CHCH2 group appear at δ 94.2 and 146.3 ppm. The 29Si NMR spectrum displays a single resonance at δ −17.0 ppm (for 1), δ −12.1 ppm (for 5), δ −7.8 ppm (for 6), and at δ −8.9 ppm (for 7). Therefore, the replacement of a ferrocenyl moiety by a 3,3-dimethylbutyl shifts the silicon signals downfield. These resonances are even more deshielded in the spectra of compounds 6 and 7, due to the electronic influence of the –OCH
CH2 and –OH groups.
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Fig. 1 MALDI-TOF mass spectrum of the reaction mixture of disiloxanes 8–10. The insets show the experimental (top) and calculated (bottom) isotopic patterns for compounds 9 and 10. |
Unfortunately, significant amounts of pure samples of multiferrocenyl disiloxanes 9 and 10 could not be isolated, so far, due to their similar solubility properties. However, their existence is fully supported by the MALDI-TOF mass spectrometric study and, in the case of disiloxane 9 by X-ray diffraction analysis (see below).
On the basis of the formation of silylated acetaldehyde species 6, it seems reasonable to assume that disiloxanes 8 and 9 were formed as a result of the competing metathesis reactions of FcLi and CH2CH–OLi to react with the hexachlorodisiloxane, according to Scheme 5.
As can be observed, the reaction between FcLi and Cl3Si–O–SiCl3 fails to give the desired hexaferrocenyl 10 in preparative amounts, which might be due to the steric repulsion of the six ferrocenyl moieties in close contact across the siloxane bond. Therefore, it is very likely that the difficulty entailed in effectively bonding six ferrocenyl units to the Si–O–Si bridge facilitates, as an alternative reaction route, the incorporation of the less bulky vinyloxy group.
We have to note that neither disiloxane 8 nor vinylsilanes 5 and 6 are accessible by conventional organosilicon chemistry methods, illustrating again the synthetic potential of THF-cleavage reactions.
Multinuclear NMR (1H, 13C and 29Si) analyses of the new disiloxane 8 were consistent with the proposed structure. Thus, the protons of the –O–CHCH2 groups appear in the 1H NMR spectrum at 6.82 ppm (double doublet) and at δ 4.68 and 4.26 ppm (doublets). The 29Si NMR of 8 presents a single resonance at δ −27.7 ppm, in good agreement with values found for other ferrocenyl disiloxanes.14
Diffraction-grade single crystals were obtained by crystallisation at 4 °C in n-hexane/CH2Cl2 (10:
2) for 5, at room temperature in CH2Cl2 for 6 and 7 and at 4 °C in n-hexane/CH2Cl2 (10
:
3) for 8 and 9. The resulting structures are shown in Fig. 2 and 3, and complete structural information is collected in the ESI.† The three bimetallic silanes 5–7 and the pentametallic disiloxane 9 crystallise in the triclinic space group P
with one (6, 7 and 9) or two (5) molecules per asymmetric unit, while tetrametallic disiloxane 8 belongs to the monoclinic P21/n space group. The two crystallographic independent molecules in the asymmetric unit cell of 5 (5A and 5B) are shown in Fig. 2 (top); they differ only slightly in their bond lengths and angles.
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Fig. 2 Molecular structures of silanes 5–7 with selected atoms labelled. Hydrogen atoms (except the hydroxylic one) have been removed for clarity. |
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Fig. 3 Molecular structures of disiloxanes 8 and 9 with selected atoms labelled. Hydrogen atoms have been removed for clarity. |
In both molecules, the two ferrocenyl groups attached to the silicon atoms are disposed in a nearly perpendicular arrangement. The cyclopentadienyl rings in 5 are parallel (maximum deviation 2.22° for the Cps attached to Fe2) and essentially eclipsed in three of the ferrocenyl moieties, while in the fourth one (the one comprising Fe3) they are completely staggered. The intramolecular distances between Fe atoms are 6.0556(8) Å (Fe1–Fe2) and 6.1853(8) Å (Fe3–Fe4). The supramolecular arrangement is achieved by van der Waals forces, giving rise to four-molecule rings.
In the bifunctional compound 6 (Fig. 2, middle), the cyclopentadienyl rings are also essentially parallel (maximum deviation 2.81° in the ferrocene containing Fe1) and eclipsed. Iron atoms are separated by 6.0857(6) Å and no relevant supramolecular interactions have been found.
In diferrocenylsilanol 7 (Fig. 2, bottom) the disposition of the Fc units is very similar to the one observed in 6, with the cyclopentadienyl rings parallel (maximum deviation 2.36° in the Fc with Fe2) and eclipsed, presenting an intramolecular distance between Fe atoms of 6.1174(6) Å. However, in this structure hydrogen bonds between the pairs of molecules are responsible for the formation of dimeric units (see the ESI, Fig. S31† and Table S12†). This is in agreement with the IR data, where a ν(OH) band at 3413 cm−1 was observed, which corresponds to Si–OH groups linked by hydrogen bonds. The fact that the two diferrocenylsilanols 6 and 7 show an almost identical molecular conformation and very similar packing patterns (see the ESI, Fig. S32†) regardless of the difference in supramolecular interactions, proves the important role that the shape and size of these molecules play in their arrangement in the crystal state. In this case, the smaller substituent in 7 together with the existence of hydrogen bonds, lead to a closer packing of the molecules involved in the supramolecular interactions, which in turn yields a denser crystal (calculated density values are 1.473 for 6 and 1.526 Mg cm−3 for 7).
In disiloxanes 8 and 9 (Fig. 3) the ferrocenyl units are placed as distant as possible from each other in order to avoid steric congestion around the silicon atoms, and the Si–O–CHCH2 groups are arranged in zig-zag chains. These two disiloxanes show a bent arrangement of the disiloxane linkage, with Si–O–Si angles of 160.0(1)° for 8 and 152.9(2)° for 9. The Fe atoms of the ferrocenyl substituents attached to the same silicon centre are separated by 5.9037(5) and 6.1052(5) Å (8) and by 5.444(1), 6.501(1) and 6.077(1) Å (9). Meanwhile, the iron centres of the ferrocenyl units attached to different silicon atoms (see the ESI, Table S11†) are separated by larger distances, ranging from 6.3853(7) to 8.4029(6) Å (for 8) and from 6.501(1) to 9.327(1) Å (for 9).
In all of the crystal structures 5–9, the silicon atoms are nearly tetrahedral with C–Si–C (for 5–9), C–Si–O (for 6–9) and O–Si–O (for 8 and 9) bond angles close to 109° (see the ESI, Fig. Table S13†) and similar to the ones obtained for 1.9
Diferrocenyl silanes 5–7 constitute the simplest molecules described here and they are structurally related to the homoleptic vinylsilane 1 and heteroleptic diferrocenyl-vinylsilane Fc2(CH3)SiCHCH2 previously investigated by us.14d,16 They are constituted by a vinyl reactive group and two identical ferrocenyl units, linked together by a silicon bridge, and they vary in the nature of the non-electroactive –O–CH
CH2, –(CH2)2C(CH3)3 or –OH substituent (R in Fig. 4 top). As expected, this leads to qualitatively similar voltammetric responses which differ only slightly in the half-wave potentials E1/2, reflecting the different electronic influences of the fourth substituent (R) at silicon. As representative examples, Fig. 4(A–D) present the CV and SWV responses obtained for 5. In CH2Cl2 using either the traditional [PF6]− or the non-coordinating [B(C6F5)4]− electrolyte anion, the electrochemical oxidation of 5 takes place in two well-resolved voltammetric waves, which correspond to the sequential oxidation of the two ferrocenyl moieties, giving the ferrocenium species 5+ and 52+. Experimentally measured potential values are 1E1/2 = 0.420 and 2E1/2 = 0.620 V (ΔE1/2 = 2E1/2 − 1E1/2 = 200 mV) (in [n-Bu4N][PF6]) and 1E1/2 = 0.422 and 2E1/2 = 0.737 V (ΔE1/2 = 315 mV) (in [n-Bu4N][B(C6F5)4]). Similarly, the CVs and SWVs of 6 and 7 also showed two successive clearly defined ferrocene-based oxidation waves separated by ΔE1/2 = 180 and 170 mV (in [n-Bu4N][PF6]) and by ΔE1/2 = 280 and 264 mV (in [n-Bu4N][B(C6F5)4]). These findings suggest the existence of appreciable iron–iron interactions between the two neighboring ferrocenyl units linked to the silicon atom. The structurally related linear and cyclic oligo- and polyferrocenylsilanes, having similar silicon-bridged ferrocenyl moieties, have been extensively studied by Manners21 and Pannell22 and exhibit electronic communication between adjacent iron centres.23
For redox-active multimetallic compounds, the magnitude of the separation between the half-wave potentials (ΔE1/2) of two redox sites has usually been taken as a measure of electronic interactions between metal centres. However, one should be extremely careful when using electrochemical data since voltammetric separations are influenced by the effects of the solvent/supporting electrolyte media, which can modify the electrostatic interactions in polycationic species.
The graphical comparison of ΔE1/2 values shown in the bottom of Fig. 4 is also representative of the changes in the redox splitting between the first and second redox events observed for diferrocenylsilanes 5–7 when changing the anion of the supporting electrolyte from nucleophilic [PF6]− to weakly coordinating fluoroarylborate anion. The fact that in the three compounds the low ion-pairing supporting electrolyte [n-Bu4N][B(C6F5)4] increases the separation of the two one-electron oxidations suggests that the through-space interaction is also significant. In addition, this figure shows that the incorporation of –(CH2)2C(CH3)3 substituent in the bridging silicon of diferrocenyl 5 results in an enlarged peak separation, which can be attributed to more effective intermetallic communication between the two ferrocenyl units.
The determination of redox potentials for the successive oxidations of 5–7 allowed us to estimate the comproportionation constant, Kc, relative to the equilibrium [FeII–FeII] + [FeIII–FeIII] ↔ [FeII–FeIII].24 The wave splitting (ΔE1/2) between the first and second oxidations measured in the weakly coordinating supporting electrolyte [n-Bu4N][B(C6F5)4] and the Kc are both indicative of the thermodynamic stability of the mixed valence state of these molecules relative to other redox systems.25 The resulting values of Kc are 211.15 × 103 (for 5), 54.07 × 103 (for 6) and 29.01 × 103 (for 7), calculated from ΔE1/2 electrochemical values, indicating that intermetallic interaction exists in the partially oxidised multiferrocenyl compounds 5–7.19b,26
Many times, a strong electronic communication between active redox centres is allowed by the presence of unsaturated or aromatic units in the bridge. This is nicely reflected in the shape of the HOMO, which involves the bridge, as a sign of delocalisation of the charge. However, neither 6–727 nor 5 (see Fig. 5A) present a HOMO orbital involving the silicon bridges, something not surprising in class II mixed-valence compounds. When dealing with these systems in a vacuum, i.e., looking strictly at the chemical structure, weak non-covalent interactions in the van der Waals range are already observed between the substituents in the silicon bridge and the ferrocenyl units, as evidenced by the NCI (Non Covalent Interaction) analysis represented by green isosurfaces in Fig. 5B. Undoubtedly, the solvent/electrolyte medium plays a very important role on modulating and reinforcing these interactions between centres, as previously observed in the voltammetric measurements. Upon oxidation, the corresponding SOMO orbital occupies the next ferrocenyl unit to be oxidised (Fig. 5A). We obtain a vertical ionisation potential value of 6.08 eV for 5, in agreement with previous values for compounds 6 and 7 (6.16 and 6.08 eV).27 The calculated UV-Vis spectrum of 5 in CH2Cl2 along with the different orbital contributions to each transition is provided in Fig. S35 and Table S14 (see the ESI†).
In addition, electronic structure calculations show that compound 5 presents a different variation of the partial charge of both Fe atoms (0.119 and 0.190 a.u.) after the first oxidation, in agreement with the electrochemical results. This compound exhibits slightly larger iron charge variations on their response to oxidation with respect to values reported for compounds 6 and 7 at the same level of theory.27 Accordingly, spin densities on iron atoms in the radical species present values of 0.699 and 0.398 a.u.
We have also explored the electrochemical oxidation of 8 since the four ferrocenyl redox moieties linked by the Si–O–Si bridge provide an excellent opportunity to study multi-step electron-transfer processes. As shown in Fig. 6, the CV of 8 in CH2Cl2/0.1 M [n-Bu4N][PF6] is considerably more complex than that of the diferrocenyl compounds 5–7, as it exhibits a sequence of several overlapped, and poorly resolved, waves (from about +0.45 to +0.85 V vs. SCE), thereby preventing a detailed analysis of the successive individual oxidations. The more anodic wave is not a diffusion-controlled process and a sharp cathodic stripping wave is observed on the return sweep. This indicates that for disiloxane 8, a change in solubility accompanies the change in the oxidation state, very likely due to the rapid precipitation of the hexafluorophosphate salt [84+][PF6]4 on the electrode surface. On the reverse scan, this tetraoxidised cation is redissolved as it is reduced. Such electrochemical phenomena are well known for multi-ferrocenyl compounds,28 where solubility problems and follow-up reactions result in deviations from ideality when using the traditional nucleophilic electrolyte anion [PF6]− in low-polarity solvents.
By using [n-Bu4N][B(C6F5)4] as an electrolyte, we hoped to accurately investigate the multistep electron-transfer processes of tetrametallic 8, because the weakly coordinating [B(C6F5)4]− anion is extremely effective in solubilising positively charged species produced in anodic processes.
Thus, Fig. 6 compares the CV of 8 in CH2Cl2/[NBu4][PF6] with those of the same molecule in CH2Cl2 with 0.1 M [n-Bu4N][B(C6F5)4], and shows the striking improvement observed for the anodic reaction of this tetrametallic disiloxane. With [B(C6F5)4]− the adsorption effects on the working electrode were minimised, which indicates an increase in solubility of the tetracationic species 84+ in this solvent/electrolyte medium. In addition, in agreement with the results reported by Geiger and coworkers, as compared to the small inorganic [PF6]− anion, the [B(C6F5)4]− electrolyte anion has a lower coordinating power and restrains ion pairing, allowing the development of interactions between the four metallocene units in 8, which are electrostatic in nature, that is, mostly through-space interactions. This results in the observation of four well-resolved one-electron oxidation waves, at different potentials, for each of the four ferrocenyl moieties. Likewise, SWV of 8 measured in CH2Cl2/[n-Bu4N][B(C6F5)4] (Fig. 6C) also shows four well-separated waves. The height peak of the two more anodic waves is somewhat smaller than that of the first two waves. This effect has been previously observed in ferrocenyl29 and fulvalenediyl multimetallic compounds30 and can be taken as a qualitative indication that the last one-electron transfers are slightly slower than that of the first two oxidations.31
The mechanism for the electrochemical oxidation of this tetrametallic disiloxane is shown in Fig. 6 and involves a first oxidation (at 1E1/2 = +0.484 V vs. SCE) corresponding to the generation of monocationic species 8+. At a higher potential (2E1/2 = +0.696 V) a second electron is removed from a ferrocenyl moiety attached to the neighbouring silicon atom, at the other end of the Si–O–Si bridge, yielding the dicationic species 82+. The potential separation between the second and third redox processes, ΔE1/2 = 3E1/2 − 2E1/2 = 256 mV, is larger than 2E1/2 − 1E1/2 = 212 mV and 4E1/2 − 3E1/2 = 228 mV, implying that the third oxidation (at 3E1/2 = +0.952 V) occurs at one of the two remaining ferrocenyl moieties, the adjacent to the last oxidised ferrocenyl subunit.14e,16 The final oxidation of the last neutral ferrocenyl centre is the most difficult one and takes place at more anodic potential (4E1/2 = +1.180 V), giving the tetracationic species 84+. The considerable spread of the four oxidations in disiloxane 8 suggests appreciable intermetallic interactions between the Si- and Si–O–Si-bridged ferrocenyl moieties.14e,16 The observed shifts of the oxidation potential values for the 8/8+/82+/83+/84+ couples (see Fig. 6) when going from [PF6]− to [B(C6F5)4]− media are consistent with a considerable decrease in the ion pairing of the FeIII centres with the weakly coordinating fluoroarylborate anion as the ferrocenyl moieties are progressively oxidised.
Electrochemical studies reveal that, in both electrolyte systems containing either the traditional [PF6]− or the weakly coordinating [B(C6F5)4]− anion, the silicon-bridged diferrocenylvinyl compounds 5–7 undergo two well-separated reversible one-electron oxidations, indicating intermetallic interactions between the ferrocenyl moieties. The introduction of the 3,3-dimethylbutyl group in the silicon bridge of 5 seems to increase the metal–metal interaction with respect to that of the structurally related diferrocenyl systems 6 and 7. In addition, tetraferrocenyl disiloxane 8 displays an interesting redox behaviour that can be switched from a poorly unresolved multistep redox process, to four consecutive, clearly defined, one-electron oxidations by changing the anion of the supporting electrolyte from [PF6]− to the weak nucleophilic and ion-pairing [B(C6F5)4]− anion. Future studies will focus on studying the reactivity of 6, 7 and 8 as redox-active bifunctional silyl monomers.
Footnote |
† Electronic supplementary information (ESI) available: Supplementary figures referenced in the text; spectroscopic, theoretical, X-ray crystallographic and CV and SWV data. CCDC 1556608–1556612. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c7dt02286g |
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