Open Access Article
Ulrike
Pfaff
,
Grzegorz
Filipczyk
,
Alexander
Hildebrandt
,
Marcus
Korb
and
Heinrich
Lang
*
Technische Universität Chemnitz, Faculty of Natural Sciences, Institute of Chemistry, Inorganic Chemistry, D-09107 Chemnitz, Germany. E-mail: heinrich.lang@chemie.tu-chemnitz.de; Fax: +49 (0)371-531-21219; Tel: +49 (0)371-531-21210
First published on 4th September 2014
The consecutive synthesis of 1,3,5-triferrocenyl-2,4,6-tris(ethynylferrocenyl)benzene (6c) is described using 1,3,5-Cl3-2,4,6-I3-C6 (2) as starting compound. Subsequent Sonogashira C,C cross-coupling of 2 with FcC
CH (3) in the molar ratio of 1
:
4 afforded solely 1,3,5-Cl3-2,4,6-(FcC
C)3-C6 (4c) (Fc = Fe(η5-C5H4)(η5-C5H5)). However, when 2 is reacted with 3 in a 1
:
3 ratio a mixture of 1,3,5-Cl3-2-(FcC
C)-4,6-I2-C6 (4a) and 1,3,5-Cl3-2,4-(FcC
C)2-6-I-C6 (4b) is obtained. Negishi C,C cross-coupling of 4c with FcZnCl (5) in the presence of catalytic amounts of [Pd(CH2C(CH3)2P(tC4H9)2)(μ-Cl)]2 gave 1,3-Cl2-5-Fc-2,4,6-(FcC
C)3-C6 (6a), 1-Cl-3,5-Fc2-2,4,6-(FcC
C)3-C6 (6b) and 1,3,5-Fc3-2,4,6-(FcC
C)3-C6 (6c) of which 6b is the main product. Column chromatography allowed the separation of these organometallic species. The structures of 4a,b and 6a in the solid state were determined by single crystal X-ray diffractometry showing a π–π interacting dimer (4b) and a complex π–π pattern for 6a. The electrochemical properties of 4a–c and 6a–c were studied by cyclic voltammetry (=CV) and square wave voltammetry (=SWV). It was found that the FcC
C-substituted benzenes 4a–c show only one reversible redox event, indicating a simultaneous oxidation of all ferrocenyl units, whereby 4c is most difficult to oxidise (4a, E°′1 = 190, ΔEp = 71; 4b, E°′1 = 195, ΔEp = 59; 4c, E°′1 = 390, ΔEp = 59 mV). In case of 4c, the oxidation states 4cn+ (n = 2, 3) are destabilised by the partial negative charge of the electronegative chlorine atoms, which compensates the repulsive electrostatic Fc+–Fc+ interactions with attractive electrostatic Fc+–Clδ− interactions. When ferrocenyl units are directly attached to the benzene C6 core, organometallic 6a shows three, 6b five and 6c six separated reversible waves highlighting that the Fc units can separately be oxidised. UV-Vis/NIR spectroscopy allowed to determine IVCT absorptions (=Inter Valence Charge Transfer) for 6cn+ (n = 1, 2) (n = 1: νmax = 7860 cm−1, εmax = 405 L mol−1 cm−1, Δν1/2 = 7070 cm−1; n = 2: νmax = 9070 cm−1, εmax = 620 L mol−1 cm−1, Δν1/2 = 8010 cm−1) classifying these mixed-valent species as weakly coupled class II systems according to Robin and Day, while for 6a,b only LMCT transitions (=ligand to metal charge transfer) could be detected.
Super-crowded ferrocenyl-based organometallic compounds are moreover remarkable species because the expected steric encumbrance may hinder chemical conjugation between the aromatic core and the ferrocenyl substituents. Representatives of this class of compounds are, for example, ferrocenyl-end-grafted dendrimers6,7 in which the intramolecular distance between the ferrocenyls is enlarged by various units such as ethynyl,6a–c ethynyl benzene,6d–e and ethynyl thiophene1f or amidoamine-based dendrimers.7 Further examples of multi-ferrocenyl organometallic compounds are benzenes,6b,c,8,9 5-membered heterocycles10,11 or even cobalt12 and manganese13 half-sandwich species with up to six terminal ferrocenyl or ethynyl ferrocenyl entities, i.e. (FcC
C)6C6, Fc6C6, 2,3,4,5-Fc4-cC4E (E = O, S, NPh, NMe), Co(η4-Fc4C4)(η5-C5H5), and Mn(η5-Fc5C5)(CO)3. Electrochemical studies revealed that for the respective super-crowded ferrocenyl thiophene significant electrostatic interaction among the four ferrocenyl groups occurs as oxidation progresses. The spectroelectrochemical results showed several UV-Vis and NIR peaks appearing or disappearing between 280 and 3000 nm as this compound is stepwisely oxidised to ultimately generate [2,3,4,5-Fc4-cC4S]4+. For the respective pyrrole compounds electronic interaction between the ferrocenyl/ferrocenium units is evidenced by in situ UV-Vis/NIR spectroscopy.10b In contrast, Vollhardt's hexaferrocenyl benzene9 and Astruc's hexa-ethynylferrocenyl benzene6b,c show three separated redox events.
We here enrich this family of perferrocenylated benzenes and describe for the first time the synthesis of multiferrocenyl-substituted benzenes featuring alternating ferrocenyl and ethynyl ferrocenyl functionalities, which represent a combination of the structural motifs of Vollhardt's9 and Astruc's6b,c benzenes. The physical and chemical properties of 1,3,5-Cl3-2-(FcC
C)-4,6-I2-C6, 1,3,5-Cl3-2,4-(FcC
C)2-6-I-C6, 1,3,5-Cl3-2,4,6-(FcC
C)3-C6, 1,3-Cl2-5-Fc-2,4,6-(FcC
C)3-C6, 1-Cl-3,5-Fc2-2,4,6-(FcC
C)3-C6 and 1,3,5-Fc3-2,4,6-(FcC
C)3-C6 (Fc = Fe(η5-C5H4)(η5-C5H5)) as well as their electrochemical properties will be highlighted.
C)3-C6 (4c) in a Sonogashira C,C cross-coupling reaction16 (Scheme 1). It appeared that four equivalents of 3 is imperative to the success of the reaction, since with a 1
:
3 stoichiometry of 2 and 3 only the mono- and di-substituted species 1,3,5-Cl3-2-(FcC
C)-4,6-I2-C6 (4a) and 1,3,5-Cl3-2,4-(FcC
C)2-6-I-C6 (4b), respectively, are formed (Scheme 1). Furthermore, the concentration of the palladium catalyst [PdCl2(PPh3)2] in the Sonogashira C,C cross-coupling plays a crucial role. For the synthesis of 4c, 1 mol% of the catalyst is required to obtain virtually quantitative yield of 4c (Experimental section), while for the synthesis of 4a and 4b 0.5 mol% of the palladium catalyst is adequate. The separation of 4a from 4b was realised by column chromatography.
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| Scheme 1 Synthesis of 214 and 4a–c. | ||
The introduction of the ferrocenyl substituents in 4c to give 1,3,5-Fc3-2,4,6-(FcC
C)3-C6 (6c) was realized by the synthetic methodology shown in Scheme 2. The best results were obtained, when 9 eq. of FcZnCl (5) as ferrocenyl source were reacted with 4c under typical Negishi C,C cross-coupling conditions17 using [Pd(CH2C(CH3)2P(tC4H9)2)(μ-Cl)]2 (0.25 mol%) as catalyst (Scheme 2, Experimental section). After appropriate work-up, compounds 6a–c, in which alternating Fc and FcC
C units are attached to the benzene core, were isolated in the ratio of 1
:
11.2
:
3.6 (= 6a
:
6b
:
6c) (Scheme 2).
The Fc and FcC
C multi-substituted benzenes 4a–c and 6a–c (Schemes 1 and 2) were obtained as red (4b, 6b) or orange (4a,c and 6a,c) solids, which dissolve in almost all common organic solvents, including toluene, dichloromethane and tetrahydrofuran. They are stable towards air and moisture in the solid state and in solution.
For comparison (see Spectroelectrochemistry part) 1-FcC
C-2-FcC6H4 (9) has been synthesized starting from 1-Br-2-I-C6H4 (7).18 When 7 was reacted with FcC
CH (3), then 1-bromo-2-ethynylferrocenyl benzene (8) was formed, which on treatment with FcZnCl (5) under typical Negishi C,C cross-coupling conditions gave 9.18
Organometallics 4a–c and 6a–c have been identified by elemental analysis, NMR (1H, 13C{1H}) and IR spectroscopy as well as high resolution ESI-TOF mass spectrometry (Experimental section). In addition, they were analysed electrochemically using cyclic voltammetry and square wave voltammetry. Spectroelectrochemistry measurements were carried out to prove if intramolecular electron transfer occurs in the mixed-valent species using in situ UV-Vis/NIR spectroscopy.
The 1H and 13C{1H} NMR spectroscopic properties of 4a–c and 6a–c correlate with their formulations as Fc and FcC
C multi-functionalised benzenes showing the respective signal patterns for the Fc, C
C and C6 core building blocks. Most distinctive for the formation of these molecules is the appearance of the expected AA′XX′ signal pattern19 for the C5H4 units (JHH = 1.9 Hz) and the singlet for the C5H5 moieties (Experimental section). Further characteristic in the 13C{1H} NMR spectra of all complexes are the signals for the ethynyl units, which resonate at ca. 65 ppm (C
C–C6) and ca. 100 ppm (C
C–Fc), respectively (Experimental section). 2D experiments such as COSY, HSQC and HMBC were applied to assign the carbon signals in 4a–c and 6a–c unequivocally. Most characteristic in the IR spectrum of all newly synthesised compounds is the appearance of one sharp C
C stretching vibration between 2200 and 2220 cm–1, specific for this distinctive unit.20
The formation of 4a–c and 6a–c was additionally evidenced from ESI-TOF mass spectrometric investigations. All organometallic compounds show the molecular ion peak [M]+ (Experimental section). Moreover, comparison of the measured isotope patterns (Cl, I) of 4a–c and 6a,b with the calculated ones confirm the elemental composition and charge state.
Furthermore, single crystal X-ray diffraction studies have been carried out to determine the molecular structures of 4a (Fig. 1), 4b (Fig. 2) and 6a (Fig. 3) in the solid state. Suitable single crystals of 4a,b and 6a could be obtained either by crystallisation of 4a and 6a from dichloromethane solutions, or by slow diffusion of n-hexane into a dichloromethane solution containing 4b at ambient temperature (Experimental section). Important bond distances (Å), bond angles (°) and torsion angles (°) are summarised in the captions of Fig. 1–3. For crystal and structure refinement data see ESI.‡ Compound 4a crystallises in the triclinic space group P
, 4b in the monoclinic space group C2/c and 6a in the orthorhombic space group Pccn.
The asymmetric unit for 4a contains one molecule, whereas half of a dimer of 4b is characteristic for the unit cell. In the case of 6a, two molecules describe the asymmetric unit. The carbon–carbon bond lengths of the benzene cores of 4a,b and 6a in (average 1.394 Å) (Fig. 1–3) are in agreement with the distances found in unsubstituted benzene (1.39 Å).21 The C,C distances of the ethynyl units agree with C
C bond lengths of this type of building blocks (1.20 Å).21
The orientation of the cyclopentadienyl rings of the syn-oriented ferrocenyls to the six membered C6 cycle is almost coplanar in molecule 4b (3.6(10), 3.5(10)°), however, it somewhat deviates from planarity in 4a (14.6(2)°). All ferrocenyls in 4a,b and 6a possess an eclipsed conformation (4a, −0.8(2)°; 4b, −1.4(12), 1.1(9)°; 6a, 8.5(10), 9.0(11), 2.6(11), 1.8(12)°). The more sterically demanding FcC
C and Fc groups are bonded to the benzene core, the lower is the coplanarity of the ferrocenyls with the C6 unit in 6a. However, for all iron-centroid distances in 4a,b and 6a as well as for all torsion angles, no significant differences occur. Reasons for the orientation of the ferrocenyls in 6a are the T-shaped π–π interactions between two ferrocenyls including intra-molecular (Fig. 4; 4.784(11) Å) as well as inter-molecular ones (Fig. 4; 4.981(13) Å). Furthermore, π–π interactions between the C5H5 moieties with the benzene core (Fig. SI1‡) could be found.
Compound 4b can best be transcribed by the symmetry operation −x, 1 − y, −z, which results in a rectangular shaped dimer (Fig. SI3‡) with parallel displaced π–π interactions between both C6 cycles of 3.615(13) Å.22 Furthermore, 4b is strongly disordered over two positions (0.6
:
0.4) in which the ferrocenes of the disordered part correspond to the corners of the rectangle formed by the initial dimer. However, the C6 core is rotated by 45° providing interaction with a third ferrocenyl corner (Fig. SI2 and SI3, ESI‡).
| Compd |
E°′1 a (ΔEp)b |
E°′2 a (ΔEp)b |
E°′3 a (ΔEp)b |
E°′4 a (ΔEp)b |
E°′5 a (ΔEp)b |
E°′6 a (ΔEp)b |
ΔE°′ c |
|---|---|---|---|---|---|---|---|
| a E°′ = formal potential. b ΔEp = difference between oxidation and reduction potential. c ΔE°′ = potential difference between the redox processes. d Potential difference between the two redox processes determined by the application of the Richardson and Taube method.31 When using the deconvolution of the redox separation of the oxidation potentials in SWV (Fig. SI4), ΔE°′ = 60 mV. e Values determined using Square Wave Voltammetry. | |||||||
| 4a | 190 (71) | — | — | — | — | — | — |
| 4b | 195 (59) | — | — | — | — | — | — |
| 4c | 390 (59) | — | — | — | — | — | — |
| 6a | 40 (74) | 225 (108) | 360 (84) | — | — | — | 185/68d/135 |
| 6b | −50 | 90 | 250 | 335 | 485 | — | 140/160/85/150 |
| 6c | −80 (75) | 70 (68) | 220 (69) | 420 (65) | 530 (63) | 660 (147) | 150/150/200/110/130 |
From Fig. 5 it can be seen that the cyclic and square wave voltammograms of 4a–c show only one reversible redox event irrespective of the number of FcC
C units present, evincing the simultaneous oxidation of the Fc groups. Furthermore, it is found that an increasing number of redox-active Fc groups at the benzene core results in a shift of the E°′1 values to higher potentials (4a, E°′1 = 190 mV; 4b, E°′1 = 195 mV; 4c, E°′1 = 390 mV) (Table 1). This indicates that the more FcC
C moieties are present, the more difficult is the oxidation of the Fe(II) centres, which is in agreement with the electron withdrawing character of the ferrocenyl ethynyl building blocks. In contrast to 4c, 1,3,5-tris(ethynylferrocenyl) benzene (dichloromethane, [nBu4N][B(3,5-C6H3(CF3)2)4] as supporting electrolyte)6b possesses three well-separated reversible redox events with redox splittings of ΔE°′1 ≈ 200 mV and ΔE°′2 ≈ 170 mV.6b Geiger has shown that [nBu4N][B(3,5-(CF3)2-(C6H3)4] and [nBu4N][B(C6F5)4] possess quite similar ion pairing capabilities in dichloromethane and both these fluorinated borates act as very weak coordinating counter ions, thus it is expected that the appropriate ΔE°′ values are similar for both electrolytes.23 Against this background the different redox behaviour of 4c and 1,3,5-tris(ethynylferrocenyl) benzene is surprising. On the one hand it could be shown that the electronic communication between the terminal ferrocenyl units is suppressed, when electron poor aromatics are used as bridging systems.1c,10b,26 On the other hand, the electron withdrawing effect of the chlorine atom leads to a partially negative charge, which enables attractive interactions with the neighbouring Fc+C
C units, compensating the repulsive electrostatic destabilisation (Fig. 6). Thus, the thermodynamic stability of mixed-valent oxidation states 4cn+ (n = 1, 2) is reduced and no redox splitting could be observed. The importance of electrostatic effects on the ΔE°′ values especially in case of weakly coupled systems has recently been pointed out by Winter, who strongly emphasizes that ΔE°′ is not a sufficient measure for the electron delocalisation within mixed-valent species.27 However, attempts to accurately model such electrostatic interactions and their effect on ΔE°′ may in future help for a better understanding of the electrochemical properties of mixed-valent systems.28
![]() | ||
| Fig. 6 Repulsive (red) and attractive (blue) electrostatic interactions within 1,3,5-tris(ethynylferrocenyl) benzene, 4c3+ and 6c6+. | ||
When the chlorine substituents of 4c were stepwisely replaced with ferrocenyl units in 6a–c, a more resolved redox behaviour with a separate oxidation of the individual ferrocenyls could be observed. A comparison of the formal oxidation potentials of ferrocenyl benzene (E°′ = 40 mV)29 and ethynylferrocenyl benzene (E°′ = 115 mV)30 allows to estimate that the ferrocenyls are oxidised prior to the FcC
C units in 6a–c. The oxidation potential of the 1st Fc oxidation decreases from 6a (E°′ = 40 mV) to 6c (E°′ = −80 mV) as the electron withdrawing chlorine substituents are replaced by electron-rich ferrocenyl termini. The redox splitting between the directly bonded ferrocenyl groups for 6c (ΔE°′1 = ΔE°′2 = 150 mV) resembles those of triferrocenyl benzene (ΔE°′1 = 140 mV; ΔE°′2 = 145 mV). In contrast to 4c, the ethynylferrocenyl units of 6c are oxidised separately. For 6c3+ the directly bonded Fc units are oxidised to ferrocenium termini which possess an equal or ever stronger electron withdrawing character as the chlorine substituents in 4c, nevertheless, those groups are positively charged and therefore, add further repulsive electrostatic interactions in 6c (Fig. 6).
Noteworthy is the high ΔEp value of 108 mV for the second redox wave of 6a, suggesting that two individual reversible one-electron processes take place in a close potential range. Hence, the square wave voltammogram gives an integrated peak area of 1
:
2
:
1, which verifies the presence of two closely spaced one-electron processes (Fig. 5). Deconvolution of the SWV of 6a using four Gaussian-shaped functions resulted in ΔE°′2 = 60 mV (ESI‡ Fig. SI4). The calculation of the signal width at half of the maximum current31 to estimate the redox separation gave a similar value of ΔE°′2 = 68 mV. This clearly confirms that the second oxidation process consists of two superimposed redox waves.
It was found that the reduction process of the sixth redox wave of 6c shows a somewhat sharper current peak and hence suggests the precipitation of 6c6+ on the surface of the working electrode, which is not unusual for highly charged ions.4,24e
Due to the use of different electrolytes in the electrochemical measurements a comparison with related work is difficult. Vollhart's hexaferrocenyl benzene gave only three redox processes consistent of a one (E°′1 = −163 mV), a two (E°′2 = −32 mV) and a three (E°′3 = 222 mV) electron process (dichloromethane, [nBu4N][PF6] as supporting electrolyte).9
However, the use of the classical [PF6]− counter ion compensates most of the electrostatic repulsion by ion-pairing with the analyte. Hence, it is expected that the use of a weakly coordinating anion (= WCA, i.e. [nBu4N][B(C6F5)4]) would probably enable the separate oxidation of all six ferrocenyl units. In the case of hexakis(ethynylferrocenyl)benzene (E°′1 = −50 mV, E°′2 = 170 mV, E°′3 = 360 mV; dichloromethane, [nBu4N][B(3,5-(CF3)2-(C6H3)4] as supporting electrolyte)6b,c even the use of WCA electrolytes only resulted in the observation of three reversible redox waves. The combination of both structural motifs, however, led to a well-separated redox behaviour as the ferrocenium units in-between the Fc+C
C moieties of 6c stabilise the mixed-valent forms 6c3–6+ by additional repulsive electrostatic interactions.
For a further investigation of the electronic properties of 6a–cin situ spectroelectrochemical UV–Vis/NIR measurements have been carried out to prove, if the interactions between the Fc/Fc+ groups are solely caused by electrostatic contributions or if an intramolecular electron transfer between the redox-active ferrocenyl moieties via the carbon-rich connectivities occurs.
For neutral 6a,b, as expected, no absorptions in the NIR region (1000–3000 nm) were observed. Upon subsequent oxidation steadily increasing absorptions with low extinctions (εmax = 50–270 L mol−1 cm−1) at 1270 nm (6an+, n = 1–4) and 1300 nm (6bn+, n = 1–5) were found (Fig. SI5 and SI6‡). These absorptions can be assigned to LMCT (=Ligand-to-Metal Charge Transfer) transitions.33 In the UV-Vis region (250–750 nm), excitations including the π–π* transitions of the benzene core as well as the d–d transitions of the Fc substituents could be detected.34 Since no IVCT (=Inter-Valence Charge Transfer) absorptions were observed, mainly electrostatic interactions (ΔEe) are responsible for the observed redox splittings between the equally charged redox centres in 6a,bn+ (6a, n = 2–4; 6b, n = 2–5). Therefore, in 6a,b any oxidation state can be classified as class I system according to Robin and Day.35 However, upon oxidation of 6c, a weak and broad excitation in the NIR region (Fig. 7) was observed of which the band of the dicationic species is hypso- and hyperchromically shifted compared with 6c+. The physical parameters have been determined by deconvolution of the experimental spectra using three Gaussian-shaped functions (Fig. 7) (6c+, νmax = 7860 cm−1, Δν1/2 = 7070 cm−1, εmax = 405 L mol−1 cm−1; 6c2+, νmax = 9070 cm−1, Δν1/2 = 8010 cm−1, εmax = 620 L mol−1 cm−1). Due to the low absorption in the NIR region detected for 6c+/2+, the compounds can be classified as weakly coupled class II systems according to Robin and Day.35 On further oxidation of 6c2+ to 6c3+ (400 to 1000 mV) this excitation disappeared. The spectroelectrochemical behaviour of 6c is similar to that of 1,3,5-Fc3C6H3 and 2,4,6-Fc3C5H2N (1,3,5-Fc3C6H3+, νmax = 6970 cm−1, Δν1/2 = 6240 cm−1, εmax = 35 L mol−1 cm−1; 1,3,5-Fc3C6H32+, νmax = 6590 cm−1, Δν1/2 = 6220 cm−1, εmax = 105 L mol−1 cm−1 | 2,4,6-Fc3C5H2N+, νmax = 6010 cm−1, Δν1/2 = 7515 cm−1, εmax = 30 L mol−1 cm−1; 2,4,6-Fc3C5H2N2+, νmax = 6290 cm−1, Δν1/2 = 7550 cm−1, εmax = 65 L mol−1 cm−1).1c However, upon consecutive oxidation of 1,3,5-Fc3C6H3 a bathochromic shift of the IVCT absorption was observed, while the IVCT transition of 2,4,6-Fc3C5H2N shifts hypsochromically, when oxidation from the mono- to the dicationic species takes place. This indicates that an increasing electron poorness of the aromatic core, caused by the nitrogen atom1c or the electron-withdrawing FcC
C groups in 6c, is responsible for the shift of the IVCT bands towards higher energy, when the mixed-valent Fe(II)/Fe(II)/Fe(III) species is oxidised to the Fe(II)/Fe(III)/Fe(III) system.
Besides the electronic interaction pathway along the meta-substituted directly bonded ferrocenyl units, an interaction between ortho-substituted Fc and FcC
C moieties seems possible. In this respect, 1-FcC
C-2-FcC6H4 (9) has been investigated by in situ UV-Vis/NIR spectroscopy. In contrast to the UV-Vis/NIR spectrum of 6cn+ (n = 1, 2) mixed-valent 9+ shows no IVCT but a LMCT absorption at 760 cm−1 (Fig. SI9‡), indicating no electronic interactions between the Fe(II)/Fe(III) centres of the FcC
C and Fc units. This observation confirms that the charge transfer in 6cn+ (n = 1, 2) occurs solely between the directly bonded Fc/Fc+ termini.
The electron poor character of the benzene core of 6b, caused by the electron-withdrawing effect of the chlorine in position 1, is not capable of facilitating the charge transfer between Fc/Fc+ in 3,5-positions.
C)-4,6-I2-C6 (4a), 1,3,5-Cl3-2,4-(FcC
C)2-6-I-C6 (4b), 1,3,5-Cl3-2,4,6-(FcC
C)3-C6 (4c), 1,3-Cl2-5-Fc-2,4,6-(FcC
C)3-C6 (6a), 1-Cl-3,5-Fc2-2,4,6-(FcC
C)3-C6 (6b) and 1,3,5-Fc3-2,4,6-(FcC
C)3-C6 (6c) (Fc = Fe(η5-C5H4)(η5-C5H5) have been prepared using palladium-catalysed Sonogashira and Negishi C,C cross-coupling reactions of halogenated aromatics with ethynylferrocene and ferrocenyl zinc chloride, respectively. The concentration of the [PdCl2(PPh3)2] and the amount of FcC
CH in the Sonogashira C,C cross-coupling plays a crucial role for the formation of 4c. The structures of 4a,b and 6a, in the solid state were determined by single crystal X-ray diffraction analysis. Compound 4b forms a dimeric structure in the solid state, caused by parallel displaced π–π interactions between the centroids of the two C6 cores of this dimer.22 For 6a more complex T-shaped π–π interactions, which are of intra- as well as of intermolecular type, occur. The redox properties of 4a–c and 6a–c were studied by cyclic and square wave voltammetry. The ferrocenyl units within compounds 4a–c are oxidised simultaneously. The partial negative charge of the electronegative chlorine atom in between the Fc+ moieties of 4cn+ (n = 2, 3) compensates the repulsive electrostatic Fc+–Fc+ interactions with attractive electrostatic Fc+–Clδ− interactions, destabilising the mixed-valent oxidation states. The absence of these chlorine atoms in 1,3,5-tris(ethynylferrocenyl) benzene thus leads to the observation of three well-separated reversible redox events, when weakly coordination anions as supporting electrolytes are applied.6b,c,23 A comparison of ferrocenyl benzene29 and ethynylferrocenyl benzene30 shows that most likely the directly bonded ferrocenyl units are oxidised at lower potential than the ethynylferrocenyl units in 6a–c. The first three redox events in 6c are resolved into one-electron waves as is typical for triferrocenyl benzenes, oxidised separately. Furthermore, the ferrocenium units of 6c3+ add further repulsive electrostatic interactions leading to a separate oxidation of the FcC
C units. This also explains the different behaviour of 6c, showing six reversible Fc–based one-electron oxidations compared to Astruc's (FcC
C)6C6 in which only three redox events have been observed using comparable measurement conditions.
In addition, in situ UV-Vis/NIR studies revealed IVCT excitations in the mixed-valent oxidation states of 6c+ and 6c2+ attributed to the Fe(II)/Fe(III) metal centres of the directly bonded ferrocenyl groups. Therefore, the mixed-valent species 6cn+ (n = 1, 2) can be classified as weakly coupled class II systems according to Robin and Day.35 The spectroscopic characteristics of 6cn+ (n = 1, 2) resemble those of 1,3,5-Fc3C6H3 and 2,4,6-Fc3C5H2N1c demonstrating that the electron transfer occurs between the Fc/Fc+ groups, while the pathway through the ortho-substituted Fc+/FcC
C units is unsuited for electronic interactions. This was confirmed by in situ UV-Vis/NIR investigations of 1-ethynylferrocenyl-2-ferrocenyl benzene (9) showing no IVCT absorptions in the mixed-valent oxidation state. Class I systems 6a,b showed only LMCT transitions during these measurements.
CH (3),36 [nBu4N][B(C6F5)4]24 and [PdCl2(PPh3)2]37 were prepared according to published procedures. The palladium pre-catalyst [P(tC4H9)2C(CH3)2CH2Pd(μ-Cl)]2 was synthesized according to Clark et al.38
:
1 (v/v) was used. The 1st fraction contained ethynylferrocene (3), while from the 2nd fraction 4a and from the 3rd fraction 4b could be isolated. All volatiles were removed under reduced pressure.
CC6), 69.84 (C5H4), 70.42 (C5H5), 72.10 (C5H4), 81.38 (Ci-C5H4), 100.59 (C–I), 101.58 (FcC
CC6), 121.90 (FcC
CC6), 142.09 (C–Cl, C-1/3), 143.63 (C–Cl, C-5). IR data [KBr, cm−1] ν: 826 (s, δo.o.p.
C–H), 1023 (m, ν
C–Cl), 1315 (s, νC–H), 1526 (w, νC
C), 2219 (s, νC
C), 3075 (w, ν
C–H). HR-ESI-MS [m/z]: calcd for C18H9FeCl3I2: 639.7154, found: 639.7204 [M+].
, λ = 0.71073 Å, a = 7.4387(5) Å, b = 10.1811(8) Å, c = 13.7230(8) Å, α = 69.747(6)°, β = 74.437(6)°, γ = 72.227(7)°, V = 912.99(11) Å3, Z = 2, ρcalcd = 2.333 g cm−3, μ = 4.643 mm−1, T = 110 K, Θ range = 3.03–26.00°, reflections collected 6949, independent 3562, R1 = 0.0243, wR2 = 0.0497 [I ≥ 2σ(I)].
CC6), 69.80 (C5H4), 70.48 (C5H5), 72.11 (C5H4), 80.41 (Ci-C5H4), 101.40 (FcC
CC6), 102.35 (C–I), 122.93 (FcC
CC6), 138.30 (C–Cl, C-3), 140.32 (C–Cl, C-1/5). IR data [KBr, cm−1] ν: 818 (s, δo.o.p.
C–H), 1002, 1024 (m, ν
C–Cl), 1346 (s, νC–H), 1540 (w, νC
C), 2209 (s, νC
C), 3097 (w, ν
C–H). HR-ESI-MS [m/z]: calcd for C30H18Fe2Cl3I: 721.8215, found: 721.8275 [M+].
898, independent 4411, R1 = 0.1063, wR2 = 0.2768 [I ≥ 2σ(I)].
CC6), 69.65 (C5H4, FcC
C), 70.43 (C5H5, FcC
C), 72.05 (C5H4, FcC
C), 79.60 (Ci-C5H4, FcC
C), 101.04 (FcC
CC6), 123.55 (FcC
CC6), 136.76 (C–Cl). IR data [KBr, cm−1] ν: 824 (s, δo.o.p.
C–H), 1025 (m, ν
C–Cl), 1359, 1383 (s, νC–H), 1532 (w, νC
C), 2209 (s, νC
C), 3088 (w, ν
C–H). HR-ESI-MS [m/z]: calcd for C42H27Fe3Cl3: 803.9226, found: 803.9222 [M+].
:
1 (v/v) was used. The first fraction contained ferrocene and unknown compounds, while thereafter 1,3-dichloro-5-ferrocenyl-2,4,6-tris(ethynylferrocenyl) benzene (6a) and 1-chloro-3,5-diferrocenyl-2,4,6-tris(ethynylferrocenyl) benzene (6b) were eluted. Pure 6c could be isolated using dichloromethane as eluent. All volatiles were removed under reduced pressure.
C), 4.30 (s, 10 H, C5H5, 4,6-FcC
C), 4.32 (pt, JHH = 1.90 Hz, 2 H, C5H4, 2-FcC
C), 4.32 (s, 5 H, C5H5, Fc), 4.33 (pt, JHH = 1.90 Hz, 4 H, C5H4, 4,6-FcC
C), 4.48 (pt, JHH = 1.90 Hz, 2 H, C5H4, Fc), 4.61 (pt, JHH = 1.90 Hz, 4 H, C5H4, 4,6-FcC
C), 4.63 (pt, JHH = 1.90 Hz, 2 H, C5H4, 2-FcC
C), 5.41 (pt, JHH = 1.90 Hz, 2 H, C5H4, Fc). 13C{1H} NMR [CDCl3, ppm] δ: 64.51 (2-FcC
CC6), 65.30 (4,6-FcC
CC6), 68.47 (C5H4, 5-Fc), 69.41 (C5H4, 4,6-FcC
C), 69.49 (C5H4, 2-FcC
C), 70.20 (C5H5, 4,6-FcC
C), 70.37 (C5H5, 2-FcC
C), 70.40 (C5H5, 5-Fc), 71.45 (C5H4, 4,6-FcC
C), 71.72 (C5H4, 5-Fc), 71.98 (C5H4, 2-FcC
C), 80.71 (Ci-C5H4, 2-FcC
C), 82.65 (Ci-C5H4, 5-Fc), 83.61 (Ci-C5H4, 4,6-FcC
C), 99.66 (2-FcC
CC6), 101.21 (4,6-FcC
CC6), 122.04 (4,6-FcC
CC6), 122.22 (2-FcC
CC6), 138.13 (C–Cl, C-1,3), 143.27 (5-Fc-C6). IR data [KBr, cm−1] ν: 818 (s, δo.o.p.
C–H), 1000 (m, ν
C–Cl), 1360 (m, νC–H), 1531 (w, νC
C), 2213 (s, νC
C), 3089 (w, ν
C–H). HR-ESI-MS [m/z]: calcd for C52H36Fe4Cl2: 953.9593, found: 953.9537 [M+].
618, independent 6835, R1 = 0.1591, wR2 = 0.3167 [I ≥ 2σ(I)].
C), 4.26 (s, 10 H, C5H5, 2,6-FcC
C), 4.27 (pt, JHH = 1.90 Hz, 2 H, C5H4, 4-FcC
C), 4.32 (s, 10 H, C5H5, 3,5-Fc), 4.33 (pt, JHH = 1.90 Hz, 4 H, C5H4, 2,6-FcC
C), 4.46 (pt, JHH = 1.90 Hz, 4 H, C5H4, 3,5-Fc), 4.48 (pt, JHH = 1.90 Hz, 2 H, C5H4, 4-FcC
C), 4.64 (pt, JHH = 1.90 Hz, 4 H, C5H4, 2,6-FcC
C), 5.32 (pt, JHH = 1.90 Hz, 4 H, C5H4, 3,5-Fc). 13C{1H} NMR [CDCl3, ppm] δ: 65.96 (2,6-FcC
CC6), 66.45 (4-FcC
CC6), 67.80 (C5H4, 3,5-Fc), 69.04 (C5H4, 4-FcC
C), 69.30 (C5H4, 2,6-FcC
C), 70.01 (C5H5, 4-FcC
C), 70.19 (C5H5, 3,5-Fc), 70.30 (C5H5, 2,6-FcC
C), 70.70 (C5H4, 4-FcC
C), 71.42 (C5H4, 2,6-FcC
C), 72.26 (C5H4, 3,5-Fc), 83.76 (Ci-C5H4, 2,6-FcC
C), 84.44 (Ci-C5H4, 4-FcC
C), 88.01 (Ci-C5H4, 3,5-Fc), 99.57 (4-FcC
CC6), 101.03 (2,6-FcC
CC6), 121.59 (2,6-FcC
CC6), 121.92 (4-FcC
CC6), 139.36 (C–Cl, C-1), 143.05 (3,5-Fc-C6). IR data [KBr, cm−1] ν: 818 (s, δo.o.p.
C–H), 1000 (m, ν
C–Cl), 1386 (m, νC–H), 1538 (w, νC
C), 2205 (s, νC
C), 3084 (w, ν
C–H). HR-ESI-MS [m/z]: calcd for C62H45Fe5Cl: 1103.9962, found: 1103.9947 [M+].
C), 4.31 (s, 15 H, C5H5, FcC
C), 4.47 (pt, JHH = 1.90 Hz, 6 H, C5H4, Fc), 4.54 (pt, JHH = 1.90 Hz, 6 H, C5H4, FcC
C), 5.24 (pt, JHH = 1.90 Hz, 6 H, C5H4, Fc). 13C{1H} NMR [CDCl3, ppm] δ: 67.09 (FcC
CC6), 67.25 (C5H4, Fc), 69.00 (C5H4, FcC
C), 70.05 (C5H5, Fc), 70.21 (C5H5, FcC
C), 70.67 (C5H4, FcC
C), 72.80 (C5H4, Fc), 85.05 (Ci–C5H4, FcC
C), 88.46 (Ci–C5H4, Fc), 100.62 (FcC
CC6), 122.46 (FcC
CC6), 142.42 (Fc–C6). IR data [KBr, cm−1] ν: 818 (s, δo.o.p.
C–H), 1106 (s, νC–C), 1383, 1411 (w, νC–H), 2210 (s, νC
C), 3094 (w, ν
C–H). HR-ESI-MS [m/z]: calcd for C72H54Fe6: 1254.0331, found: 1254.0325 [M+].
Footnotes |
| † Dedicated to Prof. Dr Gerhard Roewer on the occasion of his 75th birthday. |
| ‡ Electronic supplementary information (ESI) available: ORTEP diagram of 4b and 6a, deconvolution of the square wave voltammogram of 6a, cyclic and square wave voltammograms of 8 and 9 and UV-Vis/NIR spectra of compounds 6a,b and 9. Crystallographic data of 4a,b and 6a are also available. CCDC 986632 (4a), 986631 (4b) and 1009947 (6a). For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c4dt02307b |
| This journal is © The Royal Society of Chemistry 2014 |