1. Introduction
Among the electrically-conductive organic materials, polyacetylene (i.e., -[CH=CH]
n-) has been the first intrinsically conductive polymer to be developed. Initially, only the cis- and trans-isomers with undoped conductivity values of respectively 10
-11 and 10
-6 ohm
-1·cm
-1 were studied. In the most famous synthesis scheme, polyacetylene (PA) has been obtained by Zielgler-Natta polymerization of acetylene [
1]. In particular, a polymeric film resulted on the surface of the glass reactor by exposing the acetylene gas to a titanium salt catalyst. Subsequently, several complex chain and step polymerization methods for the high-regular PA synthesis have been developed (e.g., ring-opening metathesis polymerization from precursor, reverse Diels-Alder reaction processes, modified-Ziegler homogeneous, radiation polymerization) [
1].
Polyacetylene (PA) has very attractive electrical and non-electrical properties, potentially useful for different technological applications. In particular, the good electrical conductivity of doped PA can be advantageously exploited in the field of energy for fabricating electrodes for rechargeable batteries, current collectors, supercapacitors, etc. [
2,
3]. The most important drawback for a PA technological exploitation is represented by the very poor processability of this polymer type, which follows to its complete insolubility in organic solvents and failure to give a molten phase by heating. However, this problem could be overcome by generating PA by chemical transformation of an easily processable polymeric precursor. In this case, the polymeric precursor is first shaped in the required geometry (e.g., planar electrode) and then this piece is chemically converted to polyacetylene. With this purpose, there are a few little known approaches for the PA synthesis that use the conversion of a polymeric precursor to PA. These approaches are based on the dehydroalogenation of polymers [
4] and on the polyvinyl alcohol (PVOH) thermal dehydration [
5,
6,
7]. The dehydrochlorination of poly(vinyl chloride) (PVC) by treatment with a very strong base (e.g., t-BuO
-K
+) in a polar medium has been the first example of PA synthesis based on reducing a plastic precursor, however this elimination reaction never reaches the completion and hence it is unsuitable for producing a highly electrically-conductive material. Differently, the PVOH thermal-dehydration used for PA films synthesis [
5,
6] has shown great technological potentialities because it leads to a high conversion yield. Before the discovery of the PA Ziegler-Natta synthesis, it was found that extended polyenic groups, (-CH=CH-CH=CH-)
n, at that time named: ‘polyvinylenes’, were generated in polyvinyl alcohol (PVOH) molecules simply by exposing the polymer to a very common chemical-dehydrating agent, known as fuming sulfuric acid (H
2SO
4) [
8]. This chemical treatment leads to whole PA molecules by operating under H
2SO
4 refluxing conditions for a few days. A great potentiality of this very simple chemical approach is represented by the possibility to control the heterogeneous reaction conversion degree. For example, the process of solid PVOH reduction to PA can be end at a desired conversion degree by slightly diluting the sulfuric acid or by acting at room temperature for different time periods. The whole PVOH conversion to PA can result only under very drastic dehydration conditions (i.e., hot/boiling fuming sulfuric acid), while polyene-PVOH copolymers (i.e., -(CH=CH)
n-(CH
2-CH(OH))
m-, with n>m) are usually achieved by polymer dehydration treatments based on H
2SO
4 aqueous solutions. Thus, depending on the H
2SO
4 concentration and reaction temperature, different polyene/PVOH ratios are possible in the final linear macromolecular product. The physical properties (color, fluorescence, isomeric composition, etc.) of these polyene-PVOH copolymers significantly differ and consequently the obtained polymeric product is suitable for numerous technological applications (color filters, fluorescent plastics, molecular memories, etc.).
In particular, at quite high concentrations (‘fuming conditions’), sulfuric acid contains a small percentage of sulfuric anhydride (SO
3) and this
in situ generated chemical specie results an extremely strong dehydrating agent. As well known, fuming sulfuric acid is capable to act on alcohols and polyols at 140-180°C for generating olefins and polyenes [
9]; also carbohydrates are readily converted to carbon materials by dehydration with fuming sulfuric acid at room temperature [
10]. Similarly, sulfuric acid can act on the hydroxyl groups present in the linear PVOH molecules for generating conjugated polyenic groups of different extensions in the molecular chain, up to the limit case of a whole PA molecule formation. In this case, an hydrocarbon (C
nH
n) is obtained instead of a carbon material because PVOH has an hydrogen content slightly higher than carbohydrates; indeed, one H
2O molecule per each carbon atom is contained in carbohydrates (the carbohydrate formula can be written as: C
m(H
2O)
n, with m=n or very close) and therefore pure elemental carbon results from their dehydration. Concerning the exact type of chemical specie acting as dehydrating agent under such drastic reduction conditions (i.e., highly concentrated sulfuric acid), a compound named pyrosulfuric acid (H
2SO
4.xSO
3) and also known as disulfuric acid (ySO
3.H
2O) should be present. However, when PVOH dehydration takes place under milder conditions like, for example, by treatment with H
2SO
4 aqueous solutions (e.g., 50% by volume of H
2SO
4) at room temperature, sulfuric anhydride (SO
3) is not present and only protons/hydrogenions (H
+, H
3O
+) are involved in the dehydration process. Consequently, acid solutions lead to a mild PVOH reduction to polyene-PVOH copolymers and during this reaction also a chemical cross-linking process with condensated sulfate bridge formation could take place [
11].
Here, the fabrication of small PA pieces by chemical dehydration of conveniently shaped PVOH films with H2SO4 at room temperature has been investigated. PVOH is a hydrophilic polymer, highly soluble in polar solvents like water and ethanol. A number of coating technologies (spray, solution casting, dip-coatings, spin-coatings, etc.) can be conveniently adopted for depositing thin PVOH layers on chemically-resistant hydrophilic substrates (e.g., glass, ceramics, polymers). Aqueous PVOH solutions can be used also as an ink to achieve coating layers of complex geometry. The possibility to quantitatively convert these PVOH films to a PA layer by exposition to fuming sulfuric acid at room temperature allows to effectively overcoming the problem of the extremely poor PA workability. Many substrates are resistant to fuming sulfuric acid and therefore can be conveniently used for such a purpose. Such a process can be usefully exploited for the preparation of electrode materials, Lithium anode coatings and separators for supercapacitors and rechargeable batteries. In order to prove the formation of cis-PA isomer and to establish its amount, the dehydration product has been characterized by spectroscopic techniques (ATR and UV-Vis) and thermal analysis (DSC and TGA).
3. Results and Discussion
At beginning of the chemical dehydration process, the PVOH films resulted purple colored and also slightly fluorescent, with a white emission, when observed under the UV-light of a mercury-vapor lamp (TLC lamp, short-wave: 254nm) (see
Figure 2A,B). Such visible coloration/fluorescence phenomenon, that reduced and then disappeared with progress of PVOH conversion to PA, has been already described in the literature for thermally-dehydrated PVOH films [
12]. The visible coloration/fluorescence of partially reduced PVOH could be ascribed to the initial formation of short chains of conjugated carbon-carbon double bonds (i.e., dienes, trienes, etc.). The final polymeric sample was a rubbery black solid with a density higher than water (relative density: 1.2). The dry reaction product (deposited on a paper substrate) resulted electrically conductive and behaved like a highly resistive material (ca. 287 kΩ/sq. at 1kHz), as measured by a LCR-meter.
Since the synthesized PA is insoluble in all types of organic solvents (e.g., chloroform, acetone, ethanol), its characterization was carried out at solid state. In particular, the degree of PVOH conversion to polyene molecules was established by ATR analysis of the solid reaction product. Spectroscopic analysis is very sensible to the presence of adsorbed water molecules, which produces a strong and broad signal at 3400 cm
-1 (OH stretching vibration) and a medium-intensity signal at 1650 cm
-1 (HOH bending vibration) [
13] and these two bands could obscure important sample information within the mid-IR spectrum. Therefore, the reaction product was accurately dried before ATR-mode analysis by mildly heating the sample under vacuum first at 40 °C for 8 h and then at 60 °C for 3 h. The ATR spectrum of the pure dehydrated product is shown in
Figure 3A. The incomplete reduction of the polyalcohol to an unsaturated hydrocarbon is readily noticed for the presence of residual hydroxyl groups (OH) absorption in the spectrum. Indeed, these groups produce the characteristic intense and broad absorption band due to the O-H stretching vibration, which is centred at 3398 cm
-1. Such absorption is accompanied by the small intensity absorption band due to C-O stretching vibration at 1041 cm
-1 and a less intensive OH bending vibration band located at 1250 cm
-1. The small IR resonance appearing at 2934 cm
-1 is generated mainly by the terminal methyl groups, that are present also in the PA molecules but also the stretching vibration of methylene/methine groups in residual PVOH may contribute. Such aliphatic groups also generate bending vibrations appearing at 1039 cm
-1. As for the case of -OH stretching, these signals have strongly reduced intensities compared to that in pristine PVOH spectrum (see spectral comparison in
Figure 2B). However, the IR spectrum of reduction product also shows clear evidences of conjugated olefinic groups formation. Indeed, the IR spectrum of the dehydration product contains the four main characteristic absorption bands generated by conjugated olefinic groups: conjugated carbon-carbon double bond (C=C) stretching vibration, conjugated C-C single bond stretching vibration, in-plane =C-H olefinic (vinyl) =C-H bending vibrations, and out-of-plane olefinic =C-H bending vibrations [
14,
15,
16,
17,
18,
19]. In particular, the C=C stretching vibration band appears at a wavenumber of ca. 1632 cm
-1 and it is characterized by medium intensity absorption. This band extents over a wide spectral region (from ca. 1602 cm
-1 to ca. 1705 cm
-1) because the conjugation phenomenon variously extends in the linear polymer chains and even isolated C=C could be present in these molecules. In particular, the wavenumber of the carbon-carbon double bond absorption band decreases with the extent of conjugation since the bond order (i.e., force) reduces. On the other hand, owing to the same conjugation phenomenon, the C-C single bond stretching absorption appears at higher wavenumber (i.e., 1387 cm
-1), with an absorption band of quite high intensity. Very intensive absorption bands are also generated by the in-plane =C-H bending resonance, that is visible at 1192 cm
-1, and by the out-of-plane (oop) =C-H bending absorptions, that are located at 851 cm
-1 for the cis-isomer and at 902 cm
-1 for the trans-isomer. In particular, the comparison between the intensities of these =C-H oop bending vibration bands allows to easily distinguish the product between cis and trans isomers [
17]. In the present case, both isomers seems to be contained in the dehydrated product; however, according to the band intensities, conformation mostly corresponded to the cis-type. The generated molecular structure should be largely consisting of cis-PA, also because cis-alkenes have a non symmetric structure, and therefore they are capable to absorb more strongly than trans-alkenes at 1632 cm
-1, as found for our sample. It must be pointed out that polyenes should show also vinyl =C-H bond stretching absorption, appearing at ca. 3080 cm
-1, but in our PA sample this band is probably obscured by the broader residual hydroxyls absorption centered at ca. 3000 cm
-1 (stretching vibration). Yet carbon-carbon double bond (C=C) bending vibration is located outside the explored infrared spectral region (i.e., below 400 cm
-1 [
14]). Finally, comparison between the ATR spectra of pristine and dehydrated PVOH, shown in
Figure 3B, clearly evidences as the most intensive absorptions bands of the two compounds do not correspond. The fuming sulfuric acid treatment has caused variations in the intensity and position of bands and the appearance of completely new absorptions corresponding mostly to that of a cis-rich PA sample.
Similarly, the process of PVOH dehydration caused a drastic change of the polymeric material optical properties. Indeed, the perfectly transparent and colorless PVOH film, whose optical absorption spectrum, measured on PVOH aqueous solution by a double-beam UV-Vis spectrophotometer, showed no absorption peaks above 400 nm (see the red-curve in
Figure 4A). This type of spectrum indicates the absence of conjugated carbon-carbon double bonds as defects in the original polymeric sample. Differently, the spectrum of the dehydrated fraction recovered from the liquid phase showed a broad and strong absorption band in the visible spectral region, whose exact profile strictly depended on the dehydration extent. In particular, as visible in
Figure 4A, this electronic absorption spectrum of PA was characterized by a wide absorption band, which extended over the 250-600 nm spectral range and was generated by the convolution of five main elementary absorptions with maxima located at 272, 324, 433, 489, and 589 nm, that are generated by π→π* electronic transitions. These elementary bands correspond to the optical absorption of the generated linear polyenes, that are characterized by a variable number of conjugated carbon-carbon double bonds as predicted by the Fieser-Kuhn law [
20]. In particular, the positioning of some bands up to a quite high wavelength value indicates the presence in the product of polyvinylene unities with very extended conjugation (higher than 14 carbon-carbon double bonds). The observed UV-Vis absorption bands corresponded exactly to the optical behavior usually ascribed to PA [
21] (these spectra were obtained by using sulfuric acid as both dispersing medium for the PA molecules/nanoparticles and reference).
Polyenes obtained by reacting PVOH with H
2SO
4 aqueous solutions (e.g., 50% by volume of H
2SO
4) show a quite similar UV-Vis spectrum (see
Figure 4B). Owing to the different dehydration conditions, the absorption maxima are distributed differently. The temporal evolution of the liquid phase optical spectrum during the chemical dehydration reaction by fuming H
2SO
4 at room temperature is shown in
Figure 4C; these spectra have been acquired at time intervals of 15 min. According to the distribution of peak intensities in the spectra shown in
Figure 4 A-C, highly conjugated carbon-carbon double bonds are much more abundant in PVOH films treated by fuming H
2SO
4 respect to the case of dehydration by concentrated H
2SO
4 aqueous solution (50% by volume of H
2SO
4). The optical spectrum of the purified PA solid film is shown in
Figure 4D. As visible, the absorbance spectrum showed a continuum absorption band, covering half of the visible spectral region and it was characterized by a barely visible fine structure.
Solutions of PVOH-PA copolymer in fuming H
2SO
4 optically behave according to the Fieser-Kuhn equation, written with numerical coefficients adequate for this molecular structure. In particular, the mathematical expression capable to predict the spectral properties of the PVOH-PA copolymers assumes the following parabolic form [
20]:
where λ
max is the wavelength of the electronic absorption band maximum and n is the number of conjugated carbon-carbon double bonds contained in the copolymer blocks. Indeed, the PVOH blocks present along the linear copolymer molecules do not contribute to the electronic spectrum, because they have only n→σ* and σ→σ* electronic transitions that fall outside the experimentally measured ultraviolet spectral region (i.e., below 190 nm). Only the various polyene families in the copolymer chains, that are characterized by different lengths, may contribute to the optical spectrum. In particular, the above mathematical law predicts an increase of the wavelengths of absorption maxima of polyene bands up to 14 conjugated carbon-carbon double bonds and then a decrease of the absorption band maximum wavelength. In particular, with increasing of polyene block extension (n) from one to 14, the band moves from the ultraviolet spectral region (UV-A) to the middle of the visible spectral region, while it comes back to the blue region and then to the ultraviolet spectral region with further increase of the polyene block extension (i.e., n>14). A graphical representation of the absorption band wavelength vs. the number of carbon-carbon double bonds present in each polyene unit is given in
Figure 5.
The unique optical absorption feature of the prepared copolymer could allow to develop very useful optical devices like the optical limitators, attenuators, and high-pass filters (that is, optical media quite transparent in the NIR spectral region and fully opaque to the visible and ultraviolet electromagnetic radiations). The variable conjugation of the carbon-carbon double bonds generate multiple absorption bands (named ‘elementary absorption bands’) that are closely located to each other; indeed, these elementary bands are centered at wavelength values differing for only few nanometer tens. The high concentrations of different families of conjugated C=C in the solid copolymer cause elevated values of the optical extinction coefficients, which represent an essential characteristics for generating a saturation absorption band.
According to the differential scanning calorimetry (DSC) thermogram (1
st run, 10 °C/min) shown in
Figure 6, the obtained chemical product undergoes an exothermic thermal transition in the 100-150 °C temperature rage. Such exothermic transition should correspond to a solid-state cis-trans isomerization [
17], which consists in the conversion of the as synthesized cis-isomer to the more thermodynamically stable trans-isomer. However, this thermally-activated solid-state transition shows a complex behavior; indeed, the exothermic signal is superimposed to an endothermic signal. The phenomenon starts as an exothermic process (I step of thermal activation in the range 100-150 °C), but an endothermic signal (II step from 150 °C to ca. 220 °C) immediately follows. Such melting peak shows a complex profile constituted by the overlapping of three different endothermic signals that are probably produced by different phenomena like the evaporation of contaminants (sulfuric acid, water and other solvents trapped in the PA crystalline structure) and/or the thermal dehydration of residual PVOH blocks.
Obviously, such thermal behavior is an irreversible phenomenon; indeed, as shown in
Figure 7A,B, there are not signals in the subsequent DSC cooling/heating runs performed on the same DSC specimen (a thermal decomposition is visible in
Figure 7B, at temperatures above 300 °C). Indeed, the generated trans-PA isomer can melt (and completely decompose) only above the investigated temperature range (i.e., at ca. 467 °C [
22]). Owing to these unique thermal properties of the synthesized cis-PA, the material could be technologically exploited for developing new types of thermally activated molecular memories [
23].
The synthesized cis-PA was investigated also by thermogravimetric analysis (TGA), both in fluxing nitrogen and air atmospheres, in order to evaluate its thermal stability, possible solvent or reactants release, etc. As visible in
Figure 8, TGA-thermograms in air and nitrogen showed a quite similar behaviour, which is substantially characterized by two weight-losses, occurring at quite different temperature values. The first weight-loss is centered at ca. 150 °C and it is probably caused by different phenomena like, for example, the thermal dehydration of residual PVOH blocks present in the copolymer chain, the elimination by evaporation of H
2SO
4 molecules trapped in the copolymer, etc. The second weight-loss is centered at ca. 450 °C and it could be related to molecular hydrogen elimination from the PA molecules [
24]. Therefore, the mechanism of thermal decomposition should be the same, independently from the type of adopted atmosphere. The ratio between these two weight variations depends on the conversion degree of the chemical dehydration process, product purification level, etc. The residual weights in the two thermograms have different values (0.05 mg in air at 964 °C) and according to these values the synthesized PA sample was characterized by an exceptional thermal stability in nitrogen atmosphere. Indeed, 30-40% of the polymer endured the temperature of ca. 1000 °C under nitrogen (and up to ca. 500 °C in air). Such a behaviour could be explained on the basis of a ‘quasi-carbon’ nature of this type of polymer.
Figure 9 shows the XRD analysis of PVOH before and after the dehydration process. As visible in
Figure 9A, the XRD pattern of pure PVOH was characterized by two characteristic broad peaks at ca. 19.5° and 38.6°, due to the semi-crystalline nature of this polymer. The main peak corresponded to the PVOH (101) crystal plane. The crystalline nature of PVOH resulted from the strong intermolecular interaction between the PVOH chains through hydrogen bonding. According to the XRD diffractogram of the PA sample shown in
Figure 1B, the achieved polymer is an amorphous solid completely free from any crystalline signals.