Introduction

Poly(methyl methacrylate) (PMMA) is used in various applications, e.g., immobilization materials, nanocomposites, and sensors [14]. PMMA provides excellent resistance to both chemical and weather corrosion and demonstrates high light transmittance [5]. PMMA is a commercially available polymer which is mostly used in optical fiber technology. Polymer optical fiber (POF) has beneficial properties such as low cost, high ductility, large core diameter, and easy handling characteristics. These infer great potential for their implementation instead of traditional silica glass-based optical fibers for short-length applications. However, a relatively low glass transition temperature (Tg) (around 100 °C) and high water absorption are the main disadvantages of PMMA [68]. POF applications of PMMA are limited by high losses in the visible and near-infrared region which are dominated by the combinations of stretch and deformation vibrations of C–H bonds [9, 10]. Replacing the hydrogen atoms in C–H bond with deuterium and fluorine atoms leads to the minimization of the absorption band because of the decrease in the band vibration energy [11]. According to Imamura et al., the substitution of deuterium for hydrogen improves the transparency at 1.3 µm [12]. In the range of telecommunication wavelengths (1500–1600 nm), the transparency is increased by the replacement of a part of C–H bonds by C–F bonds [13], also providing refractive index tunability and a decrease in PMMAs sensitivity to moisture [14]. This problem can be solved by already-designed polymers including deuterated fluoromethacrylates or polysiloxanes [12, 15], fluorinated polyimides [14, 16], and perfluorocyclobutane aromatic ether polymers [17]. Unfortunately, these polymers are relatively expensive for both consumer and end user.

In order to increase the optical properties of materials used in optical fiber technology, dopants are applied [1824]. According to Sengupta et al., the polymers doped with chlorinated dopants showed no absorption peak and retained the broad windows around the source wavelength. As reported by Koike et al., DPT (diphenyl-p-tolylamine)-doped polymers provided a lower refractive index and higher Tg value. The addition of compounds with chlorine or fluorine atoms influences the transparency and attenuation [21, 24]. For this reason, the creation of new compounds is needed and investigated.

In this study, a new monomer with chlorine atoms in 2,4,6 substitutes in phenolic derivative is considered. In order to introduce vinyl functionalization, the reaction of phenolic groups with methacrylic acid was carried out. In this way, the new monomer 2,4,6-trichlorophenyl methacrylate (TClPhMA) was obtained. Next, the copolymerization reactions of TClPhMA with commercially available monomers such as methyl methacrylate (MMA), styrene (ST), 1,4-divinylbenzene (DVB) and 2-hydroxymethyl methacrylate (HEMA) were investigated.

The effect of different chemical structures of comonomers (aliphatic: MMA and HEMA and aromatic: DVB and ST) on the physico-chemical properties of the obtained copolymers was studied. Thermal properties of the obtained copolymers were investigated using differential scanning calorimetry and thermogravimetry.

Thermal stability of TClPhMA copolymers have not been published, whereas information on properties of trifunctional methacrylate monomers and their copolymers is available [25]. It can be expected that such polymers will be at least as stable as their analogues without chlorine. As the obtained copolymers may be used in polymer optical fiber technology, the refractive indices for liquid compositions were determined.

Experimental

Materials

2,4,6-trichlorophenol, triethyleneamine, methacryloyl chloride, methyl methacrylate, 2-hydroxyethyl methacrylate and dibenzoyl peroxide were purchased from Aldrich. Styrene, magnesium sulfate, and chloroform were obtained from POCh. 1,4-divinylbenzene was purchased from Merck.

Preparation of trichlorophenyl methacrylate (TClPhMA)

In a 500-cm3 round bottomed flask equipped with a mechanical stirrer, a thermometer, and a dropper, 0.2 mol of 2,4,6-trichlorophenol was placed with 35 mL of triethyleneamine and 0.22 mol of methacryloyl chloride in the ice bath and stirred for 5 h (Fig. 1). To remove the water from the product, 0.035 mol magnesium sulfate was added. The obtained trichlorophenyl methacrylate was extracted by chloroform and purified on a chromatography column.

Fig. 1
figure 1

Scheme of synthesis of TClPhMA

Copolymerization

Copolymerization of TClPhMA with MMA, ST, DVB, and HEMA was carried out in glass form (Fig. 2a–d). Composition mass ratio was always 1:10, with 1 % (w/w) benzoyl peroxide (BPO) used as an initiator. The same amount of BPO was applied for all compositions. Copolymers were obtained after 3 steps of polymerization in a water bath and heater chamber. All compositions were kept in a water bath at 70 °C for 24 h to initiate polymerization. After this, all copolymers were transferred to a heater chamber and heated at 45 °C for 24 h. Then, the temperature was increased to 120 °C and heating continued for 3 h to crosslink the residual double bound inside the copolymers. All copolymers were kept in the heater chamber until the chamber cooled to room temperature.

Fig. 2
figure 2

a Scheme of synthesis of TClPhMA-MMA, b scheme of synthesis of TClPhMA-ST, c scheme of synthesis of TClPhMA-DVB, d scheme of synthesis of TClPhMA-HEMA

Characterization

ATR-FTIR spectra were recorded on a Brucker TENSOR 27 apparatus (Germany), equipped with diamond crystal. The spectra were gathered from 600 to 4000 cm−1.

Proton nuclear magnetic resonance (1H NMR) spectra were obtained by Brucker 300 MSL instrument (Brucker, Germany) operating at the 1H resonance frequency of 300 MHz. Chemical shifts were performed with deuterated chloroform (CDCl3) serving as an internal standard. 13C NMR spectrum of the newly obtained monomer in CDCl3 was obtained using the same apparatus.

Gas chromatography–mass spectroscopy (GC–MS) result was obtained by a Thermo-Finnigan DSQ spectrometer (Finnigan, USA) hyphenated with a gas chromatograph Trace GC-Ultra equipped with a fused-silica Equity-5 capillary column (20 m × 0.18 mm I.D., film thickness 0.20 µm). The conditions were as follows: injector PTV-split 1:20; program temperature 50–320 °C with the rate 15 °C min−1; MS electron ionization at 70 eV; temperature of ion volume 220 °C.

Differential scanning calorimetry (DSC) curves were obtained with the use of a DSC Netzsch 204 calorimeter (Netzsch, Günzbung, Germany) with the sample mass of ~5–10 mg in close aluminum crucible under nitrogen atmosphere (30 mL min−1). Dynamic scans were performed at a heating rate of 10 °C min−1 in temperature range 20–550 °C.

Thermogravimetry (TG) studies were performed on STA 449 Jupiter F1 instrument, Netzsch (Germany), with the sample mass of ~5–10 mg in open porcelain crucible in both oxidative and inert atmospheres (20 mL min−1). In the argon atmosphere, the temperature range was 20–550 °C, whereas in the air the range was 20–600 °C. The loss mass temperatures (T 5%, T 20%, T 50%), and first, second, and third decomposition temperatures (T 1, T 2, T 3) were determined.

Results and discussion

Properties of the liquid compositions

Properties of the compositions such as refractive index and density are presented in Table 1. All of the liquid compositions have densities close to methyl methacrylate, but their refractive indices are higher than that of commercial methyl methacrylate. This property of the obtained polymers allows them to be used as a core material. Among them, TClPhMA-ST has the lowest refractive index and density. This result shows that these copolymers can be useful as a core material for POF.

Table 1 Properties of the liquid compositions

ATR-FTIR spectroscopy

In order to confirm the chemical formula of the new monomer, ATR-FTIR studies were performed. The ATR-FTIR spectrum of the TClPhMA is presented in Fig. 3. In the spectrum, absorption of C–O–C group gives strong peak at 1128 cm−1. The aromatic skeletal absorption is observed at 1440 and 1633 cm−1. The signal of C=O group occurs at 1732 cm−1. The stretching vibrations band of vinyl groups (C–H) are seen at 942 cm−1 and for methyl groups (C–H) at 2924 cm−1. A C–H bands are observed at 1232 and 1319 cm−1, whereas the C–Cl group occurs at 796 cm−1.

Fig. 3
figure 3

ATR-FTIR spectra of the new obtained monomer

NMR spectroscopy

In order to identify the structures of monomer, the 1H NMR and 13C NMR spectra were recorded (Fig. 4a, b). In the 1H NMR spectrum of the new obtained monomer, the signals of –CH2, –CH3, and –CH groups were observed in 5.90 and 6.50, 2.10 and 7.40 ppm, respectively. In the 13C NMR spectrum, the most important signal is shown at 165.0 ppm. The signal expresses the carbonyl group of ester in the compound. Signals 2 and 3 refer to vinyl group, whereas 5, 6, 7 refer to carbon atoms in aromatic ring.

Fig. 4
figure 4

a 1H NMR spectrum of TClPhMA, b 13C NMR spectrum of TClPhMA

GC–MS

The chemical structure of TClPhMA was additionally confirmed by GC–MS. As its spectrum was not available in the literature, identification was achieved by analyzing molecular and fragmentary ions. In the spectrum presented in Fig. 5, molecular ion corresponding to the calculated molecular weight of TClPhMA (264) is visible. A large number of fragmentary ions are also noticeable.

Fig. 5
figure 5

GC–MS spectrum of the new obtained monomer

Thermogravimetry and DSC analysis

The DSC curves of the copolymers are presented in Fig. 6. The DSC analyses show the different thermal behaviors of the studied copolymers. In the range of 100–280 °C for MMA and HEMA copolymers, some endothermic effects corresponding to the degradation of linear aliphatic fragments are observed [26]. In the case of TClPhMA-DVB, a small exothermic peak at 160 °C is visible, probably connected with the crosslinking effect of DVB. The endothermic effects related to the thermal degradation of the samples occur at above 360 °C for TClPhMA-HEMA, at above 380 °C for TClPhMA-MMA, at above 420 °C TClPhMA-ST and at above 440 °C for TClPhMA-DVB polymeric samples. The highest degradation temperature of TClPhMA-DVB is associated with the aromatic structure and crosslinking character (two vinyl groups) of the DVB comonomer.

Fig. 6
figure 6

DSC results of the copolymers

Representative results of TG and DTG analyses obtained in an inert condition. TG results are shown in Fig. 7 and collected in Table 2. It can be seen that the 5 % (w/w) mass loss of copolymer is in the range from 196.6 °C for TClPhMA-MMA, to 345.1 °C for TClPhMA-ST, 291.1 °C for TClPhMA-DVB, 223.9 °C for TClPhMA-HEMA and 346 °C for commercial PMMA. The highest thermal resistance exhibits the TClPhMA-ST copolymer.

Fig. 7
figure 7

TG curves of the copolymers in inert condition

Table 2 Thermal stabilities of the studied copolymers in inert condition

TG-FTIR measurements were taken in an inert condition and presented in Fig. 8a–d. In the case of TClPhMA-MMA, evaporation of unreacted MMA is observed at 178 °C, whereas its depolymerization occurred at 290–390 °C. Depolymerization of TClPhMA-ST occurs at 346 °C, and degradation of the copolymer starts at 400 °C. In the case of TClPhMA-DVB, evaporation of unreacted TClPhMA occurs at 178 °C. Decomposition of this copolymer-crosslinked network starts at 320 °C and goes through 3 maxima (357, 457, 605 °C). As main volatile products, CO2, CO and H2O are observed. For TClPhMA-HEMA, evaporation of moisture takes place at 100 °C. Its depolymerization is observed at 230–380 °C.

Fig. 8
figure 8

TG-FTIR graphics of TClPhMA-MMA (a), TClPhMA-ST (b), TClPhMA-DVB (c), TClPhMA-HEMA (d)

Table 3 Thermal stabilities of the studied copolymers in oxidative condition

The results of DTG measurements are presented in Fig. 9. In the case of TClPhMA-MMA copolymer, the DTG curve contains three separated degradation steps. The first, second, and third decomposition peaks are observed in the range 150–190, 260–290, and 380–390 °C, respectively. A decomposition peak for TClPhMA-ST is observed at 420 °C, whereas for TClPhMA-DVB in the range 390–410 °C. For TClPhMA-HEMA, the decomposition peak is observed in the range of 350–360 °C with the maximum mass loss. The obtained TG/DTG results confirm the results obtained earlier by DSC analysis.

Fig. 9
figure 9

DTG curves of the copolymers in inert condition

For overall study of copolymer thermal properties, TG–DTG analyses in oxidative conditions were also carried out. The obtained results are presented in Figs. 10 and 11, as well as the datas are collected in Table 3. It can be seen that the starting mass loss of copolymer ranges from 210 °C for the TClPhMA-HEMA, 280 °C for the TClPhMA-DVB, TClPhMA-MMA and PMMA, to 340 °C for the TClPhMA-ST. The final decomposition temperature is in the range 360–550 °C.

Fig. 10
figure 10

TG curves of the copolymers in oxidative condition

Fig. 11
figure 11

DTG curves of the copolymers in oxidative condition

Comparing the course of the curves obtained in the inert and oxidative conditions, one can see that up to 180 °C the studied copolymers are stable. As expected, their thermal resistances in an oxidative condition are lower. The most rapidly decomposed copolymer (TClPhMA-HEMA) possesses linear aliphatic fragments in its structure.

Conclusions

Synthesis of the TClPhMA, its copolymerization with commercial compounds such as MMA, ST, DVB and HEMA of different chemical structures and their physical and thermal properties are presented. TClPhMA-ST and TClPhMA-DVB copolymers due to their low refractive indices have potential application in polymer optical fiber technology. However, DVB as tetrafunctional monomer leads to crosslinked polymer and therefore TClPhMA-DVB cannot be used in POF technology.

Considering the conditions of POF drawing process, TClPhMA-ST copolymer which additionally indicates the highest thermal resistance is the most suitable for drawing fibers. The obtained 2,4,6-trichlorophenyl methacrylate can be used as a dopant compound that reduces fibers attenuation.