# Synthesis and Characterizations of Poly(trimethylene terephthalate)-b-poly(tetramethylene glycol) Copolymers

Authors: Feng Liu; Meng Yao; Ming-tao Run
Journal: International Journal of Polymer Science
 (2013)

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## Abstract

A series of poly(trimethylene terephthalate)-b-poly(tetramethylene glycol) (PTT-PTMEG) copolymers were synthesized by two-step melt-polycondensation. The copolymers were characterized by using Fourier transform infrared spectroscopy (FTIR), 1H NMR spectroscopy, rheometer, differential scanning calorimetry (DSC), polarized optical microscopy (POM), thermal gravimetric analysis (TGA), and mechanical properties. The results suggest that by increasing the flexible PTMEG contents from 0% to 60 wt%, the copolymers show decreased glass transition temperatures, melting points, melt-crystallization temperatures, hardness, tensile strength, thermostability, and smaller spherulites dimensions; however it has much increased impact strength and elongation at breaking point. Compared with commercial poly(butylene terephthalate) (PBT)-type TPEE with 25 mol% flexible segments, PTT-type TPEE having 25 mol% flexible segments has a lower glass transition temperature, melting point, crystallization temperature, and much lower tensile strength although it has a much higher impact strength than that of PBT-type TPEE, and it is not suitably used as a commercial TPEE.


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## Body

## 1. Introduction

Thermoplastic polyester elastomers (TPEEs) are linear block copolymers which contain rigid polyester segments and soft polyether segments [1]. In TPEE, both polyether segments and uncrystallized polyester form amorphous phase, while some of the rigid polyester segments form crystals that play the role of physical cross-linking points; thus, TPEEs possess both the elasticity of the rubber and good processability of the thermoplastics. By varying the content of flexible and rigid segments along the chains, the mechanical properties can be adjusted to meet the requirements. Therefore, intensive studies have been carried out on this kind of polymer material. Poly(butylene terephthalate) (PBT) is an industrially used rigid segment in TPEE, and this PBT-type TPEE shows excellent mechanical properties [1]. Polyglycol ether was first introduced to poly(ethylene terephthalate) molecular chains by Du Pont Company, which had better hydrophilicity thus improving the dye ability of products (Hytrel). Multiple TPEE products were developed successively by Toyobo company (Pelprene), GE company (Lomed), Hoechst Celanese company (Retiflex), DSM company (Arnitel), and Elana company (Elitel), and they have been widely used in many fields such as auto manufactory, cable wire, electronic appliances, industrial products, and sports goods [2]. Witsiepe synthesized a poly(ether-ester) by the transesterification and polycondensation in the melt of dimethyl terephthalate and 1,4-butanediol [2]. Nishimura and Kornogata synthesized a kind of poly(ether-ester) elastic fiber based on PBT as rigid segments and poly(tetramethylene glycol) (PTMEG) as polyether flexible segments; this kind of fiber had good tensile elastic recovery at room temperature but relatively poor at 100°C which can be improved by adding a bit monomer of trifunctionality [3]. In order to obtain a new type of TPEE, the rigid segments other than PBT have been changed and applied in the synthesis of new TPEE. In addition to PBT, poly(ethylene terephthalate) (PET) [1, 4], poly(butylene 2,6-naphthalene dicarboxylate) [5, 6], poly(butylene-co-isophthalate) [7], and aromatic polycarbonate [8] were used as rigid segments.As a linear aromatic polyester, poly(trimethylene terephthalate) (PTT) was first produced by Shell Chemicals Co. (Corterra) [9, 10]. Compared to PBT and PET, PTT has been strong competitive power due to its excellent properties including good tensile behavior, resilience, outstanding elastic recovery, and dyeability, which make it an ideal candidate for use in applications such as textile fibers, carpets, or as an engineering plastic [11–13]. PTT has been received much attention from many industrial and academic research institutions [14–18]. As we know, less research work on TPEE based on PTT as rigid segments has been reported [19, 20]. In the US Patent [19], a PTT-based polyether-ester elastomer was synthesized comprising polytrimethylene ether-ester flexible segment and tetramethylene ester rigid segment. Szymczyk et al. [20] synthesized multiblock poly(ether-ester)s based on PTT as rigid segments and studied the PTT contents on the properties of the copolymers; the results suggest that a copolymer composed of 50% rigid segments has preferred properties.In this work, a series of poly(trimethylene terephthalate)-b-poly(tetramethylene glycol) (PTT-PTMEG) copolymers were synthesized, and their chemical structure, crystal morphology, thermostability, crystallization and melting behaviors, mechanical properties, and rheology were studied in detail. Additionally, a PTT-PTMEG composed of the same mole ratio of rigid segments to soft segments (PTT : PTMEG = 75 mol% : 25 mol%) was synthesized and compared with the properties of a commercial PBT-type TPEE (PBT : PTMEG = 75 mol% : 25 mol%). The PTT-PTMEG copolymers are expected to possess good thermoplastic elastomer properties, such as low glass transition temperature (Tg), a relatively high melting point (Tm), and a temperature independent rubbery plateau.


## 2. Experimental

### 2.1. Materials

Dimethyl terephthalate (DMT), AR, Sinapharm Chemical Reagent Co., LTD, China; 1,3-propanenediol (PDO), AR, Tianjin Guangfu Fine Chemical Industry Research Institute, China; poly(tetramethylene glycol) with the molecular weight of 1000 g/mol (PTMEG), AR, Du Pont Co., USA; PBT-type TPEE (PBT% = 75 mol%, PTMEG% = 25 mol%), CH765, Sichuan Sunshine Plastic CO., Ltd.; and as the catalysts, tetrabutyl titanate (Ti(OBu)4, Tianjin Kermel Chemical Reagent Co., Ltd.) and the antimony trioxide (Sb2O3, Tianjin Chemical Reagent Factory) were used. As the solvents, the phenol (Tianjin Kermel Chemical Reagent Co., Ltd) and the tetrachloroethane (Tianjin Guangfu Fine Chemical Industry Research Institute, China) were used. As an antioxidant, the tetrakis(methylene(3,5-di-t-butyl-4-hydroxyphenylhydro-cinnamate))methane (1010, Beijing Dilong Chemical Co. Ltd, China) was used.


### 2.2. Synthesis of PTT-PTMEG

The synthesis of poly(trimethylene terephthalate)-b-poly(tetramethylene glycol) (PTT-PTMEG) copolymers was shown in Scheme 1. These copolymers were prepared by conventional melt transesterification and polycondensation methods, and the products are linear multiblock copolymers with random distribution of the rigid and flexible segments. The reaction was carried in a vacuum flask equipped with a condenser, a stirrer, and a nitrogen atmosphere inlet. The reactions were described as follows: a mixture of DMT, PDO, PTMEG, Ti(OBu)4 (DMT : Ti(OBu)4 = 1 : 2 × 10−4(mol : mol)), and 1010 (0.5% of total comonomers mass) was put into the flask under N2 atmosphere. The mixture was heated to 220°C at a heating rate of 20°C/min and held at 220°C for 1.5 h, then Sb2O3 (DMT : Sb2O3 = 1 : 2 × 10−3(mol : mol)) was added into the flask and the mixture was slowly heated to 230°C and kept for 0.5 h to reach the endpoint of transesterification, then the melt was heated and kept at 255–265°C under gradually reduced pressure (the final pressure was 60–70 Pa) for a period of time to acquire satisfied molecular weight. Finally, the resulting copolymer was extruded from flask under nitrogen, cooled to room temperature by water, and granulated, dried in a vacuum oven.Scheme 1
Synthetic reactions of PTT-PTMEG.


### 2.3. FTIR Analysis

FTIR spectra were recorded with a Varian-640 spectrophotometer (KBr pellet technique) in the wavenumbers from 4000 to 500 cm−1 with a resolution of 1 cm−1 and averaged over 48 scans.


### 2.4. Nuclear Magnetic Resonance (1H NMR) Analysis

The1H NMR spectra were recorded by an AVIII type NMR 600 MHz spectrometer (Bruker BioSpin Co., Germany). CF3COOD was used as a solvent.


### 2.5. Intrinsic Viscosity Characterization

The intrinsic viscosity of PTT-PTMEG copolymers was measured at25±0.1°C on an Ubbelohde viscometer (DC9V/0, Schott Co., Germany) using a mixed solvent of phenol/tetrachloroethane (50 wt/50 wt). Because the Mark-Houwink constant is not known for PTT-PTMEG copolymers, the Mark-Houwink relationship determined for PTT [η]=2.11×10-5Mw0.98 [21] was used to calculate the molecular weight of PTT-PTMEG. The intrinsic viscosity and the molecular weight of the various samples were listed in Table 1.Table 1
Intrinsic viscosity and molecular weight of the various samples.
PTT/PTMEG (wt%/wt%)
[η] (dL/g)
Mw (g/mol)
C0-100/0
0.3027
17400
C1-83/17
0.4481
26000
C2-66/34
0.2763
15900
C3-40/60
0.4827
28080


### 2.6. Differential Scanning Calorimetry Characterization

The melting and crystallization measurements were performed on a Perkin-Elmer Diamond DSC instrument (USA), which was calibrated with indium; the weights of the samples were approximately 6.0 mg. The dried samples were heated to 260°C from −30°C at a rate of 10°C/min under nitrogen atmosphere, held for 5 min, then cooled to 30°C at a rate of 10°C/min, held for 5 min, and finally heated again to 260°C at a rate of 10°C/min; the first and the second melting and the first cooling processes were recorded, respectively.The samples were also heated to 260°C from 30°C at a rate of 80°C/min under nitrogen atmosphere, held for 5 min, and then quickly quenched to −50°C under a cooling rate of 100°C/min (the fastest cooling rate of the DSC used), then held at −50°C for 5 min. Subsequently, the glass transition temperature (Tg), cold-crystallization temperature (Tcc), and melting point temperature (Tm) were measured by heating the sample to 260°C at a heating rate of 10°C/min.


### 2.7. Polarized Optical Microscopy Characterization

The spherulites morphology was observed on a polarized optical microscopy (BX-51, Olympus, Japan) with a digital camera system. Samples were pressed between two glass slides with a separating of 100μm after first melting on a hot stage at 250°C for 5 min; they were then cooled to room temperature at a cooling rate of 1°C/min, with the photographs taken at room temperature.


### 2.8. Thermostability Characterization

The thermostability testing was performed on a Perkin-Elmer Pyris 6 type TG instrument (USA), and the samples’ weight was about 6.0 mg. The dried samples were heated from 30°C to 700°C at a rate of 20°C/min under nitrogen atmosphere; the weight loss behaviors were recorded.


### 2.9. Rheological Characterization

The copolymer sheets were made into standard wafers with size ofϕ25×2 mm using a micro-injection molding machine (SZ-15, Wuhan Ruiming Machinery, China) with cylinder temperature in the range of 200–250°C and a mold temperature of 20°C. The dynamic rheological property of the copolymers was performed on a rotational rheometer (AR2000ex, Waters-TA Co., USA) with the plate diameter of 25 mm and a gap width of 1.0 mm. The frequency scan was from 0.628 to 628 rad/s and the testing temperature was held on 240°C with N2 protection.


### 2.10. Mechanical Properties Testing

The tensile testing was done according to the ASTMD 638-99 normative with 1BA type specimens on a universal testing machine (WSM20, Changchun Intelligent Instrument & Equipment Co. Ltd, China) at room temperature, using the crosshead speed of 10 mm/min. Charpy impact tests were carried out according to the ISO 179-1982 standard using samples with V-notch splines and an impact tester (JJ-20, Changchun Intelligent Instrument Co. Ltd., China); the data reported were the mean and standard deviation from five determinations. Hardness measurements were performed on a Shore D apparatus (HT-6510D, Landtek Apparatus Co., China) according to a standard DIN 53505 and ISO 868.


## 2.1. Materials

Dimethyl terephthalate (DMT), AR, Sinapharm Chemical Reagent Co., LTD, China; 1,3-propanenediol (PDO), AR, Tianjin Guangfu Fine Chemical Industry Research Institute, China; poly(tetramethylene glycol) with the molecular weight of 1000 g/mol (PTMEG), AR, Du Pont Co., USA; PBT-type TPEE (PBT% = 75 mol%, PTMEG% = 25 mol%), CH765, Sichuan Sunshine Plastic CO., Ltd.; and as the catalysts, tetrabutyl titanate (Ti(OBu)4, Tianjin Kermel Chemical Reagent Co., Ltd.) and the antimony trioxide (Sb2O3, Tianjin Chemical Reagent Factory) were used. As the solvents, the phenol (Tianjin Kermel Chemical Reagent Co., Ltd) and the tetrachloroethane (Tianjin Guangfu Fine Chemical Industry Research Institute, China) were used. As an antioxidant, the tetrakis(methylene(3,5-di-t-butyl-4-hydroxyphenylhydro-cinnamate))methane (1010, Beijing Dilong Chemical Co. Ltd, China) was used.


## 2.2. Synthesis of PTT-PTMEG

The synthesis of poly(trimethylene terephthalate)-b-poly(tetramethylene glycol) (PTT-PTMEG) copolymers was shown in Scheme 1. These copolymers were prepared by conventional melt transesterification and polycondensation methods, and the products are linear multiblock copolymers with random distribution of the rigid and flexible segments. The reaction was carried in a vacuum flask equipped with a condenser, a stirrer, and a nitrogen atmosphere inlet. The reactions were described as follows: a mixture of DMT, PDO, PTMEG, Ti(OBu)4 (DMT : Ti(OBu)4 = 1 : 2 × 10−4(mol : mol)), and 1010 (0.5% of total comonomers mass) was put into the flask under N2 atmosphere. The mixture was heated to 220°C at a heating rate of 20°C/min and held at 220°C for 1.5 h, then Sb2O3 (DMT : Sb2O3 = 1 : 2 × 10−3(mol : mol)) was added into the flask and the mixture was slowly heated to 230°C and kept for 0.5 h to reach the endpoint of transesterification, then the melt was heated and kept at 255–265°C under gradually reduced pressure (the final pressure was 60–70 Pa) for a period of time to acquire satisfied molecular weight. Finally, the resulting copolymer was extruded from flask under nitrogen, cooled to room temperature by water, and granulated, dried in a vacuum oven.Scheme 1
Synthetic reactions of PTT-PTMEG.


## 2.3. FTIR Analysis

FTIR spectra were recorded with a Varian-640 spectrophotometer (KBr pellet technique) in the wavenumbers from 4000 to 500 cm−1 with a resolution of 1 cm−1 and averaged over 48 scans.


## 2.4. Nuclear Magnetic Resonance (1H NMR) Analysis

The1H NMR spectra were recorded by an AVIII type NMR 600 MHz spectrometer (Bruker BioSpin Co., Germany). CF3COOD was used as a solvent.


## 2.5. Intrinsic Viscosity Characterization

The intrinsic viscosity of PTT-PTMEG copolymers was measured at25±0.1°C on an Ubbelohde viscometer (DC9V/0, Schott Co., Germany) using a mixed solvent of phenol/tetrachloroethane (50 wt/50 wt). Because the Mark-Houwink constant is not known for PTT-PTMEG copolymers, the Mark-Houwink relationship determined for PTT [η]=2.11×10-5Mw0.98 [21] was used to calculate the molecular weight of PTT-PTMEG. The intrinsic viscosity and the molecular weight of the various samples were listed in Table 1.Table 1
Intrinsic viscosity and molecular weight of the various samples.
PTT/PTMEG (wt%/wt%)
[η] (dL/g)
Mw (g/mol)
C0-100/0
0.3027
17400
C1-83/17
0.4481
26000
C2-66/34
0.2763
15900
C3-40/60
0.4827
28080


## 2.6. Differential Scanning Calorimetry Characterization

The melting and crystallization measurements were performed on a Perkin-Elmer Diamond DSC instrument (USA), which was calibrated with indium; the weights of the samples were approximately 6.0 mg. The dried samples were heated to 260°C from −30°C at a rate of 10°C/min under nitrogen atmosphere, held for 5 min, then cooled to 30°C at a rate of 10°C/min, held for 5 min, and finally heated again to 260°C at a rate of 10°C/min; the first and the second melting and the first cooling processes were recorded, respectively.The samples were also heated to 260°C from 30°C at a rate of 80°C/min under nitrogen atmosphere, held for 5 min, and then quickly quenched to −50°C under a cooling rate of 100°C/min (the fastest cooling rate of the DSC used), then held at −50°C for 5 min. Subsequently, the glass transition temperature (Tg), cold-crystallization temperature (Tcc), and melting point temperature (Tm) were measured by heating the sample to 260°C at a heating rate of 10°C/min.


## 2.7. Polarized Optical Microscopy Characterization

The spherulites morphology was observed on a polarized optical microscopy (BX-51, Olympus, Japan) with a digital camera system. Samples were pressed between two glass slides with a separating of 100μm after first melting on a hot stage at 250°C for 5 min; they were then cooled to room temperature at a cooling rate of 1°C/min, with the photographs taken at room temperature.


## 2.8. Thermostability Characterization

The thermostability testing was performed on a Perkin-Elmer Pyris 6 type TG instrument (USA), and the samples’ weight was about 6.0 mg. The dried samples were heated from 30°C to 700°C at a rate of 20°C/min under nitrogen atmosphere; the weight loss behaviors were recorded.


## 2.9. Rheological Characterization

The copolymer sheets were made into standard wafers with size ofϕ25×2 mm using a micro-injection molding machine (SZ-15, Wuhan Ruiming Machinery, China) with cylinder temperature in the range of 200–250°C and a mold temperature of 20°C. The dynamic rheological property of the copolymers was performed on a rotational rheometer (AR2000ex, Waters-TA Co., USA) with the plate diameter of 25 mm and a gap width of 1.0 mm. The frequency scan was from 0.628 to 628 rad/s and the testing temperature was held on 240°C with N2 protection.


## 2.10. Mechanical Properties Testing

The tensile testing was done according to the ASTMD 638-99 normative with 1BA type specimens on a universal testing machine (WSM20, Changchun Intelligent Instrument & Equipment Co. Ltd, China) at room temperature, using the crosshead speed of 10 mm/min. Charpy impact tests were carried out according to the ISO 179-1982 standard using samples with V-notch splines and an impact tester (JJ-20, Changchun Intelligent Instrument Co. Ltd., China); the data reported were the mean and standard deviation from five determinations. Hardness measurements were performed on a Shore D apparatus (HT-6510D, Landtek Apparatus Co., China) according to a standard DIN 53505 and ISO 868.


## 3. Results and Discussions

### 3.1. Chemical Structure of PTT-PTMEG Copolymers

The FTIR spectra of PTT-PTMEG copolymer is shown in Figure1. The vibration at 1712 cm−1 corresponds to C=O stretching vibration of the terephthalate units. Those vibrations at 1265 and 1132 cm−1 correspond, respectively, to C–O–C asymmetric and symmetric stretching vibration. The vibration at 726 cm−1 corresponds to –CH2– rocking vibration of the PTMEG units and those vibrations at 2951 cm−1 and 2856 cm−1 correspond, respectively, to –CH2– asymmetric and symmetric stretching vibration. The vibrations at 1503 and 1463 cm−1 correspond to C=C stretching vibration of the phenyl group, and those vibrations at 1018 and 829 cm−1 correspond, respectively, to the C–H out-plane and in-plane deformation vibration of paradisplacement benzene ring.Figure 1
FTIR spectra of PTT-PTMG copolymer.The1H NMR spectra of PTT-PTMEG copolymers is shown in Figure 2. In 1H NMR spectra, the chemical shifts at 2.58 ppm (peak a; 2H, C–CH2–C) and at 4.84 ppm (peak b; 4H, O–CH2–C) were mainly the methylene protons of the short chain diol (PDO). The signals at 8.31 ppm (peak c; 4H) correspond to the aromatic proton of the terephthalate units. The chemical shifts at 3.74 ppm (peak e; O–CH2–C) and at 1.7 ppm (peak f; C–CH2–C) were for the methylene protons of the PTMEG repeating blocks. Small signals at 4.55 ppm (peak h; COO–CH2–C) correspond to the methylene protons neighboring to the ester group in the chain of PTMEG. The signals at 11.5 ppm correspond to the proton of TFA as a solvent.Figure 2
1H NMR spectra of PTT-PTMEG copolymers.PTT-PTMEG copolymer can be presented as linear multiblock copolyester composed of rigid and soft units. It gives possibility to calculate the degree of polymerization of the rigid segment, and the rigid segment content has been calculated based on the conventional soft segments definition, which includes one terephthalate unit (T) with each PTMEG sequence and called PTMEG-T as illustrated in Scheme1. In Scheme 1, x is the degree of polymerization of the rigid segment (where y=1, n=13.6). The weight and mole fraction of rigid and flexible segments were calculated from the 1H NMR spectra according to (1)–(3) and are listed in Table 2. The average length of the rigid PTT segments was also calculated from the ratio (b : h in Figure 2) of the peak intensities, based on the assumption that flexible segment length is equal to the length of starting PTMEG. The calculated degree of polymerization of the PTT segments (x) in the macrochain from 1H NMR spectra was between 24.1 (C1) and 2.3 (C3). For all the samples with exception of C1, the difference between the experimental (Exp) and theoretical (Theo) composition was less than 2%. Consider
(1)x=bh,(2)n=eh,(3)PTT(mol%)=x(1+x).Table 2
The composition of the synthesized PTT-PTMEG copolymers determined from1H NMR spectra.
PTT/PTMEG(wt%/wt%)
PTT(mol%)
PTT(wt%)
x
PTMEG(mol%)
PTMEG(wt%)
n
Theo
Exp
Theo
Exp
Theo
Exp
Theo
Exp
Theo
Exp
Theo
Exp
C1-83/17
96.0
94.8
81.5
76.9
24.1
18.2
4.0
5.2
18.5
23.1
13.6
11.2
C2-66/34
90.0
89.2
62.1
60.1
9.0
8.3
10.0
10.8
37.9
39.9
13.6
12.6
C3-40/60
70.0
71.4
29.8
31.3
2.3
2.4
30.0
28.6
70.2
68.7
13.6
11.9The results from FTIR and1H NMR measurements for the PTT-PTMEG copolymers suggest that the products are basically consistent with our expected chemical structures, as shown in Figure 2.


### 3.2. Melting and Crystallization Behaviors

Figure3 shows the glass transition temperatures of the various copolymers, and the parameters are listed in Table 3. It can be seen in Figure 3 that C0 (pure PTT) and C1 only show one glass transition (Tg1) and a cold-crystallization peak (Tcc) in each DSC curve, in which Tg1 and Tcc of C1 are much lower than those of C0, while, for C2 and C3, they both show two glass transitions (Tg1 and Tg2) but without any cold-crystallization behavior. In Table 3, C0 has the largest value of Tg1 among these samples, while Tg1s of C1, C2, and C3 decrease slightly; additionally, C3 has a larger Tg2 than that of C2. There may be a mixed amorphous phase of PTT and PTMEG (Tg1s of C2 and C3 that are lower than that of C0) and an amorphous PTMEG phase (Tg2) occurred in the materials, so they both show two glass transitions in C2 and C3 copolymers.Table 3
DSC melting and crystallization parameters of the various samples.
PTT/PTMEG(wt%/wt%)
First heating process
Cooling process
T
g
1 (°C)
T
g
2 (°C)
T
cc (°C)
T
re (°C)
Δ
H
re (J·g−1)
T
m
1 (°C)
T
m
2 (°C)
Δ
H
m (J·g−1)
T
c (°C)
Δ
H
c (J·g−1)
FWHP(°C)
C0-100/0
—
49.3
67.8
199.3
−7.05
—
229.2
62.01
202.8
−57.88
8.6
C1-83/17
—
26.4
49.7
188.3
−5.37
208.6
221.8
48.96
191.4
−41.69
8.7
C2-66/34
−64.5
24.7
—
166.7
−3.48
199.8
206.7
42.41
185.3
−40.83
12.7
C3-40/60
−67.7
22.5
—
—
—
—
180.7
25.19
160.8
−15.81
13.9Figure 3
Glass transitions of the various copolymers.Figure4 shows the DSC melting thermograms of the various samples with the crystallization parameters summarized in Table 3. It can be seen from Figure 4 and Table 4 that these DSC curves have one or two asymmetrical melting peaks (Tm1, Tm2), and they tend to be narrow and shift to higher temperature with increasing PTT content in the copolymers because more PTT content will improve the regularity of molecular chains and the crystallizability of the copolymer; that is to say, when the PTT content increases, the longer rigid and crystallizable chain segments will form in the copolymers, so the longer and rigid segments will crystallize into larger crystals and they will melt at higher temperature. The multiple melting peaks behavior may be due to the different kinds of the copolymers formed with different length of rigid segments. The melting enthalpy (ΔHm) also decreases greatly with increasing PTEMG content in the copolymers.Table 4
Parameters of the TGA curves for the various samples.
PTT/PTMEG(wt%/wt%)
T
2
%  (°C)
T
5
%  (°C)
T
max  (°C)
W
600
°
C  (%)
η
0
*  (Pa·s)
σ
t
a  (MPa)
ε
b
b  (%)
σ
i
c  (KJ·m−2)
H
d  (Sh D)
C0-100/0
343.8
369.0
406.5
0.69
345.1
30.4
33.3
7.6
76
C1-83/17
345.8
367.9
409.9
0.75
230.2
11.4
249.1
16.5
58
C2-66/34
324.3
362.4
408.0
0.83
168.8
8.7
398.6
28.8
41
C3-40/60
274.8
351.3
408.0
0.26
111.5
5.8
589.1
47.2
26
aTensile strength.
bElongation at breaking point.
cImpact strength.
dShore hardness.Figure 4
DSC first melting thermograms of the various samples.In addition, except for the sample C3, each of the curves exhibits a recrystallization peak (Tre) before the melting peak, which shifts to higher temperature with increasing PTT rigid segments content. This result is also correlated to the molecular structure of the copolymer. Because the sample with more PTMEG content has lower crystallizability, some microcrystallites with lower perfection and smaller size will form in the material; these microcrystallites will melt and recrystallize at low temperatures in the heating process. The sample C3 having the most PTMEG contents in the copolymer shows no recrystallization peak because of its lowest crystallizability. The recrystallization enthalpy (ΔHre) also decreases with increasing PTMEG content in the copolymers. On the other hand, in the DSC curves of C2 and C3, the melting peaks are shown with much wide distribution, indicating that the length of the rigid segments may have a wide distribution in the copolymers and they form spherulites with different sizes that melt at different temperatures.Figure5 shows the DSC melt-crystallization curves of the various samples and their crystallization parameters were summarized in Table 3. As seen from Figure 5, except for C3, each of the curves is shown with good symmetrical crystallization peak, and they also tend to be narrow and shift to high temperature with increasing PTT contents. The crystallization enthalpy (ΔHc) also increases with increasing PTT contents. Moreover, the full width at half-height of the crystallization peak (FWHP) decreases as PTT content increases. It can be concluded that the sample with higher PTT content has higher onset-crystallization temperature and faster crystallization rate. Their crystallization behaviors are also correlated to the content of the rigid segments, as explained above. The sample C3 has an unobvious crystallization peak mainly because of its lower crystalline content of rigid PTT.Figure 5
DSC crystallization curves of the various samples.From the above results of glass transitions, cold-crystallization, melting points, and crystallization behaviors of the various copolymers, we may give the following conclusions: (1) there may be four different domains in the copolymers: a crystalline PTT phase, an amorphous PTT phase, an amorphous PTMEG phase, and a mixed amorphous phase depending on the sample composition. When PTMEG content is 17 wt% (C1), a mixed amorphous phase shows lowerTg2 and Tcc than those of C0; when PTMEG contents are 34 wt% (C2) and 60 wt% (C3), both a mixed amorphous phase and an amorphous PTMEG phase occur in the materials, so they both show two glass transitions (Tg2 and Tg1). The presence of four different domains depends on the thermal history and composition in the elastomers based on PET and PEO which have been observed by Fakirov et al. [22]. (2) When the PTT-PTMEG copolymers contain above 34 wt% of soft segments, low-temperature glass transition and a high melting point can be observed, thus the microphase separation structure occurred in the copolymers, which are two important characters for the thermoplastic elastomers.


### 3.3. Spherulite Morphology

Figure6 shows the spherulite morphology of the various samples. As seen in Figure 6(a), the spherulites of PTT are fairly large with perfect Maltese cross extinctions, while for C1 (Figure 6(b)), it exhibits a relatively well-defined spherulitic texture with Maltese cross extinctions but with small spherulite size; additionally, some microspherulites are observed in some area. As shown in Figures 6(c) and 6(d), C2 and C3 images exhibit large number of small bright spots, and nearly no clear Maltese cross extinctions can be observed, indicating that only some microcrystallites can be formed in these samples. The above results suggest that the spherulite size of PTT-PTMEG copolymers decreases with the decreasing contents of rigid PTT segments. We believe that the crystallization behavior of PTT segments is limited by the soft PTMEG segments, and PTMEG and some uncrystallized PTT form the amorphous phase in the material.Figure 6
POM micrographs of crystallized samples (a) C0; (b) C1; (c) C2; and (d) C3.


### 3.4. Thermal Stability

Figure7 shows the TG curves of the various samples and the parameters are listed in Table 4. It can be seen that each curve has one predominant degradation stage. The temperatures at weight losses of 2% (T2%) and 5% (T5%) decrease with increasing soft PTMEG segments, while the fastest thermolysis temperatures (Tmax) and the residues weight (W600°C) are nearly the same at 600°C. These results suggest that the thermal stability of the copolymers becomes worse with more soft PTMEG content.Figure 7
TG curves of the various samples.


### 3.5. Rheology Behaviors

Figure8 is the plots of complex viscosity versus frequency (η*-ω) of different samples. For PTT, its complex viscosity remains nearly stable as ω<102 rad/s, indicating that PTT melt is Newtonian liquid at low shearing frequencies, while it turns into pseudoplastic fluid as ω<102 rad/s. In the low shearing frequencies range, the entangling rate and unentangling rate of molecular chains achieve a dynamic balance, so the complex viscosity presents a platform. When the shearing frequency exceeds a critical value, the unentangling rate is faster than entangling rate, so the complex viscosity decreases. On the other hand, it can be seen from Figure 8 that the copolymer with more PTMEG content has larger zero shear viscosity (η0*) values (Table 4), suggesting that the copolymer with more flexible segments can form more entangled points in the polymer. For three copolymers, their η* slowly decreases first, then remains stable and then decreases at high shearing frequency. Because PTT-PTMEG copolymers have more flexible segments than that in pure PTT, there are more entangled points in the copolymers, and some entangled points are easily destroyed at low shearing frequency, so the η* decreases at low frequencies range and the more the flexible PTMEG contents in the copolymers, the more sharply the decrease of η*. The three copolymers are pseudoplastic fluids at low shearing frequencies. At high frequencies, their η* values are close to each other due to the high shearing rate which makes most entangled points unentangle.Figure 8
Curves ofη* versus ω of the various copolymers.


### 3.6. Mechanical Properties

The mechanical properties of the various copolymers are tested and their stress-strain curves are shown in Figure9 and the data are listed in Table 4. It can be seen that the tensile strength decreases while the elongation at breaking point increases with increasing flexible segments (Table 4). These results are mainly because of the decrease of the crystallinity in the copolymers. On the other hand, as shown in Table 4, the impact strength increases and the Shore hardness decreases with increasing soft PTMEG segments in the copolymers.Figure 9
The stress-strain properties of PTT-PTMEG copolymers.


### 3.7. Comparison of PTT-Type TPEE and PBT-Type TPEE

In this part, in order to compare the properties of the copolymer based on PTT as rigid segments (PTT-type TPEE) to the commercially produced TPEE based on PBT as rigid segments (PBT-type TPEE), a PTT-type TPEE copolymer composed of PTT rigid segments of 75 mol% was synthesized; that is, it has the same compositions of commercially produced PBT-type TPEE (PBT mol% = 75%), and their thermal and mechanical properties were characterized. In Table5, PTT-type TPEE has higher (η) and Mw than those of PBT-type TPEE. Figure 10 shows the DSC melting thermograms of the PTT-type TPEE and PBT-type TPEE samples, and the crystallization parameters are summarized in Table 5. It can be seen that PBT-type TPEE’s DSC curve has higher glass transition temperature (Tg) and melting point (Tm) than those of PTT-type TPEE. Figure 11 shows the DSC crystallization curves of PTT-type TPEE and PBT-type TPEE samples with the crystallization parameters summarized in Table 5. It can be seen that PBT-type TPEE’s crystallization peak value (Tc), and crystallization enthalpy (ΔHc) are both larger than those of PTT-type TPEE, while its FWHP is lower than that of PTT-type TPEE. These results suggest that PBT-type TPEE has higher crystallization temperature and larger crystallization rate and material crystallinity than those of PTT-type TPEE.Table 5
DSC melting and crystallization parameters of the various samples.
Sample
[η] (dL/g)
Mw  (g/mol)
T
g  (°C)
T
m  (°C)
Δ
H
m  (J·g−1)
T
c  (°C)
Δ
H
c  (J·g−1)
FWHP(°C)
PBT-type
0.50
28919
12.6
204.7
29.38
155.2
−35.06
21.2
PTT-type
1.02
60274
−68.1
171.9
31.36
101.6
−21.93
25.7Figure 10
DSC melting curves of two copolymers.Figure 11
DSC crystallization curves of two copolymers.Figure12 shows the TG curves of PTT-type and PBT-type TPEE samples and the parameters are listed in Table 6. It can be seen that PTT-type TPEE has a better thermostability than that of PBT-type TPEE.Table 6
TG parameters and mechanical properties for PBT-type and PTT-type TPEE.
TPEE
T
5
%  (°C)
T
max  (°C)
σ
t  (MPa)
E
a  (MPa)
ε
b  (%)
σ
i  (KJ·m−2)
H  (Sh D)
PBT-type
385.8
428.3
26.0
322
291
9.6
39
PTT-type
370.3
425.7
4.4
24.8
647
51.3
22
aElastic modulus.Figure 12
TG curves of two copolymers.The mechanical properties of PTT-type and PBT-type TPEEs’ tensile curves are shown in Figure13, and the data are also listed in Table 6. It can be seen that PTT-type TPEE’s stress-strain curve is a typical elastic curve with large elongation at breaking point but without yield behavior, while, for that of PBT-type TPEE, it shows a small yield behavior with lower elongation at breaking point. PBT-type TPEE has much larger tensile strength and modulus than those of PTT-type TPEE.Figure 13
The stress-strain curves of two copolymers.Moreover, PTT-type TPEE has much larger impact strength than those of PBT-type TPEE (Table6), and the hardness of PTT-type TPEE is smaller than that of PBT-type TPEE due to its larger crystallinity.As we know, PBT molecular chains are more flexible than that of PTT, and PBT segments can crystallize at fast crystallization rate at high temperature; therefore, PBT-type TPEE has higher melting point than that of PTT-type TPEE. PBT-type TPEE’s high tensile strength and hardness are also due to its larger crystallinity, while PTT-type TPEE’s larger impact strength is due to its lower crystallinity and lower glass transition temperature. However, although this PTT-type TPEE has large impact stress, it is not suitable to be used as a commercial TPEE with this mole ratio of rigid and soft segments because of its low tensile strength. PTT-type TPEE containing less than 25 mol% PTMEG may be more suitably served as thermoplastic elastomer because of its high melting point, fast crystallization rate, and a relatively lower glass transition temperature.


## 3.1. Chemical Structure of PTT-PTMEG Copolymers

The FTIR spectra of PTT-PTMEG copolymer is shown in Figure1. The vibration at 1712 cm−1 corresponds to C=O stretching vibration of the terephthalate units. Those vibrations at 1265 and 1132 cm−1 correspond, respectively, to C–O–C asymmetric and symmetric stretching vibration. The vibration at 726 cm−1 corresponds to –CH2– rocking vibration of the PTMEG units and those vibrations at 2951 cm−1 and 2856 cm−1 correspond, respectively, to –CH2– asymmetric and symmetric stretching vibration. The vibrations at 1503 and 1463 cm−1 correspond to C=C stretching vibration of the phenyl group, and those vibrations at 1018 and 829 cm−1 correspond, respectively, to the C–H out-plane and in-plane deformation vibration of paradisplacement benzene ring.Figure 1
FTIR spectra of PTT-PTMG copolymer.The1H NMR spectra of PTT-PTMEG copolymers is shown in Figure 2. In 1H NMR spectra, the chemical shifts at 2.58 ppm (peak a; 2H, C–CH2–C) and at 4.84 ppm (peak b; 4H, O–CH2–C) were mainly the methylene protons of the short chain diol (PDO). The signals at 8.31 ppm (peak c; 4H) correspond to the aromatic proton of the terephthalate units. The chemical shifts at 3.74 ppm (peak e; O–CH2–C) and at 1.7 ppm (peak f; C–CH2–C) were for the methylene protons of the PTMEG repeating blocks. Small signals at 4.55 ppm (peak h; COO–CH2–C) correspond to the methylene protons neighboring to the ester group in the chain of PTMEG. The signals at 11.5 ppm correspond to the proton of TFA as a solvent.Figure 2
1H NMR spectra of PTT-PTMEG copolymers.PTT-PTMEG copolymer can be presented as linear multiblock copolyester composed of rigid and soft units. It gives possibility to calculate the degree of polymerization of the rigid segment, and the rigid segment content has been calculated based on the conventional soft segments definition, which includes one terephthalate unit (T) with each PTMEG sequence and called PTMEG-T as illustrated in Scheme1. In Scheme 1, x is the degree of polymerization of the rigid segment (where y=1, n=13.6). The weight and mole fraction of rigid and flexible segments were calculated from the 1H NMR spectra according to (1)–(3) and are listed in Table 2. The average length of the rigid PTT segments was also calculated from the ratio (b : h in Figure 2) of the peak intensities, based on the assumption that flexible segment length is equal to the length of starting PTMEG. The calculated degree of polymerization of the PTT segments (x) in the macrochain from 1H NMR spectra was between 24.1 (C1) and 2.3 (C3). For all the samples with exception of C1, the difference between the experimental (Exp) and theoretical (Theo) composition was less than 2%. Consider
(1)x=bh,(2)n=eh,(3)PTT(mol%)=x(1+x).Table 2
The composition of the synthesized PTT-PTMEG copolymers determined from1H NMR spectra.
PTT/PTMEG(wt%/wt%)
PTT(mol%)
PTT(wt%)
x
PTMEG(mol%)
PTMEG(wt%)
n
Theo
Exp
Theo
Exp
Theo
Exp
Theo
Exp
Theo
Exp
Theo
Exp
C1-83/17
96.0
94.8
81.5
76.9
24.1
18.2
4.0
5.2
18.5
23.1
13.6
11.2
C2-66/34
90.0
89.2
62.1
60.1
9.0
8.3
10.0
10.8
37.9
39.9
13.6
12.6
C3-40/60
70.0
71.4
29.8
31.3
2.3
2.4
30.0
28.6
70.2
68.7
13.6
11.9The results from FTIR and1H NMR measurements for the PTT-PTMEG copolymers suggest that the products are basically consistent with our expected chemical structures, as shown in Figure 2.


## 3.2. Melting and Crystallization Behaviors

Figure3 shows the glass transition temperatures of the various copolymers, and the parameters are listed in Table 3. It can be seen in Figure 3 that C0 (pure PTT) and C1 only show one glass transition (Tg1) and a cold-crystallization peak (Tcc) in each DSC curve, in which Tg1 and Tcc of C1 are much lower than those of C0, while, for C2 and C3, they both show two glass transitions (Tg1 and Tg2) but without any cold-crystallization behavior. In Table 3, C0 has the largest value of Tg1 among these samples, while Tg1s of C1, C2, and C3 decrease slightly; additionally, C3 has a larger Tg2 than that of C2. There may be a mixed amorphous phase of PTT and PTMEG (Tg1s of C2 and C3 that are lower than that of C0) and an amorphous PTMEG phase (Tg2) occurred in the materials, so they both show two glass transitions in C2 and C3 copolymers.Table 3
DSC melting and crystallization parameters of the various samples.
PTT/PTMEG(wt%/wt%)
First heating process
Cooling process
T
g
1 (°C)
T
g
2 (°C)
T
cc (°C)
T
re (°C)
Δ
H
re (J·g−1)
T
m
1 (°C)
T
m
2 (°C)
Δ
H
m (J·g−1)
T
c (°C)
Δ
H
c (J·g−1)
FWHP(°C)
C0-100/0
—
49.3
67.8
199.3
−7.05
—
229.2
62.01
202.8
−57.88
8.6
C1-83/17
—
26.4
49.7
188.3
−5.37
208.6
221.8
48.96
191.4
−41.69
8.7
C2-66/34
−64.5
24.7
—
166.7
−3.48
199.8
206.7
42.41
185.3
−40.83
12.7
C3-40/60
−67.7
22.5
—
—
—
—
180.7
25.19
160.8
−15.81
13.9Figure 3
Glass transitions of the various copolymers.Figure4 shows the DSC melting thermograms of the various samples with the crystallization parameters summarized in Table 3. It can be seen from Figure 4 and Table 4 that these DSC curves have one or two asymmetrical melting peaks (Tm1, Tm2), and they tend to be narrow and shift to higher temperature with increasing PTT content in the copolymers because more PTT content will improve the regularity of molecular chains and the crystallizability of the copolymer; that is to say, when the PTT content increases, the longer rigid and crystallizable chain segments will form in the copolymers, so the longer and rigid segments will crystallize into larger crystals and they will melt at higher temperature. The multiple melting peaks behavior may be due to the different kinds of the copolymers formed with different length of rigid segments. The melting enthalpy (ΔHm) also decreases greatly with increasing PTEMG content in the copolymers.Table 4
Parameters of the TGA curves for the various samples.
PTT/PTMEG(wt%/wt%)
T
2
%  (°C)
T
5
%  (°C)
T
max  (°C)
W
600
°
C  (%)
η
0
*  (Pa·s)
σ
t
a  (MPa)
ε
b
b  (%)
σ
i
c  (KJ·m−2)
H
d  (Sh D)
C0-100/0
343.8
369.0
406.5
0.69
345.1
30.4
33.3
7.6
76
C1-83/17
345.8
367.9
409.9
0.75
230.2
11.4
249.1
16.5
58
C2-66/34
324.3
362.4
408.0
0.83
168.8
8.7
398.6
28.8
41
C3-40/60
274.8
351.3
408.0
0.26
111.5
5.8
589.1
47.2
26
aTensile strength.
bElongation at breaking point.
cImpact strength.
dShore hardness.Figure 4
DSC first melting thermograms of the various samples.In addition, except for the sample C3, each of the curves exhibits a recrystallization peak (Tre) before the melting peak, which shifts to higher temperature with increasing PTT rigid segments content. This result is also correlated to the molecular structure of the copolymer. Because the sample with more PTMEG content has lower crystallizability, some microcrystallites with lower perfection and smaller size will form in the material; these microcrystallites will melt and recrystallize at low temperatures in the heating process. The sample C3 having the most PTMEG contents in the copolymer shows no recrystallization peak because of its lowest crystallizability. The recrystallization enthalpy (ΔHre) also decreases with increasing PTMEG content in the copolymers. On the other hand, in the DSC curves of C2 and C3, the melting peaks are shown with much wide distribution, indicating that the length of the rigid segments may have a wide distribution in the copolymers and they form spherulites with different sizes that melt at different temperatures.Figure5 shows the DSC melt-crystallization curves of the various samples and their crystallization parameters were summarized in Table 3. As seen from Figure 5, except for C3, each of the curves is shown with good symmetrical crystallization peak, and they also tend to be narrow and shift to high temperature with increasing PTT contents. The crystallization enthalpy (ΔHc) also increases with increasing PTT contents. Moreover, the full width at half-height of the crystallization peak (FWHP) decreases as PTT content increases. It can be concluded that the sample with higher PTT content has higher onset-crystallization temperature and faster crystallization rate. Their crystallization behaviors are also correlated to the content of the rigid segments, as explained above. The sample C3 has an unobvious crystallization peak mainly because of its lower crystalline content of rigid PTT.Figure 5
DSC crystallization curves of the various samples.From the above results of glass transitions, cold-crystallization, melting points, and crystallization behaviors of the various copolymers, we may give the following conclusions: (1) there may be four different domains in the copolymers: a crystalline PTT phase, an amorphous PTT phase, an amorphous PTMEG phase, and a mixed amorphous phase depending on the sample composition. When PTMEG content is 17 wt% (C1), a mixed amorphous phase shows lowerTg2 and Tcc than those of C0; when PTMEG contents are 34 wt% (C2) and 60 wt% (C3), both a mixed amorphous phase and an amorphous PTMEG phase occur in the materials, so they both show two glass transitions (Tg2 and Tg1). The presence of four different domains depends on the thermal history and composition in the elastomers based on PET and PEO which have been observed by Fakirov et al. [22]. (2) When the PTT-PTMEG copolymers contain above 34 wt% of soft segments, low-temperature glass transition and a high melting point can be observed, thus the microphase separation structure occurred in the copolymers, which are two important characters for the thermoplastic elastomers.


## 3.3. Spherulite Morphology

Figure6 shows the spherulite morphology of the various samples. As seen in Figure 6(a), the spherulites of PTT are fairly large with perfect Maltese cross extinctions, while for C1 (Figure 6(b)), it exhibits a relatively well-defined spherulitic texture with Maltese cross extinctions but with small spherulite size; additionally, some microspherulites are observed in some area. As shown in Figures 6(c) and 6(d), C2 and C3 images exhibit large number of small bright spots, and nearly no clear Maltese cross extinctions can be observed, indicating that only some microcrystallites can be formed in these samples. The above results suggest that the spherulite size of PTT-PTMEG copolymers decreases with the decreasing contents of rigid PTT segments. We believe that the crystallization behavior of PTT segments is limited by the soft PTMEG segments, and PTMEG and some uncrystallized PTT form the amorphous phase in the material.Figure 6
POM micrographs of crystallized samples (a) C0; (b) C1; (c) C2; and (d) C3.


## 3.4. Thermal Stability

Figure7 shows the TG curves of the various samples and the parameters are listed in Table 4. It can be seen that each curve has one predominant degradation stage. The temperatures at weight losses of 2% (T2%) and 5% (T5%) decrease with increasing soft PTMEG segments, while the fastest thermolysis temperatures (Tmax) and the residues weight (W600°C) are nearly the same at 600°C. These results suggest that the thermal stability of the copolymers becomes worse with more soft PTMEG content.Figure 7
TG curves of the various samples.


## 3.5. Rheology Behaviors

Figure8 is the plots of complex viscosity versus frequency (η*-ω) of different samples. For PTT, its complex viscosity remains nearly stable as ω<102 rad/s, indicating that PTT melt is Newtonian liquid at low shearing frequencies, while it turns into pseudoplastic fluid as ω<102 rad/s. In the low shearing frequencies range, the entangling rate and unentangling rate of molecular chains achieve a dynamic balance, so the complex viscosity presents a platform. When the shearing frequency exceeds a critical value, the unentangling rate is faster than entangling rate, so the complex viscosity decreases. On the other hand, it can be seen from Figure 8 that the copolymer with more PTMEG content has larger zero shear viscosity (η0*) values (Table 4), suggesting that the copolymer with more flexible segments can form more entangled points in the polymer. For three copolymers, their η* slowly decreases first, then remains stable and then decreases at high shearing frequency. Because PTT-PTMEG copolymers have more flexible segments than that in pure PTT, there are more entangled points in the copolymers, and some entangled points are easily destroyed at low shearing frequency, so the η* decreases at low frequencies range and the more the flexible PTMEG contents in the copolymers, the more sharply the decrease of η*. The three copolymers are pseudoplastic fluids at low shearing frequencies. At high frequencies, their η* values are close to each other due to the high shearing rate which makes most entangled points unentangle.Figure 8
Curves ofη* versus ω of the various copolymers.


## 3.6. Mechanical Properties

The mechanical properties of the various copolymers are tested and their stress-strain curves are shown in Figure9 and the data are listed in Table 4. It can be seen that the tensile strength decreases while the elongation at breaking point increases with increasing flexible segments (Table 4). These results are mainly because of the decrease of the crystallinity in the copolymers. On the other hand, as shown in Table 4, the impact strength increases and the Shore hardness decreases with increasing soft PTMEG segments in the copolymers.Figure 9
The stress-strain properties of PTT-PTMEG copolymers.


## 3.7. Comparison of PTT-Type TPEE and PBT-Type TPEE

In this part, in order to compare the properties of the copolymer based on PTT as rigid segments (PTT-type TPEE) to the commercially produced TPEE based on PBT as rigid segments (PBT-type TPEE), a PTT-type TPEE copolymer composed of PTT rigid segments of 75 mol% was synthesized; that is, it has the same compositions of commercially produced PBT-type TPEE (PBT mol% = 75%), and their thermal and mechanical properties were characterized. In Table5, PTT-type TPEE has higher (η) and Mw than those of PBT-type TPEE. Figure 10 shows the DSC melting thermograms of the PTT-type TPEE and PBT-type TPEE samples, and the crystallization parameters are summarized in Table 5. It can be seen that PBT-type TPEE’s DSC curve has higher glass transition temperature (Tg) and melting point (Tm) than those of PTT-type TPEE. Figure 11 shows the DSC crystallization curves of PTT-type TPEE and PBT-type TPEE samples with the crystallization parameters summarized in Table 5. It can be seen that PBT-type TPEE’s crystallization peak value (Tc), and crystallization enthalpy (ΔHc) are both larger than those of PTT-type TPEE, while its FWHP is lower than that of PTT-type TPEE. These results suggest that PBT-type TPEE has higher crystallization temperature and larger crystallization rate and material crystallinity than those of PTT-type TPEE.Table 5
DSC melting and crystallization parameters of the various samples.
Sample
[η] (dL/g)
Mw  (g/mol)
T
g  (°C)
T
m  (°C)
Δ
H
m  (J·g−1)
T
c  (°C)
Δ
H
c  (J·g−1)
FWHP(°C)
PBT-type
0.50
28919
12.6
204.7
29.38
155.2
−35.06
21.2
PTT-type
1.02
60274
−68.1
171.9
31.36
101.6
−21.93
25.7Figure 10
DSC melting curves of two copolymers.Figure 11
DSC crystallization curves of two copolymers.Figure12 shows the TG curves of PTT-type and PBT-type TPEE samples and the parameters are listed in Table 6. It can be seen that PTT-type TPEE has a better thermostability than that of PBT-type TPEE.Table 6
TG parameters and mechanical properties for PBT-type and PTT-type TPEE.
TPEE
T
5
%  (°C)
T
max  (°C)
σ
t  (MPa)
E
a  (MPa)
ε
b  (%)
σ
i  (KJ·m−2)
H  (Sh D)
PBT-type
385.8
428.3
26.0
322
291
9.6
39
PTT-type
370.3
425.7
4.4
24.8
647
51.3
22
aElastic modulus.Figure 12
TG curves of two copolymers.The mechanical properties of PTT-type and PBT-type TPEEs’ tensile curves are shown in Figure13, and the data are also listed in Table 6. It can be seen that PTT-type TPEE’s stress-strain curve is a typical elastic curve with large elongation at breaking point but without yield behavior, while, for that of PBT-type TPEE, it shows a small yield behavior with lower elongation at breaking point. PBT-type TPEE has much larger tensile strength and modulus than those of PTT-type TPEE.Figure 13
The stress-strain curves of two copolymers.Moreover, PTT-type TPEE has much larger impact strength than those of PBT-type TPEE (Table6), and the hardness of PTT-type TPEE is smaller than that of PBT-type TPEE due to its larger crystallinity.As we know, PBT molecular chains are more flexible than that of PTT, and PBT segments can crystallize at fast crystallization rate at high temperature; therefore, PBT-type TPEE has higher melting point than that of PTT-type TPEE. PBT-type TPEE’s high tensile strength and hardness are also due to its larger crystallinity, while PTT-type TPEE’s larger impact strength is due to its lower crystallinity and lower glass transition temperature. However, although this PTT-type TPEE has large impact stress, it is not suitable to be used as a commercial TPEE with this mole ratio of rigid and soft segments because of its low tensile strength. PTT-type TPEE containing less than 25 mol% PTMEG may be more suitably served as thermoplastic elastomer because of its high melting point, fast crystallization rate, and a relatively lower glass transition temperature.


## 4. Conclusions

A series of poly(trimethylene terephthalate)-b-poly(tetramethylene glycol) (PTT-PTMEG) copolymers can be synthesized by conventional two-step melt polycondensation. By increasing the flexible segment contents, the copolymers show lower glass transition temperatures, melting points, melt-crystallization temperature, less thermostability, lower tensile strength, and smaller spherulites size; however, the complex viscosity, the elongation at breaking point, and impact strength increase with increasing flexible segments. Compared with PBT-type TPEE, PTT-type TPEE has lower glass transition temperatures, melting and crystallization temperature, crystallinity, lower tensile strength, and lower hardness but higher impact stress. PTT-type TPEE containing less than 25 mol% PTMEG may be more suitably served as thermoplastic elastomer.



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*Source: 156289-2013-11-13.xml*