Open Access Article
Keren
Zhang
,
Ashley M.
Nelson
,
Samantha J.
Talley
,
Mingtao
Chen
,
Evan
Margaretta
,
Amanda G.
Hudson
,
Robert B.
Moore
and
Timothy E.
Long
*
Department of Chemistry, Macromolecules Innovation Institute, Virginia Tech, Blacksburg, VA 24061, USA. E-mail: telong@vt.edu
First published on 19th May 2016
A two-step synthesis of epoxidation and carbonation afforded a hetero-functional AB monomer with cyclic carbonate and methyl ester (CC-ME) using plant oil-based methyl 9-decenoate and CO2. A unprecedented one-pot synthetic platform of CC-ME with 1,12-diaminododecane and poly(tetramethylene oxide) (PTMO)-based polyether diamine allowed synthesis of both nonsegmented poly(amide-hydroxyurethane) (PA12HU) and segmented PA12HU-PTMOs with varying polyether contents. 1H NMR spectroscopy confirmed complete conversion of cyclic carbonates and methyl esters to hydroxyurethanes and amides, respectively. Thermal analysis revealed distinctive thermal stability and transitions of PA12HU and PA12HU-PTMOs compared to their precursors and model oligomers. PA12HU and PA12HU-PTMOs were melt compression molded into semicrystalline, free-standing films, except for PA12HU-PTMO100 with 100% polyether diamine. PA12HU-PTMO100 was a viscous liquid with a glass transition temperature (Tg) of −64 °C and zero-shear melt viscosity of 449 Pa s. PA12HU formed a semicrystalline, rigid film with Tg of 11 °C. Polyether incorporation afforded creasable PA12HU-PTMO films with broad glass transitions near −50 °C. Thermal and thermomechanical analysis revealed significant phase-mixing of the hard and soft segments from annealed PA12HU-PTMO films. Polyether soft segments mixed with the amorphous hard segments, forming a miscible soft phase; crystallizable hard segments with ordered hydrogen bonding formed a hard phase. Surface morphological analysis of each PA12HU-PTMO film displayed ribbon-like, hard domains with composition-dependent aspect ratios. PA12HU-PTMOs exhibited higher moisture uptake than traditional thermoplastic polyurethane (TPU) due to resultant hydroxyls. Variable temperature FTIR spectroscopy demonstrated that ordered hydrogen bonding in the crystalline domains was disrupted or dissociated as the crystallites melted. Although tensile strength of segmented PA12HU-PTMOs proved lower than traditional polyurethanes due to phase-mixing, these compositions represent the first examples of film-forming, linear isocyanate-free polyurethanes with mechanical integrity and processability.
However, progress lags on developing linear or branched NIPUs to compete with conventional thermoplastic polyurethanes (TPUs). Endo and many others ultilized polyaddition of bis(cyclic carbonate)s and diamine to synthesize linear NIPU.1,19–23 Cramail et al. recently reported the synthesis of aliphatic bis(6-membered cyclic carbonate)s using castor oil-based methyl undecenoate. Polymerization of the cyclic carbonates and diamine produced NIPUs with relative Mn values as high as 23 kDa.22 Another study from the same group also used methyl undecenoate to synthesize amide-containing bis(cyclic carbonate), and melt polymerization yielded amide-containing NIPUs. However, the products were blends due to heterogeneous mixtures of amines and cyclic carbonates. Despite many efforts devoted to developing linear NIPUs for thermoplastics, most studies were limited to synthesis, spectroscopic validations, and thermal properties. Only Nanclares et al. very recently reported stress–strain profiles of segmented bisphenol A-based NIPUs with elastomeric properties.24 To our knowledge, a report does not exist for bio-based NIPU thermoplastics with mechanical ductility or detailed morphological analysis.
This manuscript details the synthesis and characterization of nonsegmented and segmented NIPUs with various physical properties, ranging from film-forming solids to viscous liquids. A commercialized biochemical refinery produced methyl 9-decenoate using metathesis reactions of unsaturated fatty acids. Sequential epoxidation and carbonation yielded a cyclic carbonate-methyl ester (CC-ME) monomer, which is a stable solid at room temperature. An one-pot synthetic platform afforded a series of novel bio-based poly(amide hydroxyurethane)s (PAHUs) using CC-ME, an aliphatic diamine, and a polyether diamine. Polymerization proceeded through ring opening of five-membered cyclic carbonates and amidation of the methyl esters, forming both hydroxyurethanes and amides on the polymer backbone. The reported PAHU series spans both nonsegmented and segmented polyurethanes with tunable thermomechanical properties and crystallinity. The segmented PAHUs with aliphatic diamine incorporation were homogeneous melts during polymerization and compression molded into free-standing films. In addition, atomic force microscopy (AFM) and X-ray scattering experiments elucidated the influence of hard segment percentage on the morphology of annealed PAHU films. The PAHU with the highest soft segment percentage was a clear, viscous liquid that displayed shear thinning during rheological shear-sweep experiment. This manuscript represents the first report of bio-based, semicrystalline NIPUs with mechanical integrity, microphase-separated morphology, and processability. Various physical characterization techniques assisted in establishing the structure–morphology–property relationships of PAHUs. This versatile synthetic platform also enables the preparation of a wide variety of NIPUs with tunable properties using many diamines and cyclic carbonate-ester monomers.
Dynamic mechanical analysis (DMA) utilized a TA Instruments Q800 dynamic mechanical analyzer in tension mode at an oscillatory amplitude of 10 μm, a frequency of 1 Hz, and a static force of 0.01 N. Rectangular film samples were cooled to −100 °C, equilibrated for 2 min, length measured, and heated at a rate of 3 °C min−1. The peaks of tan delta curves determined Tg values. A Veeco MultiMode scanning probe microscope provided AFM phase and height images using the tapping mode. Samples were imaged with Veeco's Nanosensor silicon tips with spring constants of 10–100 N at set-point ratios near 0.7. A TA Instruments Q5000 thermogravimetric sorption analyzer (TGA-SA) measured room-temperature water sorption of compression molded PAHU samples at relative humidity (RH) steps from 0–95% RH with 5% increments. Each RH step proceeded until the sample weight equilibrated with less than 0.01% weight change in 10 min. An instrumental pre-drying method at 25 °C and 0% RH was applied to each sample until the weight equilibrated. Water sorption was calculated based on the percentage weight gain of a dried sample. An Instron 5500R universal testing instrument measured tensile properties of several segmented PA12HU-PTMO rectangular film samples at a crosshead speed of 10 mm min−1. Tensile analysis data represented an average of five specimens with calculated standard deviations.
Small angle X-ray scattering (SAXS) and wide-angle X-ray diffraction (WAXD) experiments were performed using a Rigaku S-Max 3000 3 pinhole SAXS system, equipped with a rotating anode emitting X-ray with a wavelength of 0.154 nm (Cu Kα). The sample-to-detector distance was 1603 mm for SAXS and 109 mm for WAXD, and the q-range was calibrated using a silver behenate standard. Two-dimensional SAXS patterns were obtained using a 2D multiwire, proportional counting, gas-filled detector, with an exposure time of 1 h. Two-dimensional WAXD diffraction patterns were obtained using an image plate with an exposure time of 1 h. The SAXS data were corrected for sample thickness, and the SAXS/WAXD profiles were vertically shifted to facilitate a comparison of peak positions. All the SAXS and WAXD data were analyzed using the SAXSGUI software package to obtain radially integrated SAXS and WAXD intensity versus the scattering vector q (SAXS) or 2θ (WAXD) respectively, where q = (4π/λ)sin(θ), θ is one half of the scattering angle and λ is the X-ray wavelength.
Variable temperature FTIR (VT-FTIR) experiments were performed on a Varian 670-IR spectrometer (DTGS detector) with Pike Technologies variable temperature GladiATR™ attachment (diamond crystal). The spectra were collected at 4 cm−1 resolution and as an average of 32 scans. The samples were subjected to a temperature ramp of 1 °C min−1, starting from 30 °C to 180 °C, and FTIR spectra were collected every 10 °C beginning from 30 °C. Rheology experiments were conducted on a TA instrument Discovery AR-G2 rheometer with a cone and plate geometry (20 mm in diameter, 2° cone angle, truncation gap 60 μm). The samples were subjected to a shear sweep ramping from 1 s−1 to 200 s−1. All samples were maintained in a desiccator prior to an experiment.
In the second step, methyl 9,10-epoxydecanoate (4.0 g, 20 mmol), NMP (10 mL), and LiBr (0.087 g, 1.0 mmol) were added into a 100 mL, round-bottomed flask equipped with a magnetic stir bar. The reaction mixture was stirred at 80 °C with constant CO2 bubbling for 24 h. After cooling back to room temperature, the reaction mixture was dissolved in 100 mL EtOAc and washed with 150 mL brine. The organic phase was dried with MgSO4 and rotatory evaporated to remove EtOAc. Resulting light brown oil was dried in vacuo at 50 °C for 24 h and cooled to room temperature to obtain a salmon color solid (4.9 g, 89% yield) (Fig. S2†). 1H NMR (400 MHz, CDCl3, Fig. S2†): 4.67 (m, 1H, Ha), 4.50 (dd, 1H, J1 = 8.2 Hz, J2 = 8.4 Hz, Hb), 4.05 (dd, 1H, J1 = 7.2 Hz, J2 = 8.4 Hz, Hc), 3.65 (s, 3H, Hd), 2.29 (t, 2H, Hf), 1.82–1.55 (m, 4H, Hg), 1.46–1.28 (m, 8H, Hh). 13C NMR (100 MHz, CDCl3): 174.14, 154.98, 76.93, 69.32, 51.44, 33.95, 33.84, 28.92, 28.88, 28.85, 24.77, 24.28. HRMS (ES+): m/z calculated for [M + H]+ 245.1384 g mol−1; found 245.1384 g mol−1. Melting point 36–37 °C.
![]() | ||
| Scheme 3 One-pot melt polymerization of segmented poly(amide-hydroxyurethane) with PTMO-based polyether 1 kDa soft segment (PA12HU-PTMO). | ||
:
88, respectively. Separation of polymers with primary or secondary hydroxyls proved challenging due to the limited solubility in common solvents. The ratio of primary to secondary hydroxyls is tunable through variation of catalyst, reaction temperature, and amine according to Endo et al.19,20
| PA12HU | PA12HU-PTMO10 | PA12HU-PTMO25 | PA12HU-PTMO33 | PA12HU-PTMO50 | PA12HU-PTMO67 | PAHU-PTMO100 | PTMO-diamine | |
|---|---|---|---|---|---|---|---|---|
| PTMO mol% in total amines | 0% | 10% | 25% | 33% | 50% | 67% | 100% | NA |
| Soft segment wt% | 0% | 19% | 39% | 47% | 59% | 68% | 80% | NA |
| T d (°C, 5 wt%) | 272 | 273 | 302 | 296 | 305 | 316 | 319 | 273 |
| T g (°C) | 11 | NA | −44 | −47 | −53 | −59 | −64 | −85 |
| T m (°C) | 113, 128, 152 | 103, 143 | 61, 96, 127 | 54, 90, 139 | 46, 76, 103 | 39, 68, 93 | NA | 9 |
| ΔHm (J g−1) | 98 | 67 | 52 | 41 | 25 | 15 | 0 | 29 |
| Percent of crystallinity (WAXD) | 25 | 19 | 12 | 13 | 9 | 9 | 0 | NA |
A rheological shear-sweep experiment measured melt viscosities of PAHU-PTMO100 and 1 kDa PTMO diamine to be 449 Pa s and 0.2 Pa s at 25 °C, respectively (Fig. S16†). PAHU-PTMO100 started to shear thin near a shear rate of 25 s−1, while 1 kDa PTMO diamine remained in the linear viscoelastic region up to 200 s−1. The higher viscosity and shear thinning reflected the higher molecular weight of PAHU-PTMO100 compared to the 1 kDa precursor. Hydrogen bonding of the urethanes and amides also contributed to higher viscosity and longer relaxation time for PAHU-PTMO. Direct calculation of molecular weight for PAHUs based on melt viscosity proved challenging. PAHU-PTMO100 exhibited miscibility with DMF, but column interactions prohibited the elution of PAHU-PTMO100 from the SEC with a mobile phase of DMF + 0.05 M LiBr. PA12HU-PTMO solids only dissolved in HFIP and TFA, which limited the availability of molecular weight characterization through SEC.
![]() | ||
| Fig. 2 Representative TGA thermograms of nonsegmented PA12HU and segmented PA12HU-PTMOs, along with PTMO-diamine precursor and CC-ME monomer under nitrogen purge. | ||
DSC revealed thermal transitions of PA12HU and PA12HU-PTMOs, comparing to PTMO diamine (Fig. 3), CC-ME monomer (melting point 36–37 °C), and trimers (Fig. S14†). The differences between their thermal transitions again confirmed polymer formation. Table 1 summarizes compositions and thermal properties of PA12HU and PA12HU-PTMOs. Heat of fusion (ΔHm) was normalized against weight percent of the hard segments. PA12HU showed a Tg of 11 °C and multiple melting exothermic peaks, indicative of a semicrystalline polymer. The complex melting exotherms presumably resulted from different crystalline structures, due to possible differences in packing of the dodecane units flanked when by amides or hydroxyurethanes. However, other explanations such as recrystallization of imperfect crystals and re-melting lamellae with different thicknesses should not be ruled out without further investigation.31 Bidentate hydrogen bonding of amide and urethane units generally assists crystallization in polyamides and polyurethanes, respectively.28 The highest melting point of PA12HU was significantly lower than typical polyamide melting points (180–270 °C),32 due to hydroxyurethane units disrupting the long range periodic packing of polyamide segments. Shorter amide segment length generally results in thinner lamellae with lower melting points. The primary hydroxyls and secondary hydroxyls on the polymer chains also possibly interfered with chain packing, as most reported poly(hydroxyurethane)s are amorphous.10
![]() | ||
| Fig. 3 Representative DSC thermograms of nonsegmented PA12HU and segmented PA12HU-PTMOs, compared with PTMO-diamine 1 kDa. | ||
DSC thermograms of segmented PA12HU-PTMOs contained melting exotherms except for amorphous PAHU-PTMO100 (Fig. 3). However, the ΔHm values were significantly lower than the nonsegmented PA12HU (Table 1). Furthermore, ΔHm decreased with increasing soft segment content. This discussion only involves qualitative comparisons due to unknown ΔHm for fully crystalline PAHU. Although the DSC profile of PTMO-diamine showed an exothermic melting peak near 0 °C, PA12HU-PTMOs did not display any thermal transition indicative of crystallinity of the soft segments. Polymer formation and relatively low polyether molecular weight (1 kDa) hindered the crystallization of the soft segments, as commonly seen in segmented polyurethanes and polyamides.27,33,34 Higher polyether incorporations led to lower crystallinities and melting temperatures, mainly due to a dilution effect of crystallizable hard segments.35,36 Hydrogen bonding in close proximity typically proves more effective in forming ordered structure due to cooperative effect. Flexible polyether segments between the hydrogen bonding groups resulted in shorter hard segment lengths and therefore weaker neighboring cooperative effects. This interference strengthened when the hard segments phase-mixed with polyether segments.
Amorphous PAHU-PTMO100 showed a single Tg at −63 °C, nearly 20 °C higher than the PTMO diamine (Tg = −85 °C), indicative of complete phase-mixing of polyether segments and urethane/amide-containing segments. Hydrogen bonding of the urethanes and amides resulted in higher Tg of PAHU-PTMO100 relative to PTMO diamine. Tg values of segmented PA12HU-PTMOs increased and broadened with increasing hard segment content, indicative of phase-mixing (Fig. S15†). This phase-mixing likely resulted from relatively short polyether segment (low degree of polymerization, N), similar polarity of hard segments and polyether segments (small Flory–Higgins interaction parameter, χ), or both.37 Yu et al. observed similar phase-mixing properties of segmented polyamides with 460 g mol−1 poly(propylene oxide) soft segment.31 The aliphatic spacers in CC-ME monomer and 1,12-diaminododecane contributed to more hydrophobic hard segments of PA12HU-PTMOs than conventional segmented polyurethanes, which commonly utilize butane diol or ethylene glycol as chain extenders.
DMA investigated the thermomechanical properties of segmented PA12HU-PTMOs from −100 °C to 100 °C (Fig. 4). All compression molded films showed similar moduli in the glassy region below −70 °C. Modulus curves started to drop near −60 °C, representing onset of the glass transition. The following gradual decreases of moduli and broad tan delta peaks indicated significant phase-mixing of the soft segments and the amorphous hard segments, which agreed with the DSC results. Tan delta peaks shifted to lower temperature with increasing polyether contents, attributed to increasing low-Tg component of the amorphous phase. The crystalline phase maintained the mechanical integrity for PA12HU-PTMO films, affording small plateau regimes from 0 °C to 40 °C, which became more distinguishable at higher polyether contents. Crystalline domains of segmented PA12HU-PTMO films served as reinforcing fillers to preserve the modulus level with increasing temperature until the onset of melting. The final drop in moduli corresponded to crystallites melting, and the observed temperature agreed well with melting temperatures from DSC.
Comparing the series of PA12HU-PTMOs with varying soft segment contents, samples with higher polyether mol% exhibited lower moduli and bigger tan delta peaks. The magnitude of tan delta peak generally correlates to the relative amount of the amorphous phase, which undergoes glass transition.31 PA12HU-PTMOs with higher polyether contents proved less crystalline, demonstrating a similar trend to the DSC results (Table 1). Increasing soft segment also led to earlier onset of flow due to reduction in both crystallinity and hydrogen bonding. Two broad tan delta peaks of PA12HU-PTMO10 near −70 °C and 10 °C suggested the presence of phase-separation. The tan delta peak of PA12HU-PTMO67 also contained a shoulder around 0 °C. However, phase-mixing still dominated the thermomechanical properties of PA12HU-PTMOs. Annealing at 130 °C afforded insignificant effects on the DMA results for PA12HU-PTMO films.
![]() | ||
| Fig. 5 SAXS for compression molded films of nonsegmented PA12HU and segmented PA12HU-PTMOs after annealing at 130 °C for 12 h. | ||
![]() | ||
| Fig. 6 WAXD for compression molded films of nonsegmented PA12HU and segmented PA12HU-PTMOs after annealing at 130 °C for 12 h. Curves were shifted vertically for visual clarity. | ||
WAXD further enabled characterization of the degree of crystallinity of annealed PA12HU and PA12HU-PTMO films (Fig. 6). Prominent crystalline peaks were observed for nonsegmented PA12HU, and WAXD measurements were taken at room temperature, above the Tm of pure PTMO (Table 1). Therefore, these peaks corresponded to the crystalline order of the poly(amide-hydroxyurethane) segment in PA12HU-PTMO films. As shown in Fig. 6, these crystalline reflections appeared at 6.5°, 20.0°, and 23.0°. Table 1 summarizes the degree of crystallinity, Xc, calculated for each copolymer using the WAXD data. Crystalline peaks were deconvoluted using a fit of Gaussian and Lorentzian functions with minimized residuals (Fig. S18†). The ratio of combined area under the three crystalline peaks to total area determined the degree of crystallinity. As expected, the degree of crystallinity in the segmented block copolymer decreased with increasing polyether content (i.e. a decrease in the amount of the crystallizable hard segment).
Atomic force microscopy (AFM) commonly applies to surface morphological characterization of segmented polyurethanes and polyamides.38Fig. 7 reveals the microphase-separated surface morphologies of annealed PA12HU-PTMO films. The light areas represented the hard, crystalline domains, and the dark areas represented the amorphous, soft domains, which contained intermixed polyether segments and non-crystallized hard segments. All PA12HU-PTMO samples displayed ribbon-like crystalline domains on the surface. AFM images of nonsegmented PA12HU showed a continuous crystalline matrix with isolated amorphous domains (Fig. S17†), which explained its rigidity. The incorporation of polyether segments contributed to densely packed ribbons for PA12HU-PTMO25 and PA12HU-PTMO33. With increasing soft segment content, the crystalline phase formed more loosely packed ribbons randomly dispersed in the amorphous matrix for PA12HU-PTMO50 and PA12HU-PTMO67. The wider-field images more clearly depicted the general trend of light, crystalline phase shrinking with increasing polyether incorporation, agreeing with both DSC and WAXD results. The width of these ribbons appeared rather constant with changing hard segment contents, likely due to the chain-folding mechanism.39 However, the lengths of crystalline ribbons appeared to increase with decreasing hard segment content from PA12HU-PTMO10 to 50. Increasing the content of polyether incorporation in the mixed amorphous phase led to lower Tg and higher chain mobility, which facilitated long-range packing of the crystallizable hard segments. The increasing lengths of the crystalline domains compensated for their loosening distribution as polyether content increased, which explained the relatively constant interlamellar spacing observed from SAXS. When polyether content increased beyond 50 mol%, the hard segment content proved insufficient to form one-micron size ribbons, accounting for the shorter crystalline domains in PA12HU-PTMO67. The crystalline domains of PA12HU-PTMO67 displayed more curvature, which explained the disappearance of the scattering peak in Fig. 5 for the SAXS profile of PA12HU-PTMO67.
![]() | ||
| Fig. 7 AFM phase images of compression molded segmented PA12HU-PTMOs after annealing at 130 °C for 12 h. | ||
O and N–H units of amides and urethanes form hydrogen bonds, their signature infrared absorption frequencies shift due to bond length changes. In poly(amide-hydroxyurethane), the hydroxyls also provide hydrogen bonding donors and acceptors. VT-FTIR is a valuable tool for monitoring hydrogen bonding association and dissociation with changing temperature.40–42Fig. 8a demonstrates VT-FTIR spectra of nonsegmented PA12HU in the 1500–1700 cm−1 region with increasing temperature from dark to light curves. This carbonyl stretching region contains three distinctive contributions: ordered hydrogen bonded, disordered hydrogen bonded, and free (non-hydrogen bonded) carbonyls near 1624 cm−1, 1645 cm−1, and 1670 cm−1, respectively. Hydrogen bonding formation results in the red shift of C
O stretching vibration band, due to bond lengthening.40 Increasing temperature leads to a blue shift of the C
O stretching vibration band to higher frequency when hydrogen bond weakens or dissociates. In Fig. 8a, a sharp absorption band near 1624 cm−1 decreased with increasing temperature and a broad band gradually increased at higher frequency, indicating a blue shift due to hydrogen bond weakening and dissociation. This onset occurred near 100 °C, which correlated to the melting onset of nonsegmented PA12HU in Fig. 3. Melting of PA12HU finished near 170 °C in DSC, when the ordered hydrogen bonded carbonyl absorption disappeared completely. This indicated that ordered hydrogen bonded carbonyls existed mostly within the crystalline domains. Disordered hydrogen bonded and free carbonyls became predominant above 170 °C due to melting of the crystallites. N–H bending absorption red-shifted to lower frequency with decreasing intensity due to weakening hydrogen bonding as temperature increased.40,42,43Fig. 8b illustrates that N–H and O–H stretching vibration bands shifted to higher wavenumbers with increasing temperature, attributed to hydrogen bond weakening. A decrease in the absorption coefficient accounted for the dramatic band intensity decrease due to hydrogen bonding weakening.42 Segmented PA12HU-PTMO50 exhibited a similar phenomenon in Fig. 9. The absorption band of ordered hydrogen bonded carbonyls blue-shifted with increasing temperature. This shift started above 30 °C until ordered hydrogen bonded carbonyl band disappeared near 120 °C, which matched closely to the melting range of PA12HU-PTMO50 in Fig. 3. VT-FTIR revealed the melting point difference between segmented PA12HU-PTMO50 and nonsegmented PA12HU. The FTIR spectrum of PA12HU-PTMO50 at 30 °C contained a more obvious, relatively broader shoulder from the disordered hydrogen bonded and free carbonyls, compared to nonsegmented PA12HU at 30 °C. Polyether incorporation disrupted ordered hydrogen bonding formation, and resulted in a higher percentage of disordered and free hydrogen bonding donors and acceptors for PA12HU-PTMO50.
![]() | ||
| Fig. 8 Variable temperature FT-IR spectra of nonsegmented PA12HU (a) in the 1500–1700 cm−1 region and (b) in the 3000–3500 cm−1 region. | ||
![]() | ||
| Fig. 9 Variable temperature FT-IR spectra of segmented PA12HU-PTMO50 (a) in the 1500–1700 cm−1 region. | ||
![]() | ||
| Fig. 10 Equilibrium water sorption of nonsegmented PA12HU and segmented PA12HU-PTMOs in relative humidity steps from 0% to 95%. | ||
![]() | ||
| Fig. 11 Stress–strain curves of compression molded segmented PA12HU-PTMOs with 25–50 mol% soft segments. | ||
| Young's modulus (MPa) | Strain at break (%) | Stress at break (MPa) | |
|---|---|---|---|
| PA12HU-PTMO25 | 94.2 ± 24.5 | 25 ± 8 | 5.7 ± 0.4 |
| PA12HU-PTMO33 | 108.8 ± 8.1 | 21 ± 6 | 5.3 ± 0.5 |
| PA12HU-PTMO50 | 26.5 ± 2.3 | 51 ± 4 | 2.1 ± 0.0 |
A scalable, two-step synthesis converted methyl 9-decenoate to CC-ME monomer using CO2. A one-pot melt polymerization of CC-ME with diamines afforded synthesis of isocyanate-free PAHUs. Diaminododecane reacted with CC-ME to synthesize nonsegmented PA12HU, a semicrystalline copolymer with Tg of 11 °C and multiple melting exotherms at 100–150 °C. Incorporation of a low Tg 1 kDa polyether diamine added flexibility to segmented PA12HU-PTMOs. Segmented PA12HU-PTMOs exhibited broad glass transitions near −60 to –50 °C and lower crystallinity compared to nonsegmented PA12HU. Increasing ratio of polyether diamine to dodecane diamine resulted in lower crystallinity and lower melting point of PA12HU-PTMO due to shorter and fewer hard segments. Both DSC and DMA results indicated significant phase-mixing of polyether segments and the hard segments. Crystallizable hard segments formed crystalline domains, supporting mechanical strength of compression-molded PA12HU-PTMO films. The ribbon-like crystalline domains of PA12HU-PTMOs displayed constant width and varying lengths with different extent of polyether incorporation. VT-FTIR proved that most ordered hydrogen bonded carbonyls existed within the crystalline domains. The carbonyl vibration band shifts occurred in the same temperature range with melting of the crystalline domains of PA12HU or PA12HU-PTMOs. PA12HU exhibited minimal water uptake due to relatively high crystallinity. PA12HU-PTMOs showed slightly higher water uptake than conventional segmented polyurethanes. Reported poly(amide-hydroxyurethane)s displayed similar thermal degradation temperature as conventional polyurethanes, however lacked tensile strength due to their phase-mixed morphologies and possibly low molecular weights.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c6gc01096b |
| This journal is © The Royal Society of Chemistry 2016 |