3.1 Characterization of Boz-ph/BMI-80 prepolymers
In order to evaluate the molecular weight and gel time of Boz-ph and Boz-ph/BMI-80 prepolymers, the Boz-ph/BMI-80-100% prepolymers were confirmed by GPC and gel time tester, as given in Fig. 2. As can be seen from Fig. 2a, the weight average molecular weight (Mw) and number average molecular weight (Mn) of Boz-ph/BMI-80-100% prepolymers were 33769 g/mol and 6368 g/mol, respectively. The results indicated that the BMI-80 resin was reacted with the pendant allyl groups of Boz-ph by in-situ polymerization to form the Boz-ph/BMI-80 prepolymers. The gel time of Boz-ph and Boz-ph/BMI-80-100% prepolymers was tested and shown in Fig. 2b. It can be seen that the gel time of Boz-ph prepolymers at 190°C is about 795 s, while the gel time of Boz-ph/BMI-80-100% prepolymers is increased to 1520 s, which is mainly attributed to the introduction of BMI-80 units with low chemical reactivity. Obviously, the gel time of Boz-ph and Boz-ph/BMI-80-100% prepolymers decreased with the further increase of temperature. When the temperature reached 230 ℃, the gel time of Boz-ph and Boz-ph/BMI-80-100% prepolymers decreased 218 s and 280 s, respectively. Compared with pure BMI-80 resin, the gel time of Boz-ph/BMI-80-100% prepolymers was significantly shortened, which is the key parameter during the processing of the resin matrix.
3.2 Curing behavior of Boz-ph/BMI-80 prepolymers
Figure 3a shows the digital images of Boz-ph/BMI-80 prepolymers with 70 wt% (top) and 30wt% (bottom) solid content in DMF solution, respectively. When the solid content is more than 50%, the Boz-ph/BMI-80 system presents a reddish-brown transparent viscous liquid, and there is no precipitation or phase separation during three months of storage. Then, DSC curves were used to study curing behavior of pure BMI-80, Boz-ph and Boz-ph/BMI-80 prepolymers, as shown in Fig. 3b. There are an obvious endothermic peak around 165 ℃ and an exothermic peak near 295 ℃, which belong to the melting peak and curing peak of pure BMI-80. However, the melting point peak of BMI-80 resin did not appear in the DSC curves of Boz-ph/BMI-80 prepolymers, indicating that BMI-80 was involved in the prepolymerization of Boz-ph. Moreover, Boz-ph/BMI-80 prepolymers exhibited two curing peaks, the first peak corresponds to its oxazine ring-opening reaction while the second peak is mainly the exothermic peak of polymerization of phthalonitrile groups and double bonds in the presence of phenol [14]. With the increase of BMI-80 content, the two curing peaks of Boz-ph/BMI-80 prepolymers gradually moved to the high temperature zone, indicating that the introduction of BMI-80 reduces the reactivity of the cross-linking groups. In summary, the Boz-ph/BMI-80 prepolymers exhibited lower curing temperature in comparison with pure BMI-80 resin.
3.3 FTIR characteristics of Boz-ph/BMI-80 resins
The chemical structure of pure BMI-80, Boz-ph prepolymer and Boz-ph/BMI-80 resins were confirmed by FTIR as shown in Fig. 4. As you can see from Fig. 4a, the characteristic absorption peak at 2230 cm− 1 corresponds to the symmetrical stretching vibration of –CN groups [15, 16]. The peaks at 1712 cm− 1 and 1580 cm-1 are assigned to the stretching vibration absorption peak of the carbonyl groups (-C = O) on the imide ring and skeleton vibration peak of benzene rings, respectively. The band at 1245 cm− 1 is the reflection of stretching vibrations of aromatic C–O–C groups, and the bands at 1327 cm-1, 1229 cm-1 corresponding to the vibration peaks of methylene groups and antisymmetric stretching vibration peaks of ether bonds connected with the oxazine rings [17]. The peak at 1158 cm-1 corresponded to the asymmetric contraction vibration peak of C-N-C, and the bands at 947 cm-1and 996 cm-1corresponding to the characteristic absorption peak of oxazine ring and the in-plane bending vibration peak of -C-H on allyl group, which are consistent with previous literature reports [18]. Besides, the characteristic peak at 692 cm-1 is attributed to the = C-H in the maleimide groups [11]. After high-temperature curing in Fig. 4b, the peaks at 947 cm-1, 1229 cm-1 disappeared, indicating that the oxazine ring of benzoxazine had been opened and solidified [19]. Meanwhile, the triazine absorption peaks at 1360 cm− 1 were observed as the result of the curing of nitrile (-CN) groups. Moreover, the depressed absorption peaks of = C-H proved the copolymerization of BMI-80 and Boz-ph resins.
In this work, the Boz-ph was selected as the based matrices to modify BMI-80 resin, which is expected to obtain a kind of thermosets with excellent comprehensive properties. The ring-opening polymerization of benzoxazine rings (seen from Fig. 5a) and ring-forming polymerization of nitrile groups (seen from Fig. 5b) will be very beneficial to improve its thermal stability, mechanical and dielectric properties.
3.4 Morphology of cured Boz-ph/BMI-80 resins
The morphologies of cured Boz-ph and Boz-ph/BMI-80 resins are evaluated by SEM images, as given in Fig. 6. In Fig. 6a and Fig. 6b, cured Boz-ph resin shows a good homogeneous phase structure, indicating that the resin was fractured by rapid crack growth without obvious macroscopic deformation. When the molar ratios of Boz-ph to BMI-80 was designed as 4:1, the Boz-ph/BMI-80-25% resins is still dominated by Boz-ph, and the polymer chain segment formed by the self-polymerization shows brittle fracture (seen from Fig. 6c and Fig. 6d). With the further addition of BMI-80 content, a continuous wavy-like phase structure indicates composite starts to be formed (seen from Fig. 6e-6i), with a shadowy outline of matrix and toughening phase. That is to say, the introduction of BMI-80 units changed the cross-linking structure of the Boz-ph/BMI-80 resins. Whether the pendant allyl groups of Boz-ph were reacted with the double bond of BMI, or the Boz-ph after ring-opening was inserted into the triazine ring to form cyanuric acid ester, and then isomerized to form a more complex interpenetrating network structure (IPN), it can significantly improve the toughness of Boz-ph/BMI-80 resins. Thus, it is can predicted that the Boz-ph/BMI-80 resins will present excellent mechanical properties.
3.5 Mechanical properties of cured Boz-ph/BMI-80 resins
It is well-known that the structure formation of the cross-linking network played a key role in in the comprehensive properties of resins system. Cured Boz-ph/BMI-80 system shows a characteristically black and rigid form, and the mechanical properties are shown in Fig. 7a-b and Table 1. Obviously, the typical stress-strain curve of cured Boz-ph resin suggests a brittle fracture characteristic and similar to the thermosetting-based resins, which is consistent with SEM image in Fig. 6. With the increase of BMI-80 content, the slope of stress-strain curves has decreased slightly, indicating that the rigidity of the Boz-ph/BMI-80 system is weakened. In particular, the flexural strength of Boz-ph/BMI-80 resins significantly increased, it reaches the maximum in Boz-ph/BMI-80-100%. Compared with pure Boz-ph resin (70.1 MPa), the flexural strength of the Boz-ph/BMI-80-100% resins increased by 46.6%. However, the flexural modulus of Boz-ph/BMI-80 resins showed the opposite trend, decreasing first rapidly and then slowly, which can be attributed to two reasons as follows. On the one hand, the allyl groups of Boz-ph react with the C = C of BMI-80 may disrupt the chain packing, increase the free volume, and then lower the cross-linking density; on the other hand, the long chain structure and ether linkage (-O-) of BMI-80 had a positive effect on the toughness of interpenetrating polymer networks (IPN) system [20,21].
Table 1
Mechanical properties of cured BMI-80, Boz-ph and Boz-ph/BMI-80 resins
Samples | Flexural Strength/MPa | Flexural modulus/MPa |
Cured Boz-ph | 70.1 | 3070 |
Boz-ph/BMI-80-25% | 74.8 | 2820 |
Boz-ph/BMI-80-50% | 84.6 | 2540 |
Boz-ph/BMI-80-100% | 96 | 2450 |
Cured BMI-80 | 102.8 | 2400 |
3.6 Thermal properties of the cured Boz-ph/BMI-80 resins
TGA and DTG analysis were used to evaluate the thermal properties of the cured BMI-80, Boz-ph and Boz-ph/BMI-80 resins as shown in Fig. 8 and Table 2. It can be seen from Fig. 8a and Table 2, the cured Boz-ph resin shows good thermal properties, and the T5% (5% weight loss temperature) is up to 385 ℃. Obviously, the introduction of BMI-80 into Boz-ph made Boz-ph/BMI-80 resins shift to a higher temperature. The T5% of Boz-ph/BMI-80-25%, Boz-ph/BMI-80-50% and Boz-ph/BMI-80-100% resins are 387 ℃, 401 ℃ and 402 ℃, respectively, which is due to the highly heat-resistant aromatic heterocyclic cured structure of BMI-80 resin (T5% is up to 477 ℃). Besides, the Tmax (maximum decomposition temperature) was obtained from the peaks of the DTG curves. As shown in Figs. 8b and Table 2, the Tmax of Boz-ph/BMI-80 resins is in the range of 420–468 ℃, which is much higher than that of pure Boz-ph resin (Tmax is only 405 ℃). These results confirmed that BMI-80 could obviously improve the thermal properties of Boz-ph resin.
Table 2
Thermal performance of cured BMI-80, Boz-ph and Boz-ph/BMI-80 resins
Samples | T5%/℃ | Tmax/℃ | Cy800/% |
Cured Boz-ph | 385 | 405 | 69.2 |
Boz-ph/BMI-80-25% | 387 | 420 | 66.7 |
Boz-ph/BMI-80-50% | 401 | 437 | 66.2 |
Boz-ph/BMI-80-100% | 402 | 468 | 60.8 |
Cured BMI-80 | 477 | 491 | 41.9 |
3.7 DMA curves of the cured Boz-ph/BMI-80 resins
Figure 9 shows the relationship curves of the energy storage modulus (E'), loss tangent (tan δ) and temperature of cured BMI-80, Boz-ph and Boz-ph/BMI-80 resins. As can be seen from Fig. 9a and Table 3, when the temperature is 50 ℃, the E' of cured samples of each formula is above 1.6 GPa. With the increase of temperature, the E' of all cured samples gradually decreases due to the gradual relaxation of copolymer network, and the E' drops sharply when the temperature is about 300 ℃. In the cured Boz-ph/BMI-80 resins, it can be clearly seen that the E' of cured Boz-ph/BMI-80-25% is the highest at low temperature. With the addition of BMI-80, the E' of Boz-ph/BMI-80 resins gradually decreases, it reaches the minimum in Boz-ph/BMI-80-100%. This is mainly because cured Boz-ph has higher rigidity than cured BMI-80, and the increase of Boz-ph content will inevitably lead to the increase of rigidity and modulus of Boz-ph/BMI-80 resins. Figure 9b displays the glass transition temperature (Tg, top temperature of tan δ peak) of all samples. Obviously, the Tg of Boz-ph/BMI-80 resins is between 325–333 ℃, which is far more superior Tg than diallylbisphenolA (DBA) modified bismaleimide-triazine (BT) system (Tg=228ཞ316 ℃) [22].
Table 3
Storage modulus and glass-transition temperature (Tg) of cured BMI-80, Boz-ph and Boz-ph/BMI-80 resins
Samples | Initial Storage modulus at 50 ℃ (MPa) | Tg |
Cured Boz-ph | 3619 | 321 |
Boz-ph/BMI-80-25% | 2462 | 325 |
Boz-ph/BMI-80-50% | 2963 | 329 |
Boz-ph/BMI-80-100% | 3123 | 333 |
Cured BMI-80 | 1629 | 343 |
3.8 Dielectric properties and water absorption of cured Boz-ph/BMI-80 resins
The introduction of BMI-80 resin was expected to decrease the dielectric constant and dielectric loss of Boz-ph/BMI-80 resins. The dielectric properties with a function of frequency for cured BMI-80, Boz-ph and Boz-ph/BMI-80 resins were presented in Fig. 10. From Fig. 10a, the dielectric constants (ε) of all samples showed a slightly decrease with frequency in the low frequency region. However, it can be clearly seen that all samples exhibited relatively stable dielectric constants at high frequencies, which will be very potential applications in high-frequency communications. In the Boz-ph/BMI-80 resins, the ε of the cured Boz-ph/BMI-80 decreased gradually with the increase of BMI-80 loading, from 4.16 to 3.51 (at 10 MHz). In addition, the cured Boz-ph/BMI-80 resins exhibited low and relatively stable dielectric loss, and the dielectric loss (tan δ) of Boz-ph/BMI-80-100% was as low as 0.008 (see from Fig. 10b). Besides, the corresponding dielectric constants and dielectric loss of Boz-ph/BMI-80 resins reduce, accompanying the increase of BMI-80 loading, owning to two factors: (1) the molecular structure of Boz-ph contains a large number of polar groups such as allyl and nitrile groups, and the molecular polarity is difficult to offset, resulting in high dielectric constant and dielectric loss; (2) the molecular structure of BMI-80 is symmetrical, the polarity cancels each other out, and the dipole loss is small over a wide temperature range, so it has excellent dielectric properties [23–25].
Furthermore, the water absorption of cured BMI-80, Boz-ph and Boz-ph/BMI-80 resins were tested in boiled water for 12 h, and the results are presented in Fig. 11. It can be seen that the water absorption of cured BMI-80 is as low as 2.1%. The water absorption of Boz-ph/BMI decreased with increasing BMI-80 (less than 2.5%), indicating that the introduction of the alkyl structure (-CH3) increased the hydrophobic nature of Boz-ph/BMI-80.