Morphology characteristics
The morphology of electronspun NC-based composite fibers characterized by SEM and TEM were shown in Fig. 3. The optical photographs of electronspun NC-based composite fibers were shown in Fig. 4.
It can be seen from Fig. 3 that all NC-based composites were composed of cross overlapped fibers with the order of hundreds of nanometers microscopically. Many fiber bundles can be found in SEM images of samples 1–3 containing ADN, However, single fibers with smooth surface can be seen for sample 4 without ADN. As shown from TEM images in Fig. 3, solid particles were found to be imbedded in NC matrix. Macroscopically, as shown in Fig. 4 (a-c), NC-based composites with fluffy 3D macrostructure were fabricated by addition of ADN, and had cotton-like shapes. However, the electropspun NC without ADN is just a 2D web (Fig. 4d). The vertical growth of fibers can be seen and many tiny fibers were formed on the outside of needle outlet (Fig. 4e).
Traditionally, the electrical field force overcame the surface tension and dragged the drops forward flying to the collector. In this process, as the solvents evaporated quickly, the gradually dried fibers reached to the collector and overlapped layer by layer forming a non-woven fabric. Although the mechanism of promoting the formation of 3D macrostructure by addition of ADN is still under exploration, the following points can be ascertained (Akos et al.2020). Firstly, the surface tension would be reduced much compared to the spun solution without ADN addition. Furthermore, the surface charge would be increased much compared to the spun solution without ADN addition. Last but not the least, the solution conductivity would be improved a lot. Those factors synergistically improve the repulsion force on the liquid surface, which caused the difficult formation of the Tyler cone and the stable jet flow like in traditional electrospinning. Phenomenally, as shown in Fig. 4 (e), the jet containing ADN preferred to disperse into MANY tiny jets at the needle outlet, which accelerated the vaporization of solvent. The electrostatic repulsion on the jet surface and the gradually dried fibers made the jets and the fibers scatter haphazardly, which resulted in the solvent vaporization completely ahead of time a lot before the fiber reached to the collector, finally contributed to the formation of fluffy 3D macrostructure.
Thermal behaviors under linear heating conditions
The thermal behaviors of samples 1–4 under linear heating rate of 10 oC/min were tested, the DSC curves were shown in Fig. 5, and the peak temperature data of the main decomposition processes were listed in Table 2.
Table 2
Characteristic data for the thermal decomposition of NC-based samples
sample
|
The first exothermal peak temperature pertaining ADN (℃)
|
The second exothermal peak temperature pertaining to NC (℃)
|
The third exothermal peak temperature pertaining to additives (℃)
|
1
|
178.9
|
201.5
|
227.3
|
2
|
184.5
|
204.3
|
235.4
|
3
|
185.7
|
202.1
|
—
|
4
|
—
|
209.0
|
—
|
It can be seen from Fig. 5 that the melting point of ADN and RDX disappeared for NC-based electrospun samples, compared to the DSC curves of ADN and RDX, which can be attributed to ADN and RDX particles were imbedded in the fluffy NC nanometric fibers (Fig. 4). Compared to pure NC, the thermal decomposition peak temperature (Tp) of NC in sample 4 moved forward by 1.1 oC, much less than decrement of electrospun NC fiber reported (Yang et al. 2020), indicating that the thermal stability of NC fibers obtained by traditional electrospinning can be retained. For samples 1-3 containing ADN, the Tp of ADN decreased from 189.0 oC to 178.9 oC, 184.5 oC or 185.7 oC, respectively, compared to pure ADN. The Tp of NC decreased from 210.1 oC to 201.5 oC, 204.3 oC or 202.1 oC, respectively, compared to pure NC. The Tp decrease indicated that reactions happened between ADN and NC in heating. It can be seen that the Tp of NC+ADN decreased by 24.2 oC compared to pure NC, and 3.1 oC compared to pure ADN, which showed that the intensive interactions exited between ADN and NC. Compared the DSC curves of sample 3 to that of NC+ADN mixture, it can be seen that an unique Tp 185.9 oC appeared in the DSC curves of NC+ADN mixture, however, two Tp corresponding to ADN (185.7 oC ) and NC (202.1 oC) appeared in that of sample 3. The difference between these two samples with the same components may be caused by the different NC/ADN mass ratio in samples. The same phenomenon can be observed for sample 1 and 2. The addition of ADN, exactly the intensive interactions between ADN and NC was recognized as the main reason for the Tp decrease of ADN and NC in sample 1, 2 and 3. The Tp of RDX in NC-based fibers (sample 1) decreased by 14.2 oC compared to pure RDX, which is totally differently from the result that a little Tp increase of RDX in NC-based fibers reported by Yang (2020). This large Tp decrease of RDX in sample 1 can be ascribed to the following two aspects. The first one is that RDX was prone to decompose when the particle size was reduced from micrometer to nanometer scale (Liu et al. 2018). The second one is the acceleration influence of ADN on the thermal decomposition of RDX. Similarly, the Tp decrease of CL-20 in NC-based fibers containing CL-20 (sample 2) from 251.3 oC to 235.4 oC which is about 4.2 oC lower than that reported by Guo et al. (2015) can be explained. Taking the Tp of NC as an indicator, the thermal stability order was [sample1] < [sample 3] < [sample 2] < [sample4].
Thermal behaviors under thermostatic conditions
The thermal behaviors of samples 1–4 at 100 oC were tested by the gas pressure measurement in the process of thermal decomposition, and the pressure curves were shown in Fig. 6.
It can be seen from Fig. 6 that the pressure of sample 4 contained only NC did not change much in the whole heating process, which was much lower than that of sample 1, 2 and 3. Furthermore, the thermal decomposition can be accelerated after being heated 1.5 h, 2.0 h and 1.1 h for sample 1, 2 and 3, respectively, which were much shorter than the initial pressure rise time of sample 4 containing NC alone. The first pressure rise process for sample 1, 2 and 3 can be ascribed to the thermal decomposition of ADN, because ADN decomposed ahead of NC as shown in DSC curves in Fig. 5. Obviously, as ADN was introduced, the thermal decomposition of fibers was accelerated. This was due to the intense interactions between ADN and NC, as analyzed in the previous section. Compared the pressure curve of sample 3 with sample 4 shown in Fig. 6, the intensive interactions between ADN and NC also can be ascertained. As high-energy compound, CL-20 or RDX, was extra added, the pressure rise time delayed a little. Except that, a comparative study on the decomposition behavior of NC + ADN mixture with that of sample 3 was conducted. From the Fig. 6, it can be seen that the pressure of NC + ADN mixture began to rise after heating for 30 h, about 28.9 h later than that of sample 3, which indicated that the more intensive interactions between ADN and NC can be prompted by electrospinning. This acceleration effect brought by electrospinning can be ascribed to better dispersion uniformity than simple mixing, and resulting large contact area between ADN and NC.
Combustion performance
The ignition delay time of sample 1, 2, 3, and 4 were measured with the laser power 40 W and 67 W, respectively, and the results were shown in Fig. 7.
It can be seen from Fig. 7 that as the laser power increased, the ignition delay time of all samples decreased, and the difference among those four samples decreased. Under laser irradiation of 40 W, the order of the ignition delay time was [sample 8 (33 ms)]\(\gg\) [sample 1 (14.5 ms)] > [sample 2 (9 ms)] = [sample7 (9 ms)]. However, as the power increased to 67 W, the order of the ignition delay time was [sample 8 (14.5 ms)]\(\gg\) [sample 1 (7.5 ms)] ≈ [sample 2 (7 ms)] ≈[sample7 (6 ms)]. The pure NC electrospun fibers had the longest ignition delay time under these two power laser irradiations. As ADN were added separately, the ignition delay time decreased the most. When CL-20 and ADN were added together to NC-based matrix, the ignition delay time changed a little compared to that of NC-based fibers containing ADN-added alone, but decreased a lot compared to that of pure NC electrospun fibers. The phenomenon was a little different when RDX and ADN were added together to NC-based matrix. The ignition delay time changed a little under laser power 67 W and increased a lot under laser power 40 W compared to that of NC-based fibers with ADN alone. Compared to the results reported by Wang et al. (2021) that the ignition delay time of the electrospun NC fibers containing RDX was higher than that of NC fibers, it’s easy to conclude that the addition of ADN can substantially reduce the ignition delay time of NC fibers containing RDX. This can be explained from the following two aspects. Firstly, due to the laser ignition started with the thermal decomposition of material, the one with lower thermal decomposition temperature more inclined to ignite (Lee et al. 2008). As shown in Fig. 5, the first decomposition peak temperature of samples containing ADN (178.9 oC, 184.5 oC and 185.7 oC for sample 1, 2 and 3, respectively) were much lower than that of sample 4 (209.0 oC), hence the ignition delay time of sample 1–3 was shorter than that of sample 4. However, this is not true for the three samples 1–3 containing ADN, namely, the sample 1 with the lowest first decomposition temperature (178.9 oC) has the longest ignition delay time. The reason was that RDX has a retarding effect on the laser ignition process of the NC composite fibers (Wang et al. 2021), which was consistent with the reported results (Hao et al. 2011). Secondly, the intensive interactions between ADN and NC made ADN addition played the critical role in igniting tests.
The combustion processes were captured with a high-speed camera during the laser ignition tests, and some corresponding snapshots were shown in Fig. 8.
The combustion flames were weak in whole process for sample 4 composed of pure NC, and the combustion flame became brighter as ADN, RDX or CL-20 was added, as shown in Fig. 8. It indicated that the burning became more violently as the composition became more energetic when high explosives were added into NC matrix. This phenomenon was consistent with the ignition delay time results. The reason for improvement in burning intensity by adding ADN is that the energetic salt possesses positive oxygen balance (Emeline et al. 2021). From the ignition delay time and combustion flame in the burning process, it can be seen that the combustion performance of NC-based composite fibers can be improved significantly by addition of ADN.
Mechanical sensitivity
The impact sensitivity and friction sensitivity of samples 1, 2, 3 and 4 were tested, and compared with that of pure ADN, RDX and CL-20. The results were listed in Table 3.
Table 3
The test results of mechanical sensitivity
Sample
|
Impact sensitivity (%)
|
Friction sensitivity (%)
|
1
|
56
|
60
|
2
|
56
|
64
|
3
|
52
|
60
|
4
|
64
|
72
|
ADN
|
48
|
40
|
RDX
|
88
|
84
|
CL-20
|
100
|
100
|
It can be seen that the impact sensitivity and friction sensitivity for sample 1 and 2 were reduced much compared to those of pure RDX and CL-20, which may be due to the synergistic effects of decreasing particle size from micrometer to nanometer (Wang et al. 2016) and NC coating over the sensitive particle (Chen et al. 2022; Zhang et al. 2019). Compared to sample 3 and 4, the addition of ADN can reduce the mechanical sensitivity, apart from the reasons mentioned above, another probable reason is that ADN can lubricate the NC matrix and adsorb heat in melting process under impact or friction.