Electrospinning of ABS
In previous reports, acetone and DMSO were used as solvents for electrospinning ABS [18, 19]. However, there are disadvantages using these two solvents. Acetone has a low boiling point of 56.5 °C and high vapor pressure of 24.6 kPa (20 °C) [21], which lead to a fast evaporation during electrospinning. Therefore, ABS precipitates easily at the electrospinning nozzle, disturbing the continuous jet formation. By comparison, DMSO has a very high boiling point of 189 °C and very low vapor pressure of 55 Pa (20 °C) [21], causing deposition of wet fibers gluing together and losing fiber morphology. Chloroform is another common solvent for electrospinning. It has a slightly higher boiling point of 61.2 °C and lesser vapor pressure of 21.1 kPa than acetone [21]. Similar to acetone, it is also a good solvent for ABS. Our initial studies on the electrospinning of ABS/CHCl3 solutions showed a blockage of the electrospinning nozzle due to the fast solidification of the solution at the nozzle tip. Therefore, in this work, a solvent mixture of DMSO and CHCl3 with equal weight ratio was used for the electrospinning.
The initial investigation was focused on the electrospinning of ABS solutions with high concentrations (S1: 25 wt%, S2: 20 wt% and S6: 15 wt%). These three solutions showed very good electrospinnability with the continuous electrospinning process. The increased concentration is beneficial to eliminate the beads on the fibers, but the fiber diameter also increases (Fig. 1). The electrospun fibers from 25 to 20 wt% ABS solution showed bead-free fibers and the average fiber diameters were 2800 ± 350 and 2180 ± 390 nm, respectively. The 15 wt% ABS solution led to a quite different fiber morphology. Many beads were observed on the fibers and the average fiber diameter was decreased greatly to 598 ± 254 nm. Higher magnification SEM images showed that the fiber surface was rough with particles embedded in the fibers. These particles could be from the PB dispersed in the styrene-acrylonitrile matrix in ABS, which is inherent during ABS synthesis.
Confocal two-dimensional (2D) Raman imaging was performed in order to probe the spatial distribution of SAN and PB in the fibers. It can be clearly deduced from the color-coded 2D Raman images shown in Fig. 2 that the supporting fiber consists of SAN and the embedded particles correspond to the PB particles in the ABS.
Conductivity plays an important role in the electrospinning process and the fiber morphology. The addition of salts in the electrospinning solutions could change the conductivity significantly. In this work, we first investigated the addition of a small amount of SDS and PF on the solution conductivity, the electrospinnability and the fiber morphology. Figure 3 presents the relationship between the conductivity of ABS solutions (20 wt%) and the added amount of SDS and PF salts. The addition of both SDS and PF into the ABS solutions could increase the conductivity, but SDS exhibits a much more obvious effect. With the addition of 1 wt%, SDS increased the conductivity up to 68.5 µs/cm, which was seven times more than that by adding PF (9.1 µs/cm). A further increase of the amount of SDS led to greatly increased conductivity but also introduced the problem for the electrospinnability that big droplets were formed during the electrospinning process.
The addition of salts (SDS and PF) also affected the fiber morphologies significantly. Figure 4 shows the fiber morphologies electrospun from ABS solutions (20 wt%) with different amounts of SDS from 0.1 to 8 wt% and PF from 0.1 to 1.0 wt%. Compared to the fibers from the ABS solution without salt additives, the addition of salt is useful to decrease the fiber diameters. A small amount of SDS (0.1, 0.2 and 0.5 wt%) led to a decrease of the fiber diameter to 1150 ± 346, 926 ± 151 and 908 ± 208 nm, respectively, which was half the diameter of the fibers from the solution without salts (2180 ± 390 nm). Interestingly, this relatively high salt amount led to the fact that the fiber was branched with very fine fibers, which could be attributed to the strong repelling effect from the high conductivity. In comparison to the fibers from solution without additives, the addition of PF could also decrease the fiber diameter but not much more than the addition of SDS, which could be due to the weak effect on conductivity from PF (Fig. 4).
More solutions with different ABS concentrations and different amounts of salt additives of SDS and PF were prepared according to the Table S1 (1–5) to optimize the electrospinning conditions to achieve a good electrospinning process and obtain fibers with small diameters. The cross effect of ABS concentration and additive amounts on the electrospinnability and fiber diameter is shown in Fig. 5. It is obvious that the fiber diameter decreases as the ABS concentration decreases (0 wt% SDS) and a small amount of SDS up to 0.2 wt% is useful to decrease the fiber diameter. Increasing the salt amount by more is not expected to further decrease the fiber diameter, but the fiber diameter is still much smaller than the fibers from a solution without salt. Fixing the ABS concentration to 10 wt% and changing the SDS amount (0.1, 0.2, 0.25, 0.3, 0.35 and 0.4 wt%) cannot change the fiber diameter much. However, by fixing the SDS amount to 0.2 wt% and changing the ABS concentration from 20 wt% to 10 wt%, it is easy to get tunable fiber diameters from 1 µm to 150 nm (Figure S1).
Due to the hydrophobicity of ABS, the self-standing porous electrospun membrane showed the efficient separation of oil and water. In this work, we also tried to find some applications for electrospun ABS fibers. The electrospun ABS fibrous membrane could be used for oil/water separation due to the hydrophobicity with a water contact angle of 130° (Fig. 6, SI Video). The mixture with oil (perfluorodecalin, 3 mL) and water (dyed with Rhodamine B, 9 mL) was filled into the container equipped with ABS fibrous separator (thickness: 0.1 mm; diameter: 15 mm). After about 6 min, the oil/water mixture separated. The clear oil dripped into the collector and the red water was kept on the top of the ABS filter. These findings made electrospun ABS fibrous membranes possible for oil/water separation.
Pore size and coating density
Pore size and coating density are very important parameters for achieving the high filtration efficiency when randomly oriented fibers are coated on a filter substrate. In this work, we first prepared electrospun ABS nonwoven fibers with different fiber diameters and then measured the pore size of these nonwoven fibers. Figure 7a plots the relationship between the fiber diameter and the pore size. Interestingly, the fiber diameter showed a linear relationship with the average pore size. When the fiber diameter came down to 300 nm from 2800 nm, the average pore size dropped dramatically to 2 µm from 13.5 µm. If the fiber diameter decreases to 100 nm, then the average pore size could drop to even about 1 µm. These fine fibers and small pore size would greatly improve the filtration efficiency.
Commercial filters usually have a coating of electrospun fibers with a weight per area in the range of 0.3–0.8 g/m2. We established a simple method to measure the coating density (weight per area, g/m2) of electrospun ABS fibers on MFPP (9 × 9 cm2): (1) Electrospinning ABS fibers on the substrates for different time (0.5, 1, 2, 4, 6 and 8 min); (2) Drying the samples in a vacuum oven at 55 °C for 18 h to remove residual solvents; (3) Put the substrate with coating fibers on balance (0.01 mg deviation) and set weight to 0.00 mg; (4) Remove the coating fibers from the substrate; (5) Put the substrate on balance again and a minus value was obtained. The absolute value is the weight of the coating fibers on the substrate; (6) Repeat 4 times for each sample. Figure 7b shows that the coating density was linearly increased with the coating time. When the coating time was 2, 4 and 6 min, the coating weight per area was in the commercial range, which implied the commercial application of this coating filters.
Heat resistance
Due to the heat pressing process during the fabrication of filters, it is necessary to evaluate the heat resistance of electrospun ABS nonwovens. As shown in Fig. 8, the ABS nonwovens could stand the same shape under 110 °C for 2 min. Higher temperatures led to the shrinkage of the nonwovens. The SEM images showed that no changes were found in the fiber morphology when the heating temperature reached around 110 °C. When the samples were heated between 120 and 130 °C, the fibers became smoother due to the melting of the dispersed polybutadiene particles. In addition, junctions between the fibers were also observed due to the partial melting of ABS fibers.
Filtration efficiency
The filtration measurement was performed to evaluate the effect of the electrospun fiber diameter and the coating time (coating density) on the filtration efficiency in comparison to the blank MFPP samples (MFPP-01 and MFPP-02) and the commercial filter (C-Filter). Before we measured the filtration efficiency, we first checked the fiber morphology of MFPP and C-Filter. As shown in Figure S2, the MFPP was composed of smooth fibers. The average fiber diameters are 23 ± 4 µm and junctions between the fibers were observed. A commercial filter contains two layers. One layer is a substrate layer with a homogeneous fiber diameter of 16.5 ± 1.1 µm and the other layer is composed of much thinner fibers with ununiformed fiber diameters of 1.3 ± 1.2 µm. The two layers were glued together to improve the adhesion.
The electrospun fiber diameter and the coating density play a crucial role in the filtration efficiency of salt particles (0.2–10 μm) (Fig. 9). As expected, the microfiber fibrous MFPP (MFPP-01 and MFPP-02) showed the worst filtration efficiency due to their large pore size. A coating of electrospun ABS fibers on the substrate improved the filtration efficiency. When fixing the coating time to 2 min, the coating layer with a fiber diameter of 428 nm showed much better filtration efficiency than that with 2800 nm fiber diameter. The same results were also found when the coating time was fixed to 4 and 6 min. Two exceptional samples were outside the rule of fiber diameter-related filtration efficiency. The first one is the sample coated with electrospun fibers of 598 nm. This sample showed worse filtration efficiency than the sample coated with electrospun fibers of 2800 nm, which could be due to the large beads on the fibers. Another exceptional sample was the filter coating with 149 nm ABS fibers, which showed very bad filtration efficiency among all coating samples. This could be due to the quite inhomogeneous coating on the MFPP (Fig. 9d). As the coating time (coating density) increased, the filtration efficiency also improved. When the fiber diameter was 428 nm and the coating time was 2 min, the filtration efficiency was as good as the commercial filter (C-filter) with the particle size larger than 2.5 μm. When the coating time was 4 min, the coated filter showed comparable filtration efficiency to the commercial filter and when the coating time was increased to 6 min, the coating filter showed even better filtration efficiency than the commercial filter (Fig. 9).
Differential pressure (pressure drop) is an important parameter to evaluate the efficiency of filters. It is defined as the pressure difference between the two sides of the filter during the filtration test. Electrospun ABS fibers on MFPP, smaller fiber diameter and increasing the coating time generally lead to the increase of differential pressure (Fig. 10). Due to the large pore size, the MFPP showed the smallest differential pressure of 1.98 Pa, while the commercial filter showed a differential pressure of 13.5 Pa. By comparison, the samples coated with 457 and 428 nm for 2 and 4 min, respectively, which showed comparable filtration efficiency, presented similar or a little higher differential pressure.
Ashby figures of coating density-dependent pressure drop and the quality factor (QF) from different filter mediums were plotted to compare the quality of the filter prepared in this work to other filter mediums. As illustrated in Fig. 11, the filters in this work showed a much better filtration performance in terms of the pressure drop and QF. When comparing the pressure drop of different filter mediums (pressure drop > 30 Pa), the ABS filters occupied a very important area where the small pressure drop < 30 Pa could be achieved with a sample coating density smaller than 0.8 g/m2 (Fig. 11a). The quality of the filters could be evaluated by QF based on the comprehensive evaluation on the pressure drop and filtration drop. It can be calculated by the following equation:
$${\text{QF}} = \frac{{ - \ln \left( {1 - \eta } \right)}}{\Delta P}$$
where η and ΔP are the filtration efficiency and the pressure drop between the upstream and downstream pressure, respectively. The higher the QF is, the more efficient the filters are [22]. Figure 11b plotted the Ashby figure of QF for the 300 nm particle size in this work in comparison to other filter mediums. The ABS fibrous filters showed a tunable QF from 0.055 to 0.477 with a coating density < 0.8 g/m2. This QF is larger than most other filter mediums in previous work. In addition, the pressure drop and QF of ABS fibrous filters are comparable to or even better than those of other filter mediums, suggesting these are ideal candidates as filter mediums for filtration applications.