Applications of Polymer Nanofibers. Группа авторов
stretching and a stronger electric field. (Andrady 2008). For polyacrylonitrile in DMF, fiber diameter was reduced from ~95 to 50 nm by increasing the voltage from 5 to 25 kV. Conversely, fiber size has increased with increasing voltage. For example, the polystyrene (PS) fibers increased in diameter from 0.31 to 1.72 μm when the applied voltage increased from 5 to 25 kV. The discrepancy in experimental observations indicates that the effect of voltage on fiber size needs to be considered with other process parameters, especially the feed rate and tip‐to‐collector distance. Notably, at higher applied voltages, there is a greater tendency for bead formation. The bead density increased with increasing voltage and the shape of the beads transitioned from spindle‐like to spherical‐like indicating instability of the jet (Ramakrishna 2005).
Tip‐to‐collector distance influences the time of travel, amount of drying, and electric field strength (depending on the applied voltage) and thus the resulting fiber diameter and morphology. Practically, the distance must be large enough to prevent corona discharge. Generally, increasing the tip‐to‐collector distance with other parameters kept constant reduces fiber diameter. For example, electrospinning polystyrene in chloroform, the fiber diameter decreased from 1 to 0.66 μm by increasing the distance from 5 to 25 cm due to increased time of travel and stretching. Conversely, increasing the distance has also been observed to increase fiber diameter due to the reduced electric field strength. Decreasing the tip‐to‐collector distance and resulting time of travel and amount of drying can lead to deposition of “wet” fibers that fuse on the collector. While higher electric field strengths can be achieved at shorter distances, it can often result in the formation of beads or an unstable Taylor cone if the distance is not sufficient for development of the whipping instability (Andrady 2008; Ramakrishna 2005).
Continuous nanofibers of uniform diameter are achieved when the feed rate matches the rate of at which solution is removed from the tip. At lower feed rates, fibers may form intermittently. Higher feed rates increase the tendency to form beads. Given sufficient applied voltage, the average fiber diameter increases with feed rate. Increasing the feed rate can also result in fused fibers. With larger volume of solution drawn from the needle top, the solvent may not completely evaporate. The residual solvent may cause the fibers to fuse together when deposited (Andrady 2008; Ramakrishna 2005).
Overall, the experimental results generally agree with the scaling analysis, i.e. the final fiber diameter is directly proportional to volumetric flow rate as well as polymer concentration/viscosity. The electric field strength, dictated by the applied voltage and tip to collector distance, also affects fiber diameter. However, various effects have been observed (e.g. increasing the applied voltage may increase, decrease, or have no effect on the fiber diameter depending on the system) due to the complexity of the process. Some authors have performed systematic experiments varying process parameters and used regression analysis (Cui et al. 2007) or neural network models (Sarkar et al. 2009) to establish quantitative relationships. However, these analyses are system‐dependent. There are no methods to date to predict the fiber size based on solution properties and process parameters (Helgeson et al. 2008; Thompson et al. 2007).
1.3 Effect of Setup Parameters
The effect of process parameters (e.g. flow rate, tip‐to‐collector distance, applied voltage) has been widely studied with conflicting experimental results. An alternative approach to tuning nanofiber and membrane properties has been adjusting parameters of the electrospinning setup.
Ambient conditions (temperature and humidity) affect the electrospinning process and fiber characteristics. The temperature of the spinning solution affects the evaporation rate and the viscosity. At higher temperatures, lower viscosities lead to increased stretching force and result in smaller fibers. Humidity affects solvent evaporation which can affect the resulting fiber characteristics. Using PEO in water as a model system, a twofold monotonic decrease in fiber size was observed with increasing relative humidity. At low humidity, solvent evaporation may be faster than removal of the solution away from the tip of the needle and can lead to needle clogging, especially with volatile solvents. Leveraging humidity to create porous fibers is further discussed in Section 1.6.2. Although, the relative humidity cannot always be readily controlled (Cai and Gevelber 2013), monitoring the ambient temperature and humidity during electrospinning is of practical importance.
Generally, electrospinning is performed in air. Controlling the gaseous environment can be advantageous for affecting fiber diameter. To slow the rate of drying, a gas‐jacketed capillary tip can be used to surround the jet with nitrogen saturated with spinning solvent. With slower solvent evaporation, stable Taylor cones could be achieved by electrospinning poly‐L‐lactic acid in dichloromethane (high volatility). Notably, the flow rate of gas affected the rate of electrospinning. Accelerating the rate of evaporation using an external heat source has also been reported to improve the mat quality of hyaluronic acid fibers spun from water. The improved fiber quality was attributed to increased stretching, enhanced solvent evaporation, and a threefold reduction in viscosity due to the flow of hot air (~60 °C). The composition of the gaseous environment is also an important consideration; it affects leakage of the surface charge on the jet to the surrounding environment and ultimately the fiber size. For example, when using Freon‐12 as the electrospinning environment, the fiber diameter was twofold larger than air at the same conditions. This result was attributed to the higher breakdown voltage of Freon‐12 compared to air. With a higher breakdown voltage, the fiber retained its electric charge for a longer period of time which would increase the jet velocity and ultimately result in a larger fibers (Ramakrishna 2005; Baumgarten 1971).
Polarity of the applied electric field also affects fiber quality and size. For nylon‐6 in formic acid, the average fiber diameter was approximately twofold smaller when the capillary was charged with a negative polarity compared to when a positive polarity at the same conditions. Further, the area over which the fibers deposited was smaller in the case of a positive polarity. The difference in fiber quality and size was attributed to increased charge density in the case of negative polarity (Andrady 2008).
Generally, DC voltage is used in electrospinning. The use of alternating current (AC) potential has also been reported. Since the charging of the solution is very rapid, jet initiation occurs before the voltage alternates. The jet contains positive and negative charged which reduces the repulsive forces and bending instability in the jet. Therefore, using AC the fibers are larger when compared to DC at the same voltage. In AC, there is reduced accumulation of like charges on the deposited fiber. Therefore, thicker layers of electrospun fibers can be achieved, especially when using an insulating collector (Ramakrishna 2005).
Notably, using sharp, pointed needles, i.e. capillary tips results in more efficient charging of the solution. The tip diameter is also an important consideration. Practically, the tip diameter selection is important in avoiding needle clogging due to solvent evaporation. Smaller internal diameters have been observed to reduce beading and reduce the diameter of the fibers (in some cases). As the internal diameter decreases, the surface tension increases and a greater electrostatic force is required for jet initiation leading to smaller fibers. Therefore, the smallest tip that facilitates extrusion of the solution is generally selected. Generally, electrospinning is performed with 16G–27G needles (Andrady 2008; Ramakrishna 2005).
In more complex setups, additional electrodes can be added to tune fiber deposition (Teo and Ramakrishna 2006; Teo et al. 2011). These auxiliary electrodes can be base electrodes, steering electrodes, focusing electrodes, and guiding electrodes (Figure 1.2). The base electrode is usually a conductive plate placed parallel to the collector at the needle tip to improve the uniformity of the electric field and minimize the effect of surrounding objects on the electric field. Since the base electrode increases the stability of the jet, fibers with smaller diameters have been observed. The base electrode should be level with the needle top. Notably, using a base electrode, a higher applied voltage is required to initiate spinning (Teo and Ramakrishna 2006; Teo et al. 2011). Focusing electrodes are used to damp the whipping of the electrostatic jet to achieve more localized deposition. The electrodes are ring‐shaped, cylinder,