Electrospinning techniques can create a variety of nanofibrous scaffolds for tissue engineering or other applications. We describe here a procedure to optimize the parameters of the electrospinning solution and apparatus to obtain fibers with the desired morphology and alignment. Common problems and troubleshooting techniques are also presented.
Electrospun nanofiber scaffolds have been shown to accelerate the maturation, improve the growth, and direct the migration of cells in vitro. Electrospinning is a process in which a charged polymer jet is collected on a grounded collector; a rapidly rotating collector results in aligned nanofibers while stationary collectors result in randomly oriented fiber mats. The polymer jet is formed when an applied electrostatic charge overcomes the surface tension of the solution. There is a minimum concentration for a given polymer, termed the critical entanglement concentration, below which a stable jet cannot be achieved and no nanofibers will form – although nanoparticles may be achieved (electrospray). A stable jet has two domains, a streaming segment and a whipping segment. While the whipping jet is usually invisible to the naked eye, the streaming segment is often visible under appropriate lighting conditions. Observing the length, thickness, consistency and movement of the stream is useful to predict the alignment and morphology of the nanofibers being formed. A short, non-uniform, inconsistent, and/or oscillating stream is indicative of a variety of problems, including poor fiber alignment, beading, splattering, and curlicue or wavy patterns. The stream can be optimized by adjusting the composition of the solution and the configuration of the electrospinning apparatus, thus optimizing the alignment and morphology of the fibers being produced. In this protocol, we present a procedure for setting up a basic electrospinning apparatus, empirically approximating the critical entanglement concentration of a polymer solution and optimizing the electrospinning process. In addition, we discuss some common problems and troubleshooting techniques.
1. Choose a Polymer
2. Choose a Collector
3. Approximate the Critical Entanglement Concentration Empirically1
4. Troubleshooting – the Stream:
5. Troubleshooting – Fiber Morphology6,7,8 (refer to Figure 4)
6. Representative Results:
Please refer to Figure 4 for depictions of typical fiber results.
Figure 1. A typical electrospinning setup. A polymer solution (blue) is dispensed from a syringe pump (orange). A high voltage DC power supply (green) grounds a rapidly rotating wheel collector (grey) onto which aligned nanofibers are collected. The polymer jet between the syringe and collector consists of a steady streaming segment and a rapidly oscillating whipping segment.
Figure 2. The streaming jet is visible exiting the syringe tip; the whipping jet is too small to be seen.
Approximating the critical entanglement concentration of PLLA
PLLA (% wt/v) | Observation | Concentration Adjustment |
0.5 | Dripping; no stream | Increase |
2.0 | Spitting small globs; no stream | Increse slightly |
4.0 | Steady stream | Good |
6.0 | Spitting large globs or beads | Decrease slightly |
12.0 | Clumping at the tip; no stream | Decrease |
Table 1. An example depicting the approximation of the critical entanglement concentration of PLLA. Various polymer concentrations are tried and the resulting streaming jets observed until a steady stream is obtained.
Figure 3. The distance between the syringe tip and the collector must be balanced with the applied voltage to obtain a steady streaming jet. Excess applied voltage causes an oscillating or ‘wagging’ jet to form that results in less well-aligned fibers. When the voltage is too low, no jet will form and the solution will only drip from the syringe tip. The purple shaded region above represents the voltage range over which a steady streaming jet can be obtained for PLLA as a function of syringe-to-collector distance.
Figure 4. Electrospun fibers can exhibit a variety of morphologies, including beading (A), ribbons (B), curlicues (C), porous globs (D), good alignment (E) and poor alignment (F).
Note: The majority of the examples presented here deal with electrospinning poly-L-lactic acid (PLLA) nanofibers. This is simply because PLLA is the most commonly spun polymer in our laboratory. However, we have also successfully used these methods to electrospin other polymers (e.g., PLGA, PCL, PS) and believe that the techniques presented here are easily applicable to the majority of mid- to high-molecular weight polymer solutions.
The authors have nothing to disclose.
This work was supported by NIH K08 EB003996 and the Paralyzed Veterans of America Research Foundation Grant 2573.
Material Name | Type | Company | Catalogue Number | Comment |
---|---|---|---|---|
High voltage DC power supply | Gamma High Voltage | ES40P-5W | ||
Syringe pump | KD Scientific | KDS100 | ||
Aluminum foil | Reynolds | |||
Blunt metal tips, 23ga | Fisher | 13-850-102 | ||
Polypropylene syringe | BD | 309585 | ||
Rotating or stationary collector | Custom built | |||
Various alligator clips and wires | ||||
Dimethylformamide | Fisher | AC11622-0010 | ||
Chloroform | Fisher | AC42355-0040 | ||
PLLA | Boehringer Ingelheim | Resomer L210 | ||
PLGA 85:15 | Sigma | 43471 | ||
Carbon tape | Ted Pella | 13073-1 |