Postprocesses in tubular electrospun nanofibers
A. Arinstein
1,2
and E. Zussman
2
1
Department of Physics, Bar-Ilan University, Ramat-Gan 52900, Israel
2
Department of Mechanical Engineering, Technion–Israel Institute of Technology, Haifa 32000, Israel
Received 6 August 2007; published 9 November 2007
The postprocesses that occur in coelectrospun polymer nanofibers are investigated. The high rate of solvent
evaporation during the electrospinning of fibers results in such a rapid formation of the shell of the tubular
nanofibers, that the polymer molecules composing the fibers are in a nonequilibrium state. This stretched state
of macromolecules is assumed to be stabilized in a solid matrix, and can account for the anomalous properties
of the nanofibers. During this processing stage a considerable amount of solvent remains inside the tubular
nanofibers. The evaporation of the solvent continues for several minutes, and is accompanied by further
evolution of the nanofibers in both their microstates and macrostates. In this paper, we examine possible
macrostate modifications of the nanofibers, such as radial buckling. The theoretical model which describes the
kinetics of the solvent evaporation is found to be in good agreement with experimental observations. Thus, the
physical parameters of the system in question can be estimated, and the conditions of fiber shell instability that
produce buckling of the tubular nanofibers can also be predicted.
DOI: 10.1103/PhysRevE.76.056303 PACS numbers: 47.61.k, 81.05.Lg, 81.16.c
I. INTRODUCTION
Electrospinning is a commonly used process for fabricat-
ing polymer-based nanofibers 1–4. In this process, a poly-
mer solution is extruded from a spinneret, and in the pres-
ence of a sufficiently strong electric field, a jet is formed at
the tip. This jet then undergoes extreme elongation thereby
stretching the polymer molecules within it. As this is occur-
ring, the rapid solvent evaporation fixes the polymer matrix
in this stretched, yet nonequilibrium state. This process al-
lows for the fabrication in a single stage and in less than
10 ms, of nanofibers ranging from 100 to 1000 nm in diam-
eter. The morphology and mechanical properties of the col-
lected fibers are commonly studied by focusing on the pa-
rameters of the electrospinning process 5–9. Many studies
have examined polymer rheology 10, while others have
focused on controlling the electrostatic field, or determining
the effect of various setup configurations 11. However, the
effect of the evaporation rate on the physical features of the
electrospun fibers has not been studied in detail.
The very rapid evaporation process is a challenging prob-
lem for experimental investigation. However, theoretical
analysis and computer simulations can clarify some aspects
of the problem in question. For example, the role that the
high evaporation rate plays in the fabrication of polymeric
electrospun nanofibers has already been discussed by Koom-
bhongse et al. 12 and treated quantitatively by Guenthner
et al. 13. In particular, it was demonstrated that when the
evaporation is very fast, the polymer density at the fiber/
vapor interface increases sharply, thus creating a polymer
density gradient that acts as a barrier, or skin, that resists
further solvent evaporation.
These results are in good agreement with our presumption
that despite the rapid evaporation that has occurred, the
collected electrospun nanofibers still contain a significant
amount of solvent. The presence of the solvent, which now
evaporates even slower due to the barrier that has formed,
apparently results in “relaxation” of the fabricated nanofi-
bers. This relaxation causes certain postprocesses to take
place within the system. Therefore, the effect of this residual
solvent is crucial to understanding the mechanisms that af-
fect the nanofibers’ mechanical properties, and provides the
motivation for the presented work.
The structure of this paper is as follows: First, we de-
scribe the experimental system which was designed to allow
us to observe the evaporation kinetics within the tubular
electrospun nanofibers containing the solvent. Next, we pro-
pose a physical model of the processes observed in the ex-
periments. Based on this model and the experimental obser-
vations, we are able to elucidate the effect of some of the
system parameters. Finally, we discuss one of the possible
phenomena which occurs as a result of solvent evaporation,
i.e., the radial buckling of nanofibers, which is occasionally
observed in our experimental system.
II. EXPERIMENTAL SYSTEM
As mentioned above, the investigation of the very rapid
solvent evaporation occurring in the electrospinning process
is a complex experimental problem. Therefore, we focus on a
special case of the system discussed by Guenthner et al. 13.
Their theoretical analysis and simulation have shown that the
polymer molecules in the electrospun fibers are inhomoge-
neously distributed in the cross section of the nanofiber,
forming a compact surface or “shell.” Also, a spongy core is
formed as a result of the entrapped solvent which cannot
quickly escape, due to the low penetrability of the formed
shell. Clearly, a tubular nanofiber filled with solvent can be
considered as a special case of the Guenther et al. system. In
our experimental system, we used tubular nanofibers, thereby
enabling us to observe the decrease in the amount of solvent
inside the nanofibers due to evaporation. In this manner, we
are able to track the kinetics of solvent evaporation through
the shell.
The method of fabricating such tubular nanofibers is pre-
sented in detail in Ref. 14. Briefly, two polymer solutions
PHYSICAL REVIEW E 76, 056303 2007
1539-3755/2007/765/0563037 ©2007 The American Physical Society 056303-1