Accurate
jet diameters have been experimentally obtained during
electrospinning by the light-scattering technique together with the
Mie theory for cylinder scattering. Afterward, the fluid velocity
and extension rate in the jet from the apex of the flow-modified Taylor
cone to the straight jet end prior to the jet whipping are feasibly
derived. It is found that the extension rate ε̇ is position
(or time) dependent; its magnitude is the highest at the apex (region
I with ε̇I) and rapidly decreases to a relatively
constant value in the main jet (region II with ε̇II) before reaching the jet end (region III), where the extension
rate is zero. It is of importance to notice that ε̇I could be as high as 4000 s–1, which is
much higher than the chain retraction rate τe
–1 obtained from the rheological measurement. This experimentally
measured ε̇I is consistent with that derived
theoretically based on a simple energy conservation between the electric
work and the drag flow energy, i.e., ε̇I =
(κ/ηe)0.5Φ0.5
E
s, where κ is the solution conductivity,
ηe is the elongational viscosity, E
s is the electric field at the cone apex, and a parameter
Φ to characterize the viscoelasticity of the flowing jet. Our
analyses of the extension rate in the straight jet reveal the general
trend of ε̇I > ε̇II >
τe
–1 > τd
–1, suggesting likely a sequential structure evolution
leading eventually to the strings within the jet due to, first, the
flow-induced large concentration fluctuations in single phase solution
(at τd
–1 < ε̇ <
ε̇inst. < τe
–1) and, subsequently, phase separation (at ε̇inst. < ε̇ < τe
–1) eventually leading to evolution of the strings with increasing
ε̇ (at ε̇ > τe
–1), where τd
–1 is the chain disentanglement
rate, and ε̇inst. is the critical stretching
reate for onset of the flow-induced thermodynamically instability.
To validate this hypothesis, we have developed a simple collecting
method to receive the fast-flowing jet in a nonsolvent reservoir in
an attempt to quickly freeze its internal structures developed, if
any, for the off-line optical and electron microscopy observations.
Based on the results obtained from six polymer solutions studied,
the formation of dissipative structures of “strings”
with various widths due to growth or ordering of phase-separated structures
developed on a mesoscopic scale seems to be a general phenomenon.
In situ observation of the straight jet by a high-speed camera is
also performed to reveal the rapid flowing of dissipative structures
of “bulges” developed by macroscopic phase separation
in the jet. We conclude that the extremely high extension rate at
the cone apex plays a dominant role in the subsequent structure evolution,
generally producing the flow-induced phase-separated structures.