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However, the high surface tension and low conductivity make a powerful barrier against fiber jet formation.
Upon exposure to an electric field, the charged polymer solution is drawn towards the grounded collector forming a thin continuously elongating fiber jet.
The resulting fiber jet was collected onto a grounded rotating and translating aluminum drum to collect a large mesh of uniform thickness (300 μm).
In electrospinning, a continuous fiber jet is ejected from the needle tip of a syringe containing a polymer solution, which is driven by the balancing of surface tension and electrostatic (repulsive) forces under an applied high voltage.
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The fiber jets can be considered as dynamic slender bodies.
These fiber jets also imply a heat source q jets in the energy equation.
Their computation requires in principle a coupling of fiber jets and flow with appropriate interface conditions.
External loads rise from gravity ρ ⋆ g e g and forces due to the immersed fiber jets f jets.
Then, glass jets and air flow become stationary, presupposing that we consider spun fiber jets of certain length.
However, in view of quality assessment, slenderness and homogeneity of the spun fiber jets play an important role.
In case of k slender bodies in the air flow, we have Ψ i, i = 1, …, k, representing the quantities of each Cosserat rod, here k = M N. Assuming no contact between neighboring fiber jets, every single jet can be described by the stated rod system (1).
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