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Membrane and Desalination Technologies - TCE Moodle Website

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Preparation of Polymeric <strong>Membrane</strong>s 87<br />

Fig. 2.32 Velocity distribution of nascent hollow fiber membranes verse distance at the air gap.<br />

I. relative low extension viscosity<br />

II. relative high extension viscosity<br />

III. solidification (high extension viscosity)<br />

At region I, the nascent hollow fiber membranes are just spun from the exit of the<br />

spinneret, they have the same rheological characteristics as the dope solution inside the<br />

spinneret. When the nascent hollow fiber membranes goes into region II, the elongation<br />

viscosity increases greatly with the time because of the solvent exchange, temperature change<br />

<strong>and</strong> the phase inversion induced by the exchange of solvent <strong>and</strong> nonsolvent between the<br />

nascent membrane <strong>and</strong> the bore fluid. Due to the high elongation viscosity, the elongation rate<br />

will decrease, which causes a lower slope of spinline in region II. When the vitrifiction or<br />

solidification occurs in region III, the polymer structure is solidified <strong>and</strong> the velocity can be<br />

kept at the drawing rate.<br />

For different polymer solutions, bore fluids <strong>and</strong> spinning conditions, the different spinline<br />

velocities can be achieved at the same draw ratio. When the instantaneous demixing occurs<br />

inside the air gap, three distinct regions exist in the air gap <strong>and</strong> the drawing speed is mainly<br />

accelerated in the beginning part of the air gap. For the delay demixing in the air gap, the<br />

region I <strong>and</strong> II may describe its spinline velocity in the air gap, whereas the region II may be<br />

extended into the coagulation bath. When the nascent polymer cannot be solidified because of<br />

the poor coagulant or short air gap, the region III will not exist <strong>and</strong> the region II is extended<br />

into the coagulation below the water surface <strong>and</strong> the final velocity is attained under the water<br />

surface (96).

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