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Membrane and Desalination Technologies - TCE Moodle Website

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Preparation of Polymeric <strong>Membrane</strong>s 73<br />

polymer properties for gas separation, pervaporation, reverse osmosis, et al. For the second<br />

path (path 2), the decomposition path of the membrane surface will go to the binodal curve.<br />

And the polymer concentration at the membrane surface will be always on the binodal<br />

position, which is in equilibrium with solvent concentration of the coagulant bath at the<br />

interface between the membrane <strong>and</strong> coagulant bath (38, 65, 67). With the time going on, the<br />

polymer concentration will change along the binodal curve, but no liquid–liquid demixing<br />

occurs on the surface layer because no polymer-poor phase is formed. At this period the skin<br />

layer cannot be solidified. The liquid–liquid demixing occurring at the sublayer underneath<br />

the membrane surface will influence the skin layer, <strong>and</strong> cause different pore size distributions<br />

<strong>and</strong> different skin thicknesses. The surface structure with different pore size distributions will<br />

be solidified until it reaches point B. The resulting membranes may be ultrafiltration,<br />

microfiltration <strong>and</strong> some gas separation membranes et al. Actually, for a dry-phase inversion<br />

process induced by forced-convective evaporation, the polymer concentration on the membrane<br />

surface sometimes crosses the binodal curve <strong>and</strong> goes into the spinodal decomposition<br />

(path 3) (68). Because of relative long gelation time, the coarsening of the bicontinuous<br />

structure occurs at a later stage of the phase separation process (before solidification) to form<br />

spherical nodules. Because of an additional physical process such as capillary pressure arising<br />

from the curvature of the interface of polymer-poor phase contacting with an external gas<br />

phase, an essentially homogeneous nascent skin layer will be formed by the coalescence of<br />

highly plasticized nodule network (43, 68, 69), shown in Fig. 2.21.<br />

4.2.6. Macrovoid Formation<br />

Macrovoids are very large elongated pores which can extend over the membrane thickness.<br />

It may have different shapes such as tear-like, pin-like, finger-like <strong>and</strong> so on. Macrovoids are<br />

undesirable because they cause poor mechanical strength in the membrane. The formation of<br />

macrovoids in the phase inversion process has been studied extensively in the literature (1, 4,<br />

70–77). And a variety of mechanisms have been proposed <strong>and</strong> used to describe the formation<br />

of macrovoids such as the shrinkage of polymer matrix (71, 72), surface tension gradientinduced<br />

convective flow (75), osmotic pressure (73), instantaneous phase demixing (70), <strong>and</strong><br />

concentration gradient-induced instability (76). However, a lot of controversy exists<br />

concerning the original of the macrovoids.<br />

Fig. 2.21 Contracting<br />

forces of polymer<br />

particles resulting from<br />

capillary pressure in<br />

interstitial spaces of film<br />

[adapted from ref. (68)].

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