Szilagyi Istvan, Trefalt Gregor, Tiraferri Alberto, Maroni Plinio, Borkovec Michal
Department of Inorganic and Analytical Chemistry, University of Geneva, Sciences II, Quai Ernest-Ansermet 30, 1205 Geneva, Switzerland.
Soft Matter. 2014 Apr 21;10(15):2479-502. doi: 10.1039/c3sm52132j.
This review summarizes the current understanding of adsorption of polyelectrolytes to oppositely charged solid substrates, the resulting interaction forces between such substrates, and consequences for colloidal particle aggregation. The following conclusions can be reached based on experimental findings. Polyelectrolytes adsorb to oppositely charged solid substrates irreversibly up to saturation, whereby loose and thin monolayers are formed. The adsorbed polyelectrolytes normally carry a substantial amount of charge, which leads to a charge reversal. Frequently, the adsorbed films are laterally heterogeneous. With increasing salt levels, the adsorbed mass increases leading to thicker and more homogeneous films. Interaction forces between surfaces coated with saturated polyelectrolyte layers are governed at low salt levels by repulsive electric double layer interactions, and particle suspensions are stable under these conditions. At appropriately high salt levels, the forces become attractive, principally due to van der Waals interactions, but eventually also through other forces, and suspensions become unstable. This situation can be rationalized with the classical theory of Derjaguin, Landau, Verwey, and Overbeek (DLVO). Due to the irreversible nature of the adsorption process, stable unsaturated layers form in colloidal particle suspensions at lower polyelectrolyte doses. An unsaturated polyelectrolyte layer can neutralize the overall particle surface charge. Away from the charge reversal point, electric double layer forces are dominant and particle suspensions are stable. As the charge reversal point is approached, attractive van der Waals forces become important, and particle suspensions become unstable. This behaviour is again in line with the DLVO theory, which may even apply quantitatively, provided the polyelectrolyte films are sufficiently laterally homogeneous. For heterogeneous films, additional attractive patch-charge interactions may become important. Depletion interactions may also lead to attractive forces and suspension destabilization, but such interactions become important only at high polyelectrolyte concentrations.
本综述总结了目前对聚电解质吸附到带相反电荷的固体基质上的理解、此类基质之间产生的相互作用力以及对胶体颗粒聚集的影响。基于实验结果可得出以下结论。聚电解质不可逆地吸附到带相反电荷的固体基质上直至饱和,从而形成松散且薄的单层。吸附的聚电解质通常带有大量电荷,这会导致电荷反转。通常,吸附膜在横向是不均匀的。随着盐浓度增加,吸附量增加,导致形成更厚且更均匀的膜。在低盐浓度下,覆盖有饱和聚电解质层的表面之间的相互作用力由排斥性的电双层相互作用控制,在这些条件下颗粒悬浮液是稳定的。在适当高的盐浓度下,这些力变为吸引力,主要是由于范德华相互作用,但最终也通过其他力,悬浮液变得不稳定。这种情况可以用经典的德亚金、朗道、韦弗伊和奥弗贝克(DLVO)理论来解释。由于吸附过程的不可逆性,在较低聚电解质剂量下,胶体颗粒悬浮液中会形成稳定的不饱和层。不饱和聚电解质层可以中和颗粒表面的总电荷。远离电荷反转点时,电双层力占主导,颗粒悬浮液是稳定的。随着接近电荷反转点,有吸引力的范德华力变得重要,颗粒悬浮液变得不稳定。这种行为再次符合DLVO理论,只要聚电解质膜在横向足够均匀,该理论甚至可能定量适用。对于不均匀的膜,额外的吸引性补丁电荷相互作用可能变得重要。耗尽相互作用也可能导致吸引力和悬浮液失稳,但这种相互作用仅在高聚电解质浓度下才变得重要。