Particulate Fluids Processing Centre, The University of Melbourne, Parkville, Victoria 3010 Australia.
Langmuir. 2011 Oct 4;27(19):12025-32. doi: 10.1021/la202804c. Epub 2011 Sep 7.
Bubble coalescence behavior in aqueous electrolyte (MgSO(4), NaCl, KCl, HCl, H(2)SO(4)) solutions exposed to an ultrasound field (213 kHz) has been examined. The extent of coalescence was found to be dependent on electrolyte type and concentration, and could be directly linked to the amount of solubilized gas (He, Ar, air) in solution for the conditions used. No evidence of specific ion effects in acoustic bubble coalescence was found. The results have been compared with several previous coalescence studies on bubbles in aqueous electrolyte and aliphatic alcohol solutions in the absence of an ultrasound field. It is concluded that the impedance of bubble coalescence by electrolytes observed in a number of studies is the result of dynamic processes involving several key steps. First, ions (or more likely, ion-pairs) are required to adsorb at the gas/solution interface, a process that takes longer than 0.5 ms and probably fractions of a second. At a sufficient interfacial loading (estimated to be less than 1-2% monolayer coverage) of the adsorbed species, the hydrodynamic boundary condition at the bubble/solution interface switches from tangentially mobile (with zero shear stress) to tangentially immobile, commensurate with that of a solid-liquid interface. This condition is the result of spatially nonuniform coverage of the surface by solute molecules and the ensuing generation of surface tension gradients. This change reduces the film drainage rate between interacting bubbles, thereby reducing the relative rate of bubble coalescence. We have identified this point of immobilization of tangential interfacial fluid flow with the "critical transition concentration" that has been widely observed for electrolytes and nonelectrolytes. We also present arguments to support the speculation that in aqueous electrolyte solutions the adsorbed surface species responsible for the immobilization of the interface is an ion-pair complex.
在超声场(213 kHz)作用下,研究了水基电解质(MgSO4、NaCl、KCl、HCl、H2SO4)溶液中气泡的聚并行为。发现聚并程度取决于电解质的类型和浓度,并与溶液中溶解气体(He、Ar、空气)的量直接相关,对于所采用的条件,没有发现声空化气泡聚并中存在特定离子效应的证据。将结果与以前在没有超声场的情况下,对水基电解质和脂肪醇溶液中气泡的几次聚并研究进行了比较。结论是,在许多研究中观察到的电解质对气泡聚并的阻抗是涉及几个关键步骤的动态过程的结果。首先,需要离子(或更可能是离子对)在气/溶液界面上吸附,这个过程需要超过 0.5 ms 的时间,并且可能需要几分之一秒的时间。在吸附物种的界面负载足够高(估计小于 1-2%单层覆盖率)的情况下,气泡/溶液界面的流体动力边界条件从切向可动(零剪切应力)切换为切向不可动,与固液界面的情况一致。这种情况是由于溶质分子在表面上的空间非均匀覆盖以及随之产生的表面张力梯度的结果。这种变化降低了相互作用气泡之间的薄膜排水速率,从而降低了气泡聚并的相对速率。我们已经将这种切向界面流体流动的固定点与广泛观察到的电解质和非电解质的“临界转变浓度”联系起来。我们还提出了一些论据,支持这样的推测,即在水基电解质溶液中,负责界面固定的吸附表面物种是离子对复合物。