控制电位条件下的胶体沉积

W. Albery, R. A. Fredlein, G. O'Shea, A. L. Smith
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引用次数: 8

摘要

利用通过载玻片的光束的倏逝波散射光,测量了涂有锡掺杂氧化铟的载玻片上炭黑胶体沉积的速率。速率可以实时测量,ITO涂层允许改变表面的电极电位。利用撞击射流的流体力学控制粒子的质量输运;根据射流的大小,流体动力学可以是壁管式的,也可以是壁射流式的。当表面电位为正时,没有阻挡带负电粒子沉积的屏障;在壁管和壁喷两种情况下,颗粒均以质量输运控制速率沉积。在两种状态下所测得的粒子扩散系数值吻合较好。根据滑块的年龄,当电位为负时,颗粒要么不沉积,要么沉积到次级最小值。壁面喷射状态下的径向变化表明,如果它们确实沉积,它们会以质量输运控制的速率再次沉积。可以计算出二次极小值的位置,结果表明,计算出的位置与倏逝波的侵彻有很好的一致性。当离子强度> 10 mmol dm-3时,没有屏障,颗粒在所有电位下都沉积。根据这一结果,我们估计Hamaker常数为23.8 kBT。利用这个值,我们就可以计算出较低离子强度的势垒坍塌和粒子从次级最小值转移到初级最小值的势垒。理论与实验结果吻合较好。
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Colloidal deposition under conditions of controlled potential
The rate of colloidal deposition of carbon black onto a microscope slide coated with tin-doped indium oxide has been measured using light scattered from the evanescent wave of a light beam passing through the slide. The rate can be measured in real time and the ITO coat allows the electrode potential of the surface to be changed. The mass transport of the particles is controlled by using the hydrodynamics of the impinging jet; depending on the size of the jet the hydrodynamics can either be wall-pipe or wall-jet. When the potential of the surface is positive there is no barrier to the deposition of the negatively charged particles; under both the wall-pipe and wall-jet regimes the particles deposit as the mass transport-controlled rate. Good agreement is found between the values of the diffusion coefficient of the particles measured in the two regimes. Depending on the age of the slide, when the potential is negative the particles either do not deposit or they deposit into the secondary minimum. The radial variation under the wall-jet regime shows that if they do deposit they do so again at the mass transport-controlled rate. The position of the secondary minimum can be calculated and it is shown that there is good agreement between the calculated position and the penetration of the evanescent wave. For ionic strengths > 10 mmol dm–3 there is no barrier and the particles deposit at all potentials. From this result we estimate a value of the Hamaker constant of 23.8 kBT. Using this value one can then calculate for lower ionic strengths the potential at which the barrier collapses and the particles transfer from the secondary into the primary minimum. Reasonable agreement is found between the theoretical and experimental results.
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