Soft Materials Laboratory, Department of Physics, IIT Madras, Chennai-600036, India.
Soft Matter. 2017 Aug 16;13(32):5445-5452. doi: 10.1039/c7sm00567a.
The drying of a sessile drop consisting of colloidal particles and the formation of particulate deposits with spatially periodic cracks were ubiquitous. The drying induced stress, which is generated during the evaporation of a colloidal drop, is released by the formation of cracks. We find that the morphology of cracks formed in particulate films dried at substrate temperature, T = 25 °C is markedly different from that of cracks formed at T > 45 °C. The cracks are disordered in the former case, but ordered and periodic in the latter. The disorderedness of cracks observed at T = 25 °C is mainly due to the formation of a coffee-ring like particle deposit that exhibits a larger height gradient. The ultimate deposit pattern after complete drying is observed to be different for colloidal dispersion drops evaporated at different substrate temperatures. This is attributed to temperature-dependent solvent flow mechanisms and capillary-driven flow, which occur inside the colloidal drop during the course of drying. In addition, for the coffee-ring-like particulate deposit obtained at T ≤ 45 °C, the ratio between the width of the deposit w and the radius of the ring R scales with the volume fraction of the colloids φ, w/R ∼ φ, in the range of volume fractions studied in this work. The deposited patterns obtained at temperature T > 45 °C are largely dominated by the capture of particles by the receding liquid-vapor interface. This is due to the faster rate of decrease of the liquid-vapor interface position with an increase in substrate temperature.
液滴中胶体颗粒的干燥和具有空间周期性裂缝的颗粒沉积物的形成无处不在。在胶体液滴蒸发过程中产生的干燥诱导应力通过裂缝的形成而释放。我们发现,在基底温度为 T=25°C 下干燥的颗粒膜中形成的裂缝的形态与在 T>45°C 下形成的裂缝明显不同。在前一种情况下,裂缝是无序的,但在后一种情况下则是有序且周期性的。在 T=25°C 下观察到的裂缝无序主要是由于形成了咖啡环状颗粒沉积物,其具有更大的高度梯度。在不同基底温度下蒸发的胶体分散液滴完全干燥后的最终沉积图案观察到不同。这归因于溶剂流动机制和毛细驱动流动的温度依赖性,这些机制在干燥过程中发生在胶体液滴内部。此外,对于在 T≤45°C 下获得的咖啡环状颗粒沉积物,沉积层的宽度 w 与环的半径 R 之间的比值与胶体的体积分数φ有关,在本工作研究的体积分数范围内,w/R∼φ。在温度 T>45°C 下获得的沉积图案主要由后退的液-气界面捕获颗粒主导。这是由于随着基底温度的升高,液-气界面位置的下降速度更快。