What is Dynamic Contact Angle?
A contact angle is defined by intersect of the three phase boundary between liquid, solid and vapor, and it is often described by Young’s equation,
γsv = γsl + γlv cos θ
Young’s equation only applies to ideal solids with smooth, inert, homogeneous and nonporous surfaces. However, surface roughness and chemical heterogeneity is often present on real surfaces, and as a result the accurate determination of contact angles is challenging as surface irregularities can cause contact angle hysteresis. The static contact angle is normally defined as the average value of various contact angle measurements. However, this can lead to great errors due to the irregularity of the real surface. The dynamic contact angles are the extremes of a possible contact angle range and they occur when the three-phase boundary is in motion. Dynamic contact angles provide information on the topography and homogeneity of the surface.
Dynamic contact angles can be measured with several Attension tensiometers.
With the Attension Sigma force tensiometer, the Wilhelmy method can be used to define dynamic contact angles. The solid surface is attached to a balance hook and is immersed in a test liquid to calculate the advancing contact angle. The solid is then lifted from the test liquid and the receding angle can be calculated.
There are two methods for measuring dynamic contact angles with the Attension Theta optical tensiometer. The dynamic contact angles can either be measured by expanding (advancing contact angle) and decreasing (receding contact angle) the drop size with the dispenser or by tilting the sample stage so that the sample and the drop lying on top of it are tilted. This requires a special Theta tilting cradle.
The tilting cradle can be also used for measuring the roll off angle of a surface. The roll off angle refers to the inclination angle of a solid surface in which a droplet rolls off the surface. The roll off angle is mostly used for characterizing superhydrophobic surfaces.