Suppose a liquid droplet is deposited onto a solid surface. In that case, it will form a contact angle depending on its surface tension, the surface tension of the solid substrate, and the interfacial tension between solid and liquid.
This equation is referred to as the "Young equation", and the angle θ formed by the solid surface and the tangent of the droplet is called the "contact angle".
The "contact angle" is intuitive and easy to understand as an indicator of wettability and has been adopted widely in industrial fields as an evaluation method of surfaces.
The θ/2 or height-width method is generally used for the measurement of contact angle. The equation given below determines the contact angle. Where radius r and height h of the droplet.
In addition, the contact angle is obtained from the angle of straight lines connecting the left and right ends and the apex of the droplet against a solid surface.
In the θ/2 method, since the shape of the droplet is assumed to be part of the outline of an imaginary circle, measurement is done with a tiny droplet that can ignore the effect of gravitational force.
This can also be processed very quickly by computer analysis, as it is a simple calculation.
The droplet's shape is assumed to be part of the outline of an imaginary circle. This method obtains the center of the imaginary circle and determines the contact angle as the angle and straight lines tangent to the circle. For example, from the figure below, the three arc points L1, L2, and L3 form the imaginary circle. The angle between the tangent line m and the drop baseline l is the left contact angle. The right contact angle can be measured similarly using points R1, R2, and R3. The contact angle is determined as the average of the left and right endpoints. Conversely, with the Tangent method, it is possible to independently determine the contact angle by the left and right endpoints. Thus, it is an effective measurement method for uneven surfaces with different left and right contact angles.
Curve fitting method
Assuming that the contour shape of the droplet forms part of a true circle or ellipse, the Least square method is performed using the coordinates of all observations (fitting section) in a given interval. This calculation determines the perfect circle or ellipse parameters, and the contact angle differential coefficients of the endpoint are calculated. With the Tangent method, a perfect circle has been assumed as the contour shape. However, compared with the results of fitting the perfect circle, the second is the better fitting perfect circle as it uses more coordinates for a smaller variation.
Measurement of Dynamic Contact Angle
On the assumption that the droplet is at rest on a solid surface and reaches equilibrium quickly if compared to differences at a specific time after the droplet deposition, the contact angle data of the preceding paragraph is beneficial. However, this only applies if the data is not altered much. For example, assuming a case of various states, such as coating or cleaning, where the liquid and solid interface is dynamic, sufficient data is not obtained. This case simulates (with the advancing and receding contact angle) a dynamic situation where the interface of the liquid droplet moves and has been increasing. Conducting this analysis with a personal computer has become common practice, so you can easily capture dozens of frames per second to measure the time-dependent change of the droplet (contact angle).
The following describes methods for measuring the dynamic contact angle.
Sessile Drop method in time function
The measurement of the contact angle in the preceding paragraph is performed continuously to observe variations over time. Although there is no precise definition between dynamic and static, we are treating it as one type of dynamic contact angle, for time intervals of one second or less. This can also be used for the purpose of following the absorption and other volatile situations.
By inflating a droplet in contact with a solid surface and increasing and decreasing the size of the droplet, the contact angle is measured when advanced and receded (advancing contact angle and receding contact angle).
With the Expansion/Contraction Method, there is also a disadvantage where the non-uniformity of the solid surface is large, such as stick-slip behavior at the interface, which often causes data of a less smooth curve. Thus, it is important to perform repeated measurements to fully grasp these movements.
Sliding method – measurement on a slope
A solid surface is tilted in order to measure the droplets on the surface as they slide. Dedicated hardware is required; data can be obtained on "adhesion" and "slipperiness", etc. for solid-liquid (see below), which cannot be obtained by data-plane measurements.
When the measuring unit (Wilhelmy plate) makes contact with the surface of the liquid, the liquid will wet the Wilhelmy plate upwards. In this case, the surface tension acts along the perimeter of the plate and the liquid pulls in the plate. This method detects the pulling force is read and determines the surface tension. At this time, the surface tension can be determined by using a plate material that has a contact angle of 0º with the liquid to the measuring unit (plate). Platinum is commonly used as the plate material. Conversely, with the Wilhelmy method contact angle measurement, we measured the force of the solid sample when the liquid sample is brought into contact with the suspended sample. The contact angle of the liquid sample and the solid sample is mediated by the difference between the surface tension measurements, and the pulling force is less than the surface tension of the liquid. The contact angle is calculated from the relationship between the surface tension and the decline in force.
F…Forces acting on the solid (measured) γ…The surface tension of the liquid (must be known in the case of contact angle measurements) L…The circumference of the solid sample perimeter (must be known) θ…The contact angle of the liquid with the solid (assumed to be 0º) S…The cross-sectional area of the solid sample distance h…The Immersion depth of the solid sample ρ…The density of the liquid sample g…The gravitational acceleration
A solid sample is suspended from the balance and immersed in the liquid. Raising the stage will immerse the solid sample deeper into the liquid and the advancing contact angle θA can be measured. Lowering the stage will pull the solid out of the liquid and the receding contact angle θR can be measured.
The more the solid sample is immersed in the liquid, the more the buoyant force increases, causing the force acting on the balance to decrease. Therefore, for both the advancing contact angle θA and the receding contact angle θR, the obtained weight curves (see the figure on the right) have to be determined through linear regression and the wetting forces have to be extrapolated to zero-depth immersion.
It is known that the penetration rate of liquid into the powder is represented by the Washburn equation.
ｌ… Height of the liquid front ｔ… Time ｒ… Capillary radius of the compressed powder γ… Surface tension of the liquid η… Viscosity of the liquid θ… Contact angle
In the actual measurement, a liquid sample is infiltrated into a column filled with powder, and the change in the weight W is tracked for the elapsed time t. Ideally, the linear relationship is obtained by plotting t for W2. The contact angle and infiltration rate are calculated from the slope of this line. In addition, in order to calculate the contact angle, the powder-filled capillary radius value is required besides the values of liquid surface tension and viscosity. That capillary radius value is determined experimentally by measuring the sufficiently wet liquid for the powder and regarding the contact angle as 0º.