Contact Angle, θ 

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When a liquid does not completely spread on a substrate (usually a solid), a contact angle (θ) is formed, which is geometrically defined as the angle on the liquid side of the tangential line drawn through the three phase boundary where a liquid, gas and solid intersect, or two immiscible liquids and solid intersect.

Summary/Description:

Contact angle is a quantitative measure of the wetting of a solid by a liquid. It is the angle formed by the liquid at the three phase boundary where a liquid, gas (or a second immiscible liquid) and solid intersect. It is a direct measure of interactions taking place between the participating phases (gas/liquid/solid or liquid/liquid/solid). The contact angle is determined by drawing a tangent at the contact where the liquid and the solid intersect.

The shape of the drop and the magnitude of the contact angle are controlled by three interaction forces of interfacial tension of each participating phase (gas, liquid and solid). In an ideal situation the relation between these forces and the contact angle can be described by the Young's equation and is often also referred to as Young's contact angle. However, often non-ideal conditions due environmental, roughness and chemical heterogeneity effects leads to deviations from this relationship. Many other theoretical approaches based on the Young's equation have therefore been developed to account for these non-ideal contributions. The non-ideal contact angles are referred to as apparent contact angles.

It is often necessary to distinguish between the Static (Equilibrium) Contact Angle (θe) and Dynamic Contact Angles (DCA) i.e. Advancing Contact Angle (θa) and Receding Contact Angle (θr). When θr α θa the system is said to exhibit contact angle hysteresis.






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