Measurements

Surface Roughness

- Dip Coating
- QCM-D
- Contact Angle
- Critical Micelle Concentration
- Density
- Dynamic Contact Angle
- Interfacial Rheology
- Interfacial Tension
- Powder Wettability
- Surface Roughness
- Sedimentation
- Surface Free Energy
- Surface Tension
- Adhesion force
- Langmuir & Langmuir Blodgett
- Interfacial Shear Rheometry
- Brewster Angle Microscopy
- Surface Potential Sensing

- Measurements
- Surface Roughness

- Dip Coating
- QCM-D
- Contact Angle
- Critical Micelle Concentration
- Density
- Dynamic Contact Angle
- Interfacial Rheology
- Interfacial Tension
- Powder Wettability
- Surface Roughness
- Sedimentation
- Surface Free Energy
- Surface Tension
- Adhesion force
- Langmuir & Langmuir Blodgett
- Interfacial Shear Rheometry
- Brewster Angle Microscopy
- Surface Potential Sensing

Wettability can be studied by measuring the contact angle of a surface with a given liquid. However, the Young equation that describes contact angle assumes that the surface is chemically homogenous and topographically smooth. This is however not true in the case of most real surfaces. In order to get the actual contact angle, surface roughness and contact angle are to be measured simultaneously to get the roughness corrected contact angle.

Both chemical and topographical properties of the surface are important parameters in many different applications and processes, where wetting and adhesion behavior needs to be optimized. Wettability can be studied by measuring the contact angle of the substrate with the given liquid. The well-known Young equation describes the balance at the three-phase contact of solid, liquid and vapor.

γ_{sv}=γ_{sl}+γ_{lv}· cosθ_{Y}

The interfacial tensions, *γ*_{sv}, *γ*_{sl} and *γ*_{lv}, form the equilibrium contact angle of wetting, often referred to as the Young contact angle *θ*_{Y}. The Young equation assumes that the surface is chemically homogenous and topographically smooth. This is however not true in the case of real surfaces, which instead of having one equilibrium contact angle value exhibit a range of contact angles between the advancing and receding ones.

The figure shows the droplet on ideal and real surfaces. On an ideal surface, the Young equation applies and the measured contact angle is equal to the Young contact angle (upper image). On a real surface the actual contact angle is the angle between the tangent to the liquid-vapor interface and the actual, local surface of the solid (lower image). However, the measured (apparent) contact angle is the angle between the tangent to the liquid-vapor interface and the line that represents the apparent solid surface, as seen macroscopically. Actual and apparent contact angle values can deviate substantially from each other. To calculate real surface free energies of the solid the actual contact angles should be used.

*Contact angles and surface roughness.*

The relationship between roughness and wettability was defined in 1936 by Wenzel, who stated that adding surface roughness would enhance the wettability caused by the chemistry of the surface^{3}. For example, if the surface is chemically hydrophobic, it will become even more hydrophobic when surface roughness is added. Wenzel statement can be described with equation below.

cos

θ_{m }=r· cosθ_{Y}

Where *θ*_{m} is the measured contact angle, *θ*_{Y} is the Young contact angle and *r* is the roughness ratio. The roughness ratio is defined as the ratio between the actual and projected solid surface area (*r *= 1 for a smooth surface and *r *> 1 for a rough one) and can be calculated from a 3D roughness parameter *S*_{dr} as shown already. It is important to notice that the Wenzel equation is based on the assumption that the liquid penetrates into the roughness grooves (as in Figure 1). It has been stated that if the droplet is larger than the roughness scale by two to three orders of magnitude, the Wenzel equation applies^{4}. Wenzel corrected contact angles have been utilized for example to study the wettability of paper sheets^{5} and cell adhesion to biomaterial surfaces^{6}. Both micro and nanoscale roughness have been shown to have influence on surface wettability.

For additional information on applications, see:

**Application Note 16 — Adhesion to Wood-Plastic Composites**

**Application Note 17 — Influence of Topography and Wettability on Biocompatibility**

In cases where the liquid does not penetrate into the grooves, the Wenzel equation does not apply. In this case the Cassie equation is used instead. The Cassie equation was first developed to describe chemically heterogeneous surfaces, with two different chemistries^{7}.

cos

θ_{m }=x_{1 }· cosθ_{Y1 }+x_{2 }· cosθ_{Y2}

In the equation above, *x* is the area fraction characterized by the given chemistry and subscripts 1 and 2 indicate two different surface chemistries (Figure a). If, instead of having different chemistries on the surface, the second area is air like (Figure b), then equation can be written as,

cos

θ_{m }=x_{1}(cosθ_{Y}+ 1) – 1

Since contact angle against liquid and air can be considered to be 180° (cos *θ*_{Y2} is -1) and the area fraction *x*_{2} = 1 – *x*_{1}. This equation was developed by Cassie and Baxter^{7} and is thus often called the Cassie-Baxter equation. It has been found that for the droplet to achieve the real Cassie-Baxter stage (no penetration of the liquid inside the grooves), the geometry of the roughness has to be carefully designed^{8}.

The most stable contact angle is the one associated with the absolute minimum of the Gibbs energy curve, which can be connected to Young’s contact angle. The contact angles calculated from the Wenzel and Cassie-Baxter equations have been found to be good approximations of the most stable contact angles^{9}.* *

Surface roughness is a measurement of surface texture. It is defined as a vertical deviation of a real surface from its ideally smooth form. Roughness plays an important role in various processes such as friction and adhesion and is widely measured. Surface roughness cannot be accurately characterized by using a single parameter. Instead, a set of surface roughness parameters is defined. Parameters that characterize surface profiles are called 2D parameters and are marked with the letter ‘*R*’. These parameters are widely utilized in different applications but are not really able to provide the full information on the three-dimensional surfaces. Parameters to characterize surface topography are called 3D parameters and are marked with the letter ‘*S*’. Some of the 3D parameters have their 2D counterparts; others are specifically developed for 3D surfaces^{1}. A summary of these parameters as stated by the ISO 25178 (and their 2D counterparts) is presented in table below^{2, ISO 25178}. *S _{a}* is an arithmetic mean height of the surface.

r= 1 +S_{dr}⁄ 100

- K.J. Stout, P.J. Sullivan, W.P. Dong, E. Mainsah, N. Luo, T. Mathia and H. Zahouani, ‘
*The development of methods for the characterization of roughness in three dimensions*’ (1993) - L. Blunt and X. Jiang, ‘
*Advanced techniques for the assessment of surface topography, Development of a basis for 3D surface texture standards ‘SURFSTAND’*’, Chapter 2, 2003.[ISO 25178]*Geometrical product specifications (GPS) – Surface texture: Areal-Part 2: Terms, definitions and surface texture parameters.* - R. N. Wenzel, ‘
*Resistance of solid surfaces to wetting by water*’, Industrial and engineering chemistry 28 (1936) 988. - A. Marmur, ‘
*Soft contact: Measurement and interpretation of contact angles*’, Soft Matter 2 (2006) 12. - I. Moutinho, M. Figueiredo and P. Ferreira, ‘
*Evaluating surface energy of laboratory-made paper sheets by contact angle measurements*’, TAPPI Journal 6 (2007) 26. - J. I. Rosales-Leal, M. A. Rodríguez-Valverde, G. Mazzaglia, P. J. Ramón-Torregrosa, L. Díaz-Rodríguez, O. García-Martínez, M. Vallecillo-Capilla, C. Ruiz and M. A. Cabrerizo-Vílchez, ‘
*Effect of roughness, wettability and morphology of engineered titanium surfaces on osteoblast-like cell adhesion*’, Colloids and Surfaces A: Physicochemical and Engineering aspects 365 (2010) 222. - A. B. D. Cassie and S. Baxter, ‘
*Wettability of porous surfaces*’, Transactions of the Faraday Society 40 (1944) 546. - A. Tuteja, W. Choi, M. Ma, J. M. Mabry, S. A. Mazzella, G. C. Rutledge, G. H. McKinley and R. H. Cohen, ‘
*Designing superoleophobic surfaces*’, Science 318 (2007) 1618. - A. Marmur, ‘
*Solid-surface characterization by wetting*’, Annual Review of materials research 39 (2009) 473.