Reservoir Engineering: Contact Angle Measurement

1. To what extent, the ‘gravitational force’ plays a crucial role:

(a) when the fluid flow remains to be perfectly horizontal;

(b) when the fluid flow remains to be perfectly vertical;

(c) when the fluid flows at an angle towards gravity; and

(d) when the fluid flows at an angle against gravity; - towards dictating whether

(i) the cohesive forces between the liquid molecules remain to be stronger than the adhesive forces between the solid and liquid molecules (and as a result, the liquid balls up and tending to avoid contact with the surface); or,

(ii) the solid/liquid adhesion remaining stronger than the cohesion within the liquid molecules (and as a result, no drop forms and the liquid tending to spread on the surface)?

Whether such role of ‘gravity’ would remain to be similar both @ laboratory-scale as well as @ field-scale?

If not, how would ‘contact angle’ measured @ laboratory-scale would be able to provide ‘an inverse measure of wettability’ @ field-scale?

2. In the absence of an atomically flat and chemically homogenous ideal surface – associated with a real field reservoir scenario; (for that matter, even with laboratory-scale experimental conditions), whether force per unit length OR energy per unit area would remain to be more apt towards the determination of contact angles (where, the formation of a perfect spherical cap geometry remains ruled out)?

3. Which one of the following essentially controls the wettability @ laboratory-scale? (a) the advancement of solid/liquid interface to a certain area; OR (b) the advancement of three-phase contact line to a certain length; upon placing a sessile droplet on a substrate?

4. Which one of them plays a very crucial role in ceasing the apparent contact angle @ field-scale?

(a) the surface roughness;

(b) the chemical heterogeneity of surface; or

(c) physical/chemical properties of reservoir fluids.

5. Even, if we manage to measure advancing, receding and static apparent contact angles along with the details of contact angle hysteresis – towards determining the properties of surface; whether the nature of surface roughness, chemical heterogeneity and shear hydrophobicity @ laboratory-scale and @ field-scale would more or less remain to be the same?

6. Why does apparent contact angle remain to be significantly different from (a) advancing contact angle;

(b) receding contact angle; and

(c) local contact angle?

7. How important is the ratio of drop-size to wavelength towards contact angle measurement?

8. How exactly could we get rid-off stick-slip movement of drops; and what exactly happens when the drop volume exceeds 10 micro-liters – towards contact angle measurement?

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