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Q9.2(b):
Explain why (b) Water on a clean glass surface tends to spread out while mercury on the same surface tends to form drops. (Put differently, water wets glass while mercury does not.)

Solution :

Theoretical Foundation: Intermolecular Forces

The behavior of a liquid in contact with a solid surface is determined by the competition between two types of molecular forces:

  • Cohesive Forces ($F_c$): Forces of attraction between molecules of the same substance.
  • Adhesive Forces ($F_a$): Forces of attraction between molecules of different substances (liquid and solid).

The wetting behavior is defined by the angle of contact ($\theta$), which is the angle between the tangent to the liquid surface at the point of contact and the solid surface inside the liquid.

Step 1: Analysis of Water on Clean Glass

In the case of water on glass, the adhesive forces between water molecules and glass molecules are significantly stronger than the cohesive forces between water molecules ($F_a > F_c$).

Per the conditions of surface tension equilibrium at the solid-liquid-gas interface:

  • Since $F_a > F_c$, the liquid molecules are pulled toward the glass surface.
  • This results in an acute angle of contact ($\theta < 90^\circ$).
  • The surface tension of the solid-gas interface ($\gamma_{sg}$) is greater than the sum of the liquid-solid ($\gamma_{ls}$) and liquid-gas ($\gamma_{lg}$) interfacial tensions, expressed by Young’s Equation: $\cos \theta = \frac{\gamma_{sg} - \gamma_{ls}}{\gamma_{lg}}$.
  • Because $\theta$ is acute, the water spreads to maximize contact with the surface, thereby "wetting" the glass.

Step 2: Analysis of Mercury on Clean Glass

In the case of mercury on glass, the cohesive forces between mercury molecules are significantly stronger than the adhesive forces between mercury and glass molecules ($F_c \gg F_a$).

  • Because $F_c$ dominates, the mercury molecules prefer to stay attached to each other rather than adhering to the glass.
  • This leads to a convex meniscus and an obtuse angle of contact ($\theta > 90^\circ$, typically $\approx 135^\circ$).
  • The energy required to wet the surface is unfavorable; therefore, the mercury minimizes its surface area in contact with the glass by forming spherical or near-spherical droplets.

Visual Representation of Contact Angles

Water: $\theta < 90^\circ$ Mercury: $\theta > 90^\circ$

Summary Table of Interfacial Characteristics

Liquid Dominant Force Contact Angle ($\theta$) Surface Behavior
Water Adhesion ($F_a > F_c$) Acute Wetting (Spreading)
Mercury Cohesion ($F_c > F_a$) Obtuse Non-wetting (Droplet formation)

Final Solution: Water wets glass because the adhesive forces between water and glass molecules dominate, causing the liquid to spread to minimize surface energy at an acute contact angle. Conversely, mercury forms droplets because its cohesive forces are significantly stronger than the adhesive forces, forcing the liquid to minimize its contact area with the glass at an obtuse contact angle.


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