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Q10.2(c):
Explain why (c) Surface tension of a liquid is independent of the area of the surface

Solution :

Theoretical Foundation: The Molecular Basis of Surface Tension

Surface tension ($\gamma$) is defined as the force per unit length acting perpendicular to an imaginary line drawn on the liquid surface. It arises due to the unbalanced cohesive forces experienced by molecules at the surface interface [Molecular Theory of Matter].

Step 1: Analyzing Potential Energy at the Interface

Inside the bulk of a liquid, a molecule is surrounded by neighbors on all sides, resulting in a net cohesive force of zero. Conversely, a molecule at the surface experiences a net inward attractive force because there are no liquid molecules above it to balance the downward pull [Newton’s Third Law of Motion applied to Intermolecular Forces].

To move a molecule from the bulk to the surface, work must be done against these inward cohesive forces. This work is stored as potential energy. Thus, the surface of a liquid possesses an excess surface energy.

Step 2: Derivation of the Surface Tension Constant

Consider a rectangular film of liquid of length $l$ being extended by a small distance $\Delta x$.

  • The total work done ($W$) to increase the surface area ($\Delta A$) is given by: $W = \gamma \cdot \Delta A$.
  • Since the surface area has two sides, $\Delta A = 2 \cdot l \cdot \Delta x$.
  • The work done per unit area is: $\gamma = \frac{W}{\Delta A} = \frac{F \cdot \Delta x}{2 \cdot l \cdot \Delta x} = \frac{F}{2l}$.
[Per the principle of Virtual Work].

Step 3: Independence from Surface Area

The surface tension ($\gamma$) is a property that depends solely on the nature of the liquid and the surrounding medium (temperature and impurities).

  • If the area of the surface increases, the number of molecules at the surface increases proportionally.
  • While the total surface energy ($U = \gamma A$) increases, the energy per unit area ($\gamma = \frac{dU}{dA}$) remains constant.
  • Because $\gamma$ is a scalar property defined by the net inward force per unit length—which is a local molecular phenomenon—it does not depend on the macroscopic geometric extent of the surface.

Visual Representation of Surface Molecules

Liquid Surface Interface Inward Pull

Conclusion

Surface tension is an intensive property of the substance. Just as density ($\rho = \frac{m}{V}$) is independent of the total volume of the substance, surface tension is independent of the surface area because it is defined by the average molecular interactions at the boundary layer, which are uniform regardless of the scale of the surface.

Final Solution: Surface tension is an intensive property determined by the cohesive forces between liquid molecules at the interface; therefore, it remains constant irrespective of the total macroscopic area of the surface.


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