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Physics · Ch 7 — Properties of Matter

Surface energy (S.E.) and surface tension (S.T.)

7.5.3

Surface energy (S.E.) and surface tension (S.T.)

SURFACE ENERGY. Inside a liquid, a molecule is pulled equally in all directions by its neighbours; but near the surface, a molecule is pulled predominantly downward (only by molecules below it), so the whole surface layer of the liquid is effectively being pulled inward at all times, and the liquid surface naturally tends toward the smallest possible area. To INCREASE the surface area -- by bringing molecules up from the interior to the surface -- work must be done against this inward-pulling force, and the amount of work done is stored as potential energy in the newly created surface: this is why surface molecules always carry greater potential energy than molecules deeper in the liquid. SURFACE ENERGY is defined as this excess energy per unit area of the liquid's free surface, or equivalently the work done in increasing the surface area per unit increase in that area: S.E.=ΔWΔA\text{S.E.}=\dfrac{\Delta W}{\Delta A}, expressed in units of J m−2^{-2} (equivalently N m−1^{-1}). SURFACE TENSION is separately defined as the force per unit length of the liquid's surface, T=FlT=\dfrac{F}{l}, with SI unit N m−1^{-1} and dimensional formula MT−2MT^{-2}. RELATION BETWEEN SURFACE TENSION AND SURFACE ENERGY. Consider a rectangular wire frame ABCD holding a horizontal soap film, with side AB free to slide. The soap film, having TWO free surfaces (front and back), pulls AB inward with a force F=(2T)lF=(2T)l due to surface tension. If AB is moved outward by a small distance Δx\Delta x to a new position A'B', the work done against this inward force is Work=F×Δx=(2Tl)(Δx)\text{Work}=F\times\Delta x=(2Tl)(\Delta x), while the increase in the film's total surface area (counting both faces) is ΔA=(2l)(Δx)=2l Δx\Delta A=(2l)(\Delta x)=2l\,\Delta x. Therefore, surface energy=work doneincrease in surface area=2Tl Δx2l Δx=T\text{surface energy}=\dfrac{\text{work done}}{\text{increase in surface area}}=\dfrac{2Tl\,\Delta x}{2l\,\Delta x}=T -- proving that the surface energy per unit area of a liquid surface is NUMERICALLY EQUAL to its surface tension, which is why the two quantities are so often used interchangeably in practice even though they are conceptually disti …

Figure 7.25Horizontal soap film on a rectangular frame of wire ABCD

What this figure shows. A rectangular wire frame ABCD holds a horizontal soap film, with side AB free to slide; a force F = 2Tl (the factor of 2 present because the film has two free surfaces, front and back) pulls AB inward due to surface tension. The figure shows AB displaced outward by a small distance delta-x to a new position A'B', stretching the soap film and increasing its total surface area by 2l times delta-x; equating the work done, (2Tl)(delta-x), to this increase in area is the derivation that shows surface energy per unit area equals surf …

Misc Example 7.10Surface tension of soap solution from work done

Worked out. Given that 2.4 x 10^-4 J of work increases the area of a soap-bubble film from 50 square centimetres to 100 square centimetres, the increase in surface area is doubled to account for the bubble's two free surfaces, giving delta-A = 100 x 10^-4 square metres; dividing the work done by this doubled area gives the surface tension of the soap solution as 2.4 x 10^-2 N per metre, a direct numerical use of the surface-energy-equals-surface-tension relation for a …