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Question: A disc of paper of radius \(r\) is floating on the surface of water of surface tension \(T\). Then f...

A disc of paper of radius rr is floating on the surface of water of surface tension TT. Then force of surface tension on the disc is
(A) T.πrT.\pi r
(B) T.2πrT.2\pi r
(C) T.4πrT.4\pi r
(D) T2πr\dfrac{T}{{2\pi r}}

Explanation

Solution

Consider a liquid filled in a beaker and imagine a line at the surface of the liquid which divides the surface into two parts, then it is observed that the surfaces pull each other apart with a force that is proportional to the length of the imaginary line. This force is perpendicular to the imaginary line. The force is known as the surface tension. Use this concept to find the force of surface tension on the paper disc.

Complete step by step solution:
The force due to surface tension is proportional to the length considered, it is given as FlF=TlF \propto l \to F = Tl, where TT is the surface tension. If you consider an elementary length dldl, then the force on the infinitesimally small element will be F=TdlF = Tdl.
Consider a paper disc floating on the surface of water having surface tension TT. If you observe the rim of the paper disc, the water will apply force on each element on the rim perpendicular to the length of the element, that is radially outward. Now, consider any element on the rim of length dldl.
The force on this element will be dF=TdldF = Tdl as discussed above. The length of this element can be written in terms of the radius and the angle subtended by the element at the centre and will be given as dl=rdθdl = rd\theta . So, the force will be dF=TrdθdF = Trd\theta . If you want the total force on the disc, then integrate the force taking the limit of θ\theta going from 02π0 \to 2\pi .
Ftotal=dF=02πTrdθ=Tr02πdθ=Tr2π{F_{total}} = \int {dF = \int\limits_0^{2\pi } {Trd\theta } } = Tr\int\limits_0^{2\pi } {d\theta } = Tr2\pi
Therefore, force of surface tension on the disc is T.2πrT.2\pi r
Option (B) is correct.

Note: If you imagine a line on the surface of a liquid, it is found that the surface on one side of the line pulls the surface on the other side of the line. This force is proportional to the length of the imaginary line. Mathematically, FlF=TlF \propto l \to F = Tl where TT is the surface tension. So, while solving for questions of this type, always take elemental length and find the force on that element, then integrate to find the net force on the boundary of the object.