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Question: A drop of liquid of radius \(R = {10^{ - 2\,}}\,m\) having surface tension \(S = \dfrac{{0.1}}{{4\pi...

A drop of liquid of radius R=102mR = {10^{ - 2\,}}\,m having surface tension S=0.14πNm1S = \dfrac{{0.1}}{{4\pi }}\,N{m^{ - 1}} divides itself into KK identical drops. In this process the total change in the surface energy ΔU=103J\Delta U = {10^{ - 3}}\,J. If K=10αK = \,{10^\alpha } then the value of the α\alpha is

Explanation

Solution

From the given radius of the large raindrop, calculate the relation for the area of the small and the large raindrop. Using the formula of loss of energy, and the relation of the areas of the small and the large raindrop, find the value of the KK. From it, find α\alpha .

Useful formula:
(1) The volume of the sphere is given by
V=43πR3V = \dfrac{4}{3}\pi {R^3}
Where VV is the volume of the sphere and RR is the radius of the sphere.
(2) The loss in the energy is given by
ΔU=S×dA\Delta U = S \times dA
Where ΔU\Delta U is the loss in the energy, SS is the surface tension of the raindrop and dAdA is the increase in the area of the small rain drops.
Complete step by step solution:
It is given that
The large raindrop is divided into many small rain drops.

The radius of the large rain drops, R=102mR = {10^{ - 2\,}}\,m
The surface tension of the raindrop, S=0.14πNm1S = \dfrac{{0.1}}{{4\pi }}\,N{m^{ - 1}}
The change in the energy, ΔU=103J\Delta U = {10^{ - 3}}\,J
From the question, it is clear that the large volume of rain drops breaks into KK small volume of rain drops.
V=KvV = Kv
43πR3=K(43πr3)\dfrac{4}{3}\pi {R^3} = K\left( {\dfrac{4}{3}\pi {r^3}} \right)
By simplifying the above equation,
R3=Kr3{R^3} = K{r^3}
r=K13Rr = {K^{\dfrac{{ - 1}}{3}}}R -------------------(1)
The difference in the area of the water drop is obtained by subtracting the area of the small water drop from the large.
dA=AadA = A - a
dA=K4πr24πR2dA = K4\pi {r^2} - 4\pi {R^2}
By simplifying the above equation and also substituting (1) in above equation.
dA=4πR2(K131)dA = 4\pi {R^2}\left( {{K^{\dfrac{1}{3}}} - 1} \right)
By using the formula for loss in energy,
ΔU=S×dA\Delta U = S \times dA
103=0.14π×4πR2(K131){10^{ - 3}} = \dfrac{{0.1}}{{4\pi }} \times 4\pi {R^2}\left( {{K^{\dfrac{1}{3}}} - 1} \right)
By further simplification of the above equation.
102=K131{10^2} = {K^{\dfrac{1}{3}}} - 1
100=K131100 = {K^{\dfrac{1}{3}}} - 1
By doing simple arithmetic operation,
K=106K = {10^6}

It is given that the K=10αK = \,{10^\alpha }, from that the value of the α\alpha is obtained as 66.

Note: The shape of the rain drop is larger at the bottom and the smaller at the top. This is mainly due to the surface tension of the rain water. This forms the spherical skin for the raindrop. Remember the formula of the loss in the energy.