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Question: One drop of soap bubble of diameter\(D\)breaks into 27 drops having surface tension \(\sigma .\)The ...

One drop of soap bubble of diameterDDbreaks into 27 drops having surface tension σ.\sigma .The change in surface energy is?
(A) 2πσD22\pi \sigma {D^2}
(B) 4πσD24\pi \sigma {D^2}
(C) 8πσD28\pi \sigma {D^2}
(D) πσD2\pi \sigma {D^2}

Explanation

Solution

As one drop breaks into number of drops then by volume conservation. We can conclude that, volume of one drop of bubble will be equal to the sum of volumes of 27 drops of soap bubbles.
Formula used:
ΔE=T.ΔA\Delta E = T.\Delta A
Here, ΔE\Delta E is the change in energy
TT is the surface tension
AA is the cross-sectional area
Complete step by step answer:
Soap bubble is of spherical shape and the volume of sphere is 43πr3\dfrac{4}{3}\pi {r^3}
Since the volume of larger drop is equal to the sum of volumes of the smaller drops
43πR3=n43πr3\dfrac{4}{3}\pi {R^3} = n\dfrac{4}{3}\pi {r^3}
Where, RR is radius of large drop
rr is radius of small drops
n=27n = 27is the number of drops
Put these values in the above equation
43πR3=\Rightarrow \dfrac{4}{3}\pi {R^3} = 27×43πr327 \times \dfrac{4}{3}\pi {r^3}
Common factors will cancel each other
R=27  13×r\Rightarrow R\:=\:{{27}\;^\dfrac{1}{3}}\times{r}
Simplifying and rearranging the equation, we get
r=R3r = \dfrac{R}{3} . . . (1)
We know that the surface tension is equal to the surface energy per unit area.
\therefore Surface energy =T.A = T.A
Final surface area of Bubble droplets (A2)=n.4πr2({A_2}) = n.4\pi {r^2}
Initial surface area of Bubble drop(A1)=4πR2({A_1}) = 4\pi {R^2}
Change in energyΔE=T.ΔA\Delta E = T.\Delta A
Where ΔA\Delta Ais changed in the area.
ΔE=T(A2A1)\Rightarrow \Delta E = T({A_2} - {A_1})
=T[n.4πr24πR2]= T[n.4\pi {r^2} - 4\pi {R^2}]
Take common terms out
ΔE=T.4π[nr2R2]\therefore \Delta E = T.4\pi [n{r^2} - {R^2}]
Substitute the value of rr from equation (1) in the above equation
ΔE=T.4π[27(R3)2R2]\Rightarrow \Delta E = T.4\pi \left[ {27{{\left( {\dfrac{R}{3}} \right)}^2} - {R^2}} \right]
Take R2{R^2}common
ΔE=T.4πR2[2791]\Rightarrow \Delta E = T.4\pi {R^2}\left[ {\dfrac{{27}}{9} - 1} \right]
On simplifying we get
ΔE=T.4πR2[31]\Delta E = T.4\pi {R^2}[3 - 1]
ΔE=T.4πR2[2]\Rightarrow \Delta E = T.4\pi {R^2}[2]
=8πR2T= 8\pi {R^2}T
Since, it is given that the surface tension is σ,\sigma ,we get
ΔE=2.4πR2.σ\Delta E = 2.4\pi {R^2}.\sigma
ΔE=2πD2σ\Rightarrow \Delta E = 2\pi {D^2}\sigma
Hence,option (A) is the correct one.

Note: Surface tension is the tendency of liquid surface to shrink into the minimum surface area possible. We should know that surface energy decreases with increase in temperature and it will also change when larger drop breaks into smaller droplets.