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Question

Derive Laplace's law for spherical membrane of bubble due to surface tension.

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Solution

Consider a spherical liquid drop and let the outside pressure be P0 and inside pressure be Pi, such that the excess pressure is PiPo.
Let the radius of the drop increase from Δr, where Δr is very small, so that the pressure, inside the drop remains almost constant.
Initial surface area (A1)=4πr2
Final surface area (A2)=4πr2
=4π(r+Δr)2
=4π(r2+2rΔr+Δr2)
=4πr2+8πrΔr+4πΔr2
As Δr is very small Δr2 is neglected (i.e. 4πΔr2=0)
Increase in surface area (dA)=A2=A1=4πr2+8πrΔr4πr2
In crease in surface area (dA)=8πrΔr
Work done to increase the surface area 8πrΔr is extra energy.
dW=TdA
dW=T×8πrΔr .....(1)
This work done is equal to the product of the force and the distance Δr
dF=(PiPo)4πr2×r2
The increase in the radius of the bubble is Δr.
dW=dFΔr=(PiPo)4πr2×Δr2 ...(2)
Comparing equation (1) and (2), we get
(PiPo)4πr2×Δr=T×8πrΔr
(PiPo)=2T/r
This is called the Laplace's law of spherical membrane.
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