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 Pi−Po. 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+8πrΔr−4πr2 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=(Pi−Po)4πr2×r2 The increase in the radius of the bubble is Δr. dW=dFΔr=(Pi−Po)4πr2×Δr2 ...(2) Comparing equation (1) and (2), we get (Pi−Po)4πr2×Δr=T×8πrΔr ∴(Pi−Po)=2T/r This is called the Laplace's law of spherical membrane.