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Derive Laplace’s law for spherical membrane of bubble due to surface tension. - Physics

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

Derive Laplace’s law for a spherical membrane.

Derivation
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Solution 1

Consider a spherical liquid drop and let the outside pressure be Po and inside pressure be Pi, such that the excess pressure is Pi − P

Let the radius of the drop increase from r to 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) = 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  

Increase in surface area (dA) =8ΠΔr

Work done to increase the surface area by 8ΠrΔr is extra energy.

∴ dW = TdA

∴ dW = T*8πrΔr         .......(Equ.1)

This work done is equal to the product of the force and the distance Δr.

dF=(P1 - P0)4πr

The increase in the radius of the bubble is Δr.

dW = dFΔr = (P1 - P0)4Πr2*Δr  ..........(Equ.2)

Comparing Equations 1 and 2, we get

(P1 - P0)4πr2*Δr = T*8πrΔr 

∴`(P_1 - P_0) = (2T)/R`

This is called Laplace’s law of spherical membrane.  

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Solution 2

  1. The free surface of drops or bubbles is spherical in shape.
    Let,
    Pi = inside pressure of a drop or air bubble
    Po = outside pressure of the bubble
    r = radius of drop or bubble.
  2. As drop is spherical, Pi > Po
    ∴ excess pressure inside drop = Pi − P
  3. Let the radius of drop increase from r to r + ∆r so that inside pressure remains constant.
  4. Initial area of drop A1 = 4πr2 ,
    Final surface area of drop A2 = 4π (r + ∆r)
    Increase in surface area,
    ∆A = A2 − A1 = 4π[(r + ∆r)2 − r2]
    = 4π[r2 + 2r∆r + ∆r2 − r2]
    = 8πr∆r + 4π∆r2
  5. As ∆r is very small, the term containing ∆r2 can be neglected.
    ∴ dA = 8πr∆r
  6. Work is done by a force of surface tension,
    dW = TdA = (8πr∆r)T ….(1)
    This work done is also equal to the product of the force F which causes an increase in the area of the bubble and the displacement Δr which is the increase in the radius of the bubble.
    ∴ dW = FΔr
    The excess force is given by,
    (Excess pressure) × (Surface area)
    ∴ F = (Pi – Po) × 4πr
    ∴ dF = (Pi – Po)A
    dW = F∆r = (Pi − Po) A∆r
    From equation (1),
    (Pi − Po) A∆r = (8πr∆r) T
    ∴ Pi − Po = `(8pirDeltarT)/(4pir^2Deltar)` ........(∵ A = 4πr2)
    ∴ Pi − Po = `(2T)/r` ….(2)

Equation (2) represents Laplace’s law of spherical membrane. 

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Chapter 2: Mechanical Properties of fluids - Long Answer

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