How Do Soluble Bubble Dynamics Change in Deep Liquid Pools?

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SUMMARY

The discussion focuses on the dynamics of soluble bubble behavior in deep liquid pools, specifically addressing the material balance equations governing their rise. It establishes that the mass transfer coefficient, k_c, remains constant for spherical bubbles in free rise, leading to a specific relationship between bubble radius and pressure. The transformation of variables allows the material balance equation to be reformulated, demonstrating the relationship between bubble size and dissolution effects. Key equations include the ideal gas law for molar density and the pressure-depth relationship in the liquid.

PREREQUISITES
  • Understanding of the ideal gas law and its application in fluid dynamics.
  • Familiarity with mass transfer concepts, particularly the mass transfer coefficient, k_c.
  • Basic knowledge of calculus and algebra for manipulating differential equations.
  • Comprehension of fluid mechanics principles, including pressure and buoyancy effects.
NEXT STEPS
  • Study the derivation and implications of the material balance equation for soluble bubbles.
  • Research the effects of liquid viscosity on bubble rise velocity and size.
  • Explore the relationship between molar solubility and gas dissolution in liquids.
  • Learn about advanced fluid dynamics simulations to model bubble behavior in various liquid depths.
USEFUL FOR

Researchers in fluid dynamics, chemical engineers, and students studying mass transfer phenomena in liquids will benefit from this discussion, particularly those focusing on bubble dynamics and dissolution processes.

VinnyCee
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Homework Statement



When an insoluble bubble rises in a deep pool of liquid, its volume increases according to the ideal gas law. However, when a soluble bubble rises from deep submersion, there is a competing action of dissolution that tends to reduce size. Under practical conditions, it has been proven that the mass transfer coefficient, k_c, for spherical bubbles in free-fall (or free-rise) is constant. Thus, for sparingly soluble bubbles released from rest, the applicable material balance is

\frac{d}{dt}\,\frac{4\,C\,\pi}{3}\,R^3\,=\,-k_c\,C^*\,4\pi\,R^2

where the molar density of the gas

C\,=\,\frac{P}{R_g\,T}

with R_g and T as the ideal gas constant and temperature, respectively. C^* is the molar solubility of the gas in the liquid, and R(t) is the bubble radius, which changes over time. The pressure P at a distance z from the top of the liquid surface is

P\,=\,P_A\,+\,\rho_L\,g\,z

where \rho_Lis the liquid density and g is the gravitational acceleration. The rise velocity, \frac{dz}{dt}, follows a linear relation between speed and size

\frac{dz}{dt}\,=\,\beta\,R(t)

where \beta is a constant that depends on the liquid viscosity.SHOW that a change of variables allows the material balance equation to be written as

R\,\frac{dR}{dP}\,+\,\left(\frac{1}{3}\right)\,\frac{R^2}{P}\,=\,-\frac{\lambda}{P}

and

\lambda\,=\,\frac{k_c\,R_g\,T\,C^*}{\rho_L\,g\,\beta}

Homework Equations



Algebra and the Calculus.

The Attempt at a Solution



\frac{dz}{dt}\,=\,\beta\,R(t)

\frac{d}{dt}\,=\,\beta\,R(t)\,\frac{d}{dz}

Substituting into the original material balance equation:

\beta\,R(t)\,\frac{d}{dz}\,\left(\frac{P}{R_g\,T}\,\frac{4\pi\,R^3}{3}\right)\,=\,-k_c\,C^*\,4\pi\,R^2

Here I am stuck, how do I "show" that the two versions of the material balance equations are equivalent?
 
Last edited:
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Hey I am doing this question at the moment, I found this thread while doing a google search. Do you remember how you solved it?

I've reached about just as far, but I've found lambda by using dP/dz = rhoL*g

(Don't really know how to use html code tbh.)

Any help is appreciated, thanks.
 

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