Describing the motion of a bubble through water

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SUMMARY

The motion of a 1 mm diameter air bubble released in glycerol at room temperature is analyzed using the drag force equation, Drag Force = -4πηRv, where η is the viscosity of glycerol, R is the bubble's radius, and v is its velocity. The bubble's initial acceleration is determined to be 2g, contrasting with the calculated 1g using F = ma. The negligible mass of the air inside the bubble and the influence of Archimedes' principle are critical in understanding the dynamics of the bubble's motion through the viscous liquid.

PREREQUISITES
  • Understanding of fluid dynamics principles
  • Familiarity with Newton's second law (F=ma)
  • Knowledge of drag force calculations
  • Basic concepts of buoyancy and Archimedes' principle
NEXT STEPS
  • Study the effects of viscosity on bubble dynamics in different fluids
  • Learn about the derivation and application of the drag force equation for non-rigid bodies
  • Explore the implications of Archimedes' principle in fluid mechanics
  • Investigate the behavior of bubbles in various liquid viscosities and temperatures
USEFUL FOR

Students and professionals in physics, particularly those focusing on fluid dynamics, as well as engineers working with bubble dynamics in various applications.

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Homework Statement



A bubble of air which is 1 mm in diameter is released without initial velocity in the
volume of glycerol at room temperature. Describe the motion of the bubble as a
function of time assuming that its diameter remains unchanged. Note that friction
force acting on the bubble is given by

Drag Force = -4\pi\etaRv

where h is the viscosity of the liquid, R is the radius of the bubble, and v is its
velocity. Note that the numerical coefficient in this formula is different from that for a
solid sphere moving in the liquid (which is 6π). Explain qualitatively why the
numerical coefficients in tbubble are different.


Homework Equations



F=ma
F=\rhoVg


The Attempt at a Solution



Tell me if I'm going about this the wrong way. To describe the motion of the bubble, which is essentially finding the function of position with respect to time, I equated F = ma = Fb - Ff. Then integrating knowing that the initial conditions for velocity and position are 0, perhaps this could be it?

As I researched, however, I had found that the initial acceleration for the bubble starting at rest to be 2g, whereas, by my method, i would only get 1g.

Other considerations I had heard from discussion are that the mass of the air inside the bubble is negligible, so am i supposed to use the mass of water in contact to the surface when calculating "m" ? In addition I had also heard something about work, but i have no idea how that plays in this problem.

As for the second part, I thought about how...since the bubble is not a rigid body, the molecules themselves are in a circular flow that ultimately act as a .. buffer of some sort? i know I am not making sense but i know there should be a difference between fluid in contact with fluid and fluid in contact with a solid.
 
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Do not forget about Archimedes' principle when counting forces.

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