Viscosity and thermal diffusivity in liquids and gases

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SUMMARY

Viscosity (μ) measures momentum flux, while thermal diffusivity (α) measures heat flux in fluids. In gases, both properties are similar due to molecular collisions, but this relationship diverges in liquids, particularly in very viscous fluids where μ/ρ >> α (ρ being density). Liquid metals exhibit the opposite behavior with μ/ρ << α. The differences in these properties are further elucidated through the Prandtl number and are discussed in detail in the book "Transport Phenomena." Understanding statistical physics and kinetic theory is essential for a deeper grasp of these concepts.

PREREQUISITES
  • Understanding of viscosity and thermal diffusivity
  • Familiarity with the Prandtl number
  • Basic knowledge of molecular collisions in gases
  • Introduction to statistical mechanics
NEXT STEPS
  • Study the Prandtl number and its implications in fluid dynamics
  • Explore the concepts of kinetic theory of gases
  • Read "Transport Phenomena" for in-depth analysis of viscosity and thermal diffusivity
  • Investigate the behavior of liquid metals in thermal and viscous contexts
USEFUL FOR

Students and professionals in physics, chemical engineering, and materials science who are interested in fluid dynamics, particularly those studying the properties of liquids and gases.

dRic2
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Hi PF, I was wondering about this for some time and I can get my head around it.

Viscosity ##\mu## is a "measure" of the momentum flux
Thermal diffusivity ##\alpha## is a "measure" of the heat flux (kinetic energy of molecules)

In gases both viscous stresses and heat flux take place due to collisions between molecules thus the value of viscosity and thermal diffusivity is similar. That doesn't apply to liquids. In particular for very viscous fluids
##\frac \mu \rho >> \alpha## (##\rho## is the density). Since both phenomena happen for the same reason (collisions) I can't explain myself why there is this huge difference.

Ps: for liquid metals ##\frac \mu \rho << \alpha##
 
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The molecular derivation of these quantities and their comparisons (the Prandtl number) are explained in detail in Transport Phenomena.
 
Yes, but there is a lot of statistical physics (kinetic theory of gases) which I know nothing about. I was looking for an easier explanation if possible... Otherwise I'll have to wait until I know something about statistical mechanics
 

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