Thermal: Entropy of Ideal Gas (Sackur-Tetrode equation)

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SUMMARY

The discussion focuses on the Sackur-Tetrode equation, which describes the entropy of an ideal gas and incorporates mass as a critical parameter. Mass influences the thermal wavelength, defined as ##\lambda = (\frac{\beta \hbar^2}{2\pi m})^{1/2}##, establishing the classical regime for the gas. The relationship between mass and multiplicity of states is emphasized, as mass affects the spacing between energy levels, thereby impacting the number of accessible microstates. This connection illustrates that mass is integral to understanding entropy in thermal systems.

PREREQUISITES
  • Understanding of the Sackur-Tetrode equation
  • Familiarity with thermal wavelength concepts
  • Knowledge of microstates and multiplicity in statistical mechanics
  • Basic principles of classical ideal gas behavior
NEXT STEPS
  • Study the derivation and implications of the Sackur-Tetrode equation
  • Explore the concept of thermal wavelength in detail
  • Investigate the relationship between mass and energy levels in quantum systems
  • Examine statistical mechanics principles related to microstates and entropy
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Students and professionals in physics, particularly those studying thermodynamics, statistical mechanics, and quantum mechanics, will benefit from this discussion.

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okay so I suck at La-Tex so I'm not going to put the actual equation, but it's not important for my question.

In the equation the entropy is dependent on the natural log with mass in the numerator of the argument. Why is mass involved when talking about entropy at all?

I mean I think of entropy as being related to multiplicity of states or whatever, which is independent of mass? is rest mass energy being involved here?
 
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The mass (which yes means the rest mass) is one of the parameters in the thermal wavelength of the gas that appears in the Sackur-Tetrode equation ##\lambda = (\frac{\beta \hbar^2}{2\pi m})^{1/2}## and it defines the characteristic length scale of the thermal system. In other words it sets the scale for which the gas can actually be considered classical i.e. for which the Sackur-Tetrode equation is actually valid. So in this sense it is almost self-evident that the mass should show up in the expression for the entropy.

Now as far as multiplicity goes, there is no reason to expect mass not to be a factor in the multiplicity. Recall the multiplicity is the number of accessible microstates of a system in between two infinitesimally separated average energy levels of the system and as such the multplicity will involve some characteristic spacing between average energy levels in the determination of this volume; this characteristic spacing will of course depend on various scales of the system. For a two-level system of spins with magnetic moment ##\mu## in an external uniform magnetic field ##B## we have ##\Omega \propto \frac{\delta E}{2\mu B}## where the proportionality is the number of microstates for a given average energy. This characteristic spacing clearly depends on properties of the system such as the applied magnetic field and the intrinsic magnetic moment of the spins. For an ideal gas it is the thermal wavelength that we are interested in and in particular for a classical ideal gas we must have the intermolecular spacings much larger than the thermal wavelength so this will definitely show up in the entropy.
 

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