How Does Kinetic Theory Apply to Real Gas Behavior with Few Atoms?

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Discussion Overview

The discussion revolves around the application of kinetic theory to real gas behavior, particularly in scenarios involving a small number of atoms. Participants explore the derivation of the ideal gas equation and the implications of momentum changes during atomic collisions with container walls.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how momentum changes from individual atomic collisions can be considered collectively to derive pressure in the context of kinetic theory.
  • Another participant uses an analogy of spraying a hose to explain how individual momentum contributions from gas molecules result in a net force that averages to produce pressure.
  • A participant raises concerns about the assumption of a large number of atoms in the gas, suggesting that with few atoms, the concept of average pressure over a large area may not be valid.
  • Further clarification is provided that the impulse transferred during collisions is what contributes to pressure, and that the mean pressure can be calculated from the mean impulses and impact frequency.
  • One participant asserts that kinetic theory assumes a large number of identical molecules, citing that even a small volume of gas contains a significantly large number of molecules (approximately 6x10^23 for 1 mol).

Areas of Agreement / Disagreement

Participants express differing views on the necessity of a large number of atoms for kinetic theory to apply effectively. While some agree on the importance of averaging effects over many collisions, others question the validity of this assumption in cases with few atoms.

Contextual Notes

The discussion highlights limitations in applying kinetic theory to systems with a small number of atoms, particularly regarding the assumptions of averaging and the definition of pressure in such contexts.

kelvin490
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I have a question about deriving the equation of kinetic theory of ideal gas - PV=1/3 Nmcr2, where N is number of atoms, cr is root mean square of atom speed and m is mass of one atom.

In deriving the equation, many textbooks consider the total rate of change of momentum within a certain time and calculate the pressure. However, in actual case the atoms collide on the wall of container separately at different position at different time, how can these changes of momentum be considered as a whole?
 
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If you spray a hose against a door, the door will move. each drop of water has imparted its share of momentum. Likewise with the molecules hitting the sides of the container. It is the normal component of the momentum of each that imparts an impulse onto the side. The effect is to produce a net force that is averaged over the area to give a pressure. Is that enough or is something still not right for you? This has given a number of people trouble.
 
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sophiecentaur said:
If you spray a hose against a door, the door will move. each drop of water has imparted its share of momentum. Likewise with the molecules hitting the sides of the container. It is the normal component of the momentum of each that imparts an impulse onto the side. The effect is to produce a net force that is averaged over the area to give a pressure. Is that enough or is something still not right for you? This has given a number of people trouble.

You answer helps me to understand, but I still have a point needs to clarify. In your example the sprayed water has huge amount of molecules. In kinetic theory, is it also a necessary assumption that huge amount of atoms are present in the container of gas? Imagine in the case there is a few number of atoms, the container wall is just collided occasionally and it doesn't seem make sense to consider the average pressure for a relatively large area of container wall.
 
kelvin490 said:
However, in actual case the atoms collide on the wall of container separately at different position at different time, how can these changes of momentum be considered as a whole?

If by this you are wondering about molecules impacting on the wall with every possible angle of incidence and a wide distribution of free-path energies, you can relax. Those changes in momentum are defined as impulses.

Only the impulse normal to and toward the wall is transferred at the instant of impact. The mean pressure in Pascals is the simple product of the mean value of those impulses in Newtons and the mean number of impacts per square meter of surface (flux).

Pressure equals flux times the impulse.
 
kelvin490 said:
You answer helps me to understand, but I still have a point needs to clarify. In your example the sprayed water has huge amount of molecules. In kinetic theory, is it also a necessary assumption that huge amount of atoms are present in the container of gas? Imagine in the case there is a few number of atoms, the container wall is just collided occasionally and it doesn't seem make sense to consider the average pressure for a relatively large area of container wall.

Kinetic theory assumes a huge number of identical molecules. As an example, 0.024 m3 volume contains1 mol gas at room temperature and at atmospheric pressure. 1 mol substance contains about 6x1023 molecules. Is it big enough?



ehild
 
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