Average velocity of gas molecules in a container

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SUMMARY

The average vertical component of the velocity of gas molecules in a container can be derived using the principles of momentum and pressure. The force exerted by the gas on the walls of the container is calculated using the equation F = ma, where F is the force, m is the mass of the gas molecules, and a is the acceleration. The pressure P is defined as P = F/A, where A is the area of the wall. The discussion highlights the importance of understanding the time Δt as the time between collisions rather than the contact time with the wall, emphasizing that pressure is an average quantity over time.

PREREQUISITES
  • Understanding of ideal gas laws
  • Familiarity with Newton's second law (F = ma)
  • Knowledge of pressure calculations (P = F/A)
  • Concept of momentum and its relation to collisions
NEXT STEPS
  • Study the derivation of the ideal gas law and its applications
  • Learn about elastic collisions and their impact on momentum
  • Explore the concept of pressure as an average force over time
  • Investigate the kinetic theory of gases and its implications for molecular behavior
USEFUL FOR

Students studying physics, particularly those focusing on thermodynamics and gas laws, as well as educators seeking to clarify concepts related to gas behavior and pressure calculations.

steven george
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Homework Statement


An ideal gas with molecules of mass m is contained in a cube with sides of area A. The pressure exerted by the gas on the top of the cube is P, and N molecules hit the top of the cube in a time
Δt. What is the average vertical component of the velocity of the gas molecules.

Homework Equations


F = ma P = f/A

The Attempt at a Solution



F = ma
F = mΔV /Δt
F = 2mV / Δt (ΔV = 2V since collisions are elastic)

Putting this into P = F/A leads to the correct answer but my problem is with the Δt. When used in the acceleration Δt should be the time that the molecules is in contact with the wall of the container and it seems to me to be unrelated to the Δt as specified in the question.

Thanks to anybody that can help clear this up.
 
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steven george said:

Homework Statement


An ideal gas with molecules of mass m is contained in a cube with sides of area A. The pressure exerted by the gas on the top of the cube is P, and N molecules hit the top of the cube in a time
Δt. What is the average vertical component of the velocity of the gas molecules.

Homework Equations


F = ma P = f/A

The Attempt at a Solution



F = ma
F = mΔV /Δt
F = 2mV / Δt (ΔV = 2V since collisions are elastic)

Putting this into P = F/A leads to the correct answer but my problem is with the Δt. When used in the acceleration Δt should be the time that the molecules is in contact with the wall of the container and it seems to me to be unrelated to the Δt as specified in the question.

Thanks to anybody that can help clear this up.
The wall exerts bigger force on the molecule while in contact with it, but the pressure it exerts on the gas is also average quantity: the time average of the force exerted by unit area. It exerts some force f to one molecule during the collision , and zero between the collisions.
 
ehild said:
The wall exerts bigger force on the molecule while in contact with it, but the pressure it exerts on the gas is also average quantity: the time average of the force exerted by unit area. It exerts some force f to one molecule during the collision , and zero between the collisions.
Thanks, Maybe I'm missing something that will seem obvious once it makes sense, but when considering the acceleration shouldn't we just consider the time that the molecule is actually in contact with the wall? It really doesn't seem right to me to use the same Δt.
 
Instead of thinking in terms of acceleration, think of the force in terms of momentum delivered per unit of time. It's the momentum per collision divided by the time between collisions.
 

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