Expanding Plasma: Equation Governing Gas Expansion

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    Expanding Plasma
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SUMMARY

The discussion focuses on the equations governing gas expansion when air is heated to plasma, emphasizing the use of the ideal gas law and adiabatic expansion principles. The relevant equations include P * V = N * R * T for the ideal gas law and P * V^γ = constant for adiabatic processes, where γ is 5/3 for monatomic gases. The analysis suggests that heating air leads to dissociation, effectively doubling the number of moles of gas, which impacts pressure and volume relationships during expansion. The Nuclear Weapon FAQ is recommended for further reading on these principles.

PREREQUISITES
  • Understanding of ideal gas law (P * V = N * R * T)
  • Familiarity with adiabatic processes and equations (P * V^γ = constant)
  • Knowledge of thermodynamic principles, particularly regarding gas behavior
  • Basic concepts of plasma physics and gas dissociation
NEXT STEPS
  • Study the Nuclear Weapon FAQ for detailed thermodynamic relationships
  • Learn about the behavior of perfect monatomic gases under extreme conditions
  • Explore the implications of adiabatic expansion in various physical scenarios
  • Investigate the effects of gas dissociation on pressure and volume in thermodynamic systems
USEFUL FOR

Physicists, engineers, and researchers interested in thermodynamics, plasma physics, and gas dynamics, particularly in contexts involving high-energy processes and explosions.

rich_mmiv
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Hi,

When air is heated to a point where it turns into a plasma, is there any equation which governs how much the gas expands in the explosion?

Thanks
 
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That's rather vague. Generally, you would not have a single equation and what you use depends on what you want to find out and the physical situation. A set of fluid equations, Maxwell's equations and thermodynamic relationships may all be needed.
 
rich_mmiv said:
Hi,

When air is heated to a point where it turns into a plasma, is there any equation which governs how much the gas expands in the explosion?

Thanks

You can treat a plasma pretty much as an ideal gas

As the nucear weapon FAQ suggests

NukeFaq

Perfect monatomic gases are of special interest to us here, not only because they are particularly simple to analyze, but because under many extreme physical regimes all matter tends to behave like a perfect monatomic gas (kinetic energy dominates other forms of energy present).

The law for adiabatic expansion and compression is given in the FAQ. Assuming the expansion is adiabiatic ignores the energy loss due to radiation. Presumably the expansion is happening quickly enough that the energy loss to radiation is small, even though the amount of radiation may be large. This assumption really needs to be checked. Assuming it's correct, we can write:

[tex]P * V^\gamma[/tex] = constant

where P is the pressure, V is the volume, and [tex]\gamma[/tex] is 5/3 for a monatomic gas

Combine this with the ideal gas law, and one should be able to find the solution to your question.

The ideal gas law is

P * V = N * R * T

P and V have been previously defined, N is the number of moles in the gas, R is the universal gas constant, and T is the temperature

There's a lot more info in the FAQ, it's worth giving a closer read if you are interested in this problem.

To discuss your particular problem in more detail, I am assuming we are heating up a some number of moles N of air originally at some temperature T to a new, much higher temperature T', dissasociating it in the process.

Assuming the air dissasociates, we will have some greater number of moles of the new gas N'. Since nitrogen is the main component of air, N2 changing to N1 will roughly double the number of moles of gas. This process will of course require a lot of energy. The small percentage of air that is triatomic, such as CO2 and water vapor will make this factor slightly larger than 2.

Originally we had P * V = N * R * T

Keeping the volume constant, the ratio of the new pressure to the old pressure (which would typically be atmospheric pressure) is

P'/P = (N'/N) * (T'/T)

where N'/N should be roughly 2 as I argued previously.

If the expansion then continues adiabatically until P'=P, the volume should increase by a factor of

[tex](\,\frac{N'}{N}\frac{T'}{T}\,)^{\frac{1}{\gamma}}[/tex]

Disclaimer - I think this analysis is correct, but I don't offer a guarantee, thermo isn't one of my strong points.
 

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