Saturated vapour pressure - why an equilibrum is reached?

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Discussion Overview

The discussion centers on the concept of saturated vapor pressure and the reasons behind the establishment of equilibrium between the number of particles leaving and joining the surface of a liquid. Participants explore the randomness of particle behavior, the role of kinetic energy, and the conditions under which equilibrium is reached.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question why the number of particles leaving and joining the surface cannot change over time, suggesting that randomness plays a role in these processes.
  • Others propose that the act of leaving the surface is determined by the kinetic energy of particles and their proximity to the surface, which they view as random.
  • A participant introduces the concept of fluctuation theory to explain the significance of random exchanges in discrete particle systems.
  • There is a discussion about whether the number of particles leaving and joining increases over time until equilibrium is reached, with some participants asserting that it does not increase indefinitely.
  • One participant states that the number of particles in the vapor phase is limited by the volume available and the vapor pressure of the liquid, suggesting that equilibrium is reached when the rates of leaving and joining particles are equal.
  • Another participant provides a mathematical perspective, indicating that the rates of particles leaving and joining depend on the area of the surface, temperature, and vapor density, leading to a constant vapor density at equilibrium.

Areas of Agreement / Disagreement

Participants express differing views on the role of randomness and the conditions under which equilibrium is achieved. There is no consensus on the specifics of how the number of particles behaves over time or the factors that influence equilibrium.

Contextual Notes

Participants highlight the dependence of the equilibrium state on temperature and surface area, but the discussion remains unresolved regarding the exact mechanisms and conditions leading to equilibrium.

Greg777
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Hello,
I've read about the concept of saturated vapour pressure on some sites but none of them really explain why the equilibrum happens and that's what I want to ask you. Why the number of particles leaving the surface and joining the surface can't change over time and never reach the equilibrum?
 
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Greg777 said:
Why the number of particles leaving the surface and joining the surface can't change over time
How do you think it might change?
 
For example the act of leaving the surface by the particle is determined by whether it has sufficient "excess" of kinetic energy. But whether the particle will leave the surface depends if it's close to the surface and I think that's completely random. And also rejoining the surface seems random to me. I don't see why an equilibrum should be reached.
 
The difference between "Avogadro's Number" and "Avogadro's Number + 1?" You might want to look at "fluctuation theory/phenomena" to get a sense for the scales of systems for which "random" exchanges/motions of discrete particles/molecules are at all significant.
 
Ok, so now I know that randomness doesn't really matter but I'm still confused about the equilibrum - I know that the same amount of particles leave and rejoin the surface but does this number of leaving/joining particles increase over time? So e.g. X particles leave and X particles return and after a while 2X particle leave and 2X particles return, then 3X leave and 3X return and so on?
 
No.
 
So the number of particles leaving and joining the surface increases up to the equilibrum and then stays constant?
 
Or, decreases, depending upon the direction from which the equilibrium is approached. Other thing to examine is the definition of pressure, particularly in respect to vapor pressure; pressure can be considered in terms of d(mv)/dt per unit area. If you increase or decrease the collision rates of molecules, you are changing their partial pressures.
 
Under what circumstances the number may decrease?
I understood that randomness don't matter but the most important concept I don't get is why the number of leaving/joining particles may increase but then stay constant? Why (even if in isolated container) all the particles won't turn into gas after some time? In other words, why a fixed number of gaseous particles is reached and it stops changing after that?
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  • #10
Greg777 said:
may decrease
Supersaturated vapor condenses until it reaches equilibrium.
Greg777 said:
increase but then stay constant
Liquid evaporates until it saturates a vapor volume.
Greg777 said:
all the particles won't turn into gas
Amount of vaporization is limited by the volume available to vapor at the vapor pressure of the liquid. The number of molecules in the vapor phase does not keep increasing. The vapor pressure is the upper limit of pressure the liquid can contribute to the pressure in the available volume.
 
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  • #11
Greg777 said:
And also rejoining the surface seems random to me. I don't see why an equilibrum should be reached.
What factors determine how many particles will rejoin the surface?

I think you are focusing too much on the "leaving".
 
  • #12
Lets say you have one molecule of water leaving the surface of some water into a vacuum. This one particle of water bounces around the vacuum container for 5 seconds before it hits the surface of the water again and rejoins the body of water. Let's say only one molecule of water has the energy to escape from the surface of the water every five seconds. You then, on average, have reached an equilibrium of one particle in the vacuum above the water at any time.
 
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  • #13
Greg777 said:
I understood that randomness don't matter but the most important concept I don't get is why the number of leaving/joining particles may increase but then stay constant?
At equilibrium, the number dN1/dt of particles leaving the liquid phase for unit time is equal to the number dN2/dt of those joining the liquid phase (or you won't have equilibrium) but this number is proportional to the area A of the separation surface and also depends on the temperature T and on the vapour density rho:

dN1/dt = A*f(T)
dN2/dt = A*g(T)*rho

At the equilibrium: dN1/dt = dN2/dt so :

f(T) = g(T)*rho --> rho = f(T)/g(T) = h(T)

so at constant temperature T the vapour density rho (and so even its pressure) is constant. Conclusion: the number dN1/dt or dN2/dt doesn't vary *if the temperature is constant and the area A doesn't vary.

Don't know if this answers your question.

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