Latent heat and unstable system

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Discussion Overview

The discussion revolves around the concept of latent heat, particularly in unstable systems, such as water at specific temperatures and pressures. Participants explore the implications of phase changes under varying conditions, questioning the definition and applicability of latent heat in these scenarios.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant defines latent heat as the variation of enthalpy between two phases and questions if it is zero in unstable conditions, suggesting that only slight changes in conditions are needed for phase change.
  • Another participant counters that latent heat cannot be disregarded and explains that latent heat content can change at constant temperature, using the example of water freezing in a freezer.
  • A subsequent participant asks if latent heat exists for liquid water at 270 K and 1 atm, indicating a need for clarification on the conditions.
  • One participant suggests considering latent heat as a process rather than a property, emphasizing the importance of system isolation and perturbations affecting the phase ratio.
  • Another participant references the Clausius-Clapeyron equation, asserting that the system is unstable and that slight changes can lead to spontaneous freezing without additional heat input.
  • A later reply acknowledges the concept of super-cooling, explaining that water can remain liquid below its freezing point until disturbed, which can trigger freezing and restore thermal equilibrium.
  • One participant illustrates the difference between stable and unstable systems using analogies, arguing that latent heat is significant in stable conditions but negligible in unstable conditions where minor perturbations can cause phase changes.

Areas of Agreement / Disagreement

Participants express differing views on the role of latent heat in unstable systems, with no consensus reached on whether latent heat can be considered zero under such conditions. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Participants highlight the need for clarity regarding definitions and conditions, such as the isolation of the system and the implications of the Clausius-Clapeyron equation. There are unresolved questions about the stability of the system and the role of perturbations in phase changes.

MiGUi
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Latent heat is the variation of entalpy between two phases (or the heat that you must provide to the system to change the phase).

But, if we are in a unstable system (such as water at 1 atm of pressure and 270 K of temperature), we need no heat to change the phase, simply we have to variate infinitesimally the conditions to make the system change.

So my question is: That reason is correct? Latent heat in unstable conditions is equal to zero?

Thanks for your replies
MiGUi
 
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MiGUi said:
That reason is correct? Latent heat in unstable conditions is equal to zero?
No. You provided the definition in your first sentence and then discarded it: heat added/subtracted to change the temperature is sensible heat and a different issue. Latent heat content can change at constant temperature.

Think about what happens to a glass of water in the freezer. First, the temperature decreases by 1 degree C for each calorie of energy removed per gram. When the water gets to 0 C, energy continues to be pulled out while it freezes. The heat of fusion for water is 80 cal/g-C, so for each 80cal taken out, 1g freezes. Once frozen, the temperature of the ice will begin to drop again.
 
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But if you have liquid water (not ice) at 270 K and 1 atm (unstable), latent heat exists?
 
Perhaps you should think of latent heat as more of a process than a property.

I'm assuming that, by "270 K" and "1 atm," you intend to specify the conditions that indicate the boundary between solid and liquid. In this case, it is crucial to determine/specify whether or not the system is isolated. If it is truly isolated (all exchanges and interactions are completely contained), then the ratio of solid to liquid H2O will persist (statistically). But, just the slightest perturbation will change this ratio. If you have 100% solid H2O, and there is an addition of heat from the environment, then this will liquify some of that H2O. Then, you have to consider what happens to the pressure to determine where the state goes.
 
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We can cool water and keep it 100% liquid at 1 atm and 270 K. But the Clausius-Clapeyron equation says that this is not an stable system.

If we change a bit the properties of the system, then water freezes spontaneously and pressure may be constant. We do not have to give aditional heat to the system to make it change.
 
Yeah, that sounds correct (except that I don't know what the Clausius-Clapeyron equation is). Hmm. I probably should not have been so hasty with my previous post. Sorry about that. I'll leave it to the experts.
 
edit: missed the key. Got it now.

You're talking about super-cooling. If you are careful not to provide a means for chrystals to form, it is possible to cool water below its freezing point (273K). But purturb it (literally, bump the vessel) and some will freeze. The temperature of the remaining water will go back up to 273K and the system will remain in thermal equilibrium.
 
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Well, I'm not talking about chrystals... only water and the possibility of cool it below its freezing point. This is an unstable system.

The point is that: The latent heat is the heat you need to make a system, change the phase. For example, at 373K and 1 atm if you give 2260 J/g of heat, you make water boil and the liquid phase dissapears.

But, if we are at 375 K and 1 atm ... we can cool very slow the system and we can have water vapour at 370 K and 1 atm. To convert that vapour into liquid water, we only have to change slightly the conditions.

The system at stable conditions (vapour at 375K, 1atm) is like a "lego castle", and we have to use a lot of energy to break it. That energy is the latent heat.

The system at unstable conditions (vapour at 370K, 1 atm) is like a "card castle" and we touch a card very slightly, the castle collapses, because is a unstable system. No energy gave, no latent heat.
 

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