Equilibrium in a pure substance

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Discussion Overview

The discussion revolves around the concept of equilibrium in a pure substance, specifically focusing on the behavior of water under heating conditions, the interpretation of vapor pressure, and the relationship between pressure and temperature in liquid-vapor systems. Participants explore theoretical aspects, graphical representations, and definitions related to phase transitions and vapor pressure curves.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the definition of pressure in a liquid-water system, asking whether it refers to the surface, bottom, or sides.
  • Another participant explains that pressure at different points in the liquid depends on surface pressure, density, and depth.
  • Some participants suggest that pressure remains constant as water expands, with density reduction offsetting the expansion effects.
  • A participant seeks clarification on the vapor-pressure curve, expressing confusion about its representation and relationship to compressed water cases.
  • Another participant notes that vapor pressure refers to the gas phase pressure in a closed system and may not reflect the liquid's pressure.
  • There is a discussion about the implications of constant pressure while temperature rises, with questions about the positioning of points relative to the vapor-pressure curve.
  • Some participants express uncertainty about the conditions under which phase transitions occur and the energy requirements for conversion from liquid to gas.
  • A participant critiques the terminology used in the literature, suggesting it may be misleading, while another defends the terminology as accurate.
  • One participant presents a different diagram from another source, prompting a comparison with the original source's diagram.

Areas of Agreement / Disagreement

Participants express various viewpoints on the definitions and implications of pressure and vapor pressure in liquid systems. There is no consensus on the interpretation of the vapor-pressure curve or the terminology used in the literature, indicating ongoing disagreement and exploration of the topic.

Contextual Notes

Participants highlight potential confusion arising from different sources and diagrams, as well as the need for clarity in definitions related to vapor pressure and phase transitions. The discussion reflects a range of interpretations and assumptions that remain unresolved.

mech-eng
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upload_2017-4-24_11-0-24.png


The book says when the water is heated, the pressure stays constant. But I do not understand pressure for a liquid-water system. What is the pressure for a liquid here? the pressure on the surface, botton or sides?

Source: Fundamentals of Thermodynamics by Sonntag/Borgnakke/Van Wylen.

Thank you.
 
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The pressure at the top surface of the water is determined by the weights and the area. The pressure at other points depends on the surface pressure AND the density and depth at that point.
 
In this case the pressure everywhere stays constant because as the water expands the density reduces. I believe these two things cancel out.

The pressure is primarily determined by the weights and area.
 
I especially ask about vapor-pressure curve. On my copy of book, I cannot find it, I can its picture later. In that curve perpendicular axis is pressure and horizontal axis is temperature and there is parabolic curve with positive slope called vapor-pressure curve again. I cannot understand what it represents. Can it be related to pic a, at the top, only compressed water case?

Thank you.
 
This is the diagram.

upload_2017-4-24_17-30-47.jpeg


It seems strange to me because for picture a at the top, compressed liquid case, there is no vapor so there should be no vapor pressure but there is a temperature value. Then should the graph start from somewhere on temperature axis, at which vapor pressure is zero, then going horizantal to saturation temperature then making the curve. But I am confused that I cannot surely determine if the pressure should only belong to vapor?

Thank you.
 
mech-eng said:
It seems strange to me because for picture a at the top, compressed liquid case, there is no vapor so there should be no vapor pressure but there is a temperature value.
Vapor pressure refers to the pressure you would get in the gas phase in a closed system with room for the gas. But it may not be the pressure of the liquid. If you have a glass of water (between 0 and 100 °C), then the water is at 1 atm pressure, whatever the value of the vapor pressure.

The process in the OP is at constant pressure, so it corresponds to a horizontal line on the graph above. Point (a) is to the left of the vapor-pressure curve, point (b) is on the curve, and point (c) is to the right of the curve.
 
DrClaude said:
The process in the OP is at constant pressure, so it corresponds to a horizontal line on the graph above. Point (a) is to the left of the vapor-pressure curve, point (b) is on the curve, and point (c) is to the right of the curve

I.e pressure is constant while temperature is always rising? And I do not understand why point c should be to the right of the curve instead of being on it?

Thank you.
 
mech-eng said:
I.e pressure is constant while temperature is always rising? And I do not understand why point c should be to the right of the curve instead of being on it?
If the external temperature is exactly equal to the phase transition temperature, then nothing will happen when the liquid reached that temperature. To be converted into a gas, additional energy is required, which is usually achieved by having an external temperature above the phase transition temperature. As a result, when the phase transition is completed, the vapor will most often be heated.

In theory, figs. 2.1 (a)-(c) could all be exactly at the transition temperature, but in practice this is never the case.
 
DrClaude said:
If the external temperature is exactly equal to the phase transition temperature, then nothing will happen when the liquid reached that temperature. To be converted into a gas, additional energy is required, which is usually achieved by having an external temperature above the phase transition temperature. As a result, when the phase transition is completed, the vapor will most often be heated.

In theory, figs. 2.1 (a)-(c) could all be exactly at the transition temperature, but in practice this is never the case.

I understood from your last post. It is the curve denoting the saturation temperatures corresponding to saturation pressures. I thought it was about vapor pressures, saturated or superheated, corresponding to temperatures. But it is not.I think the authors names it incorrectly. It is name is confusing.

Thank you.
 
  • #10
mech-eng said:
I think the authors names it incorrectly. It is name is confusing.
I don't think there is anything named incorrectly. Look up the definitions for the different names and see if you can try and sort them out.
 
  • #11
This diagram from another source, Çengel/Boles, is quite different from the belonging to Sonntag/Borgnakke.

upload_2017-4-24_21-38-46.png


Thank you.
 
  • #12
mech-eng said:
This diagram from another source, Çengel/Boles, is quite different from the belonging to Sonntag/Borgnakke.
I don't see any significant difference (especially keeping in mind that the first one is schematic).
 

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