Enthalpy - published values

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SUMMARY

The discussion centers on the interpretation of enthalpy values, specifically whether they include the work done against constant pressure, such as atmospheric pressure. Enthalpy, denoted as ##H##, is defined as ##H \equiv U + PV##, where ##U## is internal energy and ##PV## is the work done by the environment. The conversation highlights that while enthalpy is a useful parameter in thermodynamics, it is primarily a property of materials in thermodynamic equilibrium rather than a feature of specific processes. The difference in enthalpy between liquid water (H2O l) and water vapor (H2O g) is attributed mainly to differences in internal energy, with minimal contribution from PV work.

PREREQUISITES
  • Understanding of thermodynamic concepts such as internal energy (U) and pressure-volume work (PV).
  • Familiarity with the principles of statistical mechanics as they apply to thermodynamic systems.
  • Knowledge of the definitions and properties of enthalpy and entropy.
  • Basic comprehension of phase changes, particularly between liquids and gases.
NEXT STEPS
  • Study the derivation and applications of the enthalpy equation ##H = U + PV## in thermodynamics.
  • Explore the differences in thermodynamic properties between various phases of matter, focusing on water.
  • Learn about the implications of constant pressure processes in chemical reactions and their energy profiles.
  • Investigate the role of enthalpy in real-world applications, such as in chemical engineering and material science.
USEFUL FOR

Students and professionals in chemistry, physics, and engineering, particularly those involved in thermodynamics, statistical mechanics, and material science, will benefit from this discussion.

Joseph M. Zias
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Do the published values of Enthalpy include the work done against a constant pressure, e.g., the atmosphere? (I am not a chemist). I am reviewing enthalpy and entropy as part of the statistical mechanics applied to transistors. I assume, from my reading, that the work done would mostly apply to reactions involving gasses.
 
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One finds a useful definition for enthalpy ##H## in the book “Introduction to Thermal Physics” by Daniel V. Schroeder:

Enthalpy

Constant-pressure processes occur quite often, both in the natural world and in the laboratory. Keeping track of the compression-expansion work done during these processes gets to be a pain after a while, but there is a convenient trick that makes it a bit easier. Instead of always talking about the energy content of a system, we can agree to always add in the work needed to make room for it (under a constant pressure, usually 1 atm). This work is ##PV##, the pressure of the environment times the total volume of the system (that is, the total space you would need to clear out to make room for it). Adding ##PV## onto the energy gives a quantity called the enthalpy, denoted ##H##:

$$H\equiv U + PV.$$

This is the total energy you would have to come up with, to create the system out of nothing and put it into the environment (see Figure 1.15). Or, put another way, if you could somehow annihilate the system, the energy you could extract is not just ##U##, but also the work ##(PV)## done by the atmosphere as it collapses to fill the vacuum left behind.
 
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I totally oppose introducing this description in an attempt to assign a physical interpretation to enthalpy. I have seen it accomplish nothing but causing confusion among generation after generation of neophytes to the subject of thermodynamics.

Enthalpy is just a convenient shorthand parameter (for U+PV) that is useful in analyzing many kinds of thermodynamics problems. It is a property of the material being processed (exclusively for thermodynamic equilibrium states), rather than a feature of any particular kind of process (such as an isobaric process, for example). We could solve all the problems we encounter in changes between thermodynamic equilibrium states without ever introducing the enthalpy parameter H=U+PV.
 
I think we can close this thread. I found the enthalpy of H2O l is different that the enthalpy of H2Og so apparently the PV work is included when a gas is involved.
 
Joseph M. Zias said:
I think we can close this thread. I found the enthalpy of H2O l is different that the enthalpy of H2Og so apparently the PV work is included when a gas is involved.
Please provide your reference. One must be very careful when interpreting enthalpy values.
 
Joseph M. Zias said:
I think we can close this thread. I found the enthalpy of H2O l is different that the enthalpy of H2Og so apparently the PV work is included when a gas is involved.
This is not a correct interpretation. The difference between H2O l enthalpy and H20 g enthalpy is primarily the result of the difference in internal energies of the liquid and vapor, with only a veery small contribution to the difference in PV.
 

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