1 / 18

Thermodynamic Property Relations

Thermodynamic Property Relations. Chapter 12. The Maxwell Relations. The equation that relate the partial derivatives of properties P, v , T and s of a simple compressible system to each other are called the Maxwell relations. They are obtained from the four Gibb equation, expressed as:.

lyn
Télécharger la présentation

Thermodynamic Property Relations

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Thermodynamic Property Relations Chapter 12

  2. The Maxwell Relations • The equation that relate the partial derivatives of properties P, v, T and s of a simple compressible system to each other are called the Maxwell relations. • They are obtained from the four Gibb equation, expressed as:

  3. The Maxwell Relations are

  4. The Clapeyron Equation • This equation enables us to determine the enthalpy change associated with a phase change from a knowledge of P, v and T data alone.

  5. The Clapeyron – Clausius Equation • For liquid – vapor and solid – vapor phase change processes at low pressures, it can be approximated as

  6. General Relations • Internal Energy Changes

  7. Enthalpy Changes

  8. Entropy Changes

  9. Specific Heats Cv and CP

  10. Volume Expansivity (β) & Isothermal Compressibility (α)

  11. The Joule – Thomson Coefficient • It is a measure of the change in temperature of a substance with pressure during a constant enthalpy process, and it can be expressed as

  12. The enthalpy departure can be expressed as:

  13. Similarly

  14. EXAMPLE

More Related