The Mysteries of Simple Equalities in Thermodynamics

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SUMMARY

The discussion centers on the application of the thermodynamic equalities ΔH = CpΔT and ΔU = CvΔT. These equations are applicable under specific conditions, particularly when analyzing systems at constant pressure and volume, respectively. The user expresses confusion regarding the use of these equalities during gas compression and expansion. Additionally, the distinction between δf and df is clarified, with δf representing finite changes and df representing infinitesimal changes in a function.

PREREQUISITES
  • Understanding of basic thermodynamic principles
  • Familiarity with heat capacities (Cp and Cv)
  • Knowledge of derivatives in calculus
  • Concept of state functions in thermodynamics
NEXT STEPS
  • Study the conditions for applying thermodynamic equalities in various processes
  • Learn about the implications of constant pressure and volume in thermodynamic systems
  • Explore the differences between finite and infinitesimal changes in calculus
  • Investigate the role of state functions in thermodynamic analysis
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Students and professionals in physics and engineering, particularly those focusing on thermodynamics and calculus applications in physical systems.

An1MuS
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This is an important concept of thermodynamics,that I'm having some trouble understanding.

My question is, when can we use these equalities?

[tex]\Delta H=C_{p}\Delta T[/tex]

and

[tex]\Delta U=C_{v}\Delta T[/tex]

For instance, I thought the first one could only be used when the pressure of the system is constant, but I've seen it being used on compression and expansion of gases.

Does anyone know?

Thanks in advance!

By the way, there's this little thing i don't know too. What's the difference between writing

[tex]\delta f=...[/tex] and [tex]df=...[/tex]

meaning both derivative of "f"
 
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An1MuS said:
This is an important concept of thermodynamics,that I'm having some trouble understanding.

My question is, when can we use these equalities?

[tex]\Delta H=C_{p}\Delta T[/tex]

and

[tex]\Delta U=C_{v}\Delta T[/tex]

For instance, I thought the first one could only be used when the pressure of the system is constant, but I've seen it being used on compression and expansion of gases.

Does anyone know?

Thanks in advance!

By the way, there's this little thing i don't know too. What's the difference between writing

[tex]\delta f=...[/tex] and [tex]df=...[/tex]

meaning both derivative of "f"
[tex]\delta f=...[/tex] is some finite change in the function. such as evaluating f(1) then f(1.1)

[tex]df=...[/tex] is an infinitesimal change in the function.

i.e. the limit as this change goes to 0.
 

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