Thermodynamics - Enthelpy change in adiabatic expansion

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SUMMARY

The discussion focuses on calculating the enthalpy change during the adiabatic expansion of an ideal gas in a steady flow process. The initial pressure is specified as 2.5 bar, with a volume expansion from 1.2 m³ to 3.8 m³ and a heat capacity ratio (γ) of 1.42. The participant correctly identifies the need to use the equations ΔH = ΔU + Δ(PV) and W = ∫ PdV, while also considering the implications of the process being reversible. The importance of the process type, whether through a porous plug or a turbine, is emphasized as it affects the outcome.

PREREQUISITES
  • Understanding of ideal gas laws, specifically PV = nRT
  • Familiarity with thermodynamic equations, including ΔH = ΔU + Δ(PV)
  • Knowledge of work done in steady flow processes, W = ∫ PdV
  • Concept of heat capacity ratio (γ) and its significance in thermodynamics
NEXT STEPS
  • Study the implications of reversible vs. irreversible processes in thermodynamics
  • Learn about the calculation of work done in adiabatic processes using PVγ = constant
  • Explore the differences in enthalpy change calculations for various flow types, such as through porous plugs and turbines
  • Investigate the relationship between internal energy and enthalpy in ideal gases
USEFUL FOR

This discussion is beneficial for students and professionals in thermodynamics, particularly those studying or working with ideal gas behavior, steady flow processes, and enthalpy calculations in engineering applications.

ScottHendo
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Homework Statement


Adiabatic expansion of an ideal gas is carried out in a steady flow process. The initial pressure of the gas is 2.5 bar. The volume is expanded from 1.2m3 to 3.8m3. Heat capacity ratio (γ) = 1.42. Calculate enthalpy change of the process.

Homework Equations


PV = nRT

W = ∫ PdV

ΔH = ΔU + Δ(PV)

PVγ = constant

The Attempt at a Solution


Calculate work done by using work done for steady flow process equation:
W = ∫ PdV with PVγ= constant to get W = constant ∫ (dV)/Vγ .
Carry out the integration to get W.
-W = ΔU
Then use ΔH = ΔU + Δ(PV) to find enthalpy change.

I am looking for any help on 1) to make sure I am on the right track and 2) what to do with the Δ(PV) part of the last equation.

Thanks in advance!
 
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I suppose the expansion is a reversible process. In a steady flow process ##W = \Delta H = c_p*(T_2-T_1)##. Working with internal energy seems to be correct but it much more complicated.
 
Is this the exact problem statement, or is there something that you left out? The answer is different if the flow is through a porous plug compared to a turbine featuring an adiabatic reversible expansion. Did you leave out the word “reversible” from your description?
 
I missed out that it is a slow steady flow process, would this mean that I could assume it is reversible?
 

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