Enthalpy change in a flow process

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SUMMARY

The discussion centers on the justification for substituting the change in enthalpy (dH) with the product of specific heat capacity (c) and change in temperature (dT) in steady-state flow processes, specifically in pipe flow scenarios. It is established that this substitution is generally not valid unless specific heat remains constant, which may vary based on the fluid type (liquid or gas) and the nature of the calculation. The participants emphasize that for closed systems, this approximation holds true primarily under constant pressure conditions, which is not the case in pipe flow where pressure drops.

PREREQUISITES
  • Understanding of thermodynamics principles, particularly enthalpy and specific heat capacity.
  • Familiarity with steady-state flow processes in fluid mechanics.
  • Knowledge of energy balance equations in flow systems.
  • Basic concepts of pressure and temperature relationships in fluids.
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  • Research the implications of variable specific heat in fluid dynamics.
  • Study the derivation and applications of the energy balance equation for pipe flow.
  • Examine the differences in enthalpy behavior between liquids and gases under varying pressure conditions.
  • Explore advanced thermodynamic models that account for non-constant specific heat in flow processes.
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Engineers, thermodynamics students, and fluid mechanics professionals seeking to deepen their understanding of energy transfer in flow processes and the validity of thermodynamic approximations in practical applications.

ethonodon
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TL;DR
In a flow process, why do we substitute dH = c*dT if pressure is dropping during the process
I am looking at simple steady-state flow processes, say for flow through a pipe. The general energy balance for pipe flow reduces to simply heat evolved = change in enthalpy between the two states (or heat rate = mass flow rate * change in specific enthalpy). However, for a flow process, why is it justified to replace change in enthalpy with heat capacity * change in temperature. I understand that for closed systems, one can only do so for processes taking place at constant pressure (or for cases in which the enthalpy is a function only of temperature.) In the case of pipe flow, pressure obviously drops - do we simply approximate the enthalpy of the fluid to only depend on temperature? Otherwise, the dH = c*dT substitution does not seem valid to me...
 
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ethonodon said:
TL;DR Summary: In a flow process, why do we substitute dH = c*dT if pressure is dropping during the process

I am looking at simple steady-state flow processes, say for flow through a pipe. The general energy balance for pipe flow reduces to simply heat evolved = change in enthalpy between the two states (or heat rate = mass flow rate * change in specific enthalpy). However, for a flow process, why is it justified to replace change in enthalpy with heat capacity * change in temperature. I understand that for closed systems, one can only do so for processes taking place at constant pressure (or for cases in which the enthalpy is a function only of temperature.) In the case of pipe flow, pressure obviously drops - do we simply approximate the enthalpy of the fluid to only depend on temperature? Otherwise, the dH = c*dT substitution does not seem valid to me...

In general, dH = c*dT is not valid. If the specific heat c is constant enough, it may be an acceptable approximation, depending on the nature of the calculation. Or it may not be.
 
Are you talking about a liquid or a gas?
 

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