Adiabatic Process (Poisson’s equations)

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SUMMARY

The discussion centers on the adiabatic process and the equation dW = PdV, clarifying that this relation does not require pressure (P) to be constant throughout the process. The analogy of a particle moving along the x-axis with varying velocity is used to illustrate that instantaneous values can be applied even when variables change. Participants reference the Wikipedia article on the "Derivation of P–V relation for adiabatic heating and cooling" for further understanding.

PREREQUISITES
  • Understanding of thermodynamics, specifically adiabatic processes.
  • Familiarity with calculus concepts such as derivatives and integrals.
  • Knowledge of the relationship between pressure, volume, and work in thermodynamic systems.
  • Basic understanding of physics principles related to motion and velocity.
NEXT STEPS
  • Study the "Derivation of P–V relation for adiabatic heating and cooling" on Wikipedia.
  • Explore the implications of the first law of thermodynamics in adiabatic processes.
  • Investigate the mathematical modeling of non-constant pressure systems in thermodynamics.
  • Learn about the applications of adiabatic processes in real-world engineering scenarios.
USEFUL FOR

Students of thermodynamics, physics enthusiasts, and engineers involved in systems where adiabatic processes are relevant will benefit from this discussion.

Taulant Sholla
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Homework Statement
I'm lacking clarity with the statements I highlighted in the passage found in my physics textbook. It is stated that P, V, and T all vary during an adiabatic process, but the next box I highlighted uses dW=PdV which assumes pressure is constant during this process. These seem to be contradictory statements. What am I missing here? Thank you.
Relevant Equations
dW=PdV
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Taulant Sholla said:
the next box I highlighted uses dW=PdV which assumes pressure is constant during this process.

The relation ##dW = PdV## does not assume that ##P## is constant during the process.

A similar example would be a particle moving along the x-axis with a varying velocity. At some instant of time, you can write the instantaneous velocity as ##v = dx/dt##. This can be "rearranged" as ##dx = vdt##. So, the displacement during an infinitesimal time interval ##dt## is ##dx = vdt##. This is valid even though ##v## is not constant during the motion.
 
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TSny said:
The relation ##dW = PdV## does not assume that ##P## is constant during the process.

A similar example would be a particle moving along the x-axis with a varying velocity. At some instant of time, you can write the instantaneous velocity as ##v = dx/dt##. This can be "rearranged" as ##dx = vdt##. So, the displacement during an infinitesimal time interval ##dt## is ##dx = vdt##. This is valid even though ##v## is not constant during the motion.

Please accept my belated thank you! This really helped!
 
Lnewqban said:
Please, look for "Derivation of PV relation for adiabatic heating and cooling" at this article:
https://en.wikipedia.org/wiki/Adiabatic_process

I did, it didn't help. Thanks anyway - I got an assist from another kind soul.
 

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