Recent content by tracker890 Source h

  1. tracker890 Source h

    The maximum reversible work in thermodynamics

    Thank you for your suggestion. I also managed to find the book successfully. After studying some of the material, I've gained inspiration and different perspectives to ponder on.
  2. tracker890 Source h

    The maximum reversible work in thermodynamics

    Perhaps my level is not as high, but the few sentences you mentioned seem simple, yet they are insights I've obtained after about a week of research and repeatedly deriving them. Additionally, I have uploaded a new example, hoping to receive your corrections.
  3. tracker890 Source h

    The maximum reversible work in thermodynamics (2)

    reference;sol The maximum reversible work in thermodynamics Below is the process of determining the "Available energy" for an open system, shared with everyone as a reference for learning about exergy. If there are any errors in the content, please feel free to correct them. $$...
  4. tracker890 Source h

    The maximum reversible work in thermodynamics

    Thank you very much. You've mentioned the most important key point. However, explaining this part in words is quite difficult. I can only say that one must first learn about "entropy generation" in order to understand exergy.
  5. tracker890 Source h

    The maximum reversible work in thermodynamics

    To avoid confusion, I'll use the precise term "available energy" from the textbook. The method you described is the approach by the author Yunus A. Çengel: assuming the process is entirely reversible to determine the available energy. Another approach is from the authors CLAUS BORGNAKKE and...
  6. tracker890 Source h

    The maximum reversible work in thermodynamics

    Why is equation (5) not zero? reference
  7. tracker890 Source h

    The maximum reversible work in thermodynamics

    I referenced the following two thermodynamics textbooks for your consideration. reference
  8. tracker890 Source h

    The maximum reversible work in thermodynamics

    Imagine a system in a quasi-static state, with a thermodynamic process occurring from state 1 to state 2.
  9. tracker890 Source h

    The maximum reversible work in thermodynamics

    1. Regarding equation (5), the calculation error has been corrected to: $$ \sum{\left( 1-\frac{\ T_0}{T_k} \right) Q_k}=Q_k^{\nearrow -2KJ}\left[ \left( 1-\frac{\ T_0^{\nearrow 298}}{T_1^{\nearrow ^{573}}} \right) +\left( 1-\frac{\ T_0^{\nearrow 298}}{T_2^{\nearrow ^{423}}} \right) \right]...
  10. tracker890 Source h

    The maximum reversible work in thermodynamics

    Q: The maximum reversible work, self-solved, is as follows: Only when equation (5) equals zero will it match the textbook solution; kindly indicate any errors in the self-solution. reference. : sol.; exergy balance; CMS.; wrev. Q: The maximum reversible work, self-solved, is as follows: Only...
  11. tracker890 Source h

    Q2: In a relative non-inertial reference frame, why is fluid velocity zero?

    The content of this book is extremely detailed, it must be a good book. Therefore, I'd like to inquire about the title of this textbook, I hope you don't mind.
  12. tracker890 Source h

    Q2: In a relative non-inertial reference frame, why is fluid velocity zero?

    I got it. Thank you very much for teaching and explaining in such detail and patience.
  13. tracker890 Source h

    Q2: In a relative non-inertial reference frame, why is fluid velocity zero?

    I understand. ##\int_{CV}^{}{\rho d\forall}## refers to all mass elements (including solid and fluid) inside the control volume, but the fluid appears negligible within the vast control volume, so it can be ignored. However, despite this, the flow remains unsteady because, in reality...
  14. tracker890 Source h

    Q2: In a relative non-inertial reference frame, why is fluid velocity zero?

    The diagram has been modified as follows. Ans I always get confused about "why ##\frac{\partial}{\partial t}\left( u_{xyz}\cdot M_{_{CV}} \right) =0## "because ##u_{xyz}=u_{xyz}\left( t \right) ##.
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