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Thermodynamics CPP - 19

Nov 20, 2024

Lecture Notes: Thermodynamics Class

Announcements:

  • Midterm Exam:
    • Scheduled for Monday.
    • Allowed to use a 3x5 inch note card for equations only.
    • Covers sections 4.3 through 7.1.
    • More information and questions session on Friday.
  • Homework:
    • Due today.
    • Solutions posted outside the professor's office.
    • Homework will be part of the midterm material.

Example Problem Overview

  • Problem Focus: Rate of entropy generation.
  • Approach:
    • First law problem with second law considerations.
    • Solve for heat transfer rate first.
    • Entropy change calculated using inlet and exit states.
    • Mass flow rate and energy assumptions are essential.
  • Calculations and Data:
    • Use tables for superheated vapor data.
    • Key values: Enthalpy and entropy for initial and final states.

Solving Thermodynamic Problems

  • First Law Equation: Heat transfer minus work equals change in enthalpy.
  • Assumptions: No changes in potential or kinetic energy.
  • Sign Conventions: Important to maintain accuracy in equations.

Adiabatic and Isentropic Processes

  • Adiabatic Process:
    • No heat transfer.
    • Entropy change of surroundings is zero.
  • Internally Reversible Process:
    • Adiabatic reversible process is isentropic.
    • Indicated by constant entropy (S2 = S1).

Example Problems

  1. Piston-Cylinder Device:
    • Isentropic process (internally reversible and adiabatic).
    • Use specific volume to find mass.
    • Calculate work using first law.
  2. Compressor Problem:
    • Isentropic process using R134A.
    • Find exit temperature and enthalpy change.
    • Add-on: Calculate power required using volumetric flow rate.

Thermodynamic Diagrams

  • TS Diagram:
    • Illustrates isentropic processes (vertical lines).
  • HS (Mollier) Diagram:
    • Useful for superheated vapors and high-quality mixtures.
    • Previously used extensively in industry.

TDS Relationships

  • Essential for analysis of solids, liquids, and ideal gases.
  • Two key equations:
    1. Tds = du + pdv
    2. Tds = dh - vdp

Solids and Liquids Entropy Change

  • Assumption: Incompressible with negligible specific volume change.
  • Equation: ds = cdT/T
  • Integration for Constant C: S2 - S1 = C ln(T2/T1)

Conclusion

  • Midterm Preparation: Use the weekend to prepare and bring questions to Friday's class.
  • Next Steps: Further exploration of solids, liquids, and gases using specific heat data. Solve more example problems to reinforce understanding.