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ChemE 260 Thermodynamic Temperature Scales

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ChemE 260 Thermodynamic Temperature Scales & The Carnot Efficiency Dr. William Baratuci Senior Lecturer Chemical Engineering Department University of Washington – PowerPoint PPT presentation

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Title: ChemE 260 Thermodynamic Temperature Scales


1
ChemE 260 Thermodynamic Temperature Scales The
Carnot Efficiency
  • Dr. William Baratuci
  • Senior Lecturer
  • Chemical Engineering Department
  • University of Washington
  • TCD 6 F GCB 5 10 11

May 2, 2005
2
Thermodynamic Temperature Scales
  • From Ch 5
  • 2nd Carnot Principle
  • Therefore
  • Thermodynamic Temperature Scales
  • Operate a HE between two thermal reservoirs
  • Measure QC, QH and W
  • Calculate ?
  • Arbitrarily assign a value to either TC or TH
  • If we know the functionwe can calculate the
    other, unknown T.
  • This is a Thermodynamic Temperature Scale

Baratuci ChemE 260 May 2, 2005
3
QC/QH Fxn(TH, TC)
Algebra tells us that
Baratuci ChemE 260 May 2, 2005
4
The Kelvin Relationship
  • All of the T1 terms in fA and fB must drop out
    when they are multiplied together.
  • Only true if the fxn has the form
  • Conclusion
  • Lord Kelvin
  • Result

Baratuci ChemE 260 May 2, 2005
5
The Ideal Gas Temperature Scale
  • Apply the 1st Law to Steps 1-2 and 3-4 carried
    out in a closed system to determine QH and QC.
  • Use the definition of boundary work and CV for
    ideal gases.
  • Results

Baratuci ChemE 260 May 2, 2005
6
Adiabatic Steps in a Carnot Cycle
  • Apply the 1st Law to Steps 2-3 and 4-1
  • Use the definition of boundary work and CV for
    ideal gases.
  • Results
  • Conclusion

Baratuci ChemE 260 May 2, 2005
7
Ideal Gas Kelvin Scales
  • The isothermal steps
  • The adiabatic steps
  • Combining yields
  • The Ideal Gas Kelvin Scales are identical !

Baratuci ChemE 260 May 2, 2005
8
Carnot Efficiency and COP
  • Power
  • Cycles

Refrigeration Cycles
Heat Pump Cycles
Baratuci ChemE 260 May 2, 2005
9
Performance vs. Reservoir T
  • All cycles shown here are reversible.

Baratuci ChemE 260 May 2, 2005
10
The Relative Value of Energy
  • 100 J of heat at 1000 K produces more work than
    100 J of heat at 300 K
  • Heat energy available at a higher T is more
    valuable or has a higher quality.
  • You can always completely convert work into heat
    at ANY temperature using friction.
  • We can conclude that work is a more valuable form
    of energy than heat !

Baratuci ChemE 260 May 2, 2005
11
Next Class
  • Next class
  • Chapter 7 Entropy
  • Here the 2nd Law finally boils down to an
    equation that we can use to analyze thermodynamic
    cycles.
  • The Clausius Inequality leads to the definition
    of a new propertyentropy, S.
  • CIDR Learning Styles Survey

Baratuci ChemE 260 May 2, 2005
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