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Mechanical Engineering
  Thermodynamics
         2nd year Petrol dept.
               2011-2012


      Lecture (7) Gas Power Cycles


                     Lecturer : Dr. Esmail Bialy
Background

 1- Ideal Gas Relation

 2- 1st Law of Thermodynamics (Closed Systems)
Ideal Gas Relation
Forms
 1-                PV=mRT

Pressure   Volume     mass   Gas Const.   Temperature
(kPa)        (m3)     (kg)   (kJ/kg.K)       (K)
Forms
 2-               Pv=RT

Pressure   Specific Volume   Gas Const.   Temperature
(kPa)        (m3/kg)          (kJ/kg.K)       (K)
Forms
 3-                PV=nRuT

Pressure   Volume      no. of Universal   Temperature
                      kmoles Gas Const.
(kPa)       (m3)     (kmole) (kJ/kmole.K)     (K)
Specific Heats
Specific Heats
Specific Heats



     γ       γ
Specific Heats
 From the last two relations, we can drive another two
 relations

 Cp=γR/(γ-1)                  For Air= 1.0035 kJ/kg.K
 Cv=R/(γ-1)                   For Air= 0.716 kJ/kg.K
Note:
1-For Ideal Gases
 Δ h= CpΔT

 Δu = Cv ΔT

2- For Steam
 Δ h= h2-h1

 Δu = u2-u1   from steam tables
1st   Law of Thermodynamics
        (Closed Systems)
            (Revision)
Cairo 2nd Petrol Lecture 7
Cairo 2nd Petrol Lecture 7
Cairo 2nd Petrol Lecture 7
Cairo 2nd Petrol Lecture 7
Cairo 2nd Petrol Lecture 7
Cairo 2nd Petrol Lecture 7
Cairo 2nd Petrol Lecture 7
Cairo 2nd Petrol Lecture 7
Note!!!
rp, r, rc
rp: Pressure ratio (Brayton Cycle)
r: Compression ratio (Otto & Diesel Cycles)
rc: Cutoff ratio ( Diesel Cycle)
Example (5-10):
   A Diesel engine has a compression ratio of 20:1 with an inlet
state of 95 kPa, 290 K, and volume 0.5 L. The maximum cycle
temperature is 1800 K. find the maximum pressure, the net
specific work, and the thermal efficiency.

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Cairo 2nd Petrol Lecture 7

  • 1. Mechanical Engineering Thermodynamics 2nd year Petrol dept. 2011-2012 Lecture (7) Gas Power Cycles Lecturer : Dr. Esmail Bialy
  • 2. Background  1- Ideal Gas Relation  2- 1st Law of Thermodynamics (Closed Systems)
  • 4. Forms  1- PV=mRT Pressure Volume mass Gas Const. Temperature (kPa) (m3) (kg) (kJ/kg.K) (K)
  • 5. Forms  2- Pv=RT Pressure Specific Volume Gas Const. Temperature (kPa) (m3/kg) (kJ/kg.K) (K)
  • 6. Forms  3- PV=nRuT Pressure Volume no. of Universal Temperature kmoles Gas Const. (kPa) (m3) (kmole) (kJ/kmole.K) (K)
  • 10. Specific Heats  From the last two relations, we can drive another two relations  Cp=γR/(γ-1) For Air= 1.0035 kJ/kg.K  Cv=R/(γ-1) For Air= 0.716 kJ/kg.K
  • 11. Note: 1-For Ideal Gases  Δ h= CpΔT  Δu = Cv ΔT 2- For Steam  Δ h= h2-h1  Δu = u2-u1 from steam tables
  • 12. 1st Law of Thermodynamics (Closed Systems) (Revision)
  • 21. Note!!! rp, r, rc rp: Pressure ratio (Brayton Cycle) r: Compression ratio (Otto & Diesel Cycles) rc: Cutoff ratio ( Diesel Cycle)
  • 22. Example (5-10): A Diesel engine has a compression ratio of 20:1 with an inlet state of 95 kPa, 290 K, and volume 0.5 L. The maximum cycle temperature is 1800 K. find the maximum pressure, the net specific work, and the thermal efficiency.