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CARNOT CYCLE FOR DEC SYSTEM
 Almost all DEC system, except fuel cells and nuclear DEC
systems, follow Carnot principle in its working.
 The Carnot cycle has greater efficiency possible of an engine
based on the assumption of the absence of friction
 No conduction of heat between different parts of the engine at
different temperatures.
The Carnot Cycle
• Idealized thermodynamic cycle consisting of four reversible processes (any
substance):
 Reversible isothermal expansion (1-2, TH=constant)
 Reversible adiabatic expansion (2-3, Q=0, THTL)
 Reversible isothermal compression (3-4, TL=constant)
 Reversible adiabatic compression (4-1, Q=0, TLTH)
1-2 2-3 3-4 4-1
The Carnot Cycle
Work done by gas = PdV, area under the
process curve 1-2-3.
1
2
3
3
2
1
Work done on gas = PdV, area under the
process curve 3-4-1
subtract
Net work
1
2
3
4
dV>0 from 1-2-3
PdV>0
Since dV<0
PdV<0
The Carnot Principles
• The efficiency of an irreversible heat engine is always less than the efficiency of a
reversible one operating between the same two reservoirs. hth, irrev < hth, rev
• The efficiencies of all reversible heat engines operating between the same two
reservoirs are the same. (hth, rev)A= (hth, rev)B
• Both Can be demonstrated using the second law (K-P statement and C-statement).
Therefore, the Carnot heat engine defines the maximum efficiency any practical heat
engine can reach up to.
• Thermal efficiency hth=Wnet/QH=1-(QL/QH)=f(TL,TH) and it can be shown that hth=1-
(QL/QH)=1-(TL/TH). This is called the Carnot efficiency.
• For a typical steam power plant operating between TH=800 K (boiler) and TL=300
K(cooling tower), the maximum achievable efficiency is 62.5%.
THERMO ELECTRIC POWER GENERATION
THERMO IONIC POWER GENERATION
THERMO IONOC POWER GENERATION
• Thermionic power converter, also called thermionic generator, thermionic
power generator, or thermoelectric engine, any of a class of devices that
convert heat directly into electricity using thermionic emission rather than
first changing it to some other form of energy.
• Thermionic power converter has two electrodes.
• One of these is raised to a sufficiently high temperature to become a
thermionic electron emitter, or “hot plate.”
• The other electrode, called a collector because it receives the emitted
electrons, is operated at a significantly lower temperature.
• The space between the electrodes is sometimes a vacuum but is normally
filled with a vapour or gas at low pressure.
PRINCIPLES OF THERMO IONIC
GENERATION
 Thermionic power converter can be viewed as an
electronic diode that converts heat to electrical energy via
thermionic emission.
 It can also be regarded in terms of thermodynamics as a heat
engine that utilizes an electron-rich gas as its working fluid
PHOTOVOLTAIC SYSTEM
PHOTOVOLTAIC SYSTEM

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direct_energy_conversion.pptx

  • 1.
  • 2.
  • 3.
  • 4.
  • 5.
  • 6. CARNOT CYCLE FOR DEC SYSTEM  Almost all DEC system, except fuel cells and nuclear DEC systems, follow Carnot principle in its working.  The Carnot cycle has greater efficiency possible of an engine based on the assumption of the absence of friction  No conduction of heat between different parts of the engine at different temperatures.
  • 7. The Carnot Cycle • Idealized thermodynamic cycle consisting of four reversible processes (any substance):  Reversible isothermal expansion (1-2, TH=constant)  Reversible adiabatic expansion (2-3, Q=0, THTL)  Reversible isothermal compression (3-4, TL=constant)  Reversible adiabatic compression (4-1, Q=0, TLTH) 1-2 2-3 3-4 4-1
  • 8.
  • 9. The Carnot Cycle Work done by gas = PdV, area under the process curve 1-2-3. 1 2 3 3 2 1 Work done on gas = PdV, area under the process curve 3-4-1 subtract Net work 1 2 3 4 dV>0 from 1-2-3 PdV>0 Since dV<0 PdV<0
  • 10. The Carnot Principles • The efficiency of an irreversible heat engine is always less than the efficiency of a reversible one operating between the same two reservoirs. hth, irrev < hth, rev • The efficiencies of all reversible heat engines operating between the same two reservoirs are the same. (hth, rev)A= (hth, rev)B • Both Can be demonstrated using the second law (K-P statement and C-statement). Therefore, the Carnot heat engine defines the maximum efficiency any practical heat engine can reach up to. • Thermal efficiency hth=Wnet/QH=1-(QL/QH)=f(TL,TH) and it can be shown that hth=1- (QL/QH)=1-(TL/TH). This is called the Carnot efficiency. • For a typical steam power plant operating between TH=800 K (boiler) and TL=300 K(cooling tower), the maximum achievable efficiency is 62.5%.
  • 11.
  • 12.
  • 13.
  • 14.
  • 15.
  • 16. THERMO ELECTRIC POWER GENERATION
  • 17.
  • 18.
  • 19.
  • 20.
  • 21.
  • 22.
  • 23.
  • 24.
  • 25.
  • 26.
  • 27.
  • 28.
  • 29.
  • 30.
  • 31.
  • 32.
  • 33.
  • 34.
  • 35.
  • 36.
  • 37.
  • 38. THERMO IONIC POWER GENERATION
  • 39. THERMO IONOC POWER GENERATION • Thermionic power converter, also called thermionic generator, thermionic power generator, or thermoelectric engine, any of a class of devices that convert heat directly into electricity using thermionic emission rather than first changing it to some other form of energy. • Thermionic power converter has two electrodes. • One of these is raised to a sufficiently high temperature to become a thermionic electron emitter, or “hot plate.” • The other electrode, called a collector because it receives the emitted electrons, is operated at a significantly lower temperature. • The space between the electrodes is sometimes a vacuum but is normally filled with a vapour or gas at low pressure.
  • 40. PRINCIPLES OF THERMO IONIC GENERATION  Thermionic power converter can be viewed as an electronic diode that converts heat to electrical energy via thermionic emission.  It can also be regarded in terms of thermodynamics as a heat engine that utilizes an electron-rich gas as its working fluid