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l ст = C v· (T 1 – T 2) (5.4)

where Cv – specific heat at constant volume.

C  C  R
p
v

The compressive adiabatic expansion work of WF

l w = C v· (T 3 – T 4) (5.5)

The specific work of the compressor

l  C T  T  (5.6)
K pm 1 2
The turbine’s specific work

l  C T  T  (5.7)
T pm 3 4

The specific work of cycle

l C = l K + l T (5.8)

5.2 Characteristics of the Carnot’s cycle
Thermal efficiency
T
  1 1 (5.9)
tk
T 3
The absorbs specific heat energy by work fluid

  T 
m
q  T C ln   3  (5.10)
1k 3 pm T
 1 

The reject Specific heat from WF

 m T 
q  T C ln 1
2k 1 . pm   T  (5.11)
 3 

Specific work Carnot’s cycle
l k = q 1k + q 2k (5.12)

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