706 ENGINEERING THERMODYNAMICSdharm
\M-therm\Th13-6.pm5Heat supplied per kg of air with regenerator
= cp(T 5 – T′) + cp(T 7 – T 6 ′)
= 1.005 [(1023 – 722) + (1023 – 872)]
= 454.3 kJ/kg(i)ηthermal (without regenerator) =146 73
807
= 0.182 or 18.2%. (Ans.)(ii)ηthermal (with regenerator) =146 73
454 3. = 0.323 or 32.3%. (Ans.)
(iii)Mass of fluid circulated, m& :
Power developed, P = 146.73 × m& kW
∴ 350 = 146.73 × m&
i.e., m&=350
146.73 = 2.38 kg/si.e., Mass of fluid circulated = 2.38 kg/s. (Ans.)
Highlights
- A cycle is defined as a repeated series of operations occurring in a certain order.
- The efficiency of an engine using air as the working medium is known as an ‘Air standard efficiency’.
- Relative efficiency, ηrelative = Actual thermal efficiency
Air standard efficiency
. - Carnot cycle efficiency, ηCarnot = TT
T
12
1−.- Otto cycle efficiency, ηOtto = 1 –^11
()rγ−
.Mean effective pressure, pm(Otto) =prr r
r(^1) p
(^111)
11
[( )( )]
()()
γ
γ
− −−
−−.
- Diesel cycle efficiency, ηDiesel = 1 –^1111
γ
ρ
γ ργ
()r −−
−L
NM
MO
QP
PMean effective pressure, pm(Diesel) =
pr r
r1 111
11γγγρ ργ
γ[( ) ( )]
()()−− −
−−−
.- Dual cycle efficiency, ηDual = 1 –^11
()^111
(. )
rγ ()()βργ
− ββγρ−
−+ −L
NM
MO
QP
PMean effective pressure, pm(Dual) = pr^1 r r
111 1
11γγβρ β βργ
γ[( ) ( ) ( )]
()()−+ −− −
−−−
.- Atkinson cycle efficiency, ηAtkinson = 1 – γ.
()r
r
−
−α
γγα
where α = Compression ratio, r = Expansion ratio.