Power Plant Engineering

(Ron) #1
260 POWER PLANT ENGINEERING

Also, V 3 – V 2 = 0.05Vs = 0.05(V 1 – V 2 )

or, V 3 – V 2 = 0.05(13V 2 – V 2 ),^1
2

V
V

= 13

or, V 3 – V 2 = 0.06V 2


3
2

V
V

= 1.6

ηair standard = 1 – 1

1
()γ−



γr

()^1
(1)

ργ−
ρ−


= 1 – 1.4 1

1
1.4(14) −





(1.61.4 1)
(1.6 1)

−

−

= 0.615 = 61.5%

ηrelative = thermal
air standard

η
η

0.65 = thermal
0.615

η

ηthermal = 0.4

But, ηthermal =

I.P.
(C)mf×

0.4 =

I.P.

(^1441800)
3600



I.P. = 65 KW
ηmech =
B.P.
I.P.
0.76 =
B.P.
65
B.P. = 49.4 kW
Mean effective pressure can be calculated based on I.P. or B.P. of the engine
I.P. = mi.
(. LAN .10)
6
np k
, pmi = indicated mean effective pressure
65 =
2 0.25 (0.2)^2 300 1 10
4
6
pmi
π
×× × ×××
pmi = 8.27 bar
and brake mean effective pressure (pmb) = 0.76 × 8.27 = 6.28 bar.
V = V –VS1 2
1
4
2 3
0.05 VS
P
V
Fig. 8.18

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