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Module 4 - Power Production - Vapour and Gas Cucles

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This section covers thermodynamic cycles for power generation using both vapour and gas systems. It includes the Rankine cycle (ideal and real), with variants like superheating, reheating, and regeneration, using steam tables and diagrams to analyse efficiency. It also explores gas power cycles, focusing on the Brayton cycle for turbines (with and without regeneration), and the Otto and Diesel cycles for internal combustion engines.

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Uploaded on
July 7, 2025
Number of pages
13
Written in
2024/2025
Type
Class notes
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Peter hicks
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Module 4A - Production of power from heat-vapour power cycles
1 Thermodynamics diagrams and vapour quality
1.1 Temperature-specific entropy diagrams
CRITICAL POINT

TA
HERED VanSt
SAT
,




HDu
vau 47406
Y

ne 354
Lives OF CONST
Pressure


E


TWO-PHASe Region
"WET STEAM"


S

1.2 Pressure-specific enthalpy diagram

CRITICAL POIN




SathizeAnA
·
Pr YOU "
When




curve 270
naue ·
t TwoPhaseReaa LINE
S
OF

Temp
CONST




D

S



1.3 Vapour Quality (“Steam Quality”)

How do we determine the specific entropy or the specific enthalpy in the interior of the two-phase
fluid region? We define quality of the two-phase mixture to be -

X = Munrour /Moth

If our working fluid is water, we refer to the steam quality and otherwise it’s a vapour quality
We can also express quality as

X =
y -
9t

Yg- Ye

Here y is one of : • the specific enthalpy h
• the specific entropy S
• the specific volume V
• the specific internal energy U

, Example : From the steam tables we find -
Sy(60°) = 0 .
5725 v/(kgK)
Ta
Sy(60 % ) = 8 .
2570 vJ/gk)

Joi


2

Sg(502) Sg(oc)S
Now X =
S -

35 = 0 .
706 Or 70 6 %
.




Sy- Sg

As we know X =
h -
he =>
h =
hg + X (hy hs) -




hy-hy

FromThe Stratables hy(doc) = 167 57.

vT/g
hg (10°) = 2574 3 .



5/kg
WeFind h = 1866 7 /kg ·




2 Steam Turbines
Here we are thinking about turbines in which the working fluid expands from saturated vapour or
superheated vapour to either wet-steam (two-phase fluid) or superheated vapour.

Pi , hi ,Ti , si v@
Recall the Isentropic efficiency of a turbine -

is vin It = hi-hza
hi -
has




② VPz , ha , Ta ,


Worked example
Steam enters a well-designed turbine at 3 MPa and 400^C, and leaves at 50 kPa and 100^C. If the
power output of the turbine is 2 MW, then determine:

(a) The specific enthalpies of the inlet and outlet if the turbine is Isentropic
Goo
%
At 3MPa , TsaT
°
= 233 90 .
C so FLUID At C is superheated Steam.



From the superheated table at 3 MPa : Th


↓ (boo" 3 MPa) ,
= 3230 9 .


vJIng ① 3 MPa
s(booc 3 MPa) ,
= 6 9212
.


Jing ⑧




50 Pa

2a
2s


*
S
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