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Lecture 11 – Performance of simple cycles. The off-design problem Off-design operation for: the single shaft engine free turbine engine the jet engine Design Task 3 description. Design = rubber engines. The off design problem. Chapter 1-3 describes the (on) design problem - PowerPoint PPT Presentation
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Chalmers University of Technology
Lecture 11 – Performance of simple cycles
• The off-design problem
• Off-design operation for:– the single shaft engine– free turbine engine– the jet engine
• Design Task 3 description
Chalmers University of Technology
The off design problem• Chapter 1-3 describes
the (on) design problem– Downstream engine
components are adapted to upstream. For instance:
• Turbine pressure ratio is selected to deliver power required by compressor
• Exhaust nozzle is sized to swallow flow exiting from turbine
Every point correspondsto new engine design - newturbine/compressor blading nozzle areas etc
Design = rubberengines
Chalmers University of Technology
The off design problem• What happens when control
signals are changed such as:– Fuel flow– Nozzle exit area – Compressor variable
geometry• Conservation of mass flow,
energy and turbine/compressor rotational speed compatibility
Operating space reduced to an equilibrium runningline
Shows proximity to surge line
Chalmers University of Technology
The off design simulation - component models• Component performance
– Semi-empirical models• Models with some constants set by
measurements or design experience. Ex:
– Scaled maps• Existing performance maps are scaled to new design point.
– Data from component rig tests– Higher order models (2D or 3D simulation)
(6.1) 11
221
T
TKKPLF
Obtained fromexperiments
Chalmers University of Technology
The off design simulation - component modelsEngine system model is built by its component models• Iteration is frequently required
to determine the running line
• Some engine specific algorithms are found in chapter 8 and 9.
Chalmers University of Technology
Part load importance• Aircraft– High. Taxiing and landing.
• Power generation– Low (except for ambient conditions).
However, surge free starting and shut down as well as time to max. power is important.
• Naval– High. Poor gas turbine part load
performance has given rise to a number of combined cycles:
• CODOG, COSAG, COGAG
• Vehicular gas turbine– High.
1% fuel efficiency idle
WR21 better fuel efficiency
than simple cycle
Chalmers University of Technology
Layout types to be studied off design
• Single shaft engine:
• Free turbine engine:
• Jet engine:
Poses the same restriction
on upstream components
Chalmers University of Technology
Off-design of single-shaft engine• Select a constant speed line on compressor
characteristic. Reading of point gives:
0101
02
01
01 ,,,T
N
p
p
P
RTmc
!Calculated
01
03
pressuredelivery compressor
of percentage Fixed
03
02
02
01
01
01
ratio pressure turbine
ofFunction
03
03
T
T
P
P
P
P
P
Tm
P
Tm
• By approximating the fuel flow as equal to bleeds, compatibility of flow gives:
• Turbine pressure ratio is obtained from (neglect inlet and exhaust losses):
01
02
02
03
04
03
P
P
P
P
P
P
Chalmers University of Technology
Off-design of single-shaft engine• The turbine rotational speed
is now obtained:
itycompatibilflow from
Calculated
01
03
03
reading mapcompressor From
01 T
T
T
N
T
N
• Rotational speed and corrected mass flow gives turbine efficiency from turbine map.
• The power output is then:
1
1
1output power net
1
01
0201012
1
03
0403034
012034
a
a
g
g
p
pTT
p
pTT
TmcTmc
c
t
pam
pg
Chalmers University of Technology
Off-design of single-shaft engine• We have now determined the
power output corresponding to the selected point in the compressor map.
• Does it match the load?
Performance problemexam 2003
Chalmers University of Technology
Gas generator performance
Poses the same restriction
on upstream components
Jet engine
Free turbine engineDerive commonprocedure for bothengines - GASGENERATORmatching!
Chalmers University of Technology
Off-design of gas generator• Select a constant speed line on compressor
characteristic. Reading of point gives:
0101
02
01
01 ,,,T
N
p
p
P
RTmc
!Calculated
01
03
pressuredelivery compressor
of percentage Fixed
03
02
02
01
01
01
ratio pressure turbine
ofFunction
03
03
T
T
P
P
P
P
P
Tm
P
Tm
• By approximating the fuel flow as equal to bleeds, compatibility of flow gives:
• Turbine pressure ratio is relatedto (neglect inlet and exhaust losses):
0401
02
02
03
RCOMOPRESSO OFITYCOMPATIBILWORK
TO COUPLED!!KNOWN! NOT
04
03
P
P
P
P
P
P
P
P a
Chalmers University of Technology
Off-design of gas generator
• Guess turbine pressure ratio and proceed as usual:
012
???
034
1
01
0201012
1
03
0403034
1
1
TcTc
p
pTT
p
pTT
papgm
c
t
a
a
g
g
Verify assumption withpower balance
Chalmers University of Technology
Off-design of gas generator and load• Every point on compressor rotational speed has a matching point,
but only one of these will match the exhaust nozzle/free turbine!!!
• A simple nested iteration will do:
match_load: DOmatch_gas_generator: DO
! gas generator simulation code
END DO match_gas_generator ! load check simulation code
END DO match_load
Chalmers University of Technology
Off-design of free turbine engine - load match
• For the free turbine we obtain acorrected mass flow as input:
8.7 Eq.From
03
04
04
03
03
03
04
04
T
T
P
P
P
Tm
P
Tm
where:(8.7) 11
03
04
1
03
04
03
034
T
T
p
p
T
T g
g
t
• The free turbine pressure ratio is obtained from (power turbine exit pressure is approximately pa):
04
04
sticcharacteri turbinefrom
04
03
04
02
03
01
0204
P
Tm
P
P
P
P
P
P
P
P
P
P
a
a
Chalmers University of Technology
Off-design of jet engine• The characteristics of the turbine nozzles are the same as the
exhaust nozzle => we have already solved the problem
• Use same procedure but check with exhaust nozzle characteristic instead of turbine characteristic!
Chalmers University of Technology
Design Task 3
2 4 6 8 10 12 141
1.5
2
2.5
3
3.5
4
4.5
5
5.5
6
Whittle compressor characteristic
m /
r c
1 2 3 4 5 6 7 8 9 100
0.2
0.4
0.6
0.8
1x 10
-3 Whittle turbine characteristic
m
T0
3/ P
03
rt
Klassens, Wood, Schuman “Experimental Performance of a ….Centrifugal Compressor Designed
for a 6:1 Pressure Ratio”NASA TMX-3552 1977
2
*
*
3
03
03
1
11)(
t
t
grr
r
XAm
PT
)(3
03
03gXA
m
PT
You receive a Start Kit which contains characteristicsStart by solving warm up task
Chalmers University of Technology
Design Task 3 – two nested iterations
Gasgen.Gasgen.m
Turbojet.m
Odp.m (off-design performance)
• Start with inner loop – gas generator
• Check that you get (T3/T1)work=(T3/T1)flow
when you run with Design Task 1 data• Then solve inner loop with fminbnd and
continue with outer
Chalmers University of Technology
Design Task 3• Predict off-design T5,Thrust
and SFC
• Determine engine conditions at 500 mph and 30000 feet
2 4 6 8 10 12 141
1.5
2
2.5
3
3.5
4
4.5
5
5.5
6
Whittle compressor characteristic
m /
r c
Chalmers University of Technology
Use of fminbnd
Minimize a function of one variable on a fixed interval. Syntax:
x = fminbnd(fun,x1,x2)
x = fminbnd(fun,x1,x2,options)
x = fminbnd(fun,x1,x2,options,P1,P2,...)
Start by solving test example Fig217_test, that is make sure that you obtain fa = 0.01452 for t02=482.0 and t03=1046.0. (faair = 0.0, fastoch = 0.06760, Qnet=43200000 ) Make sure you understand the manual for fminbnd.
% Solve non-linear 1D equation by minimizationfa = fminbnd('fa_err',faair,fastoch,[],t02,t03,Qnet);
Chalmers University of Technology
function mfp4_err = Turbojet(rc,i,pa,P01,T01,eta_t,eta_m,eta_j,deltaP_b,A3,A5, … gamma_a,gamma_g,cp_a,cp_g,R)
[mcorr1,eta_c,ncorr1] = CompChar(i,rc);
%p02 = rc*P01;%p03 = p02*(1.0-deltaP_b);r_b = p03/p02;
theta = T01/288.15;delta = P01/101325.0;
m = (mcorr1*delta)/sqrt(theta);mfp1 = m*sqrt(T01)/P01;…..
Use of non-dimensional numbers
Chalmers University of Technology
Approximation for two turbines in series• For the gas generator exit we have:
03
04
1
03
04
03
034
03
04
04
03
03
03
04
04
11T
T
p
p
T
T
T
T
P
P
P
Tm
P
Tm
g
g
t
we can plot outflow and inflow
in same turbine map!
),(
]neglible is in changesby on effect Assume[
11
04
03
03
03
04
04
1
03
04
04
03
03
03
04
04
P
P
P
Tmf
P
Tm
p
p
P
P
P
Tm
P
Tm
t
t
g
g
Typically, variation in turbine efficiency will be limitedSame effect with nozzle
downstream of gas-generator turbine!!!
Chalmers University of Technology
The compressible continuity function (x-function):
tT
T
TTT
PrrPP
P
P
PP
MXAP
RTm
t
cb
0101
030103
010101
02
02
0303
303
03 ),(
t
rC
t
rMXrAr
MXrrt
A
P
RTm
c
ccb
cb
1
3
301
01
choked nozzle Turbine
),(
),(
Theory 11.1 – Simplified turbojet running line
Chalmers University of Technology
Theory 11.1 – Simplified turbojet running line
Assume that both exhaust nozzle and turbine operate choked:
If the exhaust nozzle operates choked,
the turbine will remain in the same
non-dimensional point! Assuming
a fixed efficiency => temperature
ratio will then remain constant.
Exhaustnozzle
03
04
constant
1
03
04 11T
T
p
p g
g
t
Nozzle choked andefficiency approx. const. => temperatureand pressure ratio isconstant over turbine
Chalmers University of Technology
Theory 11.1 – Simplified turbojet running line
Finally, a work balance will be introduced:
03
04
01
03
01
0204030102 11
T
T
T
T
c
c
T
TTTcTTc
t
pa
pgmpgmpa
The compressor pressure ratio is obtained from: 1above From
01
021
010102 1 1 1
a
a
a
a
T
Trr
TTT ccc
c
Combining yields:
11
t
1 1 1
1
2
12
1constant
03
04
a
a
a
a
a
a
c
pa
pgmcc
rC
tCT
Tt
c
cr
Chalmers University of Technology
Combining the two equations yield:
t
rC
P
RTm
rC
c
c
a
a
101
01
2
11
t1
11
11
321
01
01
a
a
a
a
c
c
c
c
r
Cr
r
CCr
P
RTm
We have derived an explicit expression for the running line!!!
Theory 11.1 – Simplified turbojet running line
Chalmers University of Technology
Learning goals
• Master algorithms for calculating performance for: – Single shaft engine– Jet engine – Free turbine engine
• Know how to derive an expression for the running line as well as to state the requirements for this expression to hold