Title: Lecture 11
1Lecture 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
2The 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
Design rubberengines
Every point correspondsto new engine design -
new turbine/compressor blading nozzle areas etc
3The 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
Shows proximity to surge line
Operating space reduced to an equilibrium
runningline
4The 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)
Obtained from experiments
5The off design simulation - component models
- Engine 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.
6Part 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.
WR21 better fuel efficiency than simple cycle
1 fuel efficiency idle
7Layout types to be studied off design
- Single shaft engine
- Free turbine engine
- Jet engine
Poses the same restriction on upstream
components
8Off-design of single-shaft engine
- Select a constant speed line on compressor
characteristic. Reading of point gives
- By approximating the fuel flow as equal to
bleeds, compatibility of flow gives
- Turbine pressure ratio is obtained from (neglect
inlet and exhaust losses)
9Off-design of single-shaft engine
- The turbine rotational speed is now obtained
- Rotational speed and corrected mass flow gives
turbine efficiency from turbine map. - The power output is then
10Off-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
11Gas generator performance
Free turbine engine
Derive common procedure for bothengines -
GAS GENERATORmatching!
Poses the same restriction on upstream
components
Jet engine
12Off-design of gas generator
- Select a constant speed line on compressor
characteristic. Reading of point gives
- By approximating the fuel flow as equal to
bleeds, compatibility of flow gives
- Turbine pressure ratio is relatedto (neglect
inlet and exhaust losses)
13Off-design of gas generator
- Guess turbine pressure ratio and proceed as
usual
Verify assumption with power balance
14Off-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 DO match_gas_generator DO ! gas
generator simulation code END DO
match_gas_generator !
load check simulation code END DO match_load
15Off-design of free turbine engine - load match
- For the free turbine we obtain acorrected mass
flow as input
where
Do they match ??
- The free turbine pressure ratio is obtained from
(power turbine exit pressure is approximately
pa)
16Off-design of jet engine
- The characteristics of the turbine nozzles are
the same as the exhaust nozzle gt we have already
solved the problem - Use same procedure but check with exhaust nozzle
characteristic instead of turbine characteristic!
17Design Task 3
Klassens, Wood, Schuman Experimental
Performance of a . Centrifugal Compressor
Designed for a 61 Pressure RatioNASA TMX-3552
1977
You receive a Start Kit which contains
characteristics Start by solving warm up task
18Design Task 3 two nested iterations
Gasgen.
Odp.m (off-design performance)
Turbojet.m
Gasgen.m
- Start with inner loop gas generator
- Check that you get (T3/T1)work(T3/T1)flowwhen
you run with Design Task 1 data - Then solve inner loop with fminbnd and continue
with outer
19Design Task 3
- Predict off-design T5,Thrust and SFC
- Determine engine conditions at 500 mph and 30000
feet
20Use 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
t02482.0 and t031046.0. (faair 0.0, fastoch
0.06760, Qnet43200000 ) Make sure you
understand the manual for fminbnd.
Solve non-linear 1D equation by minimization fa
fminbnd('fa_err',faair,fastoch,,t02,t03,Qnet)
21Use of non-dimensional numbers
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 rcP01 p03
p02(1.0-deltaP_b) r_b p03/p02 theta
T01/288.15 delta P01/101325.0 m
(mcorr1delta)/sqrt(theta) mfp1
msqrt(T01)/P01 ..
22Approximation for two turbines in series
- For the gas generator exit we have
Typically, variation in turbine efficiency
will be limited
we can plot outflow and inflow in same turbine
map!
Same effect with nozzle downstream of
gas-generator turbine!!!
23Theory 11.1 Simplified turbojet running line
The compressible continuity function (x-function)
24Theory 11.1 Simplified turbojet running line
Assume that both exhaust nozzle and turbine
operate choked
Exhaustnozzle
Nozzle choked andefficiency approx. const. gt
temperature and pressure ratio is constant over
turbine
If the exhaust nozzle operates choked, the
turbine will remain in the same non-dimensional
point! Assuming a fixed efficiency gt
temperature ratio will then remain constant.
25Theory 11.1 Simplified turbojet running line
Finally, a work balance will be introduced
The compressor pressure ratio is obtained from
Combining yields
26Theory 11.1 Simplified turbojet running line
Combining the two equations yield
We have derived an explicit expression for the
running line!!!
27Learning 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