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The 
measured 
temperature 
profile 
provided 
to 
you 
is 
not 
the 
actual 
temperature 
profile 
of 
the 
gas. 
There 
is 
heat 
transfer 
from 
the 
viscous 
dissipation 
of 
gas 
onto 
the 
thermocouple 
bead, 
leading 
to 
a 
higher 
temperature 
reading 
than 
the 
actual 
static 
temperature. 
Normally 
this 
is 
not 
an 
issue, 
however, 
because 
we 
are 
measuring 
high 
speed 
flow, 
the 
viscous 
dissipation 
is 
not 
negligible. 
There 
are 
three 
equations 
that 
can 
be 
used 
to 
describe 
this 
phenomenon: 
푇! = 푇! + 
푉! 
2푐! 
푇! = 푇! + 푟 
푉! 
2푐! 
푇! 
푇! 
= 
푃! 
푃! 
!!! 
! 
The 
first 
equation 
is 
the 
relationship 
between 
the 
total 
and 
static 
temperature. 
The 
total 
temperature 
is 
the 
temperature 
of 
the 
gas 
if 
it 
were 
to 
be 
isentropically 
brought 
to 
rest, 
in 
other 
words, 
the 
kinetic 
energy 
would 
be 
completely 
converted 
into 
thermal 
energy. 
The 
second 
equation 
describes 
how 
the 
static 
temperature 
relates 
to 
the 
temperature 
that 
was 
measured 
with 
the 
thermocouple. 
The 
variable 
“r” 
is 
called 
the 
recovery 
factor, 
and 
for 
this 
experiment 
you 
can 
set 
the 
value 
of 
this 
term 
to 
0.7. 
The 
last 
equation 
describes 
the 
ratio 
of 
total 
and 
stagnation 
temperatures 
and 
pressures, 
where 
k 
is 
the 
ratio 
of 
specific 
heats. 
The 
equation 
below 
was 
found 
by 
eliminating 
the 
total 
temperature 
and 
the 
velocity 
from 
the 
three 
equations 
above. 
The 
static 
temperature 
can 
then 
be 
solved 
for 
and 
used 
to 
calculate 
the 
velocity 
and 
temperature. 
The 
profile 
data 
provided 
on 
moodle 
gives 
the 
difference 
between 
the 
total 
and 
static 
pressures, 
and 
you 
should 
have 
the 
value 
of 
the 
ambient 
pressure 
reading 
from 
the 
day 
of 
the 
experiment. 
푇! = 푇! 푟 
푃! 
푃! 
!!! 
! 
− 1 + 1 
The 
equations 
below 
could 
be 
useful 
in 
calculating 
the 
required 
results 
for 
your 
presentation. 
The 
analysis 
of 
the 
turbine 
and 
compressor 
are 
straight 
forward, 
however 
the 
analysis 
of 
the 
combustor 
and 
nozzle 
are 
a 
little 
more 
involved. 
The 
combustor 
is 
not 
a 
perfect 
combustor, 
and 
will 
have 
an 
efficiency 
of 
less 
than 
one. 
푄!"#$ = 휂!"#$푚!퐿퐻푉 
푄!"#$ = 푚!"#ℎ!"# − 푚!"ℎ!" 
To 
analyze 
the 
nozzle 
and 
evaluate 
the 
total 
mass 
flow 
rate 
through 
the 
engine, 
the 
temperature 
and 
velocity 
profile 
at 
the 
exit 
of 
the 
nozzle 
need 
to 
be 
evaluated.
휂!! = 
푚!"! 
푉! 
2 
푚!퐿퐻푉 
Thermal 
efficiency 
푚 = 휌푉푑퐴 = 휌푉푟푑푟푑휃 
Mass 
flow 
rate 
푡ℎ푟푢푠푡 = 푚푉 = 휌푉!푑퐴 = 휌푉!푟푑푟푑휃 
Thrust 
of 
the 
engine 
푚 
푉! 
2 
= 휌 
푉! 
2 
푑퐴 = 휌 
푉! 
2 
푟푑푟푑휃 
The 
kinetic 
energy 
flux 
As 
you 
go 
through 
the 
analysis, 
ask 
yourself 
if 
your 
data 
makes 
sense. 
What 
values 
are 
you 
expecting, 
and 
what 
are 
some 
ways 
to 
estimate 
the 
values 
to 
check 
your 
calculations? 
This 
will 
help 
you 
spot 
any 
gross 
errors.

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Gas turbine analysis

  • 1. The measured temperature profile provided to you is not the actual temperature profile of the gas. There is heat transfer from the viscous dissipation of gas onto the thermocouple bead, leading to a higher temperature reading than the actual static temperature. Normally this is not an issue, however, because we are measuring high speed flow, the viscous dissipation is not negligible. There are three equations that can be used to describe this phenomenon: 푇! = 푇! + 푉! 2푐! 푇! = 푇! + 푟 푉! 2푐! 푇! 푇! = 푃! 푃! !!! ! The first equation is the relationship between the total and static temperature. The total temperature is the temperature of the gas if it were to be isentropically brought to rest, in other words, the kinetic energy would be completely converted into thermal energy. The second equation describes how the static temperature relates to the temperature that was measured with the thermocouple. The variable “r” is called the recovery factor, and for this experiment you can set the value of this term to 0.7. The last equation describes the ratio of total and stagnation temperatures and pressures, where k is the ratio of specific heats. The equation below was found by eliminating the total temperature and the velocity from the three equations above. The static temperature can then be solved for and used to calculate the velocity and temperature. The profile data provided on moodle gives the difference between the total and static pressures, and you should have the value of the ambient pressure reading from the day of the experiment. 푇! = 푇! 푟 푃! 푃! !!! ! − 1 + 1 The equations below could be useful in calculating the required results for your presentation. The analysis of the turbine and compressor are straight forward, however the analysis of the combustor and nozzle are a little more involved. The combustor is not a perfect combustor, and will have an efficiency of less than one. 푄!"#$ = 휂!"#$푚!퐿퐻푉 푄!"#$ = 푚!"#ℎ!"# − 푚!"ℎ!" To analyze the nozzle and evaluate the total mass flow rate through the engine, the temperature and velocity profile at the exit of the nozzle need to be evaluated.
  • 2. 휂!! = 푚!"! 푉! 2 푚!퐿퐻푉 Thermal efficiency 푚 = 휌푉푑퐴 = 휌푉푟푑푟푑휃 Mass flow rate 푡ℎ푟푢푠푡 = 푚푉 = 휌푉!푑퐴 = 휌푉!푟푑푟푑휃 Thrust of the engine 푚 푉! 2 = 휌 푉! 2 푑퐴 = 휌 푉! 2 푟푑푟푑휃 The kinetic energy flux As you go through the analysis, ask yourself if your data makes sense. What values are you expecting, and what are some ways to estimate the values to check your calculations? This will help you spot any gross errors.