AE 334 EXPERIMENT : DETERMINATION OF NOZZLE ...
AE 334 EXPERIMENT : DETERMINATION OF NOZZLE ...
AE 334 EXPERIMENT : DETERMINATION OF NOZZLE ...
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Introduction:<br />
<strong>AE</strong> <strong>334</strong><br />
<strong>EXPERIMENT</strong> : <strong>DETERMINATION</strong> <strong>OF</strong> <strong>NOZZLE</strong> EFFICIENCY<br />
Nozzles are suitably shaped passages in which a fluid accelerates as its pressure decreases.<br />
Nozzles are vital components in a wide variety of engineering applications: turbines, jet<br />
propulsion, rockets, ejectors.<br />
The high velocity jet of fluid leaving a nozzle may be used in several ways:<br />
• In a turbine, the kinetic energy stored in the fluid forms the energy available to the blades or the<br />
rotor for conversion to shaft work.<br />
• In rockets and jet propulsion, the change of momentum associated with the velocity changes in<br />
the nozzle provides most of the propulsion force.<br />
• In ejectors and injectors, the changes of momentum of the jet, with its entrained fluid, is used to<br />
bring about the desired pressure changes.<br />
In the ideal nozzle, flow through a perfect nozzle would be reversible, (i.e. without heat<br />
transfer and without frictional effects, shocks, etc.) and will therefore be isentropic.<br />
Objective:<br />
The aim of this experiment is to determine the effect of back pressure on the mass flow rate with a<br />
constant inlet pressure and compare the mass flow rate with the theoretical value for a perfect gas<br />
flowing isentropically and calculate the nozzle efficiency.
Experimental setup:<br />
Theory:<br />
Due to the effects of friction, uncontrolled expansion, shocks etc., the velocity of the jet of<br />
fluid leaving a nozzle will be lower than that from an ideal nozzle.<br />
The efficiency of a nozzle as a kinetic energy producer is the ratio:<br />
Kinetic energy increase across the nozzle<br />
Kinetic energy increase in an isentropic nozzle<br />
Since the kinetic energy of the fluid before the nozzle is usually insignificant,<br />
Kinetic energy of jet leaving the nozzle<br />
Nozzle Efficiency =<br />
Isentropic enthalpy change across the nozzle
For reversible and adiabatic one-dimensional expansion through a passage, the following<br />
relationships apply at any section XX.<br />
2<br />
V<br />
ht = h + = constant<br />
2<br />
2<br />
2<br />
V1<br />
Vx<br />
h1 + = hx<br />
+<br />
2 2<br />
assuming that V = 0 then<br />
V = 2( h − h )<br />
x 1 x<br />
A<br />
x<br />
.<br />
mν<br />
x =<br />
V<br />
x<br />
1<br />
where .<br />
h = total enthalpy<br />
t<br />
h = enthalpy<br />
V = velocity<br />
m = mass flow rate<br />
A = Area<br />
ν = specific volume<br />
If it is assumed the relationship between p and ν in such an expansion is pν γ = constant.<br />
1 2s<br />
2s<br />
h − h = ν dp<br />
1<br />
γ −1<br />
γ p γ<br />
2<br />
1 − 2s = 1ν ⎢<br />
1 1−<br />
⎥<br />
γ −1 ⎢ p1<br />
⎥<br />
⎣ ⎦<br />
h h p<br />
pν = RT<br />
1 1 1<br />
∫<br />
⎡ ⎤<br />
To calculate mass flow rate per unit area m/A in a nozzle from the contunuity equation<br />
we proceed as follows:<br />
(1)<br />
(2)
.<br />
m PV γTt<br />
= ρV<br />
=<br />
A RT γT<br />
.<br />
=<br />
PV<br />
γ RT<br />
γ Tt<br />
1<br />
R T T<br />
t<br />
t<br />
PM γ γ −1 2 Pt<br />
⎡ γ −1<br />
2 ⎤<br />
= 1+ M where = 1 M<br />
T R 2 P ⎢<br />
+<br />
2 ⎥<br />
⎣ ⎦<br />
t<br />
m<br />
=<br />
A<br />
(3)<br />
Pt<br />
Tt<br />
γ M<br />
R<br />
⎡ γ −1<br />
2 ⎤<br />
⎢<br />
1+<br />
M<br />
⎣ 2 ⎥<br />
⎦<br />
γ + 1<br />
2( γ −1)<br />
For choked condition Mach number equals to one, then :<br />
At<br />
.<br />
P1<br />
theoretical = 0.404 t where P1<br />
m A T<br />
1<br />
: throat area<br />
: Inlet Pressure<br />
γ<br />
γ −1<br />
D = throat diameter = 0.00202m<br />
The theoretical value of the jet velocity leaving the nozzle can be found from Equation1<br />
and the actual jet velocity can be found from V=F/m where F is the force which will be found<br />
from F/Δ graph.<br />
(4)
Experimental Procedure:<br />
1. Close the air inlet valve and open the chamber pressure control valve.<br />
2. Check that the micrometer dial has been correctly zeroed.<br />
3. Adjust the air inlet control valve to give a constant air inlet pressure of about 500-600 kN.m -2<br />
gauge with the chamber pressure control valve fully open.<br />
4. Then rotate the micrometer adjustment screw until the voltmeter and lamb indicates<br />
that the contact is just made.<br />
5. Observe the pressures, temperatures, airflow rate and the dial reading.<br />
6. Increase the chamber pressure and with the original inlet pressure repeat the test.<br />
P1(kN/m 2 ) P2(kN/m 2 ) mmeasured(g/s) Δ(dial) T1(C°) T2(C°)<br />
500 150<br />
500 200<br />
500 250<br />
500 300<br />
500 350<br />
500 400
Calculations and Results:<br />
Do the steps below for the given pressure adjustments:<br />
1. Calculate the theoretical mass flow rate.<br />
2. Calculate the jet velocity.<br />
3. Calculate the specific kinetic energy, V2/2.<br />
4. Calculate the isentropic enthalpy change.<br />
5. Calculate the nozzle efficiency.<br />
6. Tabulate all the results for each pressure adjustment.<br />
7. Plot m_ theoretical/rp.<br />
8. Plot m_ measured/rp.<br />
Note: Be careful on the units !<br />
Discussions and Conclusion:<br />
Make comment on the graph. Write your own opinions about the results. What might be the<br />
possible causes of errors in this experiment? Discuss about whether the results are acceptable or<br />
not? Make comment on the efficiency of the nozzle.