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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.

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