International Research Journal of Engineering and Technology (IRJET)
e-ISSN: 2395 -0056
Volume: 03 Issue: 08 | Aug-2016
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USE OF PULSE JET ENGINE IN FUMIGATION PROCESS
Mr. Nikhil Bhalchandra Joshi, Mr. Harshawardhan Tanajirao Jadhav,
Mr. Pratik Prakash Borude, Dr. Sandeep S Kore
Student, Sinhgad Academy of Engineering, Pune, Maharashtra, India
Student, Sinhgad Academy of Engineering, Pune, Maharashtra, India
Student, Sinhgad Academy of Engineering, Pune, Maharashtra, India
Head Of Department, Mechanical Department, Sinhgad Academy of Engineering, Pune, Maharashtra, India
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract – Jet engines are generally used to create thrust
explain the four basic phases in the pulsejet's operational
cycle.
force. We have used pulse jet engine technology for the
development of the agro product for the purpose of
fumigation. In this paper, we are going to discuss design
methodology, method of operation and results of this
technology.
1. Ignition
This is the instant that the fuel and air in the
pulsejet are ignited. The effect is that a fireball is
produced inside the engine which creates a great
deal of heat and pressure. The reed valves are
held closed by this pressure, effectively leaving
the flame and hot gases only one place to go.
2. Combustion
After ignition, the air and fuel continue to burn
and expand in a phase called the combustion
phase. During this phase the burning gases
expand and travel down the tailpipe, exiting at the
rear of the engine. The force of the gases leaving
the engine in a rearwards direction creates an
equal and opposite force that tries to move the
engine forwards -- this is thrust.
3. Intake
Because gases are elastic (they can be compressed
and stretched) and because they have mass, the
rapidly exiting exhaust gases have a tendency to
keep moving -- even after the pressure inside the
engine drops below the pressure outside. This
causes a partial vacuum to be created inside the
engine.
4. Compression
As mentioned above, gases are elastic -- so now,
having been stretched out to create a partial
vacuum, some of the hot exhaust gases are now
drawn back towards the front of the engine by the
vacuum that was created. Once again, because they
have momentum, the gases in the tailpipe continue
to move even after the pressure inside and outside
the engine is equalized. This means that the gases
continue heading towards the front of the engine -towards the fresh charge of air and fuel that has just
been drawn in. Of course, as soon as the pressure
inside the engine becomes higher than the air
pressure outside, the reed valves slam shut -stopping the air/fuel mixture from escaping.
Key Words:- Jet engines, Thrust Force, Agro product,
Fumigation, Design methodology.
1. INTRODUCTION
In agricultural farms insects feed on crops and tend to
damage them. The insecticides are sprayed on the
plant/crop and this method is called fumigation. The
conventional method of fumigation is to spray a mixture of
water and insecticide on the plant. The apparatus consists of
air blower that blows the mixture on the crop. When this
mixture is sprayed on the crop it affects the digestive system
of the plant and decreases productivity to large extent.
This gives rise to design of a system that can satisfy all the
above needs of agricultural field. One such system is using a
pulse jet engine. Jet engines are generally used to create
thrust force. Instead of continuous combustion the
combustion in pulse jet is in the form of pulse.
The mediator used here can be diesel. The combustion thrust
force of pulse jet engine is generally 800° C. Using a cooling
jacket by natural convection the temperature can be brought
down to about 200° C, at this temperature diesel will get half
burnt giving smoke as a byproduct consisting of CO2. When a
mixture of diesel and insecticide is sprayed on the plant it
creates a mist that will suffocate the insect and force it to
come on the upper portion of the leaf for atmospheric air.
The diesel being light in weight will evaporate and
insecticide will act on the insect and kill it. CO2 will by
plant/crop for photosynthesis.
2. WORKING OF PULSEJET ENGINE
Pulsejets are very simple engines but their operation is not
always easily understood -- after all, how an almost empty
pipe can run as a jet engine. This page is an attempt to
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e-ISSN: 2395 -0056
Volume: 03 Issue: 08 | Aug-2016
p-ISSN: 2395-0072
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This continued movement of the exhaust gases
causes the air-fuel mixture to be compressed -- until
the hot gases finally travel so far up the pipe that
they touch the explosive air/fuel mixture and -back to step one!
3.4. Reed Valve
Reed Valve consists of two plates with holes and a
Teflon sheet. Air is sucked in through the reed valve
from the second cycle. The distance between the plate
with holes and Teflon sheet is used to adjust the Air-Fuel
ratio.
This cycle repeats hundreds of times a second -producing the characteristic buzzing sound of the
pulsejet engine.
3.5. Combustion Chamber
Combustion of the mixture takes place in this chamber.
It is made of SS304. SS304 has a property of retaining
heat when it gets red hot. This retained heat is used to
keep the cycle running.
1.2 SCHEMATIC REPRESENTATION
3.6 Nozzle
It used to direct and modify the flow of exhaust gases.
3.7. Nozzle Pipe
It is placed after the nozzle. As the exhaust gases move
out of the nozzle pipe it creates a back pressure because
of which a fresh mixture if sucked into the secondary
combustion chamber. This helps to keep the cycle
running.
4. DESIGN METHODOLOGY
4.1 DESIGN OF NOZZLE
Fig 3.2.1: SCHEMATIC REPRESENTATION OF PROJECT WORKING
MATERIAL SELECTED: SS 304
Yield strength=215 MPa
3. DESCRIPTION OF PARTS
SS 304 has good thermal resistance. Once the material gets
red hot it does not allow the heat to go out.
3.1. Venturi
Venturi works as fuel injector similar to a carburettor. It
is a pressure reducing device. The throat of venturi has
lateral holes present in it, through which the fuel gets
injected in the throat of venturi. As per the Bernoulli's
principle, there is pressure reduction in the throat of the
venturi due to which fuel gets sucked in through the
holes. Venturi is placed in a casing that contains petrol.
Design parameters:
Mass flow rate of inlet air = 0.75kg/hr
3.2. Spark plug
The fuel used for the joule cycle to produce the thrust
force is petrol. A spark plug is used to ignite the air-fuel
mixture for the first cycle. The spark plug is given a
supply of 12V DC battery. The spark plug must be turned
off after the first cycle.
Inlet pressure P1
= 8000 kg/m2
Inlet air velocity C1
= 3.5 m/s
Inlet Temperature T1
= 800° C
Outlet Pressure P2
= 4300 kg/m2
Exhaust gas velocity C2 = 35 m/s
Outlet Temperature T2 = 600° C
3.3. Petrol and Diesel tank
Gas constant R
Petrol tank stores petrol that is used to run the pulse jet
engine. Diesel tank stores a mixture of diesel and
pesticide. Diesel is used as a secondary fuel, used for the
production of fog which contains smoke and particles of
pesticide.
= 0.287 kJ/kg °K
We know,
Pv = mRT
M= mass flow rate kg/sec
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T= Temperature in °K
V=AC
στ =
Where A= Area in m²
To calculate inlet area of nozzle
=
A1 = (mRT1) / (P1C1)
=6.833 MPa << 215 MPa
= (0.75*287*1073)/(8000*3.5*3600)
So design is safe.
= 2.29*10³ m²
Note: The pressure in nozzle pipe is assumed to same as
combustion pressure for design purpose. In an actual
case, it is less than 15 Kg/cm2 because of conversion of
pressure head into velocity head in diffuser section.
A1 = π/ d1²
d 1= 54mm.
4.3 DESIGN OF MANIFOLD PIPE
Outlet diameter can be calculate from continuity equation,
Q = A1*C1=A2*C2
MATERIAL SELECTED: SS 304
d2 = d 1 (C1 / C2)½
Yield strength=215 MPa
SS 304 has good thermal resistance. Once the material
gets red hot it does not allow the heat to go out.
= 54(3.5*35)½
= 17.076 mm
Inlet pressure of air is pressure applied by hand pump
which is same as the pressure in manifold & also in the
combustion chamber as the operation of this engine is
based on joules cycle.
Taking d 2= 18mm
Which is inside the diameter of diffuser outlet?
Taking t = 1.5mm
Here pressure at pt 2 = pressure in manifold =
combustion chamber, 1. 5 MPa
Therefore outer diameter = d2 + 2*t
Consider manifold pipe as thin cylinder, checking for
hoops stress in pipe
= 21mm
4.2 DESIGN OF NOZZLE PIPE
MATERIAL SELECTED: SS 304
στ=
Yield strength=215 MPa
Our taken c/s for nozzle pipe is having
Where,
P = pressure in manifold
O.D. = 25mm
I.D. = 20.5mm
di= inner diameter of manifold = 24mm
t
t = thickness of manifold = 1.5 mm
= 2.25mm
D/t =25/2.25 = 11.11 >10
Hence design is based on thin cylinders.
=
Maximum hoop stress
= 12 MPa <<< 53.75 MPa
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Note :
Design parameters
Our selected material is SS 304.
Mass flow rate of inlet air = 0.75kg/hr
It is having yield strength of 215MPa.
Inlet pressureP1 = 4000 kg/m2
Allowable stress = yield stress / factor of safety
Din/Dout
=2
Taking fos =4
Taper Angle
= 21°
Allowable stress =53.75 MPa
Thus 12MPa is much less than allowable stress.
4.4 DESIGN OF COMBUSTION CHAMBER
Assume, L=0.08m
Material selected Is SS 304
Allowable stress = στ = fos =1000/4 =250 MPa
We first select dimensions for combustion chamber
O.D.
= 50mm
I.D.
= 44mm
t = 3mm
D/t =50/3 = 16.67 >10
Hence design is based on thin cylinders.
Maximum hoop stress
Applying continuity equation at sections 1 and 2
στ =
=
=110 Mpa << 250 Mpa (allowable)
So design is safe.
4.5. DESIGN OF VENTURI
Applying Bernoulli’s Equation,
Material selected: BRASS
Brass has good malleability. It can be easily machined to very
minute and accurate dimensions.
It also has good corrosion resistance.
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From calculations, we get permissible stress as 45.7 MPa
which is within the allowable range.
5. NOMENCLATURE:
Symbol
M
P
C
T
R
Q
40.77 m of water
d1
d2
T
Στ
Fos
Δ
L
Cp
K
4.7. DESIGN OF FUEL TANK:
Design Parameters:
Pressure in tank P
=
8 bar
Diameter of tank Di
=
80 mm
Thickness of tank t
=
0.7 mm
µ
Consider the tank as thin cylinder, checking for hoop
stresses,
Gr no
Nu
H
Am
U
LMTD
W
η
S
Description
mass flow rate
Pressure
air velocity
Temperature
Gas constant
the volume flow
rate
outer diameter
Inner diameter
Thickness
Hoop Stress
Factor of safety
Density
Length
specific heat
Thermal
conductivity
Coefficient
of
viscosity
Grashoffs number
Nussle Number
Heat
transfer
coefficient
Mean peripheral
area
Overall
heat
transfer
coefficient
Logarithmic mean
temperature
difference
Work done
Air
standard
efficiency
Entropy
Value/Unit
kg/hr
MPa
m/s
°C
0.287 kJ/kg °K
kg/m3
Mm
Mm
Mm
MPa
-------Mm
kJ/kg K
W/Mk
Ns/m2
……….
……….
W/m2k
m2
W/m2k
°C
Joule
……….
W/k
Note:
Our material selected is Mild Steel, having a yield
strength of 250 MPa.
6. METHOD OF OPERATION:
1) Put fuel in petrol tank by opening the main cock.
2) For initial starting purpose the hand pump is
operated & ignition switch is kept „ON‟ position.
3) As fuel pump is given 2-3 strokes by hand it induces
back pressure which is given to petrol tank through
the housing.
4) The pressure in the petrol tank is now just above
atmospheric thus listing petrol tank to fuel nozzle
can be varied with cock provided.
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5) This enriched mixture flows to manifold as there is
no other place for the mixture to escape.
6) As required voltage is given back to spark plug by
pressing switch a spark is produced which initiated
the combustion.
7) Once combustion is started there is no need to
operate hand pump and switch ignition switch.
8) The high-pressure mixture then finds its way to
exhaust pipe which consequently creates pressure
in the manifold.
9) The air then sucked through air valve and back
pressure is given to carburetor which eventually
lifts petrol from the tank and again it supplies it to a
nozzle.
10) The diesel in diesel tank is pressurized by the by the
means of a flow control valve connected to the
pressure line. As a result, the diesel flows to the
nozzle.
11) The flow of diesel is controlled by the flow control
valve.
12) This process is repeated automatically.
7. CONCLUSIONS
1) Pulsejet engines offer an attractive form of propulsion
due to their simpler and cheaper construction. The
essence of this project was to improve knowledge of
pulsejet engine operation which is successfully
achieved.
2) The experimental engine included geometry
adjustability which proved advantageous in obtaining
the maximum thrust of 1.745kg, 30.3% less than the
desired 2.5kg but consistent with the results of the
theoretical model.
3) Our main aim of development of pulse jet engine for use
of fumigation purpose achieved.
8. REFERENCES
[1]
[2]
[3]
[4]
[5]
[6]
L.B.EDELMAN: The Pulsating Jet Engine.Its Evolution
and Future Prospects. SAE Quarterly transactions
1(1947),pp 204-216
SCHMIDT,PAUL:"und
Noch
Einmal
v1".Motor
Rundschau,Heft 15 (1948)
DR.GOSSALU: Development of V1 Pulse Jet ,German
military Report(1962)
DR R.K.BANSAL, Fluid Mechanics and Hydraulic
Machines ,Laxmi publications
Bhandari V. B., Design of Machine Elements , rd
Edition, Tata McGraw Hill Education Private Ltd, New
Delhi.
V. Ganesan, Internal Combustion Engines , Tata
McGraw-Hill Publishing company Ltd.
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