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Transcript of SUBHARTI
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A TRAINING PROJECT REPORT
ON
GSM TECHNOLOGY
Submitted for the partial fulfilment of the requirement for award ofthedegree
Of
BACHELOR OF TECHNOLOGY
In
ELECTRICAL AND ELECTRONICS
Submitted To:- Submitted By:-
SOURAV GOSWAMI
SUBHARTI INSTITUTE OF TECHNOLOGY AND ENGINEERING
MEERUT(U.P.)
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CERTIFICATE
This is to certify that the work which is being presented in the project report
title Electromagnetic Reciprocating Engine in partial fulfilment for
the award of the degree of B- Tech and submitted to the department ofMECHANICAL ENGINEERING, SITE, is an authentic record of our own
work carried out during the academic session 2011-2012.Under the
supervision of Er. D. P. SINGH by following students.
VISHAL SHARMA (0820940024)
NITIN MASAND (0820940412)
NISHANT SAINI (0820940015)
SUBHASHISH SOLANKI (0820940022)
DINESH RANA (0820940409)
RAHUL SINGH TOMAR (0820940018)
This is to certify that the above statement made by the above candidates is
correct to the best of my knowledge.
Date..
Place.
(Er. D.P.SINGH) (Er. G.K. VARSHNEY)
Asst. Professor. H.O.D. External Examiner
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ACKNOWLEDGEMENT
Acknowledgement is not a mere obligation but an epitome of humility and
indebtedness to all those who have helped in the compilation of this project and
without whom my project would have been anything but presentable.
First of all, we are grateful to Er. D.P.SINGH, Asst. Professor MECHANICAL
ENGINEERING Department, Subharti Institute of Technology & Engineering
for his constant encouragement and guidance during the preparation of this
work.
We express our sincere gratitude to Er.G.K.VARSHNEY, HOD, Mechanical
Engineering Department, Subharti Institute of Technology & Engineering, for
his invaluable suggestions and constructive criticism regarding this report.
Youre Faithfully
VISHAL SHARMA (0820940024)
NITIN MASAND (0820940412)
NISHANT SAINI (0820940015)
SHUBHASISH SOLANKI (0820940022)
DINESH RANA (0820940409)
RAHUL SINGH TOMAR (0820940018)
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CONTENTS
TOPICS PAGE NO.
1. Abstract
2. Overview
3. History of electromagnetic engine
4. What is electromagnet
5. Electromagnet Structure and types
6. Electromagnet Components
7. Electromagnetic reciprocating engine and its types
8. Parts of Engine
a) Electrical parts
b) Mechanical parts
9. How electromagnetic Engine works
10.Engine Performance
11.Engine Efficiency
12.Application and Maintenance
13.Fail-safe measure
14. Future Scope
15.Conclusion
16.Refrences
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Abstract
In an era where energy conservation has become the latest topic of
discussion not only among the erudite but also among the ordinary
responsible denizens , fuel efficiency along with minimum
pollution has become the benchmark for any new automobile.
And in the same context Electromagnetic Reciprocating
Engine come as the latest addition. By the name itself it can be
inferred that a Electromagnetic Reciprocating Engine is an
improvisation to the traditional gasoline engine run car combined
with the power of an electric motor.
The seminar on the above topic intends to bring to notice
the concepts associated with the hybrid technology through the
following topicscomponents , need , efficiency and performance
etc.
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Overview
Electromagnetic engine is a future generation engine , takes
electric energy as power source .
The engine is different from the ordinary engine in many ways.
The energy efficiency is much higher than the ordinary enginebecause the heat and thermal loss are negligible .
The advantages of the electromagnet is to act as pulling force that
can be control by the current supply .
The system is compact and the moving part is less than the
ordinary engine ,thats reduce the wear and tear of the engine and
deduct the maintenance cost and running cost .
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The History of the Electro-Magnetic Engine
This is the story of rise and fall of the little known electro-magnetic
engine. During the late 1700s and early 1800s many interesting and
little understood electrical experiments were conducted both here
and abroad that eventually led to the discovery of previously relied
on a form of capacitance , for electrical energy. In 1820, Oersted
discovered by accident that electricitythrough a wire woulddeflect
the needle of a compass and concluded that some form of
magnetism was present. In 1831, Faraday discovered the magnetic
field and hence the effect of an electrified coil on steel and on a
permanent magnet and vice versa. Faraday's experiments and
discoveries led to many useful inventions, including the multipolar
motor in 1838 by Jacobi, the telegraph in 1840 by Wheetstone and
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Morse, the dynamo in 1871 by Gramme, and the telephone in 1876
by Bell to mention a few. But, in 1845, one industrious
entrepreneur by the name of Bourbouze, wanted to capitalize on
the electric coil 'solenoid effect' in a grand manner. He envisioned
solenoid driven crank shaft engines powered by rooms full of
batteries, as an alternative to the then current steam power. So, in a
fashion similar to the later 'halfbreed,' Bourbouze removed the
cylinder, piston and valve system from a steam engine and replaced
them with a large electric coil, a plunger, a switch arrangement for
timing. Well-yes, the engine worked, but there wasn't enough
sulfuric acid and zinc available in quantity for the batteries to meet
the need and to compete with the low cost, readily available coal
for steam engines. So, like many other early ideas and inventions,
the electro-magnetic engine was short lived. Later, the term
electromagnetic engine was changed to electric motor.
Coincidentally, the efficiency of the early steam engine and the
electro-magnetic engine were about the same at 20-25%, as
compared to the later well-developed D.C. motor at 95%, and the
A.C. Motor at 89%
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Electromagnets:-
Electromagnets are magnets whose magnetic properties come from
or are generated through electricity. A magnet is a material (this is
usually metal), which has at least one pair of negative and positive
poles. These opposite poles' attraction produces a magnetic field.
This gives the magnet the ability to 'attract' metals such as iron or
steel. Electromagnets are soft magnets whose magnetic field can be
strengthened or weakened depending on the electric current
applied; the stronger the current, the stronger the magnetic field
produced. Electromagnets are distinct from hard magnets
(manufactured or naturally occurring). The magnetic field of hard
magnets is quite permanent or long lasting and is therefore not
dependent on electric current.
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STRUCTYRE AND DESIGN
The passage of electric charge (electrons) from a battery's or power
source's negative terminal through wires generates a weak
magnetic field. This magnetic field is so weak (or so small) that it
is generally undetected. However, a
compass will detect such a magnetic field.
To be useful, therefore, the magnetic fieldgenerated through the flow of electrons
should be strengthened. This can be done
by making a tight coil of conductive wire.
The coils will reinforce and strengthen the
magnetic field which has a direction or
orientation that is perpendicular to the direction of the electric
current.
When electricity is supplied to this coiled wire, there will result
various magnetic domains for each coil. These magnetic domains
will tend to align themselves; and the stronger the electric current
applied, the more the individual magnetic domains will be aligned.
The application of an optimal level of electric current will result in
a perfect alignment of all magnetic domainsand result in optimal
magnetic strength.
To make the electromagnet even more powerful, one can coil the
wire around a material that has magnetic permeability or
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susceptibility (simply, a material that can be magnetized). The core
material can be something that is capable of being temporarily
magnetized such as paramagnets which are susceptible to
magnetism but are unable to retain their magnetic properties after
the application of the electric current stops. The core material can
also be ferromagnets which are capable of retaining the magnetic
field they have acquired even after electric current application
cease
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Types of electromagnets
Starter solenoid
Solenoids are used to control the starter motor in virtually every
automobile. When the solenoid is energized by turning the ignition
key, a conductor is pulled against two terminals, and a large current
flows from the battery to the starter motor. It also moves the drive
pinion to connect the starter motor gear with the engine flywheel.
When the ignition key is released, the spring pushes the conductor
off the terminals and stops the starter motor, and also disengages
the pinion gear.
Troubleshooting solenoid
If a solenoid fails to move back into place when the coil current
stops flowing, the spring in the base may be broken. If a solenoid
makes a continuous clicking sound, the current is insufficient to
create a field strong enough to keep the the spring compressed.
This may be caused by a short in the coil that is preventing current
from flowing through all the coil turns.
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Linear solenoid
Another type of electromagnetic actuator that converts an electrical
signal into a magnetic field is called a Solenoid. The linear
solenoid works on the same basic principal as the
electromechanical relay (EMR) seen in the previous tutorial and
like relays, they can also be controlled by transistors or MOSFET.
A Linear Solenoid is an electromagnetic device that converts
electrical energy into a mechanical pushing or pulling force or
motion. Solenoids basically consist of an electrical coil wound
around a cylindrical tube with a ferro-magnetic actuator or
"plunger" that is free to move or slide "IN" and "OUT" of the coils
body. Solenoids are available in a variety of formats with the more
common types being the linear solenoidalso known as the linear
electromechanical actuator (LEMA) and the rotary solenoidwith
both types being available as either a holding (continuously
energized) or a latching type (ON-OFF pulse) with the latching
types being used in either energized or power-off applications.
Linear solenoids can also be designed for proportional motion
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control were the plunger position is proportional to the power
input.
When electrical current flows through a conductor it generates a
magnetic field, and the direction of this magnetic field with regards
to its North and South Poles is determined by the direction of the
current flow within the wire. This coil of wire becomes an
"Electromagnet" with its own north and south poles exactly the
same as that for a permanent type magnet. The strength of this
magnetic field can be increased or decreased by either controlling
the amount of current flowing through the coil or by changing the
number of turns or loops that the coil has. An example of an
"Electromagnet" is given below
Rotary solenoid
Most electromagnetic solenoids are linear devices producing a
linear back and forth force or motion. However, rotational
solenoids are also available which produce an angular or rotary
motion from a neutral position in either clockwise, anti-clockwise
or in both directions (bi-directional).
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Rotary solenoids can be used to replace small DC motors or
stepper motors were the angular movement is very small with the
angle of rotation being the angle moved from the start to the end
position. Commonly available rotary solenoids have movements of
25, 35, 45, 60 and 90o
as well as multiple movements to and from a
certain angle such as a 2-position self restoring or return to zero
rotation, for example 0-to-90-to-0o, 3-position self restoring, for
example 0o
to +45o
or 0o
to -45o
as well as 2-position latching.
Rotary solenoids produce a rotational movement when either
energized, de-energized, or a change in the polarity of an
electromagnetic field alters the position of a permanent magnet
rotor. Their construction consists of an electrical coil woundaround a steel frame with a magnetic disk connected to an output
shaft positioned above the coil. When the coil is energized the
electromagnetic field generates multiple north and south poles
which repel the adjacent permanent magnetic poles of the disk
causing it to rotate at an angle determined by the mechanical
construction of the rotary solenoid.
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Rotary solenoids are used in vending or gaming machines, valve
control, camera shutter with special high speed, low power or
variable positioning solenoids with high force or torque are
available such as those used in dot matrix printers, typewriters,
automatic machines or automotive applications etc.
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Electromagnetic reciprocating engine
An electromagnetic actuated reciprocating engine, said engine
comprising:
(a) a block, said block including
(1) a crankcase
(2) a crank rotatable mounted within said crankcase,
(3) at least one tubular cylinder, said cylinder having a bore of
preselected cross-section, an inward end and an outward end, and a
sidewall,
(4) a reciprocating piston disposed within said cylinder, said piston
including an upper portion having an outer radial edge, further
comprising at least one permanent magnet having a first endmounted adjacent said outer radial edge,
(5) rod means, said rod means including a crank end and a piston
end, said rod means connecting with said crank at said crank end
and with said piston at said piston end, said rod means adapted to
move with said piston inward and outward in a stroke wise fashion
as said crank rotates, and to thereby transfer force from said piston
to said crank, and from said crank to said piston,
(b) a first row of electromagnets, said row comprising at least N
electromagnets disposed stroke wise and externally along a portion
of said sidewall of said cylinder, said first row of said
electromagnets substantially radically aligned along a single radial
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axis with said first end of said at least one permanent magnet in
said piston, and where N is greater than or equal to two (2),
(c) a power source for energizing said electromagnets,
(d) an electrical switching circuit to direct electrical energy from
said power source to the first electromagnet in said row, to the Nth
electromagnet in said row, and each electromagnet there between,
(e) computer means, said means including a selection and timing
means to select direct which and when preselected electromagnets
from the first to the Nth electromagnets are energized in a temporal
fashion, so as to create an orchestrated sequence of timed and
magnetic forces for urging said piston inward or outward.
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The main types of electromagnetic engines
Single-loop electromagnetic engine
Even simple motor, apparently not requiring any loop but a piece
of the wire is shown on the photo
below.
Elements of the set:
1. Neodymium magnet.
2. Iron nail
3. Volta pile R6 (1,5 V).
4. Piece of wire (see photo 1)
Understanding the principle of operation of the engine above, it is
easy to explain the present one. This is just Newtons principle of
action and interaction. Essentially, this is the piece of wire
(forming the loop) which should spin around the magnet as in the
previous case. But now the loop is hold fixed, so by the principle of
reaction the magnet spins in the opposite direction, instead. Note
that the engine moves with the highest speed when the wire
touches the magnet in the middle of its heights: the magnetic flux
closed by such a loop is maximum. When the wire touches the
magnet below than the total flux is smaller and the turning around
is slower.
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Photo 1. The engine with one-loop: the battery,nail,magnet and
the wire. The wire should touch the magnet at
half of the height to assure the highest speed of turning.
Two-loop electromagnetic engine
Krzysztof Gobiowski2), Grzegorz Karwasz 3), Wim Peeters 4)
Elements of the set:
1. Neodymium magnet.
2. Volta pile R6 (1,5 V).
3. Loop (1-2 mm diameter) from Cu wire (1-2 mm dia.), see fig. 1.
Electromagnetic engine in order to work requires:
- the source of magnetic field (neodymium magnet - 1),
- electric current flowing in engine windings (loop - 3), placed in
this
field
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Principle of operation of two-loop engine
Electromagnetic engines working is based on the principle of
interaction between the magnetic field and the electric current. The
permanent (and strong) neodymium magnet creates the magnetic
field with a configuration shown on the fig. 1. In the region of the
upper segment of the loop the field is almost vertical, and in the
region of the lower segment it is directed in the opposite direction
as compared to the upper part, and it is much weaker 5). The
electrical current flows from the + pole of the battery and the
circuit is closed by the magnet (there is no isolation on the wire
wound around the magnet). The gap between the wire loop and the
magnet causes some discontinuity in the current flow but it does
not disturb the engine operation too much. The direction of theforce acting on every part of the wire is defined by the right hand
rule (thumb indicates the current, the indice the magnetic field
direction, the
middle the force). Alternatively, one can also use the vector
product F=qv x B. It turns out that the particular geometry of the
loop assures that the magnetic filed is approximately perpendicular
to all three single segments, assuring therefore the maximum force.
As seen from the fig. 2. the force moments acting on the two
wings of the loop do sum up. The engine turns around! In order
to invert the direction of rotation one can invert the battery or the
poles of the magnet. Principles to learn:
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- Lorentzs force acting on moving electrical charges (F = Bqv sin
_ , orF=qv x B) - electromagnetic force acting on the wire with
electrical current (F = BIlsin, orF=Il x B) , - right hand rule.
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Parts of electromagnetic engine :-
Electrical parts
Linear solenoid
This type of solenoid is generally called a Linear Solenoid due to
the linear directional movement of the plunger. Linear solenoids
are available in two basic configurations called a "Pull-type" as it
pulls the connected load towards itself when energized, and the
"Push-type" that act in the opposite direction pushing it away from
itself when energized. Both push and pull types are generally
constructed the same with the difference being in the location ofthe return spring and design of the plunger.
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Magnetic field of a solenoid
Inside
This is a derivation of the magnetic field around a solenoid that is
long enough so that fringe effects can be ignored. In the diagram to
the right, we immediately know that the field points in the positive
z direction inside the solenoid, and in the negative z direction
outside the solenoid.
http://en.wikipedia.org/wiki/Magnetic_fieldhttp://en.wikipedia.org/wiki/Magnetic_field -
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A solenoid with 3 Amprian loops
We see this by applying the right hand grip rule for the field around
a wire. If we wrap our right hand around a wire with the thumb
pointing in the direction of the current, the curl of the fingers
shows how the field behaves. Since we are dealing with a long
solenoid, all of the components of the magnetic field not pointing
upwards cancel out by symmetry. Outside, a similar cancellation
occurs, and the field is only pointing downwards.
Now consider imaginary the loop c that is located inside the
solenoid. By Amperes law, we know that the line integral of B
(the magnetic field vector) around this loop is zero, since it
encloses no electrical currents (it can be also assumed that the
circuital electric field passing through the loop is constant undersuch conditions: a constant or constantly changing current through
the solenoid). We have shown above that the field is pointing
upwards inside the solenoid, so the horizontal portions of loop c
doesn't contribute anything to the integral. Thus the integral of the
up side 1 is equal to the integral of the down side 2. Since we can
arbitrarily change the dimensions of the loop and get the same
result, the only physical explanation is that the integrands are
actually equal, that is, the magnetic field inside the solenoid is
radially uniform. Note, though, that nothing prohibits it from
varying longitudinally which in fact it does.
http://en.wikipedia.org/wiki/Amp%C3%A8re%27s_lawhttp://en.wikipedia.org/wiki/Right_hand_grip_rulehttp://en.wikipedia.org/wiki/Amp%C3%A8re%27s_lawhttp://en.wikipedia.org/wiki/Amp%C3%A8re%27s_lawhttp://en.wikipedia.org/wiki/Line_integralhttp://en.wikipedia.org/wiki/Electric_fieldhttp://en.wikipedia.org/wiki/Electric_fieldhttp://en.wikipedia.org/wiki/Line_integralhttp://en.wikipedia.org/wiki/Amp%C3%A8re%27s_lawhttp://en.wikipedia.org/wiki/Right_hand_grip_rulehttp://en.wikipedia.org/wiki/Amp%C3%A8re%27s_law -
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Construction
Step-1
We are using dc solenoid coil in our project to give angular motion
to our crank shaft.
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Coil detail:
Brand:IDEAL -1psi/10mm , dc 24v,1.5 amp
When we provide current to the coil it core.
Step-2
We design special crank shaft according to the solenoid coil. We
use aluminum rod and make the four crank at 90degree each other .
Use bearing on both side of crank shaft for support it on base and
we can use chain and sprocket for transmit power to gear box.
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Step-3
We attach solenoid coil with crank shaft .
Step-4
Use cam for magnetizing the coil at right time for performing the
operation smoothly.
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Transformer
A transformer transfers electrical energy between two circuits. It
usually consists of two wire coils wrapped around a core. These
coils are called primary and secondary windings. Energy is
transferred by mutual induction caused by a changing
electromagnetic field. If the coils have different number of turns
around the core, the voltage induced in the secondary coil will be
different to the first.
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HISTORY OF TRANSFORMERS
Transformers are based on the theory of electromagnetic induction,
which was discovered by Michael Faraday in 1831. It was not until
1836 that the first device, an induction coil, was invented. William
Stanley, who designed the first commercial model, introduced the
term "transformer" in 1885.
TYPES OF TRANSFORMERS
The two major types of transformer are laminated cores and
toroidals.
Laminated cores are those common cube-shaped transformers,
which are used in power adapters. They are stronger and cheaper
than toroidals.
Toroidals are smaller and lighter, for the same power rating. Theyalso produce less electrical noise and are more efficient. The
secondary winding can be joined in series to double the voltage or
joined in parallel for higher current.
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HOW DOES A TRANSFORMER WORK
Alternating current in the primary winding creates an
electromagnetic field that induces a current in the secondary
winding when the field changes. Small transformers use enameled
wire for their windings, while large transformers use insulated
copper strips. Transformers can be single winding, center-tap, or
multi-tap. Center-taps have a terminal at the middle point of the
secondary winding, which has half the voltage of the end terminal.
Multi-taps have many terminals along the winding, whose voltages
depend on their locations. The purpose of the core is to direct the
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electromagnetic field through the secondary winding. Silicon steel
cores are used for their high magnetic permeability. The insulated
laminations work better than solid cores, by confining eddy
currents, which reduces their losses.
USES OF TRANSFORMERS
Transformers are mainly used to convert one voltage to another.The process of increasing the voltage is called "stepping up", while
decreasing the voltage is called "stepping down". Most electronic
equipments need a transformer to lower the mains voltage to a
usable level. Transformers are also found in power adapters and
battery chargers. Inverters are transformers which step-up a low
voltage to a higher voltage, allowing a mains powered equipment
to run on a battery. Additional circuitry is required to change the
battery's direct current into alternating current. Transformers are
used for electricity distribution to minimize energy loss over long
distances. Higher voltages allow for lower currents, which reduces
the losses caused by resistance.
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POWER SUPPLY
In alternating current the electron flow is alternate, i.e. the electron
flow increases to maximum in one direction, decreases back to
zero. It then increases in the other direction and then decreases to
zero again. Direct current flows in one direction only. Rectifier
converts alternating current to flow in one direction only. When the
anode of the diode is positive with respect to its cathode, it is
forward biased, allowing current to flow. But when its anode is
negative with respect to the cathode, it is reverse biased and does
not allow current to flow. This unidirectional property of the diode
is useful for rectification. A single diode arranged back-to-back
might allow the electrons to flow during positive half cycles only
and suppress the negative half cycles. Double diodes arranged
back-to-back might act as full wave rectifiers as they may allow the
electron flow during both positive and negative half cycles. Four
diodes can be arranged to make a full wave bridge rectifier.
Different types of filter circuits are used to smooth out the
pulsations in amplitude of the output voltage from a rectifier. The
property of capacitor to oppose any change in the voltage applied
across them by storing energy in the electric field of the capacitor
and of inductors to oppose any change in the current flowing
through them by storing energy in the magnetic field of coil may
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be utilized. To remove pulsation of the direct current obtained from
the rectifier, different types of combination of capacitor, inductors
and resistors may be also be used to increase to action of filtering.
NEED OF POWER SUPPLY
Perhaps all of you are aware that a power supply is a primary
requirement for the Test Bench of a home experimenters mini
lab. A battery eliminator can eliminate or replace the batteries of
solid-state electronic equipment and the equipment thus can be
operated by 230v A.C. mains instead of the batteries or dry cells.
Nowadays, the use of commercial battery eliminator or power
supply unit has become increasingly popular as power source for
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household appliances like transreceivers, record player, cassette
players, digital clock etc.
Use of diodes in rectifiers
Electric energy is available in homes and industries in India,
in the form of alternating voltage. The supply has a voltage of
220V (rms) at a frequency of 50 Hz. In the USA, it is 110V at 60
Hz. For the operation of most of the devices in electronic
equipment, a dc voltage is needed. For instance, a transistor radio
requires a dc supply for its operation. Usually, this supply is
provided by dry cells. But sometime we use a battery eliminator in
place of dry cells. The battery eliminator converts the ac voltage
into dc voltage and thus eliminates the need for dry cells.
Nowadays, almost all-electronic equipment includes a circuit that
converts ac voltage of mains supply into dc voltage. This part of
the equipment is called Power Supply. In general, at the input of
the power supply, there is a power transformer. It is followed by adiode circuit called Rectifier. The output of the rectifier goes to a
smoothing filter, and then to a voltage regulator circuit. The
rectifier circuit is the heart of a power supply.
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Rectification
Rectification is a process of rendering an alternating current
or voltage into a unidirectional one. The component used for
rectification is called Rectifier. A rectifier permits current to flow
only during the positive half cycles of the applied AC voltage by
eliminating the negative half cycles or alternations of the applied
AC voltage. Thus pulsating DC is obtained. To obtain smooth DC
power, additional filter circuits are required.
A diode can be used as rectifier. There are various types of
diodes. But, semiconductor diodes are very popularly used as
rectifiers. A semiconductor diode is a solid-state device consistingof two elements is being an electron emitter or cathode, the other
an electron collector or anode. Since electrons in a semiconductor
diode can flow in one direction only-from emitter to collector- the
diode provides the unilateral conduction necessary for rectification.
Out of the semiconductor diodes, copper oxide and selenium
rectifier are also commonly used.
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Rectification
It is possible to rectify both alternations of the input voltage
by using two diodes in the circuit arrangement. Assume 6.3 V rms
(18 V p-p) is applied to the circuit. Assume further that two equal-
valued series-connected resistors R are placed in parallel with the
ac source. The 18 V p-p appears across the two resistors connected
between points AC and CB, and point C is the electrical midpoint
between A and B. Hence 9 V p-p appears across each resistor. At
any moment during a cycle of vin, if point A is positive relative to
C, point B is negative relative to C. When A is negative to C, point
B is positive relative
to C. The effective voltage in proper time phase which each diode
"sees" is in Fig. The voltage applied to the anode of each diode is
equal but opposite in polarity at any given instant.
When A is positive relative to C, the anode of D1 is positive
with respect to its cathode. Hence D1 will conduct but D2 will not.
During the second alternation, B is positive relative to C. The
anode of D2 is therefore positive with respect to its cathode, and
D2 conducts while D1 is cut off.
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There is conduction then by either D1 or D2 during the entire
input-voltage cycle.
Since the two diodes have a common-cathode load resistor
RL, the output voltage across RL will result from the alternate
conduction of D1 and D2. The output waveform vout across RL,
therefore has no gaps as in the case of the half-wave rectifier.
The output of a full-wave rectifier is also pulsating direct
current. In the diagram, the two equal resistors R across the input
voltage are necessary to provide a voltage midpoint C for circuit
connection and zero reference. Note that the load resistor RL is
connected from the cathodes to this center reference point C.
An interesting fact about the output waveform vout is that its peak
amplitude is not 9 V as in the case of the half-wave rectifier using
the same power source, but is less than 4 V. The reason, of
course, is that the peak positive voltage of A relative to C is 4 V,
not 9 V, and part of the 4 V is lost across R.
Though the full wave rectifier fills in the conduction gaps, it
delivers less than half the peak output voltage that results from
half-wave rectification.
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Bridge Rectifier
A more widely used full-wave rectifier circuit is the bridge
rectifier. It requires four diodes instead of two, but avoids the need
for a centre-tapped transformer. During the positive half-cycle of
the secondary voltage, diodes D2 and D4 are conducting and
diodes D1 and D3 are non-conducting. Therefore, current flows
through the secondary winding, diode D2, load resistor RL and
diode D4. During negative half-cycles of the secondary voltage,
diodes D1 and D3 conduct, and the diodes D2 and D4 do not
conduct. The current therefore flows through the secondary
winding, diode D1, load resistor RL and diode D3. In both cases,
the current passes through the load resistor in the same direction.
Therefore, a fluctuating, unidirectional voltage is developed across
the load.
Filtration
The rectifier circuits we have discussed above deliver an
output voltage that always has the same polarity: but however, this
output is not suitable as DC power supply for solid-state circuits.
This is due to the pulsation or ripples of the output voltage. This
should be removed out before the output voltage can be supplied to
any circuit. This smoothing is done by incorporating filter
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networks. The filter network consists of inductors and capacitors.
The inductors or choke coils are generally connected in series with
the rectifier output and the load. The inductors oppose any change
in the magnitude of a current flowing through them by storing up
energy in a magnetic field. An inductor offers very low resistance
for DC whereas; it offers very high resistance to AC. Thus, a series
connected choke coil in a rectifier circuit helps to reduce the
pulsations or ripples to a great extent in the output voltage. The
fitter capacitors are usually connected in parallel with the rectifier
output and the load. As, AC can pass through a capacitor but DC
cannot, the ripples are thus limited and the output becomes
smoothed. When the voltage across its plates tends to rise, it stores
up energy back into voltage and current. Thus, the fluctuations in
the output voltage are reduced considerable. Filter network circuitsmay be of two types in general:
Diode
A diode is a solid state device that allows current to flow in only
one direction, a process known as rectification. Diodes are a
fundamental component of electrical circuits. They are also used to
form other components, such as the bipolar transistor, which uses
two diodes in series.
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History of diode
Thermionic rectifiers were discovered in 1873 by FREDERICK
GUTHRIE, and later rediscover by THOMAS EDISON, while
crystal rectifiers were discovered in 1874 by KARL BRAUN it
was not until 1919 that rectifiers were renamed diodes by
WILLIAM ECCLES, although power diodes are still called
rectifiers today.
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MECHANICAL PARTS
Flywheel
A flywheel is a rotating mechanical device that is used to
storerotational energy. Flywheels have a significantmoment of
inertia, and thus resist changes in rotational speed. The amount of
energy stored in a flywheel is proportional to the square of
itsrotational speed. Energy is transferred to a flywheel by
applyingtorqueto it, thereby increasing its rotational speed, and
hence its stored energy. Conversely, a flywheel releases stored
energy by applying torque to a mechanical load, thereby decreasing
its rotational speed.
Three common uses of a flywheel include:
They provide continuous energy when the energy source isdiscontinuous. For example, flywheels are used
inreciprocating enginesbecause the energy source, torque
from the engine, is intermittent.
They deliver energy at rates beyond the ability of a continuousenergy source. This is achieved by collecting energy in the
flywheel over time and then releasing the energy quickly, at
rates that exceed the abilities of the energy source.
They control the orientation of a mechanical system. In suchapplications, the angular momentum of a flywheel is purposely
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transferred to a load when energy is transferred to or from the
flywheel.
TYPICAL FLYWHEEL STRUCTURES.
Flywheels are often used to provide continuous energy in systems
where the energy source is not continuous. In such cases, the
flywheel stores energy when torque is applied by the energy
source, and it releases stored energy when the energy source is not
applying torque to it. For example, a flywheel is used to maintain
constant angular velocity of thecrankshaftin a reciprocating
engine. In this case, the flywheelwhich is mounted on the
crankshaftstores energy when torque is exerted on it by a
firingpiston, and it releases energy to its mechanical loads when
no piston is exerting torque on it. Other examples of this
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arefriction motors, which use flywheel energy to power devices
such astoy cars.
A flywheel may also be used to supply intermittent pulses of
energy at transfer rates that exceed the abilities of its energy
source, or when such pulses would disrupt the energy supply (e.g.,
public electric network). This is achieved by accumulating stored
energy in the flywheel over a period of time, at a rate that is
compatible with the energy source, and then releasing that energy
at a much higher rate over a relatively short time. For example,
flywheels are used inpunchingmachines andrivetingmachines,
where they store energy from the motor and release it during the
punching or riveting operation.
The phenomenon ofprecessionhas to be considered when using
flywheels in vehicles. A rotating flywheel responds to any
momentum that tends to change the direction of its axis of rotation
by a resulting precession rotation. A vehicle with a vertical-axis
flywheel would experience a lateral momentum when passing the
top of a hill or the bottom of a valley (rollmomentum in response
to a pitch change). Two counter-rotating flywheels may be needed
to eliminate this effect. This effect is leveraged inmomentum
wheels, a type of flywheel employed in satellites in which the
flywheel is used to orient the satellite's instruments without thruster
rockets.
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A flywheel is a spinning wheel or disc with a fixed axle so that
rotation is only about one axis. Energy is stored in
therotoraskinetic energy, or more specifically,rotational
energy:
Where:
is theangular velocity, and is themoment of inertiaof themassabout the center of
rotation. The moment of inertia is the measure of resistance
totorqueapplied on a spinning object (i.e. the higher the
moment of inertia, the slower it will spin when a given force is
applied).
The moment of inertia for a solid cylinder is , for a thin-walled empty cylinder is , and for a thick-walled empty cylinder
is ,[4]
Where m denotes mass, and rdenotes a radius.
When calculating withSIunits, the standards would be for
mass,kilograms; for radius, meters; and for angular
velocity,radianspersecond. The resulting answer would be
injoules.
The amount of energy that can safely be stored in the rotor depends
on the point at which the rotor will warp or shatter. Thehoop
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stresson the rotor is a major consideration in the design of a
flywheel energy storage system.
Where:
is the tensile stress on the rim of the cylinder is the density of the cylinder is the radius of the cylinder, and is theangular velocityof the cylinder.
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an industrial flywheel.
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Crankshaft
The crankshaft, sometimes casually abbreviated to crank, is the
part of an engine that translates reciprocating linear piston
motion into rotation. To convert the reciprocating motion into
rotation, the crankshaft has "crank throws" or "crankpins",
additional bearing surfaces whose axis is offset from that of the
crank, to which the "big ends" of the connecting rods from each
cylinder attach.
It typically connects to a flywheel, to reduce the pulsation
characteristic of the four-stroke cycle, and sometimes a torsional
or vibrational damper at the opposite end, to reduce the torsional
vibrationsoften caused along the length of the crankshaft by the
cylinders farthest from the output end acting on the torsional
elasticity of the
Al .
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Bearing
Have you ever wondered how things like inline skate wheels and
electric motors spin so smoothly and quietly? The answer can befound in a neat little machine called a bearing.
A tapered roller bearing from a manual transmission
The bearing makes many of the machines we use every day
possible. Without bearings, we would be constantly replacing parts
that wore out from friction. In this article, we'll learn how bearings
work, look at some different kinds of bearings and explain their
common uses, and explore some other interesting uses of bearings.
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The concept behind a bearing is very simple: Things roll better
than they slide. The wheels on your car are like big bearings. If you
had something like skis instead of wheels, your car would be a lot
more difficult to push down the road.
That is because when things slide, the friction between them causes
a force that tends to slow them down. But if the two surfaces can
roll over each other, the friction is greatly reduced.
Bearings reduce friction by providing smooth metal balls or
rollers, and a smooth inner and outer metal surface for the balls to
roll against. These balls or rollers "bear" the load, allowing the
device to spin smoothly.
Bearing Loads
Bearings typically have to deal with two kinds of loading, radial
and thrust. Depending on where the bearing is being used, it may
see all radial loading, all thrust loading or a combination of both.
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The bearings that support the shafts of motors and pulleys are
subject to a radial load.
The bearings in the electric motor and the pulley pictured above
face only a radial load. In this case, most of the load comes from
the tension in the belt connecting the two pulleys.
The bearing above is like the one in a barstool. It is loaded purely
in thrust, and the entire load comes from the weight of the personsitting on the stool.
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Types of Bearings
There are many types of bearings, each used for different purposes.
These include ball bearings, roller bearings, ball thrust bearings,
roller thrust bearings and tapered roller thrust bearings.
Ball bearing
Ball bearings, as shown below, are probably the most common
type of bearing. They are found in everything from inline skates tohard drives. These bearings can handle both radial and thrust loads,
and is usually found in applications where the load is relatively
small.
In a ball bearing, the load is transmitted from the outer race to the
ball, and from the ball to the inner race. Since the ball is a sphere, itonly contacts the inner and outer race at a very small point, which
helps it spin very smoothly. But it also means that there is not very
much contact area holding that load, so if the bearing is
overloaded, the balls can deform or squish, ruining the bearing.
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Working of electromagnetic reciprocating engine
When the AC power of 240 volt supplied to the engine, current
goes to step down transformer. Transformer converts the 240 volt
supply in to 24 volt. 24 volt supply goes to the rectifier .rectifier
works as a converter which converts the ac current in to dc current
.solenoid which is used in this engine are dc solenoid. When
current is passed in to the solenoid, magnetic field produced within
solenoid .Iron core moved within the coil. Which is reciprocating
in nature .the core is attached to the crank shaft through the
connecting rod. The work of crank shaft to convert the
reciprocating motion in to rotational motion. A system is attached
to the crank shaft which makes the close circuit of all the four
solenoid at right time. It works like a camshaft .when current is
goes to the first solenoid ,solenoid magnetize. Pulling force act on
the core. When circuit is break to the first solenoid, at that time
solenoid 4th circuit is closed and it magnetized. And after that
solenoid third is magnetized and than 2nd
solenoid .one revolution
is completed after the full operation. This process is repeated again
and again.
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Engine performance
When specifying what type of engine is needed, the mechanical
power available at the shaft is used. This means that users can
predict the torque and speed of the engine without having to know
the mechanical losses associated with the engine.
power
The power output of a engine is:
Where P is in horsepower, rpm is the shaft speed in revolutions per
minute and T is the torque in foot pounds.
And for a linear motor:
Where P is the power in watts, and F is in Newtons and v is the
speed in metres per second.
Eficiency
To calculate a engine efficiency, the mechanical output power is
divided by the electrical input power: , where is energy
conversion efficiency, is electrical input power, and is
mechanical output power.
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In simplest case , and , where is input voltage,
is input current, is output torque, and is output angular
velocity. It is possible to derive analytically the point of maximum
efficiency. It is typically at less than 1/2 thestall torque.
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Applications
Electromechanical solenoid
A 1920 explanation of a commercial solenoid used as an
electromechanical actuator
Electromechanical solenoids consist of an electromagnetically
inductive coil, wound around a movable steel oriron slug (termed
the armature). The coil is shaped such that the armature can bemoved in and out of the center, altering the coil's inductance and
thereby becoming an electromagnet. The armature is used to
provide a mechanical force to some mechanism (such as
controlling a pneumatic valve). Although typically weak over
anything but very short distances, solenoids may be controlled
directly by a controller circuit, and thus have very low reaction
times.
The force applied to the armature is proportional to the change in
inductance of the coil with respect to the change in position of the
armature, and the current flowing through the coil (see Faraday's
law of induction). The force applied to the armature will always
move the armature in a direction that increases the coil's
inductance.
Electromechanical solenoids are commonly seen in electronic
paintball markers,pinball machines, dot matrix printers and fuel
injectors. A most common application is used in automobile.
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Maintenance
The maintenance of electromagnet is very important because
magnetic field which is produced with in the coil decreases after a
long time period due to losses (iron losses, eddy current losses)
generated in the coil. Proper lubrication is used in the moving parts
like crank shaft ,connecting rod joints ,bearings etc.
Fail-safe measure
Electromagnetic coil which is used in electromagnetic engine have
fail-safe measure .the current used for running the engine have
constant frequency .fluctuation in current causes damage of coil.
To reduce these problem measuring instrument are used. To
measure the voltage, voltmeter is used and for current ampere
meter is used. Design of crankshaft, connecting rod and bearing
according their load bearing capability. Types of lubricant which is
used in moving part should be design .because friction is an
important factor causes damage of moving part due to wear and
tear and thrust which is generated in moving part. Testing machine
are used for measurement the strength of the component.
Inspection of the component should be done weekly and monthly
to reduced the failure problem.
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FUTURE SCOPE
Being a electric engine it has may futuristic benefits like it is fully
pollution free engine, no carbon foot print. In present polluted
world as governments are struggling hard to cope with pollution
our engine has great significance
As carbon fuel is decreasing day by on earth petrol and diesel fuel
is costly and decreasing the availably is also hard issue, to
overcome this problem our proposed engine has great significance
for fuel consumption as its is ruing of battery.
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Conclusion
Though at present the concept has been put in the reva car, it is
indeed an important research avenue for other car manufacturing
units as well. One can surely conclude that this concept, and the
similar ones to follow with even better efficiency & conservation
rate are very much on the anvil in todays energy deficit world.
Currently the cost of the engine is more than that
the conventional engine. Electromagnetic engine is growing in
popularity and it is likely to come in more and more new vehicles.
As the systems become more commonplace the cost of the vehicles
will drop.
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Reference
1. http:\\www.howstuffworks.com2. http:\\www.howhurricaneworks.com3. http:\\www.thecarconnection.com4. http:\\www.theautochannel.com5. http:\\www.wikkipedia.com6. http:\\www.google .com7. http:\\www.gasenginefarmcollector.com8. Theory of Machine (R.K.Bansal)10. Electrical Machine (J.B.Gupta)
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