Transcripts
1. Generation, Substation, and HV Course Content: Hi, and welcome everyone to our course for
electricity generation, high voltage and
electrical substations. I am mad Maddie and
electrical engineer. And in this course, I'm going to teach you
about these three topics. So let's start by
learning what are you going to get
from this course? First, we are going to discuss the electricity
generation. So what I mean by this, we will discuss how can
we generate electricity. And we are going to discuss the different types of
electrical generators, such as synchronous
generators and the induction generators use in the electrical power system. We will discuss how do they work or reserve
principle of operation. Then we are going to discuss
hydroelectric power plants, which they use ZAP, flow of water to generate
electrical power. We will discuss
different types of hydroelectric power plants
and how do they work. Then we are going to
discuss that diesel, fossil fuel, oil
and gas or plants. We will discuss
how do they work. Or Z is generators, principle of operation and
what are the different types? Then we are going to talk
about nuclear power plants. And how do they convert
the heat energy coming from zion nuclear
officials to electrical energy? And we will understand the
whys and nuclear energy is important compared to other types of
electrical generators. Then we are going to discuss how can we generate electricity from the heat of the earth
or thermal power. We will discuss what
is the meaning of geothermal power
plant and what are the different types of xij
annual ceremony power plants. Then we are going to discuss the first or the second
renewable energy source, which is that solar energy. We will discuss how can we convert sunlight into
electrical power? And is that important concepts regarding xhat solar energy? We will talk about how it's
as solar balance that charge controllers that involves those used in that solar
energy system. Then we will talk about another
renewable energy source, which is wind energy. We will talk about
when the energy, how can we convert that
went into electrical power. We will discuss
the main concepts regarding the wind damage. You will have an excellent
knowledge about wind. Then we are going to
have another section. We will discuss the important
definitions in generation. So in this section about
the important definitions, we will talk about what the
important definitions such as that characteristics
of generators. We will discuss a zap cost of
building each power plant. And when do we use this type of project plans and when do we use as our types
of power plants? And the difference between using renewable energy sources and non-renewable
energy sources. Then we are going to discuss is the high voltage generation. We will talk about how can
we generate high voltage, such as DC, high voltage, and high voltage with
different frequencies. We will discuss how can we build generator that will
produce high voltage? Then we are going to discuss an important component in
the electrical system, which is the electrical
substations. We will discuss what are the different components inside our electrical
substations and the y electrical substations are important in the
electrical power system. We will also discuss different types of
electrical substations, different types of breakers, circuit breakers, fuses, and
much more in this course. Also, we will talk
about with overseeing system design or does
that grounding systems. We will talk about it as
a important definition. Definitions regarding
the Earth-Sun system. We will discuss also why. It's important. And we will discuss how can
we design an aliasing system. And we will design endorsing
system using a tab broken. Finally, we will talk about some basics with the electric
console station design. So we'll have a small example which will help us to understand the idea behind the design
of electrical substation. So if you are looking for one course that
will help you get an excellent knowledge about degeneration substations
and the high voltage, then this course is for you. Thank you, and see
you in our course for electrical generation
substations and the high water. And if you have any question, just to send me a message. Thank you and see
you in our course.
2. Introduction to Electricity Generation: Hi and welcome everyone to our course for
electricity generation. And this course we are
going to talk about with that different generating
power stations. And we will talk about with our different generators
used in power plants. So first, let's have an overview of the
electrical power system. So first, our
electrical power system consisting of four main stages. It consisting of
generation phase, the transmission phase,
distribution phase, which is finally the
load consumption. So first, what we are
talking about in this course is generation part
of electrical power. Okay? So first, here we have different
generating power plants. It can be a renewable
energy source or non-renewable energy source. Then after generating
this electrical power, we are going to transmit it
using transmission lines. Two sets Revolution network. In the distribution network, we start distributing our
electrical power too different. So in this part we are concerned
with generation phase. Heard is another overview of
the electrical power system. You can see we have
the generating station or the regeneration phase. Then you will find that
we have the second phase, which is a transmission. You will find that between
generation and transmission, we need to increase our voltage. Let's say e.g. we are
generating at 11 kilowatt. Okay? So the power generated from the electrical power station is at a voltage of 11 kilovolt. Okay? Now in order to transmit
this electrical power, we need to step up the voltage. We need to increase
our voltage from 11 kilo volt to any of these
values hundred 38 kilovolt, 270 kilowatt and so on. So what we are doing is
that we are stepping up the voltage or we are
increasing our voltage. Now why you are doing this? Because we would like to reduce the losses in
our transmission lines. Okay? So when the voltage increases using an electrical transformer, the current to transform it shows our transmission
line is much lower. Therefore, the power
losses will be reduced. Okay? Then you can see that after
the transmission system, we have that
distribution network. And since we are distributing our electrical power,
you'll notice that e.g. in our home, we have a
voltage of 120 volt or 240 v, depending on the country. Other countries use
as 180 volt line to line voltage or 220
volt phase voltage. Okay? So in order to transform
from this large power, larger voltage into
smaller value that's suitable for our consumer side. We need a step-down transformer. Step down transformer
is used to reduce or decrease the voltage
required for the consumer. You will find that we have
different voltages domains depending on the customer
operating voltage. Okay? Now, here is also another overview can
see we have generation. Then we have the transformer. We need a transformer to
step up the voltage, right? We said that we have
11 kilovolts, e.g. and we need to increase the voltage coming
from the generation up to 220 kilo volt or 500
kilo volt or any value. So in order to do this, we need a step up transformer. Soul finds that we have
an intermediate stage between the regeneration phase and the transmission phase. The intermediate stage between these two phases is
called substation. The substation contains
our transformers, contains is a
protection equipment such as circuit breakers, isolators, contains
all Sousa fuses, and also contains transformers, relay is, and so on. So all of the equipment which
are used for protection and for stepping up or stepping down the voltage are existing
in a substation. Okay? Now we will find after
transmission system we have another substation
which contains the step-down transformer
and also contains protection elements or equipment such as circuit breakers, fuses, and so on. Okay, Then we are distributing electrical power to our system. Okay? So what is electricity
generation? Electricity generation is
the process of generating electrical power from
primary energy sources. For electric utilities,
it is a first stage, as we have seen in
the power system. It is a first stage in delivering electricity
to the end user. The other stages, which are
transmission distribution, ends our final stage, which is lewd or the consumption of electrical power or
consuming electrical power. So why electricity is important? Because, of course,
it is used to run your own appliances
at home efficiently. E.g. it's used in
TV refrigerators, AC fan, and et cetera. It is used also in transportation systems
such as electric trains, plans, electric cars, and so on. Also in the medical sector, we use electricity for
X-ray machines and other medical equipment or devices that work
on electricity. So what are the
different sources that we use to generate
electrical power? You'll find is that we
have two primary sources. We have renewable energy sources and non-renewable energy source. So that renewable
energy sources, which does not end these
types of resources don't end. They last forever, such as e.g. Zao, wind energy,
hydro-power energy, solar energy,
geothermal, and biomass. This, these resources
never ends or never end. For the non renewable energy
resources such as oil, coal, and nuclear, natural gas. All of these have a certain
time in which a will end, okay, So you don't last forever. So we are concerned with
renewable energy is a wallet, is trying to depend more on the renewable energy
source. Why is this? Because, as you know, that's a non-renewable energy
will not exist forever. And at the same time, you will find is that
these sources causes global warming or releases
too much carbon dioxide, which causes the
global warming effect. So we have non-renewable
energy sources such as coal. When it is born, it, it
produces electricity. We have our photovoltaic
or solar energy, which results from the sun rays. We have wind energy which is produced with the help
of Zao when the miles. We have the waterfall energy
or the hydropower which is used to generate
hydroelectric energy. So before we go to the types
of electrical generators, we have to understand that. We are going to give a small hint of how words are non-renewable
energy sources. In general, how we generate
electrical power from them. And we are more
concerned about that renewable energy sources such
as solar and wind energy. We are going to give you
in this course that pays X of generating electrical
power from solar energy. And how can you generate electrical power
from wind energy? We are going also to add
in the future more about Z is the other types of
renewable energy sources. So since we are talking about with
electricity generation, we need to understand what are the different types of
electrical engineering. So we'll find is
that there are many, many types of
electrical generators. However, if you look at electrical power
system in general, you will find that we
have two main types, two main types of
electrical genital, which are widely used in
electrical power systems. The first one is a
synchronous generators. Second one is the
induction generators. So these two types, we are going to discuss them
in details in this course. So what is the
difference between them? You'll find that
synchronous generator produces or generates
active and reactive power. So active power is simply, if you don't know
what active power is, you have to go to my own
course for electric circuits, because it is important
to understand what does an active and
reactive power means. For active power, active
power is the power which we consume, e.g. which we consume in resistors, which we consume in. Providing electrical,
mechanical power, in providing motion, and in
electric bulbs and so on. So any of these powers is
called active power is a power which consumes
or does work. However, the reactive power Q is related to the
magnetic field. So you have to understand that any electrical machines
requires magnetic field, okay, in order to operate or all in order to generate
electrical power. So some types of
electrical machines absorb reactive power or
require reactive power. Other types you can generate
reactive power, e.g. is a synchronous generator, can produce reactive power, which is required to buy
any electrical machines. However, the induction generator can only generate act of power. It absorbed bit skew, or requires the active
power in order to operate. It cannot generate
reactive power. Don't worry, we'll understand
how does this work. The synchronous generator
ends induction generator. In the next lessons, we will find that most of the power system generators
are synchronous generators. And the Z are used in the hydro
and non-renewable source, non-renewable sources of energy. Okay. So funds that most of our generators are
synchronous generators. However, the inductions and
it does not exist too much. It exists this rally in the
electrical power system. It is used in
electrical generators, produce or provide
variable power, such as wind energy. You will understand that
when the energy itself is a variable or a change with depending on the
velocity of wind. So since it is changing
with velocity of wind, it produces variable power. That's why it provides this variable power to the
electrical power grid. And in this case we use
induction generators. Okay? You will find that
synchronous generator have zero on magnetic fields. It means that they don't absorb or take reactive
power from grid. Remember, reactive power is related to the magnetic field. So they have their own
magnetic fields so they don't react apart
from grid exam, magnetic field can
exist in the form of permanent magnets
or a field winding, as we will see in
the construction of the synchronous generators. In the next lessons. For induction machines, they don't have their
own magnetic field. They need to be connected to
the grid to be magnetized, or we need to add
capacitor banks to make itself x-height. Okay, Don't worry,
all of this will be discussed in details
in each lesson. So what are we going to
do in the next lesson? In the next lesson, we are
going to study how can we generate electrical power or how is electricity generated. Okay, so we are
going to discuss is our Faraday's law of
induction and Lenz law. They will help us to
understand how can we transform and mechanical
motion into electrical power, which is, of course, most of our generators walk
on the same principle. The principle of converting mechanical power into
electrical power.
3. Faraday's Law of Induction and Lenz’s Law: Hey everyone. In this lesson we are
going to talk about with the Faraday's law of
induction and Lenz law. You have to understand that
Faraday's law is really, really important
because you will find it in every
electrical machine. So Faraday's law of
induction is used to help us understand how can we
convert mechanical energy, mechanical energy, into electrical energy,
into electrical energy. So find that this
concept of four a day will help you
understand how can we do this from
mechanical to electrical or from electrical
to mechanical, e.g. from mechanical to electrical, we are talking about electrical generators
and the conversion of electrical to mechanical. We are talking about
with electric motors. Okay? So let's understand what does this law states and
what does it mean? For today's law of
electromagnetic induction states that any change in
a magnetic field, any change in a
magnetic field will induce an electromotive force in a conductive coil that is
directly proportional to the rate of a change in the
inducing magnetic field. So what does this even mean? That's, let's continue for now and then we will
understand everything. So it will induce an
electromotive force, The call the EMF and
the measured in volts, which will also create
a current flow. And here is what does it mean? Okay? So first, the Faraday law says that any change
in the magnetic field, so our magnetic field is
measured or denoted by Phi. Phi is the magnetic flux, which you can represent the magnetic flux or Z
lines of magnetic field. So the Faraday's law says that any change in a magnetic field, any change it
change, any change, we represent it as
a differentiation. So we'll say is that any
change in the magnetic field, d phi over DT, or variation of magnetic field will induce an
electromotive force. An electromotive force
means E or a voltage. Okay? So any change in the magnetic field will lead
to an electromotive force. The value of the electromotive
force is directly proportional to the rate of change of a inducing
a magnetic field. So what we learn here
is that the voltage is produced is directly
proportional to d phi over DT, or the rate of
change of the flux. Okay? So we can remove this direct
proportional to E equal to N d phi over d t,
which is this low. Faraday is a positive sign. Okay? You will understand
that there is a negative sign
due to Lenz's law. Okay? So here E or the
voltage are produced, or the electromotive force means the voltage are
produced inside a coil, is equal to n, which is the
number of turns of the coil. How many tones for this coin? D phi over d t is a
variation of magnetic field. So it means that if there is
no change in magnetic field, it means that there
will be no voltage. Okay? So how can we understand this? Okay, you can see here
we have a magnet. In a magnet produces
magnetic field. This magnetic field
is constant, okay? So this magnetic field, magnetic field is constant. Okay? So if we put a magnet like
this besides a coil, okay? Is there any change
in magnetic field? There is no change
in magnetic field. D phi over d t is equal to zero. So no voltage is produced at
the terminals of the coil. Why? Because the magnet itself
is at, it's a place. It is, fix it, it produce a fix-it
value of magnetic field. So the variation of magnetic
field is equal to z. So there is no voltage
between these two. However, however, if we
take this magnet and the store to moving to
the right or to the left, or move it to the right, you will find is that this coil, we will have an induced EMF. Why is this? Because the
motion of the magnetic field, or motion of the magnet
itself produces mixes, this coil sees the magnetic
field as a variable feed. So in this case, you
will find that we have a variation in magnetic field, which means that we
will have a voltage. So let's see this figure
to understand the idea. So if you look here, we have a magnet and then we
have a coil like this, a coil like this one, which have two wires, two terminals, several coils. How many donors? 1234567. So we have n, which is the number of turns
of the coil equal to seven. Now, if we keep this magnet
as it is in this position, you will find that
the voltage are produced at the two
terminals is equal to zero. There is no variation
in magnetic field. However, if you start
moving this one like this, you will see that the voltage
starts to be produced. Or if you move it like this
in the other direction, you can see a positive, then gets back
negative and so on. So you can see this motion
of the magnet itself produces a voltage
across the cohort, okay? If this magnitude is constant
or standing in its place, it will not produce any voltage. So the Faraday's law say is that when we have a
variation in magnetic field, we will have a voltage
which will be produced as this voltage will produce
an electric current. Okay? So let's see enormous
opposition here as legs, as you can see here, that when we have a
magnet like this, Okay, Let's see it. You can see when we move
the magnet like this to the left and then stand still, you will find that
the voltage is zero. When we start moving, you will find that the
current is produced because we have an
induced voltage, voltage which is produced at
the terminals of the coil. Okay, so the current is formed
only on the movement of the magnet itself because the magnetic field is changing
with respect to this coin. The magnetic field as seen by
this coil, is it changing? When we are becoming
close to the coil, the magnetic field
is increasing. More fluxes cutting is a coil. And the, when we
start going away, the amount of flux cuttings
or coil decreases. So you will see that this motion will lead to production
of magnetic, production of
electromotive force. When it is standard, still not moving, you will
find that the voltage is zero. When we start moving, we will have and induced EMF. Okay? So the idea of Faraday's law is that when we have
three elements, three elements, number one, when we have a magnetic fields, when we have a
mechanical motion, mechanical motion we are moving left and right, left and right. So we have motion. When we have a wire which
will take the output current. When we have this
three elements, we can generate electricity. What we can do is that we can take an electric generator is, electric generator is formed
of a rotor and stator. The rotor is rotating part. So when we add a
magnet on the router and this rotor is rotating
due to mechanical force. You will find that we will
have a varying magnetic field, or a d phi over d t. And the stator is the one which will take the output voltage. We will see this in the
synchronous generators and induction generators. Okay? So what about Lenz's Law? Lenz's Law is pretty,
pretty simple. You will find that, that
Lindsay Law states that when a changing magnetic field produces or induces a current
in a conducting required. So what is the value
of this current over? What is the direction
of this current? Or why do we have a current? We have a current because
this current will produce a magnetic field that opposes
the induced magnetic field. But it's simply the induce, the current opposes the
changing magnetic field, which is producing it, as shown in the figure
we will see here. So as you can see, we have
a magnet like this. Okay? Let's say it is in this
position, North and South. So we have some flux
lines here like this. Let's say it is reaching
here until here. Okay? So let's say it is a standstill. So there will be no voltage here because
there is no motion. Now, let's assume
that we are moving from here to war this coin. What will happen is
that if this magnet from this position
becomes in this position, this position you will see
that it cuts more of the coin. More magnetic flux
will cut the coin. Okay? This motion will produce
a varying d phi over DT, or a variation in magnetic flux, which will lead to
production of voltage. Okay? So what do you think is
phi or the amount of magnetic flux see him by the coil increasing
or decreasing. Actually it is
increasing because we are going close to this coin. So coming close, it means a
more flux will cut this coin. So what does a solution now, I would like to produce a magnetic field that
opposes this effect. So you can see magnetic field
is increasing like this. We are coming close. So the magnetic field is affecting more and
more zach coin. So the current will be
produced the like this. Okay, So we will find
that the current flowing like this, like this. Okay? So we'll find that
when we use are all called Zap Fleming
right-hand rule, you will find that this coil, due to the presence of
a currently exists. It will produce a magnetic
field in this direction, like this, north and south. So when does current
flow is like this? It will produce North and South. Why is this? Because we
have here north and south. North here means
that it will pose, it pushes this one away, stay away from me. Okay? Now it's the same
idea for this one. You see here we have
north and south. Now if we have some flux
cutting here like this. Now when this one moves in the other direction like
this, you will find that e.g. it becomes in this position. So find that in
this case you will find that it will cut like this. It will just the cost, e.g. here and here and here. The magnetic field
seen by this coin is much lower, much lower. So what will happen is
that a current will be produced like this. Like this by exist, I exist. Okay? According to the Fleming's
right-hand rule, you will find that this one will produce a magnetic flux
in this direction, like this, North and South. So what will happen
is that we have this mega which is
north and south. So this sounds will try
to attract the snow, so it will oppose the effect. It will just try to get it
back to its original position. So in the end, zach currently produced or
the voltage produced in other direction produces
a magnetic field in a direction that
opposes the change. If this one tries to get closer and increases the
magnetic field, the current will produce a magnetic field that
opposes this effect. Stay away from me. If this one stays away and
go away from the coil, the current will be produced
here to attract it, please come back so it will produce a magnetic
field in this direction to attract this magnet back
again to its position. Okay? So Windsor North of the pole of the magnet
in the figure above moves closer to or
farther from the rope. And EMF will be produced to
produce a current that will produce a magnetic field that opposes the changing magnetic
field from the magnet. So here you can see this is
the ID, exactly what happens. So here, when this one starts to
come and get close to it, you will see that a
current will be produced. The current will be produced another direction which will
produce north and south. So if you have a current in this direction and this
direction like this, okay? So we will have like this, okay? So the magnetic field
will be like this. And we will have
north and south. You can see when this one
twice to come closer, a current will be
produced the legs this. Why is this? Because you
will see that the current Like this, like this, moving down, down, down. Which means that according to
Fleming's right-hand rule, the magnetic field will
be in this direction. Of course, if you
don't know about Fleming's right-hand
rule or all of this. You can get back to our goals of electrical machines, okay, in which we discussed
in more details about magnetic flux and
the magnetic circuits. So we have North and South, and this one is north and south. So as you can see,
when this one tries to come closer to the coil, the current will be produced, will produce a magnetic
field north and south, which opposes this magnet. When it starts
going away from it, it will start reversing
its direction to produce a magnetic field that will have as house and tunnels here, so it will attract this one. Please come back. So as you can see,
when it comes closer, it produces a repulsion force. When it goes away, it produced an
attraction force because it wants it to be in
its own position, is the original position. Here is an example of the
Fleming's right-hand rule. So as you can see here,
here we have our code. Let's say it's a current
going like this. Not like this. Let me have it in
the other direction. We have positive here. So let's say the
current is like this, going down like this, like this. So if you put your
hand like this, you can see in the
direction of the current, this hand is in the same direction of
the current law exists. So we'll find that this, some of your own hand will produce the direction
of magnetic field, which is in this direction. So this is the
direction of current. This is the direction
of magnetic fields. So the current up magnetic field on the right or the nodes, since it's the magnetic
field that exists. So we have North and South. So by using this Fleming
right-hand rule, you can apply it here to find the direction of
the magnetic field. Here is more about eight. You can see we have a coil according to the direction
of motion. This will happen. So you can see we have,
this magnet is moving. So we have moving towards it. So it will produce a
current that will produce a magnetic field that
will oppose this motion. So e.g. in this one, it is moving like this, so it will produce north and
south to oppose the effect, to tell it to go away. Here if the magnet is
moving away. The same idea. This will produce North and
South in order to attract it. Come back. Please come back here
for this example, it's the same idea if we
have North and South. But this one is the one which is moving the coil
is the one which moves. This one is a stationary. So since this one is moving, it is also seeing this
magnetic field as varying. Toilet try to attract it. So it will produce
north and south to lead this one come to me. Okay? Same idea. If it is moving like this, it will produce also South and the North
to attract this one. Okay? So in the end, it
will try to keep the magnetic field
is same as before. So what we learn from this, or what is the purpose
of all of this, you will understand
that in order to generate electricity
in magnetic field, generate electricity in
electrical machines, we need three elements. One, we need a mechanical
force or motion. Number two, we need
a magnetic field. Number three, we need
a wire that will carry the output current or the wires that will have
an induced voltage. So you can see here
we have this magnet, which contains magnetic field, and it is moving left and right. So we have a mechanical force. Then we need the wires, the wires which will carry the output voltage
or output current. Okay? So we have three
elements that you will always find in every
electrical machine. Okay, so let's go to the next lesson and start
understanding the forest, the type which is a
synchronous generators. By understanding the
synchronous generators, you will be able to find
disease three elements. You will find the
mechanical force, magnetic field, and the wires. Okay?
4. Synchronous Generator Working Principle and its Types: Hey everyone. In this lesson we
will talk about with the first type of generators, which is a synchronous generate. The same idea as before. We said we need three elements. We need forest and
magnetic field. We need mechanical motion, and we need a wire that will carry the output
electrical power. So how does the synchronous
generator looks like? It is something like this. So the first element that we have is that we have
a magnetic field. And magnetic field which will be formed using field winding. We add, we connect it to a DC supply that will
provide current to a field, and this field will
produce magnetic field. Okay? So this is a forest. My second semester
is that we will have magnetic poles on
the rotor itself, the part which is rotating. So first, we have here
now and magnetic field. Second element, we need mechanical force or
mechanical motion. So we have a rotating part here, which is magnetic field, and it is rotating. How it is rotating, it says connected to a shaft or connected
to a prime mover, such as diesel generator
or a hydropower plant, which rotates atropine
and electrical turbine. And this turbine,
when it rotates, it will produce this
form of rotation. So rotation of this machine is due to the rotation
of the prime mover, which is due to the Zao
prime mover itself. So now we have a
mechanical force. So this is a magnetic field
and the mechanical force, the Soviet government, we need wires that will carry
the output power. Will find that we have
another component here, which is called the state
or state or because it is in fix it, it is not moving at all. So this part is called
stator, rotating part, called rule to the
state or has windings. You can see one and 2.3 winding. Each of these winding
represent the phase, phase a, phase b, and phase c. They are 120 degrees. You can see mechanically the
angle between here and here, hundred and 20 degrees. Between here and here, hundred and 20 degrees. And then between here
and here, 120 degrees. So finds that due
to this rotation, each, each of these coils see
different magnetic fields. Sometimes they find
the phone dissolve. They get the highest value. Also times he gets the lowest
value of zero times zero. So this is corresponding to a
three-phase voltage output. Due to the rotation of
the magnetic field. You will find that we
have three phase shifted from each other by 120 degrees. This waveform is the waveform which we have in our
electrical power system. Our electrical power system is operating on a three
phase voltage. And the three-phase voltage is, three voltages have
the same value but shifted from each
other by 120 degrees. Again, if you don't know about three-phase system or the magnitude and phase shift, you need to go to our course
for electric circuits. So here's the same idea. Can see we have a rotating
part which is rotating due to the hydro-power plant or
due to diesel generator, whatever it is, it is
causing a mechanical motion. This mechanical motion. And do we have here a
magnetic field on it? This rotation of
the magnetic field will produce a d phi over d t, which will lead to
induce the math on that state or itself on
the coils of the state. You will see that due
to this rotation, each one will have a
different magnitude according to the
position of this root. Okay? So here's the same idea. We have three equals a, b, c shifted from each
other by 120 degrees. So if you don't know how
you can see it likes us. Let's say here exists. We have phase a and
phase C like this. And FASB is like this. If you look at this positions, it is something like this. So you can see that
between here and here, 120 degrees between
here and here, hundred and 20 degrees
between here and here, hundred and 20 degrees. So what we can learn from this, we can learn is that the
three voltages are shifted from each other mechanically
by 120 degrees. And this led to what? Led to a voltage. The three phase
voltages are shifted from each other by 120 degrees. Okay? So this representing our
synchronous generator, we have the stator, which has a three-phase winding, which is a three-phase
output of the system. You can see
three-phase like this. You can see here we have the
rotor which is rotating. We have two poles, e.g. it can be more than two poles. And how can we generate
magnetic fields simply, we add a coil around it and
we connect it to a DC supply. This DC supply, or DC voltage
provides a current goal, the field, the current. This field, the current will
produce magnetic fields. So when the current
goes like this, goes like this or in
the other direction, it will produce magnetic fields. Of course, we have
discuss this in our course for
electrical machines. So if you don't know about
this or you don't have any knowledge about
electrical machines, you can go through this course. Okay? So we have this a and b and c shifted from each
other by 120 degrees. As you can see, that system, we have the field winding, which will produce
a magnetic field supplied with a DC current, which gives us the excitation or the magnetic field required. So we said the first element, we need magnetic field. How did we obtain this? By connecting this
rotating part to add DC supply to produce
a fix-it magnetic field. Then is our root will
field is rotated by an external chuffed adds
a synchronous speed. The rotor itself, as this one, is rotating by an
external shaft. This external shaft
is connected to a prime mover, such as diesel. Working by diesel or
working by hydro. Or waterfall energy. At what is the speed at
which it is rotating? Speed at which it is rotating
is a synchronous suite. All we say n s, you will understand what does
the synchronous speed mean? That Nick has to slide the
rotating magnetic field. So we have a fixed set
magnetic field and it is rotating, rotating. This magnetic field, fixed
and magnetic fields that rotates will produce
voltages in the stator at a, B, C depending on
its opposition. Okay? Why? Because this magnetic field, when it rotates, each coil, will see the magnetic
field as it is it changing or as a
varying magnetic field. Now, what is the frequency
of the output voltage? You know that any
voltage is equal to V maximum cosine omega t plus phi, which is a phase shift. So e.g. Va is maximum voltage, maximum value cosine
omega t plus phi phase shift here is equal to zero starting from
the zero position, omega t Omega is the
angular frequency. Omega is equal to two pi
multiplied by the frequency. Now, the frequency here is the frequency of the output
voltage is equal to. This frequency can
be 50 hz or 60 hz. This is the value of
the frequencies that we produce from our
electrical system. Will find that in our
electrical power system, it is operating at ease, or 50 hz or 60 hz. Okay? So we have
to make sure that the output three-phase voltage is 50 hz or second service. So how can we do this by controlling the
rule to frequency? Or to be more specific
is our role to speed. So we need to understand
what is the relation between the rotor speed and the
frequency of the output voltage? So here you will find
an important relation. You will find that N, S, or the synchronous speed. Synchronous speed is
the speed at which our rotor is rotating. Okay? So the synchronous
speed is equal to hundred and 20 F divided by P. So finding that f
is the frequency, alternating current frequency
or the AC frequency, the frequency of this signal. So what is frequency? How many cycles in 1 s? Okay? So 50 hz, this means
that our waveform will make 123 and so on, 50 of these cycles in 1 s. And the B indicates the
number of poles of the rotor, you can see here and we
have North and South. How many poles that
we have two ports. It can change from one
machine to another. So as an example, if I would like, if I would like
to produce 50 hz, let's say I would like
to produce 50 yd. So I need to control the rotating speed
of the rotor itself. So we have 120 f a over b. So let's say I selected that the output voltage
frequency is 50 hz. So I will make F equal to 50. Okay? And we see here how many poles
we have North and South. So we have two poles. So we'll make B equal to when we divide
this two together, we will have a
speed of 3,000 rpm, or say thousand revolutions,
revolutions per minute. How many revolutions in 1 min? Okay, so we need to make
this rotor rotates at a larger speed of 3,000 rpm in order to have the output
voltage equal to 50 hz. So you can see now that
that rotor speed effect as the frequency of
the output voltage. Okay? So this will lead to two types
of synchronous generators. The first one which is
called as salient generator, and the other types called
xenon salient generate. So you can see here
that two types, what are the differences
between them? The difference in
the router itself. So we'll find that that state or in both types is the same. Nothing has changed
in the state. However, if you look
at Zap Router itself, you will find that it, e.g. in the salient pole, you will find that it
consisting of large pools. You can see all of moles, pool of South Pole of
North pole of cells. So large pools. However, if you look at the
MSA consisting of slots, this load, so we add
our wiring like this. We connect the wires here so we can produce magnetic flux, unlike this one which
consisting of foods. Okay? So here's another image
you can see this is as salient pole and this
one is unknown CDN. So we add wiring here
so we can produce magnetic fields
directly like this. So we have north and
south, north and south. You can see it like this. Okay? We have North and South. However, this one, we can have
multiple north and south. We can have many nodes and diminished house
as we would like. You can see that this phi, which is a sealant,
is looked like this. You can see large pool of nodes, large pool of sours, large magnets, several magnets. Or we can have a
pole and we can add a wire here so we
can produce flux, okay, as we would like. So that's the difference
between these two types. Now, the most important
thing is that when do we use the salient and when
do we use among CBN. So we have the salient
here you can see two, another two images for the
sealant, unknown cilia. The cilia and as you can see, consisting of large
number of bolts that non salient and sometimes we
call it cylindrical root. Okay? You can see that this one is having large number of poles. This one has very
low number of poles. So if you look at the
synchronous speed, the speed at which this
rule tool will rotate. Hundred and 20 F over B. Let's say e.g. I. Need an
output frequency of 50 hz. Okay? Now, e.g. if you look
at the sealant that we have very large number of poles. So very large number of poles, it means that we
have very low speed. So you can see the
salient to have a low speed or has a low speed. If you look at the cylindrical, you can see North
and South poles or very low number of pores. So very low number of poles means that we will
have very large speed. So you can see
cylindrical rotor or the amount salient
having high speed. Okay? So what we can learn from
this week alone is that salient has larger
number of poles, which is corresponding
to very low speed. That cylindrical has
low number of poles, which is corresponding
to a very high speed. So this one has applications and this one has other applications. So the salient pole or the synchronous cilium to
pour root or generator. We use it in that
diesel generators and we use it in the
hydro power plants. So when we, when we talk about z is x and we talk about
the hydropower plants, we understand that the type of generate reused is as
in Crohn's generate. Okay? Unlike this type which
is a cylindrical water, when we talk about
steam generators, we use the cylindrical rotor or the synchronous generator
with a cylindrical. Okay, so I hope you now understand the
difference between them. High number of poles, low-speed, low number of bolts leads
to high-speed. Okay? So in this lesson, we talked about with that synchronous generator
principle of operation. And we also talked about
the different targets.
5. Wound Rotor and Squirrel Cage Induction Machines: Hi and welcome everyone
to this lesson in our course for generation. In this part, we are
going to talk about the induction machines and different types of
induction machines. So what is an induction machine? Induction machine is similar
to a synchronous machine. But the difference
is that it has zero auto is different from
the synchronous machine. Will find that as a
synchronous machine has two main types. First one is called the wound
rotor induction machine, and second type is called the squirrel cage induction machine. So the first type is a wound
rotor induction machine. So if you look at this system, you will find that we have the wound rotor
induction machine or induction generator
to be more specific. Here we have this part, which is our router, the router or the rotating part. And do we have here, this part is our estate. So similar to the
synchronous machine is estate or has a
three-phase winding, a, B, and C, which are all connected
to the power grid. Okay? Now we will find that as our router itself
or the rotating part is not like the
synchronous machine, consisting of three
phase winding two. So it has three phase winding. Now, this three-phase winding
are usually short circuit with each ours have a short
circuit between each other. Or sometimes we can add a
resistance to each branch, then we make a short circuit. Now what is the function
of this resistor? If you have seen my own
course for induction machine, you will learn is that
the rotor resistance here controls the speed
of the generator itself. Okay? So we can control the speed of the generator by controlling
the value of the resistance. And at the same time, it has our problem is that
it causes power losses. You will see some. So we
have resistance here, all resistors here, we
have a power losses, okay? Okay, You can see that the
router itself is connected to the generator or
the turbine itself. You can see as an example. As an example, the induction
machine is used in the application which
has variable speed. As an example, we have this when the turbine is this when
the turbine rotates, depending on the
velocity of wind. Now when this one rotates, we have here our router
which will rotate. And at the same time
we have our state. So when this one rotates and this one produces
magnetic field, we will be able to generate electrical power,
as we will see. So here is this type which
is called wound rotor. We can see it as a wound rotor. As you can see, it is wounded
router or wanted windings. This figure and this
figure representing the rotor of this
induction machine. You can see that we
have the three phases. We have a, b, and c inside the rotor itself. Now, what we are
going to do is that we do a short circuit on them. So you can see that this part
is rotating all the time. And we have, inside
this winding, we have a and B and C, we have three phase winding, a, B, and C, which are rotating
because the whole time. And I would like to make a
short circuit with Zoom, or I would like to
connect them to a variable resistor
to control the speed. In order to do this, we use slip rings. You can see we have rings here. You can see we have slip rings. And we have here process made of carbon in order to
connect them together. Okay? So when this part is rotating, this part is constant. And at the same time you
can see it's connected to a resistor and all of them
are short circuit with EHRs. So you can see here we have
the water itself can be represented by a three
phase ABC for Xarelto. And we have the slip
ring, which is the spot. Okay. Is this report is 12.3 and then we have
the process 12.3. As you can see here, 12.3. Usually we make a short circuit inside our induction machine. So we can, after taking
all of these branches, we will make a short
circuit like this. Other times if I would
like to control the speed, then I'm going to add
variable resistor here, so I can add a resistor here, another resistor here,
another one here. Okay, Now, the same figure
for this part in real life, you can see here
the rotor itself, which is connected
to the gearbox, so it keeps rotating depending
on the velocity of wind. And we have 12.3 the slip rings, each of these rings is
connected to one phase, this one to a, b, and c. And this process will be formed with a short circuit
between them, as you can see here. Okay, So here we discussed
the construction itself. In the next slide, we will talk about how
does this machine works. So here, here's an equivalent
circuit for the system. So we have stator
and we have root. We have a three-phase
of the state are 12 and 3abcabc and D we
have false or water, a, B, C. Okay. And this router is
short-circuits with each other using the slip rings as
we discussed before. Okay? Now what happens
exactly in this system? So if you remember, we said we need
three components. We need number one, that mechanical force or
the rotational force. The mechanical force is
coming from the wind turbine. Wind turbine provide
the z rotation or the mechanical
force to the rotor. Second part which we
need, we need wires. Wires to carry the output power. So we have the stator which
will provide the electrical current or the power to the
power system or the grid. Now the third component which we need is
the magnetic field. Okay? So the question is, where's the magnetic field? You can see that the rotor itself is a three-phase winding. So where is the magnetic field? There is no magnetic field here. Okay? So how can I excite this machine or
provide magnetic fields? So here comes the idea. So first, we are connecting this machine
tools, a power grid. Okay? Now this, in order for this
machine to start talking, it will absorb Q2 from the grid, Q, or reactive power. Now why is this in order to provide the excitation
of the machine. So it absorbs,
adds the beginning q naught active power about
Q or R reactive power. So it absorbed this
current from the grid. So we have a three-phase
balanced set current shifted by 120 degrees, IA IB IC, or IE IB IC shifted from each
other by 120 degrees. So we have a three-phase
balanced supply coming from the grid. These currents are
equivalent to Q, or the active power
absorbed bit from the grid. Then what happens is that this three-phase current
supply current sensors, they are three-phase current,
three-phase currents. And at the same time the
audit changing with time. So this three-phase current will produce a rotating
magnetic field, similar to the magnetic field. If you remember, we have
a magnetic field in the synchronous generator
inside the rotor, we had a magnetic field
and it was rotating, rotating at the speed of
the synchronous speed. That rotating magnetic field to produce the from the
synchronous machine. As similar to that
obtained from here. The three-phase
current, which are varying Goldstein will produce a magnetic field
similar to the one of the router inside the
synchronous machine. So what will happen is that, that rotating the
magnetic field produced from this three-phase when cut. So we have a magnetic field
going through the machine, through the air gap between
the stator and rotor, going to the router itself. So what will happen is that this rotating magnetic
field will cut that three-phase winding of
zero to sows are rotating. Magnetic field weld
cuts the router causing as three-phase current. So we will vision, we will generate IA, IB, IC. Remember we have
a magnetic field, the calming going
to lose our router. So it will produce a
voltage here, voltage here, voltage voltage here, and
voltage here like this. So we have IA, IB, IC since we are short
circuit, remember, wish we made a short circuit
so we can produce currents. Now, this current,
what will happen when we have
three-phase current? This three-phase current will produce another magnetic field, another rotating magnetic field. So we have a three-phase are rotating magnetic field here. As a rotating
magnetic field here, then the interaction between these two magnetic fields will lead to
production of torque, okay, will lead to
production of torque. So our router will
start rotating. Remember this is Austin zoster. Remember this point that the
rotor will start rotating. Despite having a, when
the turbine that rotates. We will understand how
can we differentiate between a motor and generator. Okay, So we are
talking here about the principle of operation
of the induction motor. Neglect as a presence of a
wind turbine and assumes that we connected here
in the mechanical route. But before we discuss how does induction machine
operates in there? Generation mode, we
will discuss first is the other type of
induction machines, which is a squirrel cage. You often know that's
a wound rotor and the squirrel cage operate
with the same principle. So here we have
the squirrel cage. If you look at the
router itself, you will find that it is in
the form of a squirrel cage, a cage of the square root. Like here. The phase three phase of
the state or ends or water itself is in the form
of squirrel cage. Okay? So we'll find that the rotor, which is used in the squirrel
cage induction motor or the induction generator is
known as squirrel cage rotor. The squirrel cage
rotor consisting of a cylindrical laminated core. So it is format of lamination. The core itself,
you can see it is cylindrical and format
of laminations. Having slots for carrying,
conducting parts. You will find that
here the squirrel cage is formed of one. To all of these are
conducting paths. Like here. All of these bars are
conducting polls. And do we have here slots so we can insert this conductors. Now, this conductors are made of aluminum or made of copper. You'll find that all of these
pores are zoned together at each end by a large shorting
rings known as end rings. So you can see here
we have a large ring here and our lungs
are larger in here. You can see that both of them are short circuit
with each ours. Okay? So what does this mean? How can we see is, as
you can see the slides, as you can see, we have a bar, bar, bar like this, which is this conductors, and it's a short-circuit
by two rings. Okay? Now, since there's a rotor
part of the squirrel cage is permanently short
circuit by n drinks. Hence, it is not possible to add any, any external resistance. We can not add any
external resistor. So as you can see if you
remember in the wound rotor, which I have discussed before, we said that we have, we had a three-phase
winding like this. And we get back to
understand this idea here. If you'll get back here, you will see that here
for the wound rotor here, we had a, B, C, and D. We had brushes, which will make a
contact between this ring and the
short-circuit here. So in this pulse, I can add any resistor
in external resistor. Okay? However, if you look
at this one here, you will find that I
cannot add any resistor. I don't have any
access to that cage itself, as you can see here. So that's why it is
not impossible to add an external resistance in order to have a large starting torque. You have to know
that from the CEO of induction machines or from the lessons of
induction machines, we said before that
in order to have a lower starting torque for
the electrical machine, one of the methods is that we can add an external resistor. So by changing that resistor, we can increase the starting
torque of the machine. However, since we
don't have any access to this cage and I cannot
add any resistance. This squirrel cage
does not have any, does not have a large
starting torque. Your funds at the
core of the rotor, why it is made of laminations and you'll find this in lots of electrical machines in order to reduce the eddy current
and hysteresis losses. So how does it work? The same idea when a
balanced three-phase supply is fed to the stator winding. So we add as three-phase
balanced supply to it. This will produce a
rotating flux or rotating magnetic field with a constant
in magnitude and speed. It is beat and the
magnitude, of course, dependent on the
frequency of the system, pays a frequency
which is 50 or 60 hz. The rotating magnetic field will pass through the air gap. And the coaches are
rotor conductors. Rotor conductor parts
which are stationary. This is similar to the
rotating magnetic field, which is coming from the
state or in the wound rotor. And the cutting
is a three-phase. So you can see that they have the same ID are rotating
magnetic field. The cutting is a root. So this will lead to an induced EMF or voltage
in this conductors, leading again to presence of a current and the production of
another magnetic field. This magnetic field of the state or the interaction between
these two magnetic fields, will lead to the
rotation of the rotor. Okay? So again, squirrel cage, we add three-phase supply, which will produce a
rotating magnetic field. This rotating magnetic
field cuts or auto, leading to currents. These currents will cause a rotating magnetic field
and the interaction between these two fields will lead to rotation
of the root. Same idea in the
three-phase wound rotor, three-phase current lead to
a rotating magnetic field. Cuttings or auto, lending to three-phase current leading
to rotating magnetic field. And again, the interaction
will lead to a torque. Okay? So this is a principle
of operation of what? Of the induction motor. Now the question is, how can I generate
electrical power? How can I generate electrical power in
the squirrel cage or inside the induction as a
one rotor induction machine. So the idea is pretty,
pretty simple. You will find that for
the induction machine, we have this curve which consisting of a
torque and the speed of the generator will
find that from speed of zero up to the
synchronous speed. So if you remember the n asynchronous is
equal to 120 f over a b. F is the frequency which we
are alternating current. So if you remember, we supply three-phase
current from the grid. This grid have a
frequency of 50 hz. And the number of poles here, representing number of poles
of the state are not zeros. Now why is this? Because the source of the magnetic field is
coming from the state. Okay? So the number of poles
will be for the state. Let's say we have a two
poles on the state, so that synchronous
speed is 3,000 rpm. Okay, remember this.
So we have a 50, 50 hz supply and the synchronous speed equivalent
to this is 3,000 rpm. Okay? Now, so we have here that curve from zero to the same constant
speed, which is e.g. 3,000 rpm, which is what? Here we are talking about
torque and speed of what? The router itself, the rotor of the induction generator or the induction
machine in general. Now, if the speed of this road, the speed of this route, is what is between from zero to the synchronous
speed in this range. So when n or the speed of the rotor is less than
the synchronous speed. You will find that our machine
is operating as a motor. You can see that the
torque here is positive, which means it consumes
electrical power or provide this
mechanical power. It is converting the electrical power
into mechanical power. Now, if you look at
this curve, wins as b, it becomes great or Zan, or beyond the synchronous
speed in this region, Windsor speed become higher
than the synchronous speed. You will find that the torque
produced by the generator is negative. What
does this mean? It means that our
generator is over. Our induction machine
is working as a generator, providing
electrical power. So in the end, what determines if
the induction machine is a generator or motor? Speed of the generator itself, or the speed of the
induction machine. If this bit is less than
the synchronous speed, it will be motor. If the speed is greater
than the synchronous speed, it will be generate. Okay. That's why if you look
here at this curve, let's say Get back here. If you look here at this
system for the wound rotor, it is connected to a wind
turbine that rotates. So when does this one
operates as a generator? Note motor operates at
a generator wins as bead of water is greater
than the synchronous speed. So how can we achieve this? We achieve this
using the gear box. So we have a low speed of wind. When we connect
this to a gearbox, it will produce a
very large speed, will make this one rotates at a very largest speed beyond
the synchronous speed. So in this case, you will find that
our machine will start to providing electrical
power to the grid. As this is the same idea
in the squirrel cage. Nothing changes
except that the shape of the rotor or the shape
of the rotating part. Okay? Okay, So now you will
find another concept here which is called the
slip, slip of generate. The slope is equal to n synchronous
synchronous speed and S minus a mechanical speed, mechanical speed here is the en route are also
rotational speed of the water divided by
the synchronous speed. Okay? Now why slip is important? Because in induction machine
we use a slip or a lot. In the equations of
induction machines. You will find also
a relation between the frequency of the
current and the slip. You will find that the
frequency of the current, rotor current is equal to Fs, which is a slope multiplied
by the supply frequency, let's say 50 hz. So it will be 50 yd
multiplied by S, which is 3,000 minus the
speed of the rotor divided by the synchronous speed sensor. We have learned that we need to increase the speed beyond
the synchronous speed. Let's see how it will
work as a generator. So again, if the router
is accelerated to the synchronous speed by a
prime mover, let's say e.g. that when the turbine the slip or dizzy and the
torque will be zero. If you get back here, you will find that when the synchronous speed
equal to the rotor speed, the slip will be equal to zero. If you look at this graph, is that when the speed is equal to the same
chromosome speed, torque produced
is equal to zero. Now why is this? Because rotating magnetic field and the rotor itself are
rotating at the same speed, which is the synchronous speed. So that magnetic field
widths respect to the rotor. There is no relative speed, Zr as if it is constant
with respect to it. Okay? So if you have this
one rotating at synchronous speed
ns zero to itself. And the magnetic
field rotates at what is speed at the
synchronous speed. So if you have
something rotating at a certain speed and another object rotating
at the same speed, the relative speed between
them will be equal to zero or as if it is a standard style, it is standing in its place. Okay? So in this case, d phi over d t is a
variation in flux will be equal to zero and the motor
torque will be produced. Okay? So the rotor
current will become zero when the rotor is
rotating at synchronous speed. Now when we start
accelerating at a speed more than the
synchronous speed, the slip will become negative
in the synchronous minus n over n asynchronous
will be a negative value. So we'll find that
the rotor current itself will be generated
in the opposite direction because it's a speed
became now higher than the synchronous speed due to the rotor conductors cutting
the stator magnetic field. Okay? So now we have two
magnetic fields, one which is in the state are
and one inside the rotor. The rotor is for me due
to their status itself. Now, when the rotor
itself is rotating at a speed beyond this
as synchronous speed, the magnetic field itself, all start of the
rotor will start the cutting against the
state or magnetic field, which will lead to an induced
the voltage on the stator, which will lead to generation
of electrical power. Generated rotor current will produce a rotating magnetic
field in the rotor, which pushes or forces in opposite way onto
the state or field. This course is an induced the
voltage on the stator here, on the stator itself, which will push a
current flowing out of the stator winding and
guinness is applied voltage. So remember that we have a
voltage coming from the grid. And the wins, this one rotates at a speed higher than
the synchronous speed. It will produce
another voltage here, which is higher than the grid. So it will push power
tools is a great. Okay, So in this case, it is working as an
induction generator, or sometimes we call it
as synchronous generator. Okay? So why does a synchronous
machine called a synchronous machine
because it is rotating at synchronous speed. Now why does induction machine called the asynchronous
generator? Because it is not rotating
at the synchronous speed. It is rotating at
different speeds. Okay? This is beat depends on the
speed of the wind itself. Okay? So what is the problem
of induction machine? If you listen carefully
to what I said, you will find that
the first problem, it does not self-excite it. So it requires the queue from the grid to provide
excitation for zero. It does not have
excitation inside it. So that is the first problem, so we need to solve it. Therefore, when running
as a generator, the machines will take
reactive power required for excitation and installed
the supplying active power back into the line. So when this one rotates at a speed higher than
the synchronous speed, it will start giving electrical
power or active power. So we need reactive power for producing the rotating
magnetic field. Unlike the synchronous machine, which had permanent magnet
or had the balls inside it, which will produce
a magnetic field. However, here, we need to absorb the queue in order to produce that acquire the magnetic field. Zack, the power supplied
back in that grid is proportional to the slip
above the synchronous speed. So the higher the
synchronous means, the more power we are going
to give back to the grid. So in this lesson, we discussed the principle of operation
of induction machine, types of induction machines, and how can we make our induction
machine as a generator? Now what is the next lessons? We will talk about power
with how can we make our machine, sulfur
excited machine. And we'll talk also about what's WT fit induction machine.
6. Doubly Fed Induction Generator: Hey everyone, In this lesson, we are going to talk about what WE fed induction generator. So in the previous lesson, we discussed the wound
rotor induction generator. We discussed this squirrel
cage induction generator. Now we have a double effect
induction generator. Now what does our lovely
fit induction generator? If you remember, if you remember from
the previous lesson, we said that for any
induction generator we have a stator,
which is this part. And then we have
the rule itself. Okay? We said that the stator
is a three-phase system. A three phase system, as you can see, 12.3
connected to the grid. So the stator connection
is to the grid. Now, if we talk about
with the router itself, we said before it is
also as three-phase. Okay? Like this. And we said it is
short circuit using slip rings and brushes, right? So you can see that
they'll double if it induction generator
is also at wound rotor. It is format of a three-phase. You can see 12.3. But instead of making a short circuit on
this three-phase, we connect them into a
back-to-back converter, which is connected to the grid. So as you can see that now the induction generator is supplied or connected to
the grid from two sides. It's connected from the grid, from the stator side. And it's also connected to the grid from the root or site. However, the rotor is
connected to the grid using a back-to-back Converters. That's why it's called double effect induction
generator because it is fed from the stator
and fed from the root. Okay? So it's connected
from two sides. Okay? So now let's discuss
how does this type of generators work and
why do we use it. So in order to connect that, WE FIT induction generator
to the electrical grid, there is a back-to-back
converter. You can see here is a back-to-back
converter or this one. This image is
similar to this one. So the converter is
formed of two voltages. Source converters link it
through a common DC circuit. You will find that the voltage
source control converter as a volt source converter is connected to the
rotor terminals, is called Zap Router
side converter. And the one which is connected
to the transformer or the grid is called as
a grid side convert. So if you look at here, we have two converters. We have between them. We can add here a
DC link like this. As you can see here. That DC link is the
one which link is between this converter
and this converter. So what happens exactly? You can see we have here grid, which is a scene. So we have a converter which
converts from AC to DC, takes at ASU of the system and converts it
into DC, DC link. Then we have another
converter that takes DC. And the converse is to
AAC require the forest as three-phase root or the
three-phase of the road. The same process can happen
in the reverse direction. We can have a three-phase
current coming from the induction generator router. Then we convert AC to DC, owns a DC link. Then from that DC, we can convert AC and supply electrical
power to the grid. So it is bi-directional. It can provide power and Q, or absorbed per power and
the q from the grid due to the presence of the back-to-back
converter with a DC link. Now, as you can see here, we have our C, which is a router
side converter, and the GSC, which is the grid side converter or auto side because it is
close to the router. You can see this is our router. And this is a converter which
is close to the router. That's why we call it
the auto side converter. If you look at the
other one here, it's called dread side converter because it's
close to the grid. You can see we have here a filter and we have
here our transformer. And this transformer
is connected to its connected
here to the grid. This transformer
is used to step up the voltage for connection
to the electrical grid. Okay? Okay, is this depends of course, on the generation voltage of this converter or the output
voltage of this converter. So what is the function
of these two converters? Why do we need them? Why do we add this converters? Because the converter, or SSE, which is a router
side converter, this converter is
responsible for. Controlling the reactive
power exchange with the grid. And the variable is speed of the rotor that determines
the active power flow. So it is use the tool, this one is used to control
the reactive power Q, which is exchanged
with the grid. And since we, if we remember before that we said we need q or reactive power in order
to magnetize our row two. So instead of taking from stator and producing a rotating
magnetic field, that will cut the router to produce the three
phase voltages. And since I'm rotating
magnetic field, we take Q directly from the grid using this
two converters. Okay? So the first converter, which is a root
of psi converter, is concerned with the
active power exchange. That is the first function. Second function is
that it is used to control the
speed of the road. Now, if you join my uncle's
for when the energy, you will have learned
that the converter here, when we control the cannons
inside the router itself, we can, we can control
the speed of the root. So by controlling the
speed of the rotor, we can control the act of power output from
the machine itself. Okay? So you have to understand that
in wind energy in general, when we have a wind turbine
at a certain speed of wind, the velocity of air
or velocity of wind. At each velocity of wind. As zeta is, one, optimum is speed of the rotor that will produce
maximum power, okay? For each wind speed, we have one is B that is required to produce
the maximum power. Okay? So we have tables and then we have graphs
that will help us to determine what is the value
of the speed that we need. Okay? So let's say V1 is e.g. two meter per second or five meter per second
or whatever it is, there is a corresponding
speed of the rotor, let's say 500 RPM as an example. Okay? So in order to achieve
this optimum is speed, we have to control the output currents
from this converter. Okay? So we control in general, in order to achieve
these two functions of the reactive power and speed, we do a vector control over, we control the id and the IQ
of the three-phase current. The three-phase
current of the router. Idea, unlike you are the direct access current and the quadrature axis current,
these two elements. So when we control them, we will be able to control the reactor power exchange
and the variable speed or the speed of the
generator itself in order to reach
the maximum power. A second converter here, which has seen it is
responsible for keeping that DC voltage constant and at the same time can keep
the voltage output here from the converter
similar to the grid, or to be more specific, synchronize with the grid. So we can say is that
this converter will keep this DC link voltage at a
constant value of one per unit. Or let's say any value, let's say 51500 volt. So we keep the DC link
voltage of Pi controlling the pulses of this convert. So our second function is a synchronization
with the current. Okay, so as you can see
this two converters, one which controls speed
and reactive power as other on which controls the DC link and the
connection with the grid. You will find that this
system back-to-back converter is available a lot
in electrical power system. You'll find it e.g. in them. When the turbines, such as e.g. the squirrel cage. Also in the wave energy systems. You will also find it in the audible effect induction
generator in the state, or sometimes instead
of adding to the router a converter like this with us to add
to the state or here, the converters here, okay? And then make a
short circuit here. So there are lots, lots of co