This content provides a comprehensive introduction to the fundamental concepts of electricity, covering static electricity, electric fields, and the basics of electric circuits, including current, voltage, resistance, power, and circuit configurations. It also touches upon electrical safety measures.
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Let's get shocked, shall we?
Electricity. Now, unit four is split
into two parts. So, electricity and
magnetism. Today, we're just focusing on
electricity. And overall, this unit is
about charges. So, what's the charge? We
discussed the charge in the structure of
an atom. How like protons and neutrons
and electrons protons electrons have
positive and negative charge. We'll deal
with that again. So we split this into
static electricity portions. So what's a
charge and what's an electric field.
That's a very minor topic. Then we talk
about electric circuits. We'll start by
talking about the properties of a
circuit. So what quantities do we
measure? Voltage and current and
resistance and power and such. And then
we go into series and parallel
connections and multiple components and
so on.
Once we're done with that, we'll just
finish things up by talking about
electrical safety because, you know,
electricity can kill you and we do want
to keep you safe. At least you should
know how to keep yourself
safe. Let's start. Uh before we
continue, the same friendly reminder.
This checklist, this list of topics uh
is from the curriculum. I want you to
use this as a checklist to see if you
understand the topic or not. So for
example, if you say that state that
there are positive and negative charges
and you understand that I'm sure you do,
uh you're fine. If not, you need to
revise that topic again. Okay, let's
electricity. First, when we talk about
electricity, we have to talk about the
electric charge. A charge is a property
of matter that experiences forces near
other charges. What do I mean? This
means that all matter in the universe
has charge. Whether it's a proton,
neutron, electron, matter, me, you,
everything is charged. But there are two
different types of charges. There are
positive charges and there are negative
charges and they're
opposites. Things can either be positive
or negative or neutral. Neutral objects
are neutral because they have both
positive and negative charges
together. So they have a resultant of
zero charge.
charge is measured in a unit called
kulum. Now I want to focus on this for a
second. The charge of one proton is 1.6
10 ^ of -19 kum and the charge of one
electron is 1.610 6 10 the^ of9 kum you
don't have to memorize these please
don't okay but what I mean is each
proton or electron like subatomic
particle isn't one charge isn't one kum
of charge it's actually like a fraction
of a charge cuz later on when I mention
something like hey uh the charge is
going to split it doesn't mean that we
physically break a charge if you have
one kum you actually have millions of
tiny little particles stuck together and
yeah sure these can split and travel
0.1.0 can travel here 0.6 can travel here
here
depends. So later on when we say half an
ampere 2 aair current splits this is why
it can split. Okay.
Okay.
Now the relationship between charges is
very basic and I'm sure you know like
charges repel. So positive and positive
repel. Negative and negative repel.
Opposites attract. Positive and negative attract.
attract.
However, neutral objects can also be
attracted to charged objects whether
it's positive or negative. Why? Because
inside a neutral object, we said you
have both positive and negative
charge. And these rearrange so that the
positive is closer. So attraction is a
bit stronger. And the same thing happens
here. If you have a negatively charged
particle next to something neutral, the
positive and negative rearrange so the
positive is closer and the attraction is
stronger than the
repulsion. Regardless, anything neutral
is attracted to anything
charged. Yeah. When it comes to
materials, we have two types of
materials. Good conductors of
electricity and bad conductors of
electricity, which we also call
insulators. Conductors are good
conductors because they have freemoving
electrons. We sometimes call them
deoized electrons or free moving ions.
So it's electrons that are free to
move. You should know that all metals
are freeing electrons. So copper, iron,
aluminium, you know, constant tan,
nickel, whatever it is. Insulators do
not conduct because they do not have
free moving electrons. Somebody forgot
the letter T here when typing this sheet
aka me well do not have free moving
electrons. Uh things like rubber and
plastic and glass and wood. You should
be familiar with different types of insulators.
However, even though
insulators cannot conduct electricity,
they can be charged like you can make
them become charged by rubbing them with
another insulator. So for example, if you
you
rub a metal rod with a
cloth, a wooden cloth, for
example, a plastic rod, not a metal rod,
a plastic rod, with a wooden
cloth, the friction between the rubbing
of the cloth and the plastic rod causes
some electrons to be transferred from
one object to another. The cloth could
lose electrons and give it to the rod or
vice versa. This depends on the
materials and we're not going to study
which materials lose or
gain. But you do need to know that if an
object loses
electrons, it becomes positively
charged. If an object gains
electrons, it becomes negatively
Right? You cannot do this with
conductors by the way. And this is
something that was removed from the
syllabus in 2023. Uh how do we charge
conductors? And it's a method called
induction, but it's not part of our
curriculum anymore. Okay? So keep that
in mind. Next, what is an electric
field? Now the word field in general
means a region, a space where something
experiences a force. So electric field
is a region where charges experience a force.
force.
Okay. What is the direction of an
electric field and how do we draw it? We
draw the direction of electric field
using straight lines coming out of a
positively charged
point. So it's always out of a point. Or
if it's a sphere, it's always out of the
positively charged sphere. or if the
point is negative, it's drawn into
it. Question is why? Like why do we draw
the field lines like that? That's
because if I zoom in and I tell you,
hey, if you decide to put a positively
charged particle here, what's going to
happen to it? Gets repelled. What about
a positively charged particle here? Gets
repelled. So each of these lines shows
you the direction of the force on a
point. Which means if you put that same
positively charged
particle here next to the negative uh
point charge, it gets
attracted, right? It gets attracted.
You might say that what what about
electrons or like negative
charges? Shouldn't we draw those? Like
we don't have to. We know that positive
and negative are always opposite to each
other. So if you have an negatively
charged particle here, it'll be
attracted or here it'll be repelled.
Which means negative charges always move
Okay. So when I ask you to draw the
field lines, you always draw them going
out of a positive charge or into a
negative charge. Out of a positive or
into a
negative. Now one more feature here. The
space between the lines shows you how
strong a field is. So, if you take a
look at this field
diagram, this is the same field, but now
it's a metal sphere that's possibly
charged. Or maybe it's a plastic sphere.
We don't care. But the closer the lines
are together, the stronger the field is.
And the farther away the lines are from
each other, the weaker the field is,
which makes a lot of sense if you think
about it, because the field has to be
stronger near the charge and weaker far
away from the charge.
So if I put two charges, one here and
one here, and I ask you which one
experiences more force, like they both
get repelled, but which one experiences
more force? B experiences more force cuz
A is further away and the field here is weaker.
weaker.
Finally, if you put a positive charge in
front of a negative charge, a plate in
front of a plate, you end up with an
electric field that is equally
spaced almost at
least. This type of field is called a
uniform field. And we always draw the
field lines from positive to
negative. Right? A uniform field means
the strength of the field is constant
Now, let me draw one more diagram.
Something that sometimes shows
up, not always, but then. Imagine that
you have a positively charged sphere and
a negatively charged sphere. And I ask
you to draw the field line between them.
So, you draw lines from positive to
negative. But because they're spheres,
the field still gets weaker as you move
So out of the
positive into the
negative. So it's as if I try to join
these two fields
together. Sure you can see it now. But
the more interesting diagram is what if
I have a positive charge next to a positive
positive
charge. Sure they should repel. But they
don't just physically repel. Even the
fields repel.
other. Out of the positive, out of the
positive. Do you know what that means?
This means that if I zoom in here and I
put something perfectly in the middle
between them, it doesn't move. If I put
a positive charge exactly in the middle,
it doesn't move because this space is a
melt space. There's no field here. Zero free
free
field. Okay?
Now let's solve a couple of questions.
Figure 8.1 shows a negatively charged
metal sphere. Draw four lines. You just
want four to show its electric field and its
its
direction. Uh let me pull out this line
tool. And let's draw. While I draw, I'll
answer a question. What if I put a
negative charge exactly in the middle in
that space in that null space? Nothing
as well. Nothing
moves. You might say, "But it gets
attracted." Yeah. To which side? You don't
don't
know if it's perfectly in the
middle. Now, because this is a
negatively charged sphere, you draw the
lines going into it. Piece of
advice. If I draw a sphere, do not draw
the field lines going inside the sphere.
You should draw nothing in here.
But if this was just a negatively
charged dot, sometimes called a point
charge, and I ask you for the same
thing. Yeah, you can draw lines exactly through
through
it and it'll look exactly the
same. Okay? So, be careful. If it's a
sphere, nothing inside the sphere. If
it's a point charge, yeah, just go
fine. A plastic rod is rubbed with a
cloth. The rod and cloth becomes charged
as electrons move between them. The rod
becomes negative. Which diagram shows
how the rod becomes negatively charged
and shows the final charge on the
cloth? All right.
right.
Uh now if the rod becomes negative this
means it
has gained electrons. It has gained
electrons which means the cloth becomes
positive. So this gains
electrons and this becomes negative and
this becomes positive. So my choice is
B. Electrons move from the cloth to the
rod and this becomes negative. This
Easy. All right. I have another
question. Do we draw arrows or just Oh
yeah, absolutely. When it comes to field
lines, you must draw
arrows. Otherwise, why did we go over
explaining drawing the lines? Because
the lines show you the direction of the
force. And force is a vector. And fields
are vectors, by the way, cuz they have
direction. You have to show the
direction with
arrows. Lines going into a negative or
out of a positive if it's a positive
charge. Okay.
You mean we draw four lines or do you
need to do more? I mean, I'm sorry, but
you're given instructions. Listen to
them. He said four lines. The examiner
on. All right. Next
up, current electricity. Another giant
checklist because it's full of tiny tiny
little dots. I'm not going to read the
full checklist.
I want to go straight into current and
voltage and
resistance. Before I do, however, before
I talk about current or voltage or
resistance, let's talk about circuits in
general. The purpose of any electric
circuit like this
one is to deliver electricity. A battery
is a source of energy. It has chemical
energy inside. Or maybe this is an
electric socket. So it's just electrical
energy direct. The point is to deliver
the electrical energy from the source of
the energy that you have to my target
that needs that source. In this case, it's
it's
what? It's the light bulb. So electric
charges travel through the circuit to
give that thing energy and it leaves.
But in order to do so, there needs to be
a force acting on it. For the time
being, and I'm going to change my mind
very quickly now. I'm going to assume
that positive charges are moving inside a
a
circuit. Now, in any circuit symbol
before I move on as well, the long line
of the battery symbol is positive. The
short line is negative. All right?
So when I close a switch, a switch needs
to be closed in order for the circuit to
work. The term open means the circuit's
not going to work. The term closed means
the circuit is now going to work cuz now
it can conduct electricity.
electricity.
Now the moment I don't know why it's I
want to choose the entire thing, please.
Thank you. There we go. The moment you
close the switch, a positive charge gets
pushed out of the positive side of the
battery. zoom moves through because it
gets repelled now because it was pushed
out. It now has energy. It goes through
the light bulb which is a target which
takes the energy away because it has
resistance. It slows it down. Slows down
the charge and takes the energy away.
The charge is still positive but it
leaves without energy and goes back to
the negative side of the battery to
essentially recharge again. Get some
more energy gets pushed out and you end
up with
a sequence and you end up with a
sequence a current that
flows. So when I say what is a current
and I ask you what is a current you say
it is the rate of flow of charge or the
amount of charge that passes through a
point per unit
time. Now charge is measured or sorry
charge is measured in kum. Current is
measured in
ampere where 1
ampere means 1 kum per second. So
there's one charge that goes through the
circuit per
second. The equation that defines
electric current is I = Q / T where I is
current. Now the reason we use I for
current is because I is currently short
for electric current intensity.
So they got the I from intensity. Q is
for charge. I don't know why they chose
Q. So many things in physics use the
letter Q. And T is for time. So current
is just how many charges go through per
second. We can measure current using an
ammeter and a meters must always be
placed in series. Okay.
Now there are two types of currents that
we have in electricity. What we call DC
and AC. DC is short for direct current.
Okay? Not the comic
books. And AC is alternating current.
Well, I I like DC more than Marvel,
though. That's my personal preference,
not the movies, the
heroes. So, what do I mean by DC and AC?
DC is a current that has a fixed
direction which means the source has a
positive and negative side that are
fixed and the value of the current or
the voltage is fixed. So the current
flows from positive to negative and it
has a fixed value that's called DC. AC
however comes from a generator or your
electric sockets which initially come
from a generator in a inside a power station.
station.
The thing is the reason it's called AC
or an alternating current is because the
positive and negative sides of the
terminals are never fixed. This side
could be positive and this side could be
negative. And in the next 0.2 seconds,
so if we have like a 50 Hz AC supply,
this could be positive and this could be
negative. Which means for 0.2 seconds,
the current flows this way. Zoom. And
for the next 0.2 seconds, the current
flows this way. And then zoom and zam.
zoom and zam and backs and back and
forth back and forth back and forth.
It's very
confusing. If I plot a graph of how the
voltage or the current changes over
time, it looks like this
positive negative. The negative sign
simply means that the
direction has changed. It's in the opposite
opposite
direction. It looks like a wave sine
wave. Okay.
Now, finally, remember how I said
there's a mistake that was made back
when I described the circuit earlier? I
said a positive charge travels from the
positive side of the battery to the
negative side of the battery. Correct?
Yes. That's physically not true because
earlier in static electricity, we said
conductors are good conductors. Metals
are good conductors because they have
free moving electrons and electrons are
negatively charged.
So this thing of us saying, "Hey, the
currents flowing from positive to
hogwash." But it's stuck. Why? A very
long time ago, scientists did not know
what was free to move inside a metal.
Like they knew charges existed. They
knew they could be positive or negative,
but they didn't even know about protons
and electrons
yet. So they decided that charges need
to flow from positive to negative. Why?
Because it's easy. Come on. like
positive, negative, it's it's nice, high to
to
low. And then decades passed
by until finally some other, you know,
good scientists discovered, hey guys, uh
what's actually free to move inside a
metal is an electron, not a proton, not
a positive
charge. But all our rules in electricity
are fine. They work just
fine. So what do we do?
What we did was we stuck to the concept
of positive to negative. We just called
it the conventional current which is the
flow from positive to negative. And if
somebody asks what are the actual
particles that flow inside a circuit, we
go ahead and we you know submit and say
oh yeah we're sorry it's actually
electrons that travel from negative to
positive. But we don't call it a current
because we don't want to be confused. We
just call it the flow of electrons or electron
electron
flow. So in all of our circuits, if I
ever discuss a
current, it is always from positive to
negative. We never use negative to
positive unless I specifically ask you about
about electrons.
electrons.
Okay, that's quantity number one. Let's
go to quantity number two. Remember
circuit delivers energy. The flow of
those charges is called current. The
energy that we
deliver is called
voltage. Voltage in general simply means
the amount of energy or work done per unit
unit
voltage is the work done or energy
transferred per unit charge. Now, what
do I mean by
that? Uh, I was just changing the
battery for one of my clocks here at
home. It's a nice small, you know, Energizer
Energizer
battery. I remember a long time ago when
Energizer had these really crazy ads
Anyway, and uh it has a positive and
negative sign and written in very small
1.5V. What is this? If I tell you that a
battery has a voltage of 1.5 volts, this
means that each charge that leaves the
battery carries with it 1 and a2 jewels.
If this is one kum, it carries with it
one and a half jewels. Remember the
charge delivers energy. The charge is
not the energy
itself. This means that each and every
single charge will carry one and a half
jewels with it. This is the capacity of
the battery. This is how much it can
give each charge that goes
through. It has nothing to do with the
maximum amount of energy inside the
battery. Because I can buy another like
I have a very old radio. I like to use
it. All right. uh it gives me like nice
old vibes especially when I don't want
to use the internet. But these batteries
the battery uh the radio uses are huge a big
big
chunky almost like toss at somebody's
head and you know give them a fracture
kind of big called D
batteries or DD I don't remember but
it's also 1.5
volts. What's the difference? They will
both give the same amount of energy per charge.
charge.
The difference is how much it
lasts. So that that changes, sure, but
voltage doesn't specify that. Voltage
just tells you how much energy does each
charge take and
deliver. So when these charges go to the
light bulb, they give the light bulb 1.5 jewles
jewles
each. Okay? Yeah, there are
actually two different terms that we use
for voltage. We have emf which is short
for electromotive force and PD which is
short for potential difference. They
both mean energy per charge. But the
difference is emf is the work done or
the energy transferred by a source in
moving a unit charge around the whole
circuit. is the energy per charge of a
source because batteries give the charge
energy. Potential difference is the work
done per unit charge or the energy per
charge lost through a component because
the light bulb takes the energy away
from the charge. So that's why we need
two different names for the same
quantity because it's either energy
gained by the charge. So we give the
charges energy or we take the energy
away from the charge but they both have
the same symbol as far as we're
concerned. It's just V from now on.
Okay. Sometimes use E for emf but
regardless V is
fine. The unit of measurement is called
volt just V as well. And we measure it
using a voltmeter. A voltmeter is this
device over here. And it must always be
connected in parallel. meaning the wires
have to be placed before and after the
thing that you're trying to measure the voltage
voltage across.
across. Okay.
Okay.
Finally, back when we talked about the
charge, we said that you know this
little dinky little charge moves through
the circuit blah blah blah blah blah and
then it has to slow down. It goes
through the light bulb and that causes
it to give the light bulb energy. The
wires however are so good at conducting
electricity the charges do not lose
energy through
it. So what's the deal? The deal is in
the final property called
resistance. What do I mean by
resistance? Resistance is a property of
matter that all conductors have. They
don't it doesn't have a definition.
You're not going to define it yourself.
But know this everything has resistance.
Some materials that are really good
conductors have very low
resistance. And if the resistance is very
very
low, the current is very high, the
charges can zoom quickly. But something
like a light bulb has high
resistance, which causes the current to
what? To decrease, to move slowly. I
want you to think of resistance like
speed bumps on the road.
If a car is traveling, you know, through
a road, and forgive me, this is a
beautiful car. I know, futuristic. But
if there are speed bumps, it slows down
a bit. The more resistance a component
has, the bigger the speed bump. So, it
essentially crashes into the wall. You
lose a lot of energy to go through that
speed bump. Okay? So, more resistance,
lower current. Less resistance, higher current.
current.
The unit of measurement of resistance is called
called
ohm. And then we have Ohm's
law which is arguably the most important
equation in electricity. R= V / I or my
personal version favorite version of it
or rearrangement of it is V=
IR. All right. Memorize this. It's going
to be very important.
Yeah, when it comes to the relationship
between V and I and R, if you take a
look, I is equal to V / R, you need to
understand something. If you increase
the voltage, the current increases as
well. So if this increases, this
increases. Makes sense? Bigger battery, faster
faster
charges. If you increase or decrease,
sorry, the resistance, the current also increases.
increases.
Because less speed bumps means faster
motion or
movement. So current and resistance are
inversely proportional but current and
voltage are directly
proportional. Voltage and current right
now have no relationship because voltage
is something that you decide. I put in a
battery, a 1.5 volt battery. I decide to
put in a 10 ohm light bulb. So just me
putting in a bigger battery doesn't
change the light bulb. Both of these are
factors that you control and they affect
who the current. Keep that in mind.
Voltage and current resistance don't
affect each other at least in simple
circuits with just one component for
now. Now let's talk about resistance
again. Resistance is affected by a few
things. Temperature for one, but we'll
discuss temperature in the next section.
We're assuming that temperature is
constant. The second would be the length
of a wire and the third would be the
cross-sectional area of a wire. What do
I mean? I mean that if I have a wire of
a certain length L, let's say that's I
don't know 10 cm or so and you double
it, the resistance also
also
doubles. the resistance also doubles
because the longer the wire the
obviously the more the charges have to
go through that slow resistance. Same
thing here about with
area. If this is the cross-sectional
area of your wire, it's very small. You
think about it, it barely allows a
charge to move through. But if you have
something that's twice as large, hey, it
doesn't just let one charge through. It
can let two charges through, three
charges through like it depends on how
thick it is. So the thicker the wire is,
the larger the area, the less resistance
it has. It's inversely
proportional. The smaller the area, the
thinner the wire, the larger the
By the way, I like to write this down as
uh just just as for me when I
practice r is equal to l / a. I know it
should be proportional, but I just like
to do this so I remember that oh yeah, r
and l are directly proportional. R and a
are inverse. Yeah, a trick that is very
often used in
exams is the concept of diameter. What
do I mean?
Let's let's assume for a second here in
this example that's already been solved
that you have a wire of a
cross-sectional area A and you double
the area. What happens to the
resistance? It decreases by a factor of
two. It gets halfed. So if the
resistance was 20, now it's going to be
10 because 20 / 2 is 10. Cool.
But if I repeat the same question again
and I say, "Hey, you have a
wire of area A and diameter D and
resistance of 20
ohms." And then you double the diameter.
Not double the area, you double the
diameter. What's the value of the
resistance? It's not going to be 10.
It's going to be 5 ohms. Wait, how did I get
get
that? Remember that the area of a circle
is pir 2 or pi d^2 over
4. So when you double the diameter, so
when the diameter is doubled,
technically the area isn't
doubled. The area gets
doubled squared because you didn't
change the area directly. You changed
the radius or you changed the diameter.
And that has a square factor in
there, which means the area is not two
times larger, it's four times larger. So
the resistance is not two times smaller,
it's four times
smaller. So 20 /
4 gives you
what? 5
ohms. This is a very evil trick. Like
when an examiner wants to make a
question harder, like if they just want
to raise the difficulty a bit, they use
the word diameter instead of area. Keep
that in
mind. How do I find the resistance of
any component? I might ask you to
describe an experiment to do so. So it's
a very simple experiment. You get your
component, whatever it
is, and you connect it to a supply. Now
this could be a variable supply like the
supply itself can change or you can have
a variable resistor in there to change
the voltage or the current and you have
an emter and a voltmeter and you say oh
yeah to find resistance I need to
measure a uh sorry measure V which is
the voltage measure I which is the
current and I can calculate resistance
using R= V over I perfect measure
voltage measure current calculate the
resistance but you know what in physics
we We don't like to do things once, we
like to do things multiple times. So
what we do is we change the voltage like
I said
sometimes by changing the value of the supply
supply
itself. Changing the value of the supply
itself and
second right and second you can change
it using a variable resistor. Assume for
now that you're changing the voltage
directly like you have a set of
batteries or like a variable battery
that you can click new values into and
you start with 0 volt so you get 0
ampere you can't really calculate
anything there but at 1 volt you get
half an ampere now you get the
resistance which is two and then we
repeat the experiment several times you
change the voltage to two volts that
gives you more current you change it to
3 volts that gives you more current you
change it to four that gives you more
current and so on and you get several
values. Now why do we do this? We do
this number one so we can get an average
because it makes sure my results are
reliable and accurate and second what we
can also do is plot a
graph of current against
voltage with voltage on the x axis
because it's the primary thing I'm
changing and currents on the y axis. If
you plot these points and it's a
resistor like a fixed resistor, you
should get a nice straight line going
through the slope of this line or like
the inverse of the slope of this line
shows you what happens to the
resistance. If the slope is
constant, the
resistance is
Now I want to go over IV graphs of
different components. Meaning we we put
a component in that circuit in this
circuit that you see right now over here
over here and we change the voltage and
we get lots of readings when we plot a
graph. There are three components that
you need to remember. One the fixed
resistor which is just a component with
resistance something has fixed
resistance. If you plot an IV graph, it
ends up being a straight line. Which
Constant. All right. But if you put a
lamp like that first light bulb that we
put up there, a filament lamp, and you
start increasing the voltage, you'll
notice that the current does increase.
Like, let's zoom in a bit. Let's zoom in
a bit. You'll notice that the current
does increase.
But it doesn't stay constant for long.
It actually starts decreasing in
slope. The question is why? Why does it
like drop down, droop down? The slope
decreases. Because the higher the
voltage, the brighter the light bulb
gets. But light bulbs don't just get
brighter, they also get hotter. So the
temperature of the light bulb also increases.
increases.
If a metal heats up, its resistance also
increases. Which means what do you think
should happen to the current? It should
decrease. But remember, you're
increasing the voltage. So the voltage
should increase the current, but the
resistance should decrease the current.
So the slope just ends up decreasing
instead because the hotter it gets, the
higher the
resistance and therefore the lower the current
current gets.
gets.
Okay? If I ask you to sketch this, you
should sketch this from memory. If I ask
you to explain why this line slopes this
way, oh yeah, it's because as the
voltage increases, the light bulb gets
brighter. And as it gets brighter, the
temperature increases. And as the
temperature increases, you know, the current
drops. Then finally, we have a
diode. I'm kind of spoiling like the
next section, but a diode is a component
that allows the current to only flow in
one direction. So current always flows
in the direction of the arrow of the diode.
But if the current tries to flow in the
opposite direction, the diode stops
it. So it's like a one-way gate. Current
goes right but can't go
left. So if I plot an IV graph for a
diode, you'll notice that just a little
bit for a small voltage, it doesn't
conduct because diodes are not made of
metals. They're made of what we call semiconductors.
semiconductors.
And it's a specific type of
semiconductor that needs a little bit of
extra voltage to start
conducting. This voltage is around 0.5
to 0.7. It depends on the material. It's
a tiny thing. But the moment the voltage
crosses that value, it shoots up like
boom. It has almost no resistance.
Almost zero. Which is why it doesn't
even have a slope. No, no, no. It's
almost vertical. But we do give it some
slope so we can see what's going
on. The the important feature here is
what? Why is this line horizontal on the other
other
side? Now we didn't focus on that in the
previous graphs because they were all
symmetrical. But the left side of the
graph shows you negative values of
voltage and negative values of current.
Negative simply means we
changed direction.
We changed
direction. All right. And obviously in a
diode, if you change the direction, it
does not let the current through. So the
zero. That's basically it. Nothing
more. Okay? You need to memorize these
all three. You should sketch them right
away and identify which component the
graph is trying to, you know, show you.
final quantity something that we call
power. Now this is honestly from unit
one. So very old quantity not not not
nothing new it's just old. So what is
power? It's the energy per unit time. All
All
right. But here's the thing though in a
circuit in a
circuit a source transfers chemical
energy into electrical energy. Right?
But then in a component like a light
bulb for example, it takes the
electrical energy and turns it into heat
or light. A resistor for example just
gives out heat. A light bulb primarily
gives out light. A speaker gives out
sound and so on. So please note that in
any cell or battery for example, you
change chemical
energy to
electrical. But in a
resistor you change electrical energy to
heat. In a light bulb you change
electrical energy to
light. Now in electricity because we
only measure voltage and current. The
equation to calculate power is not P= E
/T. It's actually P= IV or V * I.
Voltage time current.
Okay. But what if I want
energy? What if I want energy? Now
energy is power times
time back from unit one. And power in
electricity is IV or
VI time. Which means energy in
electricity can be calculated using VIT or
IBT.
Okay. I have a very bad pun. I'm holding back.
pun? Oh, well, I'll hold back. I'll hold back.
back. Yes.
Yes.
Uh, why is it that when you're feeling
down or tired, doctors always want to
give you
vitamins? Because vit gives you
energy. Anyway, I'm sorry. Don't log off now.
now.
Okay, let's keep going. Let's keep
going. I'm
sorry. Now, we have other versions of
this power equations. And we have other
versions. P= I 2 R. People are dying
now. And P= V ^2 / R. Now, where did
these come
from? P= I^2 R is actually P= VI. And I
replaced the V with
IIR. So you end up with I I R which is I^2
I^2
R. P= V ^2 / R is actually P= VI again.
But I = V / R. Back from Ohm's law, it's
the same
thing. So I replaced the I with V / R.
And I end up with VV / R, which is V ^2
/ R.
These formulas are useful if I give you
I and R and ask you to get P right away.
But honestly, if you forget them, that's
fine because if you haven't noticed,
both of them use the same two formulas
P= VI and V= IIR. If you memorize these
two, if you memorize these
two, you can solve any formula involving
I and R or I and V and V and I and P and
R and whatever. Okay. However, this
version of the formula I^2 R will be
very useful later in magnetism when we
talk about
power lost or dissipated as heat in a
transformer or when we transmit electricity.
electricity.
Now, let's talk about something new.
Essentially, we haven't seen this a lot
before because it wasn't there for a
long time in the syllabus. What is a
kilowatt hour?
Now you're like, "What? I've never seen
that." A kilowatt hour is a unit of
energy that we use at
home. It's the amount of energy consumed
by 1,000 watts of power in 1 hour. What
do I mean by
that? Uh, let's say I open up my
application to pay my, you know,
electricity bill this month and I pull
it up. I was like, "Oh, what do you mean
I need to pay £1,000?" It's like it's
not like God. But let's say I have to pay
pay
£1,000. What? How does the electricity
company measure the electrical energy
that I
use? It has that electricity meter,
right? Like right next to your door,
somewhere near your
apartment. Uh but an electricity meter
doesn't measure energy in jewels because
jewels is actually a very small unit of energy.
energy.
We measure it in kilowatt hours. Meaning
how much energy would 1,00 watts of
power like a kettle for example. My
kettle here at home has a power rating
of 1,000 watts. My vacuum cleaner is
1,500 watts. All right. Every device has
a certain wattage. My charger, my phone
charger is like 20 watts, sometimes 30
watts. Depends on if it's a high-speed
charger or not.
And then I just multiply it by 1 hour
because isn't energy power times
time? Kilowatt is power. Hour is time.
So you end up with kilowatt
hours because the values of energy that
we consume at home are super duper
large. We can't use jewels. Okay. So
what is a kilowatt hour? It is how much
energy is used by 1 kilowatt or 1000
watt in 1 hour.
How do I get the value in jewels? Like
if I tell you uh this month I used up 37
kilowatt hours for example that's that's
nothing but let's say I used 37 kilowatt
hours. How do I change that to jewels?
Remember energy is power times time.
This is 37 * kilo means times 1,000
kilo times what's 1 hour in
60 this gives my me the answer in what
in jewles let me work it out so 37 * 1 *
60 * 60 it's a giant value so standard
form 1.33
3 10 ^ of
8. The 3,600 in this uh revision sheet
is the
60. This is extremely new to the
syllabus. We've never used this before.
So, and even in 2023 up to 2024 now like
this year is 2025. Uh we haven't seen it
much yet like maybe
once. Okay. So, we're going to see that
now. Okay.
Now, let's solve a few questions. Define potential
potential
difference. Potential difference or
voltage or emf, it doesn't matter. It's
the same thing. It's the amount of
energy transferred or work done per unit
charge. But add one little extra bit. If
it's emf, it's by a
source to drive a charge per charge by a
source through the whole circuit. If
it's potential difference, it's work
done per unit charge through a component
component. All right? Sometimes these
definitions want you to mention the
energy change that has happened. By the
way, it honestly depends on how many
marks the question is. But also wants
you to mention the energy change. So
here's the question. Potential
difference is the energy change from
what? And you don't have to be specific.
general. It's the energy change from
electrical to something else like
thermal or light or something. So keep
in mind if I ask you to define potential
difference and I ask you to also include
in terms of energy explain it in terms
of energy you have to mention the energy
Okay. Next state the equation which
E equ= W / Q or you can say work per
unit charge. Just write it down as an
equation. Next emf of a battery is 9
volts. The battery is in a circuit.
Calculate the work done by the battery
when it moves a charge of 30 kum. So
this one's easy. Work is energy or sorry
emf time cube. to 9 volts time 30
me
An electric heater
ohms. The power dissipated meaning lost.
So power dissipated means power lost in
the resistance wire is
what? Wait, hate it when notification
just pops up. Okay. The power dissipate
in resistance wire is 2,500 W. Calculate
the current in the resistance wire. So
how do I calculate current? Look at what
you have. Do not automatically go for V
equals IR. I have power and I have
resistance and I want
current. Short way is to use P = I 2
R. And then I have to square
root my
answer. So square<unk> 2500 over
26 which gives you
9 81. Hey almost like the value of G,
right? Gravity does. Or if you forget
this version you can say oh yeah P
equals uh VI. So I equals P over V. But
I don't have V. So first you get V= IIR separately
separately
right what do we have power and
resistance so what can I
get say P= I V or I= P over V you have
power but you don't have this so you say
V equ=
IIR now you don't have I M you don't
have I but you can say that I * 26 is
your V and plug that in here. So it's
2500 over I *
26 which gives you I^2 = 2500 over
26. You can do
that or you can memorize all the
equations and choose the easiest one. So
So 9.81
Next the resistance of a wire the
resistance wire of a heater has a length
of 1.2 m. So this is the length and area
oh thank god he used the area of 7.9 10
^7. By the way this is a challenging
question. Okay. A new heater is designed
using wire of the same material with a
length of 1.8. 8. Ooh. The length what?
Increased. And a cross-sectional area of
5.8. Oh, and the area what?
Decreased. Calculate the resistance of this
wire.
Uh, well, what was the resistance of the
old wire? 26. So, the first wire was 26 ohms.
ohms.
So what's the new resistance? Well,
first remember
resistance is proportional to length and
inversely proportional to
area. If the length increases,
resistance should increase by how much?
Again, this is a challenging question.
By how much? So first I want to see how
much did the length increase
by? The increase in length is 1.8 over
1.2. It's a
ratio 1.8 / 1.2 which gives me 1.5
times. So the length is 1.5 times
larger. So the resistance will also be
1.5 times
area? How much did the area decrease
by? What's the ratio? What's the change
area.
It's 5.8 since that's the new
area. I just want to see how many times
smaller. So this is
0.734 times smaller.
So what's the value of the new
resistance? Okay, the old resistance was
26. The length increased 1.5 times. So
it increases by 1.5 times. This is
because of the
length. Then the area decreased by
0.73, right? Decreased by 0.73. So we
divide not times by
0.73. That's your area.
Look at this. I take the old resistance,
multiply it by whatever the length has
changed by and divide it by whatever the
area has changed by. You just do the
opposite. Everything will fix
itself. So 26 * 1.5 divided by
by
734. This gives me a
This is not an easy
question. It's actually quite
challenging because you need to m see
how much it gets multiplied by increased
Okay? We decrease the area,
right? But because resistance and area
are inversely proportional, whatever I
do, it'll be the opposite. You know what
you could have done earlier? You could
have just did the opposite ratio. So
instead of dividing, if you want to
ratio. But the reason I did this is to
keep you know my thought process the
same. What's the change in area? It's
0.7 times smaller. So how does the
resistance change? Is it multiplied by
0.7 times? No, it's inverse. So it's
Next, a 2500 W heater is used in a
country where electricity costs $0.3 per
kilowatt hour. Calculate the cost of
Okay. Uh, how do I get the cost? Well,
he said it costs $0.3 per kilowatt hour,
which means I need the number of
kilowatt hours, but I have power and
time. So, what do I do first? Step one,
let's get the energy, which is power
times time. So,
2500* 2 days. I can't use days. It has
to be in, you know, seconds, right?
or if you think about it in hours
because I want the power to be in
kilowatt and the time to be in hours. So
look at how I'm changing this. This is
the power. This is the
time. I don't want it in watts and days.
I want this in kilowatt. So this is
going to be 2.5
kilowatt times 2 days is how many
240 kilowatt hours. Now we have the
energy in kilowatt hours. Number two,
you need to get the
cost. If 1 kilowatt hour is $0.3,
then 120 kilowatt hours is how many dollars?
36. You pay
$36 because you kept your heater on
continuously for two days. Who does
Next. A wire has a uniform
cross-sectional area. Which statement is
correct? Okay, let's read. The
resistance of the wire is directly
proportional to its cross-sectional area. What? No, it's inversely
area. What? No, it's inversely proportional to the area. So,
proportional to the area. So, no. The resistance of wire is directly
no. The resistance of wire is directly proportional to cross-section area. Oh,
proportional to cross-section area. Oh, yeah. That's the same thing. The
yeah. That's the same thing. The resistance of a wire is directly
resistance of a wire is directly proportional to the length. Yes. And
proportional to the length. Yes. And inversely proportional to the area. Yes,
inversely proportional to the area. Yes, it was probably C. Well, let's read the
it was probably C. Well, let's read the last one. The resistance is directly
last one. The resistance is directly proportional to length and inversely
proportional to length and inversely proportional to
proportional to diameter.
diameter. Nuhuh. But you may say, but but it's
Nuhuh. But you may say, but but it's inversely proportional to area. Yeah,
inversely proportional to area. Yeah, but area is equal to pi d² over 4. If he
but area is equal to pi d² over 4. If he said to its diameter squared, he would
said to its diameter squared, he would be
be right. But it's not inversely
right. But it's not inversely proportional to diameter inversely
proportional to diameter inversely proportional diameter squared. So C is
proportional diameter squared. So C is still the correct answer.
Next, the diagram shows the current voltage graph for a metal wire. What can
voltage graph for a metal wire. What can be deduced from the graph? Like what can
be deduced from the graph? Like what can we find out from the
we find out from the graph? As the voltage increases, the
graph? As the voltage increases, the wait a second before before I keep
wait a second before before I keep going. Isn't this a straight
going. Isn't this a straight line? Straight line means it's a fixed
resistor. This means the resistance is constant before I even start. And the
constant before I even start. And the temperature is constant. Nothing is
temperature is constant. Nothing is changing because the voltage and current
changing because the voltage and current are increasing uniformly with each
are increasing uniformly with each other. So as the voltage increases the
other. So as the voltage increases the temperature increases. No. As the
temperature increases. No. As the voltage increases, the temperature
voltage increases, the temperature decreases. No. As the voltage increases,
decreases. No. As the voltage increases, the resistance increases. No. As the
the resistance increases. No. As the voltage increases, the resistance
voltage increases, the resistance remains constant. Yes, that's what I
remains constant. Yes, that's what I want. I didn't even need the term as the
want. I didn't even need the term as the voltage increase, resistance is
voltage increase, resistance is constant. Moving on.
Yeah. Next question. A battery is connected to a circuit. It's switched on
connected to a circuit. It's switched on for 1 minute. During that time, there is
for 1 minute. During that time, there is a current of 0.4 ampere. So, hold on. I
a current of 0.4 ampere. So, hold on. I have the time and I have the current.
have the time and I have the current. The battery supplies a total of 48
The battery supplies a total of 48 jewels. I have the energy. Which row
jewels. I have the energy. Which row gives the charge and the emf of the
gives the charge and the emf of the battery? So I want charge which is Q and
battery? So I want charge which is Q and emf which is V just
emf which is V just voltage. Now when it comes to Q, what do
voltage. Now when it comes to Q, what do I have? I have time and I have current.
I have? I have time and I have current. Oh, that's all I need. Current is charge
Oh, that's all I need. Current is charge over time, which means charge is current
over time, which means charge is current times
times time. Current is 0.4 and the time is 1
time. Current is 0.4 and the time is 1 minute. I can't use minutes, right?
minute. I can't use minutes, right? Because the term charge or current is
Because the term charge or current is ampere which is charge per second. So
ampere which is charge per second. So it's time 60 not*
it's time 60 not* 1. So 4 * 60 this gives me 24 kum. So
1. So 4 * 60 this gives me 24 kum. So the answer is either C or
the answer is either C or D. The emf of the battery. Now here you
D. The emf of the battery. Now here you have a few options. You have energy. So
have a few options. You have energy. So option one is to use the definition of
option one is to use the definition of voltage which is energy per charge or
voltage which is energy per charge or work per unit charge. And since we
work per unit charge. And since we already got the charge from the previous
already got the charge from the previous step, you can say it's 48 over 24 which
step, you can say it's 48 over 24 which gives you 2
gives you 2 volts.
volts. Or you have energy and current and you
Or you have energy and current and you want voltage and you have time. So you
want voltage and you have time. So you can use E equals
can use E equals VIT which means V is equal to E over I
VIT which means V is equal to E over I T which is 48 over uh 0.4 * 60 again
T which is 48 over uh 0.4 * 60 again it's the same answer
it's the same answer too. So the answer
too. So the answer is both options are
is both options are okay. Very
okay. Very nice. Next. Oh yeah. Time for the good
nice. Next. Oh yeah. Time for the good stuff.
stuff. Let's talk about
Let's talk about circuits. But these were circuits. Yeah.
circuits. But these were circuits. Yeah. Yeah. Yeah. Let's talk about bigger
Yeah. Yeah. Let's talk about bigger circuits. Let's first talk about all of
circuits. Let's first talk about all of these components. Now, you don't have to
these components. Now, you don't have to memorize them perfectly 100%. It's good
memorize them perfectly 100%. It's good that you remember what they look like,
that you remember what they look like, but you don't have to memorize them all.
but you don't have to memorize them all. Okay?
Okay? Okay. So, as I was saying, you don't
Okay. So, as I was saying, you don't need to memorize the components. Not all
need to memorize the components. Not all of them, not 100%. But it's good to know
of them, not 100%. But it's good to know most of the basic ones. There's a lot
most of the basic ones. There's a lot more than these, lots more, but at least
more than these, lots more, but at least these are some of the basic ones that
these are some of the basic ones that you'll see very
you'll see very frequently. So starting from the top
frequently. So starting from the top left hand, the cell and the battery are
left hand, the cell and the battery are basically the same thing. A battery is
basically the same thing. A battery is just multiple cells. Long line is
just multiple cells. Long line is positive, short line is negative,
positive, short line is negative, positive and negative. Switch is always
positive and negative. Switch is always drawn open because a closed switch is
drawn open because a closed switch is just a line. Power supply. This could
just a line. Power supply. This could mean anything. This could be like a
mean anything. This could be like a battery. It could be a battery pack full
battery. It could be a battery pack full of batteries that gives you a voltage.
of batteries that gives you a voltage. It could be your computer's ATX power
It could be your computer's ATX power supply that controls and gives you
supply that controls and gives you different voltages. Regardless, it's
different voltages. Regardless, it's just two circles. And either it could be
just two circles. And either it could be variable with an arrow through it or
variable with an arrow through it or not. It doesn't matter. An AC power
not. It doesn't matter. An AC power supply means a socket. It's the same
supply means a socket. It's the same symbol as a power supply with with an AC
symbol as a power supply with with an AC wave in the middle. Voltters and emters.
wave in the middle. Voltters and emters. You know the drill. You know what a
You know the drill. You know what a diode is. A light emmitting diode is a
diode is. A light emmitting diode is a diode that emits light. So we just draw
diode that emits light. So we just draw the diode and two light bulbs, sorry,
the diode and two light bulbs, sorry, two light rays out of it. A light bulb
two light rays out of it. A light bulb is a circle with an X. A fixed resistor
is a circle with an X. A fixed resistor is a rectangle. A variable resistor is a
is a rectangle. A variable resistor is a rectangle with an arrow. A potential
rectangle with an arrow. A potential divider is a resistor with an arrow
divider is a resistor with an arrow that's coming from the outside. We'll
that's coming from the outside. We'll see the difference near the end of the
see the difference near the end of the session. A thermister is a resistor that
session. A thermister is a resistor that changes based on temperature. So this is
changes based on temperature. So this is basically a thermometer that's placed in
basically a thermometer that's placed in it. An LDR is a resistor. It changes
it. An LDR is a resistor. It changes based on light. So you have light rays
based on light. So you have light rays coming in to hit it. A heater is like a
coming in to hit it. A heater is like a resistor but with more resistance and
resistor but with more resistance and more heat. So we just draw a few lines
more heat. So we just draw a few lines in the
in the middle. A buzzer is something that
middle. A buzzer is something that produces sound. All right. A bell also
produces sound. All right. A bell also produces
produces sound. They both basically have the same
sound. They both basically have the same symbol. It's like a half circle. doesn't
symbol. It's like a half circle. doesn't matter which side is
matter which side is up. And the fuse is a safety feature
up. And the fuse is a safety feature that we'll discuss. It's like a resistor
that we'll discuss. It's like a resistor in terms of the symbol, but there's a
in terms of the symbol, but there's a line in the middle to represent the wire
line in the middle to represent the wire inside. We will see these often.
inside. We will see these often. Okay, let's describe some of these in
Okay, let's describe some of these in more detail. First, a variable resistor.
more detail. First, a variable resistor. It's resistance resistor whose
It's resistance resistor whose resistance can change. You change the
resistance can change. You change the resistance of a variable resistor by
resistance of a variable resistor by changing the length. Now the way it
changing the length. Now the way it works and if we zoom in here, this is
works and if we zoom in here, this is the structure of it. You have a long
the structure of it. You have a long resistor
resistor wire that is connected to one side of
wire that is connected to one side of the battery, but the other side is not.
the battery, but the other side is not. The wire itself is connected to what we
The wire itself is connected to what we call a sliding contact. It's like a clip
call a sliding contact. It's like a clip that clips on and you can move it back
that clips on and you can move it back and forth and slide it back and forth.
and forth and slide it back and forth. This length is the effective length that
This length is the effective length that affects the resistance. The longer this
affects the resistance. The longer this length becomes by moving the slider to
length becomes by moving the slider to the right, the greater the resistance.
the right, the greater the resistance. The smaller this length, the lower the
The smaller this length, the lower the resistance. So if you move it to the
resistance. So if you move it to the left, the resistance decreases. If you
left, the resistance decreases. If you move it to the right, the resistance
move it to the right, the resistance increases. Okay? Now, the reason for
increases. Okay? Now, the reason for that, if you're curious, is because as
that, if you're curious, is because as the current moves from positive to
the current moves from positive to negative, it only passes through this
negative, it only passes through this section of the wire and then it goes
section of the wire and then it goes out.
out. So if this entire wire was 100 ohms and
So if this entire wire was 100 ohms and it passes only through half of the
it passes only through half of the length, then it's actually passed
length, then it's actually passed through how many ohms? 50. You can
through how many ohms? 50. You can always get the value of the resistance
always get the value of the resistance by checking the ratio of the lengths.
by checking the ratio of the lengths. Like are you through half of it, a
Like are you through half of it, a quarter of it, a tenth of it, 3/4 and so
quarter of it, a tenth of it, 3/4 and so on. Is this concept used for light
on. Is this concept used for light switches where you control the
switches where you control the brightness? Yes, absolutely. But we'll
brightness? Yes, absolutely. But we'll see that light switch control thing in
see that light switch control thing in the end cuz that's actually a potential
the end cuz that's actually a potential divider. But it does use a variable
divider. But it does use a variable resistor in it. Okay. Now the purpose of
resistor in it. Okay. Now the purpose of it is to control the
it is to control the current. Next, what's a thermister? From
current. Next, what's a thermister? From its name, it's a
its name, it's a thermal therm resistor. Depends on heat.
thermal therm resistor. Depends on heat. If the temperature of a
If the temperature of a thermister
thermister increases, its resistance decreases. It
increases, its resistance decreases. It doesn't increase like the light bulb
doesn't increase like the light bulb because thermisters are made of what we
because thermisters are made of what we call
call semiconductors. They're not metallic
semiconductors. They're not metallic conductors. All right? Metals when heat
conductors. All right? Metals when heat when they heat up, sure, their
when they heat up, sure, their resistance does increase. That's true.
resistance does increase. That's true. But non-metallic conductors which are
But non-metallic conductors which are called semiconductors are basically
called semiconductors are basically silicon and doped with boron and
silicon and doped with boron and nitrite they're non-metallic conductors
nitrite they're non-metallic conductors when they gain energy usually in the
when they gain energy usually in the form of heat in this case they get more
form of heat in this case they get more freemoving electrons they become better
freemoving electrons they become better conductors which means they resist
conductors which means they resist less and when they cool down they lose
less and when they cool down they lose that energy they lose those freemoving
that energy they lose those freemoving electrons they go back to their atoms
electrons they go back to their atoms So the resistance
So the resistance increases. So the temperature and
increases. So the temperature and resistance are inversely proportional.
resistance are inversely proportional. So be careful. If it's a metal, when the
So be careful. If it's a metal, when the temperature increases, the resistance
temperature increases, the resistance increases. When it's a non-metal, a
increases. When it's a non-metal, a thermister is the only nonmetal we'll
thermister is the only nonmetal we'll care about for now. When the temperature
care about for now. When the temperature increases, the resistance
increases, the resistance decreases. Its
decreases. Its cousin or its brother from another
cousin or its brother from another mother is the LDR.
mother is the LDR. It basically is a resistor that's
It basically is a resistor that's affected by light. Basically, when the
affected by light. Basically, when the light shining on that resistor
light shining on that resistor increases, its resistance decreases as
increases, its resistance decreases as well. It's inversely
proportional. And when the light on it decreases, meaning you put it in the
decreases, meaning you put it in the dark, its resistance
dark, its resistance increases for the exact same
increases for the exact same reasons as
reasons as what? as a
what? as a thermist. It's made of a non-metallic
thermist. It's made of a non-metallic conductor. So when it gains energy,
conductor. So when it gains energy, doesn't get hot, gains energy from the
doesn't get hot, gains energy from the light, sunlight, light bulb, doesn't
light, sunlight, light bulb, doesn't matter. It gets more freeoving electrons
matter. It gets more freeoving electrons and it becomes a better conductor. Its
and it becomes a better conductor. Its resistance
resistance decreases. Yeah. If I plot a graph of
decreases. Yeah. If I plot a graph of how the resistance changes with
how the resistance changes with temperature or light, this is how we
temperature or light, this is how we sketch it. This is how we sketch
sketch it. This is how we sketch anything that's inversely proportional.
anything that's inversely proportional. Not a straight line going down, but a
Not a straight line going down, but a curve with a negative slope. Okay, a
curve. Finally, the diode. What is a diode? We described this earlier. It is
diode? We described this earlier. It is a component that only allows the current
a component that only allows the current to flow in one
to flow in one direction. Meaning, if you take a look
direction. Meaning, if you take a look at this here, the current flows from
at this here, the current flows from positive to negative. If the current is
positive to negative. If the current is going to flow in the direction of the
going to flow in the direction of the diode, it passes through lights up the
diode, it passes through lights up the circuit as if it's not there. It has no
circuit as if it's not there. It has no resistance. But if you connect the diode
resistance. But if you connect the diode in reverse and if the current is going
in reverse and if the current is going to flow in the opposite direction, it
to flow in the opposite direction, it doesn't even leave the supply again.
doesn't even leave the supply again. Again, cuz some some some seasons think
Again, cuz some some some seasons think this, look at look at this. It does not
this, look at look at this. It does not go through the circuit. The charges
go through the circuit. The charges don't go through the circuit. meet a
don't go through the circuit. meet a diode and go like there's a diode in
diode and go like there's a diode in reverse. We need to stop now. No, no,
reverse. We need to stop now. No, no, there's no current in the first place.
there's no current in the first place. There's no current in the first place.
There's no current in the first place. Zero
Zero current. Diode stops. Now a diode has
current. Diode stops. Now a diode has primarily one function to convert AC to
primarily one function to convert AC to DC and there are two ways to do it. The
DC and there are two ways to do it. The lazy way which is called the halfwave
lazy way which is called the halfwave rectifier
rectifier method. Okay, which basically means you
method. Okay, which basically means you take
take the normal AC that you're used to
the normal AC that you're used to alternating current and you pass it
alternating current and you pass it through one diode. When the current
through one diode. When the current flows this way, it goes through.
flows this way, it goes through. Yay. And when the current tries to go in
Yay. And when the current tries to go in the opposite direction, it doesn't
the opposite direction, it doesn't because that would make it reverse that
because that would make it reverse that reverse compared to the diode. So, it
reverse compared to the diode. So, it doesn't go through zero.
But this is a very lazy way of doing it because you've essentially gotten a pair
because you've essentially gotten a pair of scissors and you've cut out half of
of scissors and you've cut out half of your energy. You only allowed one side
your energy. You only allowed one side to go through but not the other. The
to go through but not the other. The negative doesn't go
negative doesn't go through. So how do we fix
through. So how do we fix this? If we want to purely convert AC to
this? If we want to purely convert AC to DC, we use what is called a full wave
DC, we use what is called a full wave rectifier or a bridge.
rectifier or a bridge. It is essentially four diodes connected
It is essentially four diodes connected in a diamond
in a diamond pattern. Two of them look
pattern. Two of them look up and they're parallel to each other
up and they're parallel to each other and two of them look down when they're
and two of them look down when they're also parallel to each other. Two of them
also parallel to each other. Two of them look up and two of them look down. You
look up and two of them look down. You do not have to memorize this by the way,
do not have to memorize this by the way, but you do know have to you do have to
but you do know have to you do have to know if a diode is drawn correctly or a
know if a diode is drawn correctly or a bridge is drawn correctly or not.
bridge is drawn correctly or not. Remember what I'm saying. Two of them
Remember what I'm saying. Two of them are parallel to each other looking down.
are parallel to each other looking down. Two of them are looking a up. I don't
Two of them are looking a up. I don't care which is up and down though. Like
care which is up and down though. Like these could be the ones up. So these
these could be the ones up. So these have to be the ones
have to be the ones down. But if I draw the diodes like
down. But if I draw the diodes like this, like each one is in a different
this, like each one is in a different direction. this is
direction. this is wrong. So that's the first thing you
wrong. So that's the first thing you need to identify. The second is knowing
need to identify. The second is knowing how to trace the current through a
how to trace the current through a diode. Like knowing how to draw how the
diode. Like knowing how to draw how the currents flowing through the diodes. You
currents flowing through the diodes. You don't have to, like I said, memorize the
don't have to, like I said, memorize the diagram, but you have to look at how it
diagram, but you have to look at how it goes through. So I'm going to draw two
goes through. So I'm going to draw two currents. One in red when the top side
currents. One in red when the top side of the supply is positive and the bottom
of the supply is positive and the bottom is
is negative, and one in blue
negative, and one in blue which is when the top is negative and
which is when the top is negative and the bottom is positive like when the
the bottom is positive like when the current flips and look how it reaches
current flips and look how it reaches the other side like the other
the other side like the other terminal. So let's start with the red.
terminal. So let's start with the red. Current goes up, goes right, goes down,
Current goes up, goes right, goes down, reaches a
reaches a junction. It cannot go left. So it goes
junction. It cannot go left. So it goes right, reaches the next junction. It
right, reaches the next junction. It cannot go left. So it goes right. So
cannot go left. So it goes right. So this side is positive and this side is
this side is positive and this side is negative. And the current goes through.
negative. And the current goes through. No
No problem. If you want to see the current
problem. If you want to see the current going back, this is how it goes
back. Okay. How about the blue
How about the blue side? Let's follow the blue line. Now
side? Let's follow the blue line. Now the blue means the bottom terminal is
the blue means the bottom terminal is positive. So it goes down, goes to the
positive. So it goes down, goes to the right, reaches a junction, left or
right, reaches a junction, left or right. Left is blocked off. So it goes
right. Left is blocked off. So it goes right through D2. Then it meets the next
right through D2. Then it meets the next junction. Left or right? Left is
junction. Left or right? Left is completely blocked off. So it goes
completely blocked off. So it goes right. Oh, this is still
right. Oh, this is still positive. So what reaches the
positive. So what reaches the output? This is negative. So flows this
output? This is negative. So flows this way and on the way
back when it reaches the negative it flips. You essentially take the negative
flips. You essentially take the negative version of this graph and you flip it.
version of this graph and you flip it. That's all you do. This is called a full
That's all you do. This is called a full wave
wave rectifier. So again, if I tell you you
rectifier. So again, if I tell you you only use one diode, it's a jump and a
only use one diode, it's a jump and a zero. A jump and a zero. If you use a
zero. A jump and a zero. If you use a full wave rectifier, four dodes, it's
full wave rectifier, four dodes, it's jump. No negatives. No
jump. No negatives. No use. Finally, what is an LED or a light
use. Finally, what is an LED or a light emmitting
emmitting diode? It's just a diode that shines
diode? It's just a diode that shines bright, gives out light when a current
bright, gives out light when a current goes through it. That's it. So, it's
goes through it. That's it. So, it's basically a diode, but it's got the
basically a diode, but it's got the extra function of glowing or like
extra function of glowing or like emitting light.
Let's get into the highlight of this particular
particular chapter. Series and parallel
chapter. Series and parallel connections. This is the part that
connections. This is the part that confuses some people and gives them
confuses some people and gives them trouble. But you need to remember
trouble. But you need to remember something. Whatever I say in series will
something. Whatever I say in series will be the opposite of what happens in
be the opposite of what happens in parallel. All right? And then you need
parallel. All right? And then you need to memorize exactly what happens to the
to memorize exactly what happens to the current.
current. the resistance and the
the resistance and the voltage. The current, the resistance and
voltage. The current, the resistance and the
the voltage. Sometimes it increases,
voltage. Sometimes it increases, sometimes it decreases, sometimes it
sometimes it decreases, sometimes it splits, sometimes it
splits, sometimes it doesn't. Sometimes it's the same,
doesn't. Sometimes it's the same, sometimes it's not. Like you need to
sometimes it's not. Like you need to memorize how each method of connecting
memorize how each method of connecting components together changes these three
components together changes these three factors. So starting off with series
factors. So starting off with series connections. A series connection means
connections. A series connection means you connect the two resistors along the
you connect the two resistors along the same
same wire. So if I were to connect them to
wire. So if I were to connect them to let's say a 10V supply and there's a
let's say a 10V supply and there's a current I going through it. It's number
current I going through it. It's number one the current is the same. You have
one the current is the same. You have the same current going through both
the same current going through both because it's only one wire. That's the
because it's only one wire. That's the current. Second, when you connect
current. Second, when you connect resistors in series, their combined
resistors in series, their combined resistance
resistance increases and you calculate it using R1
increases and you calculate it using R1 plus R2 plus R3 plus you just add
plus R2 plus R3 plus you just add them. So if this was
them. So if this was uh 10 ohms and 10
uh 10 ohms and 10 ohms, the total would be 20 ohms.
Finally, but most importantly, what happens to the
happens to the voltage? The voltage of the supply in
voltage? The voltage of the supply in series
series gets split. Now, the voltage of the
gets split. Now, the voltage of the supply doesn't change, but the voltage
supply doesn't change, but the voltage that you try to deliver gets split. The
that you try to deliver gets split. The potential difference
potential difference splits. If I were to calculate the
splits. If I were to calculate the voltage across the first resistor, I
voltage across the first resistor, I would first need to get the current. So
would first need to get the current. So I'd say I = V / R which is 10 / 20.
I'd say I = V / R which is 10 / 20. That's the total voltage and the total
That's the total voltage and the total resistance which is 0.5 amp. And then if
resistance which is 0.5 amp. And then if I ask you to get the voltage only across
I ask you to get the voltage only across the first resistor
the first resistor V1 you would say I
V1 you would say I R1 which is 0.5 that's the
R1 which is 0.5 that's the current time 10 which is 5. This means
current time 10 which is 5. This means that this resistor only gets 5 volts
that this resistor only gets 5 volts from the supply which means the other
from the supply which means the other one also gets 5 volts from the supply.
one also gets 5 volts from the supply. The voltage the total voltage that you
The voltage the total voltage that you have gets split gets
have gets split gets divided. It's not always equal. It
divided. It's not always equal. It depends on the ratio of the resistors.
depends on the ratio of the resistors. For example, if this wasn't 10 and 10,
For example, if this wasn't 10 and 10, what if this was a Let me delete all of
what if this was a Let me delete all of this. What if this was a
this. What if this was a uh let's just use the same supply, a 10
uh let's just use the same supply, a 10 ohm resistor and uh 90 ohm resistor.
ohm resistor and uh 90 ohm resistor. Going for the extreme, the first
Going for the extreme, the first resistor will only get one volt and the
resistor will only get one volt and the second resistor only gets nine gets the
second resistor only gets nine gets the rest because the voltage gets split
rest because the voltage gets split according to the ratio of the
according to the ratio of the resistors. One will increase, the other
resistors. One will increase, the other has to decrease.
has to decrease. so that the total voltage stays the
so that the total voltage stays the same. It's 10
same. It's 10 volts. Okay, that's if they're in
volts. Okay, that's if they're in series. What if the resistors are in
series. What if the resistors are in parallel? Well, everything I said gets
parallel? Well, everything I said gets flipped over. Huh? In series, I said the
flipped over. Huh? In series, I said the current is the same. Like it doesn't
current is the same. Like it doesn't change, right?
change, right? But in
But in parallel uh you
parallel uh you have
have two branches for the current to go
two branches for the current to go through. It's not just one loop. It's
through. It's not just one loop. It's two loops actually. So the current that
two loops actually. So the current that flows through the circuit
flows through the circuit splits. Does that mean it gets smaller?
splits. Does that mean it gets smaller? On the contrary, the combined resistance
On the contrary, the combined resistance of resistors in parallel doesn't
of resistors in parallel doesn't increase. It actually decreases.
increase. It actually decreases. Because if you think about it,
Because if you think about it, connecting resistors in parallel on top
connecting resistors in parallel on top of each other is like making a wire
of each other is like making a wire thicker. You allow more charges to go
thicker. You allow more charges to go through at the same time. So connecting
through at the same time. So connecting resistors in
resistors in parallel gives the charges more space to
parallel gives the charges more space to go through which increases the current.
go through which increases the current. So the current gets very large and the
So the current gets very large and the resistance
resistance A
A decreases. How do we calculate it? Using
decreases. How do we calculate it? Using this
this rule R equals product over sum or R2 R1
rule R equals product over sum or R2 R1 * R2 over R1 +
* R2 over R1 + R2. So for them example, if this was 10
R2. So for them example, if this was 10 ohms and 10 ohms, their combined
ohms and 10 ohms, their combined resistance wouldn't be 20.
resistance wouldn't be 20. It would be 10 * 10 over 10 + 10 which
It would be 10 * 10 over 10 + 10 which gives me
gives me 5. The combined resistance of resistors
5. The combined resistance of resistors in parallel
in parallel decreases and it has to be lower than
decreases and it has to be lower than the smallest resistor. So if I have 10
the smallest resistor. So if I have 10 and 10 has to be less than 10. If I have
and 10 has to be less than 10. If I have 10 and 20 still less than 10. If I have
10 and 20 still less than 10. If I have 10 ohms and 2 ohms has to be less than 2
10 ohms and 2 ohms has to be less than 2 ohms. The resistance just decreases
ohms. The resistance just decreases drops hard.
Finally, this is also voltage is arguably very important. Why? Because in
arguably very important. Why? Because in series, if you remember, the voltage
series, if you remember, the voltage gets split. In parallel, it doesn't. In
gets split. In parallel, it doesn't. In parallel, all the components get the
parallel, all the components get the same voltage.
same voltage. This means that this 10V
This means that this 10V supply can deliver 10 volts completely
supply can deliver 10 volts completely to the first resistor and 10 volts
to the first resistor and 10 volts completely to the
completely to the second. Everything in parallel gets the
second. Everything in parallel gets the same voltage. And that's because each
same voltage. And that's because each like resistor gets its own charge. Like
like resistor gets its own charge. Like this is a charge carrying 10 volts goes
this is a charge carrying 10 volts goes through just this. Here's another charge
through just this. Here's another charge carrying another 10 volts. It only goes
carrying another 10 volts. It only goes through
through R2. In series, the same poor charge has
R2. In series, the same poor charge has to do what? If you had a charge carrying
to do what? If you had a charge carrying 10 volts, oh, it has to go through both
10 volts, oh, it has to go through both R1 and R2. So, it's forced to split its
R1 and R2. So, it's forced to split its voltage. But in parallel, each one gets
voltage. But in parallel, each one gets its own
its own voltage because it gets its own charge,
voltage because it gets its own charge, full
full voltage. Very good.
Now, obviously, parallel has a few advantages over series. What do I mean?
advantages over series. What do I mean? At home, most of your light bulbs and
At home, most of your light bulbs and switches and sockets are all connected
switches and sockets are all connected in parallel for three reasons. Number
in parallel for three reasons. Number one, everything in parallel gets the
one, everything in parallel gets the full voltage. So, at home, if my voltage
full voltage. So, at home, if my voltage is 220 volts, this light bulbs gets 220.
is 220 volts, this light bulbs gets 220. This light bulb gets 220. This light
This light bulb gets 220. This light bulb also gets
220. Everything lights up, right? Sure, you end up paying more
you end up paying more money. Capitalism,
money. Capitalism, but that sounded
Scottish. Now, uh, everything gets the same
uh, everything gets the same voltage, but here's the another
voltage, but here's the another advantage. You can switch them on and
advantage. You can switch them on and off separately. or independently,
off separately. or independently, meaning you can close the switch here
meaning you can close the switch here and open this switch and close this
and open this switch and close this switch and you have two light bulbs on,
switch and you have two light bulbs on, one light bulb off. It's up to
one light bulb off. It's up to you. And then if one of them breaks, the
you. And then if one of them breaks, the others still work. That's the advantage
others still work. That's the advantage of parallel, like having them on
of parallel, like having them on separate branches. They don't affect
separate branches. They don't affect each other. If everything in your house
each other. If everything in your house was connected in
was connected in series, if everything in your house is
series, if everything in your house is connected in
connected in series, if one light bulb breaks,
series, if one light bulb breaks, everything goes off.
everything goes off. everything turns
everything turns off.
off. Okay. However, there is something else
Okay. However, there is something else that we do connect in series is very
that we do connect in series is very important. Cells or batteries. You can
important. Cells or batteries. You can have more than one cell in series. By
have more than one cell in series. By the way, like if I put a 6V cell in this
the way, like if I put a 6V cell in this example next to a 3V cell, the voltage
example next to a 3V cell, the voltage that you deliver is not six or three.
that you deliver is not six or three. It's nine. They get added up.
It's nine. They get added up. So when you connect cells in series, you
So when you connect cells in series, you just add their voltages
together. To anybody observant, you look to the right side
observant, you look to the right side over here and say, uh, why is this four
over here and say, uh, why is this four volts not not like eight or
volts not not like eight or something? Why is it four not
eight? Because look at this first cell. It's positive and negative are pointing
It's positive and negative are pointing to the left. So the current is going to
to the left. So the current is going to flow to the left. The second cells
flow to the left. The second cells positive and negative point to the
positive and negative point to the right which means it's in the opposite
right which means it's in the opposite direction. These are in the same
direction. These are in the same direction. These both try to push the
direction. These both try to push the current in the same
current in the same direction. So what do they do? They
direction. So what do they do? They cancel out. Instead of adding them, you
cancel out. Instead of adding them, you subtract
subtract them. So if the cells are in the same
them. So if the cells are in the same direction, you add them. If the cells
direction, you add them. If the cells are in opposite direction, you
are in opposite direction, you subtract.
Yeah. Can you put an AC supply next to a battery? I mean, you
battery? I mean, you can. It's not a good idea,
can. It's not a good idea, though. Finally, let's talk about the
though. Finally, let's talk about the potential divider. A potential divider
potential divider. A potential divider is just a very fancy way of saying two
is just a very fancy way of saying two resistors in series. But the function
resistors in series. But the function here is to actually split the voltage.
here is to actually split the voltage. Like look at this example. If this was a
Like look at this example. If this was a 10 ohm and this is a 30 ohm resistor,
10 ohm and this is a 30 ohm resistor, the voltage will split with a ratio of 1
the voltage will split with a ratio of 1 to 3. So 2.5 volt to 7.5 volt. Do you
to 3. So 2.5 volt to 7.5 volt. Do you know what that means? This means if you
know what that means? This means if you connect another light bulb only parallel
connect another light bulb only parallel to the first resistor, it gets 2.5
to the first resistor, it gets 2.5 volts. You got you get to choose what
volts. You got you get to choose what the voltage is across it. No. No, no,
the voltage is across it. No. No, no, no. But what if I connect another light
no. But what if I connect another light bulb here? This will get what? 7 1/2
bulb here? This will get what? 7 1/2 volts. Because the voltage was split
volts. Because the voltage was split first according to the ratio of the
first according to the ratio of the resistors and then you ended up
resistors and then you ended up connecting this component not parallel
connecting this component not parallel to the entire circuit but parallel only
to the entire circuit but parallel only to the first resistor. So it only gets
to the first resistor. So it only gets the voltage of the first resistor.
the voltage of the first resistor. If you take a look at the second one,
If you take a look at the second one, you connect it parallel to the second
you connect it parallel to the second resistor. So it only gets the voltage of
resistor. So it only gets the voltage of the second
the second resistor. So if I were to turn this
resistor. So if I were to turn this circuit on, the light bulb on the right
circuit on, the light bulb on the right would be bright and the one on the left
would be bright and the one on the left would be
dim. A very similar circuit to this is what we call a variable potential
what we call a variable potential divider.
divider. This is a much cleaner version because
This is a much cleaner version because if I wanted to change the voltage like
if I wanted to change the voltage like increase and decrease the voltage
increase and decrease the voltage directly I don't need a potential
directly I don't need a potential divider with two resistors and then I
divider with two resistors and then I have to split the voltage and then if I
have to split the voltage and then if I want to change the ratio I have to
want to change the ratio I have to change the ratio of the resistors.
change the ratio of the resistors. I can just connect a variable
I can just connect a variable resistor completely to the supply which
resistor completely to the supply which means this entire wire gets the full 10
means this entire wire gets the full 10 volts. But then you connect your slider
volts. But then you connect your slider or sliding contact in parallel to the
or sliding contact in parallel to the light bulb that you
light bulb that you want. So if the sliding contact is in
want. So if the sliding contact is in the middle, it's not parallel to the
the middle, it's not parallel to the full wire. It's parallel to what? Half
full wire. It's parallel to what? Half of it. So it doesn't get 10 volts.
of it. So it doesn't get 10 volts. The entire wire gets 10. Sure. But if
The entire wire gets 10. Sure. But if you're only connected to half of it, you
you're only connected to half of it, you get what? 5
volts. What if you move this parallel here to the very end? You get the full
here to the very end? You get the full 10 volts. Cuz you're now parallel to the
10 volts. Cuz you're now parallel to the entire wire. What if you move it to the
entire wire. What if you move it to the left? You get
left? You get nothing. Because you're parallel to
nothing. Because you're parallel to nothing. Look, you're parallel to an
nothing. Look, you're parallel to an empty wire. Like it's nothing.
empty wire. Like it's nothing. This is called the variable potential
This is called the variable potential divider. And whoever asked me earlier,
divider. And whoever asked me earlier, uh, is this how light bulbs or like
uh, is this how light bulbs or like variable light bulbs that you have at
variable light bulbs that you have at home work? This is how they
home work? This is how they work. A variable potential divider is so
work. A variable potential divider is so much cleaner than just putting a
much cleaner than just putting a variable resistor in series with a light
variable resistor in series with a light bulb. Put it in parallel instead. This
bulb. Put it in parallel instead. This allows you to change the voltage
allows you to change the voltage directly from zero to full to 10 volts.
directly from zero to full to 10 volts. zero being zero being the slider near
zero being zero being the slider near the side that's connected to the battery
the side that's connected to the battery and the maximum being the other side the
and the maximum being the other side the other
end. Okay. So the purpose of it isn't to control current now it's to control what
control current now it's to control what voltage across
voltage across component. As one final rule, a variable
component. As one final rule, a variable potential divider can follow this rule.
potential divider can follow this rule. V_sub_1 over V2= R1 / R2. Meaning the
V_sub_1 over V2= R1 / R2. Meaning the ratio of the voltage is the same as the
ratio of the voltage is the same as the ratio of the resistors. We sometimes use
ratio of the resistors. We sometimes use this when solving questions. It does
this when solving questions. It does help. Do I always need it? Not really,
help. Do I always need it? Not really, but it does
but it does help. Okay, let's solve a few questions.
Starting off with this March question over
here. A circuit consists of a DC supply, a lamp and a
a lamp and a thermister. Draw a circuit diagram of
thermister. Draw a circuit diagram of these components connected in series. So
these components connected in series. So let's go. A DC supply. You can either
let's go. A DC supply. You can either draw just a supply and just write DC on
draw just a supply and just write DC on it or like positive and negative. Or you
it or like positive and negative. Or you can draw a battery or a cell. That's
can draw a battery or a cell. That's fine. A lamp, so light bulb, and a
fine. A lamp, so light bulb, and a thermister are all in series. Do I need
thermister are all in series. Do I need anything else?
anything else? Nope. That's
Explain what happens in the circuit you have drawn. When the temperature of the
have drawn. When the temperature of the thermister increases. Ooh. Ooh. Okay.
thermister increases. Ooh. Ooh. Okay. When the temperature increases, the
When the temperature increases, the resistance of the
resistance of the thermister
thermister decreases. And if the resistance of the
decreases. And if the resistance of the thermister
thermister decreases, the current
decreases, the current will
will increase. But there's a light bulb in
increase. But there's a light bulb in there. So the light bulb becomes what?
there. So the light bulb becomes what? Bright.
Bright. Look at the way I sequenced my
Look at the way I sequenced my logic. I started off with what happens
logic. I started off with what happens when the temperature increases. When the
when the temperature increases. When the temperature increases, the
temperature increases, the resistance decreases of the thermister.
resistance decreases of the thermister. Like I I'll be even of the
theister. But that causes what? That causes the resistance of the
what? That causes the resistance of the circuit to decrease. the total
circuit to decrease. the total resistance increases and the total
resistance increases and the total current
current increases, right? So, the current
increases, right? So, the current increases. That's honestly enough.
increases. That's honestly enough. Honestly, that's enough. But you know
Honestly, that's enough. But you know what? I just want to push
what? I just want to push through. So, the light
bulb is bright or glow bright. It's only two marks. So, honestly, I'm just
two marks. So, honestly, I'm just looking for resistance decreases. So the
looking for resistance decreases. So the current
current increases. That's that's genuinely what
increases. That's that's genuinely what I'm looking for. But I wanted to express
I'm looking for. But I wanted to express exactly what's happening inside because
exactly what's happening inside because if it was worth more marks, that's
if it was worth more marks, that's great. We end up getting more
great. We end up getting more marks. Next question. Ooh, I see an AC
marks. Next question. Ooh, I see an AC supply. Oh, what's
supply. Oh, what's this? Huh? Is this a single diode or a
this? Huh? Is this a single diode or a full wave rectifier? Like without even
full wave rectifier? Like without even reading the question, is this a single
reading the question, is this a single diode or a full wave
diode or a full wave rectifier? Just one diode. Like look at
rectifier? Just one diode. Like look at this. He has the AC supply connected to
this. He has the AC supply connected to one diode. And he's like, "What's the
one diode. And he's like, "What's the voltage across this resistor? If it was
voltage across this resistor? If it was the full wave rectifier, it would be a
the full wave rectifier, it would be a bunny hop going up, down, up, down, even
bunny hop going up, down, up, down, even if it's negative." But it's not. It's
if it's negative." But it's not. It's just one diode. So Cuts off half of the
just one diode. So Cuts off half of the voltage.
7.1 shows a circuit that contains a battery, a switch, and a voltmeter and
battery, a switch, and a voltmeter and three 40 ohm resistors. Oh, this is
three 40 ohm resistors. Oh, this is important. You didn't draw the values.
important. You didn't draw the values. You just mentioned them here. They're
You just mentioned them here. They're all 40 ohm
all 40 ohm resistors. R1 and R2 and R3.
Describe the switch is opened and R1 R2 form a potential divider. Explain what
form a potential divider. Explain what is meant by the term potential divider.
is meant by the term potential divider. So what is a potential divider? Now the
So what is a potential divider? Now the function of a potential divider is to do
function of a potential divider is to do what? Is to split the voltage or divide
what? Is to split the voltage or divide the voltage between
the voltage between two resistors.
two resistors. Right? Proportional to the ratio
Right? Proportional to the ratio depending on the ratio. That is what a
depending on the ratio. That is what a potential divider is and that's the
potential divider is and that's the function of it at the same time. So a
function of it at the same time. So a potential divider is just what a
potential divider is just what a circuit that
circuit that divides the
divides the voltage across two resistors in
voltage across two resistors in series according to their ratio or
series according to their ratio or according to the value of the resistance
according to the value of the resistance or proportional to their values.
Next up, remember all of this. All of this and the switch is still what? Open,
this and the switch is still what? Open, which means this is open, which means R3
which means this is open, which means R3 is not part of the circuit
is not part of the circuit yet cuz the current's going to flow here
yet cuz the current's going to flow here through R1 and R2 and then come back.
through R1 and R2 and then come back. It's not going through R3
It's not going through R3 yet. The reading on the voltmeter is
yet. The reading on the voltmeter is 7.5, which means this is 7.5 volts.
7.5, which means this is 7.5 volts. What is the emf of the
battery? Actually, that's easy. Didn't he say they're all 40 ohm
easy. Didn't he say they're all 40 ohm resistors? This is 40. This is 40. This
resistors? This is 40. This is 40. This is
is 40. But this doesn't
40. But this doesn't count. If I have two resistors that are
count. If I have two resistors that are equal in
equal in value in
value in series, doesn't the voltage split
series, doesn't the voltage split equally between them?
equally between them? Doesn't the voltage split equally
Doesn't the voltage split equally between
between them? So if this gets 7.5, this also
them? So if this gets 7.5, this also gets
gets what?
what? 7.5. Which means the total voltage is
7.5. Which means the total voltage is what? 15. 7.5 + 7.5 is
15. I could tell all of that just because he said, "Hey, they're all 40
because he said, "Hey, they're all 40 ohm resistors," which means they're all
ohm resistors," which means they're all the same resistance.
Okay, which means the voltage splits equally. So if the first one got 7 and
equally. So if the first one got 7 and 1/2, the second one gets 7 and a half.
1/2, the second one gets 7 and a half. If the first one got like 200 volts, the
If the first one got like 200 volts, the second should also get 200 volts.
second should also get 200 volts. However, now the switch is
However, now the switch is closed. Oh boy. What's the resistance of
closed. Oh boy. What's the resistance of the complete circuit?
the complete circuit? Yeah, I'm going to redraw the circuit
Yeah, I'm going to redraw the circuit here, but instead of vertically because
here, but instead of vertically because sometimes mentally in your head it's
sometimes mentally in your head it's hard to imagine, I'll draw it
hard to imagine, I'll draw it horizontally. Like I'm just going to
horizontally. Like I'm just going to rotate this 90°. Here's
rotate this 90°. Here's R1 and then there is
R1 and then there is R2 and then like R3 is above
R2 and then like R3 is above that. Which means what? Which means you
that. Which means what? Which means you have two resistors in parallel first
have two resistors in parallel first which are then in series with this dude
which are then in series with this dude over here.
over here. So step one I need to get these two
So step one I need to get these two together first in parallel and after I
together first in parallel and after I get their combined resistance I add it
get their combined resistance I add it to the series
one. So let's go the parallel version first. It's product
parallel version first. It's product over sum. R1 * R2 over R1 + R2, which is
over sum. R1 * R2 over R1 + R2, which is 40 *
40 * 40 over 40 + 40. This will give me 20.
40 over 40 + 40. This will give me 20. And this is something you can memorize,
And this is something you can memorize, by the way. If you have two resistors in
by the way. If you have two resistors in parallel and they have the same value,
parallel and they have the same value, their combined resistance is half of
their combined resistance is half of them. So 40 and 40 give you 20. 30 and
them. So 40 and 40 give you 20. 30 and 30 give you 15. Five and five gives you
30 give you 15. Five and five gives you two and a half. But then I need to add
two and a half. But then I need to add it to the series resistor. So the 20
it to the series resistor. So the 20 ohms, the combined 40 and 40 gives you
ohms, the combined 40 and 40 gives you 20 plus the 40 for that separate
20 plus the 40 for that separate resistor. This gives you a total of 60
ohms. Knowing what to sequence and when is
important. Calculate the reading on the voltmeter when the switch is now closed.
voltmeter when the switch is now closed. Ooh. Oh, wait, wait, wait. Hold on, hold
Ooh. Oh, wait, wait, wait. Hold on, hold on.
Let me erase this. Or maybe I didn't need to. Yeah, I
this. Or maybe I didn't need to. Yeah, I didn't need
didn't need to. Didn't we just say that these two
to. Didn't we just say that these two together are worth 20
together are worth 20 ohms? And now it's technically in series
ohms? And now it's technically in series with this, which is 40 ohms.
with this, which is 40 ohms. Will the 15 volts of the supply now
Will the 15 volts of the supply now split
split equally? No, it
equally? No, it won't. R1, which is 40, will get more
won't. R1, which is 40, will get more than
than R2. R1, which is the 40 ohms, will get
R2. R1, which is the 40 ohms, will get more than R2 and R3 because they're
more than R2 and R3 because they're together. They're 20 ohms. So, when he
together. They're 20 ohms. So, when he asks you for the reading on the
asks you for the reading on the voltmeter, he means what's the voltage
voltmeter, he means what's the voltage across this?
across this? Now that this is 40 and 20, it's going
Now that this is 40 and 20, it's going to be
to be what? 10 volts. And you can use two
what? 10 volts. And you can use two methods to get this. You can either use
methods to get this. You can either use Ohm's law, which is V= IR. Let's try
Ohm's law, which is V= IR. Let's try that one out first. Or you can use the
that one out first. Or you can use the ratio example. Remember how I used
ratio example. Remember how I used ratios? R1 / R2, V1 over V2. Let's try
ratios? R1 / R2, V1 over V2. Let's try this out. Let's try Ohm's law
this out. Let's try Ohm's law first. Step one, I need the current. So
first. Step one, I need the current. So I= V / R. The total voltage is 15 volts.
I= V / R. The total voltage is 15 volts. So the total resistance is what? 60. Oh
So the total resistance is what? 60. Oh uh wait I didn't I didn't write this.
uh wait I didn't I didn't write this. Okay
Okay 60. This gives me a current
60. This gives me a current of
4.25. Then you use Ohm's law again but to get the voltage of V1 which is the
to get the voltage of V1 which is the voltage across R1. So it's 0.25 25 * 40
voltage across R1. So it's 0.25 25 * 40 which gives you what?
which gives you what? 10.
Yay. Or you can use a ratio example. But
Or you can use a ratio example. But ratio of what exactly? I don't have V2.
ratio of what exactly? I don't have V2. Like I don't know what this voltage is,
Like I don't know what this voltage is, but I do have the total voltage. So
but I do have the total voltage. So here's another version of this ratio
here's another version of this ratio example thing. We can say V1 over V
example thing. We can say V1 over V total equals R1 / R total. It still
total equals R1 / R total. It still works if you compare it to the total,
works if you compare it to the total, not just to the one next to it. So V1
not just to the one next to it. So V1 over what's the total voltage? 15 equals
over what's the total voltage? 15 equals R1, which is the 40
R1, which is the 40 ohms that you want over the total
ohms that you want over the total resistance, which is 60. So V1 is equal
resistance, which is 60. So V1 is equal to 40 / 60 * 15. This gives you 10.
pick your poison. Doesn't matter. They're both
They're both okay. They're both
okay. They're both okay. All
okay. All right, next
right, next question. Oh, wait. Do you want to take
question. Oh, wait. Do you want to take a picture of
a picture of this? Why did it
disappear? The app's being weird. Okay, never mind. You can go back and pause
never mind. You can go back and pause and get the picture there.
Next question. I see three cells in series. I see R1 and R2 and a diode in
series. I see R1 and R2 and a diode in R3 and a
R3 and a voltmeter. The three cells have zero
voltmeter. The three cells have zero resistance. R1, R2, R3 are identical,
resistance. R1, R2, R3 are identical, meaning they're the same. The reading on
meaning they're the same. The reading on the voltmeter is six. The voltmeter
the voltmeter is six. The voltmeter reading is parallel to all three, which
reading is parallel to all three, which means the total voltage or EMF here is 6
means the total voltage or EMF here is 6 volts.
When the diode is conducting, it has zero resistance and zero potential
zero resistance and zero potential difference across it. He's just saying
difference across it. He's just saying the diode doesn't affect anything yet.
the diode doesn't affect anything yet. Determine the emf of one cell. If three
Determine the emf of one cell. If three cells have 6
cells have 6 volts, this means one cell has what? Two
volts, this means one cell has what? Two volts. Cuz 2 + 2 + 2 gives you
volts. Cuz 2 + 2 + 2 gives you six. Then determine the ratio of the
six. Then determine the ratio of the potential difference across R2 to the
potential difference across R2 to the potential difference across R3. That's a
potential difference across R3. That's a slightly challenging question. It's
slightly challenging question. It's actually
actually hard, but it's based on what we just did
hard, but it's based on what we just did earlier. Remember, if this is R1 and
earlier. Remember, if this is R1 and this is
this is R2 and this is now R3, which is in
R2 and this is now R3, which is in series to it, just like the previous 40
series to it, just like the previous 40 40 when he says, hey, what is the ratio
40 when he says, hey, what is the ratio of the voltage of R2 to R3? Uh, sorry,
of the voltage of R2 to R3? Uh, sorry, this is R2. I don't know why I wrote
this is R2. I don't know why I wrote that as R3 and this is R3.
How is the voltage going to get split? Now you might say I don't have values.
Now you might say I don't have values. That's fine. Assume
That's fine. Assume anything. Assume
anything. Assume anything. If this is 10 ohms and 10 ohms
anything. If this is 10 ohms and 10 ohms and 10 ohms, what's the combined
and 10 ohms, what's the combined resistance of R1 to
resistance of R1 to R2? R1 and R2.
R2? R1 and R2. Five. Which means this is technically 5
Five. Which means this is technically 5 to
to 10. And what does he want? He wants the
10. And what does he want? He wants the ratio of the voltage. The ratio of the
ratio of the voltage. The ratio of the voltage is the ratio of the current. So
voltage is the ratio of the current. So 5 to 10 is 1:2. So you can say it's
1:2 or 0.5. That's fine too. It's not an easy question to get. It needs you to
easy question to get. It needs you to have seen questions like this
have seen questions like this before. And the fact that you I can just
before. And the fact that you I can just get, you know, two resistors that are
get, you know, two resistors that are identical. It's half the voltage. So
identical. It's half the voltage. So this gets half, this gets one, and then
this gets half, this gets one, and then it splits. What's the ratio
1:2? Next, all the cells are
Next, all the cells are reversed. Meaning the current now wants
reversed. Meaning the current now wants to
to flow this
flow this way. Wait, if the current wants to flow
way. Wait, if the current wants to flow this way, it cannot flow through R1
this way, it cannot flow through R1 anymore because the diode stops it. So
anymore because the diode stops it. So the currents only flowing through R3 and
the currents only flowing through R3 and R2 which are now technically in what? In
R2 which are now technically in what? In series. R1 doesn't exist now because the
series. R1 doesn't exist now because the current can't go through it. The current
current can't go through it. The current can't go through
can't go through it. Right? Hey, wait a second. If if R1
it. Right? Hey, wait a second. If if R1 goes
goes away, what happens to the total
resistance? It was in parallel. Now it's only in
only in series. Remember when we added things in
series. Remember when we added things in parallel the resistance would decrease.
parallel the resistance would decrease. If you remove the parallel portion the
If you remove the parallel portion the resistance will
resistance will what? Decrease. Sorry increase. The
what? Decrease. Sorry increase. The resistance
resistance increases. You know because you lost
increases. You know because you lost that parallel connection. It's now just
that parallel connection. It's now just series. So the
series. So the current
current decreases. That's very sad.
Then finally, determine the new ratio of the voltage of R2 to
the voltage of R2 to R3. Now, this one should be easy. If you
R3. Now, this one should be easy. If you only have
R2 and R3 in parallel, in series, sorry. And
R3 in parallel, in series, sorry. And they're both the same resistance. The
they're both the same resistance. The voltage will be split
voltage will be split what? equally which as a ratio means
what? equally which as a ratio means it's what? 1
it's what? 1 one. It splits the voltage equally. So
one. It splits the voltage equally. So what's the new ratio? 1
Okay. This was a tough question by the way. Like using ratios and concepts.
way. Like using ratios and concepts. It's a tough question and I picked it on
It's a tough question and I picked it on purpose.
purpose. The final part of this unit or at least
The final part of this unit or at least this section of electricity and we're
this section of electricity and we're done. Let's talk about safety. Now,
done. Let's talk about safety. Now, obviously, obviously, electricity can
obviously, obviously, electricity can kill us. How? Well, it can give us an
kill us. How? Well, it can give us an electric shock. That's bad. And it can
electric shock. That's bad. And it can set us on fire. Not not us directly, but
set us on fire. Not not us directly, but can set everything else on fire.
can set everything else on fire. Like, okay. Can set everything else on
Like, okay. Can set everything else on fire.
fire. So in order to keep ourselves safe, we
So in order to keep ourselves safe, we need a few basic things at home like
need a few basic things at home like insulating wires, using a fuse and so
insulating wires, using a fuse and so on. So let's first take a look at what's
on. So let's first take a look at what's the electricity at home
the electricity at home like an electric
like an electric socket or electricity at home is called
socket or electricity at home is called main's electricity or a main circuit. It
main's electricity or a main circuit. It consists of two main wires and a third
consists of two main wires and a third safety feature. The two main wires are
safety feature. The two main wires are the live
the live wire and the neutral wire. There are no
wire and the neutral wire. There are no positive and negative
positive and negative wires. Why? Because electricity at home
wires. Why? Because electricity at home is always set to 220 volts
is always set to 220 volts AC. Electricity at home is 220 sometimes
AC. Electricity at home is 220 sometimes 240 like it fluctuates a little bit but
240 like it fluctuates a little bit but it's AC which means it doesn't have a
it's AC which means it doesn't have a positive or a negative.
positive or a negative. The live wire is the super high voltage
The live wire is the super high voltage wire that's always fluctuating and the
wire that's always fluctuating and the neutral wire is just there to complete
neutral wire is just there to complete the circuit. This is usually at zero
the circuit. This is usually at zero volts. This means that if I get a piece
volts. This means that if I get a piece of metal and I shove it into just one of
of metal and I shove it into just one of these openings in the socket, if I shove
these openings in the socket, if I shove it into the live wire, I'm a cooked
it into the live wire, I'm a cooked goose. And if I shove it into the
goose. And if I shove it into the neutral wire, I'm aok.
neutral wire, I'm aok. Okay. You and your luck. I don't know
Okay. You and your luck. I don't know which one is live and neutral. We never
which one is live and neutral. We never label them. Electricians and designers
label them. Electricians and designers never label these. Depends on who
never label these. Depends on who connects the wires in the walls. Now the
connects the wires in the walls. Now the earth wire is actually a safety feature.
earth wire is actually a safety feature. Not all the country, not all countries
Not all the country, not all countries have this. This is a safety feature that
have this. This is a safety feature that protects you from getting electrically
protects you from getting electrically shocked if a metal case becomes live.
shocked if a metal case becomes live. But I'll discuss this over here like uh
But I'll discuss this over here like uh we'll talk about the earth wire down
we'll talk about the earth wire down here.
So, as I said, what are the hazards? You can get electrically shocked or you can
can get electrically shocked or you can cause an electric fire. What causes
cause an electric fire. What causes these things? Insulation if it's
these things? Insulation if it's damaged. If you overheat the cables, cuz
damaged. If you overheat the cables, cuz that damages the insulation cuz wires
that damages the insulation cuz wires get too hot, it could melt the
get too hot, it could melt the insulation and it could catch on fire.
insulation and it could catch on fire. Damp conditions means if it's wet,
Damp conditions means if it's wet, obviously you don't charge your phone in
obviously you don't charge your phone in the bathroom. If you do, something's
the bathroom. If you do, something's wrong with you.
wrong with you. uh too much current because too much
uh too much current because too much current will cause the cables and the
current will cause the cables and the sockets to overheat which causes what?
sockets to overheat which causes what? Electric
Electric fires.
fires. Okay. So, what safety features do we
Okay. So, what safety features do we have at home to protect us from these
have at home to protect us from these two main problems? Too much current is
two main problems? Too much current is the reason why things overheat or things
the reason why things overheat or things burn and like you know sockets get
burn and like you know sockets get damaged and everything
damaged and everything else. And to protect you from that, we
else. And to protect you from that, we have a
have a fuse. A fuse is just a very thin wire,
fuse. A fuse is just a very thin wire, by the way. Very thin
by the way. Very thin wire that's always placed on the live
wire that's always placed on the live side of a
side of a circuit. This wire is designed to
circuit. This wire is designed to melt if the current gets too
melt if the current gets too high. So let's say for example, you have
high. So let's say for example, you have a 5 ampere lamp. It uses 5 ampers
a 5 ampere lamp. It uses 5 ampers normally and you close the switch and it
normally and you close the switch and it draws in 5 amp. That's great. It's going
draws in 5 amp. That's great. It's going to work fine. But if the current
to work fine. But if the current increases it'll burn like the lamp will
increases it'll burn like the lamp will burn out. Replace the lamp with any
burn out. Replace the lamp with any device you want. Okay. So what we do is
device you want. Okay. So what we do is we put a fuse over here. A fuse has a
we put a fuse over here. A fuse has a rating. Let's say 6 amp.
rating. Let's say 6 amp. Meaning if the current reaches 6 ampers,
Meaning if the current reaches 6 ampers, it will melt. And when I say melt, I
it will melt. And when I say melt, I don't want you to imagine it slowly
don't want you to imagine it slowly melting away. No, no, no. It just pops
melting away. No, no, no. It just pops right away. Just snaps, breaks
right away. Just snaps, breaks immediately. Okay. So, when you close
immediately. Okay. So, when you close the switch and the current that's
the switch and the current that's flowing through is less than 6 amp, it's
flowing through is less than 6 amp, it's like the normal five, no problem. Fuses
like the normal five, no problem. Fuses like a wire, no problem. But if you
like a wire, no problem. But if you close the switch and for some reason,
close the switch and for some reason, maybe there's an electric surge, maybe
maybe there's an electric surge, maybe somebody's fooled around with the
somebody's fooled around with the switches at home or the wires, whatever
switches at home or the wires, whatever it is, and the current increases for any
it is, and the current increases for any reason, it goes through what first? The
reason, it goes through what first? The fuse and it melts the fuse. This like
fuse and it melts the fuse. This like pops
pops it. So now there is no current that
it. So now there is no current that reaches the light bulb. So the light
reaches the light bulb. So the light bulb turns off, but you kept it
bulb turns off, but you kept it safe. So what we do is if that happens,
safe. So what we do is if that happens, we remove the old fuse, we throw it
we remove the old fuse, we throw it away, we plug in a new fuse, and then we
away, we plug in a new fuse, and then we flip things on again, switch things on
flip things on again, switch things on again. How do I choose a correct rating
again. How do I choose a correct rating for a fuse? You always go for like one
for a fuse? You always go for like one to three ampairs higher than what the
to three ampairs higher than what the device needs. So, for example, if I tell
device needs. So, for example, if I tell you I have an air conditioner that needs
you I have an air conditioner that needs 30 amps to work, well, I had better put
30 amps to work, well, I had better put a
a what? What fuse should I
what? What fuse should I use? Maybe a 32 or a 33
right? Similar to a fuse is a circuit breaker or a trip switch. This is just
breaker or a trip switch. This is just like the fuse. It protects the circuit
like the fuse. It protects the circuit if the current gets too high. If it gets
if the current gets too high. If it gets too high for any reason. But it doesn't
too high for any reason. But it doesn't melt. This time it uses an
melt. This time it uses an electromagnet. We have an electromagnet
electromagnet. We have an electromagnet over here next to what we call an
over here next to what we call an iron switch cuz iron is a magnetic
iron switch cuz iron is a magnetic substance. As long as the current is
substance. As long as the current is low, the magnet doesn't turn on because
low, the magnet doesn't turn on because it's connected to the live wire as well.
it's connected to the live wire as well. But if the current gets too high, the
But if the current gets too high, the current goes through the magnet first.
current goes through the magnet first. It turns on, it magnetizes, and it
It turns on, it magnetizes, and it attracts the
attracts the switch plop, opening it, and therefore
switch plop, opening it, and therefore your circuit doesn't work or your entire
your circuit doesn't work or your entire house doesn't turn
house doesn't turn on. It's exactly the same function as a
on. It's exactly the same function as a fuse. It stops the current if it's gets
fuse. It stops the current if it's gets too high. But this time by opening what?
too high. But this time by opening what? A
A switch using a
magnet. We always choose a rating that's 1 to 3 amps higher than what you need.
1 to 3 amps higher than what you need. Okay? And we also always connect it to
Okay? And we also always connect it to the live wire because if you connect it
the live wire because if you connect it to the neutral wire, this is you cutting
to the neutral wire, this is you cutting out the current on the way out of the
out the current on the way out of the circuit, not on the way in. So the
circuit, not on the way in. So the current's already gone in, burnt your
current's already gone in, burnt your house down, and as the current's going
house down, and as the current's going out, it's like, hey, you want to stop me
out, it's like, hey, you want to stop me now? Sure, go ahead. Your house is
now? Sure, go ahead. Your house is already on fire,
already on fire, though. Okay, that's the circuit
though. Okay, that's the circuit breaker. Now, final question. What's the
breaker. Now, final question. What's the earth wire?
earth wire? The earth wire or sometimes we call it
The earth wire or sometimes we call it the ground wire is a safety feature
the ground wire is a safety feature that's not in all devices and not in all
that's not in all devices and not in all countries either because it's only
countries either because it's only useful if the device you're talking
useful if the device you're talking about has a metal
about has a metal case. So think of a washing machine or a
case. So think of a washing machine or a computer, a PC or a fridge, anything
computer, a PC or a fridge, anything with metal as its outer case.
with metal as its outer case. The wires inside the washing machine,
The wires inside the washing machine, for example, have live and neutral
for example, have live and neutral connections. And if as you connect them,
connections. And if as you connect them, one of the live wires accidentally
one of the live wires accidentally touches the case and
touches the case and you touch the case as
you touch the case as well, the currents going to flow in not
well, the currents going to flow in not to the washing machine, but to you. So,
to the washing machine, but to you. So, you're a nice target. And you light
up. Now, I don't want you to light up. Okay, that's bad. So, what we do is we
Okay, that's bad. So, what we do is we connect a new wire to the metal case
connect a new wire to the metal case that's not part of the
that's not part of the circuit. And we connect it to the ground
circuit. And we connect it to the ground or the earth. When I say ground or
or the earth. When I say ground or earth, I actually mean a big metal rod
earth, I actually mean a big metal rod inside a building. It has to be a
inside a building. It has to be a conductor. We just call it earththing
conductor. We just call it earththing because it's not part of the circuit.
because it's not part of the circuit. So instead of the current going through
So instead of the current going through you that's not a good idea. The current
you that's not a good idea. The current goes through what? The earth instead.
goes through what? The earth instead. Cuz which has a lower resistance? You as
Cuz which has a lower resistance? You as a human being made of flesh and blood
a human being made of flesh and blood and bones and muscles and everything
and bones and muscles and everything else. You've got some resistance by the
else. You've got some resistance by the way. But the earth wire which is made of
way. But the earth wire which is made of copper often or even aluminium has very
copper often or even aluminium has very low resistance. The current's going to
low resistance. The current's going to prefer that over you. Not even a current
prefer that over you. Not even a current wants you.
But that's good otherwise I don't want any
tiger. Now you might be thinking but on its own this means I'm losing
its own this means I'm losing electricity all the time. Well because
electricity all the time. Well because the earth wire has very low resistance
the earth wire has very low resistance it causes the current to spike increase
it causes the current to spike increase a bit increase a lot which causes the
a bit increase a lot which causes the fuse to trip and it's gone.
So, what does it do? What does an earthwire do? It protects you from
earthwire do? It protects you from getting electrically shocked if a metal
getting electrically shocked if a metal case is
case is live. Okay? If something doesn't have a
live. Okay? If something doesn't have a metal case, you don't need a live
metal case, you don't need a live wire. And if you have that earth wire
wire. And if you have that earth wire and a fuse, the fuse will
and a fuse, the fuse will glow.
glow. Okay, let's solve the last couple of
Okay, let's solve the last couple of questions here.
questions here. So, which diagram shows a symbol for a
So, which diagram shows a symbol for a fuse? Yay. D,
fuse? Yay. D, obviously.
obviously. And an electric kettle has a metal
And an electric kettle has a metal casing. The cable for the kettle
casing. The cable for the kettle contains a wire that is connected to the
contains a wire that is connected to the earth of the plug. Which danger does
earth of the plug. Which danger does this guard
this guard against? From the cable getting too hot?
against? From the cable getting too hot? No. From the casing of the kettle
No. From the casing of the kettle becoming live? Absolutely. Because if
becoming live? Absolutely. Because if the casing is live, I get shocked. I've
the casing is live, I get shocked. I've gotten shocked before. It's not a nice
gotten shocked before. It's not a nice feeling at all. The casing of the kettle
feeling at all. The casing of the kettle becoming wet.
becoming wet. No, it's supposed to be wet. The casing
No, it's supposed to be wet. The casing of the kettle overheating. No, that's
of the kettle overheating. No, that's not the issue. The issue is you getting
not the issue. The issue is you getting electrically shocked. So,
electrically shocked. So, be and you'll notice there are no more
be and you'll notice there are no more questions. This last bit, this last
questions. This last bit, this last chapter essentially doesn't show up a
chapter essentially doesn't show up a lot. It's mostly a core part of the
lot. It's mostly a core part of the syllabus, not an extended part. So, it
syllabus, not an extended part. So, it barely shows up, but you know what?
barely shows up, but you know what? shows up in a multiple choice question
shows up in a multiple choice question or two or like maybe a one or two mark
or two or like maybe a one or two mark question paper four it could. So it's
question paper four it could. So it's important to
important to remember and that ladies and gentlemen
remember and that ladies and gentlemen is unit for at least the first half
is unit for at least the first half electricity. X time is magnetus.
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