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- [Instructor] We encounter
so many different kinds
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of forces in our day-to-day lives.
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There's gravity, there's
the tension force,
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friction, air resistance,
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spring force, buoyant forces,
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and so on and so forth, but guess what?
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Not all these forces are fundamental.
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Gravity is certainly
one of the fundamental
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forces of nature,
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but turns out that most other forces
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that we encounter in our daily life
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are actually a manifestation
of the electromagnetic forces.
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These are the forces
responsible for all the electric
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and magnetic phenomena and
most of the other forces
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that we encounter in everyday life,
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but how do electromagnetic
forces give rise
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to all of these?
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Well, let's get a glimpse
of that in this video.
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Now, there are two parts to these forces,
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the electric part and the magnetic part.
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We will save the magnetic
part for future videos.
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In this video, we'll just
stick to electric part of it,
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and even there, we'll talk
about a particular kind
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of electric force,
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which you call the electrostatic forces.
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Electrostatic,
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which we also call static electricity.
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from the word itself, you can see electro
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means we're taking to electric part,
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and static means stationary,
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where things are not moving a lot,
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or maybe they're moving very slowly.
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The reason to do that is because
we wanna take baby steps.
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So first, we'll consider what happens
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when we have static conditions,
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then we'll see what happens
when they're moving,
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and so on and so forth, okay?
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All right.
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So, when it comes to gravity,
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we'll keep comparing with gravity,
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'cause we are familiar with gravity, okay?
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When it comes to gravity,
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where does the force of gravity come from?
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What is it due to?
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Well, we know that the
force of gravity comes
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from a fundamental property
of matter, which we call mass.
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Things that have mass will produce
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gravitational force on each other, right?
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Similarly, what causes
electrostatic force?
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Well, turns out electronic force comes
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from a property of matter called,
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you've probably heard of this, charge.
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Anything that has charge will put forces
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on other things that have charge.
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Now, an immediate question
that we could have
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is, hey, if that is the case,
and if matter has charge,
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and because of the charge,
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they put electrostatic
forces on each other,
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why don't we notice that?
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Why don't we notice electrostatic
forces between, say,
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planets and stars, and
all of those things?
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Why don't we notice that in everyday life?
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Well, first of all, we do
notice them in everyday life,
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and which we will see in
this particular video,
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but the reason why we don't
notice them on a large scale
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is, well, it's a good question,
and we'll come back to that.
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But anyways, if you want
to see electrostatic
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forces in action,
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it's better to start looking at things
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inside the atom, so, let's do that.
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We've probably seen the model of an atom.
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We have the nucleus at the center,
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which contains protons and neutrons,
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and we all have, you know,
kind of like an electron cloud
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that surrounds a nucleus,
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where you have electrons over there.
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Now, these particles will have charge.
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Protons have a positive charge,
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neutrons are neutral, they have no charge,
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and electrons have a negative charge.
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Okay, but we may be wondering,
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how much charge do protons
and electrons have?
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To answer that question, we need to know
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the unit of the charge.
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Just like how mass has
a unit of kilograms,
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charge has a unit of
something called the Coulomb,
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named after the scientist,
Charles Coulomb,
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who did a lot of work on this,
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and same way we use is capital C.
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Now, it turns out that
protons and electrons
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have the same magnitude of the charge.
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They have different signs, but
they have the same magnitude,
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and we call that that number, e,
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and that happens to be roughly 1.602
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times 10 to the power -19 Coulombs,
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so, it's a very tiny value
in terms of Coulombs.
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And so, we would now say
that the charge on the proton
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is this much positive,
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so, we'll just call it +1e.
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The charge on the electron
is this much negative,
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so, -1e,
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and the charge on the
neutron, well, that is zero.
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It has no charge, so,
its charge is just zero.
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And now, we can immediately
see a big difference
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between mass and charge.
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Mass, there's only one kind,
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but charge, there are two
kinds, positives and negatives,
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and this will now help
us understand something.
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An atom has the same number
of protons and electrons,
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so, the total charge of the
atoms would just be zero,
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because the charge of the proton
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and charge of the electron
will just cancel out,
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and so, the atom itself will be neutral.
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And so, if you consider big objects,
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which has billions and billions of atoms,
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it's pretty much neutral,
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because the total number of
protons is pretty much the same
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as total number of electrons,
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and that's the reason
why most things around us
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are uncharged,
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or they might have a few
extra electrons or protons,
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so will have a very tiny
charge, but mostly uncharged,
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and that's why we don't
see electrostatic forces
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in action most of the time.
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That's why at celestial scales,
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we don't see electrostatic
forces in action,
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because they're mostly uncharged,
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or they have very tiny charge,
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but at the microscopic
level, we do see it.
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We see protons putting
forces on other protons,
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and other electrons of the
same atom, of a different atom.
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They're all there,
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but if you want to study these forces,
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the next big question we should ask
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is what is the strength of this force?
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How much force would,
say, a proton would put
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on, say, another proton, or
maybe on another electron?
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How do we figure that out?
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Well, for that, let's assume
that we have two, in general,
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let's consider two charged particles.
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Let's call these charges as q1 and q2.
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You can imagine, for example,
these are two pieces of paper,
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and, you know, these pieces of paper
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have some extra electrons, or
some extra protons, let's say.
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So, they are charged,
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so, they will put an
electrostatic force on each other.
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The question we wanna try to answer
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is what is the direction of that force,
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and what is the strength of that force?
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What does that depend on?
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Let's start with the
direction of the force.
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Positives will push and
repel other positives.
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Negatives will push and
repel other negatives.
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In other words, like charges
will repel on each other,
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but unlike charges will
attract each other.
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A proton will attract an electron.
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Positives will attract negatives.
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So, the direction of the force
depends upon their charge,
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the polarity of that charge.
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If both are positive or both
are negative, they will repel.
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If one is positive, the
other one is negative,
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they will attract.
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For simplicity, let's just assume one.
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Let's just just say
that both are positive,
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then they would repel each other.
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So, this is a repulsive
electrostatic force.
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Another big question is
what does the strength
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of this force depend on?
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Why don't you pause the video,
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and just think about how you
think they would be related
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to q1 and q2, the charges,
and the distance between them?
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Okay, since the electrostatic
forces come from the charges,
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we would expect that these
forces must be directly related
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to q1 and q2.
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If either of them increase,
we would expect the force
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to increase.
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And how would it be
related to the distance?
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Well, if you put them farther away,
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well, we expect the
force to become smaller.
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If you put them very far
away, we would expect them
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to not interact with
each other at all, right?
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On the other hand, if
we bring them closer,
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that means if you make this smaller,
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the distance to be smaller,
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you would expect the force to be larger.
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Closer they are, larger the force,
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which means you would expect
an inwards relationship
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with the distance between them.
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Now, if you put it all together,
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we'll get something
called the Coulomb's Law,
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and that looks like this.
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Notice the Coulomb's Law
is giving us something
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very similar to what we predicted.
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It is, directly, the force
between the two charges
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is directly related to
the charges themselves,
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you can see that,
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and it is inversely related
to the distance between them.
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And more importantly,
you can see an inverse
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square relationship.
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Where have we seen an inverse
square relationship before?
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Hey, we've seen it in gravity.
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We've seen the force of gravity,
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the universal law of
gravitation is very similar.
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Over here, G, which we call
the universal constant,
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its value was about this much.
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So, what is the value of K,
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which we call the Coulomb's constant?
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Well, it turns out that the value
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of the Coulomb's constant, K, is about,
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is about 8.99 times 10
to the power 9 units.
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And can you work out the units yourself?
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Well, we just have to
isolate K on one side,
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and if you do that, let
me do that very quickly,
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we'll get F times R squared
divided by q1 and q2,
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so, that will be F is newtons,
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R squared is meter squared,
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divided by q1 and q2 is Coulombs squared.
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Yeah, I don't have to remember them.
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I never remember them,
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because I can always rearrange
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and then figure out what the units are,
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but that's the value of K.
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And now that you know this,
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if you know the value of the charges,
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and you know how far they are,
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we can plug in and figure
out the force between them.
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Okay, so, let's quickly compare these two.
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Well, the one similarity
is the inverse square law.
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The farther you put
them, the farther you go,
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the smaller the force gets, the
force dies out very quickly,
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but what about some differences?
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Well, the first difference
is you can see gravity
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is always attractive,
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but the electrostatic force
can be attractive or repulsive.
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That's because we have two kinds
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of charges over here, right?
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But there's another thing that we can see.
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Look at the value of K.
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It's much bigger compared
to the value of G
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in standard units.
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From this, we can kind of
guess that the Coulomb's Law
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is much, much stronger
than the force of gravity,
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which means, if you take,
for example, two protons,
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and compare the force of gravity
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with the electrostatic
force, the Coulomb's force,
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you'll find the Coulomb's
force to be way stronger,
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orders of magnitude stronger
than the force of gravity.
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And so, that's why at
this microscopic scale,
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we can completely ignore
the force of gravity.
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It's the electronic force that dominates,
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but as we saw, once we
go at a much more larger
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celestial scale,
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well, now, the masses are so huge,
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and the charges are so
small that the force
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of gravity dominates.
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I absolutely love this, how the, you know,
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at different scale, the
different forces dominates,
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and now, we are in a
position to understand that.
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That's incredible, isn't it?
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But that's not all.
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Now, we are in a position to
answer our original question,
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how electromagnetic forces
or electrostatic forces
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get manifested as some of
the daily forces that we see?
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For example, tension, where
does tension come from?
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Well, if you had to zoom into a string,
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you'll see a lot of, you
know, atoms over there.
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And although atoms are neutral,
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since because they have
positives and negatives inside,
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they can push and pull on other, you know,
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electrons and protons.
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For example, the protons can
push on the other protons,
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the protons can pull on the electrons,
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the electrons over here can
push on the other electrons,
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the electrons over here
can pull on the protons,
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so, there are a lot of forces out there,
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and, you know, we can model
and say that, you know,
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pretty much all these forces balance out.
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They have to, because,
look, a string is, you know,
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pretty much static,
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so, you can assume that most of the atoms
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are pretty much static,
so, they are all balanced,
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and therefore, the net
force on all of the atoms
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are pretty much zero.
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We say they're in equilibrium.
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Now, what happens when
you pull on the string?
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Let's say, you put a mass on, you know,
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attach a mass over here,
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and because of gravity,
it pulls on the string.
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Well, now, because of that pull,
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some of the atoms will
start moving farther away
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from each other.
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Equilibrium gets disturbed.
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Net force is no longer zero.
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It turns out for the string,
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because the equilibrium gets disturbed,
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and the atoms go away from each other,
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the net force will try
to bring them closer
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back to each other,
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and that is how tension force
is generated in a string.
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Isn't that wonderful?
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It all comes from the
electrostatic forces.
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Similarly, think about
where does the force
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of friction come from?
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Well, again, if we were
to zoom in over here,
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we will see that, you know,
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although things look
smooth at a macroscale,
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on a microscopic scale,
things are not really smooth,
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and if we zoom in even further, again,
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we will notice that the atoms of the box
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can interact with the atoms of the floor
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via other electrostatic forces,
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and it's these electrostatic
forces which all add up
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and puts, you know, and it all adds up,
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and gives rise to the force of friction.
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Again, it is super complicated.
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We'll not try to understand
exactly how the force
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of friction comes, why it opposes, say,
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the force of, you know,
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why it opposes motion, for
example, in some cases,
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but it all comes from
the electrostatic forces.
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And we can use the same
idea, the same model
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to explain spring forces, air resistances,
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buoyant forces, pretty
much contact forces,
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other contact forces
that you pretty much see
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in your daily life,
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and I find it absolutely fascinating
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that even though these
models are not very accurate,
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I mean, today, we have
better, more accurate models,
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what we call quantum mechanical models
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to explain all these phenomena better,
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but even if we ignore that,
even if we consider, you know,
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simpler models, like
we are doing over here,
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we can just use the idea
of electrostatic forces,
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the Coulomb's forces to
try and get an intuition
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behind how it manifests as
most of these daily forces
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that we encounter in life.
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I find that absolutely beautiful.