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Coulomb's law | Physics | Khan Academy

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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.
  • 11:07 - 11:08
    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
  • 12:49 - 12:53
    behind how it manifests as
    most of these daily forces
  • 12:53 - 12:54
    that we encounter in life.
  • 12:54 - 12:56
    I find that absolutely beautiful.
Title:
Coulomb's law | Physics | Khan Academy
Description:

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Video Language:
English
Team:
Khan Academy
Duration:
12:57

English subtitles

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