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Triple Integrals 2

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    In the last video, we had this
    rectangle, and we used a triple
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    integral to figure
    out it's volume.
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    And I know you were probably
    thinking, well, I could have
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    just used my basic geometry
    to multiply the height times
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    the width times the depth.
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    And that's true because this
    was a constant-valued function.
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    And then even once we
    evaluated, once we integrated
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    with respect to z, we ended up
    with a double integral, which
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    is exactly what you would have
    done in the last several videos
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    when we just learned the
    volume under a surface.
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    But then we added a twist
    at the end of the video.
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    We said, fine, you could have
    figured out the volume within
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    this rectangular domain, I
    guess, very straightforward
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    using things you already knew.
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    But what if our goal is not
    to figure out the volume?
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    Our goal was to figure out the
    mass of this volume, and even
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    more, the material that we're
    taking the volume of-- whether
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    it's a volume of gas or a
    volume of some solid-- that
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    its density is not constant.
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    So now the mass becomes
    kind of-- I don't know--
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    interesting to calculate.
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    And so, what we defined, we
    defined a density function.
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    And rho, this p looking thing
    with a curvy bottom-- that
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    gives us the density
    at any given point.
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    And at the end of the
    last video we said,
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    well, what is mass?
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    Mass is just density
    times volume.
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    You could view it another way.
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    Density is the same thing
    as mass divided by volume.
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    So the mass around a very, very
    small point, and we called that
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    d mass, the differential of the
    mass, is going equal the
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    density at that point, or the
    rough density at exactly that
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    point, times the volume
    differential around that point,
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    times the volume of this
    little small cube.
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    And then, as we saw it on the
    last video, if you're using
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    rectangular coordinates, this
    volume differential could just
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    be the x distance times the y
    distance times the z distance.
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    So, the density was that our
    density function is defined
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    to be x, y, and z, and we
    wanted to figure out the
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    mass of this volume.
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    And let's say that our x, y,
    and z coordinates-- their
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    values, let's say they're in
    meters and let's say this
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    density is in kilograms
    per meter cubed.
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    So our answer is going to be in
    kilograms if that was the case.
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    And those are kind of the
    traditional Si units.
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    So let's figure out the mass of
    this variably dense volume.
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    So all we do is we have the
    same integral up here.
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    So the differential of mass
    is going to be this value,
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    so let's write that down.
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    It is x-- I want to make sure
    I don't run out of space.
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    xyz times-- and I'm
    going to integrate with
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    respect to dz first.
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    But you could actually
    switch the order.
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    Maybe we'll do that
    in the next video.
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    We'll do dz first, then we'll
    do dy, then we'll do dx.
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    Once again, this is just
    the mass at any small
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    differential of volume.
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    And if we integrate with z
    first we said z goes from what?
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    The boundaries on
    z were 0 to 2.
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    The boundaries on
    y were 0 to 4.
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    And the boundaries on
    x, x went from 0 to 3.
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    And how do we evaluate this?
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    Well, what is the
    antiderivative-- we're
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    integrating with
    respect to z first.
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    So what's the antiderivative
    of xyz with respect to z?
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    Well, let's see.
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    This is just a constant so
    it'll be xyz squared over 2.
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    Right?
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    Yeah, that's right.
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    And then we'll evaluate
    that from 2 to 0.
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    And so you get-- I know I'm
    going to run out of space.
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    So you're going to get
    2 squared, which is 4,
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    divided by 2, which is 2.
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    So it's 2xy minus 0.
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    So when you evaluate just this
    first we'll get 2xy, and
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    now you have the other
    two integrals left.
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    So I didn't write the
    other two integrals down.
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    Maybe I'll write it down.
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    So then you're left
    with two integrals.
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    You're left with dy and dx.
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    And y goes from 0 to 4
    and x goes from 0 to 3.
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    I'm definitely going
    to run out of space.
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    And now you take the
    antiderivative of this
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    with respect to y.
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    So what's the antiderivative
    of this with respect to y?
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    Let me erase some stuff just
    so I don't get too messy.
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    I was given the very good
    suggestion of making it
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    scroll, but, unfortunately,
    I didn't make it scroll
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    enough this time.
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    So I can delete this
    stuff, I think.
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    Oops, I deleted some of that.
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    But you know what I deleted.
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    OK, so let's take
    the antiderivative
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    with respect to y.
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    I'll start it up here
    where I have space.
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    OK, so the antiderivative of
    2xy with respect to y is y
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    squared over 2, 2's cancel out.
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    So you get xy squared.
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    And y goes from 0 to 4.
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    And then we still have the
    outer integral to do.
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    x goes from 0 to 3 dx.
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    And when y is equal
    to 4 you get 16x.
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    And then when y is 0
    the whole thing is 0.
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    So you have 16x integrated
    from 0 to 3 dx.
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    And that is equal to what?
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    8x squared.
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    And you evaluate
    it from 0 to 3.
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    When it's 3, 8 times 9 is 72.
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    And 0 times 8 is 0.
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    So the mass of our figure-- the
    volume we figured out last
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    time was 24 meters cubed.
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    I erased it, but if you
    watched the last video
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    that's what we learned.
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    But it's mass is 72 kilograms.
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    And we did that by integrating
    this 3 variable density
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    function-- this function
    of 3 variables.
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    Or in three-dimensions
    you can view it as a
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    scalar field, right?
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    At any given point, there
    is a value, but not
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    really a direction.
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    And that value is a density.
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    But we integrated the scalar
    field in this volume.
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    So that's kind of the new
    skill we learned with
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    the triple integral.
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    And in the next video I'll
    show you how to set up more
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    complicated triple integrals.
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    But the real difficulty with
    triple integrals is-- and I
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    think you'll see that your
    calculus teacher will often do
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    this-- when you're doing triple
    integrals, unless you have a
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    very easy figure like this, the
    evaluation-- if you actually
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    wanted to analytically evaluate
    a triple integral that has more
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    complicated boundaries or more
    complicated for example,
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    a density function.
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    The integral gets very
    hairy, very fast.
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    And it's often very difficult
    or very time consuming to
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    evaluate it analytically just
    using your traditional
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    calculus skills.
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    So you'll see that on a lot of
    calculus exams when they start
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    doing the triple integral, they
    just want you to set it up.
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    They take your word for it that
    you've done so many integrals
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    so far that you could
    take the antiderivative.
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    And sometimes, if they really
    want to give you something more
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    difficult they'll just say,
    well, switch the order.
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    You know, this is the integral
    when we're dealing with
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    respect to z, then y, then x.
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    We want you to rewrite
    this integral when
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    you switch the order.
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    And we will do that
    in the next video.
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    See you soon.
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Title:
Triple Integrals 2
Description:

Using a triple integral to find the mass of a volume of variable density.

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Video Language:
English
Duration:
07:26
brettle edited English subtitles for Triple Integrals 2 Apr 18, 2011, 12:32 AM
brettle edited English subtitles for Triple Integrals 2 Apr 18, 2011, 12:32 AM
brettle edited English subtitles for Triple Integrals 2 Apr 18, 2011, 12:32 AM
brettle edited English subtitles for Triple Integrals 2 Mar 2, 2011, 5:45 PM
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Amara Bot edited English subtitles for Triple Integrals 2 Mar 2, 2011, 5:45 PM
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