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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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