In the last video, we had this rectangle, and we used a triple

integral to figure out it's volume.

And I know you were probably thinking, well, I could have

just used my basic geometry to multiply the height times

the width times the depth.

And that's true because this was a constant-valued function.

And then even once we evaluated, once we integrated

with respect to z, we ended up with a double integral, which

is exactly what you would have done in the last several videos

when we just learned the volume under a surface.

But then we added a twist at the end of the video.

We said, fine, you could have figured out the volume within

this rectangular domain, I guess, very straightforward

using things you already knew.

But what if our goal is not to figure out the volume?

Our goal was to figure out the mass of this volume, and even

more, the material that we're taking the volume of-- whether

it's a volume of gas or a volume of some solid-- that

its density is not constant.

So now the mass becomes kind of-- I don't know--

interesting to calculate.

And so, what we defined, we defined a density function.

And rho, this p looking thing with a curvy bottom-- that

gives us the density at any given point.

And at the end of the last video we said,

well, what is mass?

Mass is just density times volume.

You could view it another way.

Density is the same thing as mass divided by volume.

So the mass around a very, very small point, and we called that

d mass, the differential of the mass, is going equal the

density at that point, or the rough density at exactly that

point, times the volume differential around that point,

times the volume of this little small cube.

And then, as we saw it on the last video, if you're using

rectangular coordinates, this volume differential could just

be the x distance times the y distance times the z distance.

So, the density was that our density function is defined

to be x, y, and z, and we wanted to figure out the

mass of this volume.

And let's say that our x, y, and z coordinates-- their

values, let's say they're in meters and let's say this

density is in kilograms per meter cubed.

So our answer is going to be in kilograms if that was the case.

And those are kind of the traditional Si units.

So let's figure out the mass of this variably dense volume.

So all we do is we have the same integral up here.

So the differential of mass is going to be this value,

so let's write that down.

It is x-- I want to make sure I don't run out of space.

xyz times-- and I'm going to integrate with

respect to dz first.

But you could actually switch the order.

Maybe we'll do that in the next video.

We'll do dz first, then we'll do dy, then we'll do dx.

Once again, this is just the mass at any small

differential of volume.

And if we integrate with z first we said z goes from what?

The boundaries on z were 0 to 2.

The boundaries on y were 0 to 4.

And the boundaries on x, x went from 0 to 3.

And how do we evaluate this?

Well, what is the antiderivative-- we're

integrating with respect to z first.

So what's the antiderivative of xyz with respect to z?

Well, let's see.

This is just a constant so it'll be xyz squared over 2.

Right?

Yeah, that's right.

And then we'll evaluate that from 2 to 0.

And so you get-- I know I'm going to run out of space.

So you're going to get 2 squared, which is 4,

divided by 2, which is 2.

So it's 2xy minus 0.

So when you evaluate just this first we'll get 2xy, and

now you have the other two integrals left.

So I didn't write the other two integrals down.

Maybe I'll write it down.

So then you're left with two integrals.

You're left with dy and dx.

And y goes from 0 to 4 and x goes from 0 to 3.

I'm definitely going to run out of space.

And now you take the antiderivative of this

with respect to y.

So what's the antiderivative of this with respect to y?

Let me erase some stuff just so I don't get too messy.

I was given the very good suggestion of making it

scroll, but, unfortunately, I didn't make it scroll

enough this time.

So I can delete this stuff, I think.

Oops, I deleted some of that.

But you know what I deleted.

OK, so let's take the antiderivative

with respect to y.

I'll start it up here where I have space.

OK, so the antiderivative of 2xy with respect to y is y

squared over 2, 2's cancel out.

So you get xy squared.

And y goes from 0 to 4.

And then we still have the outer integral to do.

x goes from 0 to 3 dx.

And when y is equal to 4 you get 16x.

And then when y is 0 the whole thing is 0.

So you have 16x integrated from 0 to 3 dx.

And that is equal to what?

8x squared.

And you evaluate it from 0 to 3.

When it's 3, 8 times 9 is 72.

And 0 times 8 is 0.

So the mass of our figure-- the volume we figured out last

time was 24 meters cubed.

I erased it, but if you watched the last video

that's what we learned.

But it's mass is 72 kilograms.

And we did that by integrating this 3 variable density

function-- this function of 3 variables.

Or in three-dimensions you can view it as a

scalar field, right?

At any given point, there is a value, but not

really a direction.

And that value is a density.

But we integrated the scalar field in this volume.

So that's kind of the new skill we learned with

the triple integral.

And in the next video I'll show you how to set up more

complicated triple integrals.

But the real difficulty with triple integrals is-- and I

think you'll see that your calculus teacher will often do

this-- when you're doing triple integrals, unless you have a

very easy figure like this, the evaluation-- if you actually

wanted to analytically evaluate a triple integral that has more

complicated boundaries or more complicated for example,

a density function.

The integral gets very hairy, very fast.

And it's often very difficult or very time consuming to

evaluate it analytically just using your traditional

calculus skills.

So you'll see that on a lot of calculus exams when they start

doing the triple integral, they just want you to set it up.

They take your word for it that you've done so many integrals

so far that you could take the antiderivative.

And sometimes, if they really want to give you something more

difficult they'll just say, well, switch the order.

You know, this is the integral when we're dealing with

respect to z, then y, then x.

We want you to rewrite this integral when

you switch the order.

And we will do that in the next video.

See you soon.