Triple Integrals
Pre: Interpretation of Integrals
There's no good way to visualize triple integrals, unless there is no integrand, in which case, we have
If
then the integral is just the mass, and
Suppose the domain of integration can be described as
The integral of
Evaluate
where
solution
$$ \int_{0}^1 \left(\int_{0}^{1 - y} \left[ \int_{0}^{1 - x - y} z \, dz \right] \, dx \right)\, dy = \frac{1}{24} $$The domain of integration is always the "biggest" part of the shape. This is pretty obvious when you think about it.
Notice that our integrals evaluate to a number, because they follow this pattern:
Every time we integrate, we reduce the dimension by one. From the example above, for our first integral, we're integrating over a 3-D region on a 2-D domain. Next, we're integrating over a 2-D region on a 1-D domain. Finally, we're integrating over a 1-D region with a domain consisting of a point.
Evaluate
solution
The integrand has no
Next, we integrate on
We don't use
Finally,
now we will apply change of variable to change to Polar Coordinates:
Using Cylindrical Coordinates
Taking the last example, we convert to Cylindrical Coordinates, except our y-axis is the "Cartesian part".
First, finding the Jacobian:
Since
Mount Fuji is an approximately conical mountain 3800m tall and radius 19000m with a mass density of
solution
Recall the formula for work:
we have:
so
We need our bounds
Taking the edge of the cone on the yz-plane:
Now, generalizing this for all
Since we have
Plugging this back into our integral:
Using Spherical Coordinates
Calculate the volume of
solution
Simplifying the bounds:
Taking our equation
Why?
- For
, we're technically dependent on and , but doesn't matter since it's a circle. So our radius depends on the angle of the "arm", and using a right-angled triangle, we get . - For
, we're going all the way around the sphere, so we know right away it's - For
, we go from a flat line to a vertical line, which is , or
Now, using substitution, let: