A triple integral adds up f(x, y, z) times volume over a solid region E. With f = 1 it gives the volume of E; with f a density it gives the mass. Over a box, Fubini's theorem allows any of six orders. Over a solid between two surfaces z = u₁(x, y) and z = u₂(x, y), the innermost integral runs up a vertical column from the lower surface to the upper one, and the remaining double integral covers the shadow of E on the xy-plane. Dividing moments by the mass locates the center of mass.
A double integral adds up a quantity spread over a flat region. A triple
integral adds up a quantity spread through a solid. Cut a solid region E
into small boxes of volume ΔV, multiply f at a point of each box by
ΔV, and add. The limit as the boxes shrink is
∭Ef(x,y,z)dV=lim∑f(xi∗,yj∗,zk∗)ΔV
With f=1, the sum counts boxes, and the integral is the volume of E.
When f is a density, in mass per unit volume, each term is the mass of one
box, and the integral is the mass of E.
Over a box [a,b]×[c,d]×[p,q], Fubini’s theorem works as it
did for rectangles: the triple integral equals an iterated integral in any
of six orders, all with constant limits.
Suppose E lies between a lower surface z=u1(x,y) and an upper surface
z=u2(x,y), over a region D of the xy-plane, its shadow. Group the
small boxes into vertical columns. The column over the point (x,y) runs
from u1(x,y) up to u2(x,y), so the column’s total is a single integral
in z. Adding the columns over D is then a double integral:
∭EfdV=∬D[∫u1(x,y)u2(x,y)f(x,y,z)dz]dA
Set up the limits from the inside out: first the column, from the bottom
surface to the top one, then the shadow D, described as in
double integrals over general regions.
With f=1, the inner integral is u2−u1, the height of the column,
and the formula becomes the familiar volume between two surfaces.
If a solid has density ρ(x,y,z), its mass is m=∭EρdV. Its
center of mass is the balance point, (xˉ,yˉ,zˉ), where
xˉ=m1∭ExρdV,yˉ=m1∭EyρdV,zˉ=m1∭EzρdV
Each coordinate is a weighted average, in the sense of the
average value of a function, with
density as the weight. For a constant density the center of mass is the
centroid, a purely geometric point.
Evaluate ∭ExdV, where E is the wedge 0≤x≤2, 0≤y≤1, 0≤z≤y.
Answer
1
Full solution
∫02∫01∫0yxdzdydx=∫02xdx⋅∫01ydy=2⋅21=1.
Set up, without evaluating, a triple integral for the volume of the solid between the paraboloid z=x2+y2 and the plane z=4.
Answer
∫−22∫−4−x24−x2∫x2+y24dzdydx
Full solution
Columns run from the paraboloid up to the plane. They exist where x2+y2≤4, the disk of radius 2, so the shadow is that disk. The next lesson evaluates this volume, 8π, in cylindrical coordinates.
The tetrahedron of Example 2 has constant density. Find xˉ.
Hint
The centroid of a tetrahedron is the average of its four corners.
Answer
41
Full solution
The corners are (0,0,0), (1,0,0), (0,2,0) and (0,0,3), and the average of their x-coordinates is 41. Example 4 confirmed this pattern for the tetrahedron with corners on the unit axes. By integration, ∭ExdV=∫01x⋅43(2−2x)2dx=3∫01x(1−x)2dx=41, and the volume is 1.
A student writes the volume of the tetrahedron x+y+z≤1 as ∫01−x−y∫01−x∫01dxdydz. What went wrong?
Answer
The limits are listed in reverse: the constant limits must go on the outer integral, not the inner one.
Full solution
With dx innermost, the x-limits come first, and here they are 0 to 1, while the outer z-limits contain x and y. A correct version is ∫01∫01−x∫01−x−ydzdydx=61.
Frequently asked questions
What does a triple integral measure?
It adds up f(x, y, z) times volume over a solid. With f = 1 it is the volume of the solid; with f a density, in mass per unit volume, it is the total mass.
How do you set up the limits of a triple integral?
For a solid between surfaces z = u₁(x, y) below and z = u₂(x, y) above, the z-limits are u₁ and u₂. The remaining double integral runs over the shadow of the solid on the xy-plane, with limits found as for any double integral.
In how many orders can a triple integral be written?
Six: dz dy dx, dz dx dy, dy dz dx, dy dx dz, dx dz dy and dx dy dz. Over a box all six give the same value with constant limits; over other solids the limits change with the order.
How do you find the center of mass of a solid?
Divide each first moment by the mass. For example, x-bar is the triple integral of x times the density, divided by the triple integral of the density.
Why is a triple integral not a volume in four dimensions?
It can be read that way, but the useful readings are physical: a total amount of something spread through a solid, such as mass, charge or heat.