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Example 2

Find the center of mass of a cone of constant density with height h and base a circle of radius b.

Step 1

The region is sketched in Figure 12.7.10.

12_multiple_integrals-407.gif

Figure 12.7.10

Step 2

Put the origin at the center of the base and let the z-axis be the axis of the cone. E is the cylindrical region

0 ≤ θ ≤ 2π, 0 ≤ r ≤ b, 0 ≤ z ≤ h - (h/b)r.

Step 3

Let the density be 1.

12_multiple_integrals-404.gif

12_multiple_integrals-405.gif

Since the cone is symmetric about the z-axis, x = 0 and y = 0.

12_multiple_integrals-406.gif

The point (x, y, z) is shown in Figure 12.7.11.

 

12_multiple_integrals-408.gif

Figure 12.7.11

To express a point P(x, y, z) in spherical coordinates we let ρ (rho) be the distance from the origin to P, let θ be the same angle as in cylindrical coordinates, and let φ be the angle between the positive z-axis and the line OP. Note that φ can always be chosen between 0 and n.

12_multiple_integrals-409.gif

Figure 12.7.12

We see from Figure 12.7.12 that a point (x, y, z) has spherical coordinates (θ, φ, ρ) if x = ρ sin φ cos θ, y = ρ sin φ sin θ, z = ρ cos θ.

The graph of the equation ρ = constant is a sphere with center at the origin (hence the name spherical coordinates). The graph of φ = constant is a vertical cone with vertex at the origin. The graph of θ = constant is a half-plane through the z-axis. These surfaces are shown in Figure 12.7.13.

12_multiple_integrals-410.gif

Figure 12.7.13

DEFINITION

A spherical region E is a region in (x, y, z) space given by spherical coordinate inequalities

α1 ≤ θ ≤ α2, β1(θ) ≤ φ ≤ β2(θ), c1(θ, φ) ≤ ρ ≤ c2(θ, φ),

where all the functions are continuous. To avoid overlaps we also require that for (θ, φ, ρ) in E,

0 ≤ θ ≤ 2π, 0 ≤ φ ≤ π, 0 ≤ ρ.

A spherical box is a spherical region of the simple form

α1 ≤ θ ≤ α2, β1 ≤ φ ≤ β2, c1 ≤ ρ ≤ c2.

The θ-boundaries are planes, the θ-boundaries are portions of cone surfaces, and the ρ-boundaries are portions of spherical surfaces. Figure 12.7.14 shows a spherical box.

12_multiple_integrals-411.gif

Figure 12.7.14

The spherical box

0 ≤ θ ≤ 2π, 0 ≤ φ ≤ π, 0 ≤ ρ ≤ c

is a sphere of radius c with center at the origin. The spherical box

0 ≤ θ ≤ 2π, 0 ≤ φβ, 0 ≤ ρ ≤ c

is a cone whose vertex is at the origin and whose top is spherical instead of flat. (See Figure 12.7.15.)

12_multiple_integrals-412.gif12_multiple_integrals-413.gif

Figure 12.7.15

Another important example is the spherical region

0 ≤ 0 ≤ 2π, 0 ≤ φ ≤ π/2, 0 ≤ ρ ≤ c cos φ,

which is a sphere of radius ½c whose center is on the z-axis at z = ½c (Figure 12.7.16).

12_multiple_integrals-414.gif

Figure 12.7.16

When integrating over a solid region E made up of spheres or cones, it is often easiest to use spherical coordinates.

SPHERICAL INTEGRATION FORMULA

Let E be a spherical region

α1 ≤ 0 ≤ α2, β1 ≤ φ ≤ β2(θ), cl(θ,φ) ≤ ρ ≤ c2 (θ, φ).

The triple integral of f(x, y, z) over E is

12_multiple_integrals-415.gif

In practice we make the substitution

f(x, y, z) = f(ρ sin φ cos θ, ρ sin φ sin θ, ρ cos φ)

before integrating.

PROOF

Let C be the region in the rectangular (θ, φ, ρ) space which has the same inequalities as E. We prove

12_multiple_integrals-416.gif

As usual we let f(x, y, z) > θ on E and put

12_multiple_integrals-417.gif

12_multiple_integrals-418.gif

Figure 12.7.17 Spherical Element of Volume

Consider an element of volume ΔC. As we see from Figure 12.7.17, ΔC corresponds to a spherical box ΔE. ΔE is almost a rectangular box with sides

Δρ, ρ Δφ, ρ sin (φ) Δθ

and volume

ρ2 sin φ Δθ Δφ Δρ.

Thus B(ΔC) ≈ f(x, y, z)ρ2 sin φ Δθ Δφ Δρ (compared to Δθ Δφ Δρ). By the Infinite Sum Theorem

12_multiple_integrals-419.gif

and by definition

12_multiple_integrals-420.gif

The triple integral for volume,

12_multiple_integrals-421.gif

gives us iterated integral formulas for volume in rectangular, cylindrical, and spherical coordinates.

Rectangular 12_multiple_integrals-422.gif

Cylindrical 12_multiple_integrals-423.gif

Spherical 12_multiple_integrals-424.gif

The rectangular formula is really equivalent to the double integral for the volume between two surfaces. Similarly, the cylindrical formula is equivalent to the double integral in polar coordinates for the volume between two surfaces.

On the other hand, the volume formula in spherical coordinates is something new which is useful for finding volumes of spherical regions.


Last Update: 2010-11-25