Calculus Volume 1

Chapter 6 | Applications of Integration

709

and right by the lines x = a and x = b , respectively. Let ρ denote the density of the associated lamina. Then we can make the following statements: i. The mass of the lamina is (6.18) m = ρ ∫ f ( x ) dx . ii. The moments M x and M y of the lamina with respect to the x - and y -axes, respectively, are a b

(6.19)

b ⎡

dx and M y = ρ ∫ a b

⎤ ⎦ 2

⎣ f ( x )

M x = ρ ∫

xf ( x ) dx .

2

a

⎝ x – , y –

iii. The coordinates of the center of mass ⎛

⎞ ⎠ are

M y m and y

(6.20)

– = M x m .

x – =

In the next example, we use this theorem to find the center of mass of a lamina.

Example 6.31 Finding the Center of Mass of a Lamina

Let R be the region bounded above by the graph of the function f ( x ) = x and below by the x -axis over the interval [0, 4]. Find the centroid of the region.

Solution The region is depicted in the following figure.

Figure 6.67 Finding the center of mass of a lamina.

Since we are only asked for the centroid of the region, rather than the mass or moments of the associated lamina, we know the density constant ρ cancels out of the calculations eventually. Therefore, for the sake of convenience, let’s assume ρ =1. First, we need to calculate the total mass: m = ρ ∫ f ( x ) dx = ∫ 4 xdx

a b

0

x 3/2 |

0 4

16

= 2 3

= 2 3 [8−0] =

3 .

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