Find the moments in the x-axis and y-axis and the center of mass with respect of
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Answer:
we consider centers of mass (also called centroids, under certain conditions) and moments. The basic idea of the center of mass is the notion of a balancing point. Many of us have seen performers who spin plates on the ends of sticks. The performers try to keep several of them spinning without allowing any of them to drop. If we look at a single plate (without spinning it), there is a sweet spot on the plate where it balances perfectly on the stick. If we put the stick anywhere other than that sweet spot, the plate does not balance and it falls to the ground. (That is why performers spin the plates; the spin helps keep the plates from falling even if the stick is not exactly in the right place.) Mathematically, that sweet spot is called the center of mass of the plate.
In this section, we first examine these concepts in a one-dimensional context, then expand our development to consider centers of mass of two-dimensional regions and symmetry. Last, we use centroids to find the volume of certain solids by applying the theorem of Pappus.
Center of Mass and Moments
Let’s begin by looking at the center of mass in a one-dimensional context. Consider a long, thin wire or rod of negligible mass resting on a fulcrum, as shown in Figure 6.6.1a. Now suppose we place objects having masses m1 and m2 at distances d1 and d2 from the fulcrum, respectively, as shown in Figure 6.6.1b.
This figure has two images. The first image is a horizontal line on top of an equilateral triangle. It represents a rod on a fulcrum. The second image is the same as the first with two squares on the line. They are labeled msub1 and msub2. The distance from msub1 to the fulcrum is dsub1. The distance from msub2 to the fulcrum is dsub2.
Figure 6.6.1: (a) A thin rod rests on a fulcrum. (b) Masses are placed on the rod.
The most common real-life example of a system like this is a playground seesaw, or teeter-totter, with children of different weights sitting at different distances from the center. On a seesaw, if one child sits at each end, the heavier child sinks down and the lighter child is lifted into the air. If the heavier child slides in toward the center, though, the seesaw balances. Applying this concept to the masses on the rod, we note that the masses balance each other if and only if m1d1=m2d2.
This figure is an image of the x-axis. On the axis there is a point labeled x bar. Also on the axis there is a point xsub1 with a square above it. Inside of the square is the label msub1. There is also a point xsub2 on the axis. Above this point there is a square. Inside of the square is the label msub2.
Figure 6.6.2: The center of mass
ˉ
x
is the balance point of the system.
In the seesaw example, we balanced the system by moving the masses (children) with respect to the fulcrum. However, we are really interested in systems in which the masses are not allowed to move, and instead we balance the system by moving the fulcrum. Suppose we have two point masses, m1 and m2, located on a number line at points x1 and x2, respectively (Figure 6.6.2). The center of mass,
ˉ
x
, is the point where the fulcrum should be placed to make the system balance.
Thus, we have
m1|x1−
ˉ
x
|=m2|x2−
ˉ
x
| m1(
ˉ
x
−x1)=m2(x2−
ˉ
x
) m1
ˉ
x
−m1x1=m2x2−m2
ˉ
x
ˉ
x
(m1+m2)=m1x1+m2x2
or
ˉ
x
=
m1x1+m2x2
m1+m2
The expression in the numerator of Equation 6.6.1, m1x1+m2x2, is called the first moment of the system with respect to the origin. If the context is clear, we often drop the word first and just refer to this expression as the moment of the system. The expression in the denominator, m1+m2, is the total mass of the system. Thus, the center of mass of the system is the point at which the total mass of the system could be concentrated without changing the moment.
This idea is not limited just to two point masses. In general, if n masses, m1,m2,…,mn, are placed on a number line at points x1,x2,…,xn, respectively, then the center of mass of the system is given by
ˉ
x
=
n
∑
i=1 mixi
n
∑
i=1 mi
