Problem of the Week #132 - October 6th, 2014

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SUMMARY

The problem presented involves calculating the center of gravity of a square lamina defined by the vertices (0,0), (1,0), (0,1), and (1,1), with density proportional to the square of the distance from the origin. The mass of the lamina is determined using the double integral of the density function, resulting in a mass of m = (2k/3). The moments about the axes are calculated to be M_y = (5k/12) and M_x = (5k/12), confirming the symmetry of the lamina. Consequently, the center of gravity is found to be at the coordinates (5/8, 5/8).

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Here's this week's problem!

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Problem: Find the center of gravity of the square lamina with vertices $(0,0)$, $(1,0)$, $(0,1)$ and $(1,1)$ if the density is proportional to the square of the distance from the origin.

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This week's problem was correctly answered by MarkFL. You can find his solution below.

[sp][box=blue]We define the mass of the lamina by the double integral:

$$m=\iint\limits_{R}\rho(x,y)\,dA\tag 1$$​

We define the coordinates of the center of mass (or gravity) of the lamina by:

$$\overline{x}=\frac{M_y}{m}\quad\overline{y}=\frac{M_x}{m}\tag 2$$​

where:

$$M_y=\iint\limits_{R}x\rho(x,y)\,dA\quad\text{ and }\quad M_x=\iint\limits_{R}y\rho(x,y)\,dA\tag 3$$​

are the moments of the lamina about the $y$- and $x$-axes respectively.[/box]

For this problem, we are told:

$$\rho(x,y)=k\left(x^2+y^2\right)$$

And so, using (1) we find that the mass $m$ of the given lamina is:

$$m=k\iint\limits_{R} x^2+y^2\,dA=k\int_0^1\int_0^1 x^2+y^2\,dx\,dy=k\int_0^1\left[\frac{x^3}{3}+xy^2\right]_0^1\,dy=k\int_0^1\frac{1}{3}+y^2\,dy=k\left[\frac{1}{3}y+\frac{1}{3}y^3\right]_0^1=\frac{2k}{3}$$

Now, using (3), we find:

$$M_y=k\iint\limits_{R} x^3+xy^2\,dA=k\int_0^1\int_0^1 x^3+xy^2\,dx\,dy=k\int_0^1\left[\frac{x^4}{4}+\frac{x^2}{2}y^2\right]_0^1\,dy=\frac{k}{4}\int_0^1 2y^2+1\,dy=\frac{k}{4}\left[\frac{2}{3}y^2+y\right]_0^1=\frac{5k}{12}$$

$$M_x=k\iint\limits_{R} yx^2+y^3\,dA=k\int_0^1\int_0^1 yx^2+y^3\,dx\,dy=k\int_0^1\left[y\frac{x^3}{3}+xy^3\right]_0^1\,dy=\frac{k}{3}\int_0^1 3y^3+y\,dy=\frac{k}{3}\left[\frac{3}{4}y^4+\frac{y^2}{2}\right]_0^1=\frac{5k}{12}$$

As we would expect, the moments of the lamina are the same, given the symmetry of the lamina about the line $y=x$, and so we would expect that the center of gravity would lie on this line.

Hence, by (2), we find:

$$\overline{x}=\overline{y}=\frac{\dfrac{5k}{12}}{\dfrac{2k}{3}}=\frac{5}{8}$$

Thus, we find that the center of gravity of the given lamina is:

$$(\overline{x},\overline{y})=\left(\frac{5}{8},\frac{5}{8}\right)$$[/sp]
 

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