Question Video: Finding the Coordinates of the Center of Gravity of a Nonuniform Rectangular Lamina | Nagwa Question Video: Finding the Coordinates of the Center of Gravity of a Nonuniform Rectangular Lamina | Nagwa

Question Video: Finding the Coordinates of the Center of Gravity of a Nonuniform Rectangular Lamina Mathematics

A uniform rectangular lamina has a length of 63 cm and a width of 59 cm. It is divided into three equal-sized rectangles along its length; the last of these rectangles has been folded over so that it lies flat on the middle rectangle as shown. Find the coordinates of the center of gravity of the lamina in this form.

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Video Transcript

A uniform rectangular lamina has a length of 63 centimeters and a width of 59 centimeters. It is divided into three equal-sized rectangles along its length. The last of these rectangles has been folded over so that it lies flat on the middle rectangle as shown. Find the coordinates of the center of gravity of the lamina in this form.

Remember, a lamina is a two-dimensional shape of negligible thickness. The lamina in question is uniform. This means essentially that its mass is evenly distributed throughout the shape. In fact, for a uniform lamina, the center of mass of the body is the geometric center of the body.

Now, we have a little problem here though. This third rectangle is folded over so that it rests on the second rectangle. This means that the mass of the shape created is not evenly distributed in the ๐‘ฅ-direction. It is, however, still evenly distributed in the ๐‘ฆ-direction. And so the ๐‘ฆ-coordinate of our center of mass will lie exactly halfway along the line segment ๐ด๐ท. This means that the ๐‘ฆ-coordinate of the center of mass or center of gravity will be half of 59; itโ€™s 59 over two. But how do we find the ๐‘ฅ-coordinate of the center of gravity?

Well, if we think about the rectangular lamina as being separated into three equally sized rectangles of masses ๐‘š sub one, ๐‘š sub two, and ๐‘š sub three, where ๐‘ฅ sub one, ๐‘ฅ sub two, and ๐‘ฅ sub three are their center of gravities in the ๐‘ฅ-direction, then the ๐‘ฅ-coordinate of our center of gravity will be the sum of ๐‘š sub one, ๐‘ฅ sub one; ๐‘š sub two, ๐‘ฅ sub two; and ๐‘š sub three, ๐‘ฅ sub three divided by the total mass of the system.

Letโ€™s deal with the first rectangle, the one furthest to the left. This is a uniform rectangle. And so we know its center of mass will be at a point exactly halfway along the shape. Dividing 63 by three gives us 21. So the width of each of our rectangles is 21 centimeters. And so the ๐‘ฅ-coordinate of the center of gravity of this first shape is 21 over two. The center of mass of the remaining two rectangles will lie at exactly the same point. This will be 21 plus 21 over two units from ๐ด, and thatโ€™s 63 over two. So we have the ๐‘ฅ-coordinates of the center of gravity of each of our three rectangles.

But what do we do about their mass? Since the shape is uniform and divided into three equally sized rectangles, then we can define the mass of each of our rectangles as being equal. And in fact we can let that be equal to one. So the ๐‘ฅ-coordinate of our center of gravity will be one times 21 over two plus one times 63 over two plus one times 63 over two. And weโ€™ll divide this by the total mass of our system, which is one plus one plus one; thatโ€™s three.

Note at this point that we couldโ€™ve dealt slightly differently with our second and third rectangles. We could instead have considered this to be a rectangle double the mass of the first rectangle. This wouldโ€™ve still resulted in a value of two times 63 over two and a total mass of three. So weโ€™ll get the same answers either way. And this gives us a value of 49 over two. Since we measured this value from point ๐ด, which lies at the origin, we have the coordinates of the center of gravity. The coordinates of the center of gravity are 49 over two, 59 over two.

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