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Find the center of gravity of the square lamina with vertices \((0,0),(1,0),(0,1)\), and \((1,1)\) if (a) the density is proportional to the square of the distance from the origin; (b) the density is proportional to the distance from the \(y\) axis.

Short Answer

Expert verified
(a) Center at \( (\frac{9}{16}, \frac{9}{16}) \); (b) Center at \( (\frac{2}{3}, \frac{1}{2}) \).

Step by step solution

01

Identify the Problem

We need to find the center of gravity of a square lamina given two different density functions. The vertices of the square lamina are \(0,0\), \(1,0\), \(0,1\), and \(1,1\).
02

Density Function - (a)

For part (a), the density is proportional to the square of the distance from the origin, so we set \[ ho(x, y) = k(x^2 + y^2) \] where \(k\) is a constant.
03

Density Center - (a)

To find the center \(\bar{x}, \bar{y}\), use the formulas \((\bar{x} = \frac{\iint x \rho(x, y) \, dA}{\iint \rho(x, y) \, dA})\) and similar for \(\bar{y}\). Calculate \[ \bar{x} = \frac{\int_0^1\int_0^1 x(x^2 + y^2) \, dx \, dy}{\int_0^1\int_0^1 (x^2 + y^2) \, dx \, dy} \] \[ \bar{y} = \frac{\int_0^1\int_0^1 y(x^2 + y^2) \, dx \, dy}{\int_0^1\int_0^1 (x^2 + y^2) \, dx \, dy} \]
04

Calculate Integrals - (a)

Compute the integrals: 1. \[ \int_0^1\int_0^1 (x^3 + xy^2) \, dx \, dy = \frac{1}{4} + \frac{1}{8} = \frac{3}{8} \]2. \[ \int_0^1\int_0^1 (x^2 + y^2) \, dx \, dy = \frac{1}{3} + \frac{1}{3} = \frac{2}{3} \]Substitute back to find \(\bar{x}\): \(\bar{x} = \frac{\frac{3}{8}}{\frac{2}{3}} = \frac{9}{16} \\bar{y} = \bar{x} = \frac{9}{16}\)
05

Density Function - (b)

For part (b), the density is proportional to the distance from the \(y\) axis, so we set \[ ho(x, y) = kx \] where \(k\) is a constant.
06

Density Center - (b)

Use the formulas again for density proportional to the \(x\): \((\bar{x} = \frac{\iint x \rho(x, y) \, dA}{\iint \rho(x, y) \, dA})\) and similar for \(\bar{y}\). Compute: \[ \bar{x} = \frac{\int_0^1\int_0^1 x^2 \, dx \, dy}{\int_0^1\int_0^1 x \, dx \, dy} \] \[ \bar{y} = \frac{\int_0^1\int_0^1 xy \, dx \, dy}{\int_0^1\int_0^1 x \, dx \, dy} \]
07

Calculate Integrals - (b)

Compute the integrals: 1. \[ \int_0^1\int_0^1 x^2 \, dx \, dy = \frac{1}{3} \]2. \[ \int_0^1\int_0^1 x \, dx \, dy = \frac{1}{2} \]3. \[ \int_0^1\int_0^1 xy \, dx \, dy = \frac{1}{4} \]Substitute back to find \(\bar{x}\): \(\bar{x} = \frac{\frac{1}{3}}{\frac{1}{2}} = \frac{2}{3} \\bar{y} = \frac{\frac{1}{4}}{\frac{1}{2}} = \frac{1}{2}\)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Center of Gravity
The center of gravity is a critical point in any object where the entire weight can be considered to act. For a lamina, this means it's just like finding a balance point. In this exercise, we are asked to explore this concept for a square lamina that has vertices at
  • (0,0), (1,0), (0,1), and (1,1).
This square lies in the plane. The center of gravity is determined using density functions and mathematical calculations involving integrals. Knowing the center of gravity is helpful in many real-world applications, like engineering and physics.

When the density of the lamina varies as a function of position, finding the center of gravity requires us to use calculus. This is because each part of the lamina contributes differently to the overall weight due to differing densities. Therefore, calculating where this "middle point" lies involves integrating across the entire area of the lamina. By using integrals, we accumulate small contributions over the lamina's surface. Thus, moving closer to finding the center of gravity for complex shapes.
Density Functions
Density functions tell us how much mass is in a small part of an object compared to its volume. Here, we're dealing with a square lamina, and the problem gives us different density functions to consider.
  • For part (a), the density function is proportional to the square of the distance from the origin, given by \( \rho(x, y) = k(x^2 + y^2) \).
  • In part (b), it's proportional to the distance from the \(y\) axis, or \( \rho(x, y) = kx \).
These equations indicate how density varies over the lamina. When density depends on distance, it means that different parts of the object weigh differently even if they occupy the same area. Such functions are critical in helping us calculate parameters like center of gravity.

By incorporating these density functions into our integration process, we efficiently find the distribution of mass and subsequently calculate other necessary results, like where the center of gravity might lie.
Double Integrals
Double integrals are used when we deal with functions involving two variables, like in this problem where coordinates \((x, y)\) are involved. They help integrate over two-dimensional areas, providing the tools to calculate needed quantities across surfaces or shapes.

  • In part (a), we use double integrals to process a density varying with \((x^2 + y^2)\). This requires calculating two double integrals, one for \(x\)-coordinate and one for \(y\)-coordinate, using limits that match the lamina's boundaries (0 to 1 for both x and y).
  • For part (b), the calculations involve density x-dependent equality \( kx \).
By integrating across the area of the square lamina, we accumulate contributions weighted by density. This helps find the precise location of the center of gravity.

Double integrals, by involving two steps of integration, offer greater depth and allow resolving multidimensional problems like calculating the center of gravity for irregularly shaped and non-uniformly dense bodies. Essentially, they are foundational tools in calculus, enabling us to deal with the added complexity of real-world shapes and functions.

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Most popular questions from this chapter

For single-variable definite integrals, the technique of substitution was generally used to simplify the integrand. Discuss some motivations for using a change of variables in a multiple integral.

The tendency of a lamina to resist a change in rotational motion about an axis is measured by its moment of inertia about that axis. If a lamina occupies a region \(R\) of the \(x y\) -plane, and if its density function \(\delta(x, y)\) is continuous on \(R\), then the moments of inertia about the \(x\) -axis, the \(y\) -axis, and the \(z\) -axis are denoted by \(I_{x}, I_{y}\), and \(I_{z}\), respectively, and are defined by $$\begin{aligned}&I_{x}=\iint_{R} y^{2} \delta(x, y) d A, \quad I_{y}=\iint_{R} x^{2} \delta(x, y) d A \\\&I_{z}=\iint_{R}\left(x^{2}+y^{2}\right) \delta(x, y) d A \end{aligned}$$ Use these definitions. Consider the rectangular lamina that occupies the region described by the inequalities \(0 \leq x \leq a\) and \(0 \leq y \leq b .\) Assuming that the lamina has constant density \(\delta\), show that $$I_{x}=\frac{\delta a b^{3}}{3}, \quad I_{y}=\frac{\delta a^{3} b}{3}, \quad I_{z}=\frac{\delta a b\left(a^{2}+b^{2}\right)}{3}$$

Use cylindrical coordinates to find the centroid of the solid. The solid that is bounded by the cone \(z=\sqrt{x^{2}+y^{2}}\) and the plane \(z=2\).

Use spherical coordinates to find the volume of the solid. The solid within the sphere \(x^{2}+y^{2}+z^{2}=9\), outside the cone \(z=\sqrt{x^{2}+y^{2}}\), and above the \(x y\) -plane.

Suppose that the density at a point in a gaseous spherical star is modeled by the formula $$\delta=\delta_{0} e^{-(\rho / R)^{3}}$$ where \(\delta_{0}\) is a positive constant, \(R\) is the radius of the star, and \(\rho\) is the distance from the point to the star's center. Find the mass of the star.

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