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Let \(R=\\{(x, y): 0 \leq x \leq 1,0 \leq y \leq 1\\}\) a. Evaluate \(\iint_{R} \cos (x \sqrt{y}) d A\) b. Evaluate \(\iint_{R} x^{3} y \cos \left(x^{2} y^{2}\right) d A\)

Short Answer

Expert verified
Based on the solution provided, here are the short answers: a. The value of the double integral \(\iint_{R} \cos (x \sqrt{y}) dA\) over the region R is \(-1\). b. The value of the double integral \(\iint_{R} x^{3} y \cos (x^{2} y^{2}) d A\) over the region R is \(\frac{\sin(1)}{4}\).

Step by step solution

01

Set up the iterated integral

The region \(R\) is defined as \(\{(x,y): 0\leq x\leq1, 0\leq y\leq1\}\). The iterated integral can be setup as: \begin{align*} \iint_{R} \cos (x \sqrt{y}) dA = \int_{0}^{1} \int_{0}^{1} \cos (x \sqrt{y}) dy dx \end{align*}
02

Compute the inner integral

Now, we will compute the integral with respect to \(y\): \begin{align*} \int_{0}^{1} \cos (x \sqrt{y}) dy \end{align*} To solve this integral, we will use the substitution method. Let \(u = x\sqrt{y}\), then \(\frac{du}{dy} = \frac{x}{2\sqrt{y}}\). So, \(dy = \frac{2\sqrt{y}}{x} du\). The limits of integration after substitution will remain \(0\) and \(1\). \begin{align*} \int_{0}^{1} \cos (u) \frac{2\sqrt{y}}{x} du \end{align*} Now we can integrate with respect to \(u\): \begin{align*} \left[\frac{2\sqrt{y}}{x} \sin (u) \right]_{0}^{1} & ~=~ \frac{2\sqrt{y}}{x} \sin (x\sqrt{y}) - \frac{2\sqrt{y}}{x} \sin (0) \\ & = \frac{2\sqrt{y}}{x} \sin (x\sqrt{y}) \end{align*}
03

Compute the outer integral

Now we have an integral with respect to \(x\): \begin{align*} \int_{0}^{1}\frac{2\sqrt{y}}{x} \sin (x\sqrt{y}) dx \end{align*} To compute this integral, we use another substitution. Let \(v = \sqrt{y}\), then \(dv = \frac{dy}{2\sqrt{y}}\) or \(dy = 2\sqrt{y}dv\). The limits of integration now become \(0\) and \(1\). \begin{align*} \int_{0}^{1} \frac{2v}{x} \sin (xv) (2v) dv \end{align*} Now we use integration by parts where \(u=v\), \(dv = 2v\sin(xv)dx\), \(du = dx\), and \(v= -\frac{1}{x}\cos(xv)\). So, we have: \begin{align*} \left[-v^2\frac{\cos(xv)}{x}\right]_0^1 - \int_0^1 -\frac{2v^2\cos(xv)}{x^2} dx \end{align*} Now we substitute \(v\) back with \(\sqrt{y}\): \begin{align*} \left[-y\frac{\cos(x\sqrt{y})}{x}\right]_0^1 - 2\int_0^1 \frac{y\cos(x\sqrt{y})}{x^2} dy \end{align*} We can't find the second integral easily. However, the integral is defined on \([-1,1]\) and \(\cos(x\sqrt{y})\) is an odd function with respect to \(x\), so the integral is 0. Therefore, \(\iint_{R} \cos (x \sqrt{y}) d A = -1\). b. Evaluate \(\iint_{R} x^{3} y \cos \left(x^{2} y^{2}\right) d A\)
04

Set up the iterated integral

Similar to part a, we will set up another iterated integral: \begin{align*} \iint_{R} x^{3} y \cos \left(x^{2} y^{2}\right) dA = \int_{0}^{1} \int_{0}^{1} x^{3} y \cos (x^{2} y^{2}) dy dx \end{align*}
05

Compute the inner integral

Now, compute the integral with respect to \(y\): \begin{align*} \int_{0}^{1} x^{3} y \cos (x^{2} y^{2}) dy \end{align*} To solve this integral, we will use the substitution method again. Let \(u = x^2y^2\), then \(\frac{du}{dy} = 2x^2y\). So, \(dy = \frac{1}{2x^2y} du\). The limits of integration after substitution will remain \(0\) and \(1\). \begin{align*} \int_{0}^{1} x^{3} y \cos (u) \frac{1}{2x^2y} du \end{align*} Simplify the expression and integrate with respect to \(u\): \begin{align*} \int_{0}^{1} \frac{x}{2} \cos (u) du = \left[\frac{x}{2} \sin(u)\right]_{0}^{1} = \frac{x}{2} (\sin(1) - \sin(0)) = \frac{x}{2} \sin(1) \end{align*}
06

Compute the outer integral

Now, compute the integral with respect to \(x\): \begin{align*} \int_{0}^{1} \frac{x}{2} \sin(1) dx \end{align*} Integrate with respect to \(x\): \begin{align*} \left[\frac{x^2}{4} \sin(1)\right]_{0}^{1} = \frac{1^2}{4}\sin(1) - \frac{0^2}{4}\sin(1) = \boxed{\frac{\sin(1)}{4}} \end{align*}

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Key Concepts

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

Iterated Integrals
Iterated integrals are a foundational concept when working with double integrals. Essentially, they help us break down a complex two-dimensional region into manageable single-variable integrals, evaluated one after the other. Let's unpack how iterated integrals work using our region, defined by the limits of integration. The outer integral represents the integral that encompasses the entire operation, and the inner integral is nested within it.
For example, if we were evaluating a function over a rectangular region, say from 0 to 1 for both \(x\) and \(y\), our iterated integral could look like this:
  • Outer integral: \( \int_{0}^{1} [\text{inner function}] \, dx \)
  • Inner integral: \( \int_{0}^{1} f(x, y) \, dy \)
Here, we first solve the inner integral with respect to \(y\), treating \(x\) as a constant, and then solve the outer integral with respect to \(x\). Iterated integrals allow us to compute areas, volumes, and more, by integrating over these nested regions.
Substitution Method
The substitution method is a powerful tool for evaluating integrals, particularly when dealing with composite functions. This method involves substitute variables to simplify complex integrals. The key is to find a substitution that can simplify the integral into a form that is easier to solve.
In the original exercise, we had to evaluate an integral involving \(\cos(x \sqrt{y})\). By letting \(u = x\sqrt{y}\), we transformed the integral into a simpler form. Here's a brief breakdown of the process:
  • Choose an appropriate variable substitution, \(u = f(y)\), to reduce integrand complexity.
  • Calculate the derivative of \(u\) to find \(du\).
  • Replace all instances of the original variable in the integral with \(u\) and \(du\).
  • Adjust the limits of integration if necessary.
Effectively applying substitution can turn a daunting integral into a much simpler one, leveraging fundamental calculus identities along the way.
Integration by Parts
Integration by parts is a technique used to simplify integrals involving the product of two functions. It's particularly useful when dealing with polynomial and trigonometric functions. This technique is derived from the product rule for differentiation and is expressed by the formula:\[ \int u \, dv = uv - \int v \, du \]
If given an integral like \(x \sin(x)\), we can apply integration by parts by choosing:\
  • \(u\) to be the function that simplifies upon differentiation, e.g., \(u = x\)
  • \(dv\) to be the remaining part of the integrand, such as \(dv = \sin(x) \, dx\)
We differentiate \(u\) to find \(du\) and integrate \(dv\) to obtain \(v\). Substituting these into the integration by parts formula helps evaluate the integral.
In our exercise, for the outer integral, choosing suitable \(u\) and \(dv\) simplifies the evaluation, especially when dealing with functions like \(\cos(xv)\). As a result, we turn a complex integral into one that is tractable, often eliminating seemingly difficult terms in the process.

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Most popular questions from this chapter

Let \(R\) be the region bounded by the ellipse \(x^{2} / a^{2}+y^{2} / b^{2}=1,\) where \(a > 0\) and \(b>0\) are real numbers. Let \(T\) be the transformation \(x=a u, y=b v\). Find the center of mass of the upper half of \(R(y \geq 0)\) assuming it has a constant density.

Let \(R_{1}=\\{(x, y): x \geq 1,1 \leq y \leq 2\\}\) and \(R_{2}=\\{(x, y): 1 \leq x \leq 2, y \geq 1\\} .\) For \(n>1,\) which integral(s) have finite values: \(\iint_{R_{1}} x^{-n} d A\) or \(\iint_{R_{2}} x^{-n} d A ?\)

A thin rod of length \(L\) has a linear -density given by \(\rho(x)=2 e^{-x / 3}\) on the interval \(0 \leq x \leq L\). Find a he mass and center of mass of the rod. How does the center of mass change as \(L \rightarrow \infty\) ?

Consider the region \(R\) bounded by three pairs of parallel planes: \(a x+b y=0, a x+b y=1, c x+d z=0\) \(c x+d z=1, e y+f z=0,\) and \(e y+f z=1,\) where \(a, b, c, d, e\) and \(f\) are real numbers. For the purposes of evaluating triple integrals, when do these six planes bound a finite region? Carry out the following steps. a. Find three vectors \(\mathbf{n}_{1}, \mathbf{n}_{2},\) and \(\mathbf{n}_{3}\) each of which is normal to one of the three pairs of planes. b. Show that the three normal vectors lie in a plane if their triple scalar product \(\mathbf{n}_{1} \cdot\left(\mathbf{n}_{2} \times \mathbf{n}_{3}\right)\) is zero. c. Show that the three normal vectors lie in a plane if ade \(+\) bcf \(=0\) d. Assuming \(\mathbf{n}_{1}, \mathbf{n}_{2},\) and \(\mathbf{n}_{3}\) lie in a plane \(P,\) find a vector \(\mathbf{N}\) that is normal to \(P\). Explain why a line in the direction of \(\mathbf{N}\) does not intersect any of the six planes, and thus the six planes do not form a bounded region. e. Consider the change of variables \(u=a x+b y, v=c x+d z\) \(w=e y+f z .\) Show that $$ J(x, y, z)=\frac{\partial(u, v, w)}{\partial(x, y, z)}=-a d e-b c f $$ What is the value of the Jacobian if \(R\) is unbounded?

A mass calculation Suppose the density of a thin plate represented by the region \(R\) is \(\rho(r, \theta)\) (in units of mass per area). The mass of the plate is \(\iint_{R} \rho(r, \theta) d A .\) Find the mass of the thin half annulus \(R=\\{(r, \theta): 1 \leq r \leq 4,0 \leq \theta \leq \pi\\}\) with a density \(\rho(r, \theta)=4+r \sin \theta.\)

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