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Find \(\iint_{D} \frac{(x-y)^{2}}{(x+y)^{2}} d x d y,\) where \(D\) is the square with vertices \((2,0),(4,2),(2,4),\) and (0,2) .

Short Answer

Expert verified
The integral evaluates to 0 due to symmetry.

Step by step solution

01

Define the Region

The region of integration, denoted as \(D\), is a square with vertices at \((2,0), (4,2), (2,4), (0,2)\). This implies a symmetrical square with diagonals intersecting at the origin shifted by \((2,2)\).
02

Change Variables

Use the transformation: let \(u = x - y\) and \(v = x + y\). This simplifies the process by diagonalizing the integration region. Express \(x\) and \(y\) in terms of \(u\) and \(v\): \(x = \frac{u+v}{2}\) and \(y = \frac{v-u}{2}\).
03

Determine Jacobian of Transformation

Calculate the Jacobian of the transformation: \(J = \left| \frac{\partial(x, y)}{\partial(u, v)} \right| = \left| \begin{array}{cc} 1/2 & 1/2 \ -1/2 & 1/2 \end{array} \right| = \frac{1}{2}\).
04

Rewrite the Integral

The integral \(\iint_{D} \frac{(x-y)^{2}}{(x+y)^{2}} dx dy\) becomes \(\iint_{D'} \frac{u^{2}}{v^{2}} \cdot \frac{1}{2} du dv \).
05

Determine Limits of Integration

The region \(D\) transforms to a parallelogram in the \(uv\)-plane. The limits for \(v\) are from 2 to 6, and for \(u\), it is bounded by the lines \(-v+2\) and \(v-2\).
06

Integrate with Respect to u

Calculate the inner integral \(\int_{-v+2}^{v-2} \frac{1}{2} \cdot \frac{u^{2}}{v^{2}} \, du = \frac{1}{6v^{2}}[(v-2)^{3} - (-v+2)^{3}]\).
07

Simplify and Integrate w.r.t v

After simplifying the integral with respect to \(u\), compute the outer integral with respect to \(v\): \[\int_{2}^{6} \frac{1}{6v^{2}}[(v-2)^{3} - (-v+2)^{3}] \, dv\], then evaluate.
08

Evaluate and Solve

Compute the definite integral and conclude that the integral equals zero given the symmetry of the function in the region.

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Key Concepts

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

Transformation of Variables
When solving double integrals, it's often useful to simplify the region of integration by transforming variables. This technique is called the transformation of variables and it helps in changing the coordinates to make complex integration regions simpler.

For instance, in our exercise, we transformed variables by setting:
  • \( u = x - y \)
  • \( v = x + y \)
Using these transformations allows us to describe the integration region more easily. The original square, defined with vertices, is transformed into a parallelogram in the new coordinate system.

The transformation makes it easier to handle the integration because the complexity of the region's shape is reduced.
Jacobian Determinant
In transforming coordinate systems, the Jacobian determinant is crucial because it accounts for the change in area (or volume, in higher dimensions) resulting from the transformation.

For the transformation in our exercise, where
  • \( u = x - y \)
  • \( v = x + y \)
we calculate the Jacobian as the determinant of the matrix formed by the partial derivatives of the new variables with respect to the old ones:\[J = \left| \begin{array}{cc} \frac{\partial x}{\partial u} & \frac{\partial x}{\partial v} \\frac{\partial y}{\partial u} & \frac{\partial y}{\partial v} \end{array} \right| = \left| \begin{array}{cc} \frac{1}{2} & \frac{1}{2} \-\frac{1}{2} & \frac{1}{2} \end{array} \right| = \frac{1}{2}.\]The Jacobian value of \(\frac{1}{2}\) indicates how the area is scaled in the transformation. This factor is essential in altering the differential area from \(dx \times dy\) to \(du \times dv\).
Limits of Integration
Determining the limits of integration is essential when transferring the integral to a new set of variables. After transforming to the \(uv\) plane using the transformation, the original square region is mapped onto a parallelogram.

To find the new limits:
  • The variable \(v\) has the limits of 2 to 6, determined by the transformed equations of the square's boundaries.
  • The variable \(u\) is bound between \(-v + 2\) and \(v - 2\).
Setting these correct limits ensures you're integrating over the correct area in the new coordinate plane.

Properly understanding and determining these limits is fundamental when using a transformation of variables.
Definite Integrals
A definite integral calculates the exact area under a curve within specified bounds. In double integration, you are finding the volume under a surface. After transforming the variables and setting the new limits, the original problem becomes easier to solve.

The integrand in this example is converted to \(\frac{u^2}{v^2}\) due to the variable transformation. We first integrate with respect to \(u\), and then with respect to \(v\). For the inner integral:\[\int_{-v+2}^{v-2} \frac{1}{2} \cdot \frac{u^2}{v^2} \, du = \frac{1}{6v^2}[(v-2)^3 - (-v+2)^3]\]This result is then used in the outer integral:\[\int_{2}^{6} \frac{1}{6v^2}[(v-2)^3 - (-v+2)^3] \, dv\]Finally, you compute the definite integral to find the solution.

In our problem, symmetry in the region yields a final integral value of zero, which simplifies interpretation.

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Most popular questions from this chapter

Let \(a\) and \(b\) be positive real numbers. Find the area of the region \(\frac{x^{2}}{a^{2}}+\frac{y^{2}}{b^{2}} \leq 1\) inside an ellipse by using the change of variables \(T(u, v)=(a u, b v) .\) (Recall from Chapter 5 that Area \(\left.(D)=\iint_{D} 1 d A .\right)\).

In this exercise, we evaluate the improper one-variable integral \(\int_{-\infty}^{\infty} e^{-x^{2}} d x\) by following the unlikely strategy of relating it to an improper double integral that turns out to be more tractable. Let \(a\) be a positive real number. (a) Let \(R_{a}\) be the rectangle \(R_{a}=[-a, a] \times[-a, a] .\) Show that: $$ \iint_{R_{a}} e^{-x^{2}-y^{2}} d x d y=\left(\int_{-a}^{a} e^{-x^{2}} d x\right)^{2}. $$ (b) Let \(D_{a}\) be the disk \(x^{2}+y^{2} \leq a^{2}\). Use polar coordinates to evaluate \(\iint_{D_{a}} e^{-x^{2}-y^{2}} d x d y\). (c) Note that, as \(a\) goes to \(\infty\), both \(R_{a}\) and \(D_{a}\) fill out all of \(\mathbb{R}^{2}\). It is true that both \(\lim _{a \rightarrow \infty} \iint_{R_{a}} e^{-x^{2}-y^{2}} d x d y\) and \(\lim _{a \rightarrow \infty} \iint_{D_{a}} e^{-x^{2}-y^{2}} d x d y\) exist and that they are equal. Their common value is the improper integral \(\iint_{\mathbb{R}^{2}} e^{-x^{2}-y^{2}} d x d y\). Use this information along with your answers to parts (a) and (b) to show that: $$ \int_{-\infty}^{\infty} e^{-x^{2}} d x=\sqrt{\pi}. $$

Let \(W\) be the wedge-shaped solid in \(\mathbb{R}^{3}\) that lies under the plane \(z=y,\) inside the cylinder \(x^{2}+y^{2}=1,\) and above the \(x y\) -plane. Find the centroid of \(W\).

Find \(\iint_{D} \cos \left(x^{2}+y^{2}\right) d x d y\), where \(D\) is the region described by \(4 \leq x^{2}+y^{2} \leq 16\).

Find \(\iiint_{W} \frac{z}{\left(3+x^{2}+y^{2}\right)^{2}} d x d y d z\) if \(W\) is the region in \(\mathbb{R}^{3}\) given by \(x^{2}+y^{2}+z^{2} \leq 1\) and \(z \geq 0\). (Hint: The proper coordinate system and order of integration can make a difference.).

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