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Evaluate the following integrals. $$\iint_{R} \frac{x y}{1+x^{2}+y^{2}} d A ; R=\\{(x, y): 0 \leq y \leq x, 0 \leq x \leq 2\\}$$

Short Answer

Expert verified
Question: Find the double integral of the function \(f(x, y) = \frac{xy}{1+x^2+y^2}\) over the region R, where \(0 \leq y \leq x\) and \(0 \leq x \leq 2\). Answer: The double integral of the function \(f(x, y)\) over the specified region R is given by: $$\frac{1}{2} \left[ 2^2\left(\ln(9) - \ln(5)\right) - \int_{0}^{2}\left(\frac{2x^3 dx}{1 + 2x^2} - \frac{2x^3 dx}{1 + x^2}\right)\right]$$

Step by step solution

01

Determine the limits of integration

Based on the given region R, we have the following inequalities for x and y: \(0 \leq y \leq x\) and \(0 \leq x \leq 2\). We will integrate first with respect to y and then with respect to x. So, the limits for y are from 0 to x, and the limits for x are from 0 to 2: $$\int_{0}^{2} \int_{0}^{x} \frac{x y}{1+x^{2}+y^{2}} dy dx$$
02

Compute the inner integral

Integrate the given function with respect to y: $$\int_{0}^{x} \frac{x y}{1+x^{2}+y^{2}} dy$$ We can use the substitution method: let \(u = 1 + x^2 + y^2\), then \(du = 2y dy\). So \(dy = \frac{du}{2y}\) Now, the integral becomes: $$\frac{x}{2} \int_{1+x^2}^{1+2x^2} \frac{1}{u} du$$ Solving this integral, we get: $$\frac{x}{2} \left[\ln{u}\right]_{1+x^2}^{1+2x^2}$$ $$= \frac{x}{2} (\ln{(1+2x^2)} - \ln{(1+x^2)})$$
03

Compute the outer integral

Next, we integrate the result with respect to x: $$\int_{0}^{2} \frac{x}{2} (\ln{(1+2x^2)} - \ln{(1+x^2)}) dx$$ We split the integral into two integrals: $$\frac{1}{2} \int_{0}^{2} x \ln{(1+2x^2)} dx - \frac{1}{2} \int_{0}^{2} x \ln{(1+x^2)} dx$$
04

Evaluate the integrals using integration by parts

Both integrals can be solved using integration by parts as follows: Integration by Parts Formula: \(\int udv = uv - \int v du\). For the first integral, let \(u = \ln(1 + 2x^2)\), \(dv = x dx\). Then, we have \(du = \frac{4x dx}{1 + 2x^2}\), \(v = \frac{x^2}{2}\). For the second integral, let \(u = \ln(1+x^2)\), \(dv = x dx\). Then, we have \(du = \frac{2x dx}{1 + x^2}\), \(v = \frac{x^2}{2}\). Evaluating the first integral using integration by parts: $$\frac{1}{2} \int_{0}^{2} x \ln{(1+2x^2)} dx =\frac{1}{4}(2^2 \ln(9)- \int_{0}^{2} \frac{2x^3 dx}{1 + 2x^2} )$$ Evaluating the second integral using integration by parts: $$\frac{1}{2}\int_{0}^{2} x \ln{(1+x^2)} dx = \frac{1}{4}(2^2 \ln(5) - \int_{0}^{2} \frac{2x^3 dx}{1 + x^2} )$$
05

Combine the results

Summing both integrals together: $$\frac{1}{2} \left[ 2^2\left(\ln(9) - \ln(5)\right) - \int_{0}^{2}\left(\frac{2x^3 dx}{1 + 2x^2} - \frac{2x^3 dx}{1 + x^2}\right)\right]$$ The result of this double integral is the solution to the exercise.

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Key Concepts

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

Limits of Integration
The limits of integration define the range over which you are integrating a function. For double integrals, these limits specify a region in the plane over which the integration occurs. In our exercise, the region \( R \) is defined by two conditions: \( 0 \leq y \leq x \) and \( 0 \leq x \leq 2 \). This means that for each slice of the function, defined by a constant \( x \), \( y \) will range from \( 0 \) to \( x \). After fully sweeping through all \( y \) given an \( x \), \( x \) itself will range from \( 0 \) to \( 2 \).
The limits allow you to set up the integral properly. Here, you first integrate with respect to \( y \), keeping \( x \) constant, then with respect to \( x \), analyzing each slice step by step, tracing the integral over the entire specified region.
Integration by Parts
Integration by parts is a technique derived from the product rule of differentiation. It's useful when integrating products of functions where direct integration isn't straightforward. The formula used is:\[\int u \ dv = uv - \int v \ du\]
In this exercise, the technique is applied twice, for two separate integrals, each involving a logarithmic and a polynomial function. When choosing \( u \) and \( dv \), it's often advantageous to let \( u \) be the function that becomes simpler when differentiated (like a logarithm), and \( dv \) be the function whose integral is elementary (like \( x \) dx).
For example:
  • Let \( u = \ln(1 + 2x^2) \) and \( dv = x dx \)
  • This means \( du = \frac{4x dx}{1 + 2x^2} \) and \( v = \frac{x^2}{2} \)
Using these, the integration by parts formula helps simplify the integral, reducing it to a solvable form.
Substitution Method
The substitution method is a key technique used to simplify integrals. It involves substituting a new variable to transform a complex expression into a simpler one. This is known as the "change of variables" technique.
In our problem, the substitution \( u = 1 + x^2 + y^2 \) is used during the integration with respect to \( y \). This substitution simplifies the function by turning it into a form where the variables separate, effectively reducing the interaction between \( x \) and \( y \).
Substitute and rearrange the derivative:
  • Let \( u = 1 + x^2 + y^2 \)
  • Then, \( du = 2y \, dy \), so \( dy = \frac{du}{2y} \)
This substitution converts the original function into a much easier log-integral, focusing more on integration limits, making computation straightforward.
Iterated Integrals
Iterated integrals allow you to compute double integrals by performing a sequence of single integrations. These are crucial for multi-variable calculus, helping tackle problems over two-dimensional domains by breaking them into manageable parts.
In our exercise, the iterated integral: \[\int_{0}^{2} \int_{0}^{x} \frac{x y}{1+x^{2}+y^{2}} \ dy \ dx\]first integrates with respect to \( y \), holding \( x \) constant. Once that's computed, it is then integrated with respect to \( x \).
The steps of an iterated integral can simplify complicated areas by:
  • First addressing the inner integral over a smaller range
  • Then expanding over a broader range for the outer integral
This ensures you precisely capture the total integration over the region \( R \), capturing all nuances of \( x \)-dependent changes.

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Most popular questions from this chapter

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 \(\rho(r, \theta)=4+r \sin \theta.\)

Determine whether the following statements are true and give an explanation or counterexample. a. A thin plate of constant density that is symmetric about the \(x\) -axis has a center of mass with an \(x\) -coordinate of zero. b. A thin plate of constant density that is symmetric about both the \(x\) -axis and the \(y\) -axis has its center of mass at the origin. c. The center of mass of a thin plate must lie on the plate. d. The center of mass of a connected solid region (all in one piece) must lie within the region.

The Jacobian is a magnification (or reduction) factor that relates the area of a small region near the point \((u, v)\) to the area of the image of that region near the point \((x, y)\) a. Suppose \(S\) is a rectangle in the \(u v\) -plane with vertices \(O(0,0)\) \(P(\Delta u, 0),(\Delta u, \Delta v),\) and \(Q(0, \Delta v)\) (see figure). The image of \(S\) under the transformation \(x=g(u, v), y=h(u, v)\) is a region \(R\) in the \(x y\) -plane. Let \(O^{\prime}, P^{\prime},\) and \(Q^{\prime}\) be the images of O, P, and \(Q,\) respectively, in the \(x y\) -plane, where \(O^{\prime}\) \(P^{\prime},\) and \(Q^{\prime}\) do not all lie on the same line. Explain why the coordinates of \(\boldsymbol{O}^{\prime}, \boldsymbol{P}^{\prime}\), and \(Q^{\prime}\) are \((g(0,0), h(0,0))\) \((g(\Delta u, 0), h(\Delta u, 0)),\) and \((g(0, \Delta v), h(0, \Delta v)),\) respectively. b. Use a Taylor series in both variables to show that $$\begin{aligned} &g(\Delta u, 0) \approx g(0,0)+g_{u}(0,0) \Delta u\\\ &g(0, \Delta v) \approx g(0,0)+g_{v}(0,0) \Delta v\\\ &\begin{array}{l} h(\Delta u, 0) \approx h(0,0)+h_{u}(0,0) \Delta u \\ h(0, \Delta v) \approx h(0,0)+h_{v}(0,0) \Delta v \end{array} \end{aligned}$$ where \(g_{u}(0,0)\) is \(\frac{\partial x}{\partial u}\) evaluated at \((0,0),\) with similar meanings for \(g_{v}, h_{u}\) and \(h_{v}\) c. Consider the vectors \(\overrightarrow{O^{\prime} P^{\prime}}\) and \(\overrightarrow{O^{\prime} Q^{\prime}}\) and the parallelogram, two of whose sides are \(\overrightarrow{O^{\prime} P^{\prime}}\) and \(\overrightarrow{O^{\prime} Q^{\prime}}\). Use the cross product to show that the area of the parallelogram is approximately \(|J(u, v)| \Delta u \Delta v\) d. Explain why the ratio of the area of \(R\) to the area of \(S\) is approximately \(|J(u, v)|\)

Consider the following two-and three-dimensional regions. Specify the surfaces and curves that bound the region, choose a convenient coordinate system, and compute the center of mass assuming constant density. All parameters are positive real numbers. A solid rectangular box has sides of length \(a, b,\) and \(c .\) Where is the center of mass relative to the faces of the box?

Consider the linear transformation \(T\) in \(\mathbb{R}^{2}\) given by \(x=a u+b v, y=c u+d v,\) where \(a, b, c,\) and \(d\) are real numbers, with \(a d \neq b c\) a. Find the Jacobian of \(T\) b. Let \(S\) be the square in the \(u v\) -plane with vertices (0,0) \((1,0),(0,1),\) and \((1,1),\) and let \(R=T(S) .\) Show that \(\operatorname{area}(R)=|J(u, v)|\) c. Let \(\ell\) be the line segment joining the points \(P\) and \(Q\) in the uv- plane. Show that \(T(\ell)\) (the image of \(\ell\) under \(T\) ) is the line segment joining \(T(P)\) and \(T(Q)\) in the \(x y\) -plane. (Hint: Use vectors.) d. Show that if \(S\) is a parallelogram in the \(u v\) -plane and \(R=T(S),\) then \(\operatorname{area}(R)=|J(u, v)| \operatorname{area}(S) .\) (Hint: Without loss of generality, assume the vertices of \(S\) are \((0,0),(A, 0)\) \((B, C),\) and \((A+B, C),\) where \(A, B,\) and \(C\) are positive, and use vectors.)

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