/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 18 Evaluate the following integrals... [FREE SOLUTION] | 91Ó°ÊÓ

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Evaluate the following integrals in cylindrical coordinates. $$\int_{-3}^{3} \int_{0}^{\sqrt{9-x^{2}}} \int_{0}^{2} \frac{1}{1+x^{2}+y^{2}} d z d y d x$$

Short Answer

Expert verified
Question: Evaluate the given triple integral in cylindrical coordinates: $$\iiint\limits_{V}\frac{x+y}{1+z^2}dV$$ where V is the region in the first octant inside the cylinder \(x^2 + y^2 = 9\) and below the plane \(z=2\). Answer: The value of the given triple integral in cylindrical coordinates is $$6\ln(10)$$

Step by step solution

01

Convert the given integral to cylindrical coordinates

To convert the given integral to cylindrical coordinates, we will replace the coordinates \((x, y, z)\) with \((r, \theta, z)\), where \(r^2 = x^2 + y^2\) and the Jacobian is given by \(J = r\). Let's find the bounds for \(r\), \(\theta\), and \(z\): - For \(x\), we have \(-3 \le x \le 3\). Since \(x = r\cos \theta\), we can rewrite this as \(0 \le r\cos \theta \le 3\). - For \(y\), we have \(0 \le y \le \sqrt{9 - x^2}\). Since \(y = r\sin \theta\), we can rewrite this as \(0 \le r\sin \theta \le \sqrt{9 - r^2\cos^2\theta}\). However, in cylindrical coordinates, \(y\) has limits of \(0 \le y \le 2\pi\). - For \(z\), we have \(0 \le z \le 2\). So the transformed integral becomes: $$\int \int \int \frac{r}{1+r^2} d z d r d \theta$$ Now that we've found the bounds let's proceed to evaluate the integrals.
02

Evaluate the inner integral

We first evaluate the inner integral with respect to \(z\): $$\int_{0}^{2} \frac{1}{1+r^2} dz$$ $$= \left[\frac{z}{1+r^2}\right]_{0}^{2} = \frac{2}{1+r^2}$$
03

Evaluate the middle integral

Now we evaluate the middle integral with respect to \(r\): $$\int_{0}^{\sqrt{9-x^2}} \frac{2}{1+r^2} r dr$$ Make a substitution: \(u = 1 + r^2, du = 2r dr\): $$\int_{1}^{10} \frac{r du}{u} = \int_{1}^{10} \frac{du}{u}$$ $$= \left[\ln|u|\right]_{1}^{10} = \ln(\frac{10}{1}) = \ln(10)$$ Keep in mind that in this phase, we just find the integral, but we haven't substituted back the variable yet.
04

Evaluate the outer integral

Finally, we evaluate the outer integral with respect to \(\theta\): $$\int_{-3}^{3} \ln(10) d\theta = \ln(10)\left[\theta\right]_{-3}^{3} = 6\ln(10)$$ So, the value of the given triple integral in cylindrical coordinates is: $$6\ln(10)$$

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Key Concepts

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

Triple Integral
Triple integrals are a powerful tool for integrating functions over a three-dimensional region. In conventional Cartesian coordinates, a triple integral is expressed as \( \int \int \int f(x, y, z) \, dz \, dy \, dx \). In the given exercise, we need to integrate the function \( \frac{1}{1+x^2+y^2} \) over a specific region.
Triple integrals are especially useful when dealing with volumes or when integrating across three-dimensional spaces. The three levels of integration, which correspond to the variables \(x, y, \) and \(z\), help in calculating the combined effect of the function across the region defined by the integration bounds.
The complexity of dealing with each level increases as we must keep track of transforming coordinates and respecting the integration bounds.
Change of Variables
In many integration problems, such as the one given, changing from Cartesian to cylindrical coordinates simplifies the integration process.
Cylindrical coordinates \( (r, \theta, z) \) are particularly handy when the region of integration or the function has a circular symmetry common to cylinders or revolved shapes.
To change variables in the context of cylindrical coordinates, we use the transformations:
  • \( x = r \cos \theta \)
  • \( y = r \sin \theta \)
  • \( z = z \) (remains the same)
  • \( r^2 = x^2 + y^2 \)
In this way, we handle the integration limits in terms of \(r, \theta, \) and \(z\), avoiding the cumbersome bounds that weigh down the Cartesian integration process.
This change often makes certain functions, especially those involving circular shapes, much simpler to integrate.
Jacobian Determinant
The Jacobian determinant is a crucial part of changing variables in integration. It accounts for the stretching or shrinking of the volume element when undergoing coordinate transformation.
In cylindrical coordinates, the Jacobian \( J = r \) arises from the conversion between Cartesian and cylindrical coordinates.
This Jacobian is used within the integral as a scaling factor. This means our integrand becomes \( \frac{r}{1 + r^2} \) instead of \( \frac{1}{1+x^2+y^2} \), multiplying by \( r \).
Without the Jacobian, integrating in the new coordinate system would yield incorrect results since the volume element itself changes with \( r \).This is why the Jacobian determinant is a multiplier: to ensure the nature of volume and area is preserved during integration.
Integration Bounds
When performing integration, proper specification of integration bounds is vital. These bounds define the region over which the function is integrated.
In rectangular coordinates, these are often straightforward but can become difficult to handle due to complex shapes. When using cylindrical coordinates, the integration bounds become functions of \(r, \theta, \) and \(z\).
  • For \( r \), bounds usually range from \( 0 \) to some maximum value derived from the problem's geometry.
  • For \( \theta \), it's from \( 0 \) to \( 2\pi \), covering the full rotation around an axis.
  • For \( z \), they might directly carry over from the \( z \) components of the rectangular system.
Correctly determining these limits is crucial for accurately capturing the region of interest in the integral.While transforming coordinates simplifies the function and domain in a non-trivial way, respecting these new bounds ensures we calculate the integral correctly in its new form.

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