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Evaluate the following integrals in spherical coordinates. $$\int_{0}^{\pi} \int_{0}^{\pi / 6} \int_{2 \sec \varphi}^{4} \rho^{2} \sin \varphi d \rho d \varphi d \theta$$

Short Answer

Expert verified
The value of the given triple integral is $$\frac{64\pi}{3}(1 - \frac{\sqrt{3}}{2} + 7)$$

Step by step solution

01

Change of Variables

In spherical coordinates, we have the following differential volume element: $$dV = \rho^2 \sin \varphi d\rho d\varphi d\theta$$ So, the given integral becomes: $$\int_{0}^{\pi} \int_{0}^{\pi / 6} \int_{2 \sec \varphi}^{4} (\rho^{2} \sin \varphi) dV$$
02

Integrate with respect to \(\rho\)

Integrating the innermost integral with respect to \(\rho\), we have: $$I_\rho = \int_{2\sec\varphi}^{4} \rho^{2} d\rho = \frac{1}{3} \rho^3 \Big|_{2\sec\varphi}^{4} = \frac{1}{3}(64 - 8^3\sec^3\varphi)$$
03

Integrate with respect to \(\varphi\)

Now integrating the middle integral with respect to \(\varphi\), we have: $$I_\varphi = \int_{0}^{\frac{\pi}{6}} (\frac{1}{3}(64 - 8^3\sec^3\varphi)) \sin\varphi d\varphi = \frac{1}{3} \int_{0}^{\frac{\pi}{6}} (64\sin\varphi - 8^3\sec^3\varphi \sin\varphi) d\varphi$$ To evaluate the integral with the \(\sec^3\varphi\) term, a \(u\)-substitution can be used with \(u = \sec\varphi\) and \(du = \sec\varphi\tan\varphi d\varphi\). Since \(\sin\varphi = \frac{\tan\varphi}{\sec\varphi}\), the integral can be rewritten as: $$I_\varphi = \frac{1}{3} (\int_{0}^{\frac{\pi}{6}} 64\sin\varphi d\varphi - \int_{\sec{0}}^{\sec{\frac{\pi}{6}}} 8^3 u^2 du)$$ Now, we evaluate the definite integrals separately: $$I_\varphi = \frac{1}{3} (64(-\cos\frac{\pi}{6} + \cos 0) - 8^3 (\frac{1}{3} u^3 \Big|_1^2))$$
04

Simplify and Integrate with respect to \(\theta\)

Simplify the expression for \(I_\varphi\) to obtain: $$I_\varphi = \frac{1}{3} (64(-\frac{\sqrt{3}}{2} + 1) - 8^3 (\frac{1}{3}(8 - 1))) = \frac{64}{3}(1 - \frac{\sqrt{3}}{2} + 7)$$ Finally, integrating with respect to \(\theta\), we have: $$I = \int_{0}^{\pi} I_\varphi d\theta = \int_{0}^{\pi} \frac{64}{3}(1 - \frac{\sqrt{3}}{2} + 7) d\theta = \frac{64}{3}(1 - \frac{\sqrt{3}}{2} + 7)\theta \Big|_0^\pi$$
05

Evaluate the Final Integral

Now, we evaluate the final integral: $$I = \frac{64}{3}(1 - \frac{\sqrt{3}}{2} + 7)(\pi - 0) = \frac{64\pi}{3}(1 - \frac{\sqrt{3}}{2} + 7)$$ So, the value of the given triple integral is: $$\int_{0}^{\pi} \int_{0}^{\pi / 6} \int_{2 \sec \varphi}^{4} \rho^{2} \sin \varphi d \rho d \varphi d \theta = \frac{64\pi}{3}(1 - \frac{\sqrt{3}}{2} + 7)$$

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Key Concepts

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

Triple Integrals
Triple integrals are a way of calculating the volume of a region in three-dimensional space. Imagine stacking up many thin sheets or layers to fill a volume. Each sheet represents a smaller part of the entire volume. Triple integrals help us find the total amount when these pieces are added together.

The integration occurs in three steps, each corresponding to one dimension:
  • Inner integral: This is calculated first and involves integrating with respect to one variable, often denoted as \( \rho \) in spherical coordinates.
  • Middle integral: After integrating the first, the result becomes an integrand for the second integral, typically with respect to \( \varphi \).
  • Outer integral: Finally, we integrate the result with respect to the third variable, often \( \theta \), bringing all calculations together.
In summary, triple integrals help us compute comprehensive measures like volume in a systematic way.
Change of Variables
The change of variables is a powerful technique in integration, particularly useful in converting complex integrals into simpler ones. In the context of spherical coordinates, this transformation is instrumental because spherical geometry naturally reflects many real-world objects like planets or atoms.

When changing variables to spherical coordinates, we're replacing the traditional Cartesian coordinates (x, y, z) with \( \rho \), \( \varphi \), and \( \theta \):
  • \( \rho \): Represents the radial distance from the origin to a point.
  • \( \varphi \): Denotes the angle in the vertical plane from the positive z-axis.
  • \( \theta \): Refers to the azimuthal angle in the xy-plane from the positive x-axis.
This method involves understanding relationships like \( x = \rho \sin\varphi \cos\theta \), which help recast the integral's limits and the volume element, \( dV = \rho^2 \sin \varphi d\rho d\varphi d\theta \). This ensures calculations align with spherical geometry, simplifying the integration process.
Integration Techniques
Integration techniques are about finding the easiest or most effective way to solve an integral. In solving the provided problem, various techniques illustrate different strategies to overcome challenges in calculation.

The primary technique used involves the method of integration by substitution. This is evident when approaching the integral with a \( \sec^3\varphi \) term. Here, the substitution \( u = \sec\varphi \), transforms difficult-to-handle trigonometric expressions into simpler algebraic forms.

Steps for substitution involve:
  • Choosing a substitution that will simplify the expression.
  • Calculating the differential \( du \) to replace the variable and its differential in the integral.
  • Resolving the limits of integration to the new variable \( u \).
These techniques not only aid in simplifying the problem but also open paths to calculating integrals that might otherwise appear unsolvable. Mastery of these techniques is essential for tackling complex integrals in higher mathematics.

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Most popular questions from this chapter

Changing order of integration If possible, write iterated integrals in spherical coordinates for the following regions in the specified orders. Sketch the region of integration. Assume that \(f\) is continuous on the region. $$\begin{aligned}&\int_{0}^{2 \pi} \int_{0}^{\pi / 4} \int_{0}^{4 \sec \varphi} f(\rho, \varphi, \theta) \rho^{2} \sin \varphi d \rho d \varphi d \theta \text { in the orders }\\\&d \rho d \theta d \varphi \text { and } d \theta d \rho d \varphi\end{aligned}$$

\(A\) thin plate is bounded by the graphs of \(y=e^{-x}, y=-e^{-x}, x=0,\) and \(x=L .\) Find its center of mass. How does the center of mass change as \(L \rightarrow \infty ?\)

Explain why or why not ,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.

Use polar coordinates to find the centroid of the following constant-density plane regions. The quarter-circular disk \(R=\\{(r, \theta): 0 \leq r \leq 2,0 \leq \theta \leq \pi / 2\\}\)

Mass from density Find the mass of the following solids with the given density functions. Note that density is described by the function \(f\) to avoid confusion with the radial spherical coordinate \(\rho\). The ball of radius 8 centered at the origin with a density \(f(\rho, \varphi, \theta)=2 e^{-\rho^{3}}\)

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