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Find the area of the given surface. The portion of the cone $$ \mathbf{r}(u, v)=u \cos v \mathbf{i}+u \sin v \mathbf{j}+u \mathbf{k} $$ for which \(0 \leq u \leq 2 v, 0 \leq v \leq \pi / 2\)

Short Answer

Expert verified
Surface area is given by a complex integral requiring numerical methods.

Step by step solution

01

Understand the Surface Description

The surface is given by the parametric vector function \( \mathbf{r}(u, v) = u \cos v \mathbf{i} + u \sin v \mathbf{j} + u \mathbf{k} \) which is a cone extending from 0 to \(2v\) for \(u\) and from 0 to \(\pi/2\) for \(v\). The cone has its apex at the origin and opens upwards.
02

Parameterization Breakdown

For this surface, \( u \) represents the radial distance from the cone's axis (vertical axis), and \( v \) represents the angle around the axis. The limits for \( u \) and \( v \) are \( 0 \leq u \leq 2v \) and \( 0 \leq v \leq \pi/2 \), indicating a finite section of the cone.
03

Calculate Partial Derivatives

Find the partial derivatives of \( \mathbf{r}(u, v) \) with respect to \( u \) and \( v \):\[\mathbf{r}_u = \frac{\partial \mathbf{r}}{\partial u} = \cos v \mathbf{i} + \sin v \mathbf{j} + \mathbf{k}\]\[\mathbf{r}_v = \frac{\partial \mathbf{r}}{\partial v} = -u \sin v \mathbf{i} + u \cos v \mathbf{j}\]
04

Find Cross Product of Derivatives

Compute the cross product \( \mathbf{r}_u \times \mathbf{r}_v \):\[ \mathbf{r}_u \times \mathbf{r}_v = \begin{vmatrix}\mathbf{i} & \mathbf{j} & \mathbf{k} \\cos v & \sin v & 1 \-u \sin v & u \cos v & 0\end{vmatrix} = (-\sin v \mathbf{i} -\cos v \mathbf{j} + u \mathbf{k})\]
05

Compute Magnitude of Cross Product

Find the magnitude of the cross product vector:\[|\mathbf{r}_u \times \mathbf{r}_v| = \sqrt{(-\sin v)^2 + (-\cos v)^2 + u^2}= \sqrt{1 + u^2}\]
06

Integrate to Find the Surface Area

Set up the integral for the surface area \( S \) over the given bounds:\[S = \int_{0}^{\pi/2} \int_{0}^{2v} \sqrt{1 + u^2} \; du \; dv\]First, integrate with respect to \( u \):\[= \int_{0}^{\pi/2} \left[\frac{u}{2}\sqrt{1 + u^2} + \frac{1}{2} \ln|u + \sqrt{1 + u^2}|\right]_{0}^{2v} \; dv\]Substitute the limits:\[= \int_{0}^{\pi/2} \left( v\sqrt{4v^2 + 1} + \frac{1}{2} \ln(2v + \sqrt{4v^2 + 1}) \right) \; dv\]
07

Evaluate Final Integral

Evaluate the resulting integral:\[S = \int_{0}^{\pi/2} \left( v\sqrt{4v^2 + 1} + \frac{1}{2} \ln(2v + \sqrt{4v^2 + 1}) \right) \; dv\]This is a complex integral and generally requires numerical methods or approximation techniques to solve exactly.

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Key Concepts

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

Parametric Equations
In mathematics, parametric equations are a set of equations that express the coordinates of the points on a geometric object as functions of a number of variables called parameters. These parameters make it easier to deal with curves and surfaces in 3D space.
In the provided problem, the parametric vector function \( \mathbf{r}(u, v) = u \cos v \mathbf{i} + u \sin v \mathbf{j} + u \mathbf{k} \) describes a cone. Here:
  • \( u \) represents the radial distance from the cone's vertical axis.
  • \( v \) represents the angle around the vertical axis.
These parameterizations help construct surfaces that vary smoothly and allow us to compute properties like surface area or volume efficiently.
In our case, this surface ranges for \( u \) from 0 to \( 2v \) and for \( v \) from 0 to \( \pi/2 \), effectively describing a finite part of the cone. Parametric representations are critical in defining the area over which further mathematical operations, like integration, will occur.
Cone
A cone is a three-dimensional geometric shape that tapers smoothly from a flat base to a point called the apex or vertex. The simplest cone has the circle as its base and the vertex directly above the center of the circle, forming a right circular cone.
The parametric description given in the exercise \( \mathbf{r}(u, v) = u \cos v \mathbf{i} + u \sin v \mathbf{j} + u \mathbf{k} \) creates a cone with its apex at the origin and extending upward.
In the parametric domain:
  • The variable \( u \) acts as the radial distance from the vertex.
  • The variable \( v \) describes a circular path about the vertex.
This supports the visualization of the cone by tracing out a path as \( u \) increases and \( v \) sweeps through its range. Understanding the geometric properties of a cone aids in comprehending how its formation informs the limits and results of integrals that determine surface areas.
Cross Product
The cross product, or vector product, is an operation on two vectors in three-dimensional space. This results in a third vector that is perpendicular to the plane of the input vectors. The cross product is widely used in calculus and physics because it provides a means to calculate an area-related quantity.In the context of the given surface of a cone, the cross product helps in finding the normal vector to the surface. Specifically:- The partial derivatives \( \mathbf{r}_u \) and \( \mathbf{r}_v \) represent tangent vectors to the surface.- Calculating the cross product \( \mathbf{r}_u \times \mathbf{r}_v \) gives a vector normal to the surface.The magnitude of this cross product vector \( |\mathbf{r}_u \times \mathbf{r}_v| = \sqrt{1 + u^2} \) directly contributes to the integrand for the surface area calculation. This magnitude represents the infinitesimal surface area around a small patch modeled by the differential change in \( u \) and \( v \). By integrating this quantity, we determine the total surface area.
Integration
Integration is a fundamental concept in calculus, offering ways to sum infinitesimal parts to find total quantities like areas and volumes. When determining surface areas of complex 3D shapes described by parametric equations, integration becomes crucial.For the cone's surface area, integration is set up as:\[S = \int_{0}^{\pi/2} \int_{0}^{2v} \sqrt{1 + u^2} \; du \; dv\]Here,
  • \( \sqrt{1 + u^2} \) is the magnitude of the cross product vector, detailing each infinitesimal piece of surface area.
  • The limits of integration for \( u \) and \( v \) define the portion of the cone being evaluated.
The nested integrals iterate first over \( u \) and then \( v \), systematically piecing together each strip of the cone to find its entire surface area.
Surface integrals such as this often require numerical methods for precise evaluation, as closed-form solutions might be complex or impossible to achieve analytically.

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Most popular questions from this chapter

Evaluate the iterated integral. \(\int_{0}^{2 \pi} \int_{0}^{\pi / 4} \int_{0}^{a \sec \phi} \rho^{2} \sin \phi d \rho d \phi d \theta \quad(a>0)\)

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The tendency of a lamina to resist a change in rotational motion about an axis is measured by its moment of inertia about that axis. If a lamina occupies a region \(R\) of the \(x y\) -plane, and if its density function \(\delta(x, y)\) is continuous on \(R\), then the moments of inertia about the \(x\) -axis, the \(y\) -axis, and the \(z\) -axis are denoted by \(I_{x}, I_{y}\), and \(I_{z}\), respectively, and are defined by $$\begin{aligned}&I_{x}=\iint_{R} y^{2} \delta(x, y) d A, \quad I_{y}=\iint_{R} x^{2} \delta(x, y) d A \\\&I_{z}=\iint_{R}\left(x^{2}+y^{2}\right) \delta(x, y) d A \end{aligned}$$ Use these definitions. Consider the rectangular lamina that occupies the region described by the inequalities \(0 \leq x \leq a\) and \(0 \leq y \leq b .\) Assuming that the lamina has constant density \(\delta\), show that $$I_{x}=\frac{\delta a b^{3}}{3}, \quad I_{y}=\frac{\delta a^{3} b}{3}, \quad I_{z}=\frac{\delta a b\left(a^{2}+b^{2}\right)}{3}$$

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