Chapter 16: Problem 6
In Exercises \(1-8,\) integrate the given function over the given surface. Cone \(\quad F(x, y, z)=z-x, \quad\) over \(\quad\) the cone \(\quad z=\sqrt{x^{2}+y^{2}}\) \(0 \leq z \leq 1\)
Short Answer
Expert verified
The surface integral over the cone is \( \frac{2\pi}{3} \).
Step by step solution
01
Describe the Surface
The surface of integration is a cone given by the equation \( z = \sqrt{x^2 + y^2} \). This describes a cone that is symmetric around the z-axis and extends from the apex at the origin (0,0,0) upward, and we integrate over this surface from \( z = 0 \) to \( z = 1 \).
02
Set Up the Surface Integral
The vector field \( F(x, y, z) = z - x \) is given, and we need to integrate this over the cone surface. A parametrization for the cone surface can be given by cylindrical coordinates: \( x = r\cos(\theta) \), \( y = r\sin(\theta) \), and \( z = r \), with \( 0 \leq r \leq 1 \) and \( 0 \leq \theta \leq 2\pi \).
03
Compute the Surface Element
The differential surface element is obtained by using the position vector \( \oldsymbol{r}(r, \theta) = (r\cos(\theta), r\sin(\theta), r) \). Its partial derivatives are \( \oldsymbol{r}_r = (\cos(\theta), \sin(\theta), 1) \) and \( \oldsymbol{r}_{\theta} = (-r\sin(\theta), r\cos(\theta), 0) \). The cross-product \( \oldsymbol{r}_r \times \oldsymbol{r}_{\theta} \) gives the normal vector, which yields \( \vec{n}\,dS = r\, dr\, d\theta \).
04
Evaluate the Integral
Substitute the parameters into the function: \( F(x, y, z) = r - r\cos(\theta) \). The integral becomes \( \int_0^{2\pi} \int_0^1 (r - r\cos(\theta))\, r\, dr\, d\theta \). Simplifying this gives \( \int_0^{2\pi} \int_0^1 (r^2 - r^2 \cos(\theta))\, dr\, d\theta \).
05
Integrate with Respect to \( r \)
Evaluate \( \int_0^1 (r^2 - r^2 \cos(\theta))\, dr \). This integral is linear, yielding \( \left[ \frac{r^3}{3} - \frac{r^3}{3} \cos(\theta) \right]_0^1 = \frac{1}{3}(1 - \cos(\theta)) \).
06
Integrate with Respect to \( \theta \)
Now, integrate with respect to \( \theta \): \( \int_0^{2\pi} \frac{1}{3}(1 - \cos(\theta))\, d\theta = \frac{1}{3} \left[ \theta - \sin(\theta) \right]_0^{2\pi} \). Evaluate to get \( \frac{1}{3} (2\pi) = \frac{2\pi}{3} \) since the integral of \( \sin(\theta) \) over \( [0, 2\pi] \) is zero.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Cone Surface
A cone surface is a three-dimensional geometric figure characterized by its circular base and pointed apex. The particular cone given in this exercise is described by the equation \( z = \sqrt{x^2 + y^2} \). This represents a right circular cone, symmetric around the z-axis. The apex is at the origin (0,0,0), and the cone extends upwards. For integration purposes, we consider the portion of the cone where the height \( z \) ranges from 0 to 1. This specifies a vertical slice of the cone, creating a finite cap on this otherwise infinite shape.
Cylindrical Coordinates
Cylindrical coordinates are extremely useful in problems involving symmetrical shapes like cones or cylinders. They provide a simple way to express points in 3D space using a radius \( r \), an angle \( \theta \), and a height \( z \). For the cone in this exercise, we use the transformation:
- \( x = r\cos(\theta) \)
- \( y = r\sin(\theta) \)
- \( z = r \)
Parametrization
Parametrization involves expressing a surface using a set of parameters, thereby converting a 3D surface into a more tractable form. For the given cone surface, this technique involves re-expressing its coordinates through the parameters \( r \) and \( \theta \). The position vector \( \mathbf{r}(r, \theta) = (r\cos(\theta), r\sin(\theta), r) \) is used.
- \( \mathbf{r}_r = (\cos(\theta), \sin(\theta), 1) \)
- \( \mathbf{r}_\theta = (-r\sin(\theta), r\cos(\theta), 0) \)
Surface Element
The surface element, denoted as \( dS \), is a small "piece" of the surface area over which integration is performed. In our problem, after parametrization, we calculate the differential area element using the cross-product of the partial derivatives of the position vector. Specifically, the normal vector comes from \( \mathbf{r}_r \times \mathbf{r}_\theta \).
- This results in \( \vec{n} dS = r dr d\theta \).