/*! 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 24 Consider the following vector fi... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Consider the following vector fields, where \(\mathbf{r}=\langle x, y, z\rangle\). a. Compute the curl of the field and verify that it has the same direction as the axis of rotation. b. Compute the magnitude of the curl of the field. $$\mathbf{F}=\langle 1,-1,0\rangle \times \mathbf{r}$$

Short Answer

Expert verified
Answer: The curl of the vector field \(\mathbf{F}\) is \(\langle 0, 0, 0\rangle\), and its magnitude is \(0\). Since the curl is a zero vector, it does not really have a direction, and the curl does not show any rotation around any axis in this case.

Step by step solution

01

Find the explicit form of the vector field

We are given that the vector field is formed by the cross product of \(\langle 1, -1, 0\rangle\) and \(\mathbf{r} = \langle x, y, z\rangle\). Let's find their cross product: $$ \mathbf{F} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k}\\ 1 & -1 & 0\\ x & y & z \end{vmatrix} = \mathbf{i}(0 - (-z)) - \mathbf{j}(0 - z) + \mathbf{k}(1y - (-1x)) = \langle z, z, x+y \rangle $$
02

Compute the curl of the vector field

To compute the curl of the vector field, we need to evaluate the following expression: $$ \nabla \times \mathbf{F} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k}\\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z}\\ z & z & x + y \end{vmatrix} $$ Calculating the determinants, we get: $$ \nabla \times \mathbf{F} = \mathbf{i}\left(\frac{\partial (x+y)}{\partial y} - \frac{\partial z}{\partial z}\right) - \mathbf{j}\left(\frac{\partial (x+y)}{\partial x} - \frac{\partial z}{\partial z}\right) + \mathbf{k}\left(\frac{\partial z}{\partial x} - \frac{\partial z}{\partial y}\right) = \langle 0, 0, 0 \rangle $$
03

Verify the direction of the curl

The curl of the vector field \(\nabla \times \mathbf{F}\) is found to be \(\langle 0, 0, 0\rangle\). Since the curl is a zero vector, it does not really have a direction. In other words, the curl does not show any rotation around any axis in this case.
04

Compute the magnitude of the curl

The magnitude of the curl is given by the formula: $$ ||\nabla \times \mathbf{F}|| = \sqrt{(0)^2 + (0)^2 + (0)^2} = 0 $$ So, the magnitude of the curl of the field is \(0\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Find a vector field \(\mathbf{F}\) with the given curl. In each case, is the vector field you found unique? $$\operatorname{curl} \mathbf{F}=\langle 0,1,0\rangle$$

Consider the vector field \(\mathbf{F}=\frac{-y}{x^{2}+y^{2}} \mathbf{i}+\frac{x}{x^{2}+y^{2}} \mathbf{j}+z \mathbf{k}\) a. Show that \(\nabla \times \mathbf{F}=\mathbf{0}\) b. Show that \(\oint_{C} \mathbf{F} \cdot d \mathbf{r}\) is not zero on a circle \(C\) in the \(x y\) -plane enclosing the origin. c. Explain why Stokes' Theorem does not apply in this case.

The area of a region \(R\) in the plane, whose boundary is the closed curve \(C,\) may be computed using line integrals with the formula $$\text { area of } R=\int_{C} x d y=-\int_{C} y d x$$ These ideas reappear later in the chapter. Let \(R=\\{(r, \theta): 0 \leq r \leq a, 0 \leq \theta \leq 2 \pi\\}\) be the disk of radius \(a\) centered at the origin and let \(C\) be the boundary of \(R\) oriented counterclockwise. Use the formula \(A=-\int_{C} y d x\) to verify that the area of the disk is \(\pi r^{2}.\)

Suppose an object with mass \(m\) moves in a region \(R\) in a conservative force field given by \(\mathbf{F}=-\nabla \varphi\) where \(\varphi\) is a potential function in a region \(R .\) The motion of the object is governed by Newton's Second Law of Motion, \(\mathbf{F}=m \mathbf{a}\) where a is the acceleration. Suppose the object moves from point \(A\) to point \(B\) in \(R\). a. Show that the equation of motion is \(m \frac{d \mathbf{v}}{d t}=-\nabla \varphi\) b. Show that \(\frac{d \mathbf{v}}{d t} \cdot \mathbf{v}=\frac{1}{2} \frac{d}{d t}(\mathbf{v} \cdot \mathbf{v})\) c. Take the dot product of both sides of the equation in part (a) with \(\mathbf{v}(t)=\mathbf{r}^{\prime}(t)\) and integrate along a curve between \(A\) and \(B\). Use part (b) and the fact that \(\mathbf{F}\) is conservative to show that the total energy (kinetic plus potential) \(\frac{1}{2} m|\mathbf{v}|^{2}+\varphi\) is the same at \(A\) and \(B\). Conclude that because \(A\) and \(B\) are arbitrary, energy is conserved in \(R\)

Use Stokes' Theorem to find the circulation of the following vector fields around any simple closed smooth curve \(C\). $$\mathbf{F}=\langle 2 x,-2 y, 2 z\rangle$$

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.