/*! 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 26 Evaluate \(\int_{C} \mathbf{F} \... [FREE SOLUTION] | 91Ó°ÊÓ

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Evaluate \(\int_{C} \mathbf{F} \cdot d \mathbf{r}\) for the vector field \(\mathbf{F}=y \mathbf{i}-x \mathbf{j}\) counterclockwise along the unit circle \(x^{2}+y^{2}=1\) from \((1,0)\) to \((0,1)\) .

Short Answer

Expert verified
The line integral evaluates to \(-\frac{\pi}{2}\).

Step by step solution

01

Understand the Problem

We need to evaluate the line integral \( \int_{C} \mathbf{F} \cdot d \mathbf{r} \) for the vector field \( \mathbf{F}=y \mathbf{i}-x \mathbf{j} \) along the curve \( C \) which is the unit circle \( x^{2}+y^{2}=1 \). The curve starts at \((1,0)\) and ends at \((0,1)\), and the direction is counterclockwise.
02

Apply Green's Theorem

Given that the curve \( C \) is simple and closed, and \( \mathbf{F} \) is defined such that Green's Theorem can be used, we have \( \int_{C} \mathbf{F} \cdot d \mathbf{r} = \int \int_{R} \left( \frac{\partial N}{\partial x} - \frac{\partial M}{\partial y} \right) \,dA \), where \( M = y \) and \( N = -x \).
03

Compute Partial Derivatives

Calculate the partial derivatives: \( \frac{\partial N}{\partial x} = \frac{\partial (-x)}{\partial x} = -1 \) and \( \frac{\partial M}{\partial y} = \frac{\partial y}{\partial y} = 1 \).
04

Evaluate the Double Integral

Substitute the results from Step 3 into the double integral: \[ \int \int_{R} \left( -1 - 1 \right) \,dA = \int \int_{R} -2 \,dA. \] Since \( R \) is the area enclosed by the unit circle, \( \int \int_{R} \,dA = \pi \). Thus, \( \int \int_{R} -2 \,dA = -2\pi. \)
05

Find the Arc Integral

We find that the line integral \( \int_{C} \mathbf{F} \cdot d \mathbf{r} = -2\pi \), according to Green's Theorem. However, we must take only the quarter-circle part from \((1,0)\) to \((0,1)\), which is one-fourth of the full circle.
06

Divide Result by 4

Since the path from \((1,0)\) to \((0,1)\) is one-fourth of the full circle, we divide the result by 4: \( \frac{-2\pi}{4} = -\frac{\pi}{2} \).

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Key Concepts

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

Line Integral
A line integral allows us to integrate functions along a curve. It is a powerful concept in vector calculus, especially useful for calculating work done by a force field along a path or for determining flux across a curve. In this context, the expression \( \int_{C} \mathbf{F} \cdot d \mathbf{r} \) represents a line integral of the vector field \( \mathbf{F} = y \mathbf{i} - x \mathbf{j} \) along a path \( C \). The curve \( C \) is given by the unit circle. Here, the line integral is evaluated by summing up the product of the vector field and a differential path element over the path.
Applying Green's theorem in this context transforms the problem of calculating a line integral around a circle into a simpler calculation of a double integral over the area contained by the circle. This is particularly helpful when the path is closed and simple, allowing us to focus on just the region bounded by the circle.
Vector Field
A vector field is a map that assigns a vector to every point in space. In two dimensions, this can be visualized as a collection of arrows, each pointing in a specific direction with a certain magnitude. In our exercise, the vector field is described by \( \mathbf{F} = y \mathbf{i} - x \mathbf{j} \). Each point \((x, y)\) in the plane is associated with a vector whose components depend on \(x\) and \(y\).
  • The \( y \mathbf{i} \) component suggests the vector's horizontal part will vary with the \( y \)-coordinate.
  • The \( -x \mathbf{j} \) component implies the vector's vertical part changes negatively with the \( x \)-coordinate.
Understanding this allows us to determine how the vector field behaves over the unit circle, influencing the line integral's evaluation.
Unit Circle
A unit circle is a circle centered at the origin \( (0, 0) \) with a radius of 1. Its equation is given by \( x^2 + y^2 = 1 \). The unit circle is a fundamental concept in trigonometry and calculus, and in this exercise, it is the path denoted as \( C \).
By traveling counterclockwise along the unit circle starting from \( (1,0) \) to \( (0,1) \), we traverse one quarter of the circle. This part of the circle is an arc and represents one-fourth of the entire circle. Hence, when the line integral around the entire circle yields a result such as \( -2\pi \), we need to adjust this by the portion of the circle traversed. Thus, the result is divided by 4, reflecting just the quarter circle traveled, giving the final result of \( -\frac{\pi}{2} \).
Understanding the unit circle and the path is crucial because it informs us how much of the vector field's effect is accumulated in the line integral.

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Most popular questions from this chapter

Use a parametrization to find the flux \(\iint_{S} \mathbf{F} \cdot \mathbf{n} d \sigma\) across the surface in the specified direction. \(\begin{array}{l}{\text { Cone frustum } \mathbf{F}=-x \mathbf{i}-y \mathbf{j}+z^{2} \mathbf{k} \text { outward (normal away }} \\ {\text { from the } z \text { -axis) through the portion of the cone } z=\sqrt{x^{2}+y^{2}}} \\\ {\text { between the planes } z=1 \text { and } z=2}\end{array}\)

Hyperboloid of one sheet a. Find a parametrization for the hyperboloid of one sheet \(x^{2}+y^{2}-z^{2}=1\) in terms of the angle \(\theta\) associated with the circle \(x^{2}+y^{2}=r^{2}\) and the hyperbolic parameter \(u\) associated with the hyperbolic function \(r^{2}-z^{2}=1 .\) Hint: \(\cosh ^{2} u-\sinh ^{2} u=1 . )\) b. Generalize the result in part (a) to the hyperboloid \(\left(x^{2} / a^{2}\right)+\left(y^{2} / b^{2}\right)-\left(z^{2} / c^{2}\right)=1\)

Use a CAS to perform the following steps for finding the work done by force \(\mathbf{F}\) over the given path: a. Find \(d \mathbf{r}\) for the path \(\mathbf{r}(t)=g(t) \mathbf{i}+h(t) \mathbf{j}+k(t) \mathbf{k}\) b. Evaluate the force \(\mathbf{F}\) along the path. c. Evaluate \(\int_{C} \mathbf{F} \cdot d \mathbf{r}\) $$ \begin{aligned} \mathbf{F} &=\frac{3}{1+x^{2}} \mathbf{i}+\frac{2}{1+y^{2}} \mathbf{j} ; \quad \mathbf{r}(t)=(\cos t) \mathbf{i}+(\sin t) \mathbf{j} \\ 0 & \leq t \leq \pi \end{aligned} $$

Find the area of the region cut from the plane \(x+2 y+2 z=5\) by the cylinder whose walls are \(x=y^{2}\) and \(x=2-y^{2}\).

In Exercises \(43-46,\) use a CAS and Green's Theorem to find the counterclockwise circulation of the field \(F\) around the simple closed curve C. Perform the following CAS steps. $$\begin{array}{l}{\text { a. Plot } C \text { in the } x y \text { -plane. }} \\\ {\text { b. Determine the integrand }(\partial N / \partial x)-(\partial M / \partial y) \text { for the tangen- }} \\ {\text { tial form of Green's Theorem. }} \\ {\text { c. Determine the (double integral) limits of integration from }} \\ {\text { your plot in part (a) and evaluate the curl integral for the }} \\ {\text { circulation. }}\end{array}$$ $$\begin{array}{l}{\mathbf{F}=x^{-1} e^{y} \mathbf{i}+\left(e^{y} \ln x+2 x\right) \mathbf{j}} \\ {C : \text { The boundary of the region defined by } y=1+x^{4}(\text { below }) \text { and }} \\ {y=2 \text { (above) }}\end{array}$$

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