Chapter 6: Problem 149
Evaluate the line integrals by applying Green’s theorem. \(\int_{C} \sin x \cos y d x+(x y+\cos x \sin y) d y,\) where \(C\) is the boundary of the region lying between the graphs of \(y=x\) and \(y=\sqrt{x}\) oriented in the counterclockwise direction
Short Answer
Expert verified
The line integral evaluates to \( \frac{1}{12} \).
Step by step solution
01
Understanding the Problem
We are given a line integral of the form \( \int_{C} P \, dx + Q \, dy \) where \( P = \sin x \cos y \) and \( Q = xy + \cos x \sin y \). The curve \( C \) is the boundary of the region between the curves \( y = x \) and \( y = \sqrt{x} \), oriented counterclockwise. We will apply Green's Theorem to evaluate the integral.
02
Green's Theorem Introduction
Green's Theorem relates a line integral around a simple closed curve \( C \) to a double integral over the region \( R \) bounded by \( C \). The theorem is stated as \( \oint_{C} P \, dx + Q \, dy = \iint_{R} \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) \, dA \). We need to calculate \( \frac{\partial Q}{\partial x} \) and \( \frac{\partial P}{\partial y} \).
03
Calculating the Partial Derivatives
Compute \( \frac{\partial Q}{\partial x} = \frac{\partial}{\partial x} (xy + \cos x \sin y) = y - \sin x \sin y \). Compute \( \frac{\partial P}{\partial y} = \frac{\partial}{\partial y} (\sin x \cos y) = -\sin x \sin y \).
04
Setting up the Double Integral
Now plug the partial derivatives into Green's Theorem: \( \oint_{C} P \, dx + Q \, dy = \iint_{R} (y - \sin x \sin y + \sin x \sin y ) \, dA = \iint_{R} y \, dA \). We see that the terms \( - \sin x \sin y \) cancel out.
05
Define the Region of Integration
The region \( R \) is bounded by \( y = x \) and \( y = \sqrt{x} \), with the x-range from \( 0 \) to \( 1 \). For each \( x \) value, \( y \) ranges from \( x \) to \( \sqrt{x} \).
06
Set Up the Double Integral Limits
Transform the double integral into \( \int_{0}^{1} \int_{x}^{\sqrt{x}} y \, \, dy \, dx \). This means we first integrate \( y \) from \( x \) to \( \sqrt{x} \), and then integrate the result from \( 0 \) to \( 1 \) with respect to \( x \).
07
Solve the Inner Integral
Perform the inner integral: \( \int_{x}^{\sqrt{x}} y \, dy = \left[ \frac{y^2}{2} \right]_{x}^{\sqrt{x}} = \frac{x}{2} - \frac{x^2}{2} \).
08
Solve the Outer Integral
Now solve the outer integral: \( \int_{0}^{1} \left( \frac{x}{2} - \frac{x^2}{2} \right) \, dx \). This becomes \( \left[ \frac{x^2}{4} - \frac{x^3}{6} \right]_{0}^{1} = \frac{1}{4} - \frac{1}{6} = \frac{1}{12} \).
09
Final Answer
The result of applying Green's Theorem to the line integral is \( \frac{1}{12} \).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Line Integrals
Line integrals allow us to integrate functions along a curve. Imagine you are wrapping a rope around a shape and measuring some quantity along that path. A line integral helps in calculating the total value of that quantity. In this problem, we have a line integral of the form \( \int_{C} P \, dx + Q \, dy \), representing how the functions \( P \) and \( Q \) accumulate over the curve \( C \), which is the boundary between the regions defined by \( y = x \) and \( y = \sqrt{x} \). Line integrals are very useful in physics for calculating work done by a force field along a path. They also connect with Green's Theorem which can transform a line integral into an easier double integral over the region enclosed by the path.
Partial Derivatives
Partial derivatives represent how a function changes as one of its variables change, keeping the others constant. When dealing with a function of two variables, such as \( P(x, y) \) and \( Q(x, y) \), we calculate how each function changes with respect to \( x \) and \( y \). In our solution, \( \frac{\partial Q}{\partial x} \) and \( \frac{\partial P}{\partial y} \) were key calculations. These derivatives are part of Green’s Theorem, which involves subtracting \( \frac{\partial P}{\partial y} \) from \( \frac{\partial Q}{\partial x} \). This computation changes the line integral into a more straightforward double integral, simplifying the problem solving process.
Double Integral
Double integrals allow us to sum functions over two-dimensional areas, much like a summation that happens in layers over a region. In this exercise, we convert a complex line integral into a double integral over the region \( R \) using Green’s Theorem. To set up a double integral, we must define limits correctly, understanding how \( x \) and \( y \) vary over the area \( R \). For the given problem, \( R \) is between \( y = x \) and \( y = \sqrt{x} \), making the integration limits from \( x \) to \( \sqrt{x} \) for \( y \), and from 0 to 1 for \( x \). This setup simplifies the evaluation by focusing solely on the region rather than the boundary, providing a nice symmetrical solution.
Integral Calculus
Integral calculus is a fundamental tool for understanding how functions accumulate values over intervals, whether those are lines, areas, or volumes. It is split mainly into two parts: definite and indefinite integrals. The definite integral, which we are focusing on here, provides the total accumulation over a domain. Green’s Theorem, which was applied in this exercise to transform the line integral, is a classic example of the power of integral calculus. It switches between integration in different formats (line to double) and thus unlocks a simpler way to solve problems. Mastering these transitions between different types of integrals is a powerful skill in calculus, providing tools to analyze everything from physics to engineering disciplines.