Chapter 9: Problem 11
Use Green's theorem to evaluate the given line integral. $$ \begin{aligned} &\oint_{C} x y d x+x^{2} d y \text { , where } C \text { is the boundary of the region }\\\ &\begin{array}{lll} \text { determined by the graphs of } x & 0, x^{2}+y^{2} & 1, x \geq 0 \end{array} \end{aligned} $$
Short Answer
Expert verified
The value of the line integral is 0.
Step by step solution
01
Understand Green's Theorem
Green's Theorem relates a line integral around a simple closed curve \( C \) to a double integral over the plane region \( D \) bounded by \( C \). The theorem is stated as: \[ \oint_C P\,dx + Q\,dy = \iint_D \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) dA \] where \( P(x, y) = xy \) and \( Q(x, y) = x^2 \).
02
Identify \( P(x, y) \) and \( Q(x, y) \)
From the line integral given, \( P(x, y) = xy \) and \( Q(x, y) = x^2 \). These are the components of the vector field.
03
Compute Partial Derivatives
Compute \( \frac{\partial Q}{\partial x} \) and \( \frac{\partial P}{\partial y} \). For \( Q(x, y) = x^2 \), \( \frac{\partial Q}{\partial x} = 2x \). For \( P(x, y) = xy \), \( \frac{\partial P}{\partial y} = x \).
04
Set Up Double Integral
The double integral required by Green's theorem is: \[ \iint_D \left( 2x - x \right) \, dA = \iint_D x \, dA \]
05
Define the Region \( D \)
The region \( D \) is the area bounded by the circle \( x^2 + y^2 = 1 \) in the right half-plane (\( x \geq 0 \)). This region can be described in polar coordinates with \( r \) ranging from 0 to 1, and \( \theta \) ranging from 0 to \( \pi \).
06
Convert to Polar Coordinates
In polar coordinates, the integral becomes: \[ \iint_D x \ dA = \int_0^{\pi} \int_0^1 (r\cos\theta) r \, dr \, d\theta \] where \( x = r\cos\theta \) and the differential \( dA = r\, dr\, d\theta \).
07
Evaluate the Double Integral
First evaluate the inner integral with respect to \( r \): \[ \int_0^1 r^2 \cos\theta \, dr = \cos\theta \left[ \frac{r^3}{3} \right]_0^1 = \frac{\cos\theta}{3} \]. Then evaluate the outer integral: \[ \int_0^{\pi} \frac{\cos\theta}{3} \, d\theta = \frac{1}{3} \left[ \sin\theta \right]_0^{\pi} = \frac{1}{3} (0 - 0) = 0 \].
08
Conclude the Evaluation
The value of the line integral using Green's theorem is 0.
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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 is a type of integral where a function is evaluated along a curve. Imagine you're walking along a path, and at each point, you measure some quantity like temperature or elevation. The line integral essentially adds up all these measurements along the path. It's a powerful concept used in physics and engineering to assess quantities like work done by a force field on a particle moving through space.
A line integral can be expressed in the form \( \oint_{C} P\,dx + Q\,dy \) when working with vector fields, where \( P \) and \( Q \) are functions that represent the vector field components. In our case, \( P(x, y) = xy \) and \( Q(x, y) = x^2 \). This way, the line integral measures how this vector field interacts with the path \( C \).
A line integral can be expressed in the form \( \oint_{C} P\,dx + Q\,dy \) when working with vector fields, where \( P \) and \( Q \) are functions that represent the vector field components. In our case, \( P(x, y) = xy \) and \( Q(x, y) = x^2 \). This way, the line integral measures how this vector field interacts with the path \( C \).
- Path \( C \) is typically a closed curve.
- The line integral evaluates the entire field along this path.
Vector Field
A vector field assigns a vector to every point in a plane or space. It can represent various physical and mathematical quantities like velocity fields of a fluid or electromagnetic fields. For any point \( (x, y) \) in our vector field, there is a vector with components \( (P, Q) \).
In our exercise, the vector field is given by \( P(x, y) = xy \) and \( Q(x, y) = x^2 \).
In our exercise, the vector field is given by \( P(x, y) = xy \) and \( Q(x, y) = x^2 \).
- Each component \( P \) and \( Q \) describes a different aspect of the field at the point \( (x, y) \).
- Green's Theorem connects the line integral of the vector field over a closed path to a double integral over the plane region it encloses.
Polar Coordinates
Polar coordinates are an alternative to Cartesian coordinates for representing points in a plane. Instead of using \( x \) and \( y \), polar coordinates use \( r \) (the radius) and \( \theta \) (the angle). They are particularly useful for circular or radial regions.
In our problem, we need to evaluate a double integral over a circular region in the right half-plane. Switching to polar coordinates simplifies this process.
In our problem, we need to evaluate a double integral over a circular region in the right half-plane. Switching to polar coordinates simplifies this process.
- The circle \( x^2 + y^2 = 1 \) is easily parameterized with \( r = 0 \) to \( 1 \) and \( \theta = 0 \) to \( \pi \), covering only the right half.
- With polar coordinates, \( x \) becomes \( r\cos\theta \) and the area differential \( dA \) becomes \( r\, dr\, d\theta \).
Double Integral
A double integral is used to integrate over a two-dimensional area, and it's particularly handy when you need to compute the volume under a surface or to find accumulated quantities over a region.
To apply Green’s Theorem, we convert the line integral into a double integral over the region \( D \) enclosed by the curve \( C \). For our exercise, Green's Theorem simplifies the line integral to:\[iint_D \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) dA = \iint_D x \ dA \]
To apply Green’s Theorem, we convert the line integral into a double integral over the region \( D \) enclosed by the curve \( C \). For our exercise, Green's Theorem simplifies the line integral to:\[iint_D \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) dA = \iint_D x \ dA \]
- In our particular case, the region \( D \) is circular, requiring a switch to polar coordinates.
- Evaluation proceeds by first integrating with respect to \( r \) and then \( \theta \).