Chapter 13: Problem 10
In Exercises \(3-10\), a function \(f(x, y)\) is given and a region \(R\) of the \(x-y\) plane is described. Set up and evaluate \(\iint_{R} f(x, y) d A\) using polar coordinates. \(f(x, y)=(x-y) /(x+y) ; R\) is the region enclosed by the lines \(y=x, y=0\) and the circle \(x^{2}+y^{2}=1\) in the first quadrant.
Short Answer
Step by step solution
Convert the Region to Polar Coordinates
Express the Function in Polar Coordinates
Set Up the Double Integral
Evaluate the Inner Integral
Evaluate the Outer Integral
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Polar Coordinates Transformation
In polar coordinates, any point \( (x, y) \) is represented as \( (r\cos\theta, r\sin\theta) \). For this problem, where the region is described by lines and a circle, the transformation helps in setting up the integral limits. The line \( y = x \) is simplified to \( \theta = \frac{\pi}{4} \), and \( y = 0 \) corresponds to \( \theta = 0 \). The circle \( x^2 + y^2 = 1 \) translates to \( r = 1 \). This makes defining the region in polar coordinates easier, covering angles \( 0 \leq \theta \leq \frac{\pi}{4} \) while \( 0 \leq r \leq 1 \).
Transitioning to polar coordinates allows us to leverage symmetries and simplifies the computational process of double integrals, converting complex regions into more manageable intervals.
Region in First Quadrant
Specifically, the problem defines R as enclosed by:
- The line \( y = x \)
- The line \( y = 0 \)
- The circle \( x^2 + y^2 = 1 \)
In polar coordinates, for the first quadrant, \( \theta \) ranges from \( 0 \) to \( \frac{\pi}{2} \). However, with the constraints of our region, \( \theta \) is further limited from \( 0 \) to \( \frac{\pi}{4} \), as \( y = x \) and \( y = 0 \) form the boundaries for this particular wedge-shaped region. Exploring this region bounded by these lines and curve helps in visualizing and accurately setting up our integration limits.
Double Integral Evaluation
\[ f(r, \theta) = \frac{r\cos\theta - r\sin\theta}{r\cos\theta + r\sin\theta} = \frac{\cos\theta - \sin\theta}{\cos\theta + \sin\theta}. \]
This reformatting is necessary, as it transforms the function into a more straightforward form based on trigonometric functions, making the integral easier to evaluate.
The area element \( dA \) in polar coordinates is \( r \cdot dr \cdot d\theta \), which accounts for the radial expansion of the element over angle increments. The integral becomes:
\[ \int_{0}^{\frac{\pi}{4}} \int_{0}^{1} \frac{\cos\theta - \sin\theta}{\cos\theta + \sin\theta} \cdot r \, dr \, d\theta. \]
This sets the stage to solve the integral by evaluating the bounds defined for \( r \) and \( \theta \). Carefully performing each step respects the transformed polar relationships.
Integral Substitution Method
In the outer integral \( \int_{0}^{\frac{\pi}{4}} \frac{1}{2} \frac{\cos\theta - \sin\theta}{\cos\theta + \sin\theta} \, d\theta \), substitution is used for simplifying the expression for integration. By substituting \( u = \cos\theta + \sin\theta \), we find \( du = (-\sin\theta + \cos\theta) \, d\theta \), aligning perfectly with our integrand. This substitution reduces the problem to integrating a simple logarithmic function:
\[ \frac{1}{2} \int \frac{1}{u} \, du = \frac{1}{2} \ln|u| + C. \]
The process of substitution not only streamlines the evaluation but also fractionates complex trigonometric relationships into more manageable algebraic expressions. Completing the evaluation gives the result \( \frac{1}{4} \ln(2) \), highlighting how substitution aids in reaching a clean solution.