Problem 29
Question
Evaluate the given iterated integral by changing to polar coordinates. $$ \int_{0}^{1} \int_{\sqrt{1-x^{2}}}^{\sqrt{4}-x^{2}} \frac{x^{2}}{x^{2}+y^{2}} d y d x+\int_{1}^{2} \int_{0}^{\sqrt{4}-x^{2}} \frac{x^{2}}{x^{2}+y^{2}} d y d x $$
Step-by-Step Solution
Verified Answer
The value of the iterated integral is \( \frac{3\pi}{8} \).
1Step 1: Analyze the Integral Bounds
Observe that the integral is split into two parts. For the first part, the outer limits range from 0 to 1 with the inner limits from \( y = \sqrt{1-x^2} \) to \( y = \sqrt{4-x^2} \). The second part has outer limits from 1 to 2, and inner limits of \( y = 0 \) to \( y = \sqrt{4-x^2} \). These describe a region under two parts of a circle divided at \( x = 1 \).
2Step 2: Set Up Polar Coordinates
Recall that in polar coordinates, \( x = r \cos(\theta) \) and \( y = r \sin(\theta) \). The transformation requires the region to be split as follows: for \( 0 \leq x \leq 1 \), \( r \) ranges from 1 to 2, and for \( 1 \leq x \leq 2 \), \( r \equiv \sqrt{x^2+y^2} \) ranges from 1 to 2. \( \theta \) goes from 0 to \( \pi/2 \) for both parts.
3Step 3: Convert the Function to Polar Coordinates
Substitute \( x = r \cos(\theta) \) and \( y = r \sin(\theta) \) into the expression \( \frac{x^2}{x^2+y^2} = \cos^2(\theta) \). The differential element \( dA = dy \, dx \) converts into \( r \, dr \, d\theta \) in polar coordinates.
4Step 4: Evaluate the Polar Integral
The integral becomes \( \int_{0}^{\pi/2} \int_{1}^{2} \cos^2(\theta) \, r \, dr \, d\theta \). First, evaluate the integral with respect to \( r \):\[\int_{1}^{2} r \, dr = \left[ \frac{r^2}{2} \right]_{1}^{2} = \frac{4}{2} - \frac{1}{2} = \frac{3}{2}\]Then, the integral with respect to \( \theta \):\[\int_{0}^{\pi/2} \cos^2(\theta) \, d\theta\]
5Step 5: Solve the Theta Integral
Use the trigonometric identity \( \cos^2(\theta) = \frac{1}{2}(1+\cos(2\theta)) \) to integrate:\[\int_{0}^{\pi/2} \cos^2(\theta) \, d\theta = \frac{1}{2} \int_{0}^{\pi/2} (1 + \cos(2\theta)) \, d\theta \]Evaluate this:\[\frac{1}{2} \left[ \theta + \frac{1}{2} \sin(2\theta) \right]_{0}^{\pi/2} = \frac{1}{2} \left( \frac{\pi}{2} + 0 \right) = \frac{\pi}{4}\]
6Step 6: Calculate the Final Result
Multiply the results of the \( r \) and \( \theta \) integrals: \( \frac{3}{2} \times \frac{\pi}{4} = \frac{3\pi}{8} \). Thus, the integral over the given region is \( \frac{3\pi}{8} \).
Key Concepts
Iterated IntegralTrigonometric IdentityTransformation to Polar CoordinatesIntegration in Polar Coordinates
Iterated Integral
An iterated integral refers to the successive integration of a function in multiple variables over designated limits. In the given problem, there are two variables, \(x\) and \(y\). The iterated integral is split into two parts:
- The first part integrates \(y\) from \(\sqrt{1-x^2}\) to \(\sqrt{4-x^2}\) while \(x\) goes from 0 to 1.
- The second part integrates \(y\) from 0 to \(\sqrt{4-x^2}\), with \(x\) ranging from 1 to 2.
Trigonometric Identity
Trigonometric identities are equations involving trigonometric functions that are true for every value of the occurring variables where both sides of the identity are defined. They are immensely helpful in calculus, especially during integration.In this exercise, one such identity used is \(\cos^2(\theta) = \frac{1}{2}(1 + \cos(2\theta))\). This identity facilitates the transformation of the integral into a form that is easier to compute. It helps break down the squared terms into coefficients and simpler sine and cosine functions that are straightforward to integrate.Applying this identity in the polar integral simplifies the integration over \(\theta\), transforming \(\cos^2(\theta)\) which is straightforward to integrate using the identity. This results in a simple evaluation over a defined interval.
Transformation to Polar Coordinates
Transforming Cartesian coordinates to polar coordinates involves the use of relationships between \(x\), \(y\), and the radius \(r\) along with the angle \(\theta\). These relationships are defined as:
- \(x = r \cos(\theta)\)
- \(y = r \sin(\theta)\)
Integration in Polar Coordinates
Integration in polar coordinates utilizes the radial distance \(r\) and the angle \(\theta\) as variables. In the transformation from Cartesian to polar, the area element \(dA = dy \, dx\) changes to \(r \, dr \, d\theta\).The integral \[\int_{0}^{\pi/2} \int_{1}^{2} \cos^2(\theta) \, r \, dr \, d\theta\] involves evaluating two separate integrals.First, integrating with respect to \(r\). Here, \(r\) ranges from 1 to 2, and as a result the integral becomes:\[\left[ \frac{r^2}{2} \right]_{1}^{2} = \frac{3}{2}\]Next, integrate with respect to \(\theta\). This requires the prior trigonometric identity, leading to:\[\frac{1}{2} \left[ \theta + \frac{1}{2} \sin(2\theta) \right]_{0}^{\pi/2} = \frac{\pi}{4}\]Together, these calculations provide the full integral value as \(\frac{3\pi}{8}\), successfully evaluating the region described by the original iterated integral in a much simpler form.
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