Problem 17
Question
Evaluate the Cauchy principal value of the given improper integral. $$ \int_{-\infty}^{\infty} \frac{1}{\left(x^{2}+4\right)^{2}} d x $$
Step-by-Step Solution
Verified Answer
The Cauchy principal value is \( \frac{\pi}{16} \).
1Step 1: Identify the Type of Integral
The integral given is an improper integral that needs to be handled using Cauchy principal value because it extends from negative infinity to infinity.
2Step 2: Define the Integral with Cauchy Principal Value
The Cauchy principal value of the integral \( \int_{-\infty}^{\infty} f(x) \, dx \) is defined as \( \lim_{R \to \infty} \int_{-R}^{R} f(x) \, dx \). We will apply this definition to solve the problem.
3Step 3: Set Up the Specific Integral
We set up the integral as: \[ PV \int_{-\infty}^{\infty} \frac{1}{(x^2 + 4)^2} \, dx = \lim_{R \to \infty} \int_{-R}^{R} \frac{1}{(x^2+4)^2} \, dx \] and then focus on evaluating this integral.
4Step 4: Use Symmetry of the Function
The function \( \frac{1}{(x^2+4)^2} \) is even, meaning the integral from \(-R\) to \(R\) can be simplified to twice the integral from \(0\) to \(R\): \[ \int_{-R}^{R} \frac{1}{(x^2+4)^2} \, dx = 2 \int_{0}^{R} \frac{1}{(x^2+4)^2} \, dx \]
5Step 5: Perform Substitution to Evaluate Integral
Use the substitution \( x = 2 \tan(\theta) \), which results in \( dx = 2 \sec^2(\theta) \ d\theta \) and \( x^2 + 4 = 4 \sec^2(\theta) \). The integral becomes:\[ 2 \int_{0}^{\arctan(\frac{R}{2})} \frac{1}{16 \sec^4(\theta)} 2 \sec^2(\theta) \, d\theta \]which simplifies to \[ \frac{1}{4} \int_{0}^{\arctan(\frac{R}{2})} \cos^2(\theta) \, d\theta \]
6Step 6: Simplify and Integrate
Use the identity \( \cos^2(\theta) = \frac{1 + \cos(2\theta)}{2} \) to rewrite the integral:\[ \frac{1}{4} \int_{0}^{\arctan\left(\frac{R}{2}\right)} \left(\frac{1 + \cos(2\theta)}{2}\right) \, d\theta \approx \frac{1}{4} \left[ \frac{1}{2} \theta + \frac{1}{4} \sin(2\theta) \right]_{0}^{\arctan(\frac{R}{2})} \]
7Step 7: Evaluate the Definite Integral and Limit
Evaluate the definite integral\[ \frac{1}{4} \left[ \frac{1}{2} \arctan\left(\frac{R}{2}\right) + \frac{1}{4} \sin\left(2 \arctan\left(\frac{R}{2}\right)\right) \right] - \left[ \frac{1}{4} \times 0 \right] \]And then, as \( R \to \infty \), the sine term vanishes, ultimately \( \lim_{R \to \infty} \frac{1}{4} \cdot \frac{\pi}{4} = \frac{\pi}{16} \).
8Step 8: Finalize the Cauchy Principal Value
Thus, the Cauchy principal value of the integral is \( \frac{\pi}{16} \).
Key Concepts
Improper IntegralSymmetry in IntegralsSubstitution MethodDefinite Integration
Improper Integral
Improper integrals often arise when we calculate functions extending towards infinity. These integrals are called 'improper' because they do not adhere to the traditional bounds of integration. A common way to deal with them is to use limits.
For an integral like \( \int_{-\infty}^{\infty} \frac{1}{(x^2+4)^2} \, dx \), the bounds go from negative to positive infinity. Here, the Cauchy principal value is useful.
By calculating the limit of integrals with finite bounds \(-R\) to \(R\), we deal with the infinite range in a manageable way. This approach provides a well-defined value even if the integral might not converge traditionally.
For an integral like \( \int_{-\infty}^{\infty} \frac{1}{(x^2+4)^2} \, dx \), the bounds go from negative to positive infinity. Here, the Cauchy principal value is useful.
By calculating the limit of integrals with finite bounds \(-R\) to \(R\), we deal with the infinite range in a manageable way. This approach provides a well-defined value even if the integral might not converge traditionally.
- By analyzing limits, we handle the infinity boundaries.
- This method provides a convergence mechanism for divergent-like integrals.
Symmetry in Integrals
Symmetry plays a crucial role in simplifying integrals.
When a function is even, i.e., symmetric around the y-axis, the integration range from \(-R\) to \(R\) becomes twice the range from \(0\) to \(R\). This wonderful property of even functions makes calculations simpler.
In our example, \( \frac{1}{(x^2+4)^2} \) is even because replacing \(x\) with \(-x\) doesn’t change the function. Therefore, the interval \([-R, R]\) becomes \(2\int_{0}^{R} \frac{1}{(x^2+4)^2} \, dx\).
When a function is even, i.e., symmetric around the y-axis, the integration range from \(-R\) to \(R\) becomes twice the range from \(0\) to \(R\). This wonderful property of even functions makes calculations simpler.
In our example, \( \frac{1}{(x^2+4)^2} \) is even because replacing \(x\) with \(-x\) doesn’t change the function. Therefore, the interval \([-R, R]\) becomes \(2\int_{0}^{R} \frac{1}{(x^2+4)^2} \, dx\).
- This property halves the work required to evaluate the integral.
- Only the positive half of the number line needs evaluation initially.
Substitution Method
The substitution method is a common technique for simplifying integrals by changing variables.
In our problem, we use the substitution \( x = 2 \tan(\theta) \). This transforms the integral and simplifies the expressions we need to integrate.
When substituting, we also compute the derivative, changing \(dx\) to \(2 \sec^2(\theta) \, d\theta\), and simplify \(x^2 + 4\) to \(4 \sec^2(\theta)\).
These changes help to integrate the function in terms of \(\theta\), making the problem more tractable.
In our problem, we use the substitution \( x = 2 \tan(\theta) \). This transforms the integral and simplifies the expressions we need to integrate.
When substituting, we also compute the derivative, changing \(dx\) to \(2 \sec^2(\theta) \, d\theta\), and simplify \(x^2 + 4\) to \(4 \sec^2(\theta)\).
These changes help to integrate the function in terms of \(\theta\), making the problem more tractable.
- The goal is to turn the original integral into a more straightforward form.
- This involves transforming both the function and the bounds of integration.
Definite Integration
Definite integration gives a numerical value representing the area under a curve between specific limits.
For the Cauchy principal value of our problem, integrating between finite bounds \([-R, R]\) transforms into evaluating a definite integral from 0 to \(R\).
Calculating these values provides insight into the behavior of the function across a specific range.
In our result, definite integration points to the evaluated limit, \(\frac{\pi}{16}\), describing the total net area spanning negative to positive infinity.
For the Cauchy principal value of our problem, integrating between finite bounds \([-R, R]\) transforms into evaluating a definite integral from 0 to \(R\).
Calculating these values provides insight into the behavior of the function across a specific range.
In our result, definite integration points to the evaluated limit, \(\frac{\pi}{16}\), describing the total net area spanning negative to positive infinity.
- It involves calculating an exact value, not a formula or expression.
- The outcome demonstrates how the integral converges over an infinite interval.
Other exercises in this chapter
Problem 16
Expand the given function in a Taylor series centered at the indicated point \(z_{0}\). Give the radius of convergence \(R\) of each series. $$ f(z)=\frac{1}{z}
View solution Problem 16
Determine whether the given geometric series is convergent or divergent. If convergent, find its sum. $$ \sum_{k=1}^{\infty} 4 i\left(\frac{1}{3}\right)^{k-1} $
View solution Problem 17
Determine the order of the poles for the given function. $$ f(z)=\frac{1+4 i}{(z+2)(z+i)^{4}} $$
View solution Problem 17
Use the theory of residues to compute the inverse Laplace transform \(\mathscr{L}^{-1}\\{F(s)\\}\) for the given function \(F(s)\). $$ \frac{1}{s^{4}-1} $$
View solution