Estimate the value of the integral: integral from 0
Estimate the value of the integral: $$ \int_0^{\infty} \frac{\cos ax}{4+x^2} \, dx $$
Explanation of Method
This problem asks for a numerical estimate of a definite integral, obtained by bounding the integrand (using monotonicity, a comparison inequality, or the Mean Value Theorem for integrals) rather than by finding a closed-form antiderivative; where possible, an exact value is then computed for comparison against the estimate.
We will estimate this integral using bounds and then compute the exact value.
Method 1: Simple bounds
Since $|\cos ax| \leq 1$ for all $x$:
$$\left|\frac{\cos ax}{4+x^2}\right| \leq \frac{1}{4+x^2}$$
Therefore:
$$\left|\int_0^{\infty} \frac{\cos ax}{4+x^2} \, dx\right| \leq \int_0^{\infty} \frac{1}{4+x^2} \, dx$$
Computing the right side:
$$\int_0^{\infty} \frac{dx}{4+x^2} = \int_0^{\infty} \frac{dx}{4(1+x^2/4)} = \frac{1}{4}\int_0^{\infty} \frac{dx}{1+(x/2)^2}$$
Let $u = x/2$, so $du = dx/2$:
$$= \frac{1}{4} \cdot 2\int_0^{\infty} \frac{du}{1+u^2} = \frac{1}{2}[\arctan u]_0^{\infty} = \frac{1}{2} \cdot \frac{\pi}{2} = \frac{\pi}{4}$$
Therefore:
$$\boxed{\left|I\right| \leq \frac{\pi}{4} \approx 0.785}$$
Method 2: Behavior for different values of $a$
The value of the integral depends on the parameter $a$.
Case 1: $a = 0$
$$I = \int_0^{\infty} \frac{1}{4+x^2} \, dx = \frac{\pi}{4}$$
Case 2: $a > 0$ (large)
For large $|a|$, $\cos ax$ oscillates rapidly, causing cancellation. The integral becomes smaller.
Case 3: $a < 0$
By symmetry of cosine: $\cos(-ax) = \cos(ax)$, so the integral is the same for $a$ and $-a$.
Method 3: Exact calculation using residue theorem or Laplace transform
The exact value can be computed using complex analysis or looking up tables.
The integral is related to the Laplace transform:
$$\mathcal{L}\{\cos(at)\}(s) = \frac{s}{s^2+a^2}$$
However, our integral has the form:
$$\int_0^{\infty} \frac{\cos ax}{4+x^2} \, dx$$
Using the formula for Fourier cosine transforms and properties of the Laplace transform, or using contour integration in the complex plane, the exact result is:
$$\boxed{I = \frac{\pi}{4}e^{-2|a|}}$$
Step-by-step verification of the formula
For $a = 0$:
$$I = \frac{\pi}{4}e^{0} = \frac{\pi}{4}$$
This matches our direct calculation. ✓
For $a > 0$, the integral decreases exponentially.
Numerical estimates for different values of $a$
Using $I = \frac{\pi}{4}e^{-2|a|}$:
| $a$ | $I = \frac{\pi}{4}e^{-2|a|}$ | Approximate value |
| 0 | $\frac{\pi}{4}$ | 0.785 |
| 0.5 | $\frac{\pi}{4}e^{-1}$ | 0.289 |
| 1 | $\frac{\pi}{4}e^{-2}$ | 0.106 |
| 2 | $\frac{\pi}{4}e^{-4}$ | 0.014 |
| 5 | $\frac{\pi}{4}e^{-10}$ | $3.6 \times 10^{-5}$ |
Alternative derivation using symmetry
Since $\cos ax$ is even, we can write:
$$\int_0^{\infty} \frac{\cos ax}{4+x^2} \, dx = \frac{1}{2}\int_{-\infty}^{\infty} \frac{\cos ax}{4+x^2} \, dx$$
This integral can be evaluated using the residue theorem from complex analysis.
The function has poles at $x = \pm 2i$ in the complex plane.
For $a > 0$, closing the contour in the upper half-plane and using the residue at $x = 2i$:
$$\text{Residue at } x = 2i: \lim_{x \to 2i}(x-2i)\frac{e^{iax}}{(x-2i)(x+2i)} = \frac{e^{ia(2i)}}{4i} = \frac{e^{-2a}}{4i}$$
By the residue theorem:
$$\int_{-\infty}^{\infty} \frac{\cos ax}{4+x^2} \, dx = 2\pi i \cdot \frac{e^{-2a}}{4i} = \frac{\pi e^{-2a}}{2}$$
Therefore:
$$\int_0^{\infty} \frac{\cos ax}{4+x^2} \, dx = \frac{1}{2} \cdot \frac{\pi e^{-2a}}{2} = \frac{\pi e^{-2a}}{4}$$
For $a < 0$, using $\cos(-ax) = \cos(ax)$, we get $e^{-2|a|}$.
Final answer
$$\boxed{\int_0^{\infty} \frac{\cos ax}{4+x^2} \, dx = \frac{\pi}{4}e^{-2|a|}}$$
Bounds:
$$0 \leq I \leq \frac{\pi}{4} \approx 0.785$$
The maximum occurs at $a = 0$, and the integral decays exponentially as $|a|$ increases.
Summary
- For $a = 0$: $I = \frac{\pi}{4} \approx 0.785$
- For general $a$: $I = \frac{\pi}{4}e^{-2|a|}$
- The integral decreases exponentially with $|a|$
- Upper bound: $0 \leq I \leq \frac{\pi}{4}$
Key insights:
- The integral depends exponentially on the parameter $a$
- Maximum value is $\frac{\pi}{4}$ at $a = 0$
- Rapid oscillation of $\cos ax$ causes cancellation for large $|a|$
- The formula $I = \frac{\pi}{4}e^{-2|a|}$ is exact
- This is a standard result in Fourier analysis and signal processing
Result
Therefore:
$$\boxed{\left|I\right| \leq \frac{\pi}{4} \approx 0.785}$$
$$\boxed{I = \frac{\pi}{4}e^{-2|a|}}$$
$$\boxed{\int_0^{\infty} \frac{\cos ax}{4+x^2} \, dx = \frac{\pi}{4}e^{-2|a|}}$$