How Can Bessel Functions Be Integrated Using Recurrence Relations?

In summary, the conversation discusses finding the integral of $\displaystyle x^2J_0(x)$ in terms of higher Bessel functions and $\displaystyle \int J_0(x)$, where $J_0(x)$ satisfies the differential equation $\displaystyle x^2 J_0'' + x J_0' + x^2J_0 = 0$. The solution involves using the general formula $\displaystyle \int x^{n}\ J_{n-1}(x)\ dx = x^{n}\ J_{n}(x)$ and the fact that $J_0' = - J_1$ to integrate by parts and arrive at the formula $\displaystyle \int x^{2}\ J_{
  • #1
alexmahone
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0
Find $\displaystyle\int x^2J_0(x)$ in terms of higher Bessel functions and $\displaystyle\int J_0(x)$.
 
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  • #2
$J_0(x)$ satisfies

$x^2 J_0'' + x J_0' + x^2J_0 = 0$

Integrating gives

$\displaystyle \int \left(x^2 J_0'' + xJ_0'\right) dx + \int x^2 J_0dx = c$

or

$\displaystyle x^2 J_0' - x J_0 + \int J_0 dx + \int x^2 J_0 dx = c$

then use the fact the $J_0' = - J_1$
 
  • #3
Using the general formula...

$\displaystyle \int x^{n}\ J_{n-1}(x)\ dx = x^{n}\ J_{n}(x)$ (1)

... and taking into account that $\displaystyle J^{'}_{0}(x)= - J_{1}(x)$ , integration by parts gives You ...

$\displaystyle \int x^{2}\ J_{0}(x)\ dx = \int x\ x\ J_{0}(x)\ dx= x^{2}\ J_{1}(x) - \int x\ J_{1}(x)\ dx = x^{2}\ J_{1}(x) + x\ J_{0}(x) - \int J_{0}(x)\ dx$ (2)

Kind regards

$\chi$ $\sigma$
 
  • #4
Thanks.
 
  • #5


Integrating Bessel functions can be a challenging task, but it often leads to interesting results and connections between different mathematical concepts. In this case, we are asked to find the integral of $x^2J_0(x)$, where $J_0(x)$ is the Bessel function of the first kind with order 0.

To solve this integral, we can use the well-known recurrence relation for Bessel functions: $J_{n+1}(x) = \frac{2n}{x}J_n(x) - J_{n-1}(x)$. Using this relation, we can rewrite the integral as follows:

$\displaystyle\int x^2J_0(x) = \frac{2}{x}\int xJ_1(x) - \int J_0(x)$

We can further simplify the integral by using another recurrence relation: $xJ_n(x) = \frac{1}{2}\left(x^nJ_n(x)\right)'$. Applying this to our integral, we get:

$\displaystyle\int x^2J_0(x) = \frac{2}{x}\left(\frac{1}{2}\left(x^2J_1(x)\right)' - \int J_1(x)\right) - \int J_0(x)$

We can now use the well-known integral of $J_1(x)$ to simplify the expression further:

$\displaystyle\int x^2J_0(x) = \frac{2}{x}\left(\frac{1}{2}\left(x^2J_1(x)\right)' - \frac{J_0(x)}{x}\right) - \int J_0(x)$

Finally, we can use the recurrence relation once again to express $J_1(x)$ in terms of $J_0(x)$ and $J_2(x)$:

$\displaystyle\int x^2J_0(x) = \frac{2}{x}\left(\frac{1}{2}\left(x^2\left(\frac{2}{x}J_1(x) - J_0(x)\right)\right)' - \frac{J_0(x)}{x}\right) - \int J_0(x)$

Simplifying the expression, we get:

$\displaystyle\int x^2J_0(x) = J_2(x)
 

FAQ: How Can Bessel Functions Be Integrated Using Recurrence Relations?

What are Bessel functions and why are they important?

Bessel functions are a type of special function in mathematics that arise in the solution of differential equations. They are important because they have many applications in physics, engineering, and other fields.

How are Bessel functions integrated?

Bessel functions can be integrated using various techniques such as substitution, integration by parts, and contour integration. The specific method used depends on the specific form of the Bessel function and the desired result.

What is the relationship between Bessel functions and Fourier transforms?

Bessel functions are closely related to Fourier transforms. In fact, they are the eigenfunctions of the Fourier transform and are used in the representation of periodic functions.

How do Bessel functions behave for different values of their parameters?

Depending on the values of their parameters, Bessel functions can exhibit different behaviors such as oscillations, decay, or growth. This behavior is important in understanding their applications in various fields.

Can Bessel functions be approximated or simplified?

Yes, Bessel functions can be approximated or simplified using various methods such as asymptotic expansions, series expansions, and special function identities. These approximations are often used to simplify calculations and solve problems in different areas of science and engineering.

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