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Bessel Functions Calculator

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Example
Created on 2024-06-20Asked by Olivia Allen (Solvelet student)
Find the value of the Bessel function of the first kind J0(x) J_0(x) at x=2 x = 2 .

Solution

Step 1: Identify the Bessel function of the first kind: J0(x)=m=0(1)m(m!)2(x2)2m. J_0(x) = \sum_{m=0}^{\infty} \frac{(-1)^m}{(m!)^2} \left( \frac{x}{2} \right)^{2m}. Step 2: Substitute x=2 x = 2 into the series: J0(2)=m=0(1)m(m!)2(22)2m=m=0(1)m(m!)2. J_0(2) = \sum_{m=0}^{\infty} \frac{(-1)^m}{(m!)^2} \left( \frac{2}{2} \right)^{2m} = \sum_{m=0}^{\infty} \frac{(-1)^m}{(m!)^2}. Step 3: Calculate the first few terms of the series for an approximation: J0(2)1112+122132+11+0.250.111+0.223. J_0(2) \approx 1 - \frac{1}{1^2} + \frac{1}{2^2} - \frac{1}{3^2} + \cdots \approx 1 - 1 + 0.25 - 0.111 + \cdots \approx 0.223. Step 4: Conclusion. The value of J0(2) J_0(2) is approximately 0.223. Solved on Solvelet with Basic AI Model
Some of the related questions asked by Samuel Torres on Solvelet
1. Find the first three zeros of the first kind of the Bessel function J0(x) J_0(x) 2. Determine whether the Bessel function of the second kind Y0(x) Y_0(x) is oscillatory or exponentially decaying for large x x .,
DefinitionBessel functions are a family of solutions to Bessels differential equation with a real or complex order alpha and that are not constant multiples of each other for different values of the argument. They are important in many problems in scienctific and engineering involving wave propagation (like sound, light, eletromagnetic wave), heat conduction, and vibration phenomena, with spherical or cylindric symmetry. Sine waves exhibit a unique property such that they oscillate, and this is why they are common in many areas of mathematical, physical, and engineering descriptions - such as waveforms, diffraction patterns and resonant frequencies. Bessel functions appear in the robust-object of wave acoustics, particularly inside the explanation of round acoustics. Example: In the case of a vibrating circular membrane, Bessel functions are used to describe the radial displacement at a position and time for points on the membrane.
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