2.30.16 Problem 125
Internal
problem
ID
[13786]
Book
:
Handbook
of
exact
solutions
for
ordinary
differential
equations.
By
Polyanin
and
Zaitsev.
Second
edition
Section
:
Chapter
2,
Second-Order
Differential
Equations.
section
2.1.2-4
Problem
number
:
125
Date
solved
:
Thursday, January 01, 2026 at 02:37:43 AM
CAS
classification
:
[[_2nd_order, _with_linear_symmetries]]
2.30.16.1 second order bessel ode
0.252 (sec)
\begin{align*}
x^{2} y^{\prime \prime }+y^{\prime } x -\left (x^{2}+\left (\frac {1}{2}+n \right )^{2}\right ) y&=0 \\
\end{align*}
Entering second order bessel ode solverWriting the ode as \begin{align*} x^{2} y^{\prime \prime }+y^{\prime } x +\left (-x^{2}-\frac {1}{4}-n -n^{2}\right ) y = 0\tag {1} \end{align*}
Bessel ode has the form
\begin{align*} x^{2} y^{\prime \prime }+y^{\prime } x +\left (-n^{2}+x^{2}\right ) y = 0\tag {2} \end{align*}
The generalized form of Bessel ode is given by Bowman (1958) as the following
\begin{align*} x^{2} y^{\prime \prime }+\left (1-2 \alpha \right ) x y^{\prime }+\left (\beta ^{2} \gamma ^{2} x^{2 \gamma }-n^{2} \gamma ^{2}+\alpha ^{2}\right ) y = 0\tag {3} \end{align*}
With the standard solution
\begin{align*} y&=x^{\alpha } \left (c_1 \operatorname {BesselJ}\left (n , \beta \,x^{\gamma }\right )+c_2 \operatorname {BesselY}\left (n , \beta \,x^{\gamma }\right )\right )\tag {4} \end{align*}
Comparing (3) to (1) and solving for \(\alpha ,\beta ,n,\gamma \) gives
\begin{align*} \alpha &= 0\\ \beta &= i\\ n &= -\frac {1}{2}-n\\ \gamma &= 1 \end{align*}
Substituting all the above into (4) gives the solution as
\begin{align*} y = c_1 \operatorname {BesselJ}\left (-\frac {1}{2}-n , i x \right )+c_2 \operatorname {BesselY}\left (-\frac {1}{2}-n , i x \right ) \end{align*}
Summary of solutions found
\begin{align*}
y &= c_1 \operatorname {BesselJ}\left (-\frac {1}{2}-n , i x \right )+c_2 \operatorname {BesselY}\left (-\frac {1}{2}-n , i x \right ) \\
\end{align*}
2.30.16.2 ✓ Maple. Time used: 0.003 (sec). Leaf size: 19
ode:=x^2*diff(diff(y(x),x),x)+x*diff(y(x),x)-(x^2+(n+1/2)^2)*y(x) = 0;
dsolve(ode,y(x), singsol=all);
\[
y = c_1 \operatorname {BesselI}\left (n +\frac {1}{2}, x\right )+c_2 \operatorname {BesselK}\left (n +\frac {1}{2}, x\right )
\]
Maple trace
Methods for second order ODEs:
--- Trying classification methods ---
trying a quadrature
checking if the LODE has constant coefficients
checking if the LODE is of Euler type
trying a symmetry of the form [xi=0, eta=F(x)]
checking if the LODE is missing y
-> Trying a Liouvillian solution using Kovacics algorithm
<- No Liouvillian solutions exists
-> Trying a solution in terms of special functions:
-> Bessel
<- Bessel successful
<- special function solution successful
2.30.16.3 ✓ Mathematica. Time used: 0.031 (sec). Leaf size: 34
ode=x^2*D[y[x],{x,2}]+x*D[y[x],x]-(x^2+(n+1/2)^2)*y[x]==0;
ic={};
DSolve[{ode,ic},y[x],x,IncludeSingularSolutions->True]
\begin{align*} y(x)&\to c_1 \operatorname {BesselJ}\left (n+\frac {1}{2},-i x\right )+c_2 \operatorname {BesselY}\left (n+\frac {1}{2},-i x\right ) \end{align*}
2.30.16.4 ✗ Sympy
from sympy import *
x = symbols("x")
n = symbols("n")
y = Function("y")
ode = Eq(x**2*Derivative(y(x), (x, 2)) + x*Derivative(y(x), x) - (x**2 + (n + 1/2)**2)*y(x),0)
ics = {}
dsolve(ode,func=y(x),ics=ics)
False