4.2 problem 2

4.2.1 Maple step by step solution

Internal problem ID [5661]
Internal file name [OUTPUT/4909_Sunday_June_05_2022_03_10_11_PM_14604385/index.tex]

Book: ADVANCED ENGINEERING MATHEMATICS. ERWIN KREYSZIG, HERBERT KREYSZIG, EDWARD J. NORMINTON. 10th edition. John Wiley USA. 2011
Section: Chapter 5. Series Solutions of ODEs. Special Functions. Problem set 5.5. Bessel Functions Y(x). General Solution page 200
Problem number: 2.
ODE order: 2.
ODE degree: 1.

The type(s) of ODE detected by this program : "second order series method. Regular singular point. Difference is integer"

Maple gives the following as the ode type

[_Lienard]

\[ \boxed {x y^{\prime \prime }+5 y^{\prime }+y x=0} \] With the expansion point for the power series method at \(x = 0\).

The type of the expansion point is first determined. This is done on the homogeneous part of the ODE. \[ x y^{\prime \prime }+5 y^{\prime }+y x = 0 \] The following is summary of singularities for the above ode. Writing the ode as \begin {align*} y^{\prime \prime }+p(x) y^{\prime } + q(x) y &=0 \end {align*}

Where \begin {align*} p(x) &= \frac {5}{x}\\ q(x) &= 1\\ \end {align*}

Table 20: Table \(p(x),q(x)\) singularites.
\(p(x)=\frac {5}{x}\)
singularity type
\(x = 0\) \(\text {``regular''}\)
\(q(x)=1\)
singularity type

Combining everything together gives the following summary of singularities for the ode as

Regular singular points : \([0]\)

Irregular singular points : \([\infty ]\)

Since \(x = 0\) is regular singular point, then Frobenius power series is used. The ode is normalized to be \[ x y^{\prime \prime }+5 y^{\prime }+y x = 0 \] Let the solution be represented as Frobenius power series of the form \[ y = \moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n +r} \] Then \begin{align*} y^{\prime } &= \moverset {\infty }{\munderset {n =0}{\sum }}\left (n +r \right ) a_{n} x^{n +r -1} \\ y^{\prime \prime } &= \moverset {\infty }{\munderset {n =0}{\sum }}\left (n +r \right ) \left (n +r -1\right ) a_{n} x^{n +r -2} \\ \end{align*} Substituting the above back into the ode gives \begin{equation} \tag{1} x \left (\moverset {\infty }{\munderset {n =0}{\sum }}\left (n +r \right ) \left (n +r -1\right ) a_{n} x^{n +r -2}\right )+5 \left (\moverset {\infty }{\munderset {n =0}{\sum }}\left (n +r \right ) a_{n} x^{n +r -1}\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n +r}\right ) x = 0 \end{equation} Which simplifies to \begin{equation} \tag{2A} \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{n +r -1} a_{n} \left (n +r \right ) \left (n +r -1\right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}5 \left (n +r \right ) a_{n} x^{n +r -1}\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{1+n +r} a_{n}\right ) = 0 \end{equation} The next step is to make all powers of \(x\) be \(n +r -1\) in each summation term. Going over each summation term above with power of \(x\) in it which is not already \(x^{n +r -1}\) and adjusting the power and the corresponding index gives \begin{align*} \moverset {\infty }{\munderset {n =0}{\sum }}x^{1+n +r} a_{n} &= \moverset {\infty }{\munderset {n =2}{\sum }}a_{n -2} x^{n +r -1} \\ \end{align*} Substituting all the above in Eq (2A) gives the following equation where now all powers of \(x\) are the same and equal to \(n +r -1\). \begin{equation} \tag{2B} \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{n +r -1} a_{n} \left (n +r \right ) \left (n +r -1\right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}5 \left (n +r \right ) a_{n} x^{n +r -1}\right )+\left (\moverset {\infty }{\munderset {n =2}{\sum }}a_{n -2} x^{n +r -1}\right ) = 0 \end{equation} The indicial equation is obtained from \(n = 0\). From Eq (2B) this gives \[ x^{n +r -1} a_{n} \left (n +r \right ) \left (n +r -1\right )+5 \left (n +r \right ) a_{n} x^{n +r -1} = 0 \] When \(n = 0\) the above becomes \[ x^{-1+r} a_{0} r \left (-1+r \right )+5 r a_{0} x^{-1+r} = 0 \] Or \[ \left (x^{-1+r} r \left (-1+r \right )+5 r \,x^{-1+r}\right ) a_{0} = 0 \] Since \(a_{0}\neq 0\) then the above simplifies to \[ r \,x^{-1+r} \left (4+r \right ) = 0 \] Since the above is true for all \(x\) then the indicial equation becomes \[ r \left (4+r \right ) = 0 \] Solving for \(r\) gives the roots of the indicial equation as \begin {align*} r_1 &= 0\\ r_2 &= -4 \end {align*}

Since \(a_{0}\neq 0\) then the indicial equation becomes \[ r \,x^{-1+r} \left (4+r \right ) = 0 \] Solving for \(r\) gives the roots of the indicial equation as \([0, -4]\).

Since \(r_1 - r_2 = 4\) is an integer, then we can construct two linearly independent solutions \begin {align*} y_{1}\left (x \right ) &= x^{r_{1}} \left (\moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n}\right )\\ y_{2}\left (x \right ) &= C y_{1}\left (x \right ) \ln \left (x \right )+x^{r_{2}} \left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n}\right ) \end {align*}

Or \begin {align*} y_{1}\left (x \right ) &= \moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n}\\ y_{2}\left (x \right ) &= C y_{1}\left (x \right ) \ln \left (x \right )+\frac {\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n}}{x^{4}} \end {align*}

Or \begin {align*} y_{1}\left (x \right ) &= \moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n}\\ y_{2}\left (x \right ) &= C y_{1}\left (x \right ) \ln \left (x \right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n -4}\right ) \end {align*}

Where \(C\) above can be zero. We start by finding \(y_{1}\). Eq (2B) derived above is now used to find all \(a_{n}\) coefficients. The case \(n = 0\) is skipped since it was used to find the roots of the indicial equation. \(a_{0}\) is arbitrary and taken as \(a_{0} = 1\). Substituting \(n = 1\) in Eq. (2B) gives \[ a_{1} = 0 \] For \(2\le n\) the recursive equation is \begin{equation} \tag{3} a_{n} \left (n +r \right ) \left (n +r -1\right )+5 a_{n} \left (n +r \right )+a_{n -2} = 0 \end{equation} Solving for \(a_{n}\) from recursive equation (4) gives \[ a_{n} = -\frac {a_{n -2}}{n^{2}+2 n r +r^{2}+4 n +4 r}\tag {4} \] Which for the root \(r = 0\) becomes \[ a_{n} = -\frac {a_{n -2}}{n \left (n +4\right )}\tag {5} \] At this point, it is a good idea to keep track of \(a_{n}\) in a table both before substituting \(r = 0\) and after as more terms are found using the above recursive equation.

\(n\) \(a_{n ,r}\) \(a_{n}\)
\(a_{0}\) \(1\) \(1\)
\(a_{1}\) \(0\) \(0\)

For \(n = 2\), using the above recursive equation gives \[ a_{2}=-\frac {1}{r^{2}+8 r +12} \] Which for the root \(r = 0\) becomes \[ a_{2}=-{\frac {1}{12}} \] And the table now becomes

\(n\) \(a_{n ,r}\) \(a_{n}\)
\(a_{0}\) \(1\) \(1\)
\(a_{1}\) \(0\) \(0\)
\(a_{2}\) \(-\frac {1}{r^{2}+8 r +12}\) \(-{\frac {1}{12}}\)

For \(n = 3\), using the above recursive equation gives \[ a_{3}=0 \] And the table now becomes

\(n\) \(a_{n ,r}\) \(a_{n}\)
\(a_{0}\) \(1\) \(1\)
\(a_{1}\) \(0\) \(0\)
\(a_{2}\) \(-\frac {1}{r^{2}+8 r +12}\) \(-{\frac {1}{12}}\)
\(a_{3}\) \(0\) \(0\)

For \(n = 4\), using the above recursive equation gives \[ a_{4}=\frac {1}{\left (r +6\right ) \left (r +2\right ) \left (r +8\right ) \left (4+r \right )} \] Which for the root \(r = 0\) becomes \[ a_{4}={\frac {1}{384}} \] And the table now becomes

\(n\) \(a_{n ,r}\) \(a_{n}\)
\(a_{0}\) \(1\) \(1\)
\(a_{1}\) \(0\) \(0\)
\(a_{2}\) \(-\frac {1}{r^{2}+8 r +12}\) \(-{\frac {1}{12}}\)
\(a_{3}\) \(0\) \(0\)
\(a_{4}\) \(\frac {1}{\left (r +6\right ) \left (r +2\right ) \left (r +8\right ) \left (4+r \right )}\) \(\frac {1}{384}\)

For \(n = 5\), using the above recursive equation gives \[ a_{5}=0 \] And the table now becomes

\(n\) \(a_{n ,r}\) \(a_{n}\)
\(a_{0}\) \(1\) \(1\)
\(a_{1}\) \(0\) \(0\)
\(a_{2}\) \(-\frac {1}{r^{2}+8 r +12}\) \(-{\frac {1}{12}}\)
\(a_{3}\) \(0\) \(0\)
\(a_{4}\) \(\frac {1}{\left (r +6\right ) \left (r +2\right ) \left (r +8\right ) \left (4+r \right )}\) \(\frac {1}{384}\)
\(a_{5}\) \(0\) \(0\)

Using the above table, then the solution \(y_{1}\left (x \right )\) is \begin {align*} y_{1}\left (x \right )&= a_{0}+a_{1} x +a_{2} x^{2}+a_{3} x^{3}+a_{4} x^{4}+a_{5} x^{5}+a_{6} x^{6}\dots \\ &= 1-\frac {x^{2}}{12}+\frac {x^{4}}{384}+O\left (x^{6}\right ) \end {align*}

Now the second solution \(y_{2}\left (x \right )\) is found. Let \[ r_{1}-r_{2} = N \] Where \(N\) is positive integer which is the difference between the two roots. \(r_{1}\) is taken as the larger root. Hence for this problem we have \(N=4\). Now we need to determine if \(C\) is zero or not. This is done by finding \(\lim _{r\rightarrow r_{2}}a_{4}\left (r \right )\). If this limit exists, then \(C = 0\), else we need to keep the log term and \(C \neq 0\). The above table shows that \begin {align*} a_N &= a_{4} \\ &= \frac {1}{\left (r +6\right ) \left (r +2\right ) \left (r +8\right ) \left (4+r \right )} \end {align*}

Therefore \begin {align*} \lim _{r\rightarrow r_{2}}\frac {1}{\left (r +6\right ) \left (r +2\right ) \left (r +8\right ) \left (4+r \right )}&= \lim _{r\rightarrow -4}\frac {1}{\left (r +6\right ) \left (r +2\right ) \left (r +8\right ) \left (4+r \right )}\\ &= \textit {undefined} \end {align*}

Since the limit does not exist then the log term is needed. Therefore the second solution has the form \[ y_{2}\left (x \right ) = C y_{1}\left (x \right ) \ln \left (x \right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n +r_{2}}\right ) \] Therefore \begin{align*} \frac {d}{d x}y_{2}\left (x \right ) &= C y_{1}^{\prime }\left (x \right ) \ln \left (x \right )+\frac {C y_{1}\left (x \right )}{x}+\left (\moverset {\infty }{\munderset {n =0}{\sum }}\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x}\right ) \\ &= C y_{1}^{\prime }\left (x \right ) \ln \left (x \right )+\frac {C y_{1}\left (x \right )}{x}+\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-1+n +r_{2}} b_{n} \left (n +r_{2}\right )\right ) \\ \frac {d^{2}}{d x^{2}}y_{2}\left (x \right ) &= C y_{1}^{\prime \prime }\left (x \right ) \ln \left (x \right )+\frac {2 C y_{1}^{\prime }\left (x \right )}{x}-\frac {C y_{1}\left (x \right )}{x^{2}}+\moverset {\infty }{\munderset {n =0}{\sum }}\left (\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )^{2}}{x^{2}}-\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x^{2}}\right ) \\ &= C y_{1}^{\prime \prime }\left (x \right ) \ln \left (x \right )+\frac {2 C y_{1}^{\prime }\left (x \right )}{x}-\frac {C y_{1}\left (x \right )}{x^{2}}+\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-2+n +r_{2}} b_{n} \left (n +r_{2}\right ) \left (-1+n +r_{2}\right )\right ) \\ \end{align*} Substituting these back into the given ode \(x y^{\prime \prime }+5 y^{\prime }+y x = 0\) gives \[ x \left (C y_{1}^{\prime \prime }\left (x \right ) \ln \left (x \right )+\frac {2 C y_{1}^{\prime }\left (x \right )}{x}-\frac {C y_{1}\left (x \right )}{x^{2}}+\moverset {\infty }{\munderset {n =0}{\sum }}\left (\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )^{2}}{x^{2}}-\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x^{2}}\right )\right )+5 C y_{1}^{\prime }\left (x \right ) \ln \left (x \right )+\frac {5 C y_{1}\left (x \right )}{x}+5 \left (\moverset {\infty }{\munderset {n =0}{\sum }}\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x}\right )+\left (C y_{1}\left (x \right ) \ln \left (x \right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n +r_{2}}\right )\right ) x = 0 \] Which can be written as \begin{equation} \tag{7} \left (\left (y_{1}^{\prime \prime }\left (x \right ) x +y_{1}\left (x \right ) x +5 y_{1}^{\prime }\left (x \right )\right ) \ln \left (x \right )+x \left (\frac {2 y_{1}^{\prime }\left (x \right )}{x}-\frac {y_{1}\left (x \right )}{x^{2}}\right )+\frac {5 y_{1}\left (x \right )}{x}\right ) C +x \left (\moverset {\infty }{\munderset {n =0}{\sum }}\left (\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )^{2}}{x^{2}}-\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x^{2}}\right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n +r_{2}}\right ) x +5 \left (\moverset {\infty }{\munderset {n =0}{\sum }}\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x}\right ) = 0 \end{equation} But since \(y_{1}\left (x \right )\) is a solution to the ode, then \[ y_{1}^{\prime \prime }\left (x \right ) x +y_{1}\left (x \right ) x +5 y_{1}^{\prime }\left (x \right ) = 0 \] Eq (7) simplifes to \begin{equation} \tag{8} \left (x \left (\frac {2 y_{1}^{\prime }\left (x \right )}{x}-\frac {y_{1}\left (x \right )}{x^{2}}\right )+\frac {5 y_{1}\left (x \right )}{x}\right ) C +x \left (\moverset {\infty }{\munderset {n =0}{\sum }}\left (\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )^{2}}{x^{2}}-\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x^{2}}\right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n +r_{2}}\right ) x +5 \left (\moverset {\infty }{\munderset {n =0}{\sum }}\frac {b_{n} x^{n +r_{2}} \left (n +r_{2}\right )}{x}\right ) = 0 \end{equation} Substituting \(y_{1} = \moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n +r_{1}}\) into the above gives \begin{equation} \tag{9} \frac {\left (2 \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-1+n +r_{1}} a_{n} \left (n +r_{1}\right )\right ) x +4 \left (\moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n +r_{1}}\right )\right ) C}{x}+\frac {\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-2+n +r_{2}} b_{n} \left (n +r_{2}\right ) \left (-1+n +r_{2}\right )\right ) x^{2}+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n +r_{2}}\right ) x^{2}+5 \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-1+n +r_{2}} b_{n} \left (n +r_{2}\right )\right ) x}{x} = 0 \end{equation} Since \(r_{1} = 0\) and \(r_{2} = -4\) then the above becomes \begin{equation} \tag{10} \frac {\left (2 \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-1+n} a_{n} n \right ) x +4 \left (\moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n}\right )\right ) C}{x}+\frac {\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-6+n} b_{n} \left (n -4\right ) \left (-5+n \right )\right ) x^{2}+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n -4}\right ) x^{2}+5 \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-5+n} b_{n} \left (n -4\right )\right ) x}{x} = 0 \end{equation} Which simplifies to \begin{equation} \tag{2A} \left (\moverset {\infty }{\munderset {n =0}{\sum }}2 C \,x^{-1+n} a_{n} n \right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}4 C \,x^{-1+n} a_{n}\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-5+n} b_{n} \left (-5+n \right ) \left (n -4\right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-3+n} b_{n}\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}5 x^{-5+n} b_{n} \left (n -4\right )\right ) = 0 \end{equation} The next step is to make all powers of \(x\) be \(-5+n\) in each summation term. Going over each summation term above with power of \(x\) in it which is not already \(x^{-5+n}\) and adjusting the power and the corresponding index gives \begin{align*} \moverset {\infty }{\munderset {n =0}{\sum }}2 C \,x^{-1+n} a_{n} n &= \moverset {\infty }{\munderset {n =4}{\sum }}2 C \left (n -4\right ) a_{n -4} x^{-5+n} \\ \moverset {\infty }{\munderset {n =0}{\sum }}4 C \,x^{-1+n} a_{n} &= \moverset {\infty }{\munderset {n =4}{\sum }}4 C a_{n -4} x^{-5+n} \\ \moverset {\infty }{\munderset {n =0}{\sum }}x^{-3+n} b_{n} &= \moverset {\infty }{\munderset {n =2}{\sum }}b_{n -2} x^{-5+n} \\ \end{align*} Substituting all the above in Eq (2A) gives the following equation where now all powers of \(x\) are the same and equal to \(-5+n\). \begin{equation} \tag{2B} \left (\moverset {\infty }{\munderset {n =4}{\sum }}2 C \left (n -4\right ) a_{n -4} x^{-5+n}\right )+\left (\moverset {\infty }{\munderset {n =4}{\sum }}4 C a_{n -4} x^{-5+n}\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{-5+n} b_{n} \left (-5+n \right ) \left (n -4\right )\right )+\left (\moverset {\infty }{\munderset {n =2}{\sum }}b_{n -2} x^{-5+n}\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}5 x^{-5+n} b_{n} \left (n -4\right )\right ) = 0 \end{equation} For \(n=0\) in Eq. (2B), we choose arbitray value for \(b_{0}\) as \(b_{0} = 1\). For \(n=1\), Eq (2B) gives \[ -3 b_{1} = 0 \] Which when replacing the above values found already for \(b_{n}\) and the values found earlier for \(a_{n}\) and for \(C\), gives \[ -3 b_{1} = 0 \] Solving the above for \(b_{1}\) gives \[ b_{1}=0 \] For \(n=2\), Eq (2B) gives \[ -4 b_{2}+b_{0} = 0 \] Which when replacing the above values found already for \(b_{n}\) and the values found earlier for \(a_{n}\) and for \(C\), gives \[ -4 b_{2}+1 = 0 \] Solving the above for \(b_{2}\) gives \[ b_{2}={\frac {1}{4}} \] For \(n=3\), Eq (2B) gives \[ -3 b_{3}+b_{1} = 0 \] Which when replacing the above values found already for \(b_{n}\) and the values found earlier for \(a_{n}\) and for \(C\), gives \[ -3 b_{3} = 0 \] Solving the above for \(b_{3}\) gives \[ b_{3}=0 \] For \(n=N\), where \(N=4\) which is the difference between the two roots, we are free to choose \(b_{4} = 0\). Hence for \(n=4\), Eq (2B) gives \[ 4 C +\frac {1}{4} = 0 \] Which is solved for \(C\). Solving for \(C\) gives \[ C=-{\frac {1}{16}} \] For \(n=5\), Eq (2B) gives \[ 6 C a_{1}+b_{3}+5 b_{5} = 0 \] Which when replacing the above values found already for \(b_{n}\) and the values found earlier for \(a_{n}\) and for \(C\), gives \[ 5 b_{5} = 0 \] Solving the above for \(b_{5}\) gives \[ b_{5}=0 \] Now that we found all \(b_{n}\) and \(C\), we can calculate the second solution from \[ y_{2}\left (x \right ) = C y_{1}\left (x \right ) \ln \left (x \right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}b_{n} x^{n +r_{2}}\right ) \] Using the above value found for \(C=-{\frac {1}{16}}\) and all \(b_{n}\), then the second solution becomes \[ y_{2}\left (x \right )= -\frac {1}{16}\eslowast \left (1-\frac {x^{2}}{12}+\frac {x^{4}}{384}+O\left (x^{6}\right )\right ) \ln \left (x \right )+\frac {1+\frac {x^{2}}{4}+O\left (x^{6}\right )}{x^{4}} \] Therefore the homogeneous solution is \begin{align*} y_h(x) &= c_{1} y_{1}\left (x \right )+c_{2} y_{2}\left (x \right ) \\ &= c_{1} \left (1-\frac {x^{2}}{12}+\frac {x^{4}}{384}+O\left (x^{6}\right )\right ) + c_{2} \left (-\frac {1}{16}\eslowast \left (1-\frac {x^{2}}{12}+\frac {x^{4}}{384}+O\left (x^{6}\right )\right ) \ln \left (x \right )+\frac {1+\frac {x^{2}}{4}+O\left (x^{6}\right )}{x^{4}}\right ) \\ \end{align*} Hence the final solution is \begin{align*} y &= y_h \\ &= c_{1} \left (1-\frac {x^{2}}{12}+\frac {x^{4}}{384}+O\left (x^{6}\right )\right )+c_{2} \left (\left (-\frac {1}{16}+\frac {x^{2}}{192}-\frac {x^{4}}{6144}-\frac {O\left (x^{6}\right )}{16}\right ) \ln \left (x \right )+\frac {1+\frac {x^{2}}{4}+O\left (x^{6}\right )}{x^{4}}\right ) \\ \end{align*}

Summary

The solution(s) found are the following \begin{align*} \tag{1} y &= c_{1} \left (1-\frac {x^{2}}{12}+\frac {x^{4}}{384}+O\left (x^{6}\right )\right )+c_{2} \left (\left (-\frac {1}{16}+\frac {x^{2}}{192}-\frac {x^{4}}{6144}-\frac {O\left (x^{6}\right )}{16}\right ) \ln \left (x \right )+\frac {1+\frac {x^{2}}{4}+O\left (x^{6}\right )}{x^{4}}\right ) \\ \end{align*}

Verification of solutions

\[ y = c_{1} \left (1-\frac {x^{2}}{12}+\frac {x^{4}}{384}+O\left (x^{6}\right )\right )+c_{2} \left (\left (-\frac {1}{16}+\frac {x^{2}}{192}-\frac {x^{4}}{6144}-\frac {O\left (x^{6}\right )}{16}\right ) \ln \left (x \right )+\frac {1+\frac {x^{2}}{4}+O\left (x^{6}\right )}{x^{4}}\right ) \] Verified OK.

4.2.1 Maple step by step solution

\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & x y^{\prime \prime }+5 y^{\prime }+y x =0 \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 2 \\ {} & {} & y^{\prime \prime } \\ \bullet & {} & \textrm {Isolate 2nd derivative}\hspace {3pt} \\ {} & {} & y^{\prime \prime }=-\frac {5 y^{\prime }}{x}-y \\ \bullet & {} & \textrm {Group terms with}\hspace {3pt} y\hspace {3pt}\textrm {on the lhs of the ODE and the rest on the rhs of the ODE; ODE is linear}\hspace {3pt} \\ {} & {} & y^{\prime \prime }+\frac {5 y^{\prime }}{x}+y=0 \\ \bullet & {} & \textrm {Simplify ODE}\hspace {3pt} \\ {} & {} & x^{2} y^{\prime \prime }+5 y^{\prime } x +y x^{2}=0 \\ \bullet & {} & \textrm {Make a change of variables}\hspace {3pt} \\ {} & {} & y=\frac {u \left (x \right )}{x^{2}} \\ \bullet & {} & \textrm {Compute}\hspace {3pt} y^{\prime } \\ {} & {} & y^{\prime }=-\frac {2 u \left (x \right )}{x^{3}}+\frac {u^{\prime }\left (x \right )}{x^{2}} \\ \bullet & {} & \textrm {Compute}\hspace {3pt} y^{\prime \prime } \\ {} & {} & y^{\prime \prime }=\frac {6 u \left (x \right )}{x^{4}}-\frac {4 u^{\prime }\left (x \right )}{x^{3}}+\frac {u^{\prime \prime }\left (x \right )}{x^{2}} \\ \bullet & {} & \textrm {Apply change of variables to the ODE}\hspace {3pt} \\ {} & {} & u \left (x \right ) x^{2}+u^{\prime \prime }\left (x \right ) x^{2}+u^{\prime }\left (x \right ) x -4 u \left (x \right )=0 \\ \bullet & {} & \textrm {ODE is now of the Bessel form}\hspace {3pt} \\ \bullet & {} & \textrm {Solution to Bessel ODE}\hspace {3pt} \\ {} & {} & u \left (x \right )=c_{1} \mathit {BesselJ}\left (2, x\right )+c_{2} \mathit {BesselY}\left (2, x\right ) \\ \bullet & {} & \textrm {Make the change from}\hspace {3pt} y\hspace {3pt}\textrm {back to}\hspace {3pt} y \\ {} & {} & y=\frac {c_{1} \mathit {BesselJ}\left (2, x\right )+c_{2} \mathit {BesselY}\left (2, x\right )}{x^{2}} \end {array} \]

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`
 

Solution by Maple

Time used: 0.016 (sec). Leaf size: 44

Order:=6; 
dsolve(x*diff(y(x),x$2)+5*diff(y(x),x)+x*y(x)=0,y(x),type='series',x=0);
 

\[ y \left (x \right ) = \frac {c_{1} x^{4} \left (1-\frac {1}{12} x^{2}+\frac {1}{384} x^{4}+\operatorname {O}\left (x^{6}\right )\right )+c_{2} \left (\ln \left (x \right ) \left (9 x^{4}+\operatorname {O}\left (x^{6}\right )\right )+\left (-144-36 x^{2}+\operatorname {O}\left (x^{6}\right )\right )\right )}{x^{4}} \]

Solution by Mathematica

Time used: 0.01 (sec). Leaf size: 47

AsymptoticDSolveValue[x*y''[x]+5*y'[x]+x*y[x]==0,y[x],{x,0,5}]
 

\[ y(x)\to c_2 \left (\frac {x^4}{384}-\frac {x^2}{12}+1\right )+c_1 \left (\frac {\left (x^2+8\right )^2}{64 x^4}-\frac {\log (x)}{16}\right ) \]