Internal problem ID [1371]
Internal file name [OUTPUT/1372_Sunday_June_05_2022_02_13_40_AM_86649237/index.tex]
Book: Elementary differential equations with boundary value problems. William F. Trench.
Brooks/Cole 2001
Section: Chapter 7 Series Solutions of Linear Second Equations. 7.6 THE METHOD OF
FROBENIUS II. Exercises 7.6. Page 374
Problem number: 19.
ODE order: 2.
ODE degree: 1.
The type(s) of ODE detected by this program : "second order series method. Regular singular point. Repeated root"
Maple gives the following as the ode type
[[_2nd_order, _with_linear_symmetries]]
\[ \boxed {x^{2} y^{\prime \prime }-x \left (3-2 x \right ) y^{\prime }+\left (4+3 x \right ) y=0} \] 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. \[ x^{2} y^{\prime \prime }+\left (2 x^{2}-3 x \right ) y^{\prime }+\left (4+3 x \right ) y = 0 \] 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 {-3+2 x}{x}\\ q(x) &= \frac {4+3 x}{x^{2}}\\ \end {align*}
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 \[ x^{2} y^{\prime \prime }+\left (2 x^{2}-3 x \right ) y^{\prime }+\left (4+3 x \right ) y = 0 \] 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^{2} \left (\moverset {\infty }{\munderset {n =0}{\sum }}\left (n +r \right ) \left (n +r -1\right ) a_{n} x^{n +r -2}\right )+\left (2 x^{2}-3 x \right ) \left (\moverset {\infty }{\munderset {n =0}{\sum }}\left (n +r \right ) a_{n} x^{n +r -1}\right )+\left (4+3 x \right ) \left (\moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n +r}\right ) = 0 \end{equation} Which simplifies to \begin{equation} \tag{2A} \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{n +r} a_{n} \left (n +r \right ) \left (n +r -1\right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}2 x^{1+n +r} a_{n} \left (n +r \right )\right )+\moverset {\infty }{\munderset {n =0}{\sum }}\left (-3 x^{n +r} a_{n} \left (n +r \right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}4 a_{n} x^{n +r}\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}3 x^{1+n +r} a_{n}\right ) = 0 \end{equation} The next step is to make all powers of \(x\) be \(n +r\) in each summation term. Going over each summation term above with power of \(x\) in it which is not already \(x^{n +r}\) and adjusting the power and the corresponding index gives \begin{align*} \moverset {\infty }{\munderset {n =0}{\sum }}2 x^{1+n +r} a_{n} \left (n +r \right ) &= \moverset {\infty }{\munderset {n =1}{\sum }}2 a_{n -1} \left (n +r -1\right ) x^{n +r} \\ \moverset {\infty }{\munderset {n =0}{\sum }}3 x^{1+n +r} a_{n} &= \moverset {\infty }{\munderset {n =1}{\sum }}3 a_{n -1} x^{n +r} \\ \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 \(n +r\). \begin{equation} \tag{2B} \left (\moverset {\infty }{\munderset {n =0}{\sum }}x^{n +r} a_{n} \left (n +r \right ) \left (n +r -1\right )\right )+\left (\moverset {\infty }{\munderset {n =1}{\sum }}2 a_{n -1} \left (n +r -1\right ) x^{n +r}\right )+\moverset {\infty }{\munderset {n =0}{\sum }}\left (-3 x^{n +r} a_{n} \left (n +r \right )\right )+\left (\moverset {\infty }{\munderset {n =0}{\sum }}4 a_{n} x^{n +r}\right )+\left (\moverset {\infty }{\munderset {n =1}{\sum }}3 a_{n -1} x^{n +r}\right ) = 0 \end{equation} The indicial equation is obtained from \(n = 0\). From Eq (2B) this gives \[ x^{n +r} a_{n} \left (n +r \right ) \left (n +r -1\right )-3 x^{n +r} a_{n} \left (n +r \right )+4 a_{n} x^{n +r} = 0 \] When \(n = 0\) the above becomes \[ x^{r} a_{0} r \left (-1+r \right )-3 x^{r} a_{0} r +4 a_{0} x^{r} = 0 \] Or \[ \left (x^{r} r \left (-1+r \right )-3 x^{r} r +4 x^{r}\right ) a_{0} = 0 \] Since \(a_{0}\neq 0\) then the above simplifies to \[ \left (r -2\right )^{2} x^{r} = 0 \] Since the above is true for all \(x\) then the indicial equation becomes \[ \left (r -2\right )^{2} = 0 \] Solving for \(r\) gives the roots of the indicial equation as \begin {align*} r_1 &= 2\\ r_2 &= 2 \end {align*}
Since \(a_{0}\neq 0\) then the indicial equation becomes \[ \left (r -2\right )^{2} x^{r} = 0 \] Solving for \(r\) gives the roots of the indicial equation as \([2, 2]\).
Since the root of the indicial equation is repeated, then we can construct two linearly independent solutions. The first solution has the form \begin {align*} y_{1}\left (x \right ) &= \moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n +r}\tag {1A} \end {align*}
Now the second solution \(y_{2}\) is found using \begin {align*} y_{2}\left (x \right ) &= y_{1}\left (x \right ) \ln \left (x \right )+\left (\moverset {\infty }{\munderset {n =1}{\sum }}b_{n} x^{n +r}\right )\tag {1B} \end {align*}
Then the general solution will be \[ y = c_{1} y_{1}\left (x \right )+c_{2} y_{2}\left (x \right ) \] In Eq (1B) the sum starts from 1 and not zero. In Eq (1A), \(a_{0}\) is never zero, and is arbitrary and is typically taken as \(a_{0} = 1\), and \(\{c_{1}, c_{2}\}\) are two arbitray constants of integration which can be found from initial conditions. Using the value of the indicial root found earlier, \(r = 2\), Eqs (1A,1B) become \begin {align*} y_{1}\left (x \right ) &= \moverset {\infty }{\munderset {n =0}{\sum }}a_{n} x^{n +2}\\ y_{2}\left (x \right ) &= y_{1}\left (x \right ) \ln \left (x \right )+\left (\moverset {\infty }{\munderset {n =1}{\sum }}b_{n} x^{n +2}\right ) \end {align*}
We start by finding the first solution \(y_{1}\left (x \right )\). 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 \(a_{0} = 1\). For \(1\le n\) the recursive equation is \begin{equation} \tag{3} a_{n} \left (n +r \right ) \left (n +r -1\right )+2 a_{n -1} \left (n +r -1\right )-3 a_{n} \left (n +r \right )+4 a_{n}+3 a_{n -1} = 0 \end{equation} Solving for \(a_{n}\) from recursive equation (4) gives \[ a_{n} = -\frac {a_{n -1} \left (2 n +2 r +1\right )}{n^{2}+2 n r +r^{2}-4 n -4 r +4}\tag {4} \] Which for the root \(r = 2\) becomes \[ a_{n} = \frac {a_{n -1} \left (-5-2 n \right )}{n^{2}}\tag {5} \] At this point, it is a good idea to keep track of \(a_{n}\) in a table both before substituting \(r = 2\) and after as more terms are found using the above recursive equation.
| \(n\) | \(a_{n ,r}\) | \(a_{n}\) |
| \(a_{0}\) | \(1\) | \(1\) |
For \(n = 1\), using the above recursive equation gives \[ a_{1}=\frac {-3-2 r}{\left (-1+r \right )^{2}} \] Which for the root \(r = 2\) becomes \[ a_{1}=-7 \] And the table now becomes
| \(n\) | \(a_{n ,r}\) | \(a_{n}\) |
| \(a_{0}\) | \(1\) | \(1\) |
| \(a_{1}\) | \(\frac {-3-2 r}{\left (-1+r \right )^{2}}\) | \(-7\) |
For \(n = 2\), using the above recursive equation gives \[ a_{2}=\frac {4 r^{2}+16 r +15}{\left (-1+r \right )^{2} r^{2}} \] Which for the root \(r = 2\) becomes \[ a_{2}={\frac {63}{4}} \] And the table now becomes
| \(n\) | \(a_{n ,r}\) | \(a_{n}\) |
| \(a_{0}\) | \(1\) | \(1\) |
| \(a_{1}\) | \(\frac {-3-2 r}{\left (-1+r \right )^{2}}\) | \(-7\) |
| \(a_{2}\) | \(\frac {4 r^{2}+16 r +15}{\left (-1+r \right )^{2} r^{2}}\) | \(\frac {63}{4}\) |
For \(n = 3\), using the above recursive equation gives \[ a_{3}=\frac {-8 r^{3}-60 r^{2}-142 r -105}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2}} \] Which for the root \(r = 2\) becomes \[ a_{3}=-{\frac {77}{4}} \] And the table now becomes
| \(n\) | \(a_{n ,r}\) | \(a_{n}\) |
| \(a_{0}\) | \(1\) | \(1\) |
| \(a_{1}\) | \(\frac {-3-2 r}{\left (-1+r \right )^{2}}\) | \(-7\) |
| \(a_{2}\) | \(\frac {4 r^{2}+16 r +15}{\left (-1+r \right )^{2} r^{2}}\) | \(\frac {63}{4}\) |
| \(a_{3}\) | \(\frac {-8 r^{3}-60 r^{2}-142 r -105}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2}}\) | \(-{\frac {77}{4}}\) |
For \(n = 4\), using the above recursive equation gives \[ a_{4}=\frac {16 r^{4}+192 r^{3}+824 r^{2}+1488 r +945}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2} \left (r +2\right )^{2}} \] Which for the root \(r = 2\) becomes \[ a_{4}={\frac {1001}{64}} \] And the table now becomes
| \(n\) | \(a_{n ,r}\) | \(a_{n}\) |
| \(a_{0}\) | \(1\) | \(1\) |
| \(a_{1}\) | \(\frac {-3-2 r}{\left (-1+r \right )^{2}}\) | \(-7\) |
| \(a_{2}\) | \(\frac {4 r^{2}+16 r +15}{\left (-1+r \right )^{2} r^{2}}\) | \(\frac {63}{4}\) |
| \(a_{3}\) | \(\frac {-8 r^{3}-60 r^{2}-142 r -105}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2}}\) | \(-{\frac {77}{4}}\) |
| \(a_{4}\) | \(\frac {16 r^{4}+192 r^{3}+824 r^{2}+1488 r +945}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2} \left (r +2\right )^{2}}\) | \(\frac {1001}{64}\) |
For \(n = 5\), using the above recursive equation gives \[ a_{5}=\frac {-32 r^{5}-560 r^{4}-3760 r^{3}-12040 r^{2}-18258 r -10395}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2} \left (r +2\right )^{2} \left (r +3\right )^{2}} \] Which for the root \(r = 2\) becomes \[ a_{5}=-{\frac {3003}{320}} \] And the table now becomes
| \(n\) | \(a_{n ,r}\) | \(a_{n}\) |
| \(a_{0}\) | \(1\) | \(1\) |
| \(a_{1}\) | \(\frac {-3-2 r}{\left (-1+r \right )^{2}}\) | \(-7\) |
| \(a_{2}\) | \(\frac {4 r^{2}+16 r +15}{\left (-1+r \right )^{2} r^{2}}\) | \(\frac {63}{4}\) |
| \(a_{3}\) | \(\frac {-8 r^{3}-60 r^{2}-142 r -105}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2}}\) | \(-{\frac {77}{4}}\) |
| \(a_{4}\) | \(\frac {16 r^{4}+192 r^{3}+824 r^{2}+1488 r +945}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2} \left (r +2\right )^{2}}\) | \(\frac {1001}{64}\) |
| \(a_{5}\) | \(\frac {-32 r^{5}-560 r^{4}-3760 r^{3}-12040 r^{2}-18258 r -10395}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2} \left (r +2\right )^{2} \left (r +3\right )^{2}}\) | \(-{\frac {3003}{320}}\) |
Using the above table, then the first solution \(y_{1}\left (x \right )\) is \begin{align*} y_{1}\left (x \right )&= x^{2} \left (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 \right ) \\ &= x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right ) \\ \end{align*} Now the second solution is found. The second solution is given by \[ y_{2}\left (x \right ) = y_{1}\left (x \right ) \ln \left (x \right )+\left (\moverset {\infty }{\munderset {n =1}{\sum }}b_{n} x^{n +r}\right ) \] Where \(b_{n}\) is found using \[ b_{n} = \frac {d}{d r}a_{n ,r} \] And the above is then evaluated at \(r = 2\). The above table for \(a_{n ,r}\) is used for this purpose. Computing the derivatives gives the following table
| \(n\) | \(b_{n ,r}\) | \(a_{n}\) | \(b_{n ,r} = \frac {d}{d r}a_{n ,r}\) | \(b_{n}\left (r =2\right )\) |
| \(b_{0}\) | \(1\) | \(1\) | N/A since \(b_{n}\) starts from 1 | N/A |
| \(b_{1}\) | \(\frac {-3-2 r}{\left (-1+r \right )^{2}}\) | \(-7\) | \(\frac {8+2 r}{\left (-1+r \right )^{3}}\) | \(12\) |
| \(b_{2}\) | \(\frac {4 r^{2}+16 r +15}{\left (-1+r \right )^{2} r^{2}}\) | \(\frac {63}{4}\) | \(\frac {-8 r^{3}-48 r^{2}-44 r +30}{\left (-1+r \right )^{3} r^{3}}\) | \(-{\frac {157}{4}}\) |
| \(b_{3}\) | \(\frac {-8 r^{3}-60 r^{2}-142 r -105}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2}}\) | \(-{\frac {77}{4}}\) | \(\frac {24 r^{5}+240 r^{4}+718 r^{3}+630 r^{2}-142 r -210}{\left (-1+r \right )^{3} r^{3} \left (1+r \right )^{3}}\) | \(\frac {2063}{36}\) |
| \(b_{4}\) | \(\frac {16 r^{4}+192 r^{3}+824 r^{2}+1488 r +945}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2} \left (r +2\right )^{2}}\) | \(\frac {1001}{64}\) | \(\frac {-64 r^{7}-1024 r^{6}-6096 r^{5}-16880 r^{4}-21176 r^{3}-6876 r^{2}+6756 r +3780}{\left (-1+r \right )^{3} r^{3} \left (1+r \right )^{3} \left (r +2\right )^{3}}\) | \(-{\frac {59875}{1152}}\) |
| \(b_{5}\) | \(\frac {-32 r^{5}-560 r^{4}-3760 r^{3}-12040 r^{2}-18258 r -10395}{\left (-1+r \right )^{2} r^{2} \left (1+r \right )^{2} \left (r +2\right )^{2} \left (r +3\right )^{2}}\) | \(-{\frac {3003}{320}}\) | \(\frac {160 r^{9}+3840 r^{8}+37680 r^{7}+196080 r^{6}+582498 r^{5}+971700 r^{4}+774410 r^{3}+37980 r^{2}-317448 r -124740}{\left (-1+r \right )^{3} r^{3} \left (1+r \right )^{3} \left (r +2\right )^{3} \left (r +3\right )^{3}}\) | \(\frac {323399}{9600}\) |
The above table gives all values of \(b_{n}\) needed. Hence the second solution is \begin{align*} y_{2}\left (x \right )&=y_{1}\left (x \right ) \ln \left (x \right )+b_{0}+b_{1} x +b_{2} x^{2}+b_{3} x^{3}+b_{4} x^{4}+b_{5} x^{5}+b_{6} x^{6}\dots \\ &= x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right ) \ln \left (x \right )+x^{2} \left (12 x -\frac {157 x^{2}}{4}+\frac {2063 x^{3}}{36}-\frac {59875 x^{4}}{1152}+\frac {323399 x^{5}}{9600}+O\left (x^{6}\right )\right ) \\ \end{align*} 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} x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right ) + c_{2} \left (x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right ) \ln \left (x \right )+x^{2} \left (12 x -\frac {157 x^{2}}{4}+\frac {2063 x^{3}}{36}-\frac {59875 x^{4}}{1152}+\frac {323399 x^{5}}{9600}+O\left (x^{6}\right )\right )\right ) \\ \end{align*} Hence the final solution is \begin{align*} y &= y_h \\ &= c_{1} x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right )+c_{2} \left (x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right ) \ln \left (x \right )+x^{2} \left (12 x -\frac {157 x^{2}}{4}+\frac {2063 x^{3}}{36}-\frac {59875 x^{4}}{1152}+\frac {323399 x^{5}}{9600}+O\left (x^{6}\right )\right )\right ) \\ \end{align*}
The solution(s) found are the following \begin{align*} \tag{1} y &= c_{1} x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right )+c_{2} \left (x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right ) \ln \left (x \right )+x^{2} \left (12 x -\frac {157 x^{2}}{4}+\frac {2063 x^{3}}{36}-\frac {59875 x^{4}}{1152}+\frac {323399 x^{5}}{9600}+O\left (x^{6}\right )\right )\right ) \\ \end{align*}
Verification of solutions
\[ y = c_{1} x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right )+c_{2} \left (x^{2} \left (1-7 x +\frac {63 x^{2}}{4}-\frac {77 x^{3}}{4}+\frac {1001 x^{4}}{64}-\frac {3003 x^{5}}{320}+O\left (x^{6}\right )\right ) \ln \left (x \right )+x^{2} \left (12 x -\frac {157 x^{2}}{4}+\frac {2063 x^{3}}{36}-\frac {59875 x^{4}}{1152}+\frac {323399 x^{5}}{9600}+O\left (x^{6}\right )\right )\right ) \] Verified OK.
\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & x^{2} \left (\frac {d}{d x}y^{\prime }\right )+\left (2 x^{2}-3 x \right ) y^{\prime }+\left (4+3 x \right ) y=0 \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 2 \\ {} & {} & \frac {d}{d x}y^{\prime } \\ \bullet & {} & \textrm {Isolate 2nd derivative}\hspace {3pt} \\ {} & {} & \frac {d}{d x}y^{\prime }=-\frac {\left (4+3 x \right ) y}{x^{2}}-\frac {\left (-3+2 x \right ) y^{\prime }}{x} \\ \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} \\ {} & {} & \frac {d}{d x}y^{\prime }+\frac {\left (-3+2 x \right ) y^{\prime }}{x}+\frac {\left (4+3 x \right ) y}{x^{2}}=0 \\ \square & {} & \textrm {Check to see if}\hspace {3pt} x_{0}=0\hspace {3pt}\textrm {is a regular singular point}\hspace {3pt} \\ {} & \circ & \textrm {Define functions}\hspace {3pt} \\ {} & {} & \left [P_{2}\left (x \right )=\frac {-3+2 x}{x}, P_{3}\left (x \right )=\frac {4+3 x}{x^{2}}\right ] \\ {} & \circ & x \cdot P_{2}\left (x \right )\textrm {is analytic at}\hspace {3pt} x =0 \\ {} & {} & \left (x \cdot P_{2}\left (x \right )\right )\bigg | {\mstack {}{_{x \hiderel {=}0}}}=-3 \\ {} & \circ & x^{2}\cdot P_{3}\left (x \right )\textrm {is analytic at}\hspace {3pt} x =0 \\ {} & {} & \left (x^{2}\cdot P_{3}\left (x \right )\right )\bigg | {\mstack {}{_{x \hiderel {=}0}}}=4 \\ {} & \circ & x =0\textrm {is a regular singular point}\hspace {3pt} \\ & {} & \textrm {Check to see if}\hspace {3pt} x_{0}=0\hspace {3pt}\textrm {is a regular singular point}\hspace {3pt} \\ {} & {} & x_{0}=0 \\ \bullet & {} & \textrm {Multiply by denominators}\hspace {3pt} \\ {} & {} & x^{2} \left (\frac {d}{d x}y^{\prime }\right )+x \left (-3+2 x \right ) y^{\prime }+\left (4+3 x \right ) y=0 \\ \bullet & {} & \textrm {Assume series solution for}\hspace {3pt} y \\ {} & {} & y=\moverset {\infty }{\munderset {k =0}{\sum }}a_{k} x^{k +r} \\ \square & {} & \textrm {Rewrite ODE with series expansions}\hspace {3pt} \\ {} & \circ & \textrm {Convert}\hspace {3pt} x^{m}\cdot y\hspace {3pt}\textrm {to series expansion for}\hspace {3pt} m =0..1 \\ {} & {} & x^{m}\cdot y=\moverset {\infty }{\munderset {k =0}{\sum }}a_{k} x^{k +r +m} \\ {} & \circ & \textrm {Shift index using}\hspace {3pt} k \mathrm {->}k -m \\ {} & {} & x^{m}\cdot y=\moverset {\infty }{\munderset {k =m}{\sum }}a_{k -m} x^{k +r} \\ {} & \circ & \textrm {Convert}\hspace {3pt} x^{m}\cdot y^{\prime }\hspace {3pt}\textrm {to series expansion for}\hspace {3pt} m =1..2 \\ {} & {} & x^{m}\cdot y^{\prime }=\moverset {\infty }{\munderset {k =0}{\sum }}a_{k} \left (k +r \right ) x^{k +r -1+m} \\ {} & \circ & \textrm {Shift index using}\hspace {3pt} k \mathrm {->}k +1-m \\ {} & {} & x^{m}\cdot y^{\prime }=\moverset {\infty }{\munderset {k =-1+m}{\sum }}a_{k +1-m} \left (k +1-m +r \right ) x^{k +r} \\ {} & \circ & \textrm {Convert}\hspace {3pt} x^{2}\cdot \left (\frac {d}{d x}y^{\prime }\right )\hspace {3pt}\textrm {to series expansion}\hspace {3pt} \\ {} & {} & x^{2}\cdot \left (\frac {d}{d x}y^{\prime }\right )=\moverset {\infty }{\munderset {k =0}{\sum }}a_{k} \left (k +r \right ) \left (k +r -1\right ) x^{k +r} \\ & {} & \textrm {Rewrite ODE with series expansions}\hspace {3pt} \\ {} & {} & a_{0} \left (-2+r \right )^{2} x^{r}+\left (\moverset {\infty }{\munderset {k =1}{\sum }}\left (a_{k} \left (k +r -2\right )^{2}+a_{k -1} \left (2 k +1+2 r \right )\right ) x^{k +r}\right )=0 \\ \bullet & {} & a_{0}\textrm {cannot be 0 by assumption, giving the indicial equation}\hspace {3pt} \\ {} & {} & \left (-2+r \right )^{2}=0 \\ \bullet & {} & \textrm {Values of r that satisfy the indicial equation}\hspace {3pt} \\ {} & {} & r =2 \\ \bullet & {} & \textrm {Each term in the series must be 0, giving the recursion relation}\hspace {3pt} \\ {} & {} & a_{k} \left (k +r -2\right )^{2}+a_{k -1} \left (2 k +1+2 r \right )=0 \\ \bullet & {} & \textrm {Shift index using}\hspace {3pt} k \mathrm {->}k +1 \\ {} & {} & a_{k +1} \left (k +r -1\right )^{2}+a_{k} \left (2 k +2 r +3\right )=0 \\ \bullet & {} & \textrm {Recursion relation that defines series solution to ODE}\hspace {3pt} \\ {} & {} & a_{k +1}=-\frac {a_{k} \left (2 k +2 r +3\right )}{\left (k +r -1\right )^{2}} \\ \bullet & {} & \textrm {Recursion relation for}\hspace {3pt} r =2 \\ {} & {} & a_{k +1}=-\frac {a_{k} \left (2 k +7\right )}{\left (k +1\right )^{2}} \\ \bullet & {} & \textrm {Solution for}\hspace {3pt} r =2 \\ {} & {} & \left [y=\moverset {\infty }{\munderset {k =0}{\sum }}a_{k} x^{k +2}, a_{k +1}=-\frac {a_{k} \left (2 k +7\right )}{\left (k +1\right )^{2}}\right ] \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 -> elliptic -> Legendre <- Kummer successful <- special function solution successful`
✓ Solution by Maple
Time used: 0.016 (sec). Leaf size: 69
Order:=6; dsolve(x^2*diff(y(x),x$2)-x*(3-2*x)*diff(y(x),x)+(4+3*x)*y(x)=0,y(x),type='series',x=0);
\[ y \left (x \right ) = \left (\left (c_{2} \ln \left (x \right )+c_{1} \right ) \left (1-7 x +\frac {63}{4} x^{2}-\frac {77}{4} x^{3}+\frac {1001}{64} x^{4}-\frac {3003}{320} x^{5}+\operatorname {O}\left (x^{6}\right )\right )+\left (12 x -\frac {157}{4} x^{2}+\frac {2063}{36} x^{3}-\frac {59875}{1152} x^{4}+\frac {323399}{9600} x^{5}+\operatorname {O}\left (x^{6}\right )\right ) c_{2} \right ) x^{2} \]
✓ Solution by Mathematica
Time used: 0.004 (sec). Leaf size: 122
AsymptoticDSolveValue[x^2*y''[x]-x*(3-2*x)*y'[x]+(4+3*x)*y[x]==0,y[x],{x,0,5}]
\[ y(x)\to c_1 \left (-\frac {3003 x^5}{320}+\frac {1001 x^4}{64}-\frac {77 x^3}{4}+\frac {63 x^2}{4}-7 x+1\right ) x^2+c_2 \left (\left (\frac {323399 x^5}{9600}-\frac {59875 x^4}{1152}+\frac {2063 x^3}{36}-\frac {157 x^2}{4}+12 x\right ) x^2+\left (-\frac {3003 x^5}{320}+\frac {1001 x^4}{64}-\frac {77 x^3}{4}+\frac {63 x^2}{4}-7 x+1\right ) x^2 \log (x)\right ) \]