Internal problem ID [14750]
Internal file name [OUTPUT/14430_Monday_April_08_2024_06_24_44_AM_83276714/index.tex
]
Book: INTRODUCTORY DIFFERENTIAL EQUATIONS. Martha L. Abell, James P. Braselton.
Fourth edition 2014. ElScAe. 2014
Section: Chapter 4. Higher Order Equations. Exercises 4.7, page 195
Problem number: 42.
ODE order: 2.
ODE degree: 1.
The type(s) of ODE detected by this program : "kovacic", "second_order_euler_ode", "second_order_change_of_variable_on_x_method_1", "second_order_change_of_variable_on_x_method_2", "second_order_change_of_variable_on_y_method_2"
Maple gives the following as the ode type
[[_2nd_order, _with_linear_symmetries]]
\[ \boxed {9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y=\frac {1}{x}} \] With initial conditions \begin {align*} [y \left (1\right ) = 0, y^{\prime }\left (1\right ) = -1] \end {align*}
This is a linear ODE. In canonical form it is written as \begin {align*} y^{\prime \prime } + p(x)y^{\prime } + q(x) y &= F \end {align*}
Where here \begin {align*} p(x) &=\frac {3}{x}\\ q(x) &=\frac {10}{9 x^{2}}\\ F &=\frac {1}{9 x^{3}} \end {align*}
Hence the ode is \begin {align*} y^{\prime \prime }+\frac {3 y^{\prime }}{x}+\frac {10 y}{9 x^{2}} = \frac {1}{9 x^{3}} \end {align*}
The domain of \(p(x)=\frac {3}{x}\) is \[
\{x <0\boldsymbol {\lor }0
This is second order non-homogeneous ODE. In standard form the ODE is \[ A y''(x) + B y'(x) + C y(x) = f(x) \] Where \(A=9 x^{2}, B=27 x, C=10, f(x)=\frac {1}{x}\). Let the
solution be \[ y = y_h + y_p \] Where \(y_h\) is the solution to the homogeneous ODE \( A y''(x) + B y'(x) + C y(x) = 0\), and \(y_p\) is a particular solution
to the non-homogeneous ODE \(A y''(x) + B y'(x) + C y(x) = f(x)\). Solving for \(y_h\) from \[ 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = 0 \] This is Euler second order ODE. Let the
solution be \(y = x^r\), then \(y'=r x^{r-1}\) and \(y''=r(r-1) x^{r-2}\). Substituting these back into the given ODE gives \[ 9 x^{2}(r(r-1))x^{r-2}+27 x r x^{r-1}+10 x^{r} = 0 \] Simplifying gives \[ 9 r \left (r -1\right )x^{r}+27 r\,x^{r}+10 x^{r} = 0 \]
Since \(x^{r}\neq 0\) then dividing throughout by \(x^{r}\) gives \[ 9 r \left (r -1\right )+27 r+10 = 0 \] Or \[ 9 r^{2}+18 r +10 = 0 \tag {1} \] Equation (1) is the characteristic equation. Its
roots determine the form of the general solution. Using the quadratic equation the roots are
\begin {align*} r_1 &= -1-\frac {i}{3}\\ r_2 &= -1+\frac {i}{3} \end {align*}
The roots are complex conjugate of each others. Let the roots be \begin {align*} r_1 &= \alpha + i \beta \\ r_2 &= \alpha - i \beta \\ \end {align*}
Where in this case \(\alpha =-1\) and \(\beta =-{\frac {1}{3}}\). Hence the solution becomes \begin {align*} y &= c_{1} x^{r_1} + c_{2} x^{r_2} \\ &= c_{1} x^{\alpha + i \beta } + c_{2} x^{\alpha - i \beta } \\ &= x^{\alpha } \left ( c_{1} x^{i \beta } + c_{2} x^{- i \beta }\right ) \\ &= x^{\alpha } \left ( c_{1} e^{\ln \left (x^{i \beta }\right )} + c_{2} e^{\ln \left (x^{-i \beta }\right )}\right ) \\ &= x^{\alpha } \left ( c_{1} e^{i \left (\beta \ln {x}\right )} + c_{2} e^{-i \left (\beta \ln {x}\right )}\right ) \end {align*}
Using the values for \(\alpha =-1, \beta =-{\frac {1}{3}}\), the above becomes \begin {align*} y&= x^{-1} \left ( c_{1} e^{-\frac {i \ln \left (x \right )}{3}} + c_{2} e^{\frac {i \ln \left (x \right )}{3}} \right ) \end {align*}
Using Euler relation, the expression \(c_{1} e^{i A}+ c_{2} e^{-i A}\) is transformed to \( c_{1} \cos A+ c_{1} \sin A\) where the constants are free to
change. Applying this to the above result gives \begin {align*} y&=\frac {1}{x}\left (c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )\right ) \end {align*}
Next, we find the particular solution to the ODE \[ 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = \frac {1}{x} \] The particular solution \(y_p\) can be found
using either the method of undetermined coefficients, or the method of variation of
parameters. The method of variation of parameters will be used as it is more general and can
be used when the coefficients of the ODE depend on \(x\) as well. Let \begin{equation}
\tag{1} y_p(x) = u_1 y_1 + u_2 y_2
\end{equation} Where \(u_1,u_2\) to be determined,
and \(y_1,y_2\) are the two basis solutions (the two linearly independent solutions of the homogeneous
ODE) found earlier when solving the homogeneous ODE as \begin{align*}
y_1 &= \frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x} \\
y_2 &= -\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \\
\end{align*} In the Variation of parameters \(u_1,u_2\)
are found using \begin{align*}
\tag{2} u_1 &= -\int \frac {y_2 f(x)}{a W(x)} \\
\tag{3} u_2 &= \int \frac {y_1 f(x)}{a W(x)} \\
\end{align*} Where \(W(x)\) is the Wronskian and \(a\) is the coefficient in front of \(y''\) in the
given ODE. The Wronskian is given by \(W= \begin {vmatrix} y_1 & y_{2} \\ y_{1}^{\prime } & y_{2}^{\prime } \end {vmatrix} \). Hence \[ W = \begin {vmatrix} \frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x} & -\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \\ \frac {d}{dx}\left (\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x}\right ) & \frac {d}{dx}\left (-\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x}\right ) \end {vmatrix} \] Which gives \[ W = \begin {vmatrix} \frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x} & -\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \\ -\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}-\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{3 x^{2}} & \frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}-\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{3 x^{2}} \end {vmatrix} \] Therefore \[
W = \left (\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x}\right )\left (\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}-\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{3 x^{2}}\right ) - \left (-\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x}\right )\left (-\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}-\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{3 x^{2}}\right )
\] Which
simplifies to \[
W = -\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )^{2}+\sin \left (\frac {\ln \left (x \right )}{3}\right )^{2}}{3 x^{3}}
\] Which simplifies to \[
W = -\frac {1}{3 x^{3}}
\] Therefore Eq. (2) becomes \[
u_1 = -\int \frac {-\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}}{-\frac {3}{x}}\,dx
\] Which simplifies to \[
u_1 = - \int \frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )}{3 x}d x
\]
Hence \[
u_1 = \cos \left (\frac {\ln \left (x \right )}{3}\right )
\] And Eq. (3) becomes \[
u_2 = \int \frac {\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}}{-\frac {3}{x}}\,dx
\] Which simplifies to \[
u_2 = \int -\frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )}{3 x}d x
\] Hence \[
u_2 = -\sin \left (\frac {\ln \left (x \right )}{3}\right )
\] Therefore the particular
solution, from equation (1) is \[
y_p(x) = \frac {\cos \left (\frac {\ln \left (x \right )}{3}\right )^{2}}{x}+\frac {\sin \left (\frac {\ln \left (x \right )}{3}\right )^{2}}{x}
\] Which simplifies to \[
y_p(x) = \frac {1}{x}
\] Therefore the general solution is
\begin {align*} y &= y_h + y_p \\ &= \frac {1+c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \end {align*}
Initial conditions are used to solve for the constants of integration.
Looking at the above solution \begin {align*} y = \frac {1+c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \tag {1} \end {align*}
Initial conditions are now substituted in the above solution. This will generate the required
equations to solve for the integration constants. substituting \(y = 0\) and \(x = 1\) in the above gives
\begin {align*} 0 = 1+c_{1}\tag {1A} \end {align*}
Taking derivative of the solution gives \begin {align*} y^{\prime } = -\frac {1+c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}+\frac {-\frac {c_{1} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{3 x}+\frac {c_{2} \cos \left (\frac {\ln \left (x \right )}{3}\right )}{3 x}}{x} \end {align*}
substituting \(y^{\prime } = -1\) and \(x = 1\) in the above gives \begin {align*} -1 = -c_{1} +\frac {c_{2}}{3}-1\tag {2A} \end {align*}
Equations {1A,2A} are now solved for \(\{c_{1}, c_{2}\}\). Solving for the constants gives \begin {align*} c_{1}&=-1\\ c_{2}&=-3 \end {align*}
Substituting these values back in above solution results in \begin {align*} y = \frac {1-\cos \left (\frac {\ln \left (x \right )}{3}\right )-3 \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \end {align*}
Summary
The solution(s) found are the following \begin{align*}
\tag{1} y &= \frac {1-\cos \left (\frac {\ln \left (x \right )}{3}\right )-3 \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \\
\end{align*} Verification of solutions
\[
y = \frac {1-\cos \left (\frac {\ln \left (x \right )}{3}\right )-3 \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x}
\] Verified OK. This is second order non-homogeneous ODE. Let the solution be \[
y = y_h + y_p
\] Where \(y_h\) is the solution to
the homogeneous ODE \( A y''(x) + B y'(x) + C y(x) = 0\), and \(y_p\) is a particular solution to the non-homogeneous ODE \(A y''(x) + B y'(x) + C y(x) = f(x)\). \(y_h\) is the
solution to \[
9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = 0
\] In normal form the ode \begin {align*} 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y&=0 \tag {1} \end {align*}
Becomes \begin {align*} y^{\prime \prime }+p \left (x \right ) y^{\prime }+q \left (x \right ) y&=0 \tag {2} \end {align*}
Where \begin {align*} p \left (x \right )&=\frac {3}{x}\\ q \left (x \right )&=\frac {10}{9 x^{2}} \end {align*}
Applying change of variables \(\tau = g \left (x \right )\) to (2) gives \begin {align*} \frac {d^{2}}{d \tau ^{2}}y \left (\tau \right )+p_{1} \left (\frac {d}{d \tau }y \left (\tau \right )\right )+q_{1} y \left (\tau \right )&=0 \tag {3} \end {align*}
Where \(\tau \) is the new independent variable, and \begin {align*} p_{1} \left (\tau \right ) &=\frac {\tau ^{\prime \prime }\left (x \right )+p \left (x \right ) \tau ^{\prime }\left (x \right )}{{\tau ^{\prime }\left (x \right )}^{2}}\tag {4} \\ q_{1} \left (\tau \right ) &=\frac {q \left (x \right )}{{\tau ^{\prime }\left (x \right )}^{2}}\tag {5} \end {align*}
Let \(p_{1} = 0\). Eq (4) simplifies to \begin {align*} \tau ^{\prime \prime }\left (x \right )+p \left (x \right ) \tau ^{\prime }\left (x \right )&=0 \end {align*}
This ode is solved resulting in \begin {align*} \tau &= \int {\mathrm e}^{-\left (\int p \left (x \right )d x \right )}d x\\ &= \int {\mathrm e}^{-\left (\int \frac {3}{x}d x \right )}d x\\ &= \int e^{-3 \ln \left (x \right )} \,dx\\ &= \int \frac {1}{x^{3}}d x\\ &= -\frac {1}{2 x^{2}}\tag {6} \end {align*}
Using (6) to evaluate \(q_{1}\) from (5) gives \begin {align*} q_{1} \left (\tau \right ) &= \frac {q \left (x \right )}{{\tau ^{\prime }\left (x \right )}^{2}}\\ &= \frac {\frac {10}{9 x^{2}}}{\frac {1}{x^{6}}}\\ &= \frac {10 x^{4}}{9}\tag {7} \end {align*}
Substituting the above in (3) and noting that now \(p_{1} = 0\) results in \begin {align*} \frac {d^{2}}{d \tau ^{2}}y \left (\tau \right )+q_{1} y \left (\tau \right )&=0 \\ \frac {d^{2}}{d \tau ^{2}}y \left (\tau \right )+\frac {10 x^{4} y \left (\tau \right )}{9}&=0 \\ \end {align*}
But in terms of \(\tau \) \begin {align*} \frac {10 x^{4}}{9}&=\frac {5}{18 \tau ^{2}} \end {align*}
Hence the above ode becomes \begin {align*} \frac {d^{2}}{d \tau ^{2}}y \left (\tau \right )+\frac {5 y \left (\tau \right )}{18 \tau ^{2}}&=0 \end {align*}
The above ode is now solved for \(y \left (\tau \right )\). The ode can be written as \[ 18 \left (\frac {d^{2}}{d \tau ^{2}}y \left (\tau \right )\right ) \tau ^{2}+5 y \left (\tau \right ) = 0 \] Which shows it is a
Euler ODE. This is Euler second order ODE. Let the solution be \(y \left (\tau \right ) = \tau ^r\), then \(y'=r \tau ^{r-1}\) and \(y''=r(r-1) \tau ^{r-2}\).
Substituting these back into the given ODE gives \[ 18 \tau ^{2}(r(r-1))\tau ^{r-2}+0 r \tau ^{r-1}+5 \tau ^{r} = 0 \] Simplifying gives \[ 18 r \left (r -1\right )\tau ^{r}+0\,\tau ^{r}+5 \tau ^{r} = 0 \] Since \(\tau ^{r}\neq 0\) then dividing
throughout by \(\tau ^{r}\) gives \[ 18 r \left (r -1\right )+0+5 = 0 \] Or \[ 18 r^{2}-18 r +5 = 0 \tag {1} \] Equation (1) is the characteristic equation. Its roots
determine the form of the general solution. Using the quadratic equation the roots are
\begin {align*} r_1 &= \frac {1}{2}-\frac {i}{6}\\ r_2 &= \frac {1}{2}+\frac {i}{6} \end {align*}
The roots are complex conjugate of each others. Let the roots be \begin {align*} r_1 &= \alpha + i \beta \\ r_2 &= \alpha - i \beta \\ \end {align*}
Where in this case \(\alpha ={\frac {1}{2}}\) and \(\beta =-{\frac {1}{6}}\). Hence the solution becomes \begin {align*} y \left (\tau \right ) &= c_{1} \tau ^{r_1} + c_{2} \tau ^{r_2} \\ &= c_{1} \tau ^{\alpha + i \beta } + c_{2} \tau ^{\alpha - i \beta } \\ &= \tau ^{\alpha } \left ( c_{1} \tau ^{i \beta } + c_{2} \tau ^{- i \beta }\right ) \\ &= \tau ^{\alpha } \left ( c_{1} e^{\ln \left (\tau ^{i \beta }\right )} + c_{2} e^{\ln \left (\tau ^{-i \beta }\right )}\right ) \\ &= \tau ^{\alpha } \left ( c_{1} e^{i \left (\beta \ln {\tau }\right )} + c_{2} e^{-i \left (\beta \ln {\tau }\right )}\right ) \end {align*}
Using the values for \(\alpha ={\frac {1}{2}}, \beta =-{\frac {1}{6}}\), the above becomes \begin {align*} y \left (\tau \right )&= \tau ^{{\frac {1}{2}}} \left ( c_{1} e^{-\frac {i \ln \left (\tau \right )}{6}} + c_{2} e^{\frac {i \ln \left (\tau \right )}{6}} \right ) \end {align*}
Using Euler relation, the expression \(c_{1} e^{i A}+ c_{2} e^{-i A}\) is transformed to \( c_{1} \cos A+ c_{1} \sin A\) where the constants are free to
change. Applying this to the above result gives \begin {align*} y \left (\tau \right )&=\sqrt {\tau }\left (c_{1} \cos \left (\frac {\ln \left (\tau \right )}{6}\right )+c_{2} \sin \left (\frac {\ln \left (\tau \right )}{6}\right )\right ) \end {align*}
The above solution is now transformed back to \(y\) using (6) which results in \begin {align*} y &= \frac {\left (c_{1} \cos \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+c_{2} \sin \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}}{2} \end {align*}
Therefore the homogeneous solution \(y_h\) is \[
y_h = \frac {\left (c_{1} \cos \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+c_{2} \sin \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}}{2}
\] The particular solution \(y_p\) can be found using either
the method of undetermined coefficients, or the method of variation of parameters. The
method of variation of parameters will be used as it is more general and can be used when
the coefficients of the ODE depend on \(x\) as well. Let \begin{equation}
\tag{1} y_p(x) = u_1 y_1 + u_2 y_2
\end{equation} Where \(u_1,u_2\) to be determined, and \(y_1,y_2\) are the
two basis solutions (the two linearly independent solutions of the homogeneous
ODE) found earlier when solving the homogeneous ODE as \begin{align*}
y_1 &= \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2} \\
y_2 &= \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2} \\
\end{align*} In the Variation of
parameters \(u_1,u_2\) are found using \begin{align*}
\tag{2} u_1 &= -\int \frac {y_2 f(x)}{a W(x)} \\
\tag{3} u_2 &= \int \frac {y_1 f(x)}{a W(x)} \\
\end{align*} Where \(W(x)\) is the Wronskian and \(a\) is the coefficient in
front of \(y''\) in the given ODE. The Wronskian is given by \(W= \begin {vmatrix} y_1 & y_{2} \\ y_{1}^{\prime } & y_{2}^{\prime } \end {vmatrix} \). Hence \[ W = \begin {vmatrix} \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2} & \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2} \\ \frac {d}{dx}\left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}\right ) & \frac {d}{dx}\left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}\right ) \end {vmatrix} \] Which gives \[ W = \begin {vmatrix} \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2} & \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2} \\ \frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}+\frac {\sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x} & \frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}-\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{6 x} \end {vmatrix} \]
Therefore \[
W = \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}\right )\left (\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}-\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{6 x}\right ) - \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}\right )\left (\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}+\frac {\sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}\right )
\] Which simplifies to \[
W = \frac {\cos \left (\frac {\ln \left (2\right )}{6}\right )^{2} {\cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2}+\cos \left (\frac {\ln \left (2\right )}{6}\right )^{2} {\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2}+{\cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2} \sin \left (\frac {\ln \left (2\right )}{6}\right )^{2}+\sin \left (\frac {\ln \left (2\right )}{6}\right )^{2} {\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2}}{6 x^{3}}
\] Which simplifies to \[
W = \frac {1}{6 x^{3}}
\] Therefore Eq. (2) becomes \[
u_1 = -\int \frac {\frac {\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}}{x}}{\frac {3}{2 x}}\,dx
\]
Which simplifies to \[
u_1 = - \int \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \left (-\sin \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right )}{3}d x
\] Hence \[
u_1 = \textit {undefined}
\] And Eq. (3) becomes \[
u_2 = \int \frac {\frac {\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}}{x}}{\frac {3}{2 x}}\,dx
\] Which simplifies to \[
u_2 = \int \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \left (\cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right )}{3}d x
\] Hence \[
u_2 = \textit {undefined}
\]
Therefore the particular solution, from equation (1) is \[
y_p(x) = \operatorname {undefined} \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}\right )+\operatorname {undefined} \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}\right )
\] Which simplifies to \[
y_p(x) = \sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined}
\] Therefore
the general solution is \begin{align*}
y &= y_h + y_p \\
&= \left (\frac {\left (c_{1} \cos \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+c_{2} \sin \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}}{2}\right ) + \left (\sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined}\right ) \\
\end{align*} Initial conditions are used to solve for the constants of
integration.
Looking at the above solution \begin {align*} y = \frac {\left (c_{1} \cos \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+c_{2} \sin \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}}{2}+\sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined} \tag {1} \end {align*}
Initial conditions are now substituted in the above solution. This will generate the required
equations to solve for the integration constants. substituting \(y = 0\) and \(x = 1\) in the above gives
\begin {align*} 0 = \operatorname {undefined} +\operatorname {undefined} i+\frac {i \sqrt {2}\, \left (\cos \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right ) c_{1} -\sin \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right ) c_{2} \right )}{2}\tag {1A} \end {align*}
Taking derivative of the solution gives \begin {align*} y^{\prime } = \frac {\left (\frac {c_{1} \sin \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{3 x}-\frac {c_{2} \cos \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{3 x}\right ) \sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}}{2}+\frac {\left (c_{1} \cos \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+c_{2} \sin \left (-\frac {\ln \left (2\right )}{6}+\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \sqrt {2}}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}+\frac {\left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined}}{\sqrt {-\frac {1}{x^{2}}}\, x^{3}}+\sqrt {-\frac {1}{x^{2}}}\, \left (\frac {2 \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{3 x}-\frac {\cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{3 x}\right ) \operatorname {undefined} +\sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined} \end {align*}
substituting \(y^{\prime } = -1\) and \(x = 1\) in the above gives \begin {align*} -1 = -\frac {i \sqrt {2}\, \left (c_{1} +\frac {c_{2}}{3}\right ) \cos \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right )}{2}-\frac {i \sqrt {2}\, \left (c_{1} -3 c_{2} \right ) \sin \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right )}{6}+\operatorname {undefined} +\operatorname {undefined} i\tag {2A} \end {align*}
Equations {1A,2A} are now solved for \(\{c_{1}, c_{2}\}\). Solving for the constants gives \begin {align*} c_{1}&=\left (\operatorname {undefined} +\operatorname {undefined} i\right ) \left (\cos \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right )+\sin \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right )\right )\\ c_{2}&=\left (\operatorname {undefined} +\operatorname {undefined} i\right ) \left (\cos \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right )+\sin \left (\frac {\ln \left (2\right )}{6}-\frac {i \pi }{6}\right )\right ) \end {align*}
Substituting these values back in above solution results in \begin {align*} y = \operatorname {undefined} i \sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{3}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} i \sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{3}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sinh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} i \sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} i \sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sinh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}-\operatorname {undefined} \sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )^{2} \sinh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}-\operatorname {undefined} \sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{6}\right )^{2} \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sqrt {-\frac {1}{x^{2}}}\, \sinh \left (\frac {\pi }{6}\right )+\operatorname {undefined} i \sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{3}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} i \sqrt {2}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} i \sqrt {2}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sinh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} i \sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{3}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sinh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} \sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{3}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} \sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{3}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} \sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} \sqrt {2}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \cosh \left (\frac {\pi }{6}\right ) \sqrt {-\frac {1}{x^{2}}}+\operatorname {undefined} \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\operatorname {undefined} \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \end {align*}
Summary
The solution(s) found are the following \begin{align*}
\tag{1} y &= \operatorname {undefined} \left (\left (1+i\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\left (2+i\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \sqrt {-\frac {1}{x^{2}}} \\
\end{align*} Verification of solutions
\[
y = \operatorname {undefined} \left (\left (1+i\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\left (2+i\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \sqrt {-\frac {1}{x^{2}}}
\] Warning, solution could not be verified
This is second order non-homogeneous ODE. In standard form the ODE is \[ A y''(x) + B y'(x) + C y(x) = f(x) \] Where \(A=9 x^{2}, B=27 x, C=10, f(x)=\frac {1}{x}\). Let the
solution be \[ y = y_h + y_p \] Where \(y_h\) is the solution to the homogeneous ODE \( A y''(x) + B y'(x) + C y(x) = 0\), and \(y_p\) is a particular
solution to the non-homogeneous ODE \(A y''(x) + B y'(x) + C y(x) = f(x)\). Solving for \(y_h\) from \[ 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = 0 \] In normal form the ode
\begin {align*} 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y&=0 \tag {1} \end {align*}
Becomes \begin {align*} y^{\prime \prime }+p \left (x \right ) y^{\prime }+q \left (x \right ) y&=0 \tag {2} \end {align*}
Where \begin {align*} p \left (x \right )&=\frac {3}{x}\\ q \left (x \right )&=\frac {10}{9 x^{2}} \end {align*}
Applying change of variables \(\tau = g \left (x \right )\) to (2) results \begin {align*} \frac {d^{2}}{d \tau ^{2}}y \left (\tau \right )+p_{1} \left (\frac {d}{d \tau }y \left (\tau \right )\right )+q_{1} y \left (\tau \right )&=0 \tag {3} \end {align*}
Where \(\tau \) is the new independent variable, and \begin {align*} p_{1} \left (\tau \right ) &=\frac {\tau ^{\prime \prime }\left (x \right )+p \left (x \right ) \tau ^{\prime }\left (x \right )}{{\tau ^{\prime }\left (x \right )}^{2}}\tag {4} \\ q_{1} \left (\tau \right ) &=\frac {q \left (x \right )}{{\tau ^{\prime }\left (x \right )}^{2}}\tag {5} \end {align*}
Let \(q_1=c^2\) where \(c\) is some constant. Therefore from (5) \begin {align*} \tau ' &= \frac {1}{c}\sqrt {q}\\ &= \frac {\sqrt {10}\, \sqrt {\frac {1}{x^{2}}}}{3 c}\tag {6} \\ \tau '' &= -\frac {\sqrt {10}}{3 c \sqrt {\frac {1}{x^{2}}}\, x^{3}} \end {align*}
Substituting the above into (4) results in \begin {align*} p_{1} \left (\tau \right ) &=\frac {\tau ^{\prime \prime }\left (x \right )+p \left (x \right ) \tau ^{\prime }\left (x \right )}{{\tau ^{\prime }\left (x \right )}^{2}}\\ &=\frac {-\frac {\sqrt {10}}{3 c \sqrt {\frac {1}{x^{2}}}\, x^{3}}+\frac {3}{x}\frac {\sqrt {10}\, \sqrt {\frac {1}{x^{2}}}}{3 c}}{\left (\frac {\sqrt {10}\, \sqrt {\frac {1}{x^{2}}}}{3 c}\right )^2} \\ &=\frac {3 c \sqrt {10}}{5} \end {align*}
Therefore ode (3) now becomes \begin {align*} y \left (\tau \right )'' + p_1 y \left (\tau \right )' + q_1 y \left (\tau \right ) &= 0 \\ \frac {d^{2}}{d \tau ^{2}}y \left (\tau \right )+\frac {3 c \sqrt {10}\, \left (\frac {d}{d \tau }y \left (\tau \right )\right )}{5}+c^{2} y \left (\tau \right ) &= 0 \tag {7} \end {align*}
The above ode is now solved for \(y \left (\tau \right )\). Since the ode is now constant coefficients, it can be easily
solved to give \begin {align*} y \left (\tau \right ) &= {\mathrm e}^{-\frac {3 \sqrt {10}\, c \tau }{10}} \left (c_{1} \cos \left (\frac {\sqrt {10}\, c \tau }{10}\right )+c_{2} \sin \left (\frac {\sqrt {10}\, c \tau }{10}\right )\right ) \end {align*}
Now from (6) \begin {align*} \tau &= \int \frac {1}{c} \sqrt q \,dx \\ &= \frac {\int \frac {\sqrt {10}\, \sqrt {\frac {1}{x^{2}}}}{3}d x}{c}\\ &= \frac {\sqrt {10}\, \sqrt {\frac {1}{x^{2}}}\, x \ln \left (x \right )}{3 c} \end {align*}
Substituting the above into the solution obtained gives \[
y = \frac {c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x}
\] Now the particular solution to this
ODE is found \[ 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = \frac {1}{x} \] The particular solution \(y_p\) can be found using either the method of
undetermined coefficients, or the method of variation of parameters. The method of variation
of parameters will be used as it is more general and can be used when the coefficients of the
ODE depend on \(x\) as well. Let \begin{equation}
\tag{1} y_p(x) = u_1 y_1 + u_2 y_2
\end{equation} Where \(u_1,u_2\) to be determined, and \(y_1,y_2\) are the two basis
solutions (the two linearly independent solutions of the homogeneous ODE) found
earlier when solving the homogeneous ODE as \begin{align*}
y_1 &= \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2} \\
y_2 &= \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2} \\
\end{align*} In the Variation of parameters \(u_1,u_2\) are
found using \begin{align*}
\tag{2} u_1 &= -\int \frac {y_2 f(x)}{a W(x)} \\
\tag{3} u_2 &= \int \frac {y_1 f(x)}{a W(x)} \\
\end{align*} Where \(W(x)\) is the Wronskian and \(a\) is the coefficient in front of \(y''\) in the
given ODE. The Wronskian is given by \(W= \begin {vmatrix} y_1 & y_{2} \\ y_{1}^{\prime } & y_{2}^{\prime } \end {vmatrix} \). Hence \[ W = \begin {vmatrix} \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2} & \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2} \\ \frac {d}{dx}\left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}\right ) & \frac {d}{dx}\left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}\right ) \end {vmatrix} \] Which gives \[ W = \begin {vmatrix} \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2} & \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2} \\ \frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}+\frac {\sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x} & \frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}-\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{6 x} \end {vmatrix} \] Therefore \[
W = \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}\right )\left (\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}-\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{6 x}\right ) - \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}\right )\left (\frac {\sqrt {2}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}+\frac {\sqrt {2}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2 \sqrt {-\frac {1}{x^{2}}}\, x^{3}}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{6 x}\right )
\] Which
simplifies to \[
W = \frac {\cos \left (\frac {\ln \left (2\right )}{6}\right )^{2} {\cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2}+\cos \left (\frac {\ln \left (2\right )}{6}\right )^{2} {\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2}+{\cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2} \sin \left (\frac {\ln \left (2\right )}{6}\right )^{2}+\sin \left (\frac {\ln \left (2\right )}{6}\right )^{2} {\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}^{2}}{6 x^{3}}
\] Which simplifies to \[
W = \frac {1}{6 x^{3}}
\] Therefore Eq. (2) becomes \[
u_1 = -\int \frac {\frac {\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}}{x}}{\frac {3}{2 x}}\,dx
\] Which simplifies to \[
u_1 = - \int \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \left (-\sin \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right )}{3}d x
\]
Hence \[
u_1 = \textit {undefined}
\] And Eq. (3) becomes \[
u_2 = \int \frac {\frac {\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}}{x}}{\frac {3}{2 x}}\,dx
\] Which simplifies to \[
u_2 = \int \frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \left (\cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right )}{3}d x
\] Hence \[
u_2 = \textit {undefined}
\] Therefore the particular
solution, from equation (1) is \[
y_p(x) = \operatorname {undefined} \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}+\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \sin \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}\right )+\operatorname {undefined} \left (\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (2\right )}{6}\right ) \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{2}-\frac {\sqrt {2}\, \sqrt {-\frac {1}{x^{2}}}\, \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right ) \sin \left (\frac {\ln \left (2\right )}{6}\right )}{2}\right )
\] Which simplifies to \[
y_p(x) = \sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined}
\] Therefore the general solution
is \begin{align*}
y &= y_h + y_p \\
&= \left (\frac {c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x}\right ) + \left (\sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined}\right ) \\
&= \sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined} +\frac {c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \\
\end{align*} Which simplifies to \[
y = \sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined} +\frac {c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x}
\] Initial conditions are used to solve for the constants of
integration.
Looking at the above solution \begin {align*} y = \sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined} +\frac {c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x} \tag {1} \end {align*}
Initial conditions are now substituted in the above solution. This will generate the required
equations to solve for the integration constants. substituting \(y = 0\) and \(x = 1\) in the above gives
\begin {align*} 0 = \textit {undefined}\tag {1A} \end {align*}
Taking derivative of the solution gives \begin {align*} y^{\prime } = \frac {\left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined}}{\sqrt {-\frac {1}{x^{2}}}\, x^{3}}+\sqrt {-\frac {1}{x^{2}}}\, \left (\frac {2 \sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{3 x}-\frac {\cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )}{3 x}\right ) \operatorname {undefined} +\sqrt {-\frac {1}{x^{2}}}\, \left (2 \cos \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )+\sin \left (\frac {\ln \left (-\frac {1}{x^{2}}\right )}{6}\right )\right ) \operatorname {undefined} -\frac {c_{1} \cos \left (\frac {\ln \left (x \right )}{3}\right )+c_{2} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{x^{2}}+\frac {-\frac {c_{1} \sin \left (\frac {\ln \left (x \right )}{3}\right )}{3 x}+\frac {c_{2} \cos \left (\frac {\ln \left (x \right )}{3}\right )}{3 x}}{x} \end {align*}
substituting \(y^{\prime } = -1\) and \(x = 1\) in the above gives \begin {align*} -1 = \operatorname {undefined} +\operatorname {undefined} i-c_{1} +\frac {1}{3} c_{2}\tag {2A} \end {align*}
Equations {1A,2A} are now solved for \(\{c_{1}, c_{2}\}\). There is no solution for the constants of
integrations. This solution is removed.
Verification of solutions N/A
This is second order non-homogeneous ODE. In standard form the ODE is \[
A y''(x) + B y'(x) + C y(x) = f(x)
\] Where \(A=9 x^{2}, B=27 x, C=10, f(x)=\frac {1}{x}\). Let the
solution be \[
y = y_h + y_p
\] Where \(y_h\) is the solution to the homogeneous ODE \( A y''(x) + B y'(x) + C y(x) = 0\), and \(y_p\) is a particular
solution to the non-homogeneous ODE \(A y''(x) + B y'(x) + C y(x) = f(x)\). Solving for \(y_h\) from \[
9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = 0
\] In normal form the ode
\begin {align*} 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y&=0 \tag {1} \end {align*}
Becomes \begin {align*} y^{\prime \prime }+p \left (x \right ) y^{\prime }+q \left (x \right ) y&=0 \tag {2} \end {align*}
Where \begin {align*} p \left (x \right )&=\frac {3}{x}\\ q \left (x \right )&=\frac {10}{9 x^{2}} \end {align*}
Applying change of variables on the depndent variable \(y = v \left (x \right ) x^{n}\) to (2) gives the following ode where
the dependent variables is \(v \left (x \right )\) and not \(y\). \begin {align*} v^{\prime \prime }\left (x \right )+\left (\frac {2 n}{x}+p \right ) v^{\prime }\left (x \right )+\left (\frac {n \left (n -1\right )}{x^{2}}+\frac {n p}{x}+q \right ) v \left (x \right )&=0 \tag {3} \end {align*}
Let the coefficient of \(v \left (x \right )\) above be zero. Hence \begin {align*} \frac {n \left (n -1\right )}{x^{2}}+\frac {n p}{x}+q&=0 \tag {4} \end {align*}
Substituting the earlier values found for \(p \left (x \right )\) and \(q \left (x \right )\) into (4) gives \begin {align*} \frac {n \left (n -1\right )}{x^{2}}+\frac {3 n}{x^{2}}+\frac {10}{9 x^{2}}&=0 \tag {5} \end {align*}
Solving (5) for \(n\) gives \begin {align*} n&=-1+\frac {i}{3} \tag {6} \end {align*}
Substituting this value in (3) gives \begin {align*} v^{\prime \prime }\left (x \right )+\left (\frac {-2+\frac {2 i}{3}}{x}+\frac {3}{x}\right ) v^{\prime }\left (x \right )&=0 \\ v^{\prime \prime }\left (x \right )+\frac {\left (1+\frac {2 i}{3}\right ) v^{\prime }\left (x \right )}{x}&=0 \tag {7} \\ \end {align*}
Using the substitution \begin {align*} u \left (x \right ) = v^{\prime }\left (x \right ) \end {align*}
Then (7) becomes \begin {align*} u^{\prime }\left (x \right )+\frac {\left (1+\frac {2 i}{3}\right ) u \left (x \right )}{x} = 0 \tag {8} \\ \end {align*}
The above is now solved for \(u \left (x \right )\). In canonical form the ODE is \begin {align*} u' &= F(x,u)\\ &= f( x) g(u)\\ &= \frac {\left (-1-\frac {2 i}{3}\right ) u}{x} \end {align*}
Where \(f(x)=\frac {-1-\frac {2 i}{3}}{x}\) and \(g(u)=u\). Integrating both sides gives \begin {align*} \frac {1}{u} \,du &= \frac {-1-\frac {2 i}{3}}{x} \,d x\\ \int { \frac {1}{u} \,du} &= \int {\frac {-1-\frac {2 i}{3}}{x} \,d x}\\ \ln \left (u \right )&=\left (-1-\frac {2 i}{3}\right ) \ln \left (x \right )+c_{1}\\ u&={\mathrm e}^{\left (-1-\frac {2 i}{3}\right ) \ln \left (x \right )+c_{1}}\\ &=c_{1} {\mathrm e}^{\left (-1-\frac {2 i}{3}\right ) \ln \left (x \right )} \end {align*}
Which simplifies to \[
u \left (x \right ) = \frac {c_{1} x^{-\frac {2 i}{3}}}{x}
\] Now that \(u \left (x \right )\) is known, then \begin {align*} v^{\prime }\left (x \right )&= u \left (x \right )\\ v \left (x \right )&= \int u \left (x \right )d x +c_{2}\\ &= \frac {3 i c_{1} x^{-\frac {2 i}{3}}}{2}+c_{2} \end {align*}
Hence \begin {align*} y&= v \left (x \right ) x^{n}\\ &= \left (\frac {3 i c_{1} x^{-\frac {2 i}{3}}}{2}+c_{2} \right ) x^{-1+\frac {i}{3}}\\ &= \frac {\left (3 i c_{1} x^{-\frac {2 i}{3}}+2 c_{2} \right ) x^{-1+\frac {i}{3}}}{2}\\ \end {align*}
Now the particular solution to this ODE is found \[
9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = \frac {1}{x}
\] The particular solution \(y_p\) can be found
using either the method of undetermined coefficients, or the method of variation of
parameters. The method of variation of parameters will be used as it is more general and can
be used when the coefficients of the ODE depend on \(x\) as well. Let \begin{equation}
\tag{1} y_p(x) = u_1 y_1 + u_2 y_2
\end{equation} Where \(u_1,u_2\) to be determined,
and \(y_1,y_2\) are the two basis solutions (the two linearly independent solutions of the homogeneous
ODE) found earlier when solving the homogeneous ODE as \begin{align*}
y_1 &= \frac {x^{\frac {i}{3}}}{x} \\
y_2 &= \frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x} \\
\end{align*} In the Variation of parameters \(u_1,u_2\)
are found using \begin{align*}
\tag{2} u_1 &= -\int \frac {y_2 f(x)}{a W(x)} \\
\tag{3} u_2 &= \int \frac {y_1 f(x)}{a W(x)} \\
\end{align*} Where \(W(x)\) is the Wronskian and \(a\) is the coefficient in front of \(y''\) in the
given ODE. The Wronskian is given by \(W= \begin {vmatrix} y_1 & y_{2} \\ y_{1}^{\prime } & y_{2}^{\prime } \end {vmatrix} \). Hence \[ W = \begin {vmatrix} \frac {x^{\frac {i}{3}}}{x} & \frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x} \\ \frac {d}{dx}\left (\frac {x^{\frac {i}{3}}}{x}\right ) & \frac {d}{dx}\left (\frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x}\right ) \end {vmatrix} \] Which gives \[ W = \begin {vmatrix} \frac {x^{\frac {i}{3}}}{x} & \frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x} \\ -\frac {x^{\frac {i}{3}}}{x^{2}}+\frac {i x^{\frac {i}{3}}}{3 x^{2}} & -\frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x^{2}}-\frac {i x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{3 x^{2}} \end {vmatrix} \] Therefore \[
W = \left (\frac {x^{\frac {i}{3}}}{x}\right )\left (-\frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x^{2}}-\frac {i x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{3 x^{2}}\right ) - \left (\frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x}\right )\left (-\frac {x^{\frac {i}{3}}}{x^{2}}+\frac {i x^{\frac {i}{3}}}{3 x^{2}}\right )
\] Which
simplifies to \[
W = -\frac {2 i x^{\frac {2 i}{3}} x^{-\frac {2 i}{3}}}{3 x^{3}}
\] Which simplifies to \[
W = -\frac {2 i}{3 x^{3}}
\] Therefore Eq. (2) becomes \[
u_1 = -\int \frac {\frac {x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x^{2}}}{-\frac {6 i}{x}}\,dx
\] Which simplifies to \[
u_1 = - \int \frac {i x^{-1-\frac {i}{3}}}{6}d x
\]
Hence \[
u_1 = \textit {undefined}
\] And Eq. (3) becomes \[
u_2 = \int \frac {\frac {x^{\frac {i}{3}}}{x^{2}}}{-\frac {6 i}{x}}\,dx
\] Which simplifies to \[
u_2 = \int \frac {i x^{-1+\frac {i}{3}}}{6}d x
\] Hence \[
u_2 = \textit {undefined}
\] Therefore the particular
solution, from equation (1) is \[
y_p(x) = \frac {\operatorname {undefined} \,x^{\frac {i}{3}}}{x}+\frac {\operatorname {undefined} \,x^{\frac {i}{3}} x^{-\frac {2 i}{3}}}{x}
\] Which simplifies to \[
y_p(x) = \frac {x^{\frac {i}{3}} \left (x^{-\frac {2 i}{3}}+1\right ) \operatorname {undefined}}{x}
\] Therefore the general solution
is \begin{align*}
y &= y_h + y_p \\
&= \left (\left (\frac {3 i c_{1} x^{-\frac {2 i}{3}}}{2}+c_{2} \right ) x^{-1+\frac {i}{3}}\right ) + \left (\frac {x^{\frac {i}{3}} \left (x^{-\frac {2 i}{3}}+1\right ) \operatorname {undefined}}{x}\right ) \\
&= \frac {x^{\frac {i}{3}} \left (x^{-\frac {2 i}{3}}+1\right ) \operatorname {undefined}}{x}+\left (\frac {3 i c_{1} x^{-\frac {2 i}{3}}}{2}+c_{2} \right ) x^{-1+\frac {i}{3}} \\
\end{align*} Which simplifies to \[
y = \frac {\left (3 i c_{1} +\operatorname {undefined} \right ) x^{-\frac {i}{3}}+2 x^{\frac {i}{3}} \left (c_{2} +\operatorname {undefined} \right )}{2 x}
\] Initial conditions are used to solve for the constants of
integration.
Looking at the above solution \begin {align*} y = \frac {\left (3 i c_{1} +\operatorname {undefined} \right ) x^{-\frac {i}{3}}+2 x^{\frac {i}{3}} \left (c_{2} +\operatorname {undefined} \right )}{2 x} \tag {1} \end {align*}
Initial conditions are now substituted in the above solution. This will generate the required
equations to solve for the integration constants. substituting \(y = 0\) and \(x = 1\) in the above gives
\begin {align*} 0 = \frac {3 i c_{1}}{2}+\operatorname {undefined} +c_{2}\tag {1A} \end {align*}
Taking derivative of the solution gives \begin {align*} y^{\prime } = \frac {-\frac {i \left (3 i c_{1} +\operatorname {undefined} \right ) x^{-\frac {i}{3}}}{3 x}+\frac {2 i x^{\frac {i}{3}} \left (c_{2} +\operatorname {undefined} \right )}{3 x}}{2 x}-\frac {\left (3 i c_{1} +\operatorname {undefined} \right ) x^{-\frac {i}{3}}+2 x^{\frac {i}{3}} \left (c_{2} +\operatorname {undefined} \right )}{2 x^{2}} \end {align*}
substituting \(y^{\prime } = -1\) and \(x = 1\) in the above gives \begin {align*} -1 = \operatorname {undefined} +\operatorname {undefined} i+\left (\frac {1}{2}-\frac {3 i}{2}\right ) c_{1} +\left (-1+\frac {i}{3}\right ) c_{2}\tag {2A} \end {align*}
Equations {1A,2A} are now solved for \(\{c_{1}, c_{2}\}\). There is no solution for the constants of
integrations. This solution is removed.
Verification of solutions N/A
Writing the ode as \begin {align*} 9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y &= 0 \tag {1} \\ A y^{\prime \prime } + B y^{\prime } + C y &= 0 \tag {2} \end {align*}
Comparing (1) and (2) shows that \begin {align*} A &= 9 x^{2} \\ B &= 27 x\tag {3} \\ C &= 10 \end {align*}
Applying the Liouville transformation on the dependent variable gives \begin {align*} z(x) &= y e^{\int \frac {B}{2 A} \,dx} \end {align*}
Then (2) becomes \begin {align*} z''(x) = r z(x)\tag {4} \end {align*}
Where \(r\) is given by \begin {align*} r &= \frac {s}{t}\tag {5} \\ &= \frac {2 A B' - 2 B A' + B^2 - 4 A C}{4 A^2} \end {align*}
Substituting the values of \(A,B,C\) from (3) in the above and simplifying gives \begin {align*} r &= \frac {-13}{36 x^{2}}\tag {6} \end {align*}
Comparing the above to (5) shows that \begin {align*} s &= -13\\ t &= 36 x^{2} \end {align*}
Therefore eq. (4) becomes \begin {align*} z''(x) &= \left ( -\frac {13}{36 x^{2}}\right ) z(x)\tag {7} \end {align*}
Equation (7) is now solved. After finding \(z(x)\) then \(y\) is found using the inverse transformation
\begin {align*} y &= z \left (x \right ) e^{-\int \frac {B}{2 A} \,dx} \end {align*}
The first step is to determine the case of Kovacic algorithm this ode belongs to. There are 3
cases depending on the order of poles of \(r\) and the order of \(r\) at \(\infty \). The following table
summarizes these cases. Case Allowed pole order for \(r\) Allowed value for \(\mathcal {O}(\infty )\) 1 \(\left \{ 0,1,2,4,6,8,\cdots \right \} \) \(\left \{ \cdots ,-6,-4,-2,0,2,3,4,5,6,\cdots \right \} \) 2
Need to have at least one pole
that is either order \(2\) or odd order
greater than \(2\). Any other pole order
is allowed as long as the above
condition is satisfied. Hence the
following set of pole orders are all
allowed. \(\{1,2\}\),\(\{1,3\}\),\(\{2\}\),\(\{3\}\),\(\{3,4\}\),\(\{1,2,5\}\). no condition 3 \(\left \{ 1,2\right \} \) \(\left \{ 2,3,4,5,6,7,\cdots \right \} \) The order of \(r\) at \(\infty \) is the degree of \(t\) minus the degree of \(s\). Therefore \begin {align*} O\left (\infty \right ) &= \text {deg}(t) - \text {deg}(s) \\ &= 2 - 0 \\ &= 2 \end {align*}
The poles of \(r\) in eq. (7) and the order of each pole are determined by solving for the roots of \(t=36 x^{2}\).
There is a pole at \(x=0\) of order \(2\). Since there is no odd order pole larger than \(2\) and the order at \(\infty \) is
\(2\) then the necessary conditions for case one are met. Since there is a pole of order \(2\) then
necessary conditions for case two are met. Since pole order is not larger than \(2\) and
the order at \(\infty \) is \(2\) then the necessary conditions for case three are met. Therefore
\begin {align*} L &= [1, 2, 4, 6, 12] \end {align*}
Attempting to find a solution using case \(n=1\).
Looking at poles of order 2. The partial fractions decomposition of \(r\) is \[
r = -\frac {13}{36 x^{2}}
\] For the pole at \(x=0\) let \(b\)
be the coefficient of \(\frac {1}{ x^{2}}\) in the partial fractions decomposition of \(r\) given above. Therefore \(b=-{\frac {13}{36}}\). Hence
\begin {alignat*} {2} [\sqrt r]_c &= 0 \\ \alpha _c^{+} &= \frac {1}{2} + \sqrt {1+4 b} &&= \frac {1}{2}+\frac {i}{3}\\ \alpha _c^{-} &= \frac {1}{2} - \sqrt {1+4 b} &&= \frac {1}{2}-\frac {i}{3} \end {alignat*}
Since the order of \(r\) at \(\infty \) is 2 then \([\sqrt r]_\infty =0\). Let \(b\) be the coefficient of \(\frac {1}{x^{2}}\) in the Laurent series expansion of \(r\)
at \(\infty \). which can be found by dividing the leading coefficient of \(s\) by the leading coefficient of \(t\)
from \begin {alignat*} {2} r &= \frac {s}{t} &&= -\frac {13}{36 x^{2}} \end {alignat*}
Since the \(\text {gcd}(s,t)=1\). This gives \(b=-{\frac {13}{36}}\). Hence \begin {alignat*} {2} [\sqrt r]_\infty &= 0 \\ \alpha _{\infty }^{+} &= \frac {1}{2} + \sqrt {1+4 b} &&= \frac {1}{2}+\frac {i}{3}\\ \alpha _{\infty }^{-} &= \frac {1}{2} - \sqrt {1+4 b} &&= \frac {1}{2}-\frac {i}{3} \end {alignat*}
The following table summarizes the findings so far for poles and for the order of \(r\) at \(\infty \) where \(r\)
is \[ r=-\frac {13}{36 x^{2}} \]
Now that the all \([\sqrt r]_c\) and its associated \(\alpha _c^{\pm }\) have been determined for all the poles in the set \(\Gamma \) and \([\sqrt r]_\infty \)
and its associated \(\alpha _\infty ^{\pm }\) have also been found, the next step is to determine possible non negative
integer \(d\) from these using \begin {align*} d &= \alpha _\infty ^{s(\infty )} - \sum _{c \in \Gamma } \alpha _c^{s(c)} \end {align*}
Where \(s(c)\) is either \(+\) or \(-\) and \(s(\infty )\) is the sign of \(\alpha _\infty ^{\pm }\). This is done by trial over all set of families \(s=(s(c))_{c \in \Gamma \cup {\infty }}\) until
such \(d\) is found to work in finding candidate \(\omega \). Trying \(\alpha _\infty ^{-} = \frac {1}{2}-\frac {i}{3}\) then \begin {align*} d &= \alpha _\infty ^{-} - \left ( \alpha _{c_1}^{-} \right ) \\ &= \frac {1}{2}-\frac {i}{3} - \left ( \frac {1}{2}-\frac {i}{3} \right ) \\ &= 0 \end {align*}
Since \(d\) an integer and \(d \geq 0\) then it can be used to find \(\omega \) using \begin {align*} \omega &= \sum _{c \in \Gamma } \left ( s(c) [\sqrt r]_c + \frac {\alpha _c^{s(c)}}{x-c} \right ) + s(\infty ) [\sqrt r]_\infty \end {align*}
The above gives \begin {align*} \omega &= \left ( (-)[\sqrt r]_{c_1} + \frac { \alpha _{c_1}^{-} }{x- c_1}\right ) + (-) [\sqrt r]_\infty \\ &= \frac {\frac {1}{2}-\frac {i}{3}}{x} + (-) \left ( 0 \right ) \\ &= \frac {\frac {1}{2}-\frac {i}{3}}{x}\\ &= \frac {\frac {1}{2}-\frac {i}{3}}{x} \end {align*}
Now that \(\omega \) is determined, the next step is find a corresponding minimal polynomial \(p(x)\) of degree
\(d=0\) to solve the ode. The polynomial \(p(x)\) needs to satisfy the equation \begin {align*} p'' + 2 \omega p' + \left ( \omega ' +\omega ^2 -r\right ) p = 0 \tag {1A} \end {align*}
Let \begin {align*} p(x) &= 1\tag {2A} \end {align*}
Substituting the above in eq. (1A) gives \begin {align*} \left (0\right ) + 2 \left (\frac {\frac {1}{2}-\frac {i}{3}}{x}\right ) \left (0\right ) + \left ( \left (\frac {-\frac {1}{2}+\frac {i}{3}}{x^{2}}\right ) + \left (\frac {\frac {1}{2}-\frac {i}{3}}{x}\right )^2 - \left (-\frac {13}{36 x^{2}}\right ) \right ) &= 0\\ 0 = 0 \end {align*}
The equation is satisfied since both sides are zero. Therefore the first solution to the ode \(z'' = r z\) is
\begin {align*} z_1(x) &= p e^{ \int \omega \,dx} \\ &= {\mathrm e}^{\int \frac {\frac {1}{2}-\frac {i}{3}}{x}d x}\\ &= x^{\frac {1}{2}-\frac {i}{3}} \end {align*}
The first solution to the original ode in \(y\) is found from \begin{align*}
y_1 &= z_1 e^{ \int -\frac {1}{2} \frac {B}{A} \,dx} \\
&= z_1 e^{ -\int \frac {1}{2} \frac {27 x}{9 x^{2}} \,dx} \\
&= z_1 e^{-\frac {3 \ln \left (x \right )}{2}} \\
&= z_1 \left (\frac {1}{x^{\frac {3}{2}}}\right ) \\
\end{align*} Which simplifies to \[
y_1 = x^{-1-\frac {i}{3}}
\] The second
solution \(y_2\) to the original ode is found using reduction of order \[ y_2 = y_1 \int \frac { e^{\int -\frac {B}{A} \,dx}}{y_1^2} \,dx \] Substituting gives \begin{align*}
y_2 &= y_1 \int \frac { e^{\int -\frac {27 x}{9 x^{2}} \,dx}}{\left (y_1\right )^2} \,dx \\
&= y_1 \int \frac { e^{-3 \ln \left (x \right )}}{\left (y_1\right )^2} \,dx \\
&= y_1 \left (-\frac {3 i x^{\frac {2 i}{3}}}{2}\right ) \\
\end{align*} Therefore
the solution is
\begin{align*}
y &= c_{1} y_1 + c_{2} y_2 \\
&= c_{1} \left (x^{-1-\frac {i}{3}}\right ) + c_{2} \left (x^{-1-\frac {i}{3}}\left (-\frac {3 i x^{\frac {2 i}{3}}}{2}\right )\right ) \\
\end{align*} This is second order nonhomogeneous ODE. Let the solution be \[
y = y_h + y_p
\] Where \(y_h\) is the solution to
the homogeneous ODE \( A y''(x) + B y'(x) + C y(x) = 0\), and \(y_p\) is a particular solution to the nonhomogeneous ODE \(A y''(x) + B y'(x) + C y(x) = f(x)\). \(y_h\) is
the solution to \[
9 x^{2} y^{\prime \prime }+27 y^{\prime } x +10 y = 0
\] The homogeneous solution is found using the Kovacic algorithm
which results in \[
y_h = c_{1} x^{-1-\frac {i}{3}}-\frac {3 i c_{2} x^{-1+\frac {i}{3}}}{2}
\] The particular solution \(y_p\) can be found using either the method of
undetermined coefficients, or the method of variation of parameters. The method of
variation of parameters will be used as it is more general and can be used when the
coefficients of the ODE depend on \(x\) as well. Let \begin{equation}
\tag{1} y_p(x) = u_1 y_1 + u_2 y_2
\end{equation} Where \(u_1,u_2\) to be determined, and \(y_1,y_2\) are the
two basis solutions (the two linearly independent solutions of the homogeneous
ODE) found earlier when solving the homogeneous ODE as \begin{align*}
y_1 &= x^{-1-\frac {i}{3}} \\
y_2 &= -\frac {3 i x^{-1+\frac {i}{3}}}{2} \\
\end{align*} In the Variation of
parameters \(u_1,u_2\) are found using \begin{align*}
\tag{2} u_1 &= -\int \frac {y_2 f(x)}{a W(x)} \\
\tag{3} u_2 &= \int \frac {y_1 f(x)}{a W(x)} \\
\end{align*} Where \(W(x)\) is the Wronskian and \(a\) is the coefficient in
front of \(y''\) in the given ODE. The Wronskian is given by \(W= \begin {vmatrix} y_1 & y_{2} \\ y_{1}^{\prime } & y_{2}^{\prime } \end {vmatrix} \). Hence \[ W = \begin {vmatrix} x^{-1-\frac {i}{3}} & -\frac {3 i x^{-1+\frac {i}{3}}}{2} \\ \frac {d}{dx}\left (x^{-1-\frac {i}{3}}\right ) & \frac {d}{dx}\left (-\frac {3 i x^{-1+\frac {i}{3}}}{2}\right ) \end {vmatrix} \] Which gives \[ W = \begin {vmatrix} x^{-1-\frac {i}{3}} & -\frac {3 i x^{-1+\frac {i}{3}}}{2} \\ \frac {\left (-1-\frac {i}{3}\right ) x^{-1-\frac {i}{3}}}{x} & \frac {\left (\frac {1}{2}+\frac {3 i}{2}\right ) x^{-1+\frac {i}{3}}}{x} \end {vmatrix} \]
Therefore \[
W = \left (x^{-1-\frac {i}{3}}\right )\left (\frac {\left (\frac {1}{2}+\frac {3 i}{2}\right ) x^{-1+\frac {i}{3}}}{x}\right ) - \left (-\frac {3 i x^{-1+\frac {i}{3}}}{2}\right )\left (\frac {\left (-1-\frac {i}{3}\right ) x^{-1-\frac {i}{3}}}{x}\right )
\] Which simplifies to \[
W = \frac {x^{-1-\frac {i}{3}} x^{-1+\frac {i}{3}}}{x}
\] Which simplifies to \[
W = \frac {1}{x^{3}}
\] Therefore Eq. (2) becomes \[
u_1 = -\int \frac {-\frac {3 i x^{-1+\frac {i}{3}}}{2 x}}{\frac {9}{x}}\,dx
\]
Which simplifies to \[
u_1 = - \int -\frac {i x^{-1+\frac {i}{3}}}{6}d x
\] Hence \[
u_1 = \textit {undefined}
\] And Eq. (3) becomes \[
u_2 = \int \frac {\frac {x^{-1-\frac {i}{3}}}{x}}{\frac {9}{x}}\,dx
\] Which simplifies to \[
u_2 = \int \frac {x^{-1-\frac {i}{3}}}{9}d x
\] Hence \[
u_2 = \textit {undefined}
\]
Therefore the particular solution, from equation (1) is \[
y_p(x) = \operatorname {undefined} \,x^{-1-\frac {i}{3}}-i \operatorname {undefined} \,x^{-1+\frac {i}{3}}
\] Which simplifies to \[
y_p(x) = \left (i x^{-1+\frac {i}{3}}+x^{-1-\frac {i}{3}}\right ) \operatorname {undefined}
\] Therefore
the general solution is \begin{align*}
y &= y_h + y_p \\
&= \left (c_{1} x^{-1-\frac {i}{3}}-\frac {3 i c_{2} x^{-1+\frac {i}{3}}}{2}\right ) + \left (\left (i x^{-1+\frac {i}{3}}+x^{-1-\frac {i}{3}}\right ) \operatorname {undefined}\right ) \\
\end{align*} Initial conditions are used to solve for the constants of
integration.
Looking at the above solution \begin {align*} y = c_{1} x^{-1-\frac {i}{3}}-\frac {3 i c_{2} x^{-1+\frac {i}{3}}}{2}+\left (i x^{-1+\frac {i}{3}}+x^{-1-\frac {i}{3}}\right ) \operatorname {undefined} \tag {1} \end {align*}
Initial conditions are now substituted in the above solution. This will generate the required
equations to solve for the integration constants. substituting \(y = 0\) and \(x = 1\) in the above gives
\begin {align*} 0 = \operatorname {undefined} +\operatorname {undefined} i-\frac {3}{2} i c_{2} +c_{1}\tag {1A} \end {align*}
Taking derivative of the solution gives \begin {align*} y^{\prime } = \frac {\left (-1-\frac {i}{3}\right ) c_{1} x^{-1-\frac {i}{3}}}{x}+\frac {\left (\frac {1}{2}+\frac {3 i}{2}\right ) c_{2} x^{-1+\frac {i}{3}}}{x}+\left (\frac {\left (-\frac {1}{3}-i\right ) x^{-1+\frac {i}{3}}}{x}+\frac {\left (-1-\frac {i}{3}\right ) x^{-1-\frac {i}{3}}}{x}\right ) \operatorname {undefined} +\left (i x^{-1+\frac {i}{3}}+x^{-1-\frac {i}{3}}\right ) \operatorname {undefined} \end {align*}
substituting \(y^{\prime } = -1\) and \(x = 1\) in the above gives \begin {align*} -1 = \operatorname {undefined} +\operatorname {undefined} i+\left (-1-\frac {i}{3}\right ) c_{1} +\left (\frac {1}{2}+\frac {3 i}{2}\right ) c_{2}\tag {2A} \end {align*}
Equations {1A,2A} are now solved for \(\{c_{1}, c_{2}\}\). There is no solution for the constants of
integrations. This solution is removed.
Verification of solutions N/A Maple trace
✓ Solution by Maple
Time used: 0.031 (sec). Leaf size: 24
\[
y \left (x \right ) = \frac {-3 \sin \left (\frac {\ln \left (x \right )}{3}\right )-\cos \left (\frac {\ln \left (x \right )}{3}\right )+1}{x}
\]
✓ Solution by Mathematica
Time used: 0.129 (sec). Leaf size: 28
\[
y(x)\to -\frac {3 \sin \left (\frac {\log (x)}{3}\right )+\cos \left (\frac {\log (x)}{3}\right )-1}{x}
\]
15.42.2 Solving as second order euler ode ode
15.42.3 Solving as second order change of variable on x method 2 ode
15.42.4 Solving as second order change of variable on x method 1 ode
15.42.5 Solving as second order change of variable on y method 2 ode
15.42.6 Solving using Kovacic algorithm
pole \(c\) location
pole order
\([\sqrt r]_c\)
\(\alpha _c^{+}\)
\(\alpha _c^{-}\)
\(0\) \(2\) \(0\) \(\frac {1}{2}+\frac {i}{3}\) \(\frac {1}{2}-\frac {i}{3}\)
Order of \(r\) at \(\infty \)
\([\sqrt r]_\infty \)
\(\alpha _\infty ^{+}\)
\(\alpha _\infty ^{-}\) \(2\)
\(0\) \(\frac {1}{2}+\frac {i}{3}\) \(\frac {1}{2}-\frac {i}{3}\)
`Methods for second order ODEs:
--- Trying classification methods ---
trying a quadrature
trying high order exact linear fully integrable
trying differential order: 2; linear nonhomogeneous with symmetry [0,1]
trying a double symmetry of the form [xi=0, eta=F(x)]
-> Try solving first the homogeneous part of the ODE
checking if the LODE has constant coefficients
checking if the LODE is of Euler type
<- LODE of Euler type successful
<- solving first the homogeneous part of the ODE successful`
dsolve([9*x^2*diff(y(x),x$2)+27*x*diff(y(x),x)+10*y(x)=1/x,y(1) = 0, D(y)(1) = -1],y(x), singsol=all)
DSolve[{9*x^2*y''[x]+27*x*y'[x]+10*y[x]==1/x,{y[1]==0,y'[1]==-1}},y[x],x,IncludeSingularSolutions -> True]