5.16 problem 16

Internal problem ID [7957]
Book : Own collection of miscellaneous problems
Section : section 5.0
Problem number : 16
Date solved : Monday, October 21, 2024 at 04:39:32 PM
CAS classification : [[_2nd_order, _linear, _nonhomogeneous]]

Solve

\begin{align*} y^{\prime \prime }+2 y^{\prime }-24 y&=16-\left (x +2\right ) {\mathrm e}^{4 x} \end{align*}

5.16.1 Solved as second order linear constant coeff ode

Time used: 0.148 (sec)

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 \(A=1, B=2, C=-24, f(x)=16+\left (-x -2\right ) {\mathrm e}^{4 x}\). 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 \(A y''(x) + B y'(x) + C y(x) = f(x)\). \(y_h\) is the solution to

\[ y^{\prime \prime }+2 y^{\prime }-24 y = 0 \]

This is second order with constant coefficients homogeneous ODE. In standard form the ODE is

\[ A y''(x) + B y'(x) + C y(x) = 0 \]

Where in the above \(A=1, B=2, C=-24\). Let the solution be \(y=e^{\lambda x}\). Substituting this into the ODE gives

\[ \lambda ^{2} {\mathrm e}^{x \lambda }+2 \lambda \,{\mathrm e}^{x \lambda }-24 \,{\mathrm e}^{x \lambda } = 0 \tag {1} \]

Since exponential function is never zero, then dividing Eq(2) throughout by \(e^{\lambda x}\) gives

\[ \lambda ^{2}+2 \lambda -24 = 0 \tag {2} \]

Equation (2) is the characteristic equation of the ODE. Its roots determine the general solution form.Using the quadratic formula

\[ \lambda _{1,2} = \frac {-B}{2 A} \pm \frac {1}{2 A} \sqrt {B^2 - 4 A C} \]

Substituting \(A=1, B=2, C=-24\) into the above gives

\begin{align*} \lambda _{1,2} &= \frac {-2}{(2) \left (1\right )} \pm \frac {1}{(2) \left (1\right )} \sqrt {2^2 - (4) \left (1\right )\left (-24\right )}\\ &= -1 \pm 5 \end{align*}

Hence

\begin{align*} \lambda _1 &= -1 + 5 \\ \lambda _2 &= -1 - 5 \\ \end{align*}

Which simplifies to

\begin{align*} \lambda _1 &= 4 \\ \lambda _2 &= -6 \\ \end{align*}

Since roots are real and distinct, then the solution is

\begin{align*} y &= c_1 e^{\lambda _1 x} + c_2 e^{\lambda _2 x} \\ y &= c_1 e^{\left (4\right )x} +c_2 e^{\left (-6\right )x} \\ \end{align*}

Or

\[ y =c_1 \,{\mathrm e}^{4 x}+c_2 \,{\mathrm e}^{-6 x} \]

Therefore the homogeneous solution \(y_h\) is

\[ y_h = c_1 \,{\mathrm e}^{4 x}+c_2 \,{\mathrm e}^{-6 x} \]

The particular solution is now found using the method of undetermined coefficients. Looking at the RHS of the ode, which is

\[ 16+\left (-x -2\right ) {\mathrm e}^{4 x} \]

Shows that the corresponding undetermined set of the basis functions (UC_set) for the trial solution is

\[ [\{1\}, \{{\mathrm e}^{4 x} x, {\mathrm e}^{4 x}\}] \]

While the set of the basis functions for the homogeneous solution found earlier is

\[ \{{\mathrm e}^{-6 x}, {\mathrm e}^{4 x}\} \]

Since \({\mathrm e}^{4 x}\) is duplicated in the UC_set, then this basis is multiplied by extra \(x\). The UC_set becomes

\[ [\{1\}, \{x^{2} {\mathrm e}^{4 x}, {\mathrm e}^{4 x} x\}] \]

Since there was duplication between the basis functions in the UC_set and the basis functions of the homogeneous solution, the trial solution is a linear combination of all the basis function in the above updated UC_set.

\[ y_p = A_{1}+A_{2} x^{2} {\mathrm e}^{4 x}+A_{3} {\mathrm e}^{4 x} x \]

The unknowns \(\{A_{1}, A_{2}, A_{3}\}\) are found by substituting the above trial solution \(y_p\) into the ODE and comparing coefficients. Substituting the trial solution into the ODE and simplifying gives

\[ 2 A_{2} {\mathrm e}^{4 x}+20 A_{2} x \,{\mathrm e}^{4 x}+10 A_{3} {\mathrm e}^{4 x}-24 A_{1} = 16-\left (x +2\right ) {\mathrm e}^{4 x} \]

Solving for the unknowns by comparing coefficients results in

\[ \left [A_{1} = -{\frac {2}{3}}, A_{2} = -{\frac {1}{20}}, A_{3} = -{\frac {19}{100}}\right ] \]

Substituting the above back in the above trial solution \(y_p\), gives the particular solution

\[ y_p = -\frac {2}{3}-\frac {x^{2} {\mathrm e}^{4 x}}{20}-\frac {19 \,{\mathrm e}^{4 x} x}{100} \]

Therefore the general solution is

\begin{align*} y &= y_h + y_p \\ &= \left (c_1 \,{\mathrm e}^{4 x}+c_2 \,{\mathrm e}^{-6 x}\right ) + \left (-\frac {2}{3}-\frac {x^{2} {\mathrm e}^{4 x}}{20}-\frac {19 \,{\mathrm e}^{4 x} x}{100}\right ) \\ \end{align*}

Will add steps showing solving for IC soon.

Figure 213: Slope field plot
\(y^{\prime \prime }+2 y^{\prime }-24 y = 16-\left (x +2\right ) {\mathrm e}^{4 x}\)

5.16.2 Solved as second order ode using Kovacic algorithm

Time used: 0.204 (sec)

Writing the ode as

\begin{align*} y^{\prime \prime }+2 y^{\prime }-24 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 &= 1 \\ B &= 2\tag {3} \\ C &= -24 \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 {25}{1}\tag {6} \end{align*}

Comparing the above to (5) shows that

\begin{align*} s &= 25\\ t &= 1 \end{align*}

Therefore eq. (4) becomes

\begin{align*} z''(x) &= 25 z \left (x \right ) \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	\(\left \{ 1,2\right \} \)	\(\left \{ 2,3,4,5,6,7,\cdots \right \} \)

Table 121: Necessary conditions for each Kovacic case

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) \\ &= 0 - 0 \\ &= 0 \end{align*}

There are no poles in \(r\). Therefore the set of poles \(\Gamma \) is empty. Since there is no odd order pole larger than \(2\) and the order at \(\infty \) is \(0\) then the necessary conditions for case one are met. Therefore

\begin{align*} L &= [1] \end{align*}

Since \(r = 25\) is not a function of \(x\), then there is no need run Kovacic algorithm to obtain a solution for transformed ode \(z''=r z\) as one solution is

\[ z_1(x) = {\mathrm e}^{-5 x} \]

Using the above, the solution for the original ode can now be found. 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 {2}{1} \,dx} \\ &= z_1 e^{-x} \\ &= z_1 \left ({\mathrm e}^{-x}\right ) \\ \end{align*}

Which simplifies to

\[ y_1 = {\mathrm e}^{-6 x} \]

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 {2}{1} \,dx}}{\left (y_1\right )^2} \,dx \\ &= y_1 \int \frac { e^{-2 x}}{\left (y_1\right )^2} \,dx \\ &= y_1 \left (\frac {{\mathrm e}^{-2 x} {\mathrm e}^{12 x}}{10}\right ) \\ \end{align*}

Therefore the solution is

\begin{align*} y &= c_1 y_1 + c_2 y_2 \\ &= c_1 \left ({\mathrm e}^{-6 x}\right ) + c_2 \left ({\mathrm e}^{-6 x}\left (\frac {{\mathrm e}^{-2 x} {\mathrm e}^{12 x}}{10}\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

\[ y^{\prime \prime }+2 y^{\prime }-24 y = 0 \]

The homogeneous solution is found using the Kovacic algorithm which results in

\[ y_h = c_1 \,{\mathrm e}^{-6 x}+\frac {c_2 \,{\mathrm e}^{4 x}}{10} \]

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 &= {\mathrm e}^{-6 x} \\ y_2 &= \frac {{\mathrm e}^{4 x}}{10} \\ \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

\[ W = \begin {vmatrix} {\mathrm e}^{-6 x} & \frac {{\mathrm e}^{4 x}}{10} \\ \frac {d}{dx}\left ({\mathrm e}^{-6 x}\right ) & \frac {d}{dx}\left (\frac {{\mathrm e}^{4 x}}{10}\right ) \end {vmatrix} \]

Which gives

\[ W = \begin {vmatrix} {\mathrm e}^{-6 x} & \frac {{\mathrm e}^{4 x}}{10} \\ -6 \,{\mathrm e}^{-6 x} & \frac {2 \,{\mathrm e}^{4 x}}{5} \end {vmatrix} \]

Therefore

\[ W = \left ({\mathrm e}^{-6 x}\right )\left (\frac {2 \,{\mathrm e}^{4 x}}{5}\right ) - \left (\frac {{\mathrm e}^{4 x}}{10}\right )\left (-6 \,{\mathrm e}^{-6 x}\right ) \]

Which simplifies to

\[ W = {\mathrm e}^{-6 x} {\mathrm e}^{4 x} \]

Which simplifies to

\[ W = {\mathrm e}^{-2 x} \]

Therefore Eq. (2) becomes

\[ u_1 = -\int \frac {\frac {{\mathrm e}^{4 x} \left (16+\left (-x -2\right ) {\mathrm e}^{4 x}\right )}{10}}{{\mathrm e}^{-2 x}}\,dx \]

Which simplifies to

\[ u_1 = - \int -\frac {{\mathrm e}^{6 x} \left (-16+\left (x +2\right ) {\mathrm e}^{4 x}\right )}{10}d x \]

Hence

\[ u_1 = \frac {{\mathrm e}^{10 x} x}{100}+\frac {19 \,{\mathrm e}^{10 x}}{1000}-\frac {4 \,{\mathrm e}^{6 x}}{15} \]

And Eq. (3) becomes

\[ u_2 = \int \frac {{\mathrm e}^{-6 x} \left (16+\left (-x -2\right ) {\mathrm e}^{4 x}\right )}{{\mathrm e}^{-2 x}}\,dx \]

Which simplifies to

\[ u_2 = \int \left (16 \,{\mathrm e}^{-4 x}-x -2\right )d x \]

Hence

\[ u_2 = -2 x -\frac {x^{2}}{2}-4 \,{\mathrm e}^{-4 x} \]

Therefore the particular solution, from equation (1) is

\[ y_p(x) = \left (\frac {{\mathrm e}^{10 x} x}{100}+\frac {19 \,{\mathrm e}^{10 x}}{1000}-\frac {4 \,{\mathrm e}^{6 x}}{15}\right ) {\mathrm e}^{-6 x}+\frac {{\mathrm e}^{4 x} \left (-2 x -\frac {x^{2}}{2}-4 \,{\mathrm e}^{-4 x}\right )}{10} \]

Which simplifies to

\[ y_p(x) = -\frac {2}{3}+\frac {\left (-50 x^{2}-190 x +19\right ) {\mathrm e}^{4 x}}{1000} \]

Therefore the general solution is

\begin{align*} y &= y_h + y_p \\ &= \left (c_1 \,{\mathrm e}^{-6 x}+\frac {c_2 \,{\mathrm e}^{4 x}}{10}\right ) + \left (-\frac {2}{3}+\frac {\left (-50 x^{2}-190 x +19\right ) {\mathrm e}^{4 x}}{1000}\right ) \\ \end{align*}

Will add steps showing solving for IC soon.

Figure 214: Slope field plot
\(y^{\prime \prime }+2 y^{\prime }-24 y = 16-\left (x +2\right ) {\mathrm e}^{4 x}\)

5.16.3 Solved as second order ode adjoint method

Time used: 1.121 (sec)

In normal form the ode

\begin{align*} y^{\prime \prime }+2 y^{\prime }-24 y = 16-\left (x +2\right ) {\mathrm e}^{4 x} \tag {1} \end{align*}

Becomes

\begin{align*} y^{\prime \prime }+p \left (x \right ) y^{\prime }+q \left (x \right ) y&=r \left (x \right ) \tag {2} \end{align*}

Where

\begin{align*} p \left (x \right )&=2\\ q \left (x \right )&=-24\\ r \left (x \right )&=16+\left (-x -2\right ) {\mathrm e}^{4 x} \end{align*}

The Lagrange adjoint ode is given by

\begin{align*} \xi ^{''}-(\xi \, p)'+\xi q &= 0\\ \xi ^{''}-\left (2 \xi \left (x \right )\right )' + \left (-24 \xi \left (x \right )\right ) &= 0\\ \xi ^{\prime \prime }\left (x \right )-2 \xi ^{\prime }\left (x \right )-24 \xi \left (x \right )&= 0 \end{align*}

Which is solved for \(\xi (x)\). This is second order with constant coefficients homogeneous ODE. In standard form the ODE is

\[ A \xi ''(x) + B \xi '(x) + C \xi (x) = 0 \]

Where in the above \(A=1, B=-2, C=-24\). Let the solution be \(\xi =e^{\lambda x}\). Substituting this into the ODE gives

\[ \lambda ^{2} {\mathrm e}^{x \lambda }-2 \lambda \,{\mathrm e}^{x \lambda }-24 \,{\mathrm e}^{x \lambda } = 0 \tag {1} \]

Since exponential function is never zero, then dividing Eq(2) throughout by \(e^{\lambda x}\) gives

\[ \lambda ^{2}-2 \lambda -24 = 0 \tag {2} \]

Equation (2) is the characteristic equation of the ODE. Its roots determine the general solution form.Using the quadratic formula

\[ \lambda _{1,2} = \frac {-B}{2 A} \pm \frac {1}{2 A} \sqrt {B^2 - 4 A C} \]

Substituting \(A=1, B=-2, C=-24\) into the above gives

\begin{align*} \lambda _{1,2} &= \frac {2}{(2) \left (1\right )} \pm \frac {1}{(2) \left (1\right )} \sqrt {-2^2 - (4) \left (1\right )\left (-24\right )}\\ &= 1 \pm 5 \end{align*}

Hence

\begin{align*} \lambda _1 &= 1 + 5 \\ \lambda _2 &= 1 - 5 \\ \end{align*}

Which simplifies to

\begin{align*} \lambda _1 &= 6 \\ \lambda _2 &= -4 \\ \end{align*}

Since roots are real and distinct, then the solution is

\begin{align*} \xi &= c_1 e^{\lambda _1 x} + c_2 e^{\lambda _2 x} \\ \xi &= c_1 e^{\left (6\right )x} +c_2 e^{\left (-4\right )x} \\ \end{align*}

Or

\[ \xi =c_1 \,{\mathrm e}^{6 x}+c_2 \,{\mathrm e}^{-4 x} \]

Will add steps showing solving for IC soon.

The original ode (2) now reduces to first order ode

\begin{align*} \xi \left (x \right ) y^{\prime }-y \xi ^{\prime }\left (x \right )+\xi \left (x \right ) p \left (x \right ) y&=\int \xi \left (x \right ) r \left (x \right )d x\\ y^{\prime }+y \left (p \left (x \right )-\frac {\xi ^{\prime }\left (x \right )}{\xi \left (x \right )}\right )&=\frac {\int \xi \left (x \right ) r \left (x \right )d x}{\xi \left (x \right )}\\ y^{\prime }+y \left (2-\frac {6 c_1 \,{\mathrm e}^{6 x}-4 c_2 \,{\mathrm e}^{-4 x}}{c_1 \,{\mathrm e}^{6 x}+c_2 \,{\mathrm e}^{-4 x}}\right )&=\frac {-2 c_2 x +\frac {8 c_1 \,{\mathrm e}^{6 x}}{3}-\frac {c_1 \,{\mathrm e}^{10 x}}{5}-\frac {c_2 \,x^{2}}{2}-4 c_2 \,{\mathrm e}^{-4 x}-c_1 \left (\frac {{\mathrm e}^{10 x} x}{10}-\frac {{\mathrm e}^{10 x}}{100}\right )}{c_1 \,{\mathrm e}^{6 x}+c_2 \,{\mathrm e}^{-4 x}} \end{align*}

Which is now a first order ode. This is now solved for \(y\). In canonical form a linear first order is

\begin{align*} y^{\prime } + q(x)y &= p(x) \end{align*}

Comparing the above to the given ode shows that

\begin{align*} q(x) &=-\frac {\left (1200 \,{\mathrm e}^{6 x} {\mathrm e}^{4 x} c_1 -1800 \,{\mathrm e}^{-4 x} {\mathrm e}^{4 x} c_2 \right ) {\mathrm e}^{-4 x}}{300 \left (c_1 \,{\mathrm e}^{6 x}+c_2 \,{\mathrm e}^{-4 x}\right )}\\ p(x) &=\frac {\left (-30 c_1 \,{\mathrm e}^{14 x} x -57 c_1 \,{\mathrm e}^{14 x}+800 c_1 \,{\mathrm e}^{10 x}-150 c_2 \,x^{2} {\mathrm e}^{4 x}-600 c_2 x \,{\mathrm e}^{4 x}-1200 c_2 \right ) {\mathrm e}^{-4 x}}{300 c_1 \,{\mathrm e}^{6 x}+300 c_2 \,{\mathrm e}^{-4 x}} \end{align*}

The integrating factor \(\mu \) is

\begin{align*} \mu &= e^{\int {q\,dx}}\\ &= {\mathrm e}^{\int -\frac {\left (1200 \,{\mathrm e}^{6 x} {\mathrm e}^{4 x} c_1 -1800 \,{\mathrm e}^{-4 x} {\mathrm e}^{4 x} c_2 \right ) {\mathrm e}^{-4 x}}{300 \left (c_1 \,{\mathrm e}^{6 x}+c_2 \,{\mathrm e}^{-4 x}\right )}d x}\\ &= \frac {{\mathrm e}^{6 x}}{c_1 \,{\mathrm e}^{10 x}+c_2} \end{align*}

The ode becomes

\begin{align*} \frac {\mathop {\mathrm {d}}}{ \mathop {\mathrm {d}x}}\left ( \mu y\right ) &= \mu p \\ \frac {\mathop {\mathrm {d}}}{ \mathop {\mathrm {d}x}}\left ( \mu y\right ) &= \left (\mu \right ) \left (\frac {\left (-30 c_1 \,{\mathrm e}^{14 x} x -57 c_1 \,{\mathrm e}^{14 x}+800 c_1 \,{\mathrm e}^{10 x}-150 c_2 \,x^{2} {\mathrm e}^{4 x}-600 c_2 x \,{\mathrm e}^{4 x}-1200 c_2 \right ) {\mathrm e}^{-4 x}}{300 c_1 \,{\mathrm e}^{6 x}+300 c_2 \,{\mathrm e}^{-4 x}}\right ) \\ \frac {\mathop {\mathrm {d}}}{ \mathop {\mathrm {d}x}} \left (\frac {y \,{\mathrm e}^{6 x}}{c_1 \,{\mathrm e}^{10 x}+c_2}\right ) &= \left (\frac {{\mathrm e}^{6 x}}{c_1 \,{\mathrm e}^{10 x}+c_2}\right ) \left (\frac {\left (-30 c_1 \,{\mathrm e}^{14 x} x -57 c_1 \,{\mathrm e}^{14 x}+800 c_1 \,{\mathrm e}^{10 x}-150 c_2 \,x^{2} {\mathrm e}^{4 x}-600 c_2 x \,{\mathrm e}^{4 x}-1200 c_2 \right ) {\mathrm e}^{-4 x}}{300 c_1 \,{\mathrm e}^{6 x}+300 c_2 \,{\mathrm e}^{-4 x}}\right ) \\ \mathrm {d} \left (\frac {y \,{\mathrm e}^{6 x}}{c_1 \,{\mathrm e}^{10 x}+c_2}\right ) &= \left (\frac {\left (-30 c_1 \,{\mathrm e}^{14 x} x -57 c_1 \,{\mathrm e}^{14 x}+800 c_1 \,{\mathrm e}^{10 x}-150 c_2 \,x^{2} {\mathrm e}^{4 x}-600 c_2 x \,{\mathrm e}^{4 x}-1200 c_2 \right ) {\mathrm e}^{-4 x} {\mathrm e}^{6 x}}{300 \left (c_1 \,{\mathrm e}^{6 x}+c_2 \,{\mathrm e}^{-4 x}\right ) \left (c_1 \,{\mathrm e}^{10 x}+c_2 \right )}\right )\, \mathrm {d} x \\ \end{align*}

Integrating gives

\begin{align*} \frac {y \,{\mathrm e}^{6 x}}{c_1 \,{\mathrm e}^{10 x}+c_2}&= \int {\frac {\left (-30 c_1 \,{\mathrm e}^{14 x} x -57 c_1 \,{\mathrm e}^{14 x}+800 c_1 \,{\mathrm e}^{10 x}-150 c_2 \,x^{2} {\mathrm e}^{4 x}-600 c_2 x \,{\mathrm e}^{4 x}-1200 c_2 \right ) {\mathrm e}^{-4 x} {\mathrm e}^{6 x}}{300 \left (c_1 \,{\mathrm e}^{6 x}+c_2 \,{\mathrm e}^{-4 x}\right ) \left (c_1 \,{\mathrm e}^{10 x}+c_2 \right )} \,dx} \\ &=-\frac {x^{2}}{20 c_1}-\frac {19 x}{100 c_1}+\frac {-2000 c_1 \,{\mathrm e}^{6 x}+150 c_2 \,x^{2}+570 c_2 x -57 c_2}{3000 \left (c_1 \,{\mathrm e}^{10 x}+c_2 \right ) c_1} + c_3 \end{align*}

Dividing throughout by the integrating factor \(\frac {{\mathrm e}^{6 x}}{c_1 \,{\mathrm e}^{10 x}+c_2}\) gives the final solution

\[ y = -\frac {{\mathrm e}^{-6 x} \left (c_1 \left (x^{2}-20 c_3 c_1 +\frac {19}{5} x \right ) {\mathrm e}^{10 x}-20 c_1 c_2 c_3 +\frac {40 c_1 \,{\mathrm e}^{6 x}}{3}+\frac {19 c_2}{50}\right )}{20 c_1} \]

Hence, the solution found using Lagrange adjoint equation method is

\begin{align*} y &= -\frac {{\mathrm e}^{-6 x} \left (c_1 \left (x^{2}-20 c_3 c_1 +\frac {19}{5} x \right ) {\mathrm e}^{10 x}-20 c_1 c_2 c_3 +\frac {40 c_1 \,{\mathrm e}^{6 x}}{3}+\frac {19 c_2}{50}\right )}{20 c_1} \\ \end{align*}

Will add steps showing solving for IC soon.

Figure 215: Slope field plot
\(y^{\prime \prime }+2 y^{\prime }-24 y = 16-\left (x +2\right ) {\mathrm e}^{4 x}\)

5.16.4 Maple step by step solution

\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & \frac {d}{d x}y^{\prime }+2 y^{\prime }-24 y=16-\left (x +2\right ) {\mathrm e}^{4 x} \\ \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 }=-{\mathrm e}^{4 x} x -2 y^{\prime }+24 y-2 \,{\mathrm e}^{4 x}+16 \\ \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 }+2 y^{\prime }-24 y=16-{\mathrm e}^{4 x} x -2 \,{\mathrm e}^{4 x} \\ \bullet & {} & \textrm {Characteristic polynomial of homogeneous ODE}\hspace {3pt} \\ {} & {} & r^{2}+2 r -24=0 \\ \bullet & {} & \textrm {Factor the characteristic polynomial}\hspace {3pt} \\ {} & {} & \left (r +6\right ) \left (r -4\right )=0 \\ \bullet & {} & \textrm {Roots of the characteristic polynomial}\hspace {3pt} \\ {} & {} & r =\left (-6, 4\right ) \\ \bullet & {} & \textrm {1st solution of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y_{1}\left (x \right )={\mathrm e}^{-6 x} \\ \bullet & {} & \textrm {2nd solution of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y_{2}\left (x \right )={\mathrm e}^{4 x} \\ \bullet & {} & \textrm {General solution of the ODE}\hspace {3pt} \\ {} & {} & y=\mathit {C1} y_{1}\left (x \right )+\mathit {C2} y_{2}\left (x \right )+y_{p}\left (x \right ) \\ \bullet & {} & \textrm {Substitute in solutions of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y=\mathit {C1} \,{\mathrm e}^{-6 x}+\mathit {C2} \,{\mathrm e}^{4 x}+y_{p}\left (x \right ) \\ \square & {} & \textrm {Find a particular solution}\hspace {3pt} y_{p}\left (x \right )\hspace {3pt}\textrm {of the ODE}\hspace {3pt} \\ {} & \circ & \textrm {Use variation of parameters to find}\hspace {3pt} y_{p}\hspace {3pt}\textrm {here}\hspace {3pt} f \left (x \right )\hspace {3pt}\textrm {is the forcing function}\hspace {3pt} \\ {} & {} & \left [y_{p}\left (x \right )=-y_{1}\left (x \right ) \left (\int \frac {y_{2}\left (x \right ) f \left (x \right )}{W \left (y_{1}\left (x \right ), y_{2}\left (x \right )\right )}d x \right )+y_{2}\left (x \right ) \left (\int \frac {y_{1}\left (x \right ) f \left (x \right )}{W \left (y_{1}\left (x \right ), y_{2}\left (x \right )\right )}d x \right ), f \left (x \right )=16-{\mathrm e}^{4 x} x -2 \,{\mathrm e}^{4 x}\right ] \\ {} & \circ & \textrm {Wronskian of solutions of the homogeneous equation}\hspace {3pt} \\ {} & {} & W \left (y_{1}\left (x \right ), y_{2}\left (x \right )\right )=\left [\begin {array}{cc} {\mathrm e}^{-6 x} & {\mathrm e}^{4 x} \\ -6 \,{\mathrm e}^{-6 x} & 4 \,{\mathrm e}^{4 x} \end {array}\right ] \\ {} & \circ & \textrm {Compute Wronskian}\hspace {3pt} \\ {} & {} & W \left (y_{1}\left (x \right ), y_{2}\left (x \right )\right )=10 \,{\mathrm e}^{-2 x} \\ {} & \circ & \textrm {Substitute functions into equation for}\hspace {3pt} y_{p}\left (x \right ) \\ {} & {} & y_{p}\left (x \right )=\frac {\left ({\mathrm e}^{10 x} \left (\int \left (16 \,{\mathrm e}^{-4 x}-x -2\right )d x \right )+\int {\mathrm e}^{6 x} \left (-16+\left (x +2\right ) {\mathrm e}^{4 x}\right )d x \right ) {\mathrm e}^{-6 x}}{10} \\ {} & \circ & \textrm {Compute integrals}\hspace {3pt} \\ {} & {} & y_{p}\left (x \right )=-\frac {2}{3}+\frac {\left (-50 x^{2}-190 x +19\right ) {\mathrm e}^{4 x}}{1000} \\ \bullet & {} & \textrm {Substitute particular solution into general solution to ODE}\hspace {3pt} \\ {} & {} & y=\mathit {C1} \,{\mathrm e}^{-6 x}+\mathit {C2} \,{\mathrm e}^{4 x}-\frac {2}{3}+\frac {\left (-50 x^{2}-190 x +19\right ) {\mathrm e}^{4 x}}{1000} \end {array} \]

5.16.5 Maple trace

Methods for second order ODEs:
 

5.16.6 Maple dsolve solution

Solving time : 0.003 (sec)
Leaf size : 36

dsolve(diff(diff(y(x),x),x)+2*diff(y(x),x)-24*y(x) = 16-(x+2)*exp(4*x), 
       y(x),singsol=all)
 

\[ y = -\frac {{\mathrm e}^{-6 x} \left (\left (x^{2}+\frac {19}{5} x -20 c_1 -\frac {19}{50}\right ) {\mathrm e}^{10 x}-20 c_2 +\frac {40 \,{\mathrm e}^{6 x}}{3}\right )}{20} \]

5.16.7 Mathematica DSolve solution

Solving time : 0.222 (sec)
Leaf size : 41

DSolve[{D[y[x],{x,2}]+2*D[y[x],x]-24*y[x]==16-(x+2)*Exp[4*x],{}}, 
       y[x],x,IncludeSingularSolutions->True]
 

\[ y(x)\to e^{4 x} \left (-\frac {x^2}{20}-\frac {19 x}{100}+\frac {19}{1000}+c_2\right )+c_1 e^{-6 x}-\frac {2}{3} \]