91Ó°ÊÓ

The auxiliary equation is:$r^4+2{\mathrm{r}}^2+1=0$

Now one will find the roots of this equation:

${\mathrm{r}}^4+2{\mathrm{r}}^2+1=0⇔{({\mathrm{r}}^2+1)}^2=0$

$\begin{array}{c}{\mathrm{r}}^2+1=0\\ {\mathrm{r}}^2=-1\\ {\mathrm{r}}_{1,2}=Â\pm \mathrm{i}\end{array}$

These roots are both repeated. Similarly, to the procedure when repeated roots are not complex, one has that the general solution is:

$\begin{array}{c}\mathrm{y}\left(\mathrm{t}\right)={\mathrm{c}}_1{\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{³¦´Ç²õβ³Ù}+{\mathrm{c}}_3{\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{²õ¾\pm ²Ôβ³Ù}+\mathrm{t}({\mathrm{c}}_2{\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{³¦´Ç²õβ³Ù}+{\mathrm{c}}_4{\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{²õ¾\pm ²Ôβ³Ù})\\ \mathrm{y}\left(\mathrm{t}\right)=({\mathrm{c}}_1+{\mathrm{c}}_2\mathrm{t}){\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{³¦´Ç²õβ³Ù}+({\mathrm{c}}_3+{\mathrm{c}}_4\mathrm{t}){\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{²õ¾\pm ²Ôβ³Ù}\end{array}$

Where ${\mathrm{r}}_{1,2}=\mathrm{Î\pm }Â\pm \mathrm{β¾\pm }$. In this case $\mathrm{Î\pm }=0$ and$\mathrm{β}=1$ , so the general solution of the given differential equation is$\mathrm{y}\left(\mathrm{t}\right)=({\mathrm{c}}_1+{\mathrm{c}}_2\mathrm{t})\mathrm{cost}+({\mathrm{c}}_3+{\mathrm{c}}_4\mathrm{t})\mathrm{sint}$ .

The differential equation is$\mathrm{y}\text{'}\text{'}\text{'}\text{'}+4\mathrm{y}\text{'}\text{'}\text{'}+12\mathrm{y}\text{'}\text{'}+16\mathrm{y}\text{'}+16\mathrm{y}=0.$

The auxiliary equation is: ${\mathrm{r}}^4+4{\mathrm{r}}^3+12{\mathrm{r}}^2+16\mathrm{r}+16=0$

Let’s solve this:

$\begin{array}{c}{\mathrm{r}}^4+4{\mathrm{r}}^3+12{\mathrm{r}}^2+16\mathrm{r}+16=0\\ {({\mathrm{r}}^2+2\mathrm{r}+4)}^2=0\end{array}$

role="math" localid="1654854846964" $\begin{array}{c}{\mathrm{r}}^2+2\mathrm{r}+4=0\\ {\mathrm{r}}_{1,2}=\frac{-2Â\pm \sqrt{4-16}}{2}\\ {\mathrm{r}}_{1,2}=-1Â\pm \sqrt{3}\mathrm{i}\end{array}$

As before, those roots are repeated, so the general solution is:$\mathrm{y}\left(\mathrm{t}\right)=({\mathrm{c}}_1+{\mathrm{c}}_2\mathrm{t}){\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{³¦´Ç²õβ³Ù}+({\mathrm{c}}_3+{\mathrm{c}}_4\mathrm{t}){\mathrm{e}}^{\mathrm{Î\pm ³Ù}}\mathrm{²õ¾\pm ²Ôβ³Ù}$

Where ${\mathrm{r}}_{1,2}=\mathrm{Î\pm }Â\pm \mathrm{β¾\pm }$. In this case $\mathrm{Î\pm }=-1$ and$\mathrm{β}=\sqrt{3}$ , so the general solution of the given differential equation is $\mathrm{y}\left(\mathrm{t}\right)=({\mathrm{c}}_1+{\mathrm{c}}_2\mathrm{t}){\mathrm{e}}^{-\mathrm{t}}\cos \sqrt{3}\mathrm{t}+({\mathrm{c}}_3+{\mathrm{c}}_4\mathrm{t}){\mathrm{e}}^{-\mathrm{t}}\sin \sqrt{3}\mathrm{t}$.