Below are the solutions to the Module 3 Homework Assignment for Second-Order Differential Equations. Prior to these solutions, let’s recall a few important things that I’ll have to refer back to periodically.
An n-th order Linear Differential Equation will always have the form of
\[ b_n(x)y^{(n)}+b_{n-1}(x)y^{(n-1)} + \cdots + b_2(x)y^{''}+b_1(x)y^{'} + b_0(x)y=g(x) \]
This is for 1st order, 2nd order, 3rd order, and so on. In this case, \(g(x)\) and the coefficients \(b_j(x)\) where \(j=0,1,2,\ldots, n\) depend solely on \(x\). In other words, they do not depend whatsoever on \(y\) or and derivative of \(y\).
If then the above equation is Homogeneous. If it's not, then it's Non-Homogeneous.
Once you derive your characteristic equation, then you have three possible cases for your General Solution
Two linearly independent solutions are \(e^{\lambda_1x}\) and \(e^{\lambda_2x}\) and the general solution is given by
\[ y=c_1 e^{\lambda_1x} +c_2e^{\lambda_2x} \]
In the special case that , the solution above can be written as
Since \(a_1\) and \(a_0\) are assumed to be real in your characteristic equation, the roots of the characteristic equation must appear in conjugate pairs. Therefore, the other root is \(\lambda_2=a-bi\) . Two linearly independent solutions are \(e^{(a+bi)x}\) and \(e^{(a-bi)x}\) and the general complex solution would be
\[y=d_1e^{(a+bi)x} + d_2e^{(a-bi)x} \]
which, is equivalent to a different form that some of us are used to seeing
\[ y=c_1e^{ax} \cos bx + c_2e^{ax} \sin bx \]
Two linearly independent solutions are \(e^{\lambda_1x}\) and \(xe^{\lambda_1x}\) and the general solution is given by
\[ y=c_1e^{\lambda_1x}+c_2xe^{\lambda_1x} \]
These cases are not valid if the DE is not linear or does not have constant coefficients.
Solve \[\ddot{x}-0.01x=0\]
The characteristic equation is
\[ \lambda^2-0.01=0 \]
This equation can be factored into
\[ (\lambda-0.1)(\lambda+0.1)=0 \]
By using Algebra, the roots for this equation are \(\lambda_1=0.1\) and \(\lambda_2=-0.1\). Note, they are real numbers and distinct. Therefore, the general solution to this equation would be
\[ y=c_1e^{0.1t}+c_2e^{-0.1t} \]
or, if you want to use the special case version, we have:
\[ y=c_1 \cosh 0.1t + c_2 \sinh 0.1t \]
Solve
\[ y''+4y'+5y=0 \]
The characteristic equation is
\[ \lambda^2+4\lambda+5=0 \]
Once we break out the good ’ole quadratic formula,
\[ \lambda = \frac{-b\pm \sqrt{b^2-4ac}}{2a} \]
We have
\[ \lambda = \frac{-4\pm \sqrt{4^2-4(1)(5)}}{2(1)} \]
which gives us the following roots \(-2 +i\) and \(-2-i\) or simply \(-2 \pm i\)
Remember from algebra, complex solutions are written in the form \(a\pm bi\) ? In this case, \(a=-2\) and \(b=1\) . Therefore, the general solution, because we have a complex pair of roots, is
\[ y=k_1e^{-2x}\cos x + k_2e^{-2x}\sin x \]
Solve
\[ y^{''}-3y'+4y=0 \]
First, find the characteristic equation, which is
\[ \lambda^2-3\lambda +4=0 \]
Using the quadratic formula to solve this quadratic equation, we get the following roots:
\[ \lambda = \frac{-(-3)\pm \sqrt{(-3)^2-4(1)(4)}}{2(1)} = \frac{3}{2}\pm \frac{\sqrt{7}}{2}i \]
Since \(a=\frac{3}{2}\) and \(b=\frac{\sqrt{7}}{2}\) and by using Case 2 above, we’ll have our general solution as:
\[ y=c_1e^{\frac{3}{2}x} \cos \frac{\sqrt{7}}{2} x + c_2e^{\frac{3}{2}x}\sin \frac{\sqrt{7}}{2}x \]
Solve
\[ \ddot{y}-6\dot{y}+25y=0 \]
First, the characteristic equation of this would be
\[ \lambda^2-6\lambda + 25 = 0 \]
Using the Quadratic Formula, yields our roots, which are
\[ \lambda = \frac{-(-6)\pm \sqrt{(-6)^2-4(1)(25)}}{2(1)} = 3\pm 4i \]
Since we have complex roots, our \(a=3\) and \(b=4\), giving our general solution
\[ y=c_1e^{3t} \cos 4t + c_2e^{3t}\sin 4t \]
Solve
\[ \frac{d^2I}{dt^2}+20\frac{dI}{dt}+200I = 0 \]
First, find the characteristic equation. Even though it’s written in derivative form, we can still build our characteristic equation. Thus, we’ll have
\[ \lambda^2+20\lambda + 200=0 \]
Yet again, using the Quadratic formula to solve for \(\lambda\), we’ll get our roots, which are
\[ \lambda = \frac{-20\pm \sqrt{20^2-4(1)(200)}}{2(1)} = -10\pm 10i \]
Since we have a complex roots, our \(a = -10\) and \(b=10\). Therefore, our general solution would be
\[ I=c_1e^{-10t} \cos 10t + c_2e^{-10t}\sin 10t \]
Solve
\[ y^{(4)}-9y^{''}+20y=0 \]
Firstly, the characteristic equation would be
\[ \lambda^4-9\lambda + 20=0 \]
Using long division, synthetic division, or factoring (whichever you prefer), we get our roots to be
\[ x=\pm \sqrt{5} \text{ and } x = \pm 2 \]
Therefore, we have our general solution to be either one of the two below:
\[ \begin{eqnarray*} y&=&c_1e^{2x}+c_2e^{-2x}+c_3e^{\sqrt{5}x}+c_4e^{-\sqrt{5}x}\\ &&\\ y&=& k_1\cosh 2x + k_2 \sinh{2x}+k_3\cosh \sqrt{5}x + k_4\sinh \sqrt{5}x \end{eqnarray*} \]
Solve
\[ \frac{d^4x}{dt^4}-4\frac{d^3x}{dt^3}+7\frac{d^2x}{dt^2}-4\frac{dx}{dt}+6x=0 \]
The characteristic equation would be
\[ \lambda^4-4\lambda^3+7\lambda^2-4\lambda+6=0 \]
Using Synthetic Division to work this problem down into quadratic form, then using the quadratic formula, we obtain the roots
\[ \lambda_1=2+\sqrt{2}i, \hspace{3mm} \lambda_2=2-\sqrt{2}i, \hspace{3mm} \lambda_3=i, \hspace{3mm} \lambda_4=-i \]
Therefore, since we have complex roots, we have our general solution to be
\[ x=d_1e^{(2+\sqrt{2}i)t}+d_2e^{(2-\sqrt{2}i)t}+d_3e^{it}+d_4e^{-it} \]