2.1.76 Problem 76

Internal problem ID [10062]
Book : Own collection of miscellaneous problems
Section : section 1.0
Problem number : 76
Date solved : Monday, December 08, 2025 at 07:12:59 PM
CAS classification : system_of_ODEs

\begin{align*} x^{\prime }&=2 x+y-z \\ y^{\prime }&=-x+2 z \\ z^{\prime }&=-x-2 y+4 z \\ \end{align*}

Entering first order system solver

2.1.76.1 Solution using Matrix exponential method

In this method, we will assume we have found the matrix exponential \(e^{A t}\) allready. There are different methods to determine this but will not be shown here. This is a system of linear ODE’s given as

\begin{align*} \vec {x}'(t) &= A\, \vec {x}(t) \end{align*}

Or

\begin{align*} \left [\begin {array}{c} x^{\prime } \\ y^{\prime } \\ z^{\prime } \end {array}\right ] &= \left [\begin {array}{ccc} 2 & 1 & -1 \\ -1 & 0 & 2 \\ -1 & -2 & 4 \end {array}\right ]\, \left [\begin {array}{c} x \\ y \\ z \end {array}\right ] \end{align*}

For the above matrix \(A\), the matrix exponential can be found to be

\begin{align*} e^{A t} &= \left [\begin {array}{ccc} {\mathrm e}^{2 t} & t \,{\mathrm e}^{2 t} & -t \,{\mathrm e}^{2 t} \\ -t \,{\mathrm e}^{2 t} & {\mathrm e}^{2 t} \left (1-\frac {1}{2} t^{2}-2 t \right ) & \frac {{\mathrm e}^{2 t} t \left (t +4\right )}{2} \\ -t \,{\mathrm e}^{2 t} & -\frac {{\mathrm e}^{2 t} t \left (t +4\right )}{2} & {\mathrm e}^{2 t} \left (1+\frac {1}{2} t^{2}+2 t \right ) \end {array}\right ] \end{align*}

Therefore the homogeneous solution is

\begin{align*} \vec {x}_h(t) &= e^{A t} \vec {c} \\ &= \left [\begin {array}{ccc} {\mathrm e}^{2 t} & t \,{\mathrm e}^{2 t} & -t \,{\mathrm e}^{2 t} \\ -t \,{\mathrm e}^{2 t} & {\mathrm e}^{2 t} \left (1-\frac {1}{2} t^{2}-2 t \right ) & \frac {{\mathrm e}^{2 t} t \left (t +4\right )}{2} \\ -t \,{\mathrm e}^{2 t} & -\frac {{\mathrm e}^{2 t} t \left (t +4\right )}{2} & {\mathrm e}^{2 t} \left (1+\frac {1}{2} t^{2}+2 t \right ) \end {array}\right ] \left [\begin {array}{c} c_{1} \\ c_{2} \\ c_{3} \end {array}\right ] \\ &= \left [\begin {array}{c} {\mathrm e}^{2 t} c_{1}+t \,{\mathrm e}^{2 t} c_{2}-t \,{\mathrm e}^{2 t} c_{3} \\ -t \,{\mathrm e}^{2 t} c_{1}+{\mathrm e}^{2 t} \left (1-\frac {1}{2} t^{2}-2 t \right ) c_{2}+\frac {{\mathrm e}^{2 t} t \left (t +4\right ) c_{3}}{2} \\ -t \,{\mathrm e}^{2 t} c_{1}-\frac {{\mathrm e}^{2 t} t \left (t +4\right ) c_{2}}{2}+{\mathrm e}^{2 t} \left (1+\frac {1}{2} t^{2}+2 t \right ) c_{3} \end {array}\right ]\\ &= \left [\begin {array}{c} {\mathrm e}^{2 t} \left (\left (c_{2}-c_{3}\right ) t +c_{1}\right ) \\ -\frac {{\mathrm e}^{2 t} \left (\left (c_{2}-c_{3}\right ) t^{2}+\left (2 c_{1}+4 c_{2}-4 c_{3}\right ) t -2 c_{2}\right )}{2} \\ -\frac {{\mathrm e}^{2 t} \left (\left (c_{2}-c_{3}\right ) t^{2}+\left (2 c_{1}+4 c_{2}-4 c_{3}\right ) t -2 c_{3}\right )}{2} \end {array}\right ] \end{align*}

Since no forcing function is given, then the final solution is \(\vec {x}_h(t)\) above.

2.1.76.2 Solution using explicit Eigenvalue and Eigenvector method

This is a system of linear ODE’s given as

\begin{align*} \vec {x}'(t) &= A\, \vec {x}(t) \end{align*}

Or

\begin{align*} \left [\begin {array}{c} x^{\prime } \\ y^{\prime } \\ z^{\prime } \end {array}\right ] &= \left [\begin {array}{ccc} 2 & 1 & -1 \\ -1 & 0 & 2 \\ -1 & -2 & 4 \end {array}\right ]\, \left [\begin {array}{c} x \\ y \\ z \end {array}\right ] \end{align*}

The first step is find the homogeneous solution. We start by finding the eigenvalues of \(A\). This is done by solving the following equation for the eigenvalues \(\lambda \)

\begin{align*} \operatorname {det} \left ( A- \lambda I \right ) &= 0 \end{align*}

Expanding gives

\begin{align*} \operatorname {det} \left (\left [\begin {array}{ccc} 2 & 1 & -1 \\ -1 & 0 & 2 \\ -1 & -2 & 4 \end {array}\right ]-\lambda \left [\begin {array}{ccc} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end {array}\right ]\right ) &= 0 \end{align*}

Therefore

\begin{align*} \operatorname {det} \left (\left [\begin {array}{ccc} 2-\lambda & 1 & -1 \\ -1 & -\lambda & 2 \\ -1 & -2 & 4-\lambda \end {array}\right ]\right ) &= 0 \end{align*}

Which gives the characteristic equation

\begin{align*} \lambda ^{3}-6 \lambda ^{2}+12 \lambda -8&=0 \end{align*}

The roots of the above are the eigenvalues.

\begin{align*} \lambda _1 &= 2 \end{align*}

This table summarises the above result

eigenvalue	algebraic multiplicity	type of eigenvalue
\(2\)	\(1\)	real eigenvalue

Now the eigenvector for each eigenvalue are found.

Considering the eigenvalue \(\lambda _{1} = 2\)

We need to solve \(A \vec {v} = \lambda \vec {v}\) or \((A-\lambda I) \vec {v} = \vec {0}\) which becomes

\begin{align*} \left (\left [\begin {array}{ccc} 2 & 1 & -1 \\ -1 & 0 & 2 \\ -1 & -2 & 4 \end {array}\right ] - \left (2\right ) \left [\begin {array}{ccc} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end {array}\right ]\right ) \left [\begin {array}{c} v_{1} \\ v_{2} \\ v_{3} \end {array}\right ]&=\left [\begin {array}{c} 0 \\ 0 \\ 0 \end {array}\right ]\\ \left [\begin {array}{ccc} 0 & 1 & -1 \\ -1 & -2 & 2 \\ -1 & -2 & 2 \end {array}\right ] \left [\begin {array}{c} v_{1} \\ v_{2} \\ v_{3} \end {array}\right ]&=\left [\begin {array}{c} 0 \\ 0 \\ 0 \end {array}\right ] \end{align*}

Now forward elimination is applied to solve for the eigenvector \(\vec {v}\). The augmented matrix is

\[ \left [\begin {array}{@{}ccc!{\ifdefined \HCode |\else \color {red}\vline width 0.6pt\fi }c@{}} 0&1&-1&0\\ -1&-2&2&0\\ -1&-2&2&0 \end {array} \right ] \]

Since the current pivot \(A(1,1)\) is zero, then the current pivot row is replaced with a row with a non-zero pivot. Swapping row \(1\) and row \(2\) gives

\[ \left [\begin {array}{@{}ccc!{\ifdefined \HCode |\else \color {red}\vline width 0.6pt\fi }c@{}} -1&-2&2&0\\ 0&1&-1&0\\ -1&-2&2&0 \end {array} \right ] \]

\begin{align*} R_{3} = R_{3}-R_{1} &\Longrightarrow \hspace {5pt}\left [\begin {array}{@{}ccc!{\ifdefined \HCode |\else \color {red}\vline width 0.6pt\fi }c@{}} -1&-2&2&0\\ 0&1&-1&0\\ 0&0&0&0 \end {array} \right ] \end{align*}

Therefore the system in Echelon form is

\[ \left [\begin {array}{ccc} -1 & -2 & 2 \\ 0 & 1 & -1 \\ 0 & 0 & 0 \end {array}\right ] \left [\begin {array}{c} v_{1} \\ v_{2} \\ v_{3} \end {array}\right ] = \left [\begin {array}{c} 0 \\ 0 \\ 0 \end {array}\right ] \]

The free variables are \(\{v_{3}\}\) and the leading variables are \(\{v_{1}, v_{2}\}\). Let \(v_{3} = t\). Now we start back substitution. Solving the above equation for the leading variables in terms of free variables gives equation \(\{v_{1} = 0, v_{2} = t\}\)

Hence the solution is

\[ \left [\begin {array}{c} v_{1} \\ v_{2} \\ t \end {array}\right ] = \left [\begin {array}{c} 0 \\ t \\ t \end {array}\right ] \]

Since there is one free Variable, we have found one eigenvector associated with this eigenvalue. The above can be written as

\[ \left [\begin {array}{c} v_{1} \\ v_{2} \\ t \end {array}\right ] = t \left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ] \]

Let \(t = 1\) the eigenvector becomes

\[ \left [\begin {array}{c} v_{1} \\ v_{2} \\ t \end {array}\right ] = \left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ] \]

The following table gives a summary of this result. It shows for each eigenvalue the algebraic multiplicity \(m\), and its geometric multiplicity \(k\) and the eigenvectors associated with the eigenvalue. If \(m>k\) then the eigenvalue is defective which means the number of normal linearly independent eigenvectors associated with this eigenvalue (called the geometric multiplicity \(k\)) does not equal the algebraic multiplicity \(m\), and we need to determine an additional \(m-k\) generalized eigenvectors for this eigenvalue.

	multiplicity
eigenvalue	algebraic \(m\)	geometric \(k\)	defective?	eigenvectors
\(2\)	\(3\)	\(1\)	Yes	\(\left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ]\)

Now that we found the eigenvalues and associated eigenvectors, we will go over each eigenvalue and generate the solution basis. The only problem we need to take care of is if the eigenvalue is defective. eigenvalue \(2\) is real and repated eigenvalue of multiplicity \(3\).There are three possible cases that can happen. This is illustrated in this diagram

Figure 2.162: Possible case for repeated \(\lambda \) of multiplicity 3

This eigenvalue has algebraic multiplicity of \(3\), and geometric multiplicity \(1\), therefore this is defective eigenvalue. The defect is \(2\). This falls into case \(3\) shown above. First we find generalized eigenvector \(\vec {v}_2\) of rank 2 and then use this to find generalized eigenvector \(\vec {v}_3\) of rank \(3\).\(\vec {v}_2\) is found by solving

\[ \left ( A-\lambda I \right ) \vec {v}_2 = \vec {v}_1 \]

Where \( \vec {v}_1\) is the normal (rank 1) eigenvector found above. Hence

\begin{align*} \left (\left [\begin {array}{ccc} 2 & 1 & -1 \\ -1 & 0 & 2 \\ -1 & -2 & 4 \end {array}\right ]- \left (2\right )\left [\begin {array}{ccc} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end {array}\right ]\right )\left [\begin {array}{c} v_{1} \\ v_{2} \\ v_{3} \end {array}\right ] &= \left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ]\\ \left [\begin {array}{ccc} 0 & 1 & -1 \\ -1 & -2 & 2 \\ -1 & -2 & 2 \end {array}\right ] \left [\begin {array}{c} v_{1} \\ v_{2} \\ v_{3} \end {array}\right ] &= \left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ] \end{align*}

Solving for \(\vec {v}_2\) gives

\[ \vec {v}_2 = \left [\begin {array}{c} -1 \\ 1 \\ 1 \end {array}\right ] \]

Now \(\vec {v}_3\) is found by solving

\[ \left ( A-\lambda I \right ) \vec {v}_3 = \vec {v}_2 \]

Where \( \vec {v}_2\) is the (rank 2) generalized eigenvector found above. Hence

\begin{align*} \left (\left [\begin {array}{ccc} 2 & 1 & -1 \\ -1 & 0 & 2 \\ -1 & -2 & 4 \end {array}\right ]- \left (2\right )\left [\begin {array}{ccc} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end {array}\right ]\right )\left [\begin {array}{c} v_{1} \\ v_{2} \\ v_{3} \end {array}\right ] &= \left [\begin {array}{c} -1 \\ 1 \\ 1 \end {array}\right ]\\ \left [\begin {array}{ccc} 0 & 1 & -1 \\ -1 & -2 & 2 \\ -1 & -2 & 2 \end {array}\right ] \left [\begin {array}{c} v_{1} \\ v_{2} \\ v_{3} \end {array}\right ] &= \left [\begin {array}{c} -1 \\ 1 \\ 1 \end {array}\right ] \end{align*}

Solving for \(\vec {v}_3\) gives

\[ \vec {v}_3 = \left [\begin {array}{c} 1 \\ 0 \\ 1 \end {array}\right ] \]

We have found three generalized eigenvectors for eigenvalue \(2\). Therefore the three basis solutions associated with this eigenvalue are

\begin{align*} \vec {x}_1(t) &= \vec {v}_1 e^{\lambda t}\\ &= \left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ] {\mathrm e}^{2 t}\\ &= \left [\begin {array}{c} 0 \\ {\mathrm e}^{2 t} \\ {\mathrm e}^{2 t} \end {array}\right ] \end{align*}

And

\begin{align*} \vec {x}_2(t) &= e^{\lambda t} \left (\vec {v}_1 t + \vec {v}_2\right ) \\ &= {\mathrm e}^{2 t}\left (\left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ] t + \left [\begin {array}{c} -1 \\ 1 \\ 1 \end {array}\right ]\right ) \\ &= \left [\begin {array}{c} -{\mathrm e}^{2 t} \\ {\mathrm e}^{2 t} \left (t +1\right ) \\ {\mathrm e}^{2 t} \left (t +1\right ) \end {array}\right ] \end{align*}

And

\begin{align*} \vec {x}_3(t) &=\left ( \vec {v}_1 \frac {t^{2}}{2} + \vec {v}_2 t + \vec {v}_3 \right ) e^{\lambda t} \\ &= \left (\left [\begin {array}{c} 0 \\ 1 \\ 1 \end {array}\right ] \frac {t^{2}}{2} + \left [\begin {array}{c} -1 \\ 1 \\ 1 \end {array}\right ] t + \left [\begin {array}{c} 1 \\ 0 \\ 1 \end {array}\right ] \right ) {\mathrm e}^{2 t} \\ &=\left [\begin {array}{c} {\mathrm e}^{2 t} \left (1-t \right ) \\ \frac {{\mathrm e}^{2 t} t \left (t +2\right )}{2} \\ {\mathrm e}^{2 t} \left (\frac {1}{2} t^{2}+t +1\right ) \end {array}\right ] \end{align*}

Therefore the final solution is

\begin{align*} \vec {x}_h(t) &= c_{1} \vec {x}_{1}(t) + c_{2} \vec {x}_{2}(t) + c_{3} \vec {x}_{3}(t) \end{align*}

Which is written as

\begin{align*} \left [\begin {array}{c} x \\ y \\ z \end {array}\right ] &= c_{1} \left [\begin {array}{c} 0 \\ {\mathrm e}^{2 t} \\ {\mathrm e}^{2 t} \end {array}\right ] + c_{2} \left [\begin {array}{c} -{\mathrm e}^{2 t} \\ {\mathrm e}^{2 t} \left (t +1\right ) \\ {\mathrm e}^{2 t} \left (t +1\right ) \end {array}\right ] + c_{3} \left [\begin {array}{c} {\mathrm e}^{2 t} \left (1-t \right ) \\ {\mathrm e}^{2 t} \left (\frac {1}{2} t^{2}+t \right ) \\ {\mathrm e}^{2 t} \left (\frac {1}{2} t^{2}+t +1\right ) \end {array}\right ] \end{align*}

Which becomes

\begin{align*} \left [\begin {array}{c} x \\ y \\ z \end {array}\right ] = \left [\begin {array}{c} -{\mathrm e}^{2 t} \left (\left (t -1\right ) c_3 +c_2 \right ) \\ \frac {\left (c_3 \,t^{2}+\left (2 c_2 +2 c_3 \right ) t +2 c_1 +2 c_2 \right ) {\mathrm e}^{2 t}}{2} \\ \frac {\left (c_3 \left (t^{2}+2 t +2\right )+2 c_2 t +2 c_1 +2 c_2 \right ) {\mathrm e}^{2 t}}{2} \end {array}\right ] \end{align*}

2.1.76.3 ✓ Maple. Time used: 0.069 (sec). Leaf size: 58

ode:=[diff(x(t),t) = 2*x(t)+y(t)-z(t), diff(y(t),t) = -x(t)+2*z(t), diff(z(t),t) = -x(t)-2*y(t)+4*z(t)]; 
dsolve(ode);
 

\begin{align*} x \left (t \right ) &= -{\mathrm e}^{2 t} \left (2 c_3 t +c_2 -4 c_3 \right ) \\ y \left (t \right ) &= {\mathrm e}^{2 t} \left (c_3 \,t^{2}+c_2 t +c_1 \right ) \\ z \left (t \right ) &= {\mathrm e}^{2 t} \left (c_3 \,t^{2}+c_2 t +c_1 +2 c_3 \right ) \\ \end{align*}

2.1.76.4 ✓ Mathematica. Time used: 0.003 (sec). Leaf size: 107

ode={D[x[t],t]== 2*x[t]+y[t]-z[t],D[y[t],t] == -x[t]+2*z[t],D[z[t],t]==-x[t]-2*y[t]+4*z[t]}; 
ic={}; 
DSolve[{ode,ic},{x[t],y[t],z[t]},t,IncludeSingularSolutions->True]
 

\begin{align*} x(t)&\to e^{2 t} ((c_2-c_3) t+c_1)\\ y(t)&\to -\frac {1}{2} e^{2 t} \left ((c_2-c_3) t^2+2 (c_1+2 c_2-2 c_3) t-2 c_2\right )\\ z(t)&\to -\frac {1}{2} e^{2 t} \left ((c_2-c_3) t^2+2 (c_1+2 c_2-2 c_3) t-2 c_3\right ) \end{align*}

2.1.76.5 ✓ Sympy. Time used: 0.099 (sec). Leaf size: 94

from sympy import * 
t = symbols("t") 
x = Function("x") 
y = Function("y") 
z = Function("z") 
ode=[Eq(-2*x(t) - y(t) + z(t) + Derivative(x(t), t),0),Eq(x(t) - 2*z(t) + Derivative(y(t), t),0),Eq(x(t) + 2*y(t) - 4*z(t) + Derivative(z(t), t),0)] 
ics = {} 
dsolve(ode,func=[x(t),y(t),z(t)],ics=ics)
 

\[ \left [ x{\left (t \right )} = C_{1} e^{2 t} + C_{2} t e^{2 t}, \ y{\left (t \right )} = - \frac {C_{2} t^{2} e^{2 t}}{2} - t \left (C_{1} + 2 C_{2}\right ) e^{2 t} - \left (2 C_{1} - C_{2} + C_{3}\right ) e^{2 t}, \ z{\left (t \right )} = - \frac {C_{2} t^{2} e^{2 t}}{2} - t \left (C_{1} + 2 C_{2}\right ) e^{2 t} - \left (2 C_{1} + C_{3}\right ) e^{2 t}\right ] \]