Internal problem ID [11773]
Internal file name [OUTPUT/11783_Thursday_April_11_2024_08_49_37_PM_9949308/index.tex
]
Book: Differential Equations by Shepley L. Ross. Third edition. John Willey. New Delhi.
2004.
Section: Chapter 4, Section 4.2. The homogeneous linear equation with constant coefficients.
Exercises page 135
Problem number: 46.
ODE order: 4.
ODE degree: 1.
The type(s) of ODE detected by this program : "higher_order_linear_constant_coefficients_ODE"
Maple gives the following as the ode type
[[_high_order, _missing_x]]
\[ \boxed {y^{\prime \prime \prime \prime }+3 y^{\prime \prime \prime }+y^{\prime \prime }+13 y^{\prime }+30 y=0} \] The characteristic equation is \[ \lambda ^{4}+3 \lambda ^{3}+\lambda ^{2}+13 \lambda +30 = 0 \] The roots of the above equation are \begin {align*} \lambda _1 &= -3\\ \lambda _2 &= -2\\ \lambda _3 &= 1-2 i\\ \lambda _4 &= 1+2 i \end {align*}
Therefore the homogeneous solution is \[ y_h(x)=c_{1} {\mathrm e}^{-2 x}+c_{2} {\mathrm e}^{-3 x}+{\mathrm e}^{\left (1-2 i\right ) x} c_{3} +{\mathrm e}^{\left (1+2 i\right ) x} c_{4} \] The fundamental set of solutions for the homogeneous solution are the following \begin {align*} y_1 &= {\mathrm e}^{-2 x}\\ y_2 &= {\mathrm e}^{-3 x}\\ y_3 &= {\mathrm e}^{\left (1-2 i\right ) x}\\ y_4 &= {\mathrm e}^{\left (1+2 i\right ) x} \end {align*}
Summary
The solution(s) found are the following \begin{align*} \tag{1} y &= c_{1} {\mathrm e}^{-2 x}+c_{2} {\mathrm e}^{-3 x}+{\mathrm e}^{\left (1-2 i\right ) x} c_{3} +{\mathrm e}^{\left (1+2 i\right ) x} c_{4} \\ \end{align*}
Verification of solutions
\[ y = c_{1} {\mathrm e}^{-2 x}+c_{2} {\mathrm e}^{-3 x}+{\mathrm e}^{\left (1-2 i\right ) x} c_{3} +{\mathrm e}^{\left (1+2 i\right ) x} c_{4} \] Verified OK.
\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & y^{\prime \prime \prime \prime }+3 y^{\prime \prime \prime }+y^{\prime \prime }+13 y^{\prime }+30 y=0 \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 4 \\ {} & {} & y^{\prime \prime \prime \prime } \\ \square & {} & \textrm {Convert linear ODE into a system of first order ODEs}\hspace {3pt} \\ {} & \circ & \textrm {Define new variable}\hspace {3pt} y_{1}\left (x \right ) \\ {} & {} & y_{1}\left (x \right )=y \\ {} & \circ & \textrm {Define new variable}\hspace {3pt} y_{2}\left (x \right ) \\ {} & {} & y_{2}\left (x \right )=y^{\prime } \\ {} & \circ & \textrm {Define new variable}\hspace {3pt} y_{3}\left (x \right ) \\ {} & {} & y_{3}\left (x \right )=y^{\prime \prime } \\ {} & \circ & \textrm {Define new variable}\hspace {3pt} y_{4}\left (x \right ) \\ {} & {} & y_{4}\left (x \right )=y^{\prime \prime \prime } \\ {} & \circ & \textrm {Isolate for}\hspace {3pt} y_{4}^{\prime }\left (x \right )\hspace {3pt}\textrm {using original ODE}\hspace {3pt} \\ {} & {} & y_{4}^{\prime }\left (x \right )=-3 y_{4}\left (x \right )-y_{3}\left (x \right )-13 y_{2}\left (x \right )-30 y_{1}\left (x \right ) \\ & {} & \textrm {Convert linear ODE into a system of first order ODEs}\hspace {3pt} \\ {} & {} & \left [y_{2}\left (x \right )=y_{1}^{\prime }\left (x \right ), y_{3}\left (x \right )=y_{2}^{\prime }\left (x \right ), y_{4}\left (x \right )=y_{3}^{\prime }\left (x \right ), y_{4}^{\prime }\left (x \right )=-3 y_{4}\left (x \right )-y_{3}\left (x \right )-13 y_{2}\left (x \right )-30 y_{1}\left (x \right )\right ] \\ \bullet & {} & \textrm {Define vector}\hspace {3pt} \\ {} & {} & {\moverset {\rightarrow }{y}}\left (x \right )=\left [\begin {array}{c} y_{1}\left (x \right ) \\ y_{2}\left (x \right ) \\ y_{3}\left (x \right ) \\ y_{4}\left (x \right ) \end {array}\right ] \\ \bullet & {} & \textrm {System to solve}\hspace {3pt} \\ {} & {} & {\moverset {\rightarrow }{y}}^{\prime }\left (x \right )=\left [\begin {array}{cccc} 0 & 1 & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \\ -30 & -13 & -1 & -3 \end {array}\right ]\cdot {\moverset {\rightarrow }{y}}\left (x \right ) \\ \bullet & {} & \textrm {Define the coefficient matrix}\hspace {3pt} \\ {} & {} & A =\left [\begin {array}{cccc} 0 & 1 & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \\ -30 & -13 & -1 & -3 \end {array}\right ] \\ \bullet & {} & \textrm {Rewrite the system as}\hspace {3pt} \\ {} & {} & {\moverset {\rightarrow }{y}}^{\prime }\left (x \right )=A \cdot {\moverset {\rightarrow }{y}}\left (x \right ) \\ \bullet & {} & \textrm {To solve the system, find the eigenvalues and eigenvectors of}\hspace {3pt} A \\ \bullet & {} & \textrm {Eigenpairs of}\hspace {3pt} A \\ {} & {} & \left [\left [-3, \left [\begin {array}{c} -\frac {1}{27} \\ \frac {1}{9} \\ -\frac {1}{3} \\ 1 \end {array}\right ]\right ], \left [-2, \left [\begin {array}{c} -\frac {1}{8} \\ \frac {1}{4} \\ -\frac {1}{2} \\ 1 \end {array}\right ]\right ], \left [1-2 \,\mathrm {I}, \left [\begin {array}{c} -\frac {11}{125}-\frac {2 \,\mathrm {I}}{125} \\ -\frac {3}{25}+\frac {4 \,\mathrm {I}}{25} \\ \frac {1}{5}+\frac {2 \,\mathrm {I}}{5} \\ 1 \end {array}\right ]\right ], \left [1+2 \,\mathrm {I}, \left [\begin {array}{c} -\frac {11}{125}+\frac {2 \,\mathrm {I}}{125} \\ -\frac {3}{25}-\frac {4 \,\mathrm {I}}{25} \\ \frac {1}{5}-\frac {2 \,\mathrm {I}}{5} \\ 1 \end {array}\right ]\right ]\right ] \\ \bullet & {} & \textrm {Consider eigenpair}\hspace {3pt} \\ {} & {} & \left [-3, \left [\begin {array}{c} -\frac {1}{27} \\ \frac {1}{9} \\ -\frac {1}{3} \\ 1 \end {array}\right ]\right ] \\ \bullet & {} & \textrm {Solution to homogeneous system from eigenpair}\hspace {3pt} \\ {} & {} & {\moverset {\rightarrow }{y}}_{1}={\mathrm e}^{-3 x}\cdot \left [\begin {array}{c} -\frac {1}{27} \\ \frac {1}{9} \\ -\frac {1}{3} \\ 1 \end {array}\right ] \\ \bullet & {} & \textrm {Consider eigenpair}\hspace {3pt} \\ {} & {} & \left [-2, \left [\begin {array}{c} -\frac {1}{8} \\ \frac {1}{4} \\ -\frac {1}{2} \\ 1 \end {array}\right ]\right ] \\ \bullet & {} & \textrm {Solution to homogeneous system from eigenpair}\hspace {3pt} \\ {} & {} & {\moverset {\rightarrow }{y}}_{2}={\mathrm e}^{-2 x}\cdot \left [\begin {array}{c} -\frac {1}{8} \\ \frac {1}{4} \\ -\frac {1}{2} \\ 1 \end {array}\right ] \\ \bullet & {} & \textrm {Consider complex eigenpair, complex conjugate eigenvalue can be ignored}\hspace {3pt} \\ {} & {} & \left [1-2 \,\mathrm {I}, \left [\begin {array}{c} -\frac {11}{125}-\frac {2 \,\mathrm {I}}{125} \\ -\frac {3}{25}+\frac {4 \,\mathrm {I}}{25} \\ \frac {1}{5}+\frac {2 \,\mathrm {I}}{5} \\ 1 \end {array}\right ]\right ] \\ \bullet & {} & \textrm {Solution from eigenpair}\hspace {3pt} \\ {} & {} & {\mathrm e}^{\left (1-2 \,\mathrm {I}\right ) x}\cdot \left [\begin {array}{c} -\frac {11}{125}-\frac {2 \,\mathrm {I}}{125} \\ -\frac {3}{25}+\frac {4 \,\mathrm {I}}{25} \\ \frac {1}{5}+\frac {2 \,\mathrm {I}}{5} \\ 1 \end {array}\right ] \\ \bullet & {} & \textrm {Use Euler identity to write solution in terms of}\hspace {3pt} \sin \hspace {3pt}\textrm {and}\hspace {3pt} \cos \\ {} & {} & {\mathrm e}^{x}\cdot \left (\cos \left (2 x \right )-\mathrm {I} \sin \left (2 x \right )\right )\cdot \left [\begin {array}{c} -\frac {11}{125}-\frac {2 \,\mathrm {I}}{125} \\ -\frac {3}{25}+\frac {4 \,\mathrm {I}}{25} \\ \frac {1}{5}+\frac {2 \,\mathrm {I}}{5} \\ 1 \end {array}\right ] \\ \bullet & {} & \textrm {Simplify expression}\hspace {3pt} \\ {} & {} & {\mathrm e}^{x}\cdot \left [\begin {array}{c} \left (-\frac {11}{125}-\frac {2 \,\mathrm {I}}{125}\right ) \left (\cos \left (2 x \right )-\mathrm {I} \sin \left (2 x \right )\right ) \\ \left (-\frac {3}{25}+\frac {4 \,\mathrm {I}}{25}\right ) \left (\cos \left (2 x \right )-\mathrm {I} \sin \left (2 x \right )\right ) \\ \left (\frac {1}{5}+\frac {2 \,\mathrm {I}}{5}\right ) \left (\cos \left (2 x \right )-\mathrm {I} \sin \left (2 x \right )\right ) \\ \cos \left (2 x \right )-\mathrm {I} \sin \left (2 x \right ) \end {array}\right ] \\ \bullet & {} & \textrm {Both real and imaginary parts are solutions to the homogeneous system}\hspace {3pt} \\ {} & {} & \left [{\moverset {\rightarrow }{y}}_{3}\left (x \right )={\mathrm e}^{x}\cdot \left [\begin {array}{c} -\frac {11 \cos \left (2 x \right )}{125}-\frac {2 \sin \left (2 x \right )}{125} \\ -\frac {3 \cos \left (2 x \right )}{25}+\frac {4 \sin \left (2 x \right )}{25} \\ \frac {\cos \left (2 x \right )}{5}+\frac {2 \sin \left (2 x \right )}{5} \\ \cos \left (2 x \right ) \end {array}\right ], {\moverset {\rightarrow }{y}}_{4}\left (x \right )={\mathrm e}^{x}\cdot \left [\begin {array}{c} \frac {11 \sin \left (2 x \right )}{125}-\frac {2 \cos \left (2 x \right )}{125} \\ \frac {3 \sin \left (2 x \right )}{25}+\frac {4 \cos \left (2 x \right )}{25} \\ -\frac {\sin \left (2 x \right )}{5}+\frac {2 \cos \left (2 x \right )}{5} \\ -\sin \left (2 x \right ) \end {array}\right ]\right ] \\ \bullet & {} & \textrm {General solution to the system of ODEs}\hspace {3pt} \\ {} & {} & {\moverset {\rightarrow }{y}}=c_{1} {\moverset {\rightarrow }{y}}_{1}+c_{2} {\moverset {\rightarrow }{y}}_{2}+c_{3} {\moverset {\rightarrow }{y}}_{3}\left (x \right )+c_{4} {\moverset {\rightarrow }{y}}_{4}\left (x \right ) \\ \bullet & {} & \textrm {Substitute solutions into the general solution}\hspace {3pt} \\ {} & {} & {\moverset {\rightarrow }{y}}=c_{1} {\mathrm e}^{-3 x}\cdot \left [\begin {array}{c} -\frac {1}{27} \\ \frac {1}{9} \\ -\frac {1}{3} \\ 1 \end {array}\right ]+c_{2} {\mathrm e}^{-2 x}\cdot \left [\begin {array}{c} -\frac {1}{8} \\ \frac {1}{4} \\ -\frac {1}{2} \\ 1 \end {array}\right ]+c_{3} {\mathrm e}^{x}\cdot \left [\begin {array}{c} -\frac {11 \cos \left (2 x \right )}{125}-\frac {2 \sin \left (2 x \right )}{125} \\ -\frac {3 \cos \left (2 x \right )}{25}+\frac {4 \sin \left (2 x \right )}{25} \\ \frac {\cos \left (2 x \right )}{5}+\frac {2 \sin \left (2 x \right )}{5} \\ \cos \left (2 x \right ) \end {array}\right ]+{\mathrm e}^{x} c_{4} \cdot \left [\begin {array}{c} \frac {11 \sin \left (2 x \right )}{125}-\frac {2 \cos \left (2 x \right )}{125} \\ \frac {3 \sin \left (2 x \right )}{25}+\frac {4 \cos \left (2 x \right )}{25} \\ -\frac {\sin \left (2 x \right )}{5}+\frac {2 \cos \left (2 x \right )}{5} \\ -\sin \left (2 x \right ) \end {array}\right ] \\ \bullet & {} & \textrm {First component of the vector is the solution to the ODE}\hspace {3pt} \\ {} & {} & y=-\frac {2 \left (\left (\left (\frac {11 c_{3}}{2}+c_{4} \right ) \cos \left (2 x \right )+\sin \left (2 x \right ) \left (c_{3} -\frac {11 c_{4}}{2}\right )\right ) {\mathrm e}^{4 x}+\frac {125 c_{2} {\mathrm e}^{x}}{16}+\frac {125 c_{1}}{54}\right ) {\mathrm e}^{-3 x}}{125} \end {array} \]
Maple trace
`Methods for high order ODEs: --- Trying classification methods --- trying a quadrature checking if the LODE has constant coefficients <- constant coefficients successful`
✓ Solution by Maple
Time used: 0.0 (sec). Leaf size: 35
dsolve(diff(y(x),x$4)+3*diff(y(x),x$3)+diff(y(x),x$2)+13*diff(y(x),x)+30*y(x)=0,y(x), singsol=all)
\[ y \left (x \right ) = \left (c_{3} {\mathrm e}^{4 x} \sin \left (2 x \right )+c_{4} {\mathrm e}^{4 x} \cos \left (2 x \right )+c_{2} {\mathrm e}^{x}+c_{1} \right ) {\mathrm e}^{-3 x} \]
✓ Solution by Mathematica
Time used: 0.003 (sec). Leaf size: 43
DSolve[y''''[x]+3*y'''[x]+y''[x]+13*y'[x]+30*y[x]==0,y[x],x,IncludeSingularSolutions -> True]
\[ y(x)\to c_2 e^x \cos (2 x)+e^{-3 x} \left (c_4 e^x+c_1 e^{4 x} \sin (2 x)+c_3\right ) \]