Internal problem ID [5700]
Internal file name [OUTPUT/4948_Sunday_June_05_2022_03_11_28_PM_98332360/index.tex]
Book: ADVANCED ENGINEERING MATHEMATICS. ERWIN KREYSZIG, HERBERT
KREYSZIG, EDWARD J. NORMINTON. 10th edition. John Wiley USA. 2011
Section: Chapter 6. Laplace Transforms. Problem set 6.3, page 224
Problem number: 24.
ODE order: 2.
ODE degree: 1.
The type(s) of ODE detected by this program : "second_order_laplace", "second_order_linear_constant_coeff"
Maple gives the following as the ode type
[[_2nd_order, _linear, _nonhomogeneous]]
\[
\boxed {y^{\prime \prime }+3 y^{\prime }+2 y=\left \{\begin {array}{cc} 1 & 0
This is a linear ODE. In canonical form it is written as \begin {align*} y^{\prime \prime } + p(t)y^{\prime } + q(t) y &= F \end {align*}
Where here \begin {align*} p(t) &=3\\ q(t) &=2\\ F &=\left \{\begin {array}{cc} 0 & t \le 0 \\ 1 & t <1 \\ 0 & 1\le t \end {array}\right . \end {align*}
Hence the ode is \begin {align*} y^{\prime \prime }+3 y^{\prime }+2 y = \left \{\begin {array}{cc} 0 & t \le 0 \\ 1 & t <1 \\ 0 & 1\le t \end {array}\right . \end {align*}
The domain of \(p(t)=3\) is \[
\{-\infty Solving using the Laplace transform method. Let \begin {align*} \mathcal {L}\left (y\right ) =Y(s) \end {align*}
Taking the Laplace transform of the ode and using the relations that \begin {align*} \mathcal {L}\left (y^{\prime }\right ) &= s Y(s) - y \left (0\right )\\ \mathcal {L}\left (y^{\prime \prime }\right ) &= s^2 Y(s) - y'(0) - s y \left (0\right ) \end {align*}
The given ode now becomes an algebraic equation in the Laplace domain \begin {align*} s^{2} Y \left (s \right )-y^{\prime }\left (0\right )-s y \left (0\right )+3 s Y \left (s \right )-3 y \left (0\right )+2 Y \left (s \right ) = \frac {1-{\mathrm e}^{-s}}{s}\tag {1} \end {align*}
But the initial conditions are \begin {align*} y \left (0\right )&=0\\ y'(0) &=0 \end {align*}
Substituting these initial conditions in above in Eq (1) gives \begin {align*} s^{2} Y \left (s \right )+3 s Y \left (s \right )+2 Y \left (s \right ) = \frac {1-{\mathrm e}^{-s}}{s} \end {align*}
Solving the above equation for \(Y(s)\) results in \begin {align*} Y(s) = -\frac {-1+{\mathrm e}^{-s}}{s \left (s^{2}+3 s +2\right )} \end {align*}
Taking the inverse Laplace transform gives \begin {align*} y&= \mathcal {L}^{-1}\left (Y(s)\right )\\ &= \mathcal {L}^{-1}\left (-\frac {-1+{\mathrm e}^{-s}}{s \left (s^{2}+3 s +2\right )}\right )\\ &= \frac {\operatorname {Heaviside}\left (1-t \right )}{2}+\frac {{\mathrm e}^{-2 t}}{2}-{\mathrm e}^{-t}+\frac {\left (-{\mathrm e}^{-2 t +2}+2 \,{\mathrm e}^{1-t}\right ) \operatorname {Heaviside}\left (t -1\right )}{2} \end {align*}
Converting the above solution to piecewise it becomes \[
y = \left \{\begin {array}{cc} \frac {{\mathrm e}^{-2 t}}{2}-{\mathrm e}^{-t}+\frac {1}{2} & t <1 \\ \frac {{\mathrm e}^{-2}}{2}-{\mathrm e}^{-1}+1 & t =1 \\ \frac {{\mathrm e}^{-2 t}}{2}-{\mathrm e}^{-t}-\frac {{\mathrm e}^{-2 t +2}}{2}+{\mathrm e}^{1-t} & 1 The solution(s) found are the following \begin{align*}
\tag{1} y &= \frac {\left (\left \{\begin {array}{cc} {\mathrm e}^{-2 t}-2 \,{\mathrm e}^{-t}+1 & t <1 \\ {\mathrm e}^{-2}-2 \,{\mathrm e}^{-1}+2 & t &=1 \\ {\mathrm e}^{-2 t}-2 \,{\mathrm e}^{-t}-{\mathrm e}^{-2 t +2}+2 \,{\mathrm e}^{1-t} & 1 Verification of solutions
\[
y = \frac {\left (\left \{\begin {array}{cc} {\mathrm e}^{-2 t}-2 \,{\mathrm e}^{-t}+1 & t <1 \\ {\mathrm e}^{-2}-2 \,{\mathrm e}^{-1}+2 & t =1 \\ {\mathrm e}^{-2 t}-2 \,{\mathrm e}^{-t}-{\mathrm e}^{-2 t +2}+2 \,{\mathrm e}^{1-t} & 1
\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & \left [\frac {d}{d t}y^{\prime }+3 y^{\prime }+2 y=\left \{\begin {array}{cc} 0 & t \le 0 \\ 1 & t <1 \\ 0 & 1\le t \end {array}\right ., y \left (0\right )=0, y^{\prime }{\raise{-0.36em}{\Big |}}{\mstack {}{_{\left \{t \hiderel {=}0\right \}}}}=0\right ] \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 2 \\ {} & {} & \frac {d}{d t}y^{\prime } \\ \bullet & {} & \textrm {Characteristic polynomial of homogeneous ODE}\hspace {3pt} \\ {} & {} & r^{2}+3 r +2=0 \\ \bullet & {} & \textrm {Factor the characteristic polynomial}\hspace {3pt} \\ {} & {} & \left (r +2\right ) \left (r +1\right )=0 \\ \bullet & {} & \textrm {Roots of the characteristic polynomial}\hspace {3pt} \\ {} & {} & r =\left (-2, -1\right ) \\ \bullet & {} & \textrm {1st solution of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y_{1}\left (t \right )={\mathrm e}^{-2 t} \\ \bullet & {} & \textrm {2nd solution of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y_{2}\left (t \right )={\mathrm e}^{-t} \\ \bullet & {} & \textrm {General solution of the ODE}\hspace {3pt} \\ {} & {} & y=c_{1} y_{1}\left (t \right )+c_{2} y_{2}\left (t \right )+y_{p}\left (t \right ) \\ \bullet & {} & \textrm {Substitute in solutions of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y=c_{1} {\mathrm e}^{-2 t}+c_{2} {\mathrm e}^{-t}+y_{p}\left (t \right ) \\ \square & {} & \textrm {Find a particular solution}\hspace {3pt} y_{p}\left (t \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 (t \right )\hspace {3pt}\textrm {is the forcing function}\hspace {3pt} \\ {} & {} & \left [y_{p}\left (t \right )=-y_{1}\left (t \right ) \left (\int \frac {y_{2}\left (t \right ) f \left (t \right )}{W \left (y_{1}\left (t \right ), y_{2}\left (t \right )\right )}d t \right )+y_{2}\left (t \right ) \left (\int \frac {y_{1}\left (t \right ) f \left (t \right )}{W \left (y_{1}\left (t \right ), y_{2}\left (t \right )\right )}d t \right ), f \left (t \right )=\left \{\begin {array}{cc} 0 & t \le 0 \\ 1 & t <1 \\ 0 & 1\le t \end {array}\right .\right ] \\ {} & \circ & \textrm {Wronskian of solutions of the homogeneous equation}\hspace {3pt} \\ {} & {} & W \left (y_{1}\left (t \right ), y_{2}\left (t \right )\right )=\left [\begin {array}{cc} {\mathrm e}^{-2 t} & {\mathrm e}^{-t} \\ -2 \,{\mathrm e}^{-2 t} & -{\mathrm e}^{-t} \end {array}\right ] \\ {} & \circ & \textrm {Compute Wronskian}\hspace {3pt} \\ {} & {} & W \left (y_{1}\left (t \right ), y_{2}\left (t \right )\right )={\mathrm e}^{-3 t} \\ {} & \circ & \textrm {Substitute functions into equation for}\hspace {3pt} y_{p}\left (t \right ) \\ {} & {} & y_{p}\left (t \right )=-{\mathrm e}^{-2 t} \left (\int \left (\left \{\begin {array}{cc} 0 & t \le 0 \\ {\mathrm e}^{2 t} & t <1 \\ 0 & 1\le t \end {array}\right .\right )d t \right )+{\mathrm e}^{-t} \left (\int \left (\left \{\begin {array}{cc} 0 & t \le 0 \\ {\mathrm e}^{t} & t <1 \\ 0 & 1\le t \end {array}\right .\right )d t \right ) \\ {} & \circ & \textrm {Compute integrals}\hspace {3pt} \\ {} & {} & y_{p}\left (t \right )=\frac {\left (\left \{\begin {array}{cc} 0 & t \le 0 \\ {\mathrm e}^{-2 t}-2 \,{\mathrm e}^{-t}+1 & t \le 1 \\ {\mathrm e}^{-2 t}-2 \,{\mathrm e}^{-t}-{\mathrm e}^{-2 t +2}+2 \,{\mathrm e}^{1-t} & 1 Maple trace
✓ Solution by Maple
Time used: 1.062 (sec). Leaf size: 65
\[
y \left (t \right ) = \frac {\left (\left \{\begin {array}{cc} 1-2 \,{\mathrm e}^{-t}+{\mathrm e}^{-2 t} & t <1 \\ -2 \,{\mathrm e}^{-1}+{\mathrm e}^{-2}+2 & t =1 \\ 2 \,{\mathrm e}^{1-t}-{\mathrm e}^{-2 t +2}-2 \,{\mathrm e}^{-t}+{\mathrm e}^{-2 t} & 1 ✓ Solution by Mathematica
Time used: 0.041 (sec). Leaf size: 57
\[
y(t)\to \begin {array}{cc} \{ & \begin {array}{cc} 0 & t\leq 0 \\ \frac {1}{2} e^{-2 t} \left (-1+e^t\right )^2 & 07.7.1 Existence and uniqueness analysis
7.7.2 Maple step by step solution
`Methods for second order ODEs:
--- Trying classification methods ---
trying a quadrature
trying high order exact linear fully integrable
trying differential order: 2; linear nonhomogeneous with symmetry [0,1]
trying a double symmetry of the form [xi=0, eta=F(x)]
<- double symmetry of the form [xi=0, eta=F(x)] successful`
dsolve([diff(y(t),t$2)+3*diff(y(t),t)+2*y(t)=piecewise(0<t and t<1,1,t>1,0),y(0) = 0, D(y)(0) = 0],y(t), singsol=all)
DSolve[{y''[t]+3*y'[t]+2*y[t]==Piecewise[{{1,0<t<1},{0,t>1}}],{y[0]==0,y'[0]==0}},y[t],t,IncludeSingularSolutions -> True]