Internal problem ID [6693]
Internal file name [OUTPUT/5941_Sunday_June_05_2022_04_03_03_PM_50687365/index.tex
]
Book: DIFFERENTIAL EQUATIONS with Boundary Value Problems. DENNIS G. ZILL,
WARREN S. WRIGHT, MICHAEL R. CULLEN. Brooks/Cole. Boston, MA. 2013. 8th
edition.
Section: CHAPTER 7 THE LAPLACE TRANSFORM. 7.4.1 DERIVATIVES OF A
TRANSFORM. Page 309
Problem number: 14.
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]]
\[ \boxed {y^{\prime \prime }+y=\left \{\begin {array}{cc} 1 & 0\le t <\frac {\pi }{2} \\ \sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right .} \] With initial conditions \begin {align*} [y \left (0\right ) = 1, y^{\prime }\left (0\right ) = 0] \end {align*}
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) &=0\\ q(t) &=1\\ F &=\left \{\begin {array}{cc} 0 & t <0 \\ 1 & t <\frac {\pi }{2} \\ \sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right . \end {align*}
Hence the ode is \begin {align*} y^{\prime \prime }+y = \left \{\begin {array}{cc} 0 & t <0 \\ 1 & t <\frac {\pi }{2} \\ \sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right . \end {align*}
The domain of \(p(t)=0\) 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 )+Y \left (s \right ) = \frac {-{\mathrm e}^{-\frac {\pi s}{2}}+1+s^{2}}{s \left (s^{2}+1\right )}\tag {1} \end {align*}
But the initial conditions are \begin {align*} y \left (0\right )&=1\\ y'(0) &=0 \end {align*}
Substituting these initial conditions in above in Eq (1) gives \begin {align*} s^{2} Y \left (s \right )-s +Y \left (s \right ) = \frac {-{\mathrm e}^{-\frac {\pi s}{2}}+1+s^{2}}{s \left (s^{2}+1\right )} \end {align*}
Solving the above equation for \(Y(s)\) results in \begin {align*} Y(s) = -\frac {-s^{4}-2 s^{2}+{\mathrm e}^{-\frac {\pi s}{2}}-1}{s \left (s^{2}+1\right )^{2}} \end {align*}
Taking the inverse Laplace transform gives \begin {align*} y&= \mathcal {L}^{-1}\left (Y(s)\right )\\ &= \mathcal {L}^{-1}\left (-\frac {-s^{4}-2 s^{2}+{\mathrm e}^{-\frac {\pi s}{2}}-1}{s \left (s^{2}+1\right )^{2}}\right )\\ &= 1+\frac {\left (-4+4 \sin \left (t \right )-\cos \left (t \right ) \left (2 t -\pi \right )\right ) \operatorname {Heaviside}\left (t -\frac {\pi }{2}\right )}{4} \end {align*}
Converting the above solution to piecewise it becomes \[
y = \left \{\begin {array}{cc} 1 & t <\frac {\pi }{2} \\ \sin \left (t \right )-\frac {\cos \left (t \right ) \left (2 t -\pi \right )}{4} & \frac {\pi }{2}\le t \end {array}\right .
\] Simplifying the solution gives \[
y = \left \{\begin {array}{cc} 1 & t <\frac {\pi }{2} \\ \frac {\left (-2 t +\pi \right ) \cos \left (t \right )}{4}+\sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right .
\]
The solution(s) found are the following \begin{align*}
\tag{1} y &= \left \{\begin {array}{cc} 1 & t <\frac {\pi }{2} \\ \frac {\left (-2 t +\pi \right ) \cos \left (t \right )}{4}+\sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right . \\
\end{align*} Verification of solutions
\[
y = \left \{\begin {array}{cc} 1 & t <\frac {\pi }{2} \\ \frac {\left (-2 t +\pi \right ) \cos \left (t \right )}{4}+\sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right .
\] Verified OK.
\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & \left [\frac {d}{d t}y^{\prime }+y=\left \{\begin {array}{cc} 0 & t <0 \\ 1 & t <\frac {\pi }{2} \\ \sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right ., y \left (0\right )=1, 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}+1=0 \\ \bullet & {} & \textrm {Use quadratic formula to solve for}\hspace {3pt} r \\ {} & {} & r =\frac {0\pm \left (\sqrt {-4}\right )}{2} \\ \bullet & {} & \textrm {Roots of the characteristic polynomial}\hspace {3pt} \\ {} & {} & r =\left (\mathrm {-I}, \mathrm {I}\right ) \\ \bullet & {} & \textrm {1st solution of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y_{1}\left (t \right )=\cos \left (t \right ) \\ \bullet & {} & \textrm {2nd solution of the homogeneous ODE}\hspace {3pt} \\ {} & {} & y_{2}\left (t \right )=\sin \left (t \right ) \\ \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} \cos \left (t \right )+c_{2} \sin \left (t \right )+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 <0 \\ 1 & t <\frac {\pi }{2} \\ \sin \left (t \right ) & \frac {\pi }{2}\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} \cos \left (t \right ) & \sin \left (t \right ) \\ -\sin \left (t \right ) & \cos \left (t \right ) \end {array}\right ] \\ {} & \circ & \textrm {Compute Wronskian}\hspace {3pt} \\ {} & {} & W \left (y_{1}\left (t \right ), y_{2}\left (t \right )\right )=1 \\ {} & \circ & \textrm {Substitute functions into equation for}\hspace {3pt} y_{p}\left (t \right ) \\ {} & {} & y_{p}\left (t \right )=-\cos \left (t \right ) \left (\int \left (\left \{\begin {array}{cc} 0 & t <0 \\ \sin \left (t \right ) & t <\frac {\pi }{2} \\ \sin \left (t \right )^{2} & \frac {\pi }{2}\le t \end {array}\right .\right )d t \right )+\sin \left (t \right ) \left (\int \cos \left (t \right ) \left (\left \{\begin {array}{cc} 0 & t <0 \\ 1 & t <\frac {\pi }{2} \\ \sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right .\right )d t \right ) \\ {} & \circ & \textrm {Compute integrals}\hspace {3pt} \\ {} & {} & y_{p}\left (t \right )=\left \{\begin {array}{cc} 0 & t \le 0 \\ -\cos \left (t \right )+1 & t \le \frac {\pi }{2} \\ \frac {\left (\pi -2 t -4\right ) \cos \left (t \right )}{4}+\sin \left (t \right ) & \frac {\pi }{2} Maple trace
✓ Solution by Maple
Time used: 2.734 (sec). Leaf size: 30
\[
y \left (t \right ) = \left \{\begin {array}{cc} 1 & t <\frac {\pi }{2} \\ \frac {\left (-2 t +\pi \right ) \cos \left (t \right )}{4}+\sin \left (t \right ) & \frac {\pi }{2}\le t \end {array}\right .
\]
✓ Solution by Mathematica
Time used: 0.047 (sec). Leaf size: 38
\[
y(t)\to \begin {array}{cc} \{ & \begin {array}{cc} \cos (t) & t\leq 0 \\ 1 & t>0\land 2 t\leq \pi \\ \frac {1}{4} (\pi -2 t) \cos (t)+\sin (t) & \text {True} \\ \end {array} \\ \end {array}
\]
7.6.2 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)]
-> Try solving first the homogeneous part of the ODE
checking if the LODE has constant coefficients
<- constant coefficients successful
<- solving first the homogeneous part of the ODE successful`
dsolve([diff(y(t),t$2)+y(t)=piecewise(0<=t and t<Pi/2,1,t>= Pi/2,sin(t)),y(0) = 1, D(y)(0) = 0],y(t), singsol=all)
DSolve[{y''[t]+y[t]==Piecewise[{{1,0<=t<Pi/2},{Sin[t],t>=Pi/2}}],{y[0]==1,y'[0]==0}},y[t],t,IncludeSingularSolutions -> True]