2.1.68 Problem 68

Solved as second order missing x ode
Maple
Mathematica
Sympy

Internal problem ID [10054]
Book : Own collection of miscellaneous problems
Section : section 1.0
Problem number : 68
Date solved : Thursday, November 27, 2025 at 10:07:38 AM
CAS classification : [[_2nd_order, _missing_x], [_2nd_order, _reducible, _mu_x_y1]]

Solved as second order missing x ode

Time used: 2.134 (sec)

Solve

\begin{align*} a y y^{\prime \prime }+y b&=c \\ \end{align*}
This is missing independent variable second order ode. Solved by reduction of order by using substitution which makes the dependent variable \(y\) an independent variable. Using
\begin{align*} y' &= p \end{align*}

Then

\begin{align*} y'' &= \frac {dp}{dx}\\ &= \frac {dp}{dy}\frac {dy}{dx}\\ &= p \frac {dp}{dy} \end{align*}

Hence the ode becomes

\begin{align*} a y p \left (y \right ) \left (\frac {d}{d y}p \left (y \right )\right )+y b = c \end{align*}

Which is now solved as first order ode for \(p(y)\).

Solve The ode

\begin{equation} p^{\prime } = -\frac {y b -c}{a y p} \end{equation}
is separable as it can be written as
\begin{align*} p^{\prime }&= -\frac {y b -c}{a y p}\\ &= f(y) g(p) \end{align*}

Where

\begin{align*} f(y) &= -\frac {y b -c}{a y}\\ g(p) &= \frac {1}{p} \end{align*}

Integrating gives

\begin{align*} \int { \frac {1}{g(p)} \,dp} &= \int { f(y) \,dy} \\ \int { p\,dp} &= \int { -\frac {y b -c}{a y} \,dy} \\ \end{align*}
\[ \frac {p^{2}}{2}=\frac {c \ln \left (y \right )-y b}{a}+c_1 \]
Solving for \(p\) gives
\begin{align*} p &= \frac {\sqrt {2}\, \sqrt {a \left (c \ln \left (y \right )+c_1 a -y b \right )}}{a} \\ p &= -\frac {\sqrt {2}\, \sqrt {a \left (c \ln \left (y \right )+c_1 a -y b \right )}}{a} \\ \end{align*}
For solution (1) found earlier, since \(p=y^{\prime }\) then we now have a new first order ode to solve which is
\begin{align*} y^{\prime } = \frac {\sqrt {2}\, \sqrt {a \left (c \ln \left (y\right )+c_1 a -y b \right )}}{a} \end{align*}

Solve Unable to integrate (or intergal too complicated), and since no initial conditions are given, then the result can be written as

\[ \int _{}^{y}\frac {a \sqrt {2}}{2 \sqrt {a \left (c \ln \left (\tau \right )+c_1 a -\tau b \right )}}d \tau = x +c_2 \]
For solution (2) found earlier, since \(p=y^{\prime }\) then we now have a new first order ode to solve which is
\begin{align*} y^{\prime } = -\frac {\sqrt {2}\, \sqrt {a \left (c \ln \left (y\right )+c_1 a -y b \right )}}{a} \end{align*}

Solve Unable to integrate (or intergal too complicated), and since no initial conditions are given, then the result can be written as

\[ \int _{}^{y}-\frac {a \sqrt {2}}{2 \sqrt {a \left (c \ln \left (\tau \right )+c_1 a -\tau b \right )}}d \tau = x +c_3 \]

Summary of solutions found

\begin{align*} \int _{}^{y}\frac {a \sqrt {2}}{2 \sqrt {a \left (c \ln \left (\tau \right )+c_1 a -\tau b \right )}}d \tau &= x +c_2 \\ \int _{}^{y}-\frac {a \sqrt {2}}{2 \sqrt {a \left (c \ln \left (\tau \right )+c_1 a -\tau b \right )}}d \tau &= x +c_3 \\ \end{align*}
Maple. Time used: 0.016 (sec). Leaf size: 68
ode:=a*y(x)*diff(diff(y(x),x),x)+b*y(x) = c; 
dsolve(ode,y(x), singsol=all);
 
\begin{align*} a \int _{}^{y}\frac {1}{\sqrt {a \left (2 c \ln \left (\textit {\_a} \right )+c_1 a -2 b \textit {\_a} \right )}}d \textit {\_a} -x -c_2 &= 0 \\ -a \int _{}^{y}\frac {1}{\sqrt {a \left (2 c \ln \left (\textit {\_a} \right )+c_1 a -2 b \textit {\_a} \right )}}d \textit {\_a} -x -c_2 &= 0 \\ \end{align*}

Maple trace

Methods for second order ODEs: 
--- Trying classification methods --- 
trying 2nd order Liouville 
trying 2nd order WeierstrassP 
trying 2nd order JacobiSN 
differential order: 2; trying a linearization to 3rd order 
trying 2nd order ODE linearizable_by_differentiation 
trying 2nd order, 2 integrating factors of the form mu(x,y) 
trying differential order: 2; missing variables 
   -> Computing symmetries using: way = 3 
   -> Computing symmetries using: way = exp_sym 
-> Calling odsolve with the ODE, diff(_b(_a),_a)*_b(_a)+(_a*b-c)/_a/a = 0, _b( 
_a) 
   *** Sublevel 2 *** 
   Methods for first order ODEs: 
   --- Trying classification methods --- 
   trying a quadrature 
   trying 1st order linear 
   trying Bernoulli 
   <- Bernoulli successful 
<- differential order: 2; canonical coordinates successful 
<- differential order 2; missing variables successful
 
Mathematica. Time used: 0.385 (sec). Leaf size: 44
ode=a*y[x]*D[y[x],{x,2}]+b*y[x]==c; 
ic={}; 
DSolve[{ode,ic},y[x],x,IncludeSingularSolutions->True]
 
\[ \text {Solve}\left [\int _1^{y(x)}\frac {1}{\sqrt {c_1+\frac {2 (\log (K[1]) c+c-b K[1])}{a}}}dK[1]{}^2=(x+c_2){}^2,y(x)\right ] \]
Sympy
from sympy import * 
x = symbols("x") 
a = symbols("a") 
b = symbols("b") 
c = symbols("c") 
y = Function("y") 
ode = Eq(a*y(x)*Derivative(y(x), (x, 2)) + b*y(x) - c,0) 
ics = {} 
dsolve(ode,func=y(x),ics=ics)
 
Timed Out