2.2.61 Problem 64
Internal
problem
ID
[13267]
Book
:
Handbook
of
exact
solutions
for
ordinary
differential
equations.
By
Polyanin
and
Zaitsev.
Second
edition
Section
:
Chapter
1,
section
1.2.
Riccati
Equation.
1.2.2.
Equations
Containing
Power
Functions
Problem
number
:
64
Date
solved
:
Tuesday, January 20, 2026 at 06:18:06 PM
CAS
classification
:
[_rational, _Riccati]
2.2.61.1 Solved using first_order_ode_riccati
33.451 (sec)
Entering first order ode riccati solver
\begin{align*}
\left (c_{2} x^{2}+b_{2} x +a_{2} \right ) \left (y^{\prime }+\lambda y^{2}\right )+\left (b_{1} x +a_{1} \right ) y+a_{0}&=0 \\
\end{align*}
In canonical form the ODE is \begin{align*} y' &= F(x,y)\\ &= -\frac {y^{2} c_{2} \lambda \,x^{2}+y^{2} b_{2} \lambda x +y^{2} a_{2} \lambda +y b_{1} x +y a_{1} +a_{0}}{c_{2} x^{2}+b_{2} x +a_{2}} \end{align*}
This is a Riccati ODE. Comparing the ODE to solve
\[
y' = -\frac {y^{2} c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {y^{2} b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {y^{2} a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {y b_{1} x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {y a_{1}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{0}}{c_{2} x^{2}+b_{2} x +a_{2}}
\]
With Riccati ODE standard form \[ y' = f_0(x)+ f_1(x)y+f_2(x)y^{2} \]
Shows
that \(f_0(x)=-\frac {a_{0}}{c_{2} x^{2}+b_{2} x +a_{2}}\), \(f_1(x)=-\frac {b_{1} x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{1}}{c_{2} x^{2}+b_{2} x +a_{2}}\) and \(f_2(x)=-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\). Let \begin{align*} y &= \frac {-u'}{f_2 u} \\ &= \frac {-u'}{u \left (-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\right )} \tag {1} \end{align*}
Using the above substitution in the given ODE results (after some simplification) in a second
order ODE to solve for \(u(x)\) which is
\begin{align*} f_2 u''(x) -\left ( f_2' + f_1 f_2 \right ) u'(x) + f_2^2 f_0 u(x) &= 0 \tag {2} \end{align*}
But
\begin{align*} f_2' &=\frac {c_{2} \lambda \,x^{2} \left (2 c_{2} x +b_{2} \right )}{\left (c_{2} x^{2}+b_{2} x +a_{2} \right )^{2}}-\frac {2 c_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}+\frac {b_{2} \lambda x \left (2 c_{2} x +b_{2} \right )}{\left (c_{2} x^{2}+b_{2} x +a_{2} \right )^{2}}-\frac {b_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}+\frac {a_{2} \lambda \left (2 c_{2} x +b_{2} \right )}{\left (c_{2} x^{2}+b_{2} x +a_{2} \right )^{2}}\\ f_1 f_2 &=\left (-\frac {b_{1} x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{1}}{c_{2} x^{2}+b_{2} x +a_{2}}\right ) \left (-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\right )\\ f_2^2 f_0 &=-\frac {\left (-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\right )^{2} a_{0}}{c_{2} x^{2}+b_{2} x +a_{2}} \end{align*}
Substituting the above terms back in equation (2) gives
\[
\left (-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\right ) u^{\prime \prime }\left (x \right )-\left (\frac {c_{2} \lambda \,x^{2} \left (2 c_{2} x +b_{2} \right )}{\left (c_{2} x^{2}+b_{2} x +a_{2} \right )^{2}}-\frac {2 c_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}+\frac {b_{2} \lambda x \left (2 c_{2} x +b_{2} \right )}{\left (c_{2} x^{2}+b_{2} x +a_{2} \right )^{2}}-\frac {b_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}+\frac {a_{2} \lambda \left (2 c_{2} x +b_{2} \right )}{\left (c_{2} x^{2}+b_{2} x +a_{2} \right )^{2}}+\left (-\frac {b_{1} x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{1}}{c_{2} x^{2}+b_{2} x +a_{2}}\right ) \left (-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\right )\right ) u^{\prime }\left (x \right )-\frac {\left (-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\right )^{2} a_{0} u \left (x \right )}{c_{2} x^{2}+b_{2} x +a_{2}} = 0
\]
Unable to solve. Will ask Maple to solve
this ode now.
The solution for \(u \left (x \right )\) is
\begin{equation}
\tag{3} u \left (x \right ) = c_3 \operatorname {hypergeom}\left (\left [\frac {-c_{2} +b_{1} +\sqrt {c_{2}^{2}+\left (-4 \lambda a_{0} -2 b_{1} \right ) c_{2} +b_{1}^{2}}}{2 c_{2}}, -\frac {c_{2} -b_{1} +\sqrt {c_{2}^{2}+\left (-4 \lambda a_{0} -2 b_{1} \right ) c_{2} +b_{1}^{2}}}{2 c_{2}}\right ], \left [\frac {b_{1} \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, c_{2} -2 a_{1} c_{2} +b_{1} b_{2}}{2 c_{2}^{2} \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}}\right ], \frac {-2 \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, x \,c_{2}^{2}-\sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, b_{2} c_{2} +4 c_{2} a_{2} -b_{2}^{2}}{8 c_{2} a_{2} -2 b_{2}^{2}}\right )+c_4 {\left (2 \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, x \,c_{2}^{2}+\sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, b_{2} c_{2} -4 c_{2} a_{2} +b_{2}^{2}\right )}^{\frac {-\frac {c_{2} \left (b_{1} -2 c_{2} \right ) \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}}{2}+a_{1} c_{2} -\frac {b_{1} b_{2}}{2}}{\sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, c_{2}^{2}}} \operatorname {hypergeom}\left (\left [-\frac {c_{2} \left (\sqrt {c_{2}^{2}+\left (-4 \lambda a_{0} -2 b_{1} \right ) c_{2} +b_{1}^{2}}-c_{2} \right ) \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}-2 a_{1} c_{2} +b_{1} b_{2}}{2 \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, c_{2}^{2}}, \frac {c_{2} \left (\sqrt {c_{2}^{2}+\left (-4 \lambda a_{0} -2 b_{1} \right ) c_{2} +b_{1}^{2}}+c_{2} \right ) \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}+2 a_{1} c_{2} -b_{1} b_{2}}{2 \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, c_{2}^{2}}\right ], \left [\frac {-\frac {c_{2} \left (b_{1} -4 c_{2} \right ) \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}}{2}+a_{1} c_{2} -\frac {b_{1} b_{2}}{2}}{\sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, c_{2}^{2}}\right ], \frac {-2 \sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, x \,c_{2}^{2}-\sqrt {\frac {-4 c_{2} a_{2} +b_{2}^{2}}{c_{2}^{2}}}\, b_{2} c_{2} +4 c_{2} a_{2} -b_{2}^{2}}{8 c_{2} a_{2} -2 b_{2}^{2}}\right )
\end{equation}
Taking derivative gives \begin{equation}
\tag{4} \text {Expression too large to display}
\end{equation}
Substituting equations (3,4) into (1) results in \begin{align*}
y &= \frac {-u'}{f_2 u} \\
y &= \frac {-u'}{u \left (-\frac {c_{2} \lambda \,x^{2}}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {b_{2} \lambda x}{c_{2} x^{2}+b_{2} x +a_{2}}-\frac {a_{2} \lambda }{c_{2} x^{2}+b_{2} x +a_{2}}\right )} \\
y &= \text {Expression too large to display} \\
\end{align*}
Doing change of constants, the above solution becomes \[
\text {Expression too large to display}
\]
Simplifying the above gives
\begin{align*}
\text {Expression too large to display} \\
\end{align*}
Summary of solutions found
\begin{align*}
\text {Expression too large to display} \\
\end{align*}
2.2.61.2 ✓ Maple. Time used: 0.004 (sec). Leaf size: 2072
ode:=(c__2*x^2+b__2*x+a__2)*(diff(y(x),x)+lambda*y(x)^2)+(b__1*x+a__1)*y(x)+a__0 = 0;
dsolve(ode,y(x), singsol=all);
\[
\text {Expression too large to display}
\]
Maple trace
Methods for first order ODEs:
--- Trying classification methods ---
trying a quadrature
trying 1st order linear
trying Bernoulli
trying separable
trying inverse linear
trying homogeneous types:
trying Chini
differential order: 1; looking for linear symmetries
trying exact
Looking for potential symmetries
trying Riccati
trying Riccati sub-methods:
trying Riccati to 2nd Order
-> Calling odsolve with the ODE, diff(diff(y(x),x),x) = -(b__1*x+a__1)/(c__2
*x^2+b__2*x+a__2)*diff(y(x),x)-lambda*a__0/(c__2*x^2+b__2*x+a__2)*y(x), y(x)
*** Sublevel 2 ***
Methods for second order ODEs:
--- Trying classification methods ---
trying a quadrature
checking if the LODE has constant coefficients
checking if the LODE is of Euler type
trying a symmetry of the form [xi=0, eta=F(x)]
checking if the LODE is missing y
-> Trying a Liouvillian solution using Kovacics algorithm
<- No Liouvillian solutions exists
-> Trying a solution in terms of special functions:
-> Bessel
-> elliptic
-> Legendre
-> Kummer
-> hyper3: Equivalence to 1F1 under a power @ Moebius
-> hypergeometric
-> heuristic approach
<- heuristic approach successful
<- hypergeometric successful
<- special function solution successful
<- Riccati to 2nd Order successful
Maple step by step
\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & \left (c_{2} x^{2}+b_{2} x +a_{2} \right ) \left (\frac {d}{d x}y \left (x \right )+\lambda y \left (x \right )^{2}\right )+\left (b_{1} x +a_{1} \right ) y \left (x \right )+a_{0} =0 \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 1 \\ {} & {} & \frac {d}{d x}y \left (x \right ) \\ \bullet & {} & \textrm {Solve for the highest derivative}\hspace {3pt} \\ {} & {} & \frac {d}{d x}y \left (x \right )=-\frac {y \left (x \right )^{2} c_{2} \lambda \,x^{2}+y \left (x \right )^{2} b_{2} \lambda x +y \left (x \right )^{2} a_{2} \lambda +y \left (x \right ) b_{1} x +y \left (x \right ) a_{1} +a_{0}}{c_{2} x^{2}+b_{2} x +a_{2}} \end {array} \]
2.2.61.3 ✓ Mathematica. Time used: 6.917 (sec). Leaf size: 1986
ode=(c2*x^2+b2*x+a2)*(D[y[x],x]+\[Lambda]*y[x]^2)+(b1*x+a1)*y[x]+a0==0;
ic={};
DSolve[{ode,ic},y[x],x,IncludeSingularSolutions->True]
Too large to display
2.2.61.4 ✗ Sympy
from sympy import *
x = symbols("x")
a__0 = symbols("a__0")
a__1 = symbols("a__1")
a__2 = symbols("a__2")
b__1 = symbols("b__1")
b__2 = symbols("b__2")
c__2 = symbols("c__2")
lambda_ = symbols("lambda_")
y = Function("y")
ode = Eq(a__0 + (a__1 + b__1*x)*y(x) + (lambda_*y(x)**2 + Derivative(y(x), x))*(a__2 + b__2*x + c__2*x**2),0)
ics = {}
dsolve(ode,func=y(x),ics=ics)
Timed Out
Python version: 3.12.3 (main, Aug 14 2025, 17:47:21) [GCC 13.3.0]
Sympy version 1.14.0