2.4.6 Problem 27
Internal
problem
ID
[13306]
Book
:
Handbook
of
exact
solutions
for
ordinary
differential
equations.
By
Polyanin
and
Zaitsev.
Second
edition
Section
:
Chapter
1,
section
1.2.
Riccati
Equation.
subsection
1.2.3-2.
Equations
with
power
and
exponential
functions
Problem
number
:
27
Date
solved
:
Sunday, January 18, 2026 at 07:12:02 PM
CAS
classification
:
[_Riccati]
2.4.6.1 Solved using first_order_ode_riccati
0.877 (sec)
Entering first order ode riccati solver
\begin{align*}
y^{\prime }&=a \,{\mathrm e}^{\lambda x} y^{2}-a b \,x^{n} {\mathrm e}^{\lambda x} y+b n \,x^{n -1} \\
\end{align*}
In canonical form the ODE is \begin{align*} y' &= F(x,y)\\ &= a \,{\mathrm e}^{\lambda x} y^{2}-a b \,x^{n} {\mathrm e}^{\lambda x} y+b n \,x^{n -1} \end{align*}
This is a Riccati ODE. Comparing the ODE to solve
\[
y' = a \,{\mathrm e}^{\lambda x} y^{2}-a b \,x^{n} {\mathrm e}^{\lambda x} y+\frac {b \,x^{n} n}{x}
\]
With Riccati ODE standard form \[ y' = f_0(x)+ f_1(x)y+f_2(x)y^{2} \]
Shows
that \(f_0(x)=\frac {b \,x^{n} n}{x}\), \(f_1(x)=-x^{n} {\mathrm e}^{\lambda x} a b\) and \(f_2(x)={\mathrm e}^{\lambda x} a\). Let \begin{align*} y &= \frac {-u'}{f_2 u} \\ &= \frac {-u'}{u \,{\mathrm e}^{\lambda x} a} \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' &=a \lambda \,{\mathrm e}^{\lambda x}\\ f_1 f_2 &=-x^{n} {\mathrm e}^{2 \lambda x} a^{2} b\\ f_2^2 f_0 &=\frac {{\mathrm e}^{2 \lambda x} a^{2} b \,x^{n} n}{x} \end{align*}
Substituting the above terms back in equation (2) gives
\[
{\mathrm e}^{\lambda x} a u^{\prime \prime }\left (x \right )-\left (a \lambda \,{\mathrm e}^{\lambda x}-x^{n} {\mathrm e}^{2 \lambda x} a^{2} b \right ) u^{\prime }\left (x \right )+\frac {{\mathrm e}^{2 \lambda x} a^{2} b \,x^{n} n u \left (x \right )}{x} = 0
\]
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_1 \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_2 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}
\end{equation}
Taking derivative gives \begin{equation}
\tag{4} u^{\prime }\left (x \right ) = -c_1 \,{\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_2 \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x} {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}-c_2 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}
\end{equation}
Substituting equations (3,4) into (1) results in \begin{align*}
y &= \frac {-u'}{f_2 u} \\
y &= \frac {-u'}{u \,{\mathrm e}^{\lambda x} a} \\
y &= -\frac {\left (-c_1 \,{\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_2 \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x} {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}-c_2 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}\right ) {\mathrm e}^{-\lambda x}}{a \left (c_1 \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_2 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}\right )} \\
\end{align*}
Doing
change of constants, the above solution becomes \[
y = -\frac {\left (-{\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_3 \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x} {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}-c_3 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}\right ) {\mathrm e}^{-\lambda x}}{a \left ({\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_3 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}\right )}
\]
Summary of solutions found
\begin{align*}
y &= -\frac {\left (-{\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_3 \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x} {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}-c_3 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{\lambda x} x^{n} a b \,{\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}\right ) {\mathrm e}^{-\lambda x}}{a \left ({\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}+c_3 \int \lambda \,{\mathrm e}^{\lambda x +a b \int {\mathrm e}^{\lambda x} x^{n}d x}d x {\mathrm e}^{-a b \int {\mathrm e}^{\lambda x} x^{n}d x}\right )} \\
\end{align*}
2.4.6.2 Solved using first_order_ode_riccati_by_guessing_particular_solution
0.145 (sec)
Entering first order ode riccati guess solver
\begin{align*}
y^{\prime }&=a \,{\mathrm e}^{\lambda x} y^{2}-a b \,x^{n} {\mathrm e}^{\lambda x} y+b n \,x^{n -1} \\
\end{align*}
This is a Riccati ODE. Comparing the above ODE to
solve with the Riccati standard form \[ y' = f_0(x)+ f_1(x)y+f_2(x)y^{2} \]
Shows that \begin{align*} f_0(x) & =\frac {b \,x^{n} n}{x}\\ f_1(x) & =-x^{n} {\mathrm e}^{\lambda x} a b\\ f_2(x) &={\mathrm e}^{\lambda x} a \end{align*}
Using trial and error, the following particular solution was found
\[
y_p = b \,x^{n}
\]
Since a particular solution is
known, then the general solution is given by \begin{align*} y &= y_p + \frac { \phi (x) }{ c_1 - \int { \phi (x) f_2 \,dx} } \end{align*}
Where
\begin{align*} \phi (x) &= e^{ \int 2 f_2 y_p + f_1 \,dx } \end{align*}
Evaluating the above gives the general solution as
\[
y = b \,x^{n}+\frac {{\mathrm e}^{-\frac {\left (-\lambda \right )^{-n} a b \left (x^{n} \left (-\lambda \right )^{n} n \Gamma \left (n \right ) \left (-\lambda x \right )^{-n}-x^{n} \left (-\lambda \right )^{n} {\mathrm e}^{\lambda x}-x^{n} \left (-\lambda \right )^{n} n \left (-\lambda x \right )^{-n} \Gamma \left (n , -\lambda x \right )\right )}{\lambda }}}{c_1 -\int {\mathrm e}^{-\frac {\left (-\lambda \right )^{-n} a b \left (x^{n} \left (-\lambda \right )^{n} n \Gamma \left (n \right ) \left (-\lambda x \right )^{-n}-x^{n} \left (-\lambda \right )^{n} {\mathrm e}^{\lambda x}-x^{n} \left (-\lambda \right )^{n} n \left (-\lambda x \right )^{-n} \Gamma \left (n , -\lambda x \right )\right )}{\lambda }} {\mathrm e}^{\lambda x} a d x}
\]
Summary of solutions found
\begin{align*}
y &= b \,x^{n}+\frac {{\mathrm e}^{-\frac {\left (-\lambda \right )^{-n} a b \left (x^{n} \left (-\lambda \right )^{n} n \Gamma \left (n \right ) \left (-\lambda x \right )^{-n}-x^{n} \left (-\lambda \right )^{n} {\mathrm e}^{\lambda x}-x^{n} \left (-\lambda \right )^{n} n \left (-\lambda x \right )^{-n} \Gamma \left (n , -\lambda x \right )\right )}{\lambda }}}{c_1 -\int {\mathrm e}^{-\frac {\left (-\lambda \right )^{-n} a b \left (x^{n} \left (-\lambda \right )^{n} n \Gamma \left (n \right ) \left (-\lambda x \right )^{-n}-x^{n} \left (-\lambda \right )^{n} {\mathrm e}^{\lambda x}-x^{n} \left (-\lambda \right )^{n} n \left (-\lambda x \right )^{-n} \Gamma \left (n , -\lambda x \right )\right )}{\lambda }} {\mathrm e}^{\lambda x} a d x} \\
\end{align*}
2.4.6.3 ✓ Maple. Time used: 0.003 (sec). Leaf size: 58
ode:=diff(y(x),x) = a*exp(lambda*x)*y(x)^2-a*b*x^n*exp(lambda*x)*y(x)+b*n*x^(n-1);
dsolve(ode,y(x), singsol=all);
\[
y = -\frac {c_1 \lambda \,{\mathrm e}^{a b \int x^{n} {\mathrm e}^{\lambda x}d x}}{a \left (\lambda \int {\mathrm e}^{\lambda x +a b \int x^{n} {\mathrm e}^{\lambda x}d x}d x c_1 +1\right )}+x^{n} b
\]
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_symmetries
trying Riccati to 2nd Order
-> Calling odsolve with the ODE, diff(diff(y(x),x),x) = (-a*b*x^n*exp(lambda
*x)+lambda)*diff(y(x),x)-a*exp(lambda*x)*b*n*x^(n-1)*y(x), y(x)
*** Sublevel 2 ***
Methods for second order ODEs:
--- Trying classification methods ---
trying a symmetry of the form [xi=0, eta=F(x)]
checking if the LODE is missing y
-> Heun: Equivalence to the GHE or one of its 4 confluent cases under a \
power @ Moebius
-> trying a solution of the form r0(x) * Y + r1(x) * Y where Y = exp(int\
(r(x), dx)) * 2F1([a1, a2], [b1], f)
-> Trying changes of variables to rationalize or make the ODE simpler
trying a symmetry of the form [xi=0, eta=F(x)]
checking if the LODE is missing y
-> Heun: Equivalence to the GHE or one of its 4 confluent cases under \
a power @ Moebius
-> trying a solution of the form r0(x) * Y + r1(x) * Y where Y = exp(\
int(r(x), dx)) * 2F1([a1, a2], [b1], f)
trying a symmetry of the form [xi=0, eta=F(x)]
trying 2nd order exact linear
<- 2nd order exact_linear successful
Change of variables used:
[x = ln(t)/lambda]
Linear ODE actually solved:
a*b*n*(ln(t)/lambda)^n/ln(t)*lambda*u(t)+t*(ln(t)/lambda)^n*a*b*lam\
bda*diff(u(t),t)+lambda^2*t*diff(diff(u(t),t),t) = 0
<- change of variables successful
<- Riccati to 2nd Order successful
Maple step by step
\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & \frac {d}{d x}y \left (x \right )=a \,{\mathrm e}^{\lambda x} y \left (x \right )^{2}-a b \,x^{13306} {\mathrm e}^{\lambda x} y \left (x \right )+13306 b \,x^{13305} \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 1 \\ {} & {} & \frac {d}{d x}y \left (x \right ) \\ \bullet & {} & \textrm {Solve for the highest derivative}\hspace {3pt} \\ {} & {} & \frac {d}{d x}y \left (x \right )=a \,{\mathrm e}^{\lambda x} y \left (x \right )^{2}-a b \,x^{13306} {\mathrm e}^{\lambda x} y \left (x \right )+13306 b \,x^{13305} \end {array} \]
2.4.6.4 ✓ Mathematica. Time used: 2.333 (sec). Leaf size: 260
ode=D[y[x],x]==a*Exp[\[Lambda]*x]*y[x]^2-a*b*x^(n)*Exp[\[Lambda]*x]*y[x]+b*n*x^(n-1);
ic={};
DSolve[{ode,ic},y[x],x,IncludeSingularSolutions->True]
\begin{align*} y(x)&\to -\frac {-a b c_1 \left (\frac {\log \left (e^{\lambda x}\right )}{\lambda }\right )^n \int _1^{e^{x \lambda }}\exp \left (-\int _1^{K[2]}-\frac {a b \left (\frac {\log (K[1])}{\lambda }\right )^n}{\lambda }dK[1]\right )dK[2]+c_1 \lambda \exp \left (-\int _1^{e^{x \lambda }}-\frac {a b \left (\frac {\log (K[1])}{\lambda }\right )^n}{\lambda }dK[1]\right )-a b \left (\frac {\log \left (e^{\lambda x}\right )}{\lambda }\right )^n}{a+a c_1 \int _1^{e^{x \lambda }}\exp \left (-\int _1^{K[2]}-\frac {a b \left (\frac {\log (K[1])}{\lambda }\right )^n}{\lambda }dK[1]\right )dK[2]}\\ y(x)&\to b \left (\frac {\log \left (e^{\lambda x}\right )}{\lambda }\right )^n-\frac {\lambda \exp \left (-\int _1^{e^{x \lambda }}-\frac {a b \left (\frac {\log (K[1])}{\lambda }\right )^n}{\lambda }dK[1]\right )}{a \int _1^{e^{x \lambda }}\exp \left (-\int _1^{K[2]}-\frac {a b \left (\frac {\log (K[1])}{\lambda }\right )^n}{\lambda }dK[1]\right )dK[2]} \end{align*}
2.4.6.5 ✗ Sympy
from sympy import *
x = symbols("x")
a = symbols("a")
b = symbols("b")
lambda_ = symbols("lambda_")
n = symbols("n")
y = Function("y")
ode = Eq(a*b*x**n*y(x)*exp(lambda_*x) - a*y(x)**2*exp(lambda_*x) - b*n*x**(n - 1) + Derivative(y(x), x),0)
ics = {}
dsolve(ode,func=y(x),ics=ics)
NotImplementedError : The given ODE a*b*x**n*y(x)*exp(lambda_*x) - a*y(x)**2*exp(lambda_*x) - b*n*x*
Python version: 3.12.3 (main, Aug 14 2025, 17:47:21) [GCC 13.3.0]
Sympy version 1.14.0
classify_ode(ode,func=y(x))
('1st_power_series', 'lie_group')