2.2.30 Problem 33

2.2.30.1 Solved using first_order_ode_riccati_by_guessing_particular_solution
2.2.30.2 Maple
2.2.30.3 Mathematica
2.2.30.4 Sympy

Internal problem ID [13236]
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 : 33
Date solved : Sunday, January 18, 2026 at 06:49:46 PM
CAS classification : [_Riccati]

2.2.30.1 Solved using first_order_ode_riccati_by_guessing_particular_solution

0.160 (sec)

Entering first order ode riccati guess solver

\begin{align*} y^{\prime }&=a \,x^{n} y^{2}+b \,x^{m} y+c k \,x^{k -1}-b c \,x^{m +k}-a \,c^{2} x^{n +2 k} \\ \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 {c k \,x^{k}}{x}-a \,c^{2} x^{n} x^{2 k}-b c \,x^{m} x^{k}\\ f_1(x) & =b \,x^{m}\\ f_2(x) &=x^{n} a \end{align*}

Using trial and error, the following particular solution was found

\[ y_p = c \,x^{k} \]
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

\[ y = c \,x^{k}+\frac {{\mathrm e}^{\frac {b \,x^{1+m}}{1+m}+\frac {2 a c x \,{\mathrm e}^{\ln \left (x \right ) k} {\mathrm e}^{n \ln \left (x \right )}}{1+k +n}}}{c_1 -\int {\mathrm e}^{\frac {b \,x^{1+m}}{1+m}+\frac {2 a c x \,{\mathrm e}^{\ln \left (x \right ) k} {\mathrm e}^{n \ln \left (x \right )}}{1+k +n}} x^{n} a d x} \]

Summary of solutions found

\begin{align*} y &= c \,x^{k}+\frac {{\mathrm e}^{\frac {b \,x^{1+m}}{1+m}+\frac {2 a c x \,{\mathrm e}^{\ln \left (x \right ) k} {\mathrm e}^{n \ln \left (x \right )}}{1+k +n}}}{c_1 -\int {\mathrm e}^{\frac {b \,x^{1+m}}{1+m}+\frac {2 a c x \,{\mathrm e}^{\ln \left (x \right ) k} {\mathrm e}^{n \ln \left (x \right )}}{1+k +n}} x^{n} a d x} \\ \end{align*}
2.2.30.2 Maple
ode:=diff(y(x),x) = a*x^n*y(x)^2+b*x^m*y(x)+c*k*x^(-1+k)-b*c*x^(m+k)-a*c^2*x^(n+2*k); 
dsolve(ode,y(x), singsol=all);
 
\[ \text {No solution found} \]

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) = (x^m*b*x+n)/x*diff(y 
(x),x)-a*x^n*c*(-x^(n+2*k)*a*c+x^(k-1)*k-x^(m+k)*b)*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 
      -> Trying an equivalence, under non-integer power transformations, 
         to LODEs admitting Liouvillian solutions. 
      -> Trying a solution in terms of special functions: 
         -> Bessel 
         -> elliptic 
         -> Legendre 
         -> Kummer 
            -> hyper3: Equivalence to 1F1 under a power @ Moebius 
         -> hypergeometric 
            -> heuristic approach 
            -> hyper3: Equivalence to 2F1, 1F1 or 0F1 under a power @ Moebius 
         -> Mathieu 
            -> Equivalence to the rational form of Mathieu ODE under a power @\ 
 Moebius 
      -> Heun: Equivalence to the GHE or one of its 4 confluent cases under a \ 
power @ Moebius 
      -> 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 
      <- unable to find a useful change of variables 
         trying a symmetry of the form [xi=0, eta=F(x)] 
         trying 2nd order exact linear 
         trying symmetries linear in x and y(x) 
         trying to convert to a linear ODE with constant coefficients 
         trying 2nd order, integrating factor of the form mu(x,y) 
         trying a symmetry of the form [xi=0, eta=F(x)] 
         checking if the LODE is missing y 
         -> Trying an equivalence, under non-integer power transformations, 
            to LODEs admitting Liouvillian solutions. 
         -> Trying a solution in terms of special functions: 
            -> Bessel 
            -> elliptic 
            -> Legendre 
            -> Whittaker 
               -> hyper3: Equivalence to 1F1 under a power @ Moebius 
            -> hypergeometric 
               -> heuristic approach 
               -> hyper3: Equivalence to 2F1, 1F1 or 0F1 under a power @ Moebi\ 
us 
            -> Mathieu 
               -> Equivalence to the rational form of Mathieu ODE under a powe\ 
r @ Moebius 
         -> Heun: Equivalence to the GHE or one of its 4 confluent cases under \ 
a power @ Moebius 
         -> 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 
         <- unable to find a useful change of variables 
            trying a symmetry of the form [xi=0, eta=F(x)] 
         trying to convert to an ODE of Bessel type 
   -> Trying a change of variables to reduce to Bernoulli 
   -> Calling odsolve with the ODE, diff(y(x),x)-(a*x^n*y(x)^2+y(x)+b*x^m*y(x)* 
x+x^2*(c*k*x^(k-1)-b*c*x^(m+k)-a*c^2*x^(n+2*k)))/x, y(x), explicit 
      *** Sublevel 2 *** 
      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 inverse_Riccati 
      trying 1st order ODE linearizable_by_differentiation 
   -> trying a symmetry pattern of the form [F(x)*G(y), 0] 
   -> trying a symmetry pattern of the form [0, F(x)*G(y)] 
   -> trying a symmetry pattern of the form [F(x),G(x)*y+H(x)] 
trying inverse_Riccati 
trying 1st order ODE linearizable_by_differentiation 
--- Trying Lie symmetry methods, 1st order --- 
   -> Computing symmetries using: way = 4 
   -> Computing symmetries using: way = 2 
   -> Computing symmetries using: way = 6
 

Maple step by step

\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & \frac {d}{d x}y \left (x \right )=a \,x^{13236} y \left (x \right )^{2}+b \,x^{m} y \left (x \right )+c k \,x^{k -1}-b c \,x^{m +k}-a \,c^{2} x^{13236+2 k} \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 1 \\ {} & {} & \frac {d}{d x}y \left (x \right ) \\ \bullet & {} & \textrm {Solve for the highest derivative}\hspace {3pt} \\ {} & {} & \frac {d}{d x}y \left (x \right )=a \,x^{13236} y \left (x \right )^{2}+b \,x^{m} y \left (x \right )+c k \,x^{k -1}-b c \,x^{m +k}-a \,c^{2} x^{13236+2 k} \end {array} \]
2.2.30.3 Mathematica
ode=D[y[x],x]==a*x^n*y[x]^2+b*x^m*y[x]+c*k*x^(k-1)-b*c*x^(m+k)-a*c^2*x^(n+2*k); 
ic={}; 
DSolve[{ode,ic},y[x],x,IncludeSingularSolutions->True]
 

Not solved

2.2.30.4 Sympy
from sympy import * 
x = symbols("x") 
a = symbols("a") 
b = symbols("b") 
c = symbols("c") 
k = symbols("k") 
m = symbols("m") 
n = symbols("n") 
y = Function("y") 
ode = Eq(a*c**2*x**(2*k + n) - a*x**n*y(x)**2 + b*c*x**(k + m) - b*x**m*y(x) - c*k*x**(k - 1) + Derivative(y(x), x),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