7.6 problem 6

7.6.1 Solving as riccati ode
7.6.2 Maple step by step solution

Internal problem ID [10480]
Internal file name [OUTPUT/9428_Monday_June_06_2022_02_32_08_PM_61700309/index.tex]

Book: Handbook of exact solutions for ordinary differential equations. By Polyanin and Zaitsev. Second edition
Section: Chapter 1, section 1.2. Riccati Equation. subsection 1.2.5-1. Equations Containing Logarithmic Functions
Problem number: 6.
ODE order: 1.
ODE degree: 1.

The type(s) of ODE detected by this program : "riccati"

Maple gives the following as the ode type

[_Riccati]

\[ \boxed {y^{\prime } x -a \,x^{n} y^{2}=b -a \,b^{2} x^{n} \ln \left (x \right )^{2}} \]

7.6.1 Solving as riccati ode

In canonical form the ODE is \begin {align*} y' &= F(x,y)\\ &= -\frac {a \,b^{2} x^{n} \ln \left (x \right )^{2}-a \,x^{n} y^{2}-b}{x} \end {align*}

This is a Riccati ODE. Comparing the ODE to solve \[ y' = -\frac {a \,b^{2} x^{n} \ln \left (x \right )^{2}}{x}+\frac {a \,x^{n} y^{2}}{x}+\frac {b}{x} \] With Riccati ODE standard form \[ y' = f_0(x)+ f_1(x)y+f_2(x)y^{2} \] Shows that \(f_0(x)=-\frac {-b +a \,b^{2} x^{n} \ln \left (x \right )^{2}}{x}\), \(f_1(x)=0\) and \(f_2(x)=\frac {x^{n} a}{x}\). Let \begin {align*} y &= \frac {-u'}{f_2 u} \\ &= \frac {-u'}{\frac {x^{n} a u}{x}} \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 {x^{n} a}{x^{2}}+\frac {x^{n} n a}{x^{2}}\\ f_1 f_2 &=0\\ f_2^2 f_0 &=-\frac {x^{2 n} a^{2} \left (-b +a \,b^{2} x^{n} \ln \left (x \right )^{2}\right )}{x^{3}} \end {align*}

Substituting the above terms back in equation (2) gives \begin {align*} \frac {x^{n} a u^{\prime \prime }\left (x \right )}{x}-\left (-\frac {x^{n} a}{x^{2}}+\frac {x^{n} n a}{x^{2}}\right ) u^{\prime }\left (x \right )-\frac {x^{2 n} a^{2} \left (-b +a \,b^{2} x^{n} \ln \left (x \right )^{2}\right ) u \left (x \right )}{x^{3}} &=0 \end {align*}

Solving the above ODE (this ode solved using Maple, not this program), gives

\[ u \left (x \right ) = \operatorname {DESol}\left (\left \{\textit {\_Y}^{\prime \prime }\left (x \right )-\frac {\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right )}{x}-\frac {x^{n} a \left (-b +a \,b^{2} x^{n} \ln \left (x \right )^{2}\right ) \textit {\_Y} \left (x \right )}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right ) \] The above shows that \[ u^{\prime }\left (x \right ) = \frac {\partial }{\partial x}\operatorname {DESol}\left (\left \{\textit {\_Y}^{\prime \prime }\left (x \right )-\frac {\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right )}{x}-\frac {x^{n} a \left (-b +a \,b^{2} x^{n} \ln \left (x \right )^{2}\right ) \textit {\_Y} \left (x \right )}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right ) \] Using the above in (1) gives the solution \[ y = -\frac {\left (\frac {\partial }{\partial x}\operatorname {DESol}\left (\left \{\textit {\_Y}^{\prime \prime }\left (x \right )-\frac {\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right )}{x}-\frac {x^{n} a \left (-b +a \,b^{2} x^{n} \ln \left (x \right )^{2}\right ) \textit {\_Y} \left (x \right )}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )\right ) x \,x^{-n}}{a \operatorname {DESol}\left (\left \{\textit {\_Y}^{\prime \prime }\left (x \right )-\frac {\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right )}{x}-\frac {x^{n} a \left (-b +a \,b^{2} x^{n} \ln \left (x \right )^{2}\right ) \textit {\_Y} \left (x \right )}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )} \] Dividing both numerator and denominator by \(c_{1}\) gives, after renaming the constant \(\frac {c_{2}}{c_{1}}=c_{3}\) the following solution

\[ y = -\frac {x^{1-n} \left (\frac {\partial }{\partial x}\operatorname {DESol}\left (\left \{\frac {\textit {\_Y}^{\prime \prime }\left (x \right ) x^{2}-\ln \left (x \right )^{2} x^{2 n} \textit {\_Y} \left (x \right ) a^{2} b^{2}-\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right ) x +x^{n} \textit {\_Y} \left (x \right ) a b}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )\right )}{a \operatorname {DESol}\left (\left \{\frac {\textit {\_Y}^{\prime \prime }\left (x \right ) x^{2}-\ln \left (x \right )^{2} x^{2 n} \textit {\_Y} \left (x \right ) a^{2} b^{2}-\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right ) x +x^{n} \textit {\_Y} \left (x \right ) a b}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )} \]

Summary

The solution(s) found are the following \begin{align*} \tag{1} y &= -\frac {x^{1-n} \left (\frac {\partial }{\partial x}\operatorname {DESol}\left (\left \{\frac {\textit {\_Y}^{\prime \prime }\left (x \right ) x^{2}-\ln \left (x \right )^{2} x^{2 n} \textit {\_Y} \left (x \right ) a^{2} b^{2}-\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right ) x +x^{n} \textit {\_Y} \left (x \right ) a b}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )\right )}{a \operatorname {DESol}\left (\left \{\frac {\textit {\_Y}^{\prime \prime }\left (x \right ) x^{2}-\ln \left (x \right )^{2} x^{2 n} \textit {\_Y} \left (x \right ) a^{2} b^{2}-\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right ) x +x^{n} \textit {\_Y} \left (x \right ) a b}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )} \\ \end{align*}

Verification of solutions

\[ y = -\frac {x^{1-n} \left (\frac {\partial }{\partial x}\operatorname {DESol}\left (\left \{\frac {\textit {\_Y}^{\prime \prime }\left (x \right ) x^{2}-\ln \left (x \right )^{2} x^{2 n} \textit {\_Y} \left (x \right ) a^{2} b^{2}-\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right ) x +x^{n} \textit {\_Y} \left (x \right ) a b}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )\right )}{a \operatorname {DESol}\left (\left \{\frac {\textit {\_Y}^{\prime \prime }\left (x \right ) x^{2}-\ln \left (x \right )^{2} x^{2 n} \textit {\_Y} \left (x \right ) a^{2} b^{2}-\left (-1+n \right ) \textit {\_Y}^{\prime }\left (x \right ) x +x^{n} \textit {\_Y} \left (x \right ) a b}{x^{2}}\right \}, \left \{\textit {\_Y} \left (x \right )\right \}\right )} \] Verified OK.

7.6.2 Maple step by step solution

\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & y^{\prime } x -a \,x^{n} y^{2}=b -a \,b^{2} x^{n} \ln \left (x \right )^{2} \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 1 \\ {} & {} & y^{\prime } \\ \bullet & {} & \textrm {Solve for the highest derivative}\hspace {3pt} \\ {} & {} & y^{\prime }=\frac {a \,x^{n} y^{2}+b -a \,b^{2} x^{n} \ln \left (x \right )^{2}}{x} \end {array} \]

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) = (n-1)*(diff(y(x), x))/x+x^(n-1)*a*b*(x^(n-1)*b*a*ln(x)^2*x-1)*y(x)/x, 
      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 
            trying symmetries linear in x and y(x) 
            trying to convert to a linear ODE with constant coefficients 
      <- 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 
         -> 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 
               trying symmetries linear in x and y(x) 
               trying to convert to a linear ODE with constant coefficients 
         <- 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)-(x^(n-1)*a*y(x)^2+y(x)+x^2*(-x^(n-1)*b^2*a*ln(x)^2+b/x))/x, y(x), explicit` 
      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`
 

Solution by Maple

dsolve(x*diff(y(x),x)=a*x^n*y(x)^2+b-a*b^2*x^n*(ln(x))^2,y(x), singsol=all)
 

\[ \text {No solution found} \]

Solution by Mathematica

Time used: 0.0 (sec). Leaf size: 0

DSolve[x*y'[x]==a*x^n*y[x]^2+b-a*b^2*x^n*(Log[x])^2,y[x],x,IncludeSingularSolutions -> True]
 

Not solved