2.5.5 Problem 7
Internal
problem
ID
[19734]
Book
:
Elementary
Differential
Equations.
By
Thornton
C.
Fry.
D
Van
Nostrand.
NY.
First
Edition
(1929)
Section
:
Chapter
IV.
Methods
of
solution:
First
order
equations.
section
32.
Problems
at
page
89
Problem
number
:
7
Date
solved
:
Friday, November 28, 2025 at 06:41:53 PM
CAS
classification
:
[_quadrature]
Solved using first_order_ode_parametric method
Time used: 1.180 (sec)
Solve
\begin{align*}
{y^{\prime }}^{2} \left (x^{2}-1\right )&=1 \\
\end{align*}
Let
\(y^{\prime }\) be a parameter
\(\lambda \). The ode becomes
\begin{align*} \lambda ^{2} \left (x^{2}-1\right )-1 = 0 \end{align*}
Isolating \(x\) gives
\begin{align*} x = \frac {\sqrt {\lambda ^{2}+1}}{\lambda }\\ x = F \left (y , \lambda \right ) \end{align*}
Now we generate an ode in \(y \left (\lambda \right )\) using
\begin{align*} \frac {d}{d \lambda }y \left (\lambda \right ) &= \frac { \lambda \frac {\partial F}{\partial \lambda }} { 1- \frac {\partial F}{\partial y} } \\ &= \lambda \left (\frac {1}{\sqrt {\lambda ^{2}+1}}-\frac {\sqrt {\lambda ^{2}+1}}{\lambda ^{2}}\right )\\ &= -\frac {1}{\lambda \sqrt {\lambda ^{2}+1}} \end{align*}
Which is now solved for \(y\).
Solve Since the ode has the form \(\frac {d}{d \lambda }y \left (\lambda \right )=f(\lambda )\), then we only need to integrate \(f(\lambda )\).
\begin{align*} \int {dy} &= \int {-\frac {1}{\lambda \sqrt {\lambda ^{2}+1}}\, d\lambda }\\ y \left (\lambda \right ) &= \operatorname {arctanh}\left (\frac {1}{\sqrt {\lambda ^{2}+1}}\right ) + c_1 \end{align*}
Now that we have found solution \(y\), we have two equations with parameter \(\lambda \). They are
\begin{align*}
y &= \operatorname {arctanh}\left (\frac {1}{\sqrt {\lambda ^{2}+1}}\right )+c_1 \\
x &= \frac {\sqrt {\lambda ^{2}+1}}{\lambda } \\
\end{align*}
Eliminating
\(\lambda \)
gives the solution for
\(y\). Solving for
\(y\) gives
\begin{align*}
y &= \operatorname {arctanh}\left (\frac {1}{\sqrt {\frac {x^{2}}{x^{2}-1}}}\right )+c_1 \\
\end{align*}
Summary of solutions found
\begin{align*}
y &= \operatorname {arctanh}\left (\frac {1}{\sqrt {\frac {x^{2}}{x^{2}-1}}}\right )+c_1 \\
\end{align*}
✓ Maple. Time used: 0.019 (sec). Leaf size: 33
ode:=diff(y(x),x)^2*(x^2-1) = 1;
dsolve(ode,y(x), singsol=all);
\begin{align*}
y &= \ln \left (x +\sqrt {x^{2}-1}\right )+c_1 \\
y &= -\ln \left (x +\sqrt {x^{2}-1}\right )+c_1 \\
\end{align*}
Maple trace
Methods for first order ODEs:
-> Solving 1st order ODE of high degree, 1st attempt
trying 1st order WeierstrassP solution for high degree ODE
trying 1st order WeierstrassPPrime solution for high degree ODE
trying 1st order JacobiSN solution for high degree ODE
trying 1st order ODE linearizable_by_differentiation
trying differential order: 1; missing variables
<- differential order: 1; missing y(x) successful
Maple step by step
\[ \begin {array}{lll} & {} & \textrm {Let's solve}\hspace {3pt} \\ {} & {} & \left (x^{2}-1\right ) \left (\frac {d}{d x}y \left (x \right )\right )^{2}=1 \\ \bullet & {} & \textrm {Highest derivative means the order of the ODE is}\hspace {3pt} 1 \\ {} & {} & \frac {d}{d x}y \left (x \right ) \\ \bullet & {} & \textrm {Solve for the highest derivative}\hspace {3pt} \\ {} & {} & \left [\frac {d}{d x}y \left (x \right )=\frac {1}{\sqrt {x^{2}-1}}, \frac {d}{d x}y \left (x \right )=-\frac {1}{\sqrt {x^{2}-1}}\right ] \\ \square & {} & \textrm {Solve the equation}\hspace {3pt} \frac {d}{d x}y \left (x \right )=\frac {1}{\sqrt {x^{2}-1}} \\ {} & \circ & \textrm {Integrate both sides with respect to}\hspace {3pt} x \\ {} & {} & \int \left (\frac {d}{d x}y \left (x \right )\right )d x =\int \frac {1}{\sqrt {x^{2}-1}}d x +\textit {\_C1} \\ {} & \circ & \textrm {Evaluate integral}\hspace {3pt} \\ {} & {} & y \left (x \right )=\ln \left (x +\sqrt {x^{2}-1}\right )+\textit {\_C1} \\ \square & {} & \textrm {Solve the equation}\hspace {3pt} \frac {d}{d x}y \left (x \right )=-\frac {1}{\sqrt {x^{2}-1}} \\ {} & \circ & \textrm {Integrate both sides with respect to}\hspace {3pt} x \\ {} & {} & \int \left (\frac {d}{d x}y \left (x \right )\right )d x =\int -\frac {1}{\sqrt {x^{2}-1}}d x +\textit {\_C1} \\ {} & \circ & \textrm {Evaluate integral}\hspace {3pt} \\ {} & {} & y \left (x \right )=-\ln \left (x +\sqrt {x^{2}-1}\right )+\textit {\_C1} \\ \bullet & {} & \textrm {Set of solutions}\hspace {3pt} \\ {} & {} & \left \{y \left (x \right )=-\ln \left (x +\sqrt {x^{2}-1}\right )+\mathit {C1} , y \left (x \right )=\ln \left (x +\sqrt {x^{2}-1}\right )+\mathit {C1} \right \} \end {array} \]
✓ Mathematica. Time used: 0.003 (sec). Leaf size: 41
ode=(x^2-1)*D[y[x],x]^2==1;
ic={};
DSolve[{ode,ic},y[x],x,IncludeSingularSolutions->True]
\begin{align*} y(x)&\to -\log \left (\sqrt {x^2-1}+x\right )+c_1\\ y(x)&\to \log \left (\sqrt {x^2-1}+x\right )+c_1 \end{align*}
✓ Sympy. Time used: 0.639 (sec). Leaf size: 41
from sympy import *
x = symbols("x")
y = Function("y")
ode = Eq((x**2 - 1)*Derivative(y(x), x)**2 - 1,0)
ics = {}
dsolve(ode,func=y(x),ics=ics)
\[
\left [ y{\left (x \right )} = C_{1} - \begin {cases} \log {\left (x + \sqrt {x^{2} - 1} \right )} & \text {for}\: x > -1 \wedge x < 1 \end {cases}, \ y{\left (x \right )} = C_{1} + \begin {cases} \log {\left (x + \sqrt {x^{2} - 1} \right )} & \text {for}\: x > -1 \wedge x < 1 \end {cases}\right ]
\]