Clairaut's equation

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In mathematical analysis, Clairaut's equation (or the Clairaut equation) is a differential equation of the form

[math]\displaystyle{ y(x)=x\frac{dy}{dx}+f\left(\frac{dy}{dx}\right) }[/math]

where [math]\displaystyle{ f }[/math] is continuously differentiable. It is a particular case of the Lagrange differential equation. It is named after the French mathematician Alexis Clairaut, who introduced it in 1734.[1]

Solution

To solve Clairaut's equation, one differentiates with respect to [math]\displaystyle{ x }[/math], yielding

[math]\displaystyle{ \frac{dy}{dx}=\frac{dy}{dx}+x\frac{d^2 y}{dx^2}+f'\left(\frac{dy}{dx}\right)\frac{d^2 y}{dx^2}, }[/math]

so

[math]\displaystyle{ \left[x+f'\left(\frac{dy}{dx}\right)\right]\frac{d^2 y}{dx^2} = 0. }[/math]

Hence, either

[math]\displaystyle{ \frac{d^2 y}{dx^2} = 0 }[/math]

or

[math]\displaystyle{ x+f'\left(\frac{dy}{dx}\right) = 0. }[/math]

In the former case, [math]\displaystyle{ C = dy/dx }[/math] for some constant [math]\displaystyle{ C }[/math]. Substituting this into the Clairaut's equation, one obtains the family of straight line functions given by

[math]\displaystyle{ y(x)=Cx+f(C),\, }[/math]

the so-called general solution of Clairaut's equation.

The latter case,

[math]\displaystyle{ x+f'\left(\frac{dy}{dx}\right) = 0, }[/math]

defines only one solution [math]\displaystyle{ y(x) }[/math], the so-called singular solution, whose graph is the envelope of the graphs of the general solutions. The singular solution is usually represented using parametric notation, as [math]\displaystyle{ (x(p), y(p)) }[/math], where [math]\displaystyle{ p = dy/dx }[/math].

The parametric description of the singular solution has the form

[math]\displaystyle{ x(t)= -f'(t),\, }[/math]
[math]\displaystyle{ y(t)= f(t) - tf'(t),\, }[/math]

where [math]\displaystyle{ t }[/math] is a parameter.

Examples

The following curves represent the solutions to two Clairaut's equations:

In each case, the general solutions are depicted in black while the singular solution is in violet.

Extension

By extension, a first-order partial differential equation of the form

[math]\displaystyle{ \displaystyle u=xu_x+yu_y+f(u_x,u_y) }[/math]

is also known as Clairaut's equation.[2]

See also

Notes

References

  • Kamke, E. (1944) (in de), Differentialgleichungen: Lösungen und Lösungsmethoden, 2. Partielle Differentialgleichungen 1er Ordnung für eine gesuchte Funktion, Akad. Verlagsgesell .