Difference between revisions of "Clairaut equation"
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An ordinary first-order differential equation not solved with respect to its derivative: | An ordinary first-order differential equation not solved with respect to its derivative: | ||
− | + | $$y=xy'+f(y'),\tag{1}$$ | |
− | where | + | where $f(t)$ is a non-linear function. Equation \ref{1} is named after A. Clairaut [[#References|[1]]] who was the first to point out the difference between the general and the singular solutions of an equation of this form. The Clairaut equation is a particular case of the [[Lagrange equation|Lagrange equation]]. |
− | If | + | If $f(t)\in C^1(a,b)$ and $f'(t)\neq0$ when $t\in(a,b)$, then the set of integral curves (cf. [[Integral curve|Integral curve]]) of \ref{1} consists of: a parametrically given curve |
− | + | $$x=-f'(t),\quad y=-tf'(t)+f(t),\quad a<t<b;\tag{2}$$ | |
a one-parameter family of straight lines | a one-parameter family of straight lines | ||
− | + | $$y=Cx+f(C),\quad C\in(a,b),\tag{3}$$ | |
− | tangent to the curve | + | tangent to the curve \ref{2}; curves consisting of an arbitrary segment of the curve \ref{2} and the two straight lines of the family \ref{3} tangent to \ref{2} at each end of this segment. The family \ref{3} forms the [[General solution|general solution]], while the curve \ref{2}, which is the [[Envelope|envelope]] of the family \ref{3}, is the [[Singular solution|singular solution]] (see [[#References|[2]]]). A family of tangents to a smooth non-linear curve satisfies a Clairaut equation. Therefore, geometric problems in which it is required to determine a curve in terms of a prescribed property of its tangents (common to all points of the curve) leads to a Clairaut equation. |
The following first-order partial differential equation is also called a Clairaut equation: | The following first-order partial differential equation is also called a Clairaut equation: | ||
− | + | $$z=x\frac{\partial z}{\partial x}+y\frac{\partial z}{\partial y}+f\left(\frac{\partial z}{\partial x},\frac{\partial z}{\partial y}\right);$$ | |
it has the integral | it has the integral | ||
− | + | $$x=\alpha x+\beta y+f(\alpha,\beta),$$ | |
− | where | + | where $(\alpha,\beta)$ is an arbitrary point of the domain of definition of the function $f(p,q)$ (see [[#References|[3]]]). |
====References==== | ====References==== | ||
− | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> A. Clairaut, ''Histoire Acad. R. Sci. Paris (1734)'' (1736) pp. 196–215</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> V.V. Stepanov, "A course of differential equations" , Moscow (1959) (In Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> E. Kamke, "Differentialgleichungen: Lösungen und Lösungsmethoden" , '''2. Partielle Differentialgleichungen | + | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> A. Clairaut, ''Histoire Acad. R. Sci. Paris (1734)'' (1736) pp. 196–215</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> V.V. Stepanov, "A course of differential equations" , Moscow (1959) (In Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> E. Kamke, "Differentialgleichungen: Lösungen und Lösungsmethoden" , '''2. Partielle Differentialgleichungen $\mathbf{1^\text{er}}$ Ordnung für eine gesuchte Funktion''' , Akad. Verlagsgesell. (1944)</TD></TR></table> |
Revision as of 13:44, 10 August 2014
An ordinary first-order differential equation not solved with respect to its derivative:
$$y=xy'+f(y'),\tag{1}$$
where $f(t)$ is a non-linear function. Equation \ref{1} is named after A. Clairaut [1] who was the first to point out the difference between the general and the singular solutions of an equation of this form. The Clairaut equation is a particular case of the Lagrange equation.
If $f(t)\in C^1(a,b)$ and $f'(t)\neq0$ when $t\in(a,b)$, then the set of integral curves (cf. Integral curve) of \ref{1} consists of: a parametrically given curve
$$x=-f'(t),\quad y=-tf'(t)+f(t),\quad a<t<b;\tag{2}$$
a one-parameter family of straight lines
$$y=Cx+f(C),\quad C\in(a,b),\tag{3}$$
tangent to the curve \ref{2}; curves consisting of an arbitrary segment of the curve \ref{2} and the two straight lines of the family \ref{3} tangent to \ref{2} at each end of this segment. The family \ref{3} forms the general solution, while the curve \ref{2}, which is the envelope of the family \ref{3}, is the singular solution (see [2]). A family of tangents to a smooth non-linear curve satisfies a Clairaut equation. Therefore, geometric problems in which it is required to determine a curve in terms of a prescribed property of its tangents (common to all points of the curve) leads to a Clairaut equation.
The following first-order partial differential equation is also called a Clairaut equation:
$$z=x\frac{\partial z}{\partial x}+y\frac{\partial z}{\partial y}+f\left(\frac{\partial z}{\partial x},\frac{\partial z}{\partial y}\right);$$
it has the integral
$$x=\alpha x+\beta y+f(\alpha,\beta),$$
where $(\alpha,\beta)$ is an arbitrary point of the domain of definition of the function $f(p,q)$ (see [3]).
References
[1] | A. Clairaut, Histoire Acad. R. Sci. Paris (1734) (1736) pp. 196–215 |
[2] | V.V. Stepanov, "A course of differential equations" , Moscow (1959) (In Russian) |
[3] | E. Kamke, "Differentialgleichungen: Lösungen und Lösungsmethoden" , 2. Partielle Differentialgleichungen $\mathbf{1^\text{er}}$ Ordnung für eine gesuchte Funktion , Akad. Verlagsgesell. (1944) |
Comments
References
[a1] | E.L. Ince, "Ordinary differential equations" , Dover, reprint (1956) |
Clairaut equation. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Clairaut_equation&oldid=32806