Talk:PlanetPhysics/Ordinary Differential Equations Definitions

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The term \htmladdnormallink{differential equation}{http://planetphysics.us/encyclopedia/DifferentialEquations.html} was first used by Leibniz in 1676 to denote a relationship between the

differentials $dx$ and $dy$ of two variables $x$ and $y$. Such a relationship, in general, explicitly involves the variables $x$ and $y$ together with other symbols $a, b, c, ...$ which represent constants.

This restricted use of the term was soon abandoned; differential equations are now understood to include any algebraical or transcendental equalities which involve either differentials or differential coefficients. It is to be under- stood, however, that the differential equation is not an \htmladdnormallink{identity}{http://planetphysics.us/encyclopedia/Cod.html}.

Differential equations are classified, in the first place, according to the number of variables which they involve. An \htmladdnormallink{ordinary differential equation}{http://planetphysics.us/encyclopedia/DifferentialEquations.html} expresses a \htmladdnormallink{relation}{http://planetphysics.us/encyclopedia/Bijective.html} between an independent variable, a dependent variable and one or more differential coefficients of the dependent with respect to the independent variable. A \htmladdnormallink{partial differential equation}{http://planetphysics.us/encyclopedia/DifferentialEquations.html} involves one dependent and two or more independent variables, together with partial differential coefficients of the dependent with respect to the independent variables. A total differential equation contains two or more dependent variables together with their differentials or differential coefficients with respect to a single independent variable which may, or may not, enter explicitly into the equation.

The order of a differential equation is the order of the highest differential coefficient which is involved. When an equation is polynomial in all the differential coefficients involved, the \htmladdnormallink{power}{http://planetphysics.us/encyclopedia/Power.html} to which the highest differential coefficient is raised is known as the degree of the equation. When, in an ordinary or partial differential equation, the dependent variable and its derivatives occur lo the first degree only, and not as higher powers or products, the equation is said to be linear. The coefficients of a linear equation are therefore either constants or \htmladdnormallink{functions}{http://planetphysics.us/encyclopedia/Bijective.html} of the independent variable or variables.

Thus, for example,

$$ \frac{d^2 y}{dx^2} + y = x^3$$

is an ordinary linear equation of the second order;

$$(x+y)^2 \frac{dy}{dx} = 1$$

is an ordinary \htmladdnormallink{non-linear equation}{http://planetphysics.us/encyclopedia/ErmakovLewisInvariants.html} of the first order and the first degree;

$$x \frac{\partial z}{\partial x} + y\frac{\partial z}{\partial y} - z = 0$$

is a linear partial differential equation of the first order in two independent variables;

$$ \frac{\partial^2 V}{\partial x^2} + \frac{\partial^2 V}{\partial y^2} + \frac{\partial^2 V}{\partial z^2} = 0$$

is a linear partial differential equation of the second order in three independent variables;

$$ \frac{\partial^2 z}{\partial x^2} \frac{\partial^2 z}{\partial y^2} - \left ( \frac{\partial^2 z}{\partial x \partial y} \right )^2 = 0 $$

is a non-linear partial differential equation of the second order and the second degree in two independent variables;

$$u dx + v dy + w dz = 0$$

where $u,v,$ and $w$ are functions of $x,y$ and $z$, is a total differential equation of the first order and the first degree, and

$$ x^2 dx^2 + 2xydxdy + y^2dy^2-z^2dz^2=0 $$

is a total differential equation of the first order and the second degree.

In the case of a total differential equation any one of the variables may be regarded as independent and the remainder as dependent, thus, taking $x$ as independent variable, the equation

$$u dx + v dy + w dz = 0$$

may be written

$$u + v \frac{dy}{dx} + w\frac{dz}{dx}=0$$

or an auxiliary variable $t$ may be introduced and the original variables regarded as functions of $t$, thus

$$u \frac{dx}{dt} + v\frac{dy}{dt} + w\frac{dz}{dt}=0$$

\subsection{References}

[1] Ince, E.L. "Ordinary Differential Equations." London and New York, Longmans, Green, 1920.

This entry is a derivative of the Public \htmladdnormallink{domain}{http://planetphysics.us/encyclopedia/Bijective.html} \htmladdnormallink{work}{http://planetphysics.us/encyclopedia/Work.html} [1].

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