First-order differential equation: Difference between revisions

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| [[first-order linear differential equation]] which in simplified form looks like <math>y' + p(x)y = q(x)</math> || 1 || Use the [[integrating factor]] <math>e^{H(x)}</math> where <math>H'=p</math>. The general solution is <math>y = Ce^{-H(x)} + e^{-H(x)}\int p(x)e^{H(x)} \, dx</math>
| [[first-order linear differential equation]] which in simplified form looks like <math>y' + p(x)y = q(x)</math> || 1 || Use the [[integrating factor]] <math>e^{H(x)}</math> where <math>H'=p</math>. The general solution is <math>y = Ce^{-H(x)} + e^{-H(x)}\int p(x)e^{H(x)} \, dx</math>
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| [[separable differential equation]] which is of the form <math>y' = f(x)g(y)</math> (any first-order [[autonomous differential equation]] is separable, though there are separable differential equations that aren't autonomous) || 1 || Separate and solve as <math>\int \frac{dy}{g(y)} = \int f(x) \, dx</math>. Also find solutions corresponding to <math>y = k</math> where <math>g(k) = 0</math>.
| [[separable differential equation]] which is of the form <math>y' = f(x)g(y)</math> (any [[first-order first-degree autonomous differential equation]] is separable, though there are separable differential equations that aren't autonomous) || 1 || Separate and solve as <math>\int \frac{dy}{g(y)} = \int f(x) \, dx</math>. Also find solutions corresponding to <math>y = k</math> where <math>g(k) = 0</math>.
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| [[Clairaut's equation]] which is of the form <math>y = xy' + f(y')</math> || need not be polynomial; if polynomial, may have any degree || <math>y = Cx + f(C)</math> with <math>C \in \R</math> (all straight lines) and a single other solution explicitly described as the solution to <math>x + f(dy/dx) = 0</math>, given by <math>x = -f'(p), y = f(p) - pf'(p)</math> as a parametric curve in terms of <math>p</math>.  
| [[Clairaut's equation]] which is of the form <math>y = xy' + f(y')</math> || need not be polynomial; if polynomial, may have any degree || <math>y = Cx + f(C)</math> with <math>C \in \R</math> (all straight lines) and a single other solution explicitly described as the solution to <math>x + f(dy/dx) = 0</math>, given by <math>x = -f'(p), y = f(p) - pf'(p)</math> as a parametric curve in terms of <math>p</math>.  
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Revision as of 19:09, 1 July 2012

Definition

Formal description

The term first-order differential equation is used for any differential equation whose order is 1. In other words, it is a differential equation of the form:

F(x,y,y)=0

where F is an expression (function) involving three variables. Note that F must make use of y (also written as dy/dx), but it could ignore x or y.

The theory and terminology follows that for the general concept of differential equation.

Solution concept

  • Functional solution: A function f on the domain of interest is said to be a solution (or functional solution) to the equation if, when we plug in y=f(x), the equation holds true for all x in the domain, i.e.:

F(x,f(x),f(x))=0xdom(f)

Note that in cases of functions defined on closed intervals, we exclude checking the conditions on the boundary of the domain because two-sided derivatives don't make sense at the boundary.

  • Relational solution: A relation R(x,y)=0 is termed a relational solution to the equation if F(x,y,y)=0 holds true for all x,y if we calculate the derivative y using implicit differentiation.

Initial value problem

An initial value problem is a first-order differential equation

F(x,y,y)=0

along with a point (x0,y0).

A functional solution to the initial value problem is a solution y=f(x) to the first-order differential equation such that f(x0)=y0.

A relational solution to the initial value problem is a solution R(x,y)=0 to the first-order differential equation such that R(x0,y0)=0.

Terminology

Solution terminology

Term Meaning Example
particular solution a function or relation that is a solution for the equation (see #Solution concept). A solution in the form of a function y=f(x) is termed a functional solution and a solution in the form of a relation R(x,y)=0 is termed a relational solution. y=sinx is a functional solution to y2+y'2=1.
solution family a family of functions or relations, with one or more parameters possibly subject to some constraints, such that for every choice of parameter values subject to those constraints, we get a particular solution. y=sin(x+C) with parameter CR, is a solution family for y2+y'2=1.
general solution a solution family that covers all solutions (or almost all solutions, possibly excluding some exceptions) The general solution to y=0 is y=C,CR.
solution to initial value problem a particular solution that satisfies the initial value condition. A particular solution to y+y=0 satisfying y(0)=1 is y=ex.

Facts

  • As a general principle, the way to solve a first-order differential equation is to convert it to an integration problem. The additive +C appearing in the indefinite integration gives the freely varying parameter for the solution family.
  • As a general principle, the number of degrees of freedom (i.e., the number of independent freely varying parameters) in the general solution to a first-order differential equation is 1. In other words, we expect the solution space to be one-dimensional.
  • As a general principle, the number of solutions to an initial value problem should be finite. If the differential equation is nice enough, then there should be a unique solution to any initial value problem.

Geometric description of solutions

This geometric description is qualitatively different for first-order differential equations compared to higher-order differential equations.

A solution curve to a differential equation is a curve in the xy-plane corresponding to any solution to the differential equation. For instance, if R(x,y)=0 is a relational solution, then the curve R(x,y)=0 gives a solution curve for the differential equation.

For first-order differential equations, we generally expect that specifying a point on the curve uniquely determines the solution curve (because that's an initial value specification). Thus, the solution curves are expected to be (mostly) non-intersecting curves that (hopefully) cover the plane or a large part of the plane.

Solution strategies

Solution strategies in particular cases

Below are some formats of equations for which general strategies are known. Note that the letter f is no longer used for the solution function but may be used for other functions.:

Equation type Degree (if polynomial in highest order derivative) Quick summary of solution strategy
first-order linear differential equation which in simplified form looks like y+p(x)y=q(x) 1 Use the integrating factor eH(x) where H=p. The general solution is y=CeH(x)+eH(x)p(x)eH(x)dx
separable differential equation which is of the form y=f(x)g(y) (any first-order first-degree autonomous differential equation is separable, though there are separable differential equations that aren't autonomous) 1 Separate and solve as dyg(y)=f(x)dx. Also find solutions corresponding to y=k where g(k)=0.
Clairaut's equation which is of the form y=xy+f(y) need not be polynomial; if polynomial, may have any degree y=Cx+f(C) with CR (all straight lines) and a single other solution explicitly described as the solution to x+f(dy/dx)=0, given by x=f(p),y=f(p)pf(p) as a parametric curve in terms of p.