First-order linear differential equation: Difference between revisions

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(Created page with "==Definition== ===Format of the differential equation=== A '''first-order linear differential equation''' is a differential equation of the form: <math>\frac{dy}{dx} + p(x)...")
 
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{{quotation|<math>y = e^{-H(x)}\int q(x)e^{H(x)} \, dx</math> where <math>H</math> is an antiderivative of <math>p</math>.}}
{{quotation|<math>y = e^{-H(x)}\int q(x)e^{H(x)} \, dx</math> where <math>H</math> is an antiderivative of <math>p</math>.}}
In particular, we obtain that:
<math>\mbox{General solution} = \mbox{Particular solution} + Ce^{-H(x)}, C \in \R</math>


The function <math>e^{H(x)}</math> is termed the [[integrating factor]] for the differential equation because multiplying by this turns the differential equation into an exact differential equation, i.e., a differential equation to which we can apply integration on both sides.
The function <math>e^{H(x)}</math> is termed the [[integrating factor]] for the differential equation because multiplying by this turns the differential equation into an exact differential equation, i.e., a differential equation to which we can apply integration on both sides.

Revision as of 22:54, 12 February 2012

Definition

Format of the differential equation

A first-order linear differential equation is a differential equation of the form:

where are known functions.

Solution method and formula: indefinite integral version

Let be an antiderivative for , so that . Then, we multiply both sides by . Simplifying, we get:

Integrating, we get:

Rearranging, we get:

where is an antiderivative of .

In particular, we obtain that:

The function is termed the integrating factor for the differential equation because multiplying by this turns the differential equation into an exact differential equation, i.e., a differential equation to which we can apply integration on both sides.