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Lecture Notes in Differential Equations - Bruce E. Shapiro

Lecture Notes in Differential Equations - Bruce E. Shapiro

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2 LESSON 1. BASIC CONCEPTS<br />

Ord<strong>in</strong>ary differential equations are further classified by type and degree.<br />

There are two types of ODE:<br />

• L<strong>in</strong>ear differential equations are those that can be written <strong>in</strong> a<br />

form such as<br />

a n (t)y (n) + a n−1 (t)y (n−1) + · · · + a 2 (t)y ′′ + a 1 (t)y ′ + a 0 (t) = 0 (1.4)<br />

where each a i (t) is either zero, constant, or depends only on t, and<br />

not on y.<br />

• Nonl<strong>in</strong>ear differential equations are any equations that cannot be<br />

written <strong>in</strong> the above form. In particular, these <strong>in</strong>clude all equations<br />

that <strong>in</strong>clude y, y ′ , y ′′ , etc., raised to any power (such as y 2 or (y ′ ) 3 );<br />

nonl<strong>in</strong>ear functions of y or any derivative to any order (such as s<strong>in</strong>(y)<br />

or e ty ; or any product or function of these.<br />

The order of a differential equation is the degree of the highest order<br />

derivative <strong>in</strong> it. Thus<br />

y ′′′ − 3ty 2 = s<strong>in</strong> t (1.5)<br />

is a third order (because of the y ′′′ ) nonl<strong>in</strong>ear (because of the y 2 ) differential<br />

equation. We will return to the concepts of degree and type of ODE later.<br />

Def<strong>in</strong>ition 1.1 (Standard Form). A differential equation is said to be<br />

<strong>in</strong> standard form if we can solve for dy/dx, i.e., there exists some function<br />

f(t, y) such that<br />

dy<br />

= f(t, y) (1.6)<br />

dt<br />

We will often want to rewrite a given equation <strong>in</strong> standard form so that we<br />

can identify the form of the function f(t, y).<br />

Example 1.1. Rewrite the differential equation t 2 y ′ +3ty = yy ′ <strong>in</strong> standard<br />

form and identify the function f(t, y).<br />

The goal here is to solve for y ′ :<br />

hence<br />

t 2 y ′ − yy ′ = −3ty<br />

⎫⎪ ⎬<br />

(t 2 − y)y ′ = −3ty<br />

y ′ =<br />

3ty<br />

(1.7)<br />

⎪ ⎭<br />

y − t 2<br />

f(t, y) =<br />

3ty<br />

y − t 2 (1.8)

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