Summary: first order differential equations, Summaries of Differential Equations

Summary: first order differential equations. Types discussed in class. 1. Separable equations. These are equations which may be written in the.

Typology: Summaries

2022/2023

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Summary: first order differential equations
Types discussed in class.
1. Separable equations. These are equations which may be written in the
form
y0=f(y)g(t).
To solve, you separate the variables:
1
f(y)dy =g(t)dt.
Then integrate, making sure to include one of the constants of integration:
Z1
f(y)dy =Zg(t)dt +c.
2. Linear equations. These are equations of this form:
y0+p(t)y=q(t).
To solve, make sure it’s in exactly this form, and multiply by the “inte-
grating factor” eRp(t)dt:
eRp(t)dty0+eRp(t)dtp(t)y=eRp(t)dt q(t).
Let I(t) denote the integrating factor: I(t) = eRp(t)dt . Then the left side
of the equation is the derivative of I(t)y:
(I(t)y)0=I(t)q(t).
Now integrate:
I(t)y=ZI(t)q(t)dt +c,
so
y=1
I(t)ZI(t)q(t)dt +c
I(t).
(I find it much easier to remember the procedure—multiply by eRp(t)dt
than to try to memorize this solution.)
1
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Summary: first order differential equations

Types discussed in class.

  1. Separable equations. These are equations which may be written in the form y′^ = f (y)g(t). To solve, you separate the variables:

1 f (y) dy = g(t)dt.

Then integrate, making sure to include one of the constants of integration: ∫ 1 f (y)

dy =

g(t)dt + c.

  1. Linear equations. These are equations of this form:

y′^ + p(t)y = q(t).

To solve, make sure it’s in exactly this form, and multiply by the “inte- grating factor” e

p(t)dt:

e

p(t)dty′ (^) + e

p(t)dtp(t)y = e

p(t)dtq(t).

Let I(t) denote the integrating factor: I(t) = e

p(t)dt. Then the left side of the equation is the derivative of I(t)y:

(I(t)y)′^ = I(t)q(t).

Now integrate: I(t)y =

I(t)q(t)dt + c,

so y =

I(t)

I(t)q(t)dt +

c I(t)

(I find it much easier to remember the procedure—multiply by e

p(t)dt— than to try to memorize this solution.)

Types not discussed in class. You won’t need to know these for any home- work or exams for this class, but they might come up in other courses.

  1. Homogeneous equations. (See Section 2.9.) (Warning: the word “ho- mogeneous” gets used in several different ways when studying differential equations.) A homogeneous equation is one of this form:

y′^ = f (x, y),

where the function f (x, y) depends only on the ratio y/x—say f (x, y) = (y/x)^2 + sin(3 y/x). In other words, it is an equation of the form

y′^ = F (y/x)

for some function F. Let v = y/x, so that y = vx. Then y′^ = v′x + v, and if you plug this in for y′^ and plug v in for y/x, you get

xv′^ + v = F (v).

This is separable: dv F (v) − v

dx x

So solve it for v, and then substitute back in for y: v = y/x.

  1. Bernoulli equations. (See problems 37–41 in Section 2.2.) These are a lot like linear equations; they are equations of this form:

y′^ + p(t)y = q(t)yn,

where n is any number except 0 or 1. (If n = 0, then y^0 = 1, so this is just a linear equation. If n = 1, then y^1 = y, so you can rewrite this as y′^ + [p(t) − q(t)]y = 0, which is a linear equation.) To solve it, make the substitution v = y^1 −n, so that v′^ = (1 − n)y−ny′; in other words, y−ny′^ = (^1) −^1 n v′. Multiply the original equation by y−n:

y−ny′^ + p(t)y^1 −n^ = q(t).

Now make the substitution with v: 1 1 − n

v′^ + p(t)v = q(t).

Multiply everything by 1 − n and you have a linear equation, which you can solve to find v. Once you have v, then use the equation y = v^1 /(1−n) to find y.