• Sonuç bulunamadı

2.4. Exact Di¤erential Equations

N/A
N/A
Protected

Academic year: 2021

Share "2.4. Exact Di¤erential Equations"

Copied!
3
0
0

Yükleniyor.... (view fulltext now)

Tam metin

(1)

CHAPTER 2. FIRST ORDER DIFFERENTIAL EQUATIONS

2.4. Exact Di¤erential Equations

De…nition. Let F be a function of two real variables such that F has continuous

…rst partial derivatives in a domain D: The total di¤erential dF of the function F is de…ned by the formula

dF (x; y) = @F (x; y)

@x dx + @F (x; y)

@y dy for all (x; y) 2 D:

De…nition The di¤erential form

M (x; y)dx + N (x; y)dy (1)

is called an exact di¤erential in a domain D if there exists a function F of two real variables such that this expression equals the total di¤erential dF (x; y) for all (x; y) 2 D:

That is, expression (1) is an exact di¤erential in D if there exists a function F such that

@F (x; y)

@x = M (x; y) and @F (x; y)

@y = N (x; y) for all (x; y) 2 D:

If M (x; y)dx + N (x; y)dy is an exact di¤erential, then the di¤erential equation M (x; y)dx + N (x; y)dy = 0

is called an exact di¤erential equation.

Theorem. Consider the di¤erential equation

M (x; y)dx + N (x; y)dy = 0; (2)

where M and N have continuous …rst partial derivatives at all points (x; y) in a rectangular domain D: The di¤erential equation (2) is exact if and only if

@M (x; y)

@y = @N (x; y)

@x for all (x; y) 2 D:

Example. Solve the following di¤erential equations.

1)

(3x

2

+ 4xy)dx + (2x

2

+ 2y)dy = 0:

1

(2)

Solution. We observe that the equation is exact since

@M (x; y)

@y = @N (x; y)

@x = 4x:

So, there exists a function F (x; y) such that

@F

@x = 3x

2

+ 4xy (3)

@F

@y = 2x

2

+ 2y (4)

Thus, from (3); we get

F (x; y) = x

3

+ 2x

2

y + h(y) (5) Using (4)and (5); we get

@F

@y = 2x

2

+ 2y = 2x

2

+ h

0

(y): (6) From (6) we obtain h

0

(y) = 2y and h(y) = y

2

+ c

1

: So, we obtain F (x; y) = x

3

+ 2x

2

y + y

2

+ c

1

and the solution of given di¤erential equation

x

3

+ 2x

2

y + y

2

= c:

2)

(2x cos y + 3x

2

y)dx + (x

3

x

2

sin y y) = 0; y(0) = 2:

3)

(ye

xy

tan x + e

xy

sec

2

x)dx + xe

xy

tan xdy = 0:

2.5. Integrating Factor

Consider the following di¤erential equation

M (x; y)dx + N (x; y)dy = 0 (1)

De…nition. If the di¤erential equation (1) is not exact but the di¤erential equation

(x; y)M (x; y)dx + (x; y)N (x; y)dy = 0

is exact,then (x; y) is called an integrating factor of the di¤erential equation (1).

Theorem. (i)If

M

y

N

x

N

2

(3)

depends on x only, then

(x) = exp

Z M

y

N

x

N dx

is an integrating factor.

(ii)

M

y

N

x

M depends on y only, then

(y) = exp

Z M

y

N

x

M dy

is an integrating factor.

Example. Solve the following di¤erential equations.

1)

(x

2

+ y

2

+ x)dx + xydy = 0

Solution. Let us …rst observe that this equation is not exact. It is clear that M

y

= 2y, N

x

= y and

M

y

N

x

N = 1

x :

So there exists and integrating factor which depends on x: Integrating factor is calcu¸ sated as

(x) = exp

Z M

y

N

x

N dx = x:

Multiplying equation by we obtain the equation (x

3

+ xy

2

+ x

2

)dx + x

2

ydy = 0

which is exact. Now, we have to …nd the function F (x; y) such that

@F

@x = x

3

+ xy

2

+ x

2

(i)

@F

@y = x

2

y (ii)

Integrating (i); we get F (x; y) = x

4

4 + x

2

y

2

2 + x

3

3 + h(y) (iii)

Taking the derivative of (iii) with respect to y and using (ii); we obtain the solution of di¤erential equation

3x

4

+ 6x

2

y

2

+ 4x

3

= c 2)

(2xy

2

3y

3

)dx + (7 3xy

2

)dy = 0 3)

(2xy

3

2x

3

y

3

4xy

2

+ 2x)dx + (3x

2

y

2

+ 4y)dy = 0

3

Referanslar

Benzer Belgeler

If is taken as an arbitrary function, it is not always possible to eliminate the constant a between equations (5), so it is generally not possible to express the general integral of

It is not necessary to use all of the equations (5) for a …rst integral to be found from system (5), known as Charpit equations.. However, in the …rst integral we will …nd, at least

In this section, we will examine the special types of …rst-order partial di¤er- ential equations that can be easily solved with the Charpit

They can be di¤erent

A solution of (6) obtained from a general solution of equation (6) by giving particular values to one or more of the n arbitrary constants is called a particular

If the functions M and N in equation (1) are both homogeneous with same degree, then the di¤erential equation (1) is called

First Order Linear Di¤erential

We note that a di¤erential equation which looks di¤erent from any of those that we have studied, may be solved easily by a change of variables. However, we can not give