Books
in black and white
Main menu
Share a book About us Home
Books
Biology Business Chemistry Computers Culture Economics Fiction Games Guide History Management Mathematical Medicine Mental Fitnes Physics Psychology Scince Sport Technics
Ads

Elementary Differential Equations and Boundary Value Problems - Boyce W.E.

Boyce W.E. Elementary Differential Equations and Boundary Value Problems - John Wiley & Sons, 2001. - 1310 p.
Download (direct link): elementarydifferentialequations2001.pdf
Previous << 1 .. 21 22 23 24 25 26 < 27 > 28 29 30 31 32 33 .. 609 >> Next

In each of Problems 36 and 37 use the method of Problem 35 to solve the given differential equation.
y + ay = be-Xt
y + p(t)y = g(t).
(a) If g(t) is identically zero, show that the solution is
(i)
(ii)
where A is a constant.
(b) If g(t) is not identically zero, assume that the solution is of the form
(iii)
(iv)
36. - 2y = t2e2t
37. y + (1/ t)y = 3cos2t, t > 0
40
Chapter 2. First Order Differential Equations
2.2 Separable Equations
In Sections 1.2 and 2.1 we used a process of direct integration to solve first order linear equations of the form
= ay + b, (1)
dt
where a and b are constants. We will now show that this process is actually applicable to a much larger class of equations.
We will use x to denote the independent variable in this section rather than t for two reasons. In the first place, different letters are frequently used for the variables in a differential equation, and you should not become too accustomed to using a single pair. In particular, x often occurs as the independent variable. Further, we want to reserve t for another purpose later in the section.
The general first order equation is
dy
~f = f(x, y). (2)
dx
Linear equations were considered in the preceding section, but if Eq. (2) is nonlinear,
then there is no universally applicable method for solving the equation. Here, we
consider a subclass of first order equations for which a direct integration process can be used.
To identify this class of equations we first rewrite Eq. (2) in the form
dy
M(x, y) + N(x, y)JL = 0. (3)
dx
It is always possible to do this by setting M(x, y) = - f (x, y) and N(x, y) = 1, but
there may be other ways as well. In the event that M is a function of x only and N is a
function of y only, then Eq. (3) becomes
M(x) + N (y) df = 0. (4)
dx
Such an equation is said to be separable, because if it is written in the differential form
M(x) dx + N (y) dy = 0, (5)
then, if you wish, terms involving each variable may be separated by the equals sign. The differential form (5) is also more symmetric and tends to diminish the distinction between independent and dependent variables.
1 dy _ x2
Show that the equation
dy x2
(6)
dx 1 - y2
is separable, and then find an equation for its integral curves. If we write Eq. (6) as
-x2 + (1 - y2) dy = 0, (7)
dx
2.2 Separable Equations
41
then it has the form (4) and is therefore separable. Next, observe that the first term in Eq. (7) is the derivative of -x^ /3 and that the second term, by means of the chain rule, is the derivative with respect to x of y - y3/3. Thus Eq. (7) can be written as
d
dx
3
dx
3
or
Therefore
d x3 y3
dx - + y - = 0
-x3 + 3y - y3 =
(8)
where c is an arbitrary constant, is an equation for the integral curves of Eq. (6). A direction field and several integral curves are shown in Figure 2.2.1. An equation of the integral curve passing through a particular point (x0, y0) can be found by substituting x0 and y0 for x and y, respectively, in Eq. (8) and determining the corresponding value of c. Any differentiable function y = (x) that satisfies Eq. (8) is a solution ofEq. (6).
FIGURE 2.2.1 Direction field and integral curves of / = x2/(1 - y2).
Essentially the same procedure can be followed for any separable equation. Returning to Eq. (4), let H and H2 be any functions such that
Previous << 1 .. 21 22 23 24 25 26 < 27 > 28 29 30 31 32 33 .. 609 >> Next