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Elementary differential equations 7th edition - Boyce W.E

Boyce W.E Elementary differential equations 7th edition - Wiley publishing , 2001. - 1310 p.
ISBN 0-471-31999-6
Download (direct link): elementarydifferentialequat2001.pdf
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.(1)
.(2)
CiX'"' + c2x solutions, then x = cix
Assume that if x (1)
(1)
.(2)
x
(k)
are
+ + ckx
(k)
is a solution.
Then use Theorem 7.4.1 to conclude that x + c^+1x(k+1) is
also a solution and thus c1x(1) +
+ ck+1x(k+1) is a
solution if x(1), ..., x(k+1) are solutions. 2a. From Eq.(10) we have W =
x11)
x(2)
x21)
x2
(2)
= x11) x(2)
x(1) x12)
Taking the
derivative of these two products yields four terms which may be written as
Section 7.4
135
dW = [ dt
dx11(
x22)
xi1
dx12)
] + [ x1
(1)
dx(2)
dx(1)
x(2)].
dt dt dt dt
The terms in the square brackets can now be recognized as the respective determinants appearing in the desired solution. A similar result was mentioned in Problem 20 of Section 4.1.
2b.
2c.
If x
(1)
is substituted into Eq.(3) we have = P11 x11) + P12 x21)
dx11) dt dx21) dt
Substituting the first equation above and its counterpart
= P21 x11) + P22 x21)
for x
(2)
into the first determinant appearing in dW/dt
and evaluating the result yields p11
x11)
x21)
x(2)
x(2)
= puW.
Similarly, the second determinant in dW/dt is evaluated as p22W, yielding the desired result.
dW
From prt b we have = [p11(t) + p22(t)]dt which gives
W
W(t) = c expl[pn(t) + p22 (t)]dt.
6a. W =
= 2t
2
t2 = t2.
t t2
1 2t
6b. Pick t = t0, then c1x(1) (t0) + c2x(2) (t0) = 0 implies
, which has a non-zero solution
rT O ( 12 ^ t0 ' 0 N
c1 + c2 = 0 V J
V 1 , v 2t0 ,
t0 t20
= 2t0
t02 = t20 = 0.
for c1 and c2 if and only if
1 2t0
Thus x(1) (t) and x(2) (t) are linearly independent at each point except t = 0. Thus they are linearly independent on every interval.
6c. From part a we see that the Wronskian vanishes at t = 0, but
not at any other point. By Theorem 7.4.3, if p(t), from
Eq.(3), is continuous, then the Wronskian is either identically zero or else never vanishes. Hence, we conclude that the D.E. satisfied by x(1) (t) and x(2) (t) must have at
least one discontinuous coefficient at t = 0.
6d. To obtain the system satisfied by x(1) and x
(2) we
136
Section 7.5
consider
x = c1x(1) + c2x(2), or
/ \ x1
x2
= c1
+ c2
t2
2t
( ' 3 / - ~\ / ^ \
x1 111 2t
= ci 1 + c2
v x2, V 0 V 2 y
Taking the derivative we obtain
Solving this last system for ci and c2 we find ci = xi - tx2 and c2 = x2/2. Thus
, which yields
xi = tx1 - x2 and x2 = x2. Writing this system in 2
/ \ x1 ^ t ^ x2 2 t2
. CN X V i . II +
V x2 y V 1 y 2 V 2t y
matrix form we have x =
t - t2/2
x'. Finding the
inverse of the matrix multiplying x' yields the desired solution.
Section 7.5, Page 381
1. Assuming that there are solutions of the form x = ?ert, we substitute into the D.E. to find
r%e
rt
'3 -2"
%ert. Since % = I% =
1 0
0 1
write this equation as
'3 -2"
thus we must solve
3-r -2
% - r V

%1 0
%2 y V 0
%, we can % = 0 and
for r, %i, %2-
1 0 0 1/
The determinant of the coefficients is (3-r)(-2-r) + 4 = r2 - r - 2, so the eigenvalues are r = -1, 2. The eigenvector corresponding to r = -1
satisfies
Thus x(1)(t) = %(1)e
' 4 -2 1 ' 0 N
V 2 t1 1 V%2 y II V 0 y
(1) ^-t
1
, which yields 2%1 - %2 = 0.
e , where we have set %1 = 1.
(Any other non zero choice would also work). In a similar fashion, for r = 2, we have
or ^1 - 2^2 = 0. Hence x(2)(t) = ?(2)e2t = e2t by
/ . . \ it 3 / ~ \
1 -2 %1 0
V 2 -4 y V%2 y V 0 y
2
11J
2
i2 -2 j
i2 -2 )
i 2 -2-r)
K 2 )
Section 7.5
137
setting = 1* The general solution is then
x = c^(1) (t) + c2x(2 ^ (t)* To sketch the trajectories we follow the steps illustrated in Examples 1 and 2*
/ \ x1 ' 1 '
Setting c2 = 0 we have x = = c1
V X2 y V 2 y
e or x1
c1e
-t
and x2 = 2c1e-t and thus one asymptote is given by x2 = 2x!. In a similar
fashion c! = 0 gives x2 = (l/2)x1 as a second
asymptote. Since the roots differ in sign, the trajectories for this problem are similar in nature to those in Example 1. For c2 ^ 0, all solutions will be
asymptotic to x2 = (l/2)x1 as t ^ ^. For c2 = 0, the
solution approaches the origin along the line x2 = 2x1.
5. Proceeding as in Problem 1 we assume a solution of the form x = ? ert, where r, ^1, ?2 must now satisfy
Evaluating the determinant of the
coefficients set equal to zero yields r = -1, -3 as the
eigenvalues* For r = -1 we find 't)1 = ^2 and thus
' -2-r 1^ '?1 ' ' 0 '
, 1 -2-r, v?2 y V 0 y
?(1)
?(2)
1
1
and for r = -3 we find ^2 = -^1 and hence The general solution is then
' 1N ' 1 N
x = c1 e-t + c2
V 1 y v-1 y
-3t
Since there are two negative
eigenvalues, we would expect the trajectories to be similar to those of Example 2*
Setting c2 = 0 and eliminating t (as in Problem 1) we find
that
1
1
e t approaches the
1
origin along the line x2 = x1* Similarly
the origin along the line
e 3t approaches
e
138
Section 7.5
x2 = -x2. As long as ci ^ 0 (since e- is the dominant term as t^0), all trajectories approach the origin asymptotic to x2 = x1. For c1 = 0, the trajectory approaches the origin along x2 = -x1, as shown in the graph.
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