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# 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.
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2. Hence
y(t)
2te^
The characteristic equation is
22 r + 4r + 4 = (r+2) = 0, which
has the repeated root r = -2.
Since the I.C. are given at
t = -1, write the general solution
Then
as y
-2(t + 1) -2(t + 1)
¿ + c2te
0 -2(t+1) -2(t+1) ~ . -2(t + 1) , ^
y = -2c1e + c2e - 2c2te and hence
2 and -2c1+3c2
1 which yield c1 = 7 and c2
5.
Thus y = 7e 2(t+1) + 5te 2(t+1), a decaying exponential as shown in the graph.
17a. The characteristic equation is 4r + 4r + 1 = (2r+1) = 0,
-t/2
so we have y(t) = (c1+c2t)e . Thus y(0) = c1 = 1 and y'(0) = -c1/2 + c2 = 2 and hence c2 = 5/2 and
y(t)
(1 + 5t/2)e
t/2
17b. From part (a), y'(t) =
1 -t/2 5 -t/2
— (1 + 5t/2)e ' + —e ' = 0, when
22
1 5t 5 8 -4/5
- — - ------- + — = 0, or t0 = — and y0 = 5e .
2 4 2 0 5 0
c
1
c1 c2
48
Section 3 . 5
11 17c. From part (a), - — + c2 = b or c2 = b + — and
2 2 2 2
y(t) = [1 + (b + 1)t]e-t/2.
2
1 1 -t/2 1 -t/2 17d. From part (c), y(t) = - — [1 + (b+— )t]e ' + (b+— )e ' = 0
2 2 2
4b
which yields tM = ---------- and
11 2b+1
,, 2b + 1 4b -2b/(2b+1) -2b/(2b+1)
yM = (1 + --------- • ------)e ' = (1 + 2b)e .
1 2 2b+1
rt
19. If r1 = r2 then y(t) = (c1 + c2t)e 1 . Since the exponential
is never zero, y(t) can be zero only if c1 + c2t = 0, which
yields at most one positive value of t if c1 and c2 differ
in sign. If r2 > r1 then
r,t r2t r,t , (r,-r,)t. , .
y(t) = c1e 1 + c2e 2 = e 1 (c1 + c2e 2 1 ). Again, this is
zero only if c1 and c2 differ in sign, in which case
ln(-c1/c2)
t =
(r2-r1)
21. If r2 Ï r1 then f(t;r1,r2) = (er2t - er1t)/(r2 - r1) is
defined for all t. Note that f is a liner combination of
r t r t
two solutions, e 1 and e 2 , of the D.E. Hence, f is a solution of the differential equation. Think of r1 as fixed and let r2 ^ r1. The limit of f as r2 ^ r1 is
indeterminate. If we use L'Hopital's rule, we find
r2t r.t . r2t
e 2 - e 1 • te 2 r t
lim ------------- • = lim ---------- = te 1 . Hence, the
r2 ^ r1 r 2 - r1 r2 ^ r1 1
rt
solution f(t;r1,r2) ^ te 1 as r2 ^ r1.
25. Let y2 = v/t. Then y'2 = v'/t - v/t2 and
y2 = v"/t - 2v'/t2 + 2v/t3. Substituting in the D.E. we obtain
t2 (v"/t - 2v'/t2 + 2v/t3) + 3t(v'/t - v/t2) + v/t = 0. Simplifying the left side we get tv" + v' = 0, which yields v' = c1/t. Thus v = c1lnt + c2. Hence a second solution is y2(t) = (c1lnt + c2)/t. However, we may set c2 = 0 and c1 = 1 without loss of generality and thus we have y2(t) = (lnt)/t as a second solution. Note that in
Section 3.5
49
the form we actually calculated, y2(t) is a linear combination of 1/t and lnt/t, and hence is the general solution.
27. In this case the calculations are somewhat easier if we
2
do not use the explicit form for y1(x) = sinx at the beginning but simply set y2(x) = y1v. Substituting this form for y2 in the D.E. gives x(y1v) "-(y1v)/+4x3(y1v) = 0.
On carrying out the differentiations and making use of the fact that y1 is a solution, we obtain
// f /
xy1v + (2xy1 - y1)v = 0. This is a first order linear
equation for v', which has the solution v' = cx/(sinx2) 2.
2
Setting u = x allows integration of this to get 2
v = c1 cotx + c2. Setting c1 = 1, c2 = 0 and multiplying
by y1 = sinx2 we obtain y2(x) = cosx2 as the second solution of the D.E.
30. Substituting y2(x) = y1(x)v(x) in the D.E. gives
2 n f 2 1
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