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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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Finally, we note that y = constant is also a solution of the D.E.
Following the procedure outlined, let v = dy/dt and y" = dv/dt = v dv/dy. Thus the D.E. becomes
yvdv/dy + v = 0, which is a separable equation with the solution v = c1/y. Next let v = dy/dt = c/y, which again
2
separates to give the solution y = c1t + c2.
Again let v = y' and v' = vdv/dy to obtain
22 2y v dv/dy + 2yv = 1. This is an exact equation with
-1 1/2
solution v = y (y + c^ . To solve this equation,
38
Section 3 . 2
1/2
we write it in the form ydy/(y+c1) = dt. On
observing that the left side of the equation can be
1/2
written as [(y+c1) - c1]dy/(y+c1) we integrate and
find (2/3)(y-2c1)(y+c1) 1/2 = t + c2.
39. If v = y', then v' = vdv/dy and the D.E. becomes v dv/dy + v2 = 2e y. Dividing by v we obtain
dv/dy + v = 2v 1e y, which is a Bernoulli equation (see Prob.27, Section 2.4). Let w(y) = v , then dw/dy = 2v dv/dy and the D.E. then becomes dw/dy + 2w = 4e y, which
is linear in w. Its solution is w = v2 = ce-2y + 4e-y.
Setting v = dy/dt, we obtain a separable equation in y and t, which is solved to yield the solution.
40. Since both t and y are missing, either approach used above will work. In this case it's easier to use the approach of Problems 28-33, so let v = y' and thus v' = y" and the D.E. becomes vdv/dt = 2.
43. The variable y is missing. Let v = y', then v' = y" and the D.E. becomes vv' - t = 0. The solution of the
22
separable equation is v = t + c1. Substituting v = y'
and applying the I.C. y'(1) = 1, we obtain y' = t. The positive square root was chosen because y' > 0 at t = 1. Solving this last equation and applying the I.C. y(1) = 2, 2
we obtain y = t /2 + 3/2.
Section 3.2, Page 145
2. W(cost,sint) =
cost sint -sint cost
2t ? 2t . = cos t + sin t = 1
4. W(x,xe ) =
xe
-I Ji
1 e + xe
x 2 x x 2 x
= xe + x e - xe = x e .
Dividing by (t-1) we have p(t) = -3t/(t-1), q(t) = 4/(t-1) and g(t) = sint/(t-1), so the only point of discontinuity is t = 1. By Theorem 3.2.1, the largest interval is - < t < 1, since the initial point is t0 = -2.
Section 3.2
39
12.
14.
15.
18.
21.
p(x) = 1/(x-2) and q(x) = tanx, so x = p/2, 2, 3p/2... are points of discontinuity. Since t0 = 3, the interval specified by Theorem 3.2.1 is 2 < x < 3p/2.
For y = t1/2, y' = 1-1/2 and y" = - 1-3/2. Thus
2 4
2 -1 -1 yy + (y) = -_ t + t = 0. Similarly y = 1 is also
44
1/2
a solution. If y = c1(1) + c2t is substituted in the
3/2
D.E. you will get -c1c2/4^ , which is zero only if
c1 = 0 or c2 = 0. Thus the linear combination of two
solutions is not, in general, a solution. Theorem 3.2.2 is not contradicted however, since the D.E. is not linear.
y = f (t) is a solution of the D.E. so L[f](t) = g(t). Since L is a linear operator,
L[cf](t) = cL[f](t) = cg(t). But, since g(t) n 0, cg(t) = g(t) if and only if c = 1. This is not a contradiction of Theorem 3.2.2 since the linear D.E. is not homogeneous.
W(f,g) =
t g 1 g'
f 2 t t
= tg - g = te, or g - g = te . This
1 t
g = tet
t
1 ' 1
g -
t t2
1 t
or ( g) = e . Integrating and multiplying by t we
t
obtain g(t) = tet + ct.
t -2t
From Section 3.1, e and e are two solutions, and
t -2t
since W(e ,e ) n 0 they form a fundamental set of solutions. To find the fundamental set specified by
Theorem 3 .2 .5, let y(t) = c1e + c2e -2t , where c1 and c2
satisfy
c1 + c2 = 1 and c1 - 2c2 = 0 for y1. Solving, we find
2 t y 1 = e 13 + 1 e 3 2t Likewise, c1 and c2 satisfy
c1 + c2 = 0 and c1 - 2c2 = 1 for y 2, so that
1 t y2 = _e 23 - 1 - e 3 2t
t
40
Section 3 . 2
25.
27.
30.
32.
34.
2
For y1 = x, we have x (0) - x(x+2)(1) + (x+2)(x) = 0 and
for y2 = xex we have x2(x+2)ex-x(x+2)(x+1)ex+(x+2)xex = 0.
x 2 x
From Problem 4, W(x,xe ) = x e n 0 for x > 0, so y1 and y2 form a fundamental set of solutions.
Suppose that
P(x)y" + Q(x)y' + R(x)y = [P(x)y']' + [f(x)y]'. On
expanding the right side and equating coefficients, we find f'(x) = R(x) and P'(x) + f(x) = Q(x). These two conditions on f can be satisfied if
R(x) = Q'(x) - P"(x) which gives the necessary condition
P"(x) - Q'(x) + R(x) = 0.
We have P(x) = x, Q(x) = - cosx, and R(x) = sinx and the condition for exactness is satisfied. Also, from Problem 27, f(x) = Q(x) - P'(x) = - cosx -1, so the D.E. becomes (xy')' - [(1 + cosx)y]' = 0. Hence
xy' - (1 + cosx)y = c1. This is a first order linear
D.E. and the integrating factor (after dividing by x) is m(x) = exp[-| x-1(1 + cosx)dx]. The general solution is
x
y = [m(x)] -1[c1l t-1 m(t)dt + c2]. Jx0
We want to choose m(x) and f(x) so that pi (x)P(x)y" + m(x)Q(x)y' + m (x)R(x)y = [p(x)P(x)y']' + [f(x)y]'.
Expand the right side and equate coefficients of y", y' and y. This gives m'(x)P(x) + p(x)P'(x) + f(x) = m(x)Q(x) and f'(x) = m(x)R(x). Differentiate the first equation and then eliminate f'(x) to obtain the adjoint equation Pm" + (2P' - Q)m' + (P" - Q' + R) m = 0.
2
P = 1-x , Q = -2x and R = a(a+1). Thus
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