Chapter 4, Section 5

Answers and solutions to selected problems

2. Here we consider the DE

x' + 3x = 5 cos t

a) The associated operator is L(x) = x' + 3x and this is a linear, homogeneous operator

b) The homogeneous solution, [Graphics:sect4.5_hmwkgr1.gif], is found by solving L(x) = ) or
' + 3x = 0. It should be relatively clear to us at this stage that
x = [Graphics:sect4.5_hmwkgr2.gif] is a solution, i.e. [Graphics:sect4.5_hmwkgr3.gif] (If this is not clear, separate varialbes, integrate, etc). We should also note that [Graphics:sect4.5_hmwkgr4.gif] is also a solution

c) Suppose [Graphics:sect4.5_hmwkgr5.gif] , then


[Graphics:sect4.5_hmwkgr6.gif]

d)
[Graphics:sect4.5_hmwkgr7.gif]

e)
[Graphics:sect4.5_hmwkgr8.gif]

f) For x' + 3x = 10 cos t or L(x) = 10 cos t, we have the same [Graphics:sect4.5_hmwkgr9.gif] since the homogeneous DE si the same, namely L(x) = 0 or x' + 3x = 0. The function for [Graphics:sect4.5_hmwkgr10.gif] will change, since we now need [Graphics:sect4.5_hmwkgr11.gif]; so the new [Graphics:sect4.5_hmwkgr12.gif] should be 2* the original one or [Graphics:sect4.5_hmwkgr13.gif]

4. The DE is x" + 4x = 2 which is linear by Theorem 4.7

a) The operator is L(x) = x" + 4x

b) sin 2t and cos 2t both satisfy the DE x" + 4x = 0 (Problem #8 from section 4.4 is very important in this respect) Since this is a linear homogeneous DE, the superposition principle applies and [Graphics:sect4.5_hmwkgr14.gif]
is also a solution

c) If [Graphics:sect4.5_hmwkgr15.gif] then [Graphics:sect4.5_hmwkgr16.gif] is a solution to x" + 4x = 2, since x" = 0 and [Graphics:sect4.5_hmwkgr17.gif]

d) Again we have [Graphics:sect4.5_hmwkgr18.gif]

e)
[Graphics:sect4.5_hmwkgr19.gif] ,

so [Graphics:sect4.5_hmwkgr20.gif] is not s solution.

6. The DE is v'= - g - k*v or v' + k*v = -g

a) The homogeneous solution solves v' + k*v = 0 and is the function [Graphics:sect4.5_hmwkgr21.gif] The general solution is (we can get this ourselves by using integrating factors)

[Graphics:sect4.5_hmwkgr23.gif][Graphics:sect4.5_hmwkgr22.gif]
[Graphics:sect4.5_hmwkgr23.gif][Graphics:sect4.5_hmwkgr24.gif]

We know this is the sum of the particular and homogeneous solutions, so we can see that a particular solution is [Graphics:sect4.5_hmwkgr25.gif] where the homogeneous solution(from above) is [Graphics:sect4.5_hmwkgr26.gif]

b) The position function satisfies the DE x' = v, so we simply integrate v(t) to get to x(t)

[Graphics:sect4.5_hmwkgr23.gif][Graphics:sect4.5_hmwkgr27.gif]
[Graphics:sect4.5_hmwkgr23.gif][Graphics:sect4.5_hmwkgr28.gif]

Remembering to add a constant of integration we get [Graphics:sect4.5_hmwkgr29.gif]

d) The constant [Graphics:sect4.5_hmwkgr30.gif] is the initial velocity, i.e. v(0) and the second constant [Graphics:sect4.5_hmwkgr31.gif] is the initial position, x(0).

8. For the DE x' + x/t = 1 we have an integrting factor of [Graphics:sect4.5_hmwkgr32.gif] for t>0.

Multiplying by this factor gives us t*x' + x = t or

[Graphics:sect4.5_hmwkgr33.gif] and integrating with respect to t produces

[Graphics:sect4.5_hmwkgr34.gif] or [Graphics:sect4.5_hmwkgr35.gif]

Using x(1) = 1, solving for c yields that [Graphics:sect4.5_hmwkgr36.gif] and the solution is [Graphics:sect4.5_hmwkgr37.gif]

The interval of existence is (0, ∞), since the initial value is x(1) = 1 or more specifically t = 1 and [Graphics:sect4.5_hmwkgr38.gif] has a discontinuity at t = 0 which divided the reals into two intervals ( -∞, 0 ) and ( 0, ∞); the initial value of t is in the second of these intervals, so that's our interval of existence.

[Graphics:sect4.5_hmwkgr23.gif][Graphics:sect4.5_hmwkgr39.gif]