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,
, is found by solving L(x) = ) or
' + 3x = 0. It should be relatively clear to us at this stage that
x =
is a solution, i.e.
(If this is not clear, separate varialbes, integrate, etc). We should also note that
is also a solution
c) Suppose
, then
![[Graphics:sect4.5_hmwkgr6.gif]](sect4.5_hmwkgr6.gif)
d)
![[Graphics:sect4.5_hmwkgr7.gif]](sect4.5_hmwkgr7.gif)
e)
![[Graphics:sect4.5_hmwkgr8.gif]](sect4.5_hmwkgr8.gif)
f) For x' + 3x = 10 cos t or L(x) = 10 cos t, we have the same
since the homogeneous DE si the same, namely L(x) = 0 or x' + 3x = 0. The function for
will change, since we now need
; so the new
should be 2* the original one or ![[Graphics:sect4.5_hmwkgr13.gif]](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]](sect4.5_hmwkgr14.gif)
is also a solution
c) If
then
is a solution to x" + 4x = 2, since x" = 0 and ![[Graphics:sect4.5_hmwkgr17.gif]](sect4.5_hmwkgr17.gif)
d) Again we have ![[Graphics:sect4.5_hmwkgr18.gif]](sect4.5_hmwkgr18.gif)
e)
,
so
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
The general solution is (we can get this ourselves by using integrating factors)
![[Graphics:sect4.5_hmwkgr23.gif]](sect4.5_hmwkgr23.gif)
![[Graphics:sect4.5_hmwkgr22.gif]](sect4.5_hmwkgr22.gif)
![[Graphics:sect4.5_hmwkgr23.gif]](sect4.5_hmwkgr23.gif)
![[Graphics:sect4.5_hmwkgr24.gif]](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
where the homogeneous solution(from above) is ![[Graphics:sect4.5_hmwkgr26.gif]](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]](sect4.5_hmwkgr23.gif)
![[Graphics:sect4.5_hmwkgr27.gif]](sect4.5_hmwkgr27.gif)
![[Graphics:sect4.5_hmwkgr23.gif]](sect4.5_hmwkgr23.gif)
![[Graphics:sect4.5_hmwkgr28.gif]](sect4.5_hmwkgr28.gif)
Remembering to add a constant of integration we get ![[Graphics:sect4.5_hmwkgr29.gif]](sect4.5_hmwkgr29.gif)
d) The constant
is the initial velocity, i.e. v(0) and the second constant
is the initial position, x(0).
8. For the DE x' + x/t = 1 we have an integrting factor of
for t>0.
Multiplying by this factor gives us t*x' + x = t or
and integrating with respect to t produces
or ![[Graphics:sect4.5_hmwkgr35.gif]](sect4.5_hmwkgr35.gif)
Using x(1) = 1, solving for c yields that
and the solution is ![[Graphics:sect4.5_hmwkgr37.gif]](sect4.5_hmwkgr37.gif)
The interval of existence is (0, ∞), since the initial value is x(1) = 1 or more specifically t = 1 and
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]](sect4.5_hmwkgr23.gif)
![[Graphics:sect4.5_hmwkgr39.gif]](sect4.5_hmwkgr39.gif)