Section 9.8 is entitled “Higher Order Linear Equations.”
This is another one of those sections that is filled with
the wonderful gifts of theorems and definitions and propositions. It’s also
quite long. It’s also a section that is kind of a throwback to previous
sections. I’ve only skimmed it at this point, but I saw familiar words and
terms such as “linear independent”, “uniqueness and existence”, and
“Wronskian.” Of course, this is super exciting for me because I tend to be
better at summarizing these sections. Obviously the reason for this is that I’m
familiar with these terms, and the only difference between these terms from the
past and in the present is that the context is slightly different. In any
event, it’s not like the context is super different than before.
We’ll start out by talking about what a linear equation is;
it’s of the form
Back in section 8.1, we found out how to
replace higher-order equations with a single-order equation. We did this by
replacing the variables in the equation with new ones, e.g.
This system is a system of n equations
and n unknown functions x1, x2,…, xn. Because
of how we defined our variables, this is equivalent to our original equation
involving y. The function y(t) will be a solution to our original equation if
the following vector-valued function is a solution to the system of equations:
The matrix notation of our system would
be x’ = Ax + f. In this case, the
matrix A would be
Also, f(t) = (0, 0, … , F(t))T. So our original linear
equation would be homogeneous if F(t) = 0.
Also, the initial value problem for a
higher-order equation would look like
Here is a theorem concerning existence
and uniqueness:
“Suppose the coefficients of the equation
are continuous functions of t in an
interval (α,
β).
Then, for any t0 ∈ (α, β), and for any constants y0,
y1,…, yn-1, [the equation], together with the initial
conditions
has a unique solution defined for all t ∈ (α, β)”
(434).
So y(t) is a solution to the homogeneous
and higher-order equation
This is true if and only if x(t) = (y(t), y’(t),…, y(n-1))T
is a solution to x’ = Ax. A is still defined above. A theorem
concerning this notion: “Suppose that y1(t), y2(t),…, and
yk(t) are all solutions to [the equation above]. Then any linear
combination of these functions is also a solution” (435).
Onto a definition concerning linear
independence and linear dependence: “Suppose the functions y1(t), y2(t),…,
and yn(t) are all defined on the interval (α,
β).
The functions are linearly dependent if there are constants c1, c2,…,
and cn, not all equal to 0, such that
for all t ∈ (α,
β). The functions are linearly independent if they are not
linearly dependent” (435).
No seriously, that’s the wise definition of
linear independence. Now you know something important, specifically concerning
the relationship between linear independence and dependence, specifically that
they are not the same thing.
So it’s easy to know if two or three functions
are linearly independent or not. But what if you have a lot more than two or
three functions? Why, you look at the Wronskian, of course! :D
Let’s define the Wronskian of y1, y2,…,
and yn is the Wronskian of x1,
x2,…, and xn:
A proposition about this: “The solutions y1(t),
y2(t),…, yn(t) to [the homogeneous, higher-order equation
I presented a while ago] are linearly independent if and only if the
corresponding solutions to the system [x’
= Ax] are linearly independent.
This, in turn, is equivalent to W(t0) ≠ 0 for some t0”
(437).
A theorem concerning the structure of the
general solution: “Suppose that y1(t), y2(t),…, and yn(t)
are linearly independent solutions to [the homogeneous, higher-order equation].
Then every solution to [this higher-order equation] is a linear combination of
y1(t), y2(t),…, and yn(t)” (438).
The fundamental set of solutions is the set of
n solutions y1(t), y2(t),…, and yn(t) that are
linearly independent. Then the general solution is a linear combination
Remember when we looked for exponential
solutions to solve systems? Suppose we have a solution to the system x’ = Ax, i.e. x = (y, y’,…, y(n-1))T,
in which y is a solution to
The characteristic polynomial is denoted as
p(λ) and is to the differential equation above. The following equation is
called the characteristic equation:
The roots of the characteristic equation for
the differential equation above are equal to the eigenvalues of the matrix A in
the system x’ = Ax. If the characteristic equation has n
distinct roots, then the exponential solutions to the system are linearly
independent.
A theorem for you concerning real roots:
“If λ is a real root to the characteristic
polynomial of algebraic multiplicity q, then
are q linearly independent solutions” (441).
And now the corresponding theorem concerning
complex roots:
“If λ = α + iβ is a complex root of the
characteristic polynomial with multiplicity q, then so is λ = α – iβ. In
addition,
are 2q linearly independent solutions” (442).
I’m not a tremendously big fan of ending these
summary things with direct quote (mostly because the high school English
teacher that lives within my soul likes to remind me that starting or ending
with a quote from someone else is a big no-no in the world of high school
English papers; however, the college kid that lives within my soul likes to
remind me that this is not the world of high school English papers, and I
haven’t had to write a formal paper yet in my college career) but I’m doing so
anyway since this is the end of the summary. This means I have 9.9 to summarize
and then I’m done with summarizing chapter 9.
This also means I have two more chapters (4
and 5) and 12 more sections to summarize before I’m free from summarizing these
things. I am slightly exciting but also dreading this day, considering these
summaries take a couple of hours of boredom from my 12 credit semester and turn
them into semi-useful math hours.
I don’t know if I’ll have 9.9 up by tomorrow.
Actually, I can assure you that unless I get it up tonight (which is looking
less and less likely as these minutes whiz by me), 9.9 will be up on Tuesday.
Then I’ll be moving onto (or backwards to) chapter 4!
I’ll see you when I see you.
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