dionysian said:
Chris Hillman,
Thank you for restating my question I know see what I was really asking. Now my book does give a theorem about a fundamental set of solutions and the jist of it goes something like this "a set of n linearly independent solutions of the homogenous nth order diff equation is said to be a fundamental set of solutions". I understand the part about linearly independence of the functions “the wronksian has to never equal zero", but I don’t see an explicit theorem or proof that the solution set is "complete".
Now you mentioned the solution space, I like this, does this "kind of mean" that the solution set is a basis or is it a full fledge basis? I would think that it would be a basis of the solution space. And if it is that would mean that the dimension of the solution space for the "second order linear homogenous equations with const coeff" is 2, is that correct?
Yes. It is not terribly difficult to show that the set of all solutions to a linear, homogeneous, n
th order differential equation forms an n dimensional linear vector space. If you have n independent solutions then they must form a basis and so also "span" the space of solutions: every solution can be written as a linear combination of them. By the way, while it is true that a set of n solutions is independent if and only if the Wronskian is not 0, the
definition of independence (you should remember from linear algebra) is that no vector in the set can be written as a linear combination of the others.
And if it is correct is there a theorem about the order of the equation and the dimensions of the solution space? For example, a third order equation will have a 3 dimensional solution space... etc? Because it seems to me that if there is theorem about the dimensions of a solution space of the DE and we able to find n linear independent vectors of a n dimensional solution space we could say that the fundamental set is complete. I am I on the right track here or is this a bunch of crap?
Yes, that is exactly right. As I said before the set of all solutions to a linear homogeneous n
th order differential equation forms an n dimensional vector space.
Here's an outline of the proof (which, in detail, is very deep). First rewrite the equation as a system of n first-order equations. You can do that by assigning new variable names to each derivative. For example, if you differential equation is y
(n)= f(x,y', y", ...), let u= y', v= y", ,,, w= y
(n-1)etc. so the equation becomes w'= f(x, u, v, ... , w) while we also have y'= u, u'= v, etc. Now rewrite
that as a single vector equation \frac{dY}{dx}= F(x, Y) where Y is the vector having y, u, v, etc. as components. In particular, if the original equation is a homogeneous, linear, n
th order differential equation, that final equation can be written \frac{dY}{dx}= AY where A is an n by n matrix whose components depend on x only and Y can be written as an n dimensional column vector. The "deep" part is recognizing that the set of all such vectors has much the same properties as the real numbers: it is a complete metric space. That means the "Banach fixed point principle", which is used in Poincare's "existance and uniqueness theorem" for initial value problems is valid.
Poincare's "existance and uniqueness theorem" essentially says that as long as f(x,y) is continuous in both variables and "Lipschitz" in y for some region around (x
0,y
0) then there exist a unique solution to the differential equation y'= f(x,y) satisfying y(x
0)= x
0. Use that to show that there exist a unique function y
1(x) satisfying the differential equation and initial condition y(x
0)= 1, y'(x
0)= 0, y"(x
0)= 0,.., y
(n-1)(x
0)= 0. Then there exist another function y
2[/sup], satisfying the differential equation and y(x0)= 0, y'(x0)= 1, y"(x0)= 0,... ,yn-1(x0)= 0. There exist yet a third function satisfying the differential equation and y(x0)= 0, y'(x0)= 0, y"(x0)= 1, ..., y(n-1)(x0)= 0. We can continue until we have an nth function satisfying the differential equation and y(x0)= 0, y'(x0)= 0, y"(x0)= 0, ..., yn-1(x0)= 1. Since the values are different at x0, it's easy to show that these functions are independent. Also given any function y(x) satisfying the differential equation and y(x0)= A, y'(x0)= B, y"(x0)= C, ..., y(n-1)(x0)= Z, it is easy to show that
y(x)= Ay1(x)+ By2[/sup](x)+ Cy3(x)+ ...+ Zyn(x): that is, that this set of "fundamental solutions" spans the set of all solutions. Since we have n functions (vectors) that are independent and span the space of solutions, the space is n-dimensional.
Thank you again for the help, I very much appreciate it. I am reviewing and trying to make sense of all the theory and methods for solving DEs in my DE book. I finished my DE class last year and was able to memorize all the methods I needed to solve the equations and pass my tests, but most of it still seems mysterious to me and that bugs me. Is there any book out there anyone could recommend that would help shed light on the methods such as “undetermined coefficients”, “variation of parameters” ,”exact equations”, “series solution to DE” and where they came from?[/QUOTE]