Why do 2nd-order linear ODEs have at most two independent solutions?

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Homework Help Overview

The discussion revolves around the properties of second-order linear ordinary differential equations (ODEs), specifically focusing on why such equations always have two linearly independent solutions. The original poster questions the sufficiency of the characteristic polynomial argument in this context.

Discussion Character

  • Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Some participants discuss the nature of the solution set for linear homogeneous ODEs, suggesting that it forms an n-dimensional vector space. Others explore the implications of having a non-homogeneous equation and how it relates to the solutions of the homogeneous case.

Discussion Status

Participants are actively engaging with the concepts of vector spaces and the properties of solutions to linear ODEs. There is a focus on understanding the foundational aspects of vector spaces and how they apply to the solutions of differential equations. Some guidance has been offered regarding the structure of the solution space, but no consensus has been reached.

Contextual Notes

There are references to the "existence and uniqueness theorem" and the concept of "fundamental solutions," which are being discussed in relation to the dimensionality of the solution space. The discussion also touches on the distinction between homogeneous and non-homogeneous equations.

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Homework Statement



Why does the following ODE ALWAYS have two linearly independent solutions?

x''(t) + a(t) x'(t) + b(t) x(t) = f(t)


The characteristic polynomial argument is not sufficient?
 
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That's a linear equation. It's fairly easy to show that the set of all solutions to an nth order linear homogeneous (f(t)= 0) differential equation forms an n dimensional vector space with the usual addition of functions and multiplication by a number. With f(t) NOT 0, the solution set is a "linear manifold" (think of a plane that does NOT contain the origin) so there exist a function such that every solution can be written as a member of an n dimensional vector space plus that function. The two linearly independent solutions are the "basis vectors" of the two dimensional vector space.
 
Any mathematical elaboration I can have?
 
Do you understand what a "vector space" is?

In order to show that a set, with a given "addition" and "scalar multiplication" is a vector space you must show three things:
1) It is non empty. You can do that by showing that it contains the "zero vector" (the additive identity). Here, since the addition is ordinary addition of functions, the additive identity is the 0 function: f(x)= 0 for all x. Show that y= 0 satisfies [tex]a_n(t)y^{(n)}+ a_{n-1}y^{(n-1)}+ \cdot\cdot\cdot+ a_1y'+ a_0y= 0[/tex] for any functions. (The superscript in parentheses indicates the derivative.)

2) It is "closed under scalar multiplication". To do that show that if y(t) satisfies [tex]a_n(t)y^{(n)}+ a_{n-1}y^{(n-1)}+ \cdot\cdot\cdot+ a_1y'+ a_0y= 0[/tex] then so does ay(t) for any number a. That's just a matter of factoring out a.

3) It is "closed under addition". If y= u(t) and y= v(t) both satisfy [tex]a_n(t)y^{(n)}+ a_{n-1}y^{(n-1)}+ \cdot\cdot\cdot+ a_1y'+ a_0y= 0[/tex] then so does y= u+ v. That can be done because the nth derivative is itself "linear"- the nth deriviative of u+ v is the nth derivative of u plus the nth derivative of v.

To show that the solution set of a linear homogeneous nth order equation is a vector space of dimension n, use the "existence and uniqueness theorem" to define the n functions, [itex]u_1[/itex] that satisfies the given equation with initial conditions [itex]u_1(0)= 1[/itex], [itex]u_1'(0)= u_1''(0)= \cdot\cdot\cdot= u_1^{(n-1)}(0)= 0[/itex], [itex]u_2(0)= 0[/itex], [itex]u_2'(0)= 1[/itex], [itex]u_2''(0)= \cdot\cdot\cdot= u_2^{(n-1)}(0)= 0[/itex], etc., with "[itex]u_i(t)[/itex]" being the solution to the differential equation having its ith derivative equal to 1 at t= 0 and all other values 0.

Those are sometimes referred to as the "fundamental solutions" to the differential equation. They have this very nice property: if y(t) is any solution to the differential equation, let [itex]A_1= y(0)[/itex], [itex]A_2= y'(0)[/itex], ... , [itex]A_{n}= y^{(n-1)}(0)[/itex]. Then it is easy to show that [itex]y(t)= A_1u_1(t)+ A_2 u_2(t)+ \cdot\cdot\cdot+ A_{n}u_{n-1}(t)[/itex]. That is, any solution to the differential equation can be written as a linear combination of the "fundamental solutions" so they form a basis for the vector space of all solutions showing that the vector space has dimension n. Any solution can be written as a linear combination of those n independent solutions.

Now, for the non-homogeneous equation, let Y(t) be any function satisfying the equation [itex]a_n(t)y^{(n)}+ a_{n-1}y^{(n-1)}+ \cdot\cdot\cdot+ a_1y'+ a_0y= f(x)[/itex]. Then it is easy to show that if y is any other function satisfying that equation, u(t)= y(t)-Y(t) satisfies the equation [itex]a_n(t)y^{(n)}+ a_{n-1}y^{(n-1)}+ \cdot\cdot\cdot+ a_1y'+ a_0y= 0[/itex]. That is, that y(t)= u(t)+ Y(t), it is the sum of a function in the vector space of solutions to the homogeneous equation plus that one given solution to the entire equation.
 

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