| 
 | 
|   | 
 
1  Why two terms?
 
Here's I'll explore why a second order linear homogeneous constant coefficient ordinary differential equation must always have two independent solutions.
Actually, the proof I give below will work for linear ODE's whose coefficients are not constants also.
Let's start with the differential equation
 
| 
a  | 
d2y
 dx2
  | 
+ b | 
dy
 dx
  | 
+ c y = 0. |   
 |   
Suppose we've found one solution, say y = y1(x). So, ay1"+by1�+cy1=0, since it's a solution. Suppose there is another
solution, y2(x). Whatever this other solution is, I can write y2(x) = f(x)y1(x) for some function f(x). It's very simple. Just let
 
Since I don't know y2(x), I don't know f(x) either. However, I do know that y2 (just like y1) is a solution to the differential
equation, so 
 
| 
a | 
d2
 dx
  | 
2
  
 
  | 
(f(x)y1(x)) + b | 
d
 dx
  | 
(f(x)y1(x)) + c(f(x)y1(x))=0. |   
 |   
By the product rule,
 
| 
 | 
d
 dx
  | 
(f(x)y1(x)) = f�(x)y1(x) + f(x)y1�(x) |   
 |   
and
 
| 
 | 
d2
 dxx
  | 
(f(x)y1(x)) = f"(x)y1(x) + 2f�(x)y1�(x) + f(x)y1"(x). |   
 |   
If we substitute these into the differential equation, we get
 
| 
a[f"(x)y1(x) + 2f�(x)y1�(x) + f(x)y1"(x)]+b[f�(x)y1(x) + f(x)y1�(x)]+cf(x)y1(x)=0. |   
 |   
I can rearrange this so that all the f(x) terms are together, and all the f�(x) terms, and the f"(x) term, giving
 
| 
ay1(x)f"(x) + [2ay1�(x)+by1(x)]f�(x) +[a y1"(x) + by1�(x)+cy1(x)]f(x)=0. |   
 |   
Since ay1"(x)+by1�(x)+cy1(x)=0, the last term disappears, giving 
 
| 
ay1(x)f"(x) + [2ay1�(x)+by1(x)]f�(x)=0. |   
 |   
Now remember that y1(x) is known. Letting g(x)=f�(x), so f"(x)=g�(x), this is just a first order separable ordinary differential equation for g(x).
 
| 
ay1(x) | 
dg
 dx
  | 
+ [2ay1�(x)+by1(x)]g=0, so |   
 |   
 
| 
ay1(x) | 
dg
 dx
  | 
 = - [2ay1�(x)+by1(x)]g, so |   
 |   
 
| 
a | 
� �
 | 
 | 
dg
 g
  | 
 = -  | 
� �
 | 
 | 
[2ay1�(x)+by1(x)]dx
 y1(x)
  | 
, |   
 |   
 
| 
 = - 2a  | 
� �
 | 
 | 
y1�(x)dx
 y1(x)
  | 
-  | 
� �
 | 
bdx, |   
 |   
 
Therefore (skipping a few steps), 
 
Since g(x) is not the zero function, f(x) is not a constant function, so y2(x)=f(x)y1(x) is a distinct solution 
independent of y1(x).
 
2  Finding extra solutions?
By the way, this method can be used to explain why, when the roots of the auxiliary equation are equal (say k and k), 
the general solution is y=Axekx + Bekx.
If the auxiliary equation is (m-k)2, then differential equation is ay"+by�+cy=0, where a=1, b=-2k and c=k2. 
We already have y1(x)=ekx as a solution. Then, the formula above gives
 
| 
g(x) =  | 
A e2kx
 (ekx)2
  | 
 = A. |   
 |   
If g(x)=A, then f(x) = Ax+B, so y2(x) = f(x)y1(x) = (Ax+B)ekx.
You knew there had to be a real reason, didn't you?
 
  File translated from
TEX
by 
TTH,
version 3.76. On 03 Oct 2006, 15:42.
 
 |    |