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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
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+ b |
dy
dx
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+ c y = 0. |
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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
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2
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(f(x)y1(x)) + b |
d
dx
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(f(x)y1(x)) + c(f(x)y1(x))=0. |
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By the product rule,
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d
dx
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(f(x)y1(x)) = f�(x)y1(x) + f(x)y1�(x) |
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and
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d2
dxx
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(f(x)y1(x)) = f"(x)y1(x) + 2f�(x)y1�(x) + f(x)y1"(x). |
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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. |
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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. |
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Since ay1"(x)+by1�(x)+cy1(x)=0, the last term disappears, giving
ay1(x)f"(x) + [2ay1�(x)+by1(x)]f�(x)=0. |
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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
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+ [2ay1�(x)+by1(x)]g=0, so |
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ay1(x) |
dg
dx
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= - [2ay1�(x)+by1(x)]g, so |
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a |
� �
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dg
g
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= - |
� �
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[2ay1�(x)+by1(x)]dx
y1(x)
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, |
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= - 2a |
� �
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y1�(x)dx
y1(x)
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- |
� �
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bdx, |
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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
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= A. |
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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
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by
TTH,
version 3.76. On 03 Oct 2006, 15:42.
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