Eigenvalue Method as a diferential equation!

wolly

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How did m+nt appear and how did n=0 and the other things appear? Also who is μμ?
I'm talking about an Eigenvalue Method as a differential equation and I don't know why this is solved like this.Can someone help me?
 
I don't understand the context, and I cannot read Romanian, but here is what I think about your first question:

m+ntm+nt appears because λ1\lambda_1, which is equal to -3, has multiplicity of 2.
 
I don't understand the context, and I cannot read Romanian, but here is what I think about your first question:

m+ntm+nt appears because λ1\lambda_1, which is equal to -3, has multiplicity of 2.
And n=0 c=-a-b r=d=s
IT says that IT results from Y'=AY?
 
I don't understand the context, and I cannot read Romanian, but here is what I think about your first question:

m+ntm+nt appears because λ1\lambda_1, which is equal to -3, has multiplicity of 2.
Do You have Something like a PDF that can show me how to solve this?
 
Do You have Something like a PDF that can show me how to solve this?
No, I don't have it. But it looks like pretty standard stuff about ODEs with constant coefficients. Don't you have a textbook? Where does this problem come from? Is it part of your homework?
 
No, I don't have it. But it looks like pretty standard stuff about ODEs with constant coefficients. Don't you have a textbook? Where does this problem come from? Is it part of your homework?
IT comes from a math college contest exercise book and I know how to solve some parts but not all of them!
I am referring to the eigenvalue and eigenvector Matrix Equations
 

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I am referring to the eigenvalue and eigenvector Matrix Equations
You need to learn the subject in a more systematic way. Asking for help on a forum is no substitute for studying.
 
The idea is as follows. If we have (AλI)(x)=0, (A-\lambda I)(x)=0, i.e. Ax=λx Ax=\lambda x then we solve y=λy y'=\lambda y and obtain y=meλt. y=me^{\lambda t}. However, we actually have for λ=3 \lambda=-3 that
(AλI)2(x)=0. (A-\lambda I)^2(x)=0. That means that either (AλI)(x)=0 (A-\lambda I)(x)=0 is already zero, in which case we get the solution y=meλt, y=me^{\lambda t}, or, and this is different, that (AλI)((AλI)(x))=0. (A-\lambda I)((A-\lambda I)(x))=0. Now
(AλI)(AλI)=A22λA+λ2I=0 (A-\lambda I)(A-\lambda I)=A^2-2\lambda A +\lambda^2 I=0 and we have to solve y2λy+λ2y=0. y''-2\lambda y'+\lambda^2y=0. Let's see if y=nteλt y=nte^{\lambda t} is a solution for this equation.

y=nteλty=neλt+nλteλt=neλt+λyy=nλeλt+λy=2nλeλt+λ2y\begin{array}{lll} y&=n te^{\lambda t}\\ y'&=ne^{\lambda t}+n\lambda te^{\lambda t}=n e^{\lambda t}+\lambda y\\ y''&=n\lambda e^{\lambda t}+\lambda y'=2n\lambda e^{\lambda t}+\lambda^2 y \end{array}y2λy+λ2y=2nλeλt+λ2y2λ(neλt+λy)+λ2y=0\begin{array}{lll} y''-2\lambda y'+\lambda^2 y&=2n\lambda e^{\lambda t}+\lambda^2 y-2\lambda(n e^{\lambda t}+\lambda y)+\lambda^2 y=0 \end{array}
Hence, it is a solution. Combining both, we get
y=meλt+nteλt=(m+nt)eλt. y=me^{\lambda t}+n te^{\lambda t}=(m+nt)e^{\lambda t}.This is the solution space for the generalized eigenspace λ=λ1=3 \lambda=\lambda_1=-3 with multiplicity two.
If we finally add the solution space for the generalized eigenspace λ=λ2=0 \lambda=\lambda_2=0 with multiplicity one, then we get
y=(m+nt)eλ1t+peλ2t=(m+nt)e3t+pe0t=(m+nt)e3t+p. y=(m+nt)e^{\lambda_1 t}+pe^{\lambda_2 t}=(m+nt)e^{-3t}+pe^{0\cdot t}=(m+nt)e^{-3t}+p. The parameters m,n,p m,n,p result from the initial values for the differential equation.
 
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