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Mathematics 22 Online
OpenStudy (kelvin8262):

Sturm Louiville Problem: Eigenvalues and Eigenfunction

OpenStudy (kelvin8262):

OpenStudy (kelvin8262):

what I have so far: if lambda>0, \[y(x)=c_1\cos(\sqrt(\lambda)x)+c_2\sin(\sqrt(\lambda)x)\] applied initial condition, c1 = 0. Differentiate the equation, \[y'(x) = \sqrt(\lambda)c_2\cos(\sqrt(\lambda)x\] applied the initial condition again, \[\sqrt(\lambda)c_2 \cos(4\sqrt(\lambda) = 0\] and then I am lost. as I do not how to continue: I try assuming c2 equal to zero. but still after i am not sure what to do.

OpenStudy (michele_laino):

I prefer to use complex numbers, so the solution above can be rewritten as follows: \[y\left( x \right) = {c_1}{e^{ - i\sqrt \lambda x}} + {c_2}{e^{i\sqrt \lambda x}}\] now if we apply the initial conditions, we get: \[ - i\sqrt \lambda c\left( {{e^{ - i4\sqrt \lambda }} + {e^{i4\sqrt \lambda }}} \right) = 1\]

OpenStudy (michele_laino):

wherein \(c_2=-c_1=-c\)

OpenStudy (michele_laino):

the corresponding solution of last equation is: \[\begin{gathered} 1 + {e^{i8\sqrt \lambda }} = 0 \hfill \\ \hfill \\ {e^{i8\sqrt \lambda }} = - 1 = {e^{i\left( {2n + 1} \right)\pi }},\quad n \in \mathbb{Z} \hfill \\ \end{gathered} \]

OpenStudy (michele_laino):

so we get: \[\large {\lambda _n} = \frac{{{\pi ^2}}}{{64}} \cdot {\left( {2n + 1} \right)^2},\quad n \in \mathbb{Z}\]

OpenStudy (michele_laino):

oops.. I made a typo: \[y'\left( 4 \right) = - i\sqrt \lambda c\left( {{e^{ - i4\sqrt \lambda }} + {e^{i4\sqrt \lambda }}} \right) = 0\]

OpenStudy (michele_laino):

nevertheless the solutions are the same

OpenStudy (kelvin8262):

So do you get lambda_n from the equation after applying the initial conditions?

OpenStudy (kelvin8262):

@Michele_Laino i just don't quite understand how do you transform the equation to find lambda.

OpenStudy (michele_laino):

here are the steps: \[\begin{gathered} y'\left( 4 \right) = - i\sqrt \lambda c\left( {{e^{ - i4\sqrt \lambda }} + {e^{i4\sqrt \lambda }}} \right) = 0 \Rightarrow {e^{ - i4\sqrt \lambda }} + {e^{i4\sqrt \lambda }} = 0 \Rightarrow \hfill \\ \hfill \\ \Rightarrow \frac{1}{{{e^{i4\sqrt \lambda }}}} + {e^{i4\sqrt \lambda }} = 0 \Rightarrow \frac{{1 + {e^{i8\sqrt \lambda }}}}{{{e^{i4\sqrt \lambda }}}} = 0 \Rightarrow {e^{i8\sqrt \lambda }} = - 1 \hfill \\ \end{gathered} \]

OpenStudy (michele_laino):

furthermore, in the complex plane we can write this: \[ - 1 = {e^{i\left( {2n + 1} \right)\pi }},\quad n \in \mathbb{Z}\]

OpenStudy (kelvin8262):

@Michele_Laino ah... now i see. just basically now i just apply the lambda back to my equation y. which mean my eigenfucntion would be: \[y(x) = \sin (\pi x/8)\] is it?

OpenStudy (michele_laino):

I got this: \[{y_n}\left( x \right) = {a_n}\sin \left( {\sqrt {{\lambda _n}} x} \right)\]

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